T AND-PHYSICS-OF BUILDING-MATERIALS :: ALAN-E-MUNBY :: Class No fJooR Xo- FRANKLIN INSTITUTE LIBRARY PHILADELPHIA, PA. REFERENCE Introduction to the Chemistry and Physics of Building Materials The "Westminster" Series. Crown 8vo. Fully Illustrated. $2.00 net each. The Chemistry and Physics of Building Materials, By Alan E. Munby, M.A., Cantab. The Manufacture of Paper. By R. W. Sindall F.C.S. Timber. By J. R. Baterden, A.M.I.C.E. Electric Lamps. By Maurice Solomon, A.C.G.I., A.M.I.E.E. Textiles and their Manufacture. By Aldred Barker, M.Sc, Technical College, Bradford. Gold and Precious Metals. By Thomas K. Rose, D.Sc, of the Royal Mint. Ornamental Glass Work. By A. L. Duthie. The Railway Locomotive. By Vadghan Pendred, M.I.Mech.E., late Editor of " The Engineer." Iron and Steel. By J. H. Stansbie, B.Sc. (Lond.), F.I.C. Town Gas for Lighting and Heating. By W. H. Y. Webber, C.E. Liquid and Gaseous Fuels, and the Part they play in Modern Power Production. By Professor Vivian B. Lewes, F.I.C, F.C.S. , Prof, of Chemistry, Royal Naval College, Greenwich. Electric Power and Traction. By F, H. Davies A. M.I.E.E. Coal. By James Tonge, M.I.M.E., F.G.S., etc., Lecturer on Mining at Victoria University, Manchester. India-Rubber and its Manufacture, with Chapters on Gutta-Percha and Balata. By H. L. Terry, F.I.C. Assoc.Inst.M.M. The Book: Its History and Development. By Cyril Davenport, F.S.A. Glass. By Walter Rosenhain. Superintendent of the Department of Metallurgy in the National Physical Laboratory. Patents, Trade Marks and Designs. By Kenneth R. Swan, B.A. (Oxon.), of the Inner Temple, Barrister-at- Law. Precious Stones. With a Chapter on Artificial Stones. By W. Goodchild, M.B., B.Ch. Electro- Metallurgy. By J B. C. Kershaw, F.I.C. Natural Sources of Power. By Robert S. Ball B. Sc, A.M.I.C.E. Radio-Telegraphy. By C. C. F. Monckton, M.I.E.E. * Further volumes mill appear at short intervals. Introduction to the Chemistry and Physics of Building Materials BY Alan E. Munby, M.A. (Cantab.) Associate of the Royal Institute of British Archi- tects ; Fellow of the Chemical Society; Member of the R.I.B.A. Standing Committee on Science ; Lecturer on the Chemistry and Physics of Materials to the L.C.C. School of Building; Author of " Simple Experiments in Magnetism and Electricity " ; Joint Author of "Practical Notes for Architectural Draughtsmen" NEW YORK D. VAN NOSTRAND COMPANY 23 MURRAY AND 27 WARREN STREETS 1909 PREFACE — ♦ — The great advances in science in recent years and the increasing use of scientific methods have not left the field of work connected with building materials untouched, and developments in technical training have made it essential that the elementary principles of science which underlie this study should be readily accessible. Great powers and, therefore, great responsibilities are placed in the hands of those whose duty it is to select and specify the materials used in buildings, and while a know- ledge of the principles underlying such use is an essential part of their educational equipment, these principles must be equally familiar to the manufacturers and even the workers in the building trades who wish to be prepared to meet competition, and combat causes of failure in materials. The rule of thumb methods which did duty in the past are incapable of meeting the needs of increasing knowledge, and while the specialist and expert are always ready to advise and are now necessary factors in dealing with the complex problem of modern building, those who consult them should be, at least, in a position to direct and control their assistance. 178G7 vi PEEFACE There are many workers in the field under discussion who, either through lack of training in elementary science or owing to the lapse of time since such training was acquired, find it difficult to digest with facility the legion of technical books dealing with materials. Again, other occupations often make it impossible to devote time to any general study of pure science as a preparation for such technical reading, and it is with the object of enabling those interested to attain such knowledge without recourse to a series of general text books that these pages are put together. The author's aim is, in fact, to enable anyone with no knowledge of natural science whatever to appreciate something of the chemical and physical principles which underlie the use of building materials. The first part of the book endeavours to explain the principles of chemistry, physics, and geology by drawing only on such parts of these sciences as are directly applicable to the production, use, and decay of materials, while in the second part, which comprises more than two- thirds of the volume, these principles are applied to the study of stones, brick clays, limes and cements, the metals, timber, and paints. In the space at disposal it has been impossible to do more than generalise, and to review such substances in classes, and all details of manufacture, statistics of pro- duction, and even tabulated data, have been suppressed as far as possible. Such matters are readily accessible in many excellent text books on individual subjects. The object kept in view has been rather to point out the PEEFACE vii composition, characteristics, general nature of tests applied to, and causes of failure in, materials, as giving a means of discriminating upon their employment and preservation, or as an introduction to further study. Short cuts to knowledge are always open to criticism; this book, however, makes no attempt to create scientists, but merely to inculcate an appreciation of the uses of science. In putting together these pages the writer has naturally contracted great obligations to many authors, among whose works he especially wishes to acknowledge : — Johnson's "Materials of Construction"; Eckel's "Cements, Limes and Plasters " ; Eies' " Clays : Their Occurrence, Properties and Uses " ; Harris' " The Science of Brick Making " ; Le Chatelier's " Constitution of Hydraulic Mortars " ; Michaelis' "Hardening Process of Hydraulic Cements";^ Hiorns' "Metallography"; Hurst's "Chemistry of Paints and Painting " ; Hall's " Chemistry of Paints and Paint Vehicles." He has also contracted obligations by reference to works by Professors and Messrs. Unwin, Blount and Bloxam, Sexton, Charpentier, Schnabel and Louis, Redgrave, Dibdin, Sabin, Davies, Bauerman, H. B. Woodward, Abney, Dent, and other writers, and to L'Association Internationale pour I'essai des Materiaux de Construction, The Quarry, The R.I.B.A. Journal, The Journal of the Society of Chemical Industry, The Journal of the Chemical Society, The Journal ^ For a copy of the American translation of Dr. Michaelis' paper, the writer is indebted to the kindness of Mr. Bower-Hopkinson, of the Associated Portland Cement Manufacturers, Ltd. viii PEEFAOE of the American Chemical Society, The Builders' Journal, Cement and Engineering News, Engineering News, and other publications, for information contained in these periodicals. If omissions in references and acknowledgment are found in the text, the writer hopes that they will be regarded as inadvertent errors, and he would like to conclude by an expression of thanks to the officials of the Patent Office Library for their courtesy and assistance on many occasions, and to add that in no place in this country is technical literature concerned with the subject of these pages so readily accessible as in this well-arranged institution. Alan E. Munby. 28 Martin's Lane, Cannon Street, E.G. January, 1909. CONTENTS PAET I ELEMENTARY SCIENCE CHAPTEE I PAGE NATURAL LAWS AND SCIENTIFIC INVESTIGATIONS ... 1 I. — Uses and Divisions of Science .... 1 1. Introductory. 2. Brandies of Science. II. — Natural Laws ^ III. — Methods of Investigation 4 1. Chemical and Physical Changes. 2. Heat produces Changes. 3. Moisture aids Change. 4. State of Division affects Changes. IV. — Simple and Complex Substances .... 7 1. Elements. 2. Combinations of Elements. 3. Characters of Compounds. 4. Complex Compounds. V. — Matter is Indestructible 9 CHAPTEE n ON MEASUREMENT AND THE PROPERTIES OF MATTER . . 11 I. — Standards H 1. Importance of Standards. 2. Fundamental Units. II. — The Metric System 12 III. — Derived Units 13 X CONTENTS Chapter II. — continued. PAGE IV. — Specific Gravity 14 1. Definition. 2. Determinations for Solids. 3. Determinations for Liquids. 4. Numerical Example. V. — Nature and Properties of Matter .... 18 1. Nature of Matter. 2. Solids. 3. Liquids. 4. Gases. CHAPTER III THE AIR AND COMBUSTION 22 I. — The Air : Physical Aspects 22 1. Material Nature. 2. The Barometer. 3. Boyle's Law. II. — Chemical Properties of Air 26 1. Composition of Air. 2. Preparation of Oxygen. III. — Minor Constituents of Air 28 1. Moisture. 2. Carbonic Acid Gas. IV. — Combustion 29 1. Combustion Defined. 2. Conditions for Com- bustion. 3. Instantaneous Combustion. 4. Practical Bearings. CHAPTER IV HEAT : ITS NATURE AND MEASUREMENT .... 33 I. — Nature of Heat 33 II. — Temperature 34 1. Meaning of the Term. 2. Measurement of Temperature. 3. Construction of a Ther- mometer. 4. Scales of Temperature. III. — Measurement of Heat Quantity .... 37 1. Unit of Heat. 2. Specific Heat. IV. — Change of State 39 1. Latent Heat. 2. Melting Points. 3. Change of Volume with Change of State. CONTENTS xi CHAPTEB V PAGE HEAT AND ITS EFFECTS ON MATEEIALS .... 43 I. — Expansion of Solids 43 1. Dimensions and Structure. 2. Linear Expan- sion of Solids. 3. Co-efi&cient of Linear Expansion. 4. Practical Importance. II. — Expansion of Liquids 47 1. Expansion of Water. 2. Circulation of Water. III. — Expansion of Gases 48 1. Charles' Law. 2. Ventilation. IV. — Transmission of Heat 49 1. Conduction. 2. Convection. 3. Radiation. CHAPTER VI CHEMICAL SIGNS AND CALCULATIONS 53 I. — Atomic Theory 53 II. — Atomic Weights and Symbols .... 54 1. Relative Weights of the Atoms. 2. Symbols. 3. Table of Symbols and Atomic Weights. III. — Combinations of Symbols or Formulse ... 55 IV. — The Assigning of Formulae 57 V. — Chemical Equations 59 1. Meaning of Equations. 2. Calculations. VI. — Chemical Nomenclature 61 1. Names indicate Composition. 2. List of Popular and Scientific Names. CHAPTER VII WATER AND ITS IMPURITIES 64 I. — Composition of Water 64 1. Decomposition by Metals. 2. Decomposition by Electricity. 3. Properties of Hydrogen. xii CONTENTS Chapter VII. — continued. PAGE II. — Solvent Power of Water 65 1. Solution of Solids. 2. Solution of Gases. III. — Water of Crystallisation 66 1. Meaning of the Term. 2. Efflorescence. 3. Deliquescence. IV. — Impurities in Natural Waters .... 68 1. Air and other Gases. 2. Mineral Matters. 3. Organic Impurities. 4. Suspended Matter. V. — Hardness of Water 70 1. Temporary Hardness. 2. Permanent Hardness. VI. — Effects of Water on Materials .... 72 1. Scale in Pipes. 2. Use of Lead. VII. — Analysis of Water 74 1. Total Solids. 2. Chlorine. 3. Hardness. 4. Ammonia and Nitrates. 5. Poisonous Metals. 6. Good and Bad Water. CHAPTER VIII SULPHUR AND THE NATURE OF ACIDS AND BASES . . 77 I. — Occurrence and Preparation of Sulphur . . 77 1. Occurrence. 2. Properties of Sulphur. II. — Sulphur Compounds 78 1. Sulphides of Iron. 2. Sulphuric Acid. 3. Sulphuretted Hydrogen. III. — Other Common Mineral Acids .... 81 1. Spirits of Salt. 2. Aqua fortis. IV. — Acids, Bases, and Salts 82 1. Acids. 2. Bases. 3. Salts. 4. Acid-forming Oxides. CHAPTER IX COAL AND ITS PRODUCTS 86 I.— Coal 86 1. Introductory, 2. Varieties of Coal. 3. Com- position of Coal. 4. Uses. CONTENTS xiii Chapter IX. — continued, PAGE II. — Distillation of Coal 88 1. Coal Gas. 2. Coal Tar. 3. Coke. III. — Carbon and its Oxides 90 1. Charcoal. 2. Lamp Black. 3. Graphite. 4. Carbon Dioxide. 5. Carbon Monoxide. CHAPTEE X OUTLINES OF GEOLOGY 93 I.— Earth History 93 1. Introductory. 2. Erosion. 3. Deposition. II. — Arrangement of Strata 96 1. Layers not continuous. 2. Dip. 3. Faults. III. — Identification of Strata 99 1. Characters. 2. Names and Order of Strata. IV. — Eocks not formed under Water .... 101 V. — Conclusion 104 PAET II BUILDING MATERIALS INTEODUCTION 105 CHAPTER XI THE CONSTITUENTS OF STONES, CLAYS, AND CEMENTING MATERIALS 107 I.— Mineral Constituents and their Characters . . 107 1. Composition of Natural Materials. 2. Minerals Defined. 3. Characters of Minerals. II. — Use of the Microscope in Examining Materials . Ill 1. Principles of Construction. 2. Use of Polarised Light. xiv CONTENTS Chapter XI. — continued. PAGE III. — Individual Minerals connected with Materials . 112 1. Silica. 2. Calcium Carbonate. 3. Calcium Sulphate. 4. Alumina. 5. Magnesium Car- bonate. 6. Potash and Soda Compounds. 7. Compounds of Iron. IV. — Silicate Minerals 115 1. Constitution of Silicates. 2. Felspars. 3. Micas. 4. Hornblende and Augite. 6. Chlorite. 6. Serpentine. V. — Table of Common Minerals 119-120 CHAPTER XII CLASSIFICATION OF STONES 121 I. — Introductory 121 II. — Igneous Stones 122 1. Granites. 2. Elvans. 3. Syenites. 4. Other Igneous Stones. 6. Objectionable Minerals. III. — Sedimentary Stones 125 1. Limestones. 2. Sandstones. 3. Objectionable Minerals. 4. Weathering. IV. — Metamorphic Stones 129 1. Definition. 2. Marbles. 3. Slates. CHAPTER XIII THE EXAMINATION AND TESTING OF STONES . . . 134 I. — Introductory I34 II. — Individual Tests I35 1. Specific Gravity. 2. Porosity. 3. Elasticity. 4. Adherence. 5. Expansion. 6. Conduc- tivity. 7. Hardness. 8. Crushing Stress. 9. Microscopic Tests. 10. Chemical Analysis. 11. Solubility. 12. Characters m situ. CONTENTS XV CHAPTER XIV PAGE BRICK AND OTHER CLAYS 147 I. — Geological Formation 147 II.— Varieties of Clay 148 1. Residual Clays. 2. Transported Clays. 3. Varieties of Transported Clays. III. — Physical Properties of Clay 149 IV. — Mineral Composition of Clay 150 1. Kaolin. 2. Felspars. 3. Mica. 4. Quartz. 5. Iron Pyrites. 6. Iron Oxides. 7. Calcite. 8. Selenite. 9. Dolomite. 10. Carbonaceous Matter. v.— Drying of Clays 153 VI.— Fusibility of Clays 154 1. Combinations causing Fusion. 2. Mixtures of Fluxes. 3. Molecular Proportion and Fusion. 4. Stages of Fusion. CHAPTER XV CLAYS (continued), kiln reactions and the propbetibs OF BURNT CLAYS 158 I. — Kiln and Subsequent Behaviour of Minerals . 168 1. Compounds of Ammonia. 2. Water. 3. Car- bonaceous Matter. 4. Magnesium Carbonate. 5. Magnesium Sulphate. 6. Calcium Car- bonate. 7. Calcium Sulphate. 8. Ferrous Oxide and its Compounds. 9. Ferric Oxide. 10. Iron Pyrites. 11. Potash and Soda. 12. Summary of Temperature Changes. II. — Removal of Defects in Clays 166 III. — Examination and Tests 167 xvi CONTENTS CHAPTEE XVI PAGE PLASTERS AND LIMES 168 I. — Binding Materials Classified 168 II.— Plasters 169 1. Plaster of Paris. 2. Flooring Plasters. 3. Keene's and similar Cements. III. — Non-Hydraulic Limes 171 1. Fat Limes. 2. Lean Limes. 3. Dolomitic Limes. 4. Strength of Lime Mortars. IV. — Hydraulic Limes 174 1. Characters. 2. Feebly Hydraulic Limes. 3. Selenitic Limes. 4. Eminently Hydraulic Limes. 5. Grappiers. V. — Testing of Hydraulic Limes 178 1. Chemical Analysis. 2. Mechanical and other Tests. CHAPTEE XVII CEMENTS 182 I. — Eelations between Limes and Cements . . . 182 II. — Natural Cements 183 1. General Characters. 2. Varieties. 3. Strength. III. — Portland Cement Manufacture .... 185 1. Introductory. 2. Details of Manufacture. IV. — Portland Cement Tests 187 1. Introductory. 2. Fineness. 3. Specific Gravity. 4. Expansion. 5. Tensile Strength, 6. Chemical Composition. 7. Eate of Setting. 8. Microscopic. 9. Other Tests. 10. Actual Strength of Portland Cement. V. — Pozzuolana Cements 194 1. Natural Pozzuolanas. 2. Artificial Pozzuo- lanas. 3. Properties and Strength. CONTENTS xvii CHAPTER XVIII PAGE THEORIES UPON THE SETTING OF PLASTERS AND HYDRAULIC MATERIALS 197 I. — Cohesion and Adhesion 197 1. Cohesion. 2. Adhesion. 3. Effect of Aggregates. II. — Introductory Remarks on Setting .... 199 1. General Causes. 2. Crystalloid and CoUoid Theories. III. — Theories of Setting Developed .... 201 1. Crystalloid Theory. 2. Colloid Theory. 3. Effects of Magnesia and Ferra. 4. Sum- mary of Views held. IV. — Rate of Setting of Plasters and Cements , . 207 V. — Failure of Hydraulic Materials .... 209 1. Expansion. 2. Efflorescence and Solution. 3. Defects due to Sea-vs^ater. 4. Defects due to Aggregates. CHAPTER XIX ARTIFICIAL STONE ; OXYCHLORIDE CEMENT ; ASPHALTE . 213 I. — Artificial Stone 213 1. Ransome's Process. 2. Lime-sand Bricks. II. — Stone Preservation 215 III. — Oxychloride Cements 216 IV. — Bitumen and Asphalte 217 1. Bitumen. 2. Asphalte. CHAPTER XX THE METALS : THEIR GENERAL PROPERTIES AND OCCURRENCE 221 I. — Introductory 221 II. — Micro structure of the Metals 222 B.M. h xviii CONTENTS Chapter XX — continued. PAGE III. — Physical Properties of the Metals .... 225 1. Malleability. 2. Ductility. 3. Hardness. 4. Elasticity. 5. Fusibility. 6. Expan- sion, etc. IV. — Occurrence and Extraction of the Metals . . 228 1. Occurrence. 2. Metallurgy. CHAPTER XXI IRON AND STEEL 232 I. — Ores, Metallurgy and Definitions .... 232 1. Ores of Iron. 2. Metallurgy of Iron and Steel. 3. Definitions of Iron and Steel. 4. Con- dition of Carbon in Iron and Steel. II.— Cast Iron 237 1. Preparation. 2. Subsidiary Constituents. 3. Grades and Properties. 4. Conclusion. III. — Wrought Iron 241 1. Preparation. 2. Subsidiary Constituents. 3. Grades and Properties. IV. — Steel 244 1. Preparation. 2. Subsidiary Constituents. 3. Grades and Properties. V. — Corrosion of Iron and Steel 248 1. Oxidation. 2. Electrolytic Decay. 3. Com- parative Decay. CHAPTER XXII OTHER METALS AND ALLOYS 251 I.— Copper 251 1. Ores. 2. Extraction. 3. Properties. 4. Impurities. 5. Corrosion. II. — Lead .255 1. Ores. 2. Extraction. 3. Properties. 4. Impurities. 5. Corrosion. CONTENTS xix Chapter XXII — continued. PAttB Ill.-Zino 258 1. Ores. 2. Extraction. 3. Properties. 4. Impurities. 5. Corrosion. IV.-Tin 260 1, Ores. 2. Extraction. 3. Properties. 4. Impurities and Corrosion. V. — Aluminium 1. Ores. 2. Extraction. 3. Properties. 4. Impurities and Corrosion. VI.— Alloys 264 1. Introductory. 2. Brass. 3. Bronzes. 4. Lead- tin Alloys. 5. Fusible Alloys. CHAPTER XXIII TESTS UPON AND STRENGTH OF THE METALS . . • 270 I.— Nature of Tests applied to Metals ... 270 1. Introductory. 2. Tensile Tests. 3. Com- pressive Tests. 4. Cross-Bending Tests. 5. Cold-Bending Tests. 6. Hardness Tests. 7. Shear and Torsion Tests. 8. Impact Tests. II. — Actual Strength of Metals 278 1. Introductory. 2. Cast Iron. 3. Wrought Iron. 4. Mild Steel. 5. Conclusion. CHAPTER XXIV TIMBER 282 I.— General Characters and Structure .... 282 1. Introductory. 2. Classification. 3. Structure. II —Moisture and its Effects 287 1. Occurrence of Water in Wood. 2. Shrinkage. III. — Mechanical and Other Properties .... 290 1. Composition. 2. Specific Gravity. 3. Mecha- nical Properties. IV. — Decay of Wood 292 1. Wet Rot. 2. Dry Rot. 3. Decay due to Insects. CONTENTS Chapter XXIY— continued. v. — Preservation of Wood 1. Seasoning. 2. Impregnation. 3. Eendering Wood Uninflammable. CHAPTEE XXV PAINTS : GENERAL CHARACTERS. OILS, THINNERS, AND VARNISHES I. — General Characters 1. Introductory. 2. Composition of Paint. 3. Essential Qualities. 4. Adulteration, Fillers and Thinners. II.— The Oils 1. Varieties of Oil. 2. Linseed Oil. 3. Other Oils. 4. Tests for the Oils. III. — Thinners 1. Introductory. 2. Turpentine. 3. Turpentine Substitutes. IV. — Varnishes 1. Gen eral Characters. 2. The Eesins. 3. Varieties of Eesin. CHAPTEE XXVI PAINTS : THEIR SOLID INGREDIENTS— BASES, PIGMENTS, AND DRIERS I- — White Ingredients ....... 1. Introductory. 2. White Lead. 3. Zinc White. 4. Other White Ingredients. II. — Coloured Ingredients 1. Causes of Colour. 2. Use of Pigments. 3. Beds. 4. Vermilions. 5. Yellows. 6. Browns. 7. Blues. 8. Greens. 9. Blacks. 10. Special Pigments or Coatings. III. — Driers 1. Use of Driers. 2. Varieties. PAGE 296 300 300 304 309 311 315 315 321 332 INDEX 335 INTRODUCTION TO THE CHEMISTRY AND PHYSICS OF BUILDING MATERIALS PART I.— ELEMENTARY SCIENCE CHAPTBE I NATURAL LAWS AND SCIENTIFIC INVESTIGATION I. Uses and Divisions of Science. 1. Introductory. — A reproach often levelled against this country is the lack of co-ordination between the workers in pure and applied science. The man in the laboratory patiently labours to establish abstract principles, and his time is absorbed in researches which have for their object the elucidation of the laws of Nature. The user of Nature's materials, on the other hand, is chiefly concerned with the economic aspect of the vast range of products which comes under his consideration. The scientist often complains of the lack of interest displayed by the practical man in his laborious researches, while the latter pronounces the former an idealist who gives him none of the tangible things which concern his daily requirements. The fields of these two workers are so essentially different that it is impossible to expect com- plete sympathy between them, and thus it is that the B.M. B 2 OHEMISTEY AND PHYSICS OF BUILDING MATEEIALS mediator Technology has come into existence to carry the work of pure science into practical channels on the one hand, and on the other to bring home to the practical man the value, not only educative, but also financial, of a know- ledge of the properties of those things which concern his work : knowledge whereby he can alone expect to be able to grasp the trend of new developments, and thus find him- self ready to meet competition. Though the exigencies of present-day existence leave but little time for the cultivation of fields beyond the limits of the "daily round," an acquire- ment of some knowledge of the elementary principles of science is not difl&cult, and while "short cuts," as generally tending to superficiality, are to be deprecated, a modicum of scientific training on the part of the practical man is of the greatest value if properly used. Such training will not, and should not attempt, to make him a scientist, but will enable him to understand and appreciate the work of the scientist and to utilise and direct such work to his own material advantage. These pages are devoted to the application of science to building materials in connection with which the manu- facturer, the builder, and most of all the architect under- take great responsibilities which can only be conscientiously accepted with some knowledge of the principles which underlie the preparation, use and specification of such materials. 2. Branches of Science. — Science is the English rendering of the Latin word for " knowledge," and the term is there- fore correctly applied quite generally. The knowledge of the things of Nature — that is, the tangible things which compose the earth and its surroundings, and of the forces which control these bodies — is distinguished as Natural Science. This study offers so wide a field that it is necessary to divide natural science into many branches, to a limited number of which any individual can alone devote attention ; NATURAL LAWS AND SCIENTIFIC INYESTiaATION 3 but it should be observed that this is merely a matter of convenience attributable to the limitations of life and mental capacity, and not because there are any real breaks in the continuity of Nature. Among such branches may be mentioned — (a) Physics. — The study of the action of mechanical force upon substances, and the transient effects of heat, light and sound and of magnetic and electrical energy, are relegated to the branch of science known as Physics. (b) Chemistry. — The investigation of the ultimate compo- sition of bodies, most of which can be split up into simpler substances, and the way in which such bodies combine and act upon one another, form the branch of science known as Chemistry. (c) Geology. — The study of the earth's physical character beneath its surface, where materials are found to be arranged in layers or strata possessing distinguishable characteristics, is known as Geology. (d) Other Branches. — Thus the list may be continued — the study of minerals, known as Mineralogy ; of plant life. Botany ; of animal life, Biology. All, however, are parts of one great whole, and merge into one another as their study is advanced. It is with the first three of the above-mentioned branches of science that a knowledge of building products is chiefly concerned, and in the first part of this book it is proposed to record a few simple facts culled from such sources centred, as far as may be, round concrete examples bear- ing upon the actual materials to be discussed in the later chapters. II. Natueal Laws. All applied knowledge is based upon the assumption that under a given set of conditions certain definite things will recur. To know the conditions necessary to produce a B 2 4 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS particular result requires the collection, study and arrange- ment of a large number of facts and an investigation of the effect of each factor in producing the result attributable to them all. If the relations thus established between cause and effect are found to be of wide application, the generalisation arrived at is termed a Natural Law. Thus the statement that all chemical compounds have a definite and constant composition is not a mere speculative announcement suggesting a probable truth, but is the result of the analj'sis of countless bodies prepared in many different ways, and thus rests on experimental evidence. For example, water, chalk and zinc white are chemical com- pounds. A knowledge of the above law therefore enables the certain prediction to be made that whatever means are utilised for preparing these bodies, their chemical properties, such as their action upon other substances and tendency to change under given conditions, will always be the same. This knowledge obviously supplies a broad basis of fact which, as it is applicable to all chemical compounds, must be of the greatest service. III. Methods of Investigation. 1. Chemical and Physical Changes. — Natural knowledge is obtained by making trials or experiments. From infancy our surroundings have been investigated by experiments, sometimes disastrous, always salutary. So also to know materials experiments are essential ; indeed, only by them has natural science found an existence. The procedure need not be elaborate. An experiment is scientific and valuable if (a) the conditions under which it takes place are carefully noted ; (6) the results are properly recorded ; (c) the conclusions therefrom are drawn with discretion, which rapidly increases with experience. In making an experiment, if any happens at all, some NATUEAL LAWS AND SCIENTIFIC INVESTIGATION 5 change in the substance under investigation takes place, and it is this change which must be studied. The substance may change its shape, or colour, it may break up, or alter in many other ways ; but these changes may be divided into two main classes : (a) Those which only last as long as the cause of the change operates, as when a spring is bent and flies back to its original position when released ; (b) Those which are permanent, as when concrete sets owing to the rearrangement of its constituents. The former are called physical changes, and their investiga- tion belongs to the science Physics. The latter are called chemical changes, and their study is relegated to Chemistry. Upon these changes the whole question of the manufacture, stability, and decay of building materials depends. 2. Heat produces Changes. — One of the best agencies for producing changes in bodies, and thus of investigating their properties, is Heat. Heat results in the throwing of the little particles (or molecules, as they are called) of which all substances are composed, into such violent vibrations that they often lose their hold of one another, so that the substance splits up into simpler bodies which thus reveal its composition. If a few scraps of wood be heated in a thin glass tube, known to chemists as a test-tube, water is first evolved as steam, some of which settles down as dew on the cool upper part of the tube. Then yellow gases appear, and darker oily drops condense on the glass. These gases can be lighted, and burn with a bright flame. When no further gases are evolved the remains of the wood, still retaining its original shape, are found as charcoal. Wood, therefore, consists of at least three things, or possibly more, since some of these may themselves be capable of further subdivision. 3. Moisture aids Change. — Another frequent cause of change is to be found in the presence of moisture, of which 6 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS fact the comparative rate of decay of materials inside and outside a building gives ready evidence. A substance affected by moisture may simply dissolve or, as it is expressed, pass into solution, or it may enter into chemical combination with the water and thus become permanently altered. If a little powdered sugar be dissolved in water and the solution be allowed to evaporate by exposure to the air, the whole of the sugar will be left behind in its original condi- tion, though possibly if evaporation has been slow it may appear in larger regular fragments known as crystals. This is a case of simple solution. If a few zinc clippings or iron nails be placed in spirits of salt the metal will dissolve in the liquid, but in this case with brisk effervescence. On allowing the clear liquid to evaporate, which may be accelerated by heating it, no metal will reappear. The metal and part of the liquid have combined to form a new substance. This is an instance of chemical solution. The metal remains in the solid mass finally obtained, from which its extraction is possible, but only by some further chemical action. So important a factor is water in enabling substances to act, or, as the chemist would say, to react upon one another that it is almost true to say that no chemical change or process of decay takes place unless moisture is present. There are many substances which, while entirely without action one upon the other when in a dry state, readily enter into combination in the presence of water, and the more important instances of such changes will be subsequently considered. 4. State of Division. — Ordinary experience indicates that action takes place between bodies most readily when they are intimately mixed in a fine state of division. The fine- ness of various grades of cement as influencing setting and strength forms a striking instance of this fact. Chemical NATUEAL LAWS AND SCIENTIFIC INVESTIGATION 1 forces can only act across very minute distances, and many chemical actions can be accelerated and even induced by effective sub-division and intermixture of the component substances. IV. Simple and Complex Substances. 1. Elements. — In order to understand and guard against the various changes which result through the combinations and decay of materials, it is necessary to become acquainted not only with the history of the formation of the bodies in question, but also with their ultimate chemical composition and physical structure. Fortunately almost every known substance has been dissected or submitted to analysis by the chemist, and it is found that where complex bodies are broken up and the parts thus obtained repeatedly submitted to chemical dissection, a stage is at length reached at which no new and simpler substances are obtained. These final bodies, which have resisted all the devices at the command of science for the separation of substances into their com- ponent parts, are known as Elements. Many of the elements are well known ; included in this class, for example, are the common metals such as iron, lead and zinc ; sulphur, and the two mixed gases which mainly compose the air, are also elements. The total number of elementary bodies of which all known substances are composed is not very large ; some eighty of such bodies have been isolated, but more than half of them are never found in familiar substances, while hardly more than one quarter of them are ever found in building materials, which are therefore composed of only about twenty different things. 2. Combinations of Elements. — If the elements in materials were merely mixed together, an investigation of such materials would be a fairly simple matter. A little reflec- 8 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS tion, however, must make it evident that some more subtle combination than simple juxtaposition exists in most sub- stances of a complex nature. That white lead, for example, contains the metal lead is readily admitted ; the substance is heavy like lead and lead is easily extracted from it, as by painting therewith a red-hot pipe ; but no mechanical division of the material will reveal lead, no microscope will make it visible, the lead has none of its ordinary metallic properties. The metal is, in fact, interlocked or combined with the other elements, carbon, hydrogen, and oxygen present, in some intimate and yet hardly under- stood manner, which gives the substance a new and definite character very different from a mere mixture of the metal with the other elements cited. 3. Character of Compounds. — Substances containing elements thus combined are termed Chemical Compounds, and possess characteristics which entirely distinguish them from mere mixtures. These are (a) constancy of compo- sition, i.e., a given compound always consists of the same elements, and the amount of each present is definite and fixed ; (b) The properties and characteristics of a given compound are definite and distinctive and are always in many respects different from those of the elements which compose it ; (c) Some chemical change is always neces- sary for the production or decomposition of a compound ; (d) Heat is evolved when compounds are formed from simply bodies, though sometimes delicate instruments are necessary to detect this fact. As an example of these characters, quicklime is a compound of the metal calcium and the gas oxygen, and is always composed of five parts of metal to two parts of gas by weight. It is entirely unlike either the metal or the gas which comprise it. Its caustic nature, white colour, and other properties are always retained. It cannot be decomposed by any mere mechanical process. It combines f I NATURAL LAWS AND SCIENTIFIC INVESTIGATION 9 with water to form a more complex compound, and great heat is thereby evolved. 4. Complex Compounds and Mixtures of Compounds. — Compounds, as has just been shown, may themselves com- bine to form more complex substances which still possess the characteristics cited above. In spite of this, however, the number of elements present in any compound is usually quite small. It is seldom that more than four or five elements are found in combination. The ordinary substances of every-day life are occasionally elements or simple compounds, but most usually they are mixtures of several compounds which can often be separated by mechanical means, or by suitable solution. Quartz, for example, can be picked out from crushed granite and sand removed from mortar by dissolving the remaining constituents in spirits of salt. V. Matter is Indestructible. The word " destruction," as used popularly, involves the negation of a most important principle which underlies every chemical investigation. Destruction is in reality the antithesis of creation, and it is no more possible to destroy than to create. The amount of material in the earth, for example, is a constant quantity, and none of it can be made non-existent. Apparent cases of destruction involve chemical rearrangement and the production of some in- visible or easily-overlooked substance which, mixing with the air, is lost to notice. A candle, for example, on burning away is converted into a colourless gas and water vapour, so that its constituents are not made non-existent. This truth may be realised by considering the following possible experiment. A very small piece of lighted candle is placed in a large glass globe and the vessel sealed up. If the globe (which contains the necessary air) is sufficiently 10 CHEMISTKY AND PHYSICS OF BUILDING MATEEIALS large, the candle will completely disappear, but nothing has been lost, which might have been proved by weighing the sealed globe at the beginning and at the end of the experiment. In this case the products of combustion of the candle have b^en prevented from escaping. No destruction of material has resulted, but mere chemical rearrangement. This great truth, known as the Law of the Indestructibility or Conservation of Matter, was discovered at the end of the eighteenth century by the French chemist Lavoisier, aided by the work of the English scientists Priestley and Cavendish. CHAPTEK II ON MEASUREMENT AND THE PROPERTIES OF MATTER I. Standards. 1. Importance of Standards. — As organisation and exacti- tude in any subject gain ground they proceed along the science of measurement, facilities for which are indeed an index to state of civilisation. The interchange of com- modities of all kinds involves measurement, and the more intricate and valuable such commodities become the more accurate and perfectly defined must such measurements be. The first essential in any form of measurement is an unalterable standard which shall be generally accepted. This standard must be defined in every particular in which variations are likely to occur for the special class of thing to which it refers. In certain cases the standard is a material tangible thing, such as a pound weight ; in others it is neces- sary to define it by reference to motion or energy, as in the case of time or electric power. Standards are usually purely arbitrary, that is, they are anything agreed upon at will, and owing to the necessity for standards before the days of scientific method, many of them are ill-chosen. Moreover, through the difficulties in past times of intercommunica- tion several standards for the same thing are recognised in different countries, and even in different parts of the same country. Some of these will readily suggest them- selves, such as the kilogram and pound, which latter may be the pound avoirdupois or the pound troy, while such a standard as the bushel not only varies with the produce to 12 CHEMISTRY AND PHYSICS OF BUILDING MATEEIALS which it is appUed, but even for the same produce in different counties. The power of custom and the great but temporary incon- venience involved in changes of standards is responsible for the retention of many cumbrous methods of measurement which involve enormous waste of labour, but the aim of all thinking people should be the acquisition of one universal set of standards which would be accepted by all civilised nations alike. 2. Fundamental Units. — There are three fundamental units or standards from which all others are derived. These are the units of Length, Weight (properly called Mass) and Time. In this country the standard of length is a certain distance known as one yard (a standard yard is to be seen affixed to the north wall of Trafalgar Square). For mass a certain weight of metal called one pound. For time, which obviously cannot be materialised, the standard is the interval which elapses when the earth rotates through a certain angle, which is called one second. II. The Meteio System. In most European countries and universally in all scientific work what is known as the metric system of units is adopted. In this system the unit of length is one metre, which is equal to 39*37 English inches. For mass, one kilogram, equal to 2*20 EngHsh pounds. For time, the second, which is the same in value as our own. Association with this last fact makes it difficult to realise the inconvenience which would be involved did the second possess different values in different places, or, conversely, the immense gain which would be derived were the other two units respectively universal. The advantages of the metric system lie in the facts : (a) that it is a decimal system — that is, the multiples of the ON MEASUEEMENT AND PEOPERTIES OF MATTEE 13 units are always in tens, hundreds, or thousands, and parts of the units in tenths, hundredths, or thousandths, hence all the usual labour of multiplication and division is dispensed with ; (b) One set of units is applied to all kinds of produce and materials — thus the manifold tables of weights and measures in our own system are non-existent ; (c) There is a simple connection between many of the units employed which much reduces calculation. A dis- advantage of this system is that the number ten is only divisible by two once, hence the halving of numbers involves the use of parts of whole numbers, and therefore of more figures in many simple cases than does the British system. The adoption of the metric system, however, does not preclude the use of simple fractions. Metric Tables and Equivalents. — For most purposes the only necessary parts of metric tables of length and weight are the following : — Length Table. 10 millimetres (mm.) = 1 centimetre (cm.). 100 centimetres (cm.) = 1 metre (m.). 1,000 metres (m.) = 1 kilometre (kilom.). Weight Table. 1,000 milligrams (mg.) = 1 gram (gm.). 1,000 grams (gm.) = 1 kilogram (kilog.). As an indication of the value of these units in British measures the following may be cited : — 1 inch = 2'54 cm., hence 1 mm. = about of an inch ; 1 metre = 39*37 inches ; 1 kilometre = about f of a mile ; 1 oz. = 28'36 grams, 1 kilogram = 2*20 lbs. III. Derived Units. Units formed from the fundamental trio cited above are known as derived units. That for area, for example, is 14 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS derived from the unit of length, being a length multiplied by another length. Similarly the unit of volume is formed by multiplying the unit of area by another length. The square yard and the cubic yard are thus the rational British units, and the square and cubic metres the metric units of area and volume. The British system, however, possesses special and quite unnecessary units of area and volume, such as the rod and the gallon, which bear no simple relation to the fundamental units. The unit of volume in the metric system is, as stated, the cubic metre, but since this is somewhat large, one thousandth part of it, namely, a cube 10 centimetres each way, forms a more useful starting point. This volume is called a liti-e and is equal to 1*76 pints. A litre of water weighs one kilogram. The metric units of weight are, in fact, based upon the weight of unit volume of pure water. Hence the calculation of the weight of water in vessels is directly obtainable from their capacity in this system of measurement. For example, the weight of the contents of a cistern of water 1 square metre on the base and half a metre deep, and therefore possessing a volume of half a cubic metre, is 500 kilograms (about ^ a ton). This is one of the many instances of the simplicity of the metric system. To find the weight of water in a cistern when measured in feet requires a calculation on paper. The use of the metric system is extending, and its uni- versal adoption is only a matter of time, hence an acquaint- ance with it is highly desirable. IV. Specific Gkavity. 1. Definition. — A derivation from the fundamental units of great importance in connection with many materials, is Specific Gravity. Popularly this expression is equivalent to the term " heaviness" ; thus lead would be said to have a greater specific gravity, or to be heavier, than wood. This, ON MEASUEEMENT AND PEOPERTIES OF MATTEE 15 however, implies something in reference to heaviness which is not stated, for were an endeavour made to disprove such a statement by demonstrating that a cubic inch of lead weighed less than a cubic foot of wood, the immediate objection would be raised that the pieces of material com- pared were not of the same size. In this matter of size or volume lies the whole definition of specific gravity. One piece of lead can be heavier than another piece of smaller size, but two pieces of identical material cannot have different specific gravities, and it is in the former restricted sense only that the term " heaviness " should be used. Specific gravity expresses, then, the relation between weight and volume, and the most correct popular term equivalent to it is " bulkiness." This relation may be stated thus : — Specific gravity = It is a matter of indifference which system of units be adopted for measurement of the weight and volume, pro- vided the same system be retained throughout any series of comparisons. Thus if the ounce be taken as the unit of weight and the cubic inch as the unit of volume, the numbers expressing the weights in ounces of one cubic inch of different materials will be the relative specific gravities of such materials. For such a comparison it is not necessary to provide actual cubic inches of the sub- stances ; any convenient volume may obviously be employed, the piece weighed and the weight of one cubic inch found therefrom by simple proportion. Water the Standard. — In all comparisons of solid and liquid substances water is taken as the standard or unit ; that is to say, the specific gravity of water is called 1. Thus the statement that the specific gravity of lead is 11 means ^ Strictly mass, though this fact need not be considered in calculations. 16 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS that any given volume or bulk of lead is eleven times as heavy as the same volume of water. 2. Determinations for Solids, — Although very accurate determinations of specific gravity require numerous con- siderations, the approximate values usually necessary in dealing with building materials can be ascertained by anyone with but little apparatus. The specimens examined should not be too small, since the smaller the weight and volume the greater in proportion will be any errors in the determination. The weight in all cases is found by the ordinary process of weighing on a delicate pair of scales. If the material is a solid of regular shape its volume may be obtained by cubing it up with a rule ; if it is an irregular fragment or a powder this is determined by immersing the weighed quantity in some liquid ^ standing at a given height in a measuring vessel marked, say, in cubic inches or cubic centimetres, and noting to what higher division the liquid is raised thereby, when the rise or displacement of the liquid must evidently be the same as the volume of the specimen. If the material floats it may be depressed beneath the liquid by two or three fine stiff wires, the additional displacement due to these being neglected. The liquid usually employed is water, but in the case of limes and cements oil is utilised, as combination would take place with water in such cases. If a porous material is under examination and its specific gravity with the pores full of air is required, as would generally be the case, it may be coated with a thin film of varnish before immersion. 3. Determinations for Liquids. — Liquids, since they assume the shape of any vessel in which they are placed, lend themselves very readily to specific gravity determinations. In this case it is merely necessary to counterpoise a measur- ing vessel on a pair of scales with sand or other convenient ^ The liquid must not, of course, dissolve or act upon the solid. ON MEASUREMENT AND PROPEETIES OE MATTER 17 material, and to compare the weights of water and the liquid when the vessel is filled to a given mark. The specific gravity of liquids, however, is determined in practice by a hydrometer. This is a glass tube weighted at the bottom so that it floats vertically in the liquid. It contains a graduated scale whereby the depth to which it sinks can be noted. This depth will be less in a heavy than in a Hght liquid, and will in fact be proportional to the liquid's specific gravity. For convenience in reading the scale and to avoid decimal places the height at which the tube floats when in water is marked 1,000 instead of 1, and other numbers give the specific gravities of other liquids directly. Thus if in a certain oil the reading on the scale is 935, the specific gravity of this liquid is 0-935. 4. Numerical Example. — Suppose it is required to deter- mine the specific gravity of a 6-inch cube of stone. The volume, in this case determined by direct measurement, is 6x6x6= 216 cubic inches. The weight of the block proves to be, say, 324 ounces, hence one cubic inch weighs 324 == li ounces. Now one cubic inch of water weighs roughly J ounce ; hence, volume for volume, the stone is three times as heavy — that is, its specific gravity is 3. The above reckoning, however, is too rough for the result to be of value. One cubic inch of water weighs more nearly 0-6'^ ounce, but in all cases the procedure is the same : the weight of a cubic inch of the substances is divided by the weight of a cubic inch of water and the result is the specific 1'5 gravity. Thus in this case — = 2*5 = the specific gravity of the stone. If metric measures are used the calculation is even simpler. In this case the volume of the specimen is ^ 0*6 is not exact, but the object of this example is merely to show the method of calculation. B.M. 0 18 CHEMISTKY AND PHYSICS OF BtJILDINa MATEEIALS measured in cubic centimetres and its weight ascertained in grams. Then, as before, by dividing the weight of the specimen by its volume, the weight of one cubic centimetre is deduced. Now, one cubic centimetre of water weighs by definition exactly one gram, hence the specific gravity of the stone is obtained by dividing the weight of one cubic centi- metre of it by 1 ; in other words, this weight of unit volume of the stone is its specific gravity. Thus a piece of pine 20 X 35 X 2 cms. weighs 700 grams, 20 X 35 X 2 = 1,400 c. cms. = 0-5, the specific gravity required. V. Nature and Properties of Matter. 1. Nature of Matter. — By the term " matter " is under- stood any ponderable substance, which may be solid, Hquid or gaseous. All matter is characterised by the possession of weight and requires force to set it in motion, and all matter occupies space. Thus air is matter, whereas light is not material. A vessel full of air weighs more than the same vessel exhausted, but not more in light than in the dark. Again, to move air requires force, but to move a heliostat reflecting a beam of light requires no more effort than would be necessary in the dark. Matter is not absolutely continuous, but is built up of very minute particles, called " molecules," which have spaces between them even in the case of the most compact solids. That these molecules are very small is evident from the thinness to which many substances may be brought, and which must be necessarily at least one molecule thick if they are to hold together. "Water in the film of a soap bubble, and gold leaf, the latter easily obtained goCcJoo ^^'^^ in thickness, suggest themselves. Molecules are usually complex bodies consisting of two or more similar or dissimilar particles known as atoms. ON MEASUEEMENT AND PROPERTIES OF MATTER 19 Physical changes usually involve displacement of the molecules as such, but in chemical changes the molecules are broken up individually, which results in the interchange of their constituent atoms. That spaces between molecules do exist in matter is indicated by the fact that many substances which possess no apparent porosity can be compressed. Milled lead, for example, has a higher specific gravity than cast lead. Conversely, when a body is stretched it appears to be the interspaces and not the molecules themselves which are enlarged. The pull of one molecule upon another, which accounts for the power of retention of shape in solid bodies, explains the tendency to return to the original form possessed in greater or less degree by solids under deforming forces. It has been said that matter can exist in the solid, liquid or gaseous state. The characteristics of these conditions will now be touched upon. 2. Solids. — All solids possess size and shape ; that is to say, a given amount of any solid occupies a definite space while its internal constitution is such that it retains its shape without support from outside agencies. This retention of shape is dependent upon what is called rigidity, a property possessed in varying degree by all solids in virtue of which they resist forces tending to displace their molecules. The resistance called out by any such deforming force is called a stress. The amount of deformation produced measures what is known as the strain. A body which offers great resistance to deformation, that is, one in which great internal stress is called out by a given strain, is said to possess high elasticity. Elasticity may, then, be defined as stress divided by strain. This definition differs somewhat from the popular idea of elasticness. It is not the amount which a body can stretch and yet recover which is the true measure of this property, but to what extent it can withstand efforts G 2 20 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS at deformation. Glass and steel, for example, are highly elastic bodies, though not possessed of the india-rubber- like nature which is the essence of the popular conception of this property. Bodies which show a marked absence of elasticity are termed plastic. Wet clay and lead are examples of such bodies which possess very small power of recovery under forces acting upon them. Other distinctive properties possessed in a greater or lesser degree by solids are malleahility, the property in virtue of which they may be beaten into sheets ; ductility, or powers of attenuation, as wire ; hardness, which may refer to power to resist either abrasion or indentation. Much standardisation yet remains to be done in connection with many of these properties. 3. Liquids.— Though liquids, like solids, possess definite size they have no shape, and this involves some funda- mental distinctions. This lack of shape is due to an entire absence of rigidity in liquids, and from this limpness it follows that the slightest inequality of pressure upon a liquid is able to cause movement. If two vessels contain- ing the same liquid be connected the level in each will become the same whatever the form or distance of the con- necting pipe— a fact well recognised where actual pipes are concerned, but often overlooked when water areas separated by porous soils are in question. Liquids are practically incompressible, and transmit any pressure put upon them equally in all directions, which renders them very valuable as media for pressure trans- mission in all forms of hydraulic machinery. Any force, however small, will change the shape of a liquid; for example, a stone dropped into a pond moves the whole of the water therein. The rate of this change, however, varies with different liquids. Those in which change of shape proceeds slowly are termed viscous, while limpid liquids are termed mobile. ON MEASUREMENT AND PEOPERTIES OF MATTER 21 4. Gases. — The term gas includes not only bodies popu- larly so described as coal gas and carbonic acid gas, but all matter which is neither solid nor liquid. The most important gas is thus ordinary air. Gases have much in common with liquids, and the two are indeed classed together as fluids. Gases possess, however, two important distinc- tions : they have not only no shape but no size, and they are very easily compressed. Lack of size may be realised by considering the effect of admitting, say, a cubic foot of air into a vacuous room, The air admitted would immediately expand and fill the whole room in a very attenuated form. The space occupied by a gas is thus entirely dependent upon the limits set upon it. Gases possess the simplest constitution of any of the forms of matter. While solids and liquids differ much among themselves, the physical properties of all gases are remarkably similar. Some of the laws relating to gases will be dealt with in succeeding chapters. CHAPTEK III THE AIR AND COMBUSTION I. The Air. 1. Material Nature. — Physical Aspects. — Air though invisible is material, it possesses weight, and no little energy- must be expended in pushing it on one side in moving through it. The actual weight of air may be ascertained by counterpoising an exhausted vessel on a delicate pair of scales, and then admitting air, when the vessel will require to be balanced by weights which will be equal to the weight of air then contained in it. All gases vary in volume so largely with variations in temperature and pressure that it is essential to observe and state the conditions in these particulars in dealing with the weight of gases. Under ordinary circumstances, however, a cubic foot of air weighs about 1 J ozs. The air in a building may, therefore, weigh many tons and thus exert considerable pressure. When still, this pressure, since it acts in all directions, may be neglected, but when air is in motion unbalanced pressures are pro- duced, which are often of considerable magnitude. 2. The Barometer. — If one end of a pipe be dipped below the surface of a liquid, and suction be applied to the other end, the liquid rises in the pipe. The height to which a liquid can thus be drawn is limited, however great the suction power applied, and is found to depend upon the specific gravity of the liquid. The heavier the liquid the shorter will be the column raised ; in fact, the weight of THE AIR AND COMBUSTION 23 columns of different liquids drawn up in a given tube will be in all cases the same. The liquid rises in the pipe owing to the withdrawal of air, which leaves an unbalanced pressure due to the air outside ; and it is the weight of this external air upon the exposed surface in the vessel which forces the liquid up the pipe. All cases of so-called " suction " are in reality cases of unbalanced air pressure. A convenient means is in this way provided for measur- ing air pressure, since when the column of liquid in the pipe is sufficiently long to balance the full weight of the air it will on further suction rise no higher. It is found that water can be raised in a pipe by suction some 33 feet in height above the level of that in which the pipe is standing, and this gives the extreme limit (never quite attained in practice) to which water can be raised by lift pumps or other suction appliances, such as syphons. The liquid mercury (quicksilver), which is 13 J times 33 as heavy as water, reaches its limit of height at feet or about 30 inches, and as such shorter column is more convenient than a column of water, a tube thus filled with mercury is used for measuring air pressure which is not quite constant but undergoes small though important variations. The tube need not, of course, be filled by suction. If sealed at one end the mercury may be poured into it, and it may then be temporarily closed and inverted in a dish of mercury, beneath the surface of which its open end is retained. Such a tube of glass some 33 inches long, either standing in mercury as described or with its open end bent round so as to present a surface upon which the air can press, is known as a barometer. Variations in the height of the mercury in a barometer are due to several causes. The higher the situation above 24 CHEMISTET AND PHYSICS OF BUILDING MATEEIALS the earth's surface the less is the depth of the ocean of air above, and hence the less the air pressure. Thus the height of the barometer decreases with increased altitude, falling about 1 inch for every 900 feet ascended for moderate heights. Heights, even those of lofty buildings, may be measured with considerable accuracy from barometer readings. Winds, by accumulating or dispersing air, cause local variations of pressure, and moisture by expelling air usually causes a reduction of pressure and hence a fall in the barometer. It has been stated that any force, however small, is sufficient to move a liquid, hence the barometer forms a very delicate instrument, and indicates changes of pressure long before these are evident to the senses. 3. Boyle's Law. — It has been stated that gases show much more similarity among themselves in their physical properties than do liquids or solids. All gases, for example, expand and contract to the same extent under the influence of heat and pressure. Since the volume of a given quantity of gas is dependent on the temperature and pressure to which it is subjected, any change in volume must involve a change in specific gravity. The relations between temperature pressure and volume are important, because the motion of gases in warmed rooms, chimneys, and flues, and their flow under pressure, are the result of variations in these factors. It is here proposed to investigate the relations between the pressure upon a gas and the volume it occupies. Changes in temperature will be considered in a subsequent chapter. If the tube shown in Fig. 1a be filled with mercury sufficiently to seal up the air contained in the shorter closed limb and the mercury be made to stand at the same height on each side of the bend, the enclosed air will THE AIE AND C0MBUSTI(3N 26 be under the same pressure as that of the air outside, which would otherwise push the mercury up the tube or allow the enclosed air to push it down. Let a mark be made on the closed limb where the mercury level stands and the length of the enclosed air column be measured. This enclosed air is supporting the atmospheric pressure, to be actually ascertained by reading off the height of the Volumes 0 _ Fig 1. — Eelation between the Volume of a gas and the Pressure sustained by it. barometer. Suppose this to be 30 inches. Now let mercury be poured into the open end of the tube until the difference in level between the open and the closed side is 30 inches, as shown in Fig. 1b. The enclosed air is now under twice the original pressure, namely, one 30-inch column equal to the weight of the atmosphere and another actually carried in the shape of the mercury added. It will be found that the mercury has risen halfway up the closed limb, in other words, that the volume of the air (the tube 26 CHEMISTRY AND PHYSICS OF BUILDINQ MATERIALS supposed to be of regular bore) has been halved. Thus by doubling the pressure the volume is halved, and had the tube been long enough, by adding another 30 inches of mercury and thus trebling the pressure the volume would have decreased to one-third, and so on in proportion. The result may be expressed generally by the statement that the volume varies inversely as the pressure, and this is found to be true for all gases. This fact, which lies at the root of all gaseous calculations, is known, after the name of its discoverer, as Boyle's Law, and may be stated thus : The volume of a given quantity of any gas varies inversely * as the pressure upon it. II. Chemical Properties of the Air. 1. Composition of Air. — If air be enclosed in an inverted glass vessel standing in water and some clean iron wire be pushed under the water into the vessel, the rusting of this wire, which will readily take place, will be found to be accompanied by a diminution in the volume of the enclosed air, and this decrease will continue (perhaps over a long period) until one-fifth of the air has disappeared, as evidenced by the rise of the water in the vessel. No further diminution will then take place. On taking out the wires they will be found, though much rusted, by no means entirely corroded away.^ ' The expression " varies inversely as " is a useful one for convey- ing any such relationship as the above. If one thing gets bigger in the same proportion as another gets bigger, the one is said to vary "as" or "directly as" the other. If one thing gets bigger in the same proportion as that in which another gets smaller, the one is said to vary "inversely as " the other. ^ To perform this experiment successfully, a narrow, graduated glass cylinder should be used to contain the air. The level of the water should be the same inside and outside the cylinder to begin with when the volume of the enclosed air is noted, and again after- wards (secured by pouring water into the open vessel in which the cylinder stands). The temperature should also be as nearly as possible the same at the beginning and end of the experiment. THE AIR AND COMBUSTION 27 Some important deductions may be made from this experiment. The presence of unrusted iron on removal shows that the absorption of the air by the iron did not cease owing to the want of material on which to act. It must, therefore, have ceased because the active principle in the air which is responsible for rusting had completely expended itself. Air must, then, consist of two different gases in the proportion of 1 to 4 by volume, ^ of the whole an active gas, | an inert gas. The active gas, which combines with the metals to form rust, is called oxygen, the inert gas is called nitrogen. The experiment does not show whether these gases are chemically combined or merely mixed together, or whether more than two different kinds of gas exist in the air. Although air contains small quantities of other gases it is, however, substantially composed of oxygen and nitrogen, and further experiments have shown that these gases are merely mixed together in the atmosphere. 2. Preparation and Properties of Oxygen. — A further proof that oxygen is the active constituent of the air may be made by extracting this gas from the air and observing its properties when alone, or more readily by utilising other sources for its preparation, such as red lead, nitre, or chlorate of potash, compounds which all contain oxygen obtainable in a free gaseous state by the action of heat on these bodies. In pure oxygen rusting and decay take place with increased activity, while substances which merely smoulder in air burn in oxygen with great brilliancy. The chemical activity of oxygen, however, is dependent, as are nearly all chemical actions, upon the presence of a small quantity of moisture. Air or oxygen, if absolutely dry — a condition never attained without special chemical precautions — have no action whatever on ordinary substances. If, for example, some pieces of quicklime, which absorb moisture, are allowed 28 CHEMISTEY AND PHYSICS OF BUILDINO MATEEIALS to stand in a well- stoppered bottle into which some bright iron nails are subsequently introduced, the iron will be found to retain its lustre indefinitely. That rusting is not due solely to water, but to both air and moisture together, may be proved by placing some pieces of bright iron in a stoppered bottle filled with water from which all dissolved air has been expelled by boiling briskly for some minutes. When oxygen combines with other bodies, whether actual rusting or other chemical change takes place, the process is known as oxidation, and the combination of any element with oxygen is known as an oxide. III. Minor Constituents of the Air. All air contains, in addition to oxygen and nitrogen, small quantities of moisture and carbonic acid gas, and often floating organic matter and mineral acid vapours. 1. Moistxire. — Water vapour in air is essential for respiration. The amount present in the atmosphere depends upon geographical and meteorological conditions and upon temperature. At summer temperatures air can carry about per cent, of its weight of water, but at the freezing point J per cent, is sufficient to cause saturation ; hence if warm air laden with moisture come in contact with a cold body water is deposited. The deposition of dew upon cold surfaces, such as pipes conveying cold water and upon windows of inhabited rooms, is attributable to this cause. In the latter case such deposition is much aggravated by inefficient ventilation, since respired air and the combustion products from illuminants contain large quantities of moisture. Although the amount of moisture present in air is very variable, it is seldom that actual saturation is reached under normal conditions, and on the other hand, even the driest winds contain more than one-tenth of the amount of water necessary to produce saturation. THE AIE AND COMBUSTION 29 2. Carbonic Acid Gas and Organic Matter. — This gas, more modernly called carbon dioxide, is produced by com- bustion or decay in air of all animal and vegetable sub- stances, and is also found in respired air as a waste product from the process of food assimilation. In fact, whenever carbon or any of its compounds undergo free oxidation carbon dioxide is formed. Fresh air contains some four volumes of this gas in 10,000 volumes of air, but in inhabited buildings less than six volumes in this bulk of air are seldom possible, and in badly-ventilated rooms ten, or even twenty, volumes have often been recorded. The gas itself is not injurious in quantities even much larger than that last cited, but when it results from respiration its amount becomes a measure of floating organic matter, always evolved during breathing, which taints the air and is injurious to health. The estimation of this organic matter directly is not easy, while the means for finding the amount of carbon dioxide which is pro- portional thereto is comparatively simple ; hence such latter estimation is commonly made, and in such terms the purity of the air is expressed. Further reference to the action of carbon dioxide when dissolved in water, and to mineral acid vapours and the important part they play in connection with changes in materials, will be found in subsequent chapters. IV. Combustion. 1. Combustion Defined. — When oxidation, or other chemical action, takes place with such energy that the heat thereby evolved raises the substances concerned to incandescence, that is, produces light, the process is termed " combustion." Broadly speaking, the only differ- ence between the combustion of bodies in air and slow 30 CHEMISTEY AND PHYSICS OF BUILDING MATEEIAiS oxidation or decay is one of time. The same ultimate chemical changes and the same amount of heat are pro- duced, but in the latter case the production of heat is so gradual that no change of temperature may be observ- able. Occasionally slow oxidation will develop into active combustion owing to the heat generated, as when a hay- stack fires or oily cotton waste ignites " spontaneously." Again, from the remarks in Chapter I. it will be evident that bodies in a fine state of division will oxidise much more readily than the same substances in large pieces. Fires in flour mills and coal mines resulting from the heat generated by the rapid oxidation of fine particles of materials raised as dust are by no means unknown. Even iron may be prepared in such a minute state of division that it takes fire on exposure to the air. These facts are not without some bearing on the design of many buildings. 2. Conditions for Combustion. — In order that combustion may take place, three conditions must be satisfied. The first, an obvious one, is that there shall be something capable of burning, that is, a substance not already in an oxidised condition. The second, that air (or some other substance with which combination can occur) shall be present. The third, that these two substances shall be raised to a certain temperature, different for different bodies, at which combination can take place, which is known as the " kindling point." The proper way of regarding combustion, therefore, is not as a mere inflaming of some perishable material but as an act of chemical combination between two equally neces- sary bodies — the perishable substance and the air. A lighted match, for example, will be extinguished if plunged into a vessel full of coal gas, and the gas will only burn at the aperture exposed to the air. This necessity for air can be strikingly shown by leading an air supply into a vessel filled with coal gas, when the air will burn if lighted. The THE AIE AND COMBUSTION 31 union is, of course, the same as when gas is burnt in air : it is in both cases the two gases which burn together. The necessity for raising the substances to be burnt to a certain temperature before any action can take place between them may be readily demonstrated by placing a combustible substance in contact with a flame and withdrawing the heat from it by means of some heat-absorbing material. A piece of paper pressed against a flat-iron may be held in a gas fiame without damage, or if water be placed in a paper bag the bag may be heated over a naked flame until the water has entirely boiled away, provided that the strength and texture of the paper are suitable for retaining the water. 3. Instantaneous Combustion. — The rapidity with which a body burns and the nature of the products of combustion have an important bearing on the effects of such action upon surrounding materials. If the combustion is prac- tically instantaneous and gases are produced which have no immediate means of escape an explosion results. It follows that the more nearly the combustible body and the air are present in proportions necessary for chemical com- bination the more violent will be such explosion. The disruptive effects of an explosion are due to the sudden expansion of the air and gaseous products of the combustion resulting from the heat of the chemical action. 4. Practical Bearings of Foregoing Principles. — The pre- servation of buildings from fire can alone be considered intelligently in the light of the above principles, and safety may be assured if it can be arranged that under no circum- stances can the three conditions required for combustion be fulfilled at one time. Thus if combustible materials must be employed it is obviously necessary to so place them that in presence of air they will never be raised to their kindling points, or to exclude the presence (actual or possible) of air in the likely event of their becoming overheated. This latter alternative has not received the consideration it 32 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS deserves. If, for example, the windows and other aper- tures of a building were provided with closely-fitting iron shutters, these when closed would limit the possibilities of internal combustion to the supply of oxygen contained in the air enclosed within the structure. The use of solid wooden floors, and of hard wood in which the pores are filled with solid matter, for stairs and similar structures as safeguards against fire, is based upon the same principle. CHAPTEE IV HEAT ITS NATURE AND MEASUREMENT I. Nature of Heat. The power of causing chemical changes possessed by heat has already been referred to. In this and the succeeding chapter it is proposed to discuss the nature of heat, and more particularly the physical changes which it produces in materials. The means described in Chapter III. of recognising a material body, if applied to heat would show it to possess a non-material existence. A hot body is no heavier than the same body when cold, neither does increase in heat of a body add to the necessary force required to move it. The means whereby heat may be generated throw some light on its nature. If a rope attached to a falling weight be allowed to run through the hand, heat is readily pro- duced, and since the effect of the hand is to check the weight in its fall and thus deprive it of some of its energy, it seems reasonable to assume that some connection exists between the energy thus lost and the heat so generated. Careful experiments have shown that the whole of the energy possessed by a falling weight may be converted into heat, and the conclusion arrived at is that heat is itself a form of energy into which other forms of energy may be easily converted. It has already been pointed out that the molecules of which material bodies are composed are in a state of motion, and it has been shown that the effect of heat energy is to B.M. D 34 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS increase the vibratory (or gyratory) motion of these mole- cules so that they move more rapidly and through greater distances as more heat is imparted to them. Heat may thus be looked upon as a form of internal or molecular motion, and if sufficient heat is imparted the molecules may so far lose their relative positions as to break away from one another, which explains the liquefaction and vaporisation of bodies by heat. The term "cold" is merely a relative term implying " less heat." All bodies have some internal motion, and thus possess some heat. Ordinary ice, for example, is hot as compared with liquid air. No heat in a body would mean absolute molecular rest, and recent improvements in the means of producing intense cold have almost enabled such a condition to be reached. At very low temperatures not only the physical properties but also the chemical activity of bodies are materially altered, and in a state of molecular rest it is probable that no chemical combination would take place even between the most active substances. II. Temperature. 1. Meaning of the Term. — When a body from any cause gets hotter it is said to rise in temperature. Temperature is not heat. It bears the same relation to heat that the height of a weight bears to the energy or work obtainable by letting it fall. A very small weight may drop from a great height and yet not be able to give as much energy or perform as much work as a heavy weight falling through a moderate distance. Similarly, a small body may be at a very high temperature but possess less heat than a large body only moderately hot. Temperature may be called heat level, and the difference between this and heat (energy) should be carefully considered. HEAT— ITS NATUEE AND MEASUREMENT 35 2. Measurement of Temperature. — Bodies expand when heated, and in most cases the increase in bulk caused is directly proportional to the increase in temperature of the body. Expansion thus gives a useful means of measuring temperature. Liquids expand more than solids, hence when a liquid is heated its level will be raised in spite of the simultaneous expansion of the vessel containing it. If the liquid is con- fined in a narrow tube slight increases in temperature will readily make themselves apparent, and if the tube have a regular bore the increase in the height of the column of liquid will be proportional to the increase in its volume. By placing such a tube of liquid in contact with various bodies possessing known temperatures and marking the heights at which the liquid stands, to correspond to such temperatures, the tube may be used for determining the temperatures of other bodies. Such an instrument is known as a Thermometer. 3. Construction of a Thermometer. — The liquid employed in thermometers is preferably mercury, and the tube is of glass and has a bulb at its base in order to admit of the use of a sufficient bulk of liquid to render expansion readily visible. In making a thermometer the tube is highly heated until the contained mercury fills it, and it is then sealed up ; thus all air is expelled, and nothing exists above the level of the cooled liquid to impede its subsequent expansion when used. The instrument is then placed in melting ice, and a mark made upon the tube where the mercury then stands, after which it is placed in steam above boiling water, and the increased height of the mercury recorded by another mark. These marks register the freezing and boiling points of water, and are known as the fixed points. The length of the tube between these marks is then divided into a number of equal divisions known as "degrees," and these may be continued above and below D 2 36 CHEMISTEY AND PHYSICS OF BUILDINa MATERIALS the fixed points to enable a greater range of temperature to be recorded. 4. Scales of Temperature. — The simplest method of dividing up the space between the freezing and boiling points is to mark this off into one hundred equal divisions, and to number them from 0, as the lower point, to 100, as the higher point, continuing the numbers above 100 as desired, and marking those below 0 as minus 1, minus 2, etc., down to the bulb of the thermometer. This is the scale always used in scientific work and for general pur- poses in some places abroad, and is known as the Centigrade scale (C). The word "degree" is generally expressed by a small hollow circle placed at the right hand top corner of the number ; thus if the mercury stood at the division 23, as it might do on a hot summer's day, the temperature would be registered as 23° C. Unfortunately, owing to causes explained under the dis- cussion of standards in Chapter II., the numbers above assigned to the fixed points are not employed universally, and two other scales are in common use, though only one of them, that used popularly in this country, need be referred to. This, known as the Fahrenheit scale (F.), adopts the number 32 instead of 0 for the freezing point and 212 instead of 100 for the boiling point of water, and the space between the two is divided into equal parts, of which, how- ever, there will be 180 (viz., 212 — 32). Degrees on the Fahrenheit scale are therefore less — that is, represent a smaller rise of temperature — than those on the Centigrade scale. It is, however, a very simple matter to convert one set of readings into the other, just as metres might be con- verted into yards or vice versa ; and as technological books sometimes give temperatures in one scale and sometimes in the other, it is most necessary to be able to effect this conversion in order to make comparisons of various data. Since 180 degrees F. are equal to 100 degrees C, HEAT— ITS NATUEB AND MEASUREMENT 37 1 degree F. = or f of a degree C. Hence, a Fahrenheit temperature, or "reading" as it is termed, may be converted into a Centigrade reading by multiplying by f , provided 32, the difference in the numbering of the freezing point, is first subtracted to put this point on the same footing in each case. Conversely a Centigrade reading may be turned into Fahrenheit by multiplying the reading by f and then adding 32 to the result. This conversion is very easily remembered if it is borne in mind (1) that if the numerical result is to be larger (C. to F.) the fraction must be used with the 9 above, and vice versa; (2) that the 32 never takes part in the multiplication, i.e., it is subtracted before or added afterwards, as the case may be. A few examples worked out will give immediate facility in this simple change of unit, thus 100° C. = 100 X f = 180 + 32 = 212° F. III. Measurement of Heat Quantity. 1. Unit of Heat. — The amount of heat contained in a body is dependent upon (1) the weight, or, more properly, mass of the body in question ; (2) the temperature of the body ; (3) what the body is. The unit of heat therefore should be, and is, the amount of heat required to raise unit weight of some standard substance through unit rise in temperature. The standard substance universally accepted is water, and the unit of heat is the amount of heat required to raise through 1° C. 1 pound, or 1 gram, of water, according to whether the British or Metric system is adopted. It does not follow that this amount of heat is the same for all parts of the temperature scale, i.e., that the same heat, for example, is required to raise a pound of water from 0° C. to 1° C. as is required to raise it from 68° C. to 59° C, but it has been found that the amount is so very nearly the same that the above definition of the unit is quite accurate enough for ordinary purposes. 88 CHEMISTRY AND PHYSICS OF BUILDING MATEEIALS It follows from the above statements that to raise 2 lbs. of water 1°C. requires two units of heat, and that two units of heat will also raise 1 pound of water 2° C. To find the number of units of heat, therefore, necessary to raise any weight of water to any given temperature, the weight of the water must be multiplied by the rise in temperature. The unit of heat might of course be defined in reference to the Fahrenheit scale of temperature, namely, as the amount of heat required to raise 1 pound of water 1^ Fahrenheit. In engineering work it is often so defined, but the definition as given, employing the Centigrade scale, is always used in scientific work. When water, or any other substance, cools, heat is given out to the air or surrounding bodies, and it would be equally correct to define the unit as the amount of heat given out when unit weight of water cools through unit temperature. 2. Specific Heat. — The mention of a specific substance — water — in the above discussion implies the tacit assumption that different substances require different amounts of heat to heat them up. This question may be investigated as follows : — Let a pound of iron and a pound of lead be placed for some minutes in boiling water until they have acquired the temperature of the water (100° C). Now let each be rapidly removed and placed in separate similar vessels each containing half a pint of cold water at the same temperature (say, the temperature of the air). The metals will give out their heat to the water, which will thus be raised in temperature ; but if the rise in each vessel be ascertained by a thermometer, it will be found that the water containing the iron is considerably hotter than that containing the lead. Since the iron has given out more heat than the lead it must have absorbed more heat from the boiling water ; in other words, it takes more heat to heat up iron to a given temperature than it does lead, weight HEAT— ITS NATURE AND MEASUEEMENT 39 for weight. This fact is expressed scientifically by the statement that iron has a greater specific heat than lead. By definition the specific heat of water is 1 and the specific heats of other substances are numbers showing the relative amounts of heat necessary to heat them up as compared with water. Iron only requires about -|th as much heat as water and lead as little as ^^o^^- Thus the statement that the specific heat of iron is Oil means that, weight for weight, iron only requires '11 units of heat for every 1 unit required by water when each is raised through the same range of temperature. Water possesses a much higher specific heat than any ordinary substance known. A knowledge of the capacity of bodies for heat has much practical utility. In the extraction of metals from their ores, which necessitates usually a number of heating processes, the amount of fuel required will be, among other things, dependent upon the specific heat of the materials. Again, the rate of cooling of bodies, which merits consideration in many heating problems, is proportional to their specific heats. IV. Change of State. Change of temperature is not the only effect produced in bodies by heat, and though a body generally gets hotter when heated, this is not always the case. Apart from change of temperature and chemical change, heat energy may be expended upon producing (1) a change of state in the process of melting or boiling ; (2) a change of volume ; (3) a change of internal stress. Two or more of these effects often occur simultaneously. 1. Latent Heat.— If some lumps of ice be placed in water in sufficient quantity to bring the temperature down to 0° G. and the mixture of ice and water be then heated and kept well stirred, it will be found that, although heat is being 40 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS absorbed, as evidenced by the rapid melting of the ice, a thermometer placed in the liquid will remain at 0° C. until the whole of the ice is melted, after which a regular rise in temperature will occur until the water boils, when the thermometer will again remain stationary at 100° C. while steam is generated. Heat is thus evidently used up in melting and in boiling — that is, in changing the state from solid to liquid and from liquid to gas. Admitting that heat is a form of molecular motion, this conclusion seems reasonable, since to confer increased freedom of motion upon the molecules, necessitated by conversion into the liquid and gaseous condition, must involve the expenditure of a definite amount of heat energy. Heat thus expended in changing the state of a body is known as Latent Heat, and the amount of heat necessary to produce such change of state in a given weight of any particular substance can be measured in ordinary heat units. Thus the latent heat of water is 79, that is to say, that to just melt unit weight (a pound) of ice requires 79 times as much heat as is required to raise a pound of water 1°C., i.e., 79 units of heat. Similarly, to Just boil away a pound of boiling water requires 537 units of heat, i.e., the latent heat of steam is 537. It should be remembered that all these physical changes are reversible. Thus when a pound of steam condenses into boiling water 537 units of heat are liberated and actually available for heating surrounding bodies, which accounts for the very rapid heating of water into which a jet of steam is passed. Similarly 79 units of heat are given out when a pound of water is frozen, which considerably retards the natural formation of ice. 2. Melting-Points. — A pure chemical compound (or element) melts and boils at fixed temperatures; hence a determination of the melting or boiling point often serves HEAT— ITS NATURE AND MEASUEEMENT 41 as an aid to identification, and as an indication of purity, since an impure substance will show a gradual rise of temperature during changes of state as its various con- stituents (each possessing its own melting and boiling point) undergo this change. Commercial substances are, it is true, seldom, if ever, pure compounds, but when a probable adulterant has a melting or boiling point much removed from that of the genuine constituents, an indication of its presence may be made by observing the temperature at which the change of state begins to take place. Thus good mastic melts at about 125° C, but if it is adulterated with coal-tar residues the temperature of fusion observed will be much lower. 3. Change of Volume with Change of State. — Change of state is always accompanied by some change in volume. When a liquid is converted into a gas a very large increase in volume takes place. In the case of water, for example, the expansion is about 1,700, i.e., any volume of water will produce some 1,700 times its bulk of steam. In the case of solids turning into liquids no general rule can be laid down, though most solids expand slightly on passing into the liquid form, and hence such liquids contract on solidifi- cation. Obviously no such bodies can be used for making sharp castings, as such solidified liquids will fail to fill the moulds in which they are formed. Cast iron and certain alloys, however, expand on solidification, as does also water. The expansion of water on solidification has many important effects on natural phenomena. The disintegra- tion of many materials may be traced to this cause. Water finds its way into the pores or cracks in a material, or is stored in a closed water pipe, and when cooled to the freezing point it must either secure additional space for the forma- tion of ice by bursting asunder its confining walls or remain liquid below the ordinary freezing point as the result of compression. As the expansive force involved in solidification 42 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS is much greater than the cohesive power of the particles of most substances, fracture results if the confinement is complete, and often if means of egress are much restricted. Some idea of the force of expansion may be gathered from the fact that to prevent the freezing of water at a tempera- ture of 7 degrees below its ordinary temperature, i.e., at - 7°C., a surrounding pressure of about 14,000 lbs. per square inch would have to be sustained. CHAPTEE V HEAT AND ITS EFFECTS ON MATERIALS In this chapter it is proposed to deal with the expansion caused by heat in cases where changes of state in materials are not concerned, and, as a conclusion to this subject, with the means whereby heat is transmitted from place to place. I. Expansion of Solids. 1. Dimensions and Structure. — Solids when heated expand in all directions, and if they have the same structure throughout they expand in all directions equally, or, more correctly, in proportion to their linear dimensions. Thus a cubic inch of lead will, when heated, expand to the same extent along its length, breadth and thickness, but a piece of lead three inches long and one inch square will expand three times as much along its length as in the other direc- tions, simply because each linear inch expands separately. The expansion of a body is therefore proportional to its length. If a body is not homogeneous — that is, if its properties are not the same in different directions — a cube of such substance will not expand equally in all directions. Thus the expan- sion of a piece of timber along the grain is not the same as that across the grain. 2. Linear Expansion of Solids. — It is often convenient to consider the expansion of a body in one direction only, if one of its linear dimensions exceeds the other two. A steel joist, for example, when heated expands, of course, in all 44 OHEMISTEY AND PHYSICS OF BUTLDINa MATERIALS directions, but the expansion along its length is so much greater than along its breadth and thickness that the increase to the two latter directions may usually be neglected. That expansion does take place for even moderate eleva- tions in temperature may readily be shown by heating a metal rod or tube fixed at one end and resting across a sewing-needle on a flat smooth surface at the other. If a long paper spill or a straw be speared on the point of the needle placed to overhang its support for this purpose, the rotation of the needle caused by the rolling out of the heated metal rod upon it will be made readily evident by the move- ment of the pointer. This experiment might be utilised for comparing the expansions of different materials, by heating to the same temperature rods of equal length of various materials and noting the angle through which the needle pointer was rotated in each case. This would be found to be different in different cases — that is to say, the linear expansion of different materials is not the same. 3. Co-eflBcient of Linear Expansion. — The natural unit of expansion would be the amount of increase in length which the unit length of a substance would acquire when heated through 1° C. The fraction of the original length gained when a body is heated 1° C.'- is known as its co-efficient of expansion, or, more correctly, as its co-efficient of linear expansion. As an example the co-efficient of expansion of lead in terms of degrees Centigrade will be found stated in tables of physical data as 0'000028, which means that a piece of lead of any given length increases by 0-000028 of this length for each degree C. through which it is heated. Thus 1 yard of lead heated 1° C. will become 1-000028 yards, and 7 yards will become 7 + (7 X 0*000028) ^ Strictly speaking, when heated from 0° C. to 1° C, but the above definition serves for practical purposes. HEAT AND ITS EFFECTS ON MATERIALS 45 yards. To find the increase in length when the tem- perature is raised more than 1° C. it is merely necessary to multiply the above result by the rise in temperature. Thus 1 foot of lead heated 25° C. becomes 1 + 0-000028 X 25 feet, and 18 feet heated 25° C. becomes 18 + (18 X 0'000028 X 25) feet. To determine, then, the increase in length in any case it is only necessary to multiply the number of units of length in question by the co-efficient of expansion and this result by the rise in temperature ; the product added to the original length gives the new length under the altered conditions of temperature. If the Fahrenheit scale be adopted the numbers repre- senting the co-efficients will be smaller, because degrees F. do not represent so great a rise in temperature as degrees C, but the method of calculation is the same as that just given. 4. Practical Importance of Expansion. — The expansion of bodies is of considerable importance in many constructional problems where long lengths of rigid materials are employed or when different substances of a fragile nature are united. A steel joist 30 feet long is, for example, about | of an inch longer in summer than in winter, hence long steel structures must not be rigidly fixed at both ends. The Forth Bridge, which is a yard longer in summer than in winter, forms a striking example of expansion. When hot liquids or gases are conveyed in pipes the great change in temperature which such pipes have to undergo often renders special expansion joints necessary. In such cases freedom of motion is essential, and the casing of such pipes in brick or concrete would lead to disruption of such materials. The methods employed for attaching lead and zinc to roofs and flats are intimately related to the subject under discussion. The co-efficient of expansion of these metals is very great, about 2J times that of steel. If permanently fixed in large sheets, therefore, they must necessarily 46 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS buckle when exposed to the sun's heat and eventually either tear themselves free from restraint, or fracture. The high specific gravity of lead coupled with its great expansion confers a tendency to work down a sloping roof, as when contraction occurs as an expanded sheet cools this tends to take place more at the upper than the lower end of the sheet, inasmuch as shrinkage at the lower end involves work in raising the metal to a higher level against the attraction of gravity. When a substance consisting of two or more bodies which have different co-efficients of expansion undergoes any change of temperature, it is subjected to stresses, since its various parts cannot expand freely. Thus Portland cement has a co-efficient of expansion of O'OOOOll, and cannot therefore make a reliable joint under varying temperatures with lead (co-efficient 0*000028) . On the other hand, the co-efficient for steel fortunately approaches very closely to that of concrete, so that these materials behave well in contact. In the case of brittle substances fixed together this unequal expansion is a frequent source of fracture. The cracking of glaze upon tiles and terra cotta may often be attributed to a lack of appreciation of the principles here cited. The force of expansion is very great, and to prevent expansion or contraction, which would occur with change of temperature, requires a force equal to the tensile or compressive stress which would be necessary to lengthen or compress the material to the new lengths which it tends to assume. This is occasionally taken advantage of for straightening the walls of buildings. An iron rod is attached at one end to some rigid structure and the other passed through the bulged wall, the rod is heated and then tightened up to the wall by a nut and washers externally. In order to assume its original length on cooling, the rod has to draw the wall inwards. HEAT AND ITS EFFECTS ON MATEEIALS 47 It will have been observed that the foregoing remarks on the importance of expansion have been devoted chiefly to the metals. Allowance for expansion in non-metallic bodies such as stone, brick or concrete is not usually of importance. The reason for this is partly because such bodies have, as a rule, smaller co-efficients of expansion and higher specific heats, and thus require more heat to produce a given rise in temperature than the metals, but mostly on account of their poor conductivity, which, in ordinary cases of change of temperature, makes them exceedingly slow in adapting themselves as a whole to temperature variations to which they may be exposed. II. Expansion of Liquids. It has been pointed out that liquids as a class expand more than solids. Many instances of this fact present themselves : for example, mercury or spirit would not rise to the stem of a thermometer did not these liquids expand more than the glass tube containing them. The expansion observed in all such cases is in reality the excess of expan- sion of the liquid over that of the containing vessel. 1. Expansion of Water. — The only liquid of any import- ance in this discussion is water, which behaves in a quite exceptional way at low temperatures, actually contracting in volume when its temperature is raised from 0° C. until 4° C. is reached, after which it expands continuously, though not very regularly, until it reaches its boiling point. Water has, therefore, a greater specific gravity at 4° C. than at any other temperature, and if a quantity of water is cooled the cold layers will sink to the bottom as their specific gravity increases, and finally the temperature of the lowest layers will be found to be 4° C. After the whole of the water has assumed this temperature further cooling will result in the 48 CHEMISTRY AND PHYSICS OF BUILDINa MATERIALS colder layers remaining at the surface. Hence the tempera- ture of all deep undisturbed water approximates to 4° C. When cold water is raised to its boiling point it expands by about 4 per cent. : a fact which must be allowed for in estimating the capacity of vessels which contain water which is likely to be heated. 2. Circulation of Water. — The circulation of water in pipes is entirely dependent upon the difference of specific gravity of water at different temperatures. The water in contact with the lower heated surface of a boiler expands and rises through the colder layers above it, and the heavier displaced water will fall and in turn be heated. Thus a continuous circulation is set up. It follows that the water will be heated with much greater rapidity if the heat be applied to the bottom of the boiler than if applied at the top. If pipes are attached to the boiler the circulation and consequent distribution of heat to surrounding bodies may be correspondingly extended. If the heated water be allowed to follow a continuous upward path to the furthest positions from the boiler, and to return (cooled) downhill, eventually entering the boiler again near the bottom, circu- lation will obviously be most rapidly effected. III. Expansion of Gases. 1. Charles' Law. — Gases when heated expand very much more than solids or liquids, and, whereas the expansion in the case of solids and liquids varies with each individual substance, all gases expand to the same extent for any given increase in temperature. If a bottle of known capacity filled with air be heated in boiling water and then rapidly inverted in cold water, water will enter it as the expanded air is cooled, and the volume of water which enters will be a measure of the air expelled, HEAT AND ITS EFFECTS ON MATEEIALS 49 or of the expansion which has taken place between the temperatures of the boiling and cold water. Experiments based on these lines have shown that a given quantity of any gas if heated from 0° C. expands of its original volume for each degree C. through which its temperature is raised. The discovery is known, after the name of the investigator, as " Charles' Law." This law, and that of Boyle previously explained as giving a general relation between the pressure and volume of gases, stand at the foundation of all calculations dealing with the distribution and flow of air and other gases. 2. Ventilation. — To the great co-efficient of expansion of air its movement in heated and inhabited rooms is chiefly due. The warmed air from persons or heated materials rises. This may be looked upon as the ordinary behaviour of a light body tending to float upon a heavier body, or — and this has a deeper significance — as movement due to two columns of air of unequal weight. If the heated air be considered to be enclosed in a column, say, the height of the room, this air is lighter than a similar column of cold air outside, and an unstable condition is set up as in a syphon discharging water. No longer able to balance the cold external air, that in the room will be pressed upwards and will escape through suitable outlets at the top of the room, provided that, and only provided that, the cold air is allowed to exert its pressure freely through inlets of suffi- cient area at low level. This forms the basis of a system for effecting what is known as natural ventilation. IV. Transmission^ of Heat. There are three distinct ways in which heat may pass from one body to another, known as (1) Conduction, (2) Convection, (3) Eadiation. 1. Conduction. — Heat is said to pass from one body to B.M. B 50 CHEMISTRY AND PHYSICS OF BUILDING MATEEIAXS another in contact with it or from one part of a body to another part of the same body by conduction when this transference takes place without any motion (other than molecular vibration) of the body or bodies themselves. Thus heat received by water in a boiler passes from the fire through the boiler walls by conduction. All substances conduct heat to some extent, though this power is vastly different in different bodies. (a) Measurement of Conductivity. — If a piece of iron and a piece of copper wire of similar diameter be coated with wax (which may be effected by warming them and then drawing them across a candle), and if one end of each be placed in a flame, it will be noticed that wax will melt along the copper wire to a greater distance than along the iron wire. Since the heat reaches the wire by conduction, the experi- ment shows copper to be a better conductor than iron. The point at which the melting stops on each wire will be that at which the air robs the material of its heat suffi- ciently rapidly to reduce the temperature to a point below the melting point of the wax, and the position of this point on the wire will depend upon the rate at which heat can flow through the material from the flame. The actual con- ductivity may be shown to be proportional to the square of the distance along which the wax is finally melted. (h) Good and Bad Conductors. — The metals as a class are the best conductors ; non-metallic mineral substances such as stone and concrete, and such bodies as wood, water, and glass, are bad conductors, while most carbonaceous substances, such as oils and woollen fabrics, are still worse conductors. Some idea of the variation of this property in different substances may be obtained from the statement that silver, the best-known conductor, possesses a con- ductivity some 20,000 times as great as that of dry air, which is one of the worst conductors. (c) Practical Importance. — Conductivity has many HEAT AND ITS EFFECTS ON MATERIALS 51 bearings of practical importance. The use of felt for roofing and other coverings, and the lagging of pipes, will suggest themselves, and since the rate of transmission of heat by conduction is inversely proportional to the thickness of the material, the thickness of any such layer of bad conductor specified should be based upon a knowledge of its conducting power. (d) Conduction for Heat and Electricity. — Good heat conductors are always good electrical conductors, and vice versa. The actual conducting powers for heat and electricity possessed by a given substance are not, however, identical. 2. Convection. — Heat is said to be transmitted by con- vection when the heated body or a part of it actually moves from one place to another in the process of transmission. Thus if a hot body be carried from one room to another, heat has reached the latter room by convection. The passage of heat in liquids and gases (nearly all of which are very bad conductors) takes place almost entirely by this method of transference. Hot water and hot air systems are practical examples of the use of convection. The heated particles of liquids and gases rise through the colder particles owing to expansion, thus compelling the latter to take their place and to come into contact with the source of heat, while the first heated particles eventually give up their heat by conduction, and are thus in turn brought again to the source of heat, and this cycle of operations results in a continuous circulation. 3. Radiation. — It is evident that heat is transmitted in some other manner than by conduction and convection, since it readily passes though a vacuum. A glow lamp, for example, becomes hot though the filament glows in empty space ; and the heat of the sun reaches the earth across a vacuous space of many millions of miles. (a) Nature of Radiant Heat. — In such cases heat is said to be transmitted by radiation. The chief peculiarity of B 2 52 CHEMISTEY AND PHYSIOS OF BUILDING MATEEIALS this form of transmission lies in the fact that the inter- mediate space between the source of heat and the substance thereby heated is not raised in temperature. The heat is in fact propagated as waves of energy which only become heat as ordinarily recognised when they strike some object, and for practical purposes the object must be a liquid or solid ; in other words, radiant heat passes through gases without sensible conversion into effective heat. Although the hotter a body the greater the amount of heat emitted by radiation, such emission is by no means confined to bodies hot enough to emit light. (&) Practical Value of Radiant Heat. — The aim of all artificial systems of heating should be to provide as large a proportion of radiant heat as possible, thus taking the sun, admittedly the healthiest source of heat, as a model. The chief advantage of radiant heat lies in the fact that by it persons and things are warmed directly, while the air surrounding them remains cool and suitable for respiration, whereas heated air is not only undesirable for respiratory purposes, but by promoting more rapid evaporation of moisture from the body produces, as does all evaporation, cold. It must thus be supplied at an unnaturally high temperature if the sensation of warmth is to be thereby established. The ideal method of artificial heating might possibly prove to be a sphere maintained at a white heat in each room, with means for ventilation above it, whereby any chance organic particles, produced in the surrounding atmosphere, might be rapidly removed, which would prevent their charred remains from vitiating the air. CHAPTER VI CHEMICAL SIGNS AND CALCULATIONS I. Atomic Theory. In some brief comments upon the constitution of matter reference was made in Chapter 11. to atoms and molecules' and the atom was defined as the smallest particle into which matter is divisible. This atomic theory— that is this presumption that matter can only be divided up to a fixed degree of fineness— is a very old one; but a century ago it received at the hands of John Dalton an important exten- sion which at once raised it to a position of the greatest utility, and coupled it with his name. His addition to the theory lay m the discovery of the fact that all atoms of a given element have the same weight. This discovery forms the basis of all chemical calculations, and upon it modern chemical theories have been built up. At the present time it seems likely that the atomic theory is about to experience another great development owing to the discovery of radium and the resulting work since achieved by chemists in the field of radio-activity and It is now suggested that the atoms are in combination with bodies which have been named ''electrons," which them- selves possess weight, though the weight of an electron is exceedingly minute even as compared with the almost inexpressibly small weights of atoms. These electrons appear to give a measure of the chemical activity or power of entering into combination possessed in very varvine degree by different elements. This addition to the atomic theory, though of great 54 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS interest, is hardly likely, however, to affect any of the chemical considerations discussed in these pages for some time to come. II. Atomic Weights and Symbols of the Elements. 1. Relative Weights of the Atoms.— The actual size of atoms and hence their weights, are, as has been stated, exceedingly small. Lord Kelvin has supplied a popular conception of this size by the statement that one drop of water contains more molecules than the number of cricket balls which would be required to make a sphere as large as the earth ; each of these molecules of water, moreover, consists of three atoms. It may well be asked, therefore, What is the value ot a knowledge of the weights of atoms ? The actual weights of these minute bodies are of no practical interest, but their relative wei^/ite— that is, information as to how much heavier the atoms of one element are than those of another— are ot great value, and these relative weights are known as the atomic weights of the elements. As in other comparisons, some element must be selected as a standard and the weight of its atom called 1. The element usually taken is that of the gas Hydrogen, which is the lightest common substance known. Thus the statement that the atomic weight of zinc is 65 means that the atom of the element zinc weighs 65 times as much as the atom ot hydrogen. , 2. Symljols. — Instead of writing the names of the elements in full it is customary to designate them by their initials; thus C stands for Carbon and 0 for Oxygen. Inas- much, however, as many of the elements have the same initial letter, a second letter of the name is appended where necessary and is written as a small letter alongside the first- just as, for example, the letters St. " are used to represent CHEMICAL SIGNS AND CALCULATIONS the word " street." Thus S stands for Sulphur and Si for Silicon. These chemical initials are known as Symbols. Many of the elements were discovered and named in early times when books were written in Latin, and though the^ English names have now replaced the original Latin designations, the symbols of the Latin names are in many cases retained, which accounts for many symbols possessing no apparent connection with the names of the elements as now used. For example, the symbol for Iron is Fe, from the Latin for iron — Ferrum. Although symbols have been described above as a species of chemical shorthand, they possess a much more important significance, since the symbol of an element when written is always taken to represent one atom. Thus Al does not imply an indefinite quantity of Aluminium, but one atom of the metal, or 27 parts by weight (its atomic weight) as compared with 1 part by weight of Hydrogen, represented by the symbol H. This aspect of the use of symbols is of the greatest importance in dealing with chemical equations. 3. Table of Symbols and Atomic Weights.— The table on the following page shows the symbols and approximate atomic weights of the elements found in building materials, arranged in the order of such weights. Those elements possessing the physical characters distinctive of metals are marked with an asterisk, while the elements of lesser importance are printed in smaller type. III. Combinations of Symbols, or Formul-e. It has been said that the symbol of an element expresses one atom ; if two atoms are in question, instead of writing the symbol twice over, the number 2 is placed either in large type before the symbol or in small type after and 56 CHEMISTRY AND PHYSIOS OF BUILDING MATEBIALS Table of Elements used in connection with Building Materials. Name. Hydrogen Boron Carbon Nitrogen Oxygen Fluorine ^Sodium ♦Magnesium ^Aluminium SUicon Phosphorus Sulphur Chlorine ♦Potassium ♦Calcium *Chromium Symbol. Approx. At. Wgt. Name. Symbol. Approx. At. Wgt. H 1 *Manganese Mn 55 B 11 ♦Iron Fe 56 C 12 ♦cobalt Co 58 N 14 ♦Nickel Ni 58 0 16 ♦Copper Cu 63 F 19 ♦Zinc Zn 65 Na 23 Arsenic As 75 Mg 24 ♦Silver Ag 108 Al 27 ♦cadmium Cd 111 Si 28 ♦Tm Sn 118 P 31 *Antimony Sb 120 S 32 ♦Barium Ba 136 CI 35^ *Gold Au 196 K 39 *Mercury Hg 199 Ca 40 ♦Lead Pb 205 Cr 52 •^Bismuth Bi 207 below the symbol ; thus 2 H or H2 stands for two atoms of hydrogen, and larger numbers of atoms are expressed similarly. Chemical compounds can be represented in the same manner by writing the symbols of the elements they contain side by side with the numbers (if more than one) of the atoms of the elements present. Thus the symbols PbO standing together represent litharge, or lead oxide, which consists of one atom of lead combined with one atom of oxygen. In the case of the common red oxide of iron, two atoms of iron are combined with three atoms of oxygen, and the compound is therefore expressed as FeaOs. The use of the word " symbol " is confined to elements; when these are combined as above the expression is always referred to as a Formula. Thus chemists speak of the symbol for iron, and of the formula for iron oxide. In CHEMICAL SIGNS AND CALCULATIONS 57 formulae the numbers expressing the number of atoms are always written as small numerals below the right-hand side of the symbols as shown above ; numbers in large type in front of a formula always mean that the whole formula is referred to taken so many times over. Thus 2 PbO indicates, not two atoms of lead and one of oxygen, but two of both elements, that is, two complete molecules of lead oxide, or 2 (PbO), the bracket being always understood. Again, H2O is the formula for water, and 10 H2O represents ten whole molecules of water, or twenty atoms of hydrogen and ten atoms of oxygen. If a compound consists of complex parts which can be separated as such, or sometimes if doubt exists as to the exact manner in which these parts are combined, they are often written as separate compounds, in the manner described above, but making one formula, with each part separated by a dot or full stop. Thus wash- ing-soda crystals are partly composed of carbonate of soda and partly of water which can be removed. These crystals have the formula Na2C03. IOH2O. Again, cement is com- posed of lime, CaO, and silica, Si02. If two molecules of the former are combined with one molecule of the latter, the formula might be represented as 2CaO.Si02. It should be carefully observed in such a formula that the number 2 only qualifies that part standing before the dot, which is sometimes emphasised by placing this part in brackets, thus, 2 (CaO). Si02. This formula might also be written Ca2Si04 by adding all the oxygen atoms together, but usually the former method of expression gives a better insight into the structure, and to adopt the second method in the case of washing-soda crystals by writing the formula Na2C03. 10 H2O as Na2CH2oOi3 would be very misleading. IV. The Assigning of Fokmul^. The formula proper to any compound can only be ascer- tained after a chemical analysis, showing not only what 58 CHEMISTEY AND PHYSICS OF BUILDING MATEKIALS elements it contains, but the proportion of each present, when, on dividing the amount of each element by its atomic weight, the number of atoms of each will be obtained. Thus water contains hydrogen and oxygen ; its formula, however, is not HO, because analysis shows that for every sixteen parts of oxygen there are two parts of hydrogen present. Since the atomic weight of oxygen is sixteen and that of hydrogen one, it is evident that one atom of oxygen is combined with two atoms of hydrogen, and that the simplest formula for this compound is therefore H2O. Analysis merely gives the proportion of each element present, which is most conveniently expressed as the per- centage. As an example of the construction of a formula which is obtained by dividing the percentage of each element present by the atomic weight of that element, the compound chalk may be taken. This body is found to consist of 40 per cent, of the metal calcium (Ca), 12 per cent, of carbon (C), and 48 per cent, of oxygen (0). On referring to the previous table of atomic weights, it it will be seen that Ca =: 40, C = 12, 0 = 16, and on dividing the percentages by these weights the following numbers of atoms are obtained: — 40 -r- 40 = I for calcium, 12 -f- 12 = 1 for carbon, and 48 -r- 16 = 3 for oxygen. The compound therefore consists of one atom of calcium, one atom of carbon, and three atoms of oxygen, or is CaiCiOa, or, since the symbols themselves represent single atoms, the formula is CaCOa. Naturally, all calculations are not quite so simple, but the principle utilised is always the same, and since common compounds seldom contain more than three or four atoms of any one element in their molecules, the assigning of a formula in such cases is a fairly easy matter. It may be argued that by the above determination the formula for chalk might be any multiple of the formula CaCOs. This is true, but does not affect the use of the CHEMICAL SIGNS AND CALCULATIONS formula in calculations, and for the purposes of this book it may be taken that the simplest formula which will give whole atoms is that adopted. Since mixtures of elements or compounds have no definite composition, they can have no formula, and it is often possible to tell whether a sub- stance is a true compound or not by finding out whether the elements it contains are present in a proportion repre- senting whole numbers of atoms. Thus air, though fairly uniform in composition, does not contain oxygen and nitrogen in atomic proportions ; it is a mere mixture of these two gases and possesses, therefore, no formula. V. Chemical Equations. 1. Meaning of Equations.— "When a chemical change takes place, either owing to the action of heat or some other form of energy on a compound, or to the action of one body on another, the change may be expressed by writing the formula of the compounds affected and of the new com- pounds produced in the form of an equation, just as would be done in algebra. The bodies taken are always repre- sented on the left or those resulting on the right of the equation, with the sign =, indicating the word "gives," placed between the two sides of the equation, and the sign -f- between each body. Thus, if some litharge (lead oxide) be heated with charcoal (carbon), metallic lead and an oxide of carbon result, which is expressed as follows :— Lead Oxide. Carbon. Lead. Oxide of Carbon. Pbo -h C = Pb -t- CO Again, when chalk or limestone is heated, quicklime is formed and carbonic acid gas (CO2) is driven off thus :— Chalk. Quicklime. Carbonic Acid Gas. CaCOs = CaO + CO2 If an equation really expresses the changes which take 60 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS place, it is obvious that everything taken must be accounted for and must appear in some new form of combination on the right-hand side of the equation. It is sometimes of value in more complex examples to check this by counting up the total number of atoms on each side, which should always be equal. 2. Calculations. — Since these equations represent definite chemical reactions with definite weights of bodies, they give the most valuable information as to the amount of a given substance which can be produced from a given quantity of another substance. To obtain such informa- tion, the equation representing the chemical reaction is first necessary, then atomic weights of the elements present are written below their symbols, and where more than one atom^ is present the atomic weight of such element is multiplied by the number of its atoms. The weights thus obtained are added together for each compound, giving the weight of the molecule of the compound or the "molecular weight." The weights of the bodies produced from the weights taken are thus obtained, and the relation between the two will be true whatever unit (the gram or the pound, etc.) is adopted for expressing such weights. Finally, if the weight of one or more of the bodies required to be produced is given, the weights of the bodies necessary for the purpose can be ascertained (or vice versa) by a simple proportion sum. This reasoning may be applied to the first equation given by writing the atomic weights below the elements, thus : — PbO + C =r Pb + CO 205 + 16 + 12 = 205 + 12 + 16 221 + 12 = 205 + 28 or, in words, 221 parts by weight of lead oxide heated with 12 parts by weight of carbon produce 205 parts of lead and 28 parts of oxide of carbon. From 221 pounds (or CHEMICAL SIGNS AND CALCULATIONS 61 tons or ounces) of lead oxide, therefore, 205 pounds (or tons or ounces) of metallic lead would be produced. As a second instance, the following question may be answered. What weight of quicklime (CaO) can be obtained from j&ve tons of pure chalk (CaCOs) ? CaCOg = CaO + CO2 40 + 12 + (3 X 16) = 40+16 + 12 + 32 100 = 56 100 tons of chalk would produce 56 tons of quicklime, consequently 1 ton would produce of this or tons, 56 X 5 and 5 tons five times as much, namely, — Jqq~~ ~ ^'^ tons, or 2 tons 16 cwt. In each of these equations only single molecules are involved, but the solution is no more difficult in other cases. When more than one molecule of a compound is present the whole weight of such molecule must be naturally taken the number of times over the molecule is present ; thus when spirits of salt, HCl, acts upon zinc the equation and summation of weights is as follows : — Zn + 2 HCl = H2 + ZnCla 65 + 2(1 + 35^) = 2X1 + 65+(2X35J) 65 + 73 = 2 + 136 The practical value of a knowledge of chemical equations will be obvious even from these simple examples quoted. VI. Chemical Nomenclature. 1. Names indicate Composition. — The names assigned to chemical compounds are not given haphazard, like the majority of popular names in use, but generally convey a good deal of information as to composition, and often an indication of the proportion of some of the elements present. Thus all bodies which are termed oxides contain oxygen, 62 CHEMISTRY AND PHYSIOS OF BUILDING MATERIALS and those termed sulphides, sulphur, while carbides, car- bonates, and hydrocarbons all contain the element carbon. The termination ** -um " is usually confined to elements which are metallic in character — for example, aluminium and calcium — while the ending "-a" is found in the old and still used names for certain oxides, such as alumina and silica. The termination " -ide " indicates the presence of only two elements in a compound. Thus lead oxide consists only of lead and oxygen, sodium chloride of only sodium and chlorine. The termination " -ate," as in carbonate and sulphate, indicates the presence of three or four atoms of oxygen in a compound of three or more elements. As several different compounds containing the same elements but combined in different proportions are often found, a further distinction is necessary in such cases. Thus there are two oxides of carbon, CO and CO2. In such case the prefixes "mono-" or ** mon- " and " di- " are generally added to indicate the presence of one and two atoms of oxygen. Thus CO is carbon monoxide, and CO2 carbon dioxide. The terminations " -ous " and " -ic " indicate respectively a smaller or larger proportion of non-metallic element in a compound. Thus the oxide of iron, FeO, is termed ferrous oxide, and the better known, red oxide, FesOa, ferric oxide. Many old or popular names for such compounds are, however, still in general use, and these should be remem- bered. Thus carbon dioxide is also known as carbonic acid gas. The modern chemical name for the compound Na2S04 is sodium sulphate, the older and still used name is sulphate of soda, and the popular name Glauber's salts. Similarly sodium carbonate is also called carbonate of soda, and, popularly, washing soda. In order to aid the student, a short list, showing the chemical and popular names of some commonly occurring compounds relating to building materials, is appended. POPULAE AND SCIENTIFIC NAMES FOB COMMON SUBSTANCES. Popular Name. Chemical Name. Formula. Mineralogical Name. Ammonia (hartshorn) Ammonium hydrate . NH4OH Sal volatile Ammonium car bon ate (NH4)2COs . Sal ammoniac Ammonium chloride . NH4CI Alumina Aluminium oxide AI2O3 Corundum BaCOs (Emery) Carbonate of baryta . Barium carbonate Witherite Heavy spar Barium sulphate BaSOi Barytes Carbonate of lime Calcium carbonate CaCOa Calcite, chalk, marble, lime- stone Quicklime Calcium oxide CaO Slaked lime Calcium hydroxide . CaOgHg Sulphate of lime . Calcium sulphate CaSOi Gypsum, selenite CaS04 2H2 0 Chloride of lime . Calcium hypochlorite CaOCla Chrome green (real) . Chromium oxide CraOg Carbonate of iron Ferrous carbonate FeCOs Ironstone Black oxide of iron Triferric tetroxide Magnetite Green vitriol Ferrous sulphate FeSOi. 7H2O Red oxide of iron Ferric oxide FeaOg HEematite Litharge Lead monoxide PbO Eed lead Red lead PbsOi White lead (Dutch) . Lead carbonate and PbCOg and hydrate PbOaHa Chrome yellow Lead chromate . PbCr Oi Magnesia Magnesium oxide MgO Carbonate of magnesia Magnesium carbonate MgCOs Magnesite Epsom salts Magnesium sulphate . MgSO^.THzO . Black oxide of man- Manganese per- or di- MnOa Pyrolusite ganese oxide KNO3 Alum (common) . Potassium, aluminium K2S04.Al2(S04)8 sulphate 24H20 Silica Silicon oxide SiOg Quartz, Flint (Sand) Washing soda Sodium carbonate NagCOa 10 H2O Caustic soda Sodium hydrate NaOH Chill nitre . . , Sodium nitrate » Chili saltpetre Glauber's salt Sodium sulphate NaaSO^ 10 H2O Salt Sodium chloride NaCl Rock salt Borax Sodium borate . Na2B407 10 H2O White vitriol Zinc sulphate . ZnS04 7H2O Zinc white . Zinc oxide ZnO Spirits of salt Hydrochloric acid HCl + water Aqua fortis . Nitric acid HNOs Oil of vitriol Sulphuric acid . H2SO4 Vinegar Acetic acid HC2HSO2 Carbonic acid gas Carbon dioxide CO2 Carbolic acid Phenol CeHgOH . . CHAPTBE VII WATER AND ITS IMPURITIES The physical characteristics of water have already been touched upon, but in the present chapter it is proposed to discuss the chemical composition of water and impurities contained in water as obtained from natural sources. I. Composition of Water. 1. Decomposition "by Metals. — If steam be passed through a red-hot iron pipe the issuing vapour is found to contain a gas which will burn, and an examination of the interior of the pipe will further show that the iron has been consider- ably oxidised. The steam has been decomposed into its constituent gases, namely, oxygen, which has attacked the iron ; and hydrogen, the inflammable gas which issues from the pipe. Most metals will decompose water under suitable condi- tions owing to their tendency to oxidise, and if a solvent for the oxide formed be present, fresh surfaces of metal are constantly exposed, and the evolution of hydrogen may be made continuous. The "killing" of hydrochloric acid (spirits of salt) by zinc for making soldering fluid is an instance of the decom- position of water by zinc in the presence of an acid, and forms the ordinary means of producing hydrogen gas in the laboratory. Analysis has shown that the molecules of water are composed of two atoms of hydrogen combined with one of oxygen. The formula for water is therefore H2O. WATEE AND ITS IMPUEITIES 66 The chemical equations representing the action of water upon zinc, and the solution of the resulting zinc oxide hydrochloric acid are Zn + H2O = ZnO + H2 ZnO + 2HC1 = Zn CI2 = H2O. 2. Decomposition by Electricity. — When a current of electricity from two or three electric cells is passed through water, the water is decomposed, and if the wires conveying the current to the water consist of unoxidisable metals such as gold or platinum, both the oxygen and hydrogen are liberated in a free state. When decompositions due to the passage of electricity take place the process is known as Electrolysis, and the compound thus decomposed is called an Electrolyte. 3. Properties of Hydrogen. — Hydrogen gas is almost the lightest substance known. It is colourless and invisible, and burns in air with an exceedingly hot flame to form water, which accounts for the water deposited upon cold surfaces when ordinary combustible illuminants such as oil or coal gas are burnt, since such bodies contain hydrogen. II. Solvent Power of Water. The changes which are brought about in materials through the agency of water are largely due to its great solvent powers. No substance is absolutely insoluble in water, and though many may be considered to be so for all practical purposes, water, more especially when armed with its ordinary impurities, possesses much greater solvent power than is generally imagined, and it is this fact which renders it so potent an ally in cases of chemical action. 1. Solution of Solids. — The amount of a solid body capable of solution in a given quantity of water increases (with one B.M. F 66 CHEMISTEY AND PHYSICS OP BUILDING MATERIALS or two exceptions) with increase of temperature, though by no means necessarily in proportion to the rise in tempera- ture. In all cases, however, the amount of a given sub- stance which can be dissolved by a given quantity of water at a stated temperature is limited, and when this limit is reached the water is said to be " saturated." Lowering of temperature or removal of some of the water, as by evapora- tion, result in deposition of a dissolved solid from a saturated solution, usually in a crystalline form, and the shape of such crystals of deposited solid, and more particularly their size, is greatly influenced by the rate of their formation. The more slowly this proceeds the larger are the crystalline fragments deposited. Deposition of solids from solution accounts for the forma- tion not only of many minerals, but also for not a few of the changes which occur in building materials. 2. Solution of Gases. — Many gases dissolve in water, but unlike solids, the amount which a given quantity of water can absorb is less at high than at low temperatures. Unless any chemical action takes place between the gas and the water the former is always completely expelled when the water is boiled. The solution of air and carbon dioxide in water are matters of considerable importance in connection with materials. III. Water of Crystallisation. 1. Meaning of the Term. — When substances crystallise from solution it is found that in many cases water is taken up by the solids in the process, not in the form of liquid acciden- tally entangled in the solid mass, but as a part of the solid itself, definite in amount and forming an essential in determining that regularity of form which is the charac- teristic of a crystallised compound. Water thus combined with solids is known as " water of crystallisation." WATEE AND ITS IMPURITIES 67 Thus if dry powdered carbonate of soda be dissolved in water until a saturated solution is obtained, and this solution be then cooled or evaporated, ice-like crystalline masses appear which may be removed and dried ; but if they be then heated a large amount of water will be driven off, resulting in the breaking up of the crystals, which will thereby be reduced to a shapeless powder and leave the original substance dissolved. The dry carbonate of soda has the formula Na2C03, while the crystals deposited from solutions possess the composition NaaCOs IOH2O. 2. Eflaorescence. — All compounds containing water of crystallisation can be deprived thereof by the action of heat, though not always quite so completely as in the preced- ing instance, and in many cases so feeble is the state of combination that a warm or dry atmosphere is alone sufficient to remove this water. Both carbonate and sulphate of soda lose some of their water of crystallisation on exposure to a dry atmosphere, which results in the colourless transparent crystals of these compounds falling into a white opaque powder. Bodies which thus readily part with their combined water are said to be Efflorescent. The unsightly deposits, known as " white- wash," often seen on the face of brick or stone work are usually the result of the efflorescence of soluble compounds contained in these materials, as to which more information will be found when such materials are discussed. 3. Deliquescence. — Many compounds when deprived of their water of crystallisation show a very strong tendency to re-absorb water from any available source, and in some cases this absorption will continue, not only until sufficient water has been taken up to enable such bodies to re- crystallise, but until actual solution in considerable excess of absorbed water takes place. The result of this is that such substances, when exposed to the air, which is always more F 2 68 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS or less moist, will become wet. Bodies which behave in thig manner are termed Deliquescent. Calcium chloride (CaCla), largely used to absorb moisture from air or other gases, and magnesium chloride (MgCl2), always present in common salt, are instances of deliquescent bodies. Such substances are naturally very objectionable adjuncts to building materials, more particularly where such materials have to be treated with decorative coverings. IV. Impurities in Natural Waters. The foregoing remarks apply to water considered as a pure chemical compound, but owing to its solvent power it is never found pure in nature. A brief consideration of the history of water as found will be sufficient to make this evident. Evaporated by warm air or the direct heat of the sun from the oceans or other free surface, water is constantly rising as vapour into the colder air strata above the earth, where it condenses into drops which form clouds. Eventually these drops become by successive additions so large that the air is unable to support them, and they fall as rain, which immediately begins to exert its solvent action. 1. Air and other Gases in Water. — Air is soluble in water to the extent of about 2 per cent, by volume at ordinary temperatures. In its fall through the atmosphere, there- fore, water dissolves some air and thus arrives on the earth's surface with some oxidising power, and this solution of air is also continually taking place at every free water surface. Oxygen is more soluble in water than nitrogen, and since these gases forming the air are merely mixed, each can dissolve separately, and as a result it is found that about one-third of the gas from air dissolved in rain water is oxygen, whereas it will be remembered that only one-fifth of the air consists of this component. WATEE AND ITS IMPUEITIES 69 Besides oxygen and nitrogen, air contains carbon dioxide, and since this gas is very soluble in water, it is always to be found among the gases in solution, and where water has come in contact with decaying vegetable or animal matter the quantity of this gas is very much increased, and the free oxygen directly diminished, since it is itself converted into carbon dioxide in the process of oxidising such organic matters. Under certain local circumstances water also contains acid gases derived from the atmosphere, the most important of which is that formed by the combustion of sulphur always present in coal, which with water and oxygen forms sulphuric acid. 2. Mineral Matters Dissolved in Water. — As soon as water touches the ground it adds to its impurities by the solution of substances from the soil or underlying strata through which it passes. The character of these dissolved bodies necessarily varies with the nature of the ground. For example, water which has flowed through marshy land over a clay soil will not be found to contain the same impurities as water which has traversed a limestone district. The direct solvent power of water enables it to take up such compounds as sodium chloride (salt), calcium sulphate, magnesium chloride and sulphate and sodium carbonate and sulphate, which commonly result from the disintegration of various kinds of rocky strata. The presence in water of carbon dioxide (CO2) adds very materially to its power of solution, chiefly in enabling it to dissolve calcium carbonate (CaCOa), whether in the form of chalk, limestone or marble, and armed with this gas water can also dissolve the carbonates of iron and magnesium. The "hardness" of water (see Section V.) is due to the presence of calcium and magnesium compounds. 3. Organic Impurities. — Water usually contains small 70 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS amounts of organic impurities derived from the decay of vegetation, or animal matters, or possibly from sewage contamination. This results in the eventual production of small quantities of nitrates (compounds of nitric acid (HNO3)) and of smaller quantities of ammonia, which provide the analyst with a means for detecting and estimating such impurities. Sodium chloride (salt) is also found in animal excretions, hence the presence of abnormal quantities of salt gives, in the absence of its production from mineral sources, a valuable indication of sewage contamination. 4. Suspended Matter. — Water containing all the above impurities may be perfectly bright, clear and tasteless, hence little indication as to the character of water can be obtained by simple inspection. Certain waters, particularly those of river origin, contain, in addition to dissolved matters, suspended solid particles, such as sand or mud, and these alone can be removed by ordinary filtration processes. V. Hardness of Water. The objection to " hard water " for many domestic purposes and the deposits to which it gives rise in vessels in which it is heated, are well known. Hardness is usually spoken of under two headings : {a) that which can be removed by raising the water to its boiling point and keeping it boiling for a few minutes ; {h) that which cannot be so removed. The former is known as temporary, the latter as 'permanent, hardness. 1. Temporary Hardness. — This kind of hardness is due to the presence of calcium carbonate (CaCOa) and occasionally, to a small extent, to iron and magnesium carbonates. As explained in the last section, these compounds are only soluble in water containing carbon dioxide (CO2), and since this gas is expelled when the water is boiled, they are WATEE AND ITS IMPUEITIES 71 deposited as solids after such expulsion, which chiefly accounts for the furring of pipes and vessels conveying hot water. The deposit, owing to its gradual formation in successive layers, is usually very hard and tenacious. Any other means by which carbon dioxide can be removed from water will naturally be equally efficacious in producing deposition which, while it has disadvantages when occurring in hot water systems, has at times to be resorted to in appropriate vessels for the purpose of softening the water. The cheapest and most effective means for softening, temporarily, hard water consists in adding to it quick or slaked lime, which combines with the carbon dioxide in solution forming calcium carbonate, which is itself deposited. Thus— Quicklime. Carbonate Dioxide. Cal. Carbonate. CaO + CO2 = CaCOa And after such withdrawal of the solvent, the "hardness" is removed by the inevitable deposition of the calcium carbonate originally present. Evidently the lime must be added in the proper proportion to just combine with the carbon dioxide present, which can be readily calculated from the above equation, every 44 parts by weight of the gas present requiring 56 parts of quicklime. The deposition of calcium carbonate in steam boilers is sometimes prevented by the addition to the water of sal ammoniac (NH4CI), which converts the insoluble carbonate into highly soluble calcium chloride, which remains in solution in the boiler, while the ammonium carbonate simultaneously formed is volatilised and carried off in the steam. The equation representing this reaction is — Am. Chloride. Cal. Carbonate. Am. Carbonate. Cal. Chloride. 2NH4CI + CaCOg = (NH4)2C03 + CaCla 72 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS Water treated in this manner is not, however, suitable for human consumption. A more satisfactory method of preventing scale depends upon the mechanical action of certain vegetable substances which when mixed with the water form a film upon the walls of the boiler to which scale will not adhere. 2. Permanent Hardness. — This term refers to the hardness of water due to the presence of calcium and magnesium compounds dissolved therein without the agency of carbon dioxide, and which are, therefore, unaffected by boiling the water or by the addition of lime. No means exist for the removal of permanent hardness the application of which is practicable on a large scale. Substances present in water, owing to its direct solvent action can only be completely removed by distillation, i.e., by boiling away the water and condensing the steam formed, a process much too costly for any but special purposes. The addition of certain compounds which can, by chemical action, convert the calcium and magnesium compounds present into insoluble bodies and thus withdraw them from the water, is used for domestic purposes. The most important of these is washing soda, the reaction of which with calcium sulphate is as follows : — Washing Soda. Cal. Sulphate. Cal. Carbonate. Sodium Sulphate. 1 NaaCOa + CaSO^ = CaCOg + . Na2S04 VI. Effects of Water on Materials. The nature and amount of the impurities contained in a given water have considerable bearing upon the choice and arrangement of the materials employed for its conveyance and use. ' Water of crystallisation, since it mixes with the water of the ^solution, need not be represented in actions between dissolved bodies. WATER AND ITS IMPURITIES 73 1. Scale in Pipes and Boilers. — The greatest deposition of scale in a hot water system will naturally take place where the inflowing water is first heated, for it will be here that most of the dissolved gas will be expelled, and hence this statement is particularly true for water possessing much temporary hardness. The flow pipe where it adjoins the boiler should, therefore, be of large dimensions and capable of replacement, while the bottom of the boiler especially should possess as continuous a surface, as free from sharp angles and corners, as possible. Scale is a very bad con- ductor ; hence, if allowed to form a coating of any thickness heat is prevented from readily passing through the boiler walls, which may even become red-hot, which will result in a serious loss of strength, and in the event of a flaw arising in the scale, will probably lead to fracture. The air dissolved in water will on expulsion oxidise the interior of boiler and pipes, and though these may be soon protected by the deposit of scale, the constant introduction of fresh water into a large service of piping may lead to sufficient internal rusting to produce marked discoloration of the water. The softer the water the more likely, of course, is such a result. From the above remarks it will be evident that the com- bination of hot water systems, both for warming a building and for domestic supply, must generally be undesirable. It is found that scale settles much less readily upon copper than upon iron. This may be partly due to the rough internal surface usually found in an iron pipe, but is probably also to be attributed to the greater difference in the co-eSicients of expansion of copper and scale than iron and scale, which, aided by changes of temperature, will prevent good adhesion. 2. Use of Lead Pipes and Cisterns. — The hardness of water is a great safeguard where lead is employed for its conveyance or storage, since the deposit of scale, even to 74 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS the slight extent to which it occurs in a cold water service, prevents oxidation and solution of the lead. Lead, as is well known, readily becomes covered with a film of oxide when exposed to a moist atmosphere, and the same effect is produced in water owing to the dissolved air which the water contains. Lead oxide dissolves in water, forming lead hydroxide, and since all soluble lead com- pounds are poisonous, and produce in small quantities a cumulative, and therefore particularly insidious, effect upon the human system, the slightest solution of lead must be guarded against. Soft waters are, therefore, particularly unsuited for con- veyance in lead pipes, and in water which contains ammonia, particularly in the presence of large quantities of nitrates (usually derived from decaying vegetation), the amount of lead dissolved is especially large. The formation of lead hydroxide takes place as follows : — Lead. Oxygen dissolved in Water. Lead Oxide. Pb + 0 = PbO PbO + H2O = PbOaHs lead hydroxide. Even in the absence of any deposit or protecting scale in the pipes, the presence of carbon dioxide in the hard water results in the formation of lead carbonate from the lead hydroxide first formed, and since this lead carbonate is insoluble it soon forms a protective coating. Lead Hydroxide. Lead Carbonate. PbOaHa + CO2 = PbCOa + H2O. VII. Analysis of Water. From the above discussion it will be evident that some knowledge of the amount and nature of the impurities contained in water is of considerable practical value. The WATEE AND ITS IMPUEITIES 75 methods whereby such information is obtained cannot be dealt with in these pages, for they involve a knowledge of analytical chemistry ; but the headings under which a chemical analysis is submitted may be briefly referred to in order that the reports of experts may be understood. These are usually as follows : Total Solids, Chlorine, Hardness, Free Ammonia, Albuminoid Ammonia, Nitrates and Nitrites, Poisonous Metals. 1. Total Solids. — Suspended matter (if any) is usually filtered off from the water and its amount ascertained by weighing the deposit on the filter when dried. The " total solids" comprise all dissolved substances, and are estimated by boiling away a known quantity of water and weighing the residue. 2. Chlorine is one of the constituents of salt, and hence by its determination the amount of salt present can be calculated^. It is estimated by adding to a given quantity of the water a solution of nitrate of silver of known strength when turbidity is produced, and increases until the whole of the salt has been acted upon, when its amount can be calculated from the amount of standard silver nitrate solution used. 3. Hardness. — This is estimated by finding out how much solution of soap of a given strength is required to make a lather with a given quantity of the water. In order that a lather may form, soap must freely dissolve, but when added to hard water soap immediately combines with the calcium and magnesium compounds present and is thus withdrawn. The amount of soap necessary to produce a lather, therefore, gives a measure of " hardness." 4. Ammonia and Nitrates. — These constituents from organic sources are determined by removal of ammonia as gas on distilling the water alone, and subsequently > Salt is NaCl (Na = 23, CI = 35|) ; therefore every 35| parts of chlorine found represent 58^ parts of salt. 76 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS with oxidising and with reducing agents, and observing the tint produced by the gas dissolved in water on the addition of a specially prepared reagent which is thereby turned yellow. 5. Poisonous Metals. — These usually comprise lead and copper, and should be entirely absent in all good waters. They are estimated by a colour test similar to the above. 6. Good and Bad Water. — Whether a water is to be con- sidered good or bad will naturally be largely dependent upon the use for which it is required. For domestic purposes the hardness and for consumption the organic matters are respectively the most important factors. A water which contained, say, five grains of hardness-pro- ducing compounds per gallon would be regarded as rela- tively soft. London water contains some fifteen grains per gallon, and waters supplied for use containing as much as thirty grains per gallon are known. Organically the albuminoid ammonia should certainly be less than one part in ten million parts of water, and the free ammonia in most cases much less. Lead and copper should be absent, and as regards the other constituents so much variation exists that it would not be wise to attempt any general statement. The study of actual analyses must be made for further information. One is given below to show the form often adopted in stating results. This water was reported upon as of high organic purity but exceedingly hard. Analysis of water from a spring in the Stebbing Koad, Essex, made October, 1895 : — Grains per gallon. Parts per million. Total solids . . 80-0 Free ammonia . . 0-001 Hardness (reckoned as Albuminoid ammonia 0-024 CaCOg) . . . 26-3 Nitrates and Nitrites Chlorine . . .1-3 (reckoned as HNOg) 11-9 CHAPTEE VIII SULPHUR AND THE NATURE OP ACIDS AND BASES I. Occurrence and Preparation of Sulphur. 1. Occurrence. — Sulphur is one of the few elements which are found naturally in an uncombined state; it also enters into the composition of many common substances. Volcanic districts, particularly that at the southern extremity of the Apennine Chain in Sicily, form the chief source of the element commercially. The formation of sulphur in such regions is probably due to the mutual decomposition of gaseous sulphur compounds ejected from the earth. Easily melted, the fine deposit of sulphur lodges among the warm rock and cinder in the neighbourhood of its formation and has become interstratified among the Tertiary beds of the district, in which it forms veins or basin-shaped deposits, whence it is quarried from open workings or mined like coal, but usually in a very primitive fashion. It is separated from the intermixed rock by stacking the collected fragments in kilns resembling lime kilns, and lighting the sulphur, when a small quantity burns and melts the rest, which flows out and is afterwards purified by distillation. In this manner the element is obtained in its familiar form as a yellow brittle solid, or if the condensation of the vapour is allowed to take place without subsequent melting, as a light yellow powder. 2. Properties of Sulphur. — Sulphur is exceedingly brittle and a very bad conductor of heat and electricity. In a molten condition it readily acts on all metals producing 78 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS sulphides, which, as far as their chemical constitution is concerned, much resemble the oxides. When heated, sulphur behaves in a remarkable manner. It melts at a temperature slightly higher than that of boil- ing water to a limpid liquid, but if further heated it becomes almost solid at about 230° C, and again liquefies at a still higher temperature, though it is then much darker in colour and more viscous. Finally it boils at about 444° C. If when the boiling point is approached the liquid is poured into water the solidified mass will be found to be quite plastic, but will, after an interval of a day or two, return to its original brittle condition. These changes are due to the breaking up of complex molecules into others containing smaller numbers of atoms, and are worthy of consideration when the element is melted for running joints or similar purposes. II. Sulphur Compounds. Some of the most important ores of such metals as lead, copper, and zinc are combinations of these metals with sulphur, and many other metals similarly combined are of wide distribution. Sulphur also occurs combined with metals and oxygen as sulphates, such as calcium and sodium sulphates, which have already been referred to. 1. Sulphides of Iron. — There are two naturally occurring sulphides of iron, both represented by the formula FeS2 through want of knowledge as to their molecular structure. One is called iron pyrites (pronounced py-ri-tees), the other marcasite. Both possess the yellow colour of sulphur and are also metallic in appearance, though the former is usually brighter owing to its lesser tendency to tarnish. Iron pyrites, unless in a fine state of division, is remarkably stable even in a moist atmosphere, but marcasite rapidly disintegrates, to the detriment of any materials which SULPHUE AND THE NATUEE OF ACIDS AND BASES 79 contain it. Both these minerals occur very commonly in many stones and slates, and in coal. When strongly heated in the air the sulphur from these compounds burns away, leaving eventually only iron oxide Fe203. 2. Sulphuric Acid. — When sulphur from such sources as the above, or as an element, burns in the air, a gas possessing the pungent smell characteristic of burning sulphur, known as sulphur dioxide (SO2), is produced. This gas is readily soluble in water and combines therewith to form a substance known as sulphurous acid, thus : — Sulphurous Acid. SO2 + H2O = H2SO3. Sulphurous acid has valuable bleaching properties and also arrests fermentation, but is not stable if exposed to the air, since it absorbs oxygen and is converted thereby into sulphuric acid, thus : — H2SO3 + 0 = H2SO4. This acid is the most important chemical substance manufactured, and about one million tons are produced annually in this country alone. It is used in the produc- tion of nearly all acids, to a decreasing extent in the manufacture of alkalis, in connection with artificial manures, the refining of petroleum, in dyeing and the preparation of dyes, in soap and paper manufacture, in electric cells, and in many other trades directly or indirectly. Its manufacture is carried out on the lines indicated above. The sulphur dioxide gas from burnt pyrites is led into very large leaden chambers and there mixed with steam and air, when the sulphuric acid produced falls to the bottom of the chamber with a large excess of condensed steam. This dilute acid is run off and the excess of water expelled by evaporation, when a heavy oily liquid containing 80 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS some 98 per cent, of H2SO4 remains. The concentrated acid is extremely corrosive, chiefly owing to its great tendency to absorb water, which extends even to the extraction of hydrogen and oxygen as water from bodies containing these elements. Nearly all animal and vegetable substances contain hydrogen and oxygen combined with carbon, hence the withdrawal of the two former elements from the carbon which is not acted upon, results in the charring of such substances by this acid. The heat evolved by the combination of sulphuric acid with water is very considerable, and therefore the dilution of the strong acid requires care and must be effected by slowly pouring the acid into an excess of water. Sulphuric acid has also, when mixed with water, a direct solvent action upon a very large number of substances. Most metals are attacked by it, all carbonates are readily decomposed by it, and many other chemical compounds and common substances yield to its action with greater or less rapidity. Pyrites occurs commonly in coal, which may be taken to contain on an average some 67 pounds of sulphur per ton. When coal is burnt sulphuric acid is finally produced owing to the oxidation of the sulphur dioxide in the moist atmo- sphere. The great consumption of coal in large towns renders the amount of sulphuric acid produced in this manner very considerable. In Greater London, for example, probably some 10,000,000 tons of coal are burnt annually, resulting in the production of some 300,000 tons of sulphuric acid, a large part of which descends in rain or fog upon the buildings which so recklessly emit it. 3. Sulphuretted Hydrogen. — When carbonaceous com- pounds which contain sulphur decompose in the absence of a free supply of air, part of the sulphur may combine with some of the hydrogen present in the substance to form a compound known as hydrogen sulphide, or sulphuretted SULPHUE AND THE NATUEE OF ACIDS AND BASES 81 hydrogen. This compound, a poisonous, inflammable gas, is characterised by a smell resembling that of rotten eggs, to the production of which gas in decomposing eggs this smell is, in fact, due. A small proportion of the sulphur contained in coal often finds its way into coal gas in this form, and has a ready action upon certain compounds of lead, producing lead sulphide, which is black. Sul- phuretted hydrogen when burnt is converted into sulphur dioxide and water, thus : — H2S+ 30 = H2O + SO2. In the presence of atmospheric moisture the sulphur di- oxide is converted into sulphuric acid, as already explained ; hence coal gas containing sulphur compounds exercises a deleterious effect upon the decorations and fittings of rooms in which it is used, even in the absence of any leakage. III. Other Common Mineral Acids. 1. Spirits of Salt. — If strong sulphuric acid is poured upon salt, dense white fumes possessing an irritating odour are produced. This evolved gas is known as hydrochloric acid, and results from an interchange of hydrogen in the sulphuric acid with the metal sodium in the salt. The completed reaction is as follows : — Salt. HydrocUoric Acid. 2 NaCl + H2SO4 = 2 HCl -f Na2S04. The gas is very soluble in water, one volume dissolving at ordinary temperatures some 500 volumes of gas, and the solution thus produced is known as spirits of salt or hydro- chloric acid. As sold it contains about 39 per cent, of the acid, the remainder being water. The action of this acid upon zinc, producing " soldering fluid," has already been referred to. The zinc chloride 82 CHEMISTET AND PHYSICS OF BUILDINa MATEEIAIS formed possesses great powers of absorbing oxygen, which enable it to decompose films of tarnish or oxide upon metals and thus allow solder to adhere. Like dilute sulphuric acid, hydrochloric acid readily dissolves many common substances, and on account of its solvent power upon lime and carbonate of lime it is useful in a diluted state for certain cleaning-down processes. Though it readily acts upon zinc and iron, hydrochloric acid has no action upon copper, though it dissolves copper oxide in common with most other oxides of the metals. ^ It thus forms a valuable and effective agent for cleaning copper, though it must not be used upon pewter or similar alloys. 2. Aqua Fortis. — If strong sulphuric acid is heated with nitre (saltpetre), yellow oily drops condense on the sides of the vessel, and if suitable means be taken to collect the liquid formed, as by distilling the mixture in a retort, a highly corrosive acid known as aqua fortis or nitric acid is obtained. The reaction may be represented as follows :— Nitre. Nitric Acid. 2KNO3 + H2SO4 = 2 HNO3 + K2SO4. Nitric acid is occasionally present in small quantities in the atmosphere, while nitrates, which may be looked upon as derivatives of the acid, have been referred to as existing in most natural waters. No ordinary metals withstand the corrosive action of nitric acid, and in a concentrated form it has been known to oxidise combustible substances with sufficient rapidity to set them on fire. IV. Acids, Bases, and Salts. The compounds above discussed have been termed " acids," and represent an important class of bodies which SULPHUE AND THE NATUEE OF ACIDS AND BASES 83 bear a relation to other classes of compounds, which in any study of the chemistry of materials it is essential to make clear. 1. Acids. — Popularly, an acid is regarded as a sour corrosive liquid, but acids can exist in other states. Hydro- chloric acid has been shown to be in reality a gas ; again, oxalic acid, tartaric acid, and many other bodies belonging to this class are solids. All acids have the power when in solution of changing the tint of certain vegetable matters, such as the juice of beetroot or an extract from lichens known as litmus, and these colour changes are used for detecting the presence of acid substances. Chemically, all acids contain hydrogen and have the power of nullifying or neutralising the properties of another class of bodies known as bases, which involves an exchange of hydrogen for some metal. The three best known mineral acids have been described above. 3. Bases. — These bodies may be defined as metallic oxides. Most bases are insoluble in water, and, therefore, have not the power of displaying such marked physical characters as are possessed by the acids. Those which dissolve, however, display properties which are the exact opposite of the properties possessed by acids. They are caustic or soapy to the touch, and restore the colour of vegetable tints altered by acids, or change such natural colours to different tints. Thus natural litmus is violet ; it is turned red by acids, and blue by soluble bases. Certain bases which possess the above characteristics in a very marked degree are called "alkalis." Such bases which concern this discussion are : Potash (K2O), Soda (Na20), and Lime (CaO). 3. Salts. — When an acid and a base are brought together, the one neutralises or destroys the characteristic properties of the other, and a new class of compounds which have G 2 84 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS neither corrosive nor caustic properties is produced. These compounds are known as Salts, inasmuch as ordinary common salt is one of the best known representatives of the class. In the action of acids upon bases, the hydrogen from the acid and the oxygen from the base always com- bine to form water, which is, therefore, the invariable product of such neutralisation. The following equations, showing the action of acids upon common bases, will make their relations clearer : — Base. Acid. Lime . . CaO + H2SO4 Soda . . Na20 + 2HC1 Lead oxide . PbO + H2CO3 PbO +H2Si03 CaO +H2Si08 Magnesium oxide . . MgO + 2HN03 Water. Salt. = H2O + CaSO^ (sulphate of lime). = H2O + 2NaCl (common salt). = H2O + PbCOs (carbonate of lead). = H2O + PbSiOs (silicate of lead). = H2O + CaSiOs (silicate of lime). =: H2O + Mg(N03)2 (nitrate of mag. nesia). By far the largest number of the compounds found in materials belong to the class of bodies called salts, which from their formation may be regarded as consisting of an acid part and of a basic part. Thus silicate of lime (CaSiOa) may be looked upon as composed of CaO, lime, and SiOa, which is silicic acid less water, formed as shown in the reaction given above. Since stability in most materials is generally best obtained by the use of such chemical reactions as shall pro- duce neutral compounds, i.e., salts, with neither base nor acid left over, an appreciation of the proportions of acids and bases necessary for such production is not without importance. It should always be remembered that the more unlike bodies are the greater will be their tendency to combine and the more stable will be the compound formed. Acids have no tendency to combine with acids, nor bases with bases, neither have salts with salts, though, of course, SULPHUR AND THE NATUEE OP ACIDS AND BASES 85 innumerable chemical actions take place in which an interchange of component parts of such bodies occur. 4. Acid-forming Oxides. — It sometimes happens that salts are formed without the intervention of any actual acid. Certain acids may be looked upon as consisting of a non-metallic oxide combined with water. Thus the solu- tion of carbon dioxide gas in water, known as carbonic acid and possessing the formula H2CO3, may be regarded as CO2.H2O, similar silicic acid H2Si03, may be written Si02.H20. Oxides such as these are known as acid-forming oxides, and can themselves combine with bases directly to form salts. The equations for such reactions are similar to those previously cited, with the omission of water. Thus : — Base. Acid-forming Salt. Oxide. Potash . K2O -f- CO2 = K2CO3 (potassium carbonate). Lime . CaO + CO2 = CaCOg (calcium carbonate). CaO -1- Si02 = CaSiOa (calcium silicate). Zinc oxide ZnO + SO3 = ZnSO^ (zinc sulphate). CaO + AI2O3 = CaAl204 (calcium aluminate). It may be objected that in the last example AI2O3 (aluminium oxide) is the oxide of a metal, and, therefore, a base. This is true in many reactions, but in the presence of strong bases, namely, the alkalis (potash, soda, and lime), it acts like an acid-forming oxide. In the clays combined with silica it is found acting as a base, but in limes and cements always as an acid. There is only one other oxide of importance— oxide of iron — which has the power of acting in this dual capacity, according to circumstances. CHAPTER IX COAL AND ITS PRODUCTS I. Coal. 1. Introductory. — The wide occurrence of the element carbon as an essential constituent of all animal and vegetable matter, and its existence combined with oxygen in certain minerals, such as limestone, have been already referred to. The greatest mineral supplies of carbon are found in coal, and the importance of this substance as the commercial source of all forms of energy, apart from the immense number of compounds derived from its distillation, render some account of its nature desirable. Coal is the result of the partial decay of vegetation under conditions admitting of but little oxidation : that is, it is the result of decay out of contact with the air, by a process analogous to the formation of peat at the present day. Coal occurs in one definite geological formation, and was formed under sub-tropical conditions of climate which the luxuriant character of its plant remains show to have then existed. Since thousands of feet of rock have been formed over the coal deposits, and since earth movements have produced great heat and pressure in some coal areas while affecting others comparatively little, not only is it to be expected that coal will differ in chemical composition from the original woody substances from which it is formed, but also that it will possess different characters and com- position in different localities. 2. Varieties of Coal. — The two most important varieties of coal are anthracite, which forms the greater part of the COAL AND ITS PEODUCTS 87 large fields of South Wales, and bituminous coal charac- teristic of the Newcastle and Midland coalfields. The former contains but little gaseous matter, and is composed almost entirely of carbon, while the latter often possesses sufficient volatile matter to make it cake on burning, owing to the distillation of tarry products. Anthracite, since it gives, on burning, an intense heat and but little flame, is used for raising steam and similar purposes, and is also known as steam coal; while bituminous coal is used for ordinary domestic purposes and for making gas. A third variety, known as cannel coal (the name is a corruption of "candle"), is found in irregular and more local masses. It resembles jet in appearance, and owing to the large amount of gaseous matter it yields it is used for enriching coal gas, the luminosity of which, when consumed without the use of mantles, it much improves. In later geological formations a carbonaceous substance, known as lignite (or in Germany as brown coal), is also found, which may be looked upon as a link between true coal and peat, since it partakes of the characters of both. 3. Composition of Coal.— The main constituents of coal are carbon, oxygen and hydrogen, and the effect of the two latter elements in determining the characters described above is well exemplified by the following table, showing the proportion of oxygen and hydrogen present to every 100 parts of carbon : — Carbon. Hydrogen. Oxygen. Wood Peat Lignite .... Bituminous coal . Anthracite .... 100 100 100 100 100 1218 9-85 8-37 6-12 2-84 8307 55-67 42-42 21-23 1-74 (Percy). 88 CHEMISTEY AND PHYSICS OP BtTILBlNG MATEEIALS When burnt, coal always leaves a certain amount of mineral ash, as would be expected from the method of its formation. It also as a rule contains some nitrogen and sulphur, the latter generally in the form of iron pyrites. In illustration of more complete analyses of coal two examples are appended : — Sp. Gravity. Carbon. Hydro- gen. Oxygen. Nitro- gen. Sulphur. Water. Ash. Bituminous 1-28 78-6 5-3 12-9 1-8 0-4 11-3 10 (Stafford- shire) Anthracite 1-39 90-4 3-3 2-9 0-8 0-9 2-0 1-6 (S. Wales) (Eoscoe). It should be stated that the amount of ash, which consists chiefly of silica and alumina, is often much greater than that shown in the above analyses ; indeed, ten per cent, of ash is by no means uncommon. 4. Uses. — Some 200 million tons of coal (a rapidly increas- ing quantity) are now annually raised in Britain, and a very large proportion of this is converted into coke, specially for blast furnace use in the iron and steel industry. A much smaller quantity undergoes a similar conversion, but with greater regard to the preservation of the volatile products liberated, in the manufacture of coal gas. II. Distillation op Coal. For the preparation of coal gas, coal is heated in long tubular retorts attached to a large pipe partially filled with water in which most of the condensable volatile products are retained. The gases evolved pass on and are further purified from vapours condensed on cooling, and from sulphur compounds by passage over lime. Coal and its peoducts 89 1. Coal G-as. — The gas finally obtained is a mixture the composition of which varies not only with the kind of coal employed, but with the temperature at which the distillation has been ejBfected. Its usual composition is, by volume, somewhat as follows : Hydrogen 50 per cent., methane, or marsh gas, CH4, 35 per cent., carbon monoxide 5 per cent., olefines (compounds of carbon and hydrogen, such as ethylene C2H4) 5 per cent. The remaining 5 per cent, is made up of nitrogen, carbon dioxide, and many other gases in small quantities. To the presence of hydrogen and methane coal gas owes its lightness, to the carbon monoxide its poisonous proper- ties, and to the olefines its illuminating properties when burnt in the ordinary way. 2. Coal Tar. — The tar which collects under the water in the pipe to which the gas retorts are connected is itself distilled and yields many valuable products. This dis- tillation is effected in retorts, and each fraction of the liquid, which passes over between certain temperatures, is collected separately. This process is known as " fractional distillation," and when this vaporising and condensing process involves the splitting up of a liquid into new substances, the process is known as " destructive distillation." The liquid which passes over when the tar is heated to about 105° C. is known as " first runnings," and consists mainly of water, crude naphtha, and ammonia. When the temperature of the tar rises beyond 105° C. the distillate is separately collected until 210° C. is reached, and this frac- tion, known as "light oils," yields principally naphtha. From 210 to 240° C. "carbolic oils " come over, from which carbolic acid is obtained, and from 240 to 270° C. " creosote oils," which form a valuable preservative for timber, and from which naphthaline is also extracted. Finally " anthra- cene oils " are obtained, from which many valuable coal tar 90 CHEMISTRY AND PHYSICS OP BUILDING MATERIAI.S dyes are manufactured, and the distillation is stopped at 380° C. The substance left in the retort at the end of this process is known as "coal tar pitch." It is sometimes used for adulterating asphalte ; its more legitimate purposes for employment are for making up coal dust briquettes and for preparing cheap varnishes. 3. Coke. — After all volatile matter has been extracted from coal, coke remains in the gas retorts, and in this coke the mineral ash of the coal naturally exists. This residue from gas manufacture is used as a domestic fuel, but coke is also specially prepared from coal on a large scale in coking ovens, as fuel for blast furnaces used in the manufacture of iron and steel. III. Carbon and the Oxides of Carbon. Apart from mineral ash, coke is pure carbon, which is the final product when any animal or vegetable substance is heated out of contact with the air. 1. Charcoal. — When wood is thus heated, the soft highly porous form of carbon which results is known as charcoal. It is used as a fuel for certain purposes. Charcoal acts as a powerful oxidiser, and is often used in this capacity for removing organic impurities from water. This is owing to the intimate contact brought about between the air contained in its pores and the water passing through it. It is necessary that charcoal thus employed should be periodically ridded of accumulated matters by thorough immersion in boiling water. 2. Lamp Black. — Soot obtained by allowing oil lamps to smoke, is, when freed from oily matters which volatilize in the process, a very pure form of carbon, and is known as Lamp Black, it is used for making black paints and certain oil inks. Bone black and ivory black, prepared by COAL AND ITS PEODUCTS 91 charring bones and ivory, though they contain large quantities of mineral matter, are put to similar uses. 3. Graphite. — The mineral graphite, also known as black lead and plumbago, is another form of carbon, and is formed artificially in certain processes. Most of the carbon con- tained in grey cast iron, for example, exists in the form of graphite. From the above description of the forms of carbon it will be seen that this element can display many physical differ- ences. The most striking of these is found in the diamond, which is the purest form of natural carbon known. None of the forms of the element have ever been melted, though evidence exists that carbon would melt at about 4,400° C. were any means known for attaining such a temperature. 4. Carbon Dioxide. — All forms of carbon, when heated in air or oxygen, burn with the formation of carbon dioxide gas, about which compound much has already been said. This gas is some two-and-a-half times as heavy as air, and as a product of combustion it neither burns nor sup- ports combustion. When found in vitiated air, the expan- sion which it has undergone prevents it from settling at low levels, but when produced in sewers or wells in situations in which it is neither heated nor disturbed, it may accumulate in a layer of quite definite depth. When its presence is suspected a naked light should be lowered into the cavity, and if this is extinguished respira- tion is not to be attempted until the gas has been pumped out or removed by lowering into it some hot body large enough to cause sufficient expansion to enable the gas to rise through the air above. Carbon dioxide is not only obtainable from animal and vegetable sources. All carbonates are decomposed with the liberation of this gas when acted upon by acids, and this fact provides a useful means for the recognition of carbonates. 92 CHEMISTEY ANi> PHYSICS OF BUILDING MATEEIALS e.g., carbonate of lime, and for the preparation of the gas for compression or carbonating processes. This action, in the case of carbonate of lime and hydro- chloric acid, is as follows : — Calcium Carbonate of lime. HydrocUoric acid. chloride. CaCOs + 2 HCl = CaCla + CO^ +H,0 A few drops of dilute acid placed upon a carbonate will produce effervescence, and since no materials of a stony nature effervesce with acids from any other cause, the fact furnishes a simple and readily applied test for distin- guishing limestones and marbles from siliceous stones and for detecting carbonates in granites and slates, where their presence generally indicates decay. 5. Carl)on Monoxide. — When carbon burns in a limited supply of air or whenever it has to obtain its oxygen for combustion by the decomposition of some other compound, it only partially burns. The gas formed in such cases is known as carbon monoxide, and has the formula CO. This compound, as stated, is present in coal gas and is very poisonous, its action in this respect amounting to physiological suffocation, since it absorbs oxygen from the blood. Carbon monoxide burns with an exceedingly hot flame, and is the chief component of " producer gas " and similar gaseous fuels. The lambent blue flame often seen over a red fire is due to this gas, which undergoes combustion thus : — CO + 0 = CO2. CHAPTER X OUTLINES OF GEOLOGY I. Earth History. 1. Introductory. — Just as a knowledge of the properties of manufactured materials involves some acquaintance with the methods adopted in their production, so a knowledge of natural materials necessitates some insight into the methods of Nature's workshop. Such an inquiry into the arrangement and structure of the accessible materials of which the earth is made, and the elucidation of the history of their bringing together, form the work of the geologist. There is strong presumptive evidence that the earth some millions of years ago was a molten mass and that its solidification has been a very gradual process. The universal rise in temperature observed in deep mines, and the existence of hot springs and volcanic outbursts in widely separated districts, is evidence that the earth's interior is hot,^ and as this heat is radiated into space and is not returned, a general cooling must be in progress. It has been pointed out that most bodies contract on solidifying and cooling, and as the earth is not a perfectly rigid body this process is accompanied by a wrinkling of its surface, and often also by cracks and sudden subsidences. * Some new hypotheses suggesting that radium may be an impor- tant factor in the earth's internal heat will be found in reports of the British Association meeting of 1908. 94 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS 2. Erosion. — When the earth's exterior first fell below 100° C. surface depressions formed settling grounds for condensed water, and with the presence of liquid water a ceaseless wear and tear of material was initiated. Pulled out of shape by the sun and the moon's attraction, and lagging behind the earth in its rapid rotation, this water, which now forms the oceans, is in constant motion and dashes itself against its shore lines in its ebb and flow. Evaporated by the sun and again condensed in the cool air, it descends as rain and finds its way, charged with soluble and eroded matters, back to the ocean along spring and river courses carved by its own efforts. The changing seasons, the heat and cold of day and night, the winds produced by varying temperatures and the earth's rotation, all exercise a wearing effect upon the earth's crust. The exposed rocks split by heat or frost, the wind-borne cloud bursting upon the land and washing it away to expose fresh surfaces, even the forms of life themselves, the growing roots of plants, and the teeming microbes of the soil, all aid in this constant breaking down of material and produce a ceaseless wear and tear. If these changes are not very apparent, it must be remembered that in dealing with the earth's history vast lapses of time are in question, periods compared with which the length of human history is as nothing. But the erosion of the earth even in short intervals is by no means inappreciable, in proof of which it may be cited that the solid matter carried to the sea by such a river as the Mississippi is sufficient in a single week to raise an area of a square mile more than five feet in height. 3. Deposition. — The result of this constant deposition of eroded material is seen in the formation of river deltas. Gravel, sand and mud thus slowly deposited form new land surfaces, and such materials are arranged in layers or strata, and as these deposits accumulate the lower layers become compressed and hardened. This investigation of OUTLINES OF GEOLOGY 95 Nature's present processes, which there is every reason to believe have gone on continuously since the earth possessed a cool solid surface, gives the key to the formation of the rocky strata which form the crust of the earth at the present time. This eroding power of water, or more correctly the erosion of rock particles one against the other through the agency of water, is not, however, alone sufficient to account for the vast thicknesses of strata known to geologists. Obviously the accumulation of sediment in the manner described must cease when the deposits reach the surface of the water in which such deposition occurs. The land and the ocean bed, however, are constantly subjected to slow but continuous motions of upheaval and depression, producing effects which may be quite marked within human remembrance. If examples are wanted, the change in the coast lines near such places as Blackpool and Cromer will give striking proof of the truth of this assertion. If subsidence, then, takes place as fast as the deposition of eroded matter pro- ceeds, deposits thousands of feet in thickness may in time be formed. As soon as these accumulations reach the sur- face of the water, which may be due to continued deposition of sediment or to some reversal of earth movement con- verting depression into upheaval, the eroding action of the forces of Nature at once recommences. Streams and rivers again in process of time carve out their courses and the very valleys through which they flow, and frost, wind and tide join in the attack upon the new land areas. Thus an endless cycle of operations involving destruction and rebuilding is ever in progress. The slowness of these changes, however, enables the geologist to investigate the various strata and to study their present characters and geographical limits without any fear that his landmarks will be seriously interfered with, and this study is of great economic value. 96 CHEMISTEY AND PHYSICS OF BUILDING MATERIAIiS II. Arrangement of Strata. 1, Layers Not Continuous. — It might appear at first sight that the various deposits would lie horizontally one over the other, perhaps occasionally thinning out against some older land surface where a deposit was of a limited and local nature. Thus the land might be expected to be built up of more or less continuous horizontal layers, the uppermost representing the final deposit. This is, however, by no means the case. In one district limestones are found ; in others, slates, chalk or sandstones, all of obviously different origin and age ; and further, if such beds of rock are examined they will in many cases be found to lie in positions so much removed from horizontality that it would have been quite impossible for their formation to have taken place at such inclinations. 2. Dip. — There is little doubt that such strata were originally deposited in approximately horizontal layers, but the great earth movements, already referred to, resulting in wrinkles and dislocations in the earth's crust, have subsequently displaced these strata and tilted them, and actual fracture, or more generally subsequent erosion, has thus exposed the strata once buried thousands of feet below the surface. This is illustrated in Fig. 2, where A shows the original beds as formed by deposition, B their possible upheaval due to earth movement, and C the surface exposure of the beds due to subsequent erosion. The angle which the general planes of deposition or "bedding" make with a horizontal plane is known as the dip of such strata, and the determination of this angle is obviously of great importance to the miner and quarryman. Strata are occasionally much contorted and broken, but apart from local and always recognisable exceptions, deposits are invariably found to lie one upon the other in the order in which they were originally laid down, that is to OUTLINES OF GEOLOGY 97 say, the oldest rocks ^ are the undermost, and are regularly succeeded by those of later date. Dip and subsequent erosion resulting in the exposure of once buried deposits are of great value to the geologist, for were all deposits found in their original horizontal position o/i/a/m si/pmce /7 Fig. 2. — Explanation of irregular appearance of strata on the earth's surface. vertical borings could alone procure information as to the strata below the earth's surface, whereas under existing conditions, by measurement of the extent of the exposed 1 The geologist uses the term " rock " not only as popularly applied but as indicative of any deposit, such as a bed of clay or gravel, and the word is so used in these chapters. B.M. H 98 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS edges of the deposits and then making allowance for the dip, the thickness of the strata can be ascertained directly, while their characters on a large scale can be investigated on the earth's surface, as will be apparent from a study of Fig. 3. Fig. 3. — Measurement of dip or inclination of strata from surface exposure. 3. Faults. — Strata are not only bent and eroded, but often actually broken, and this usually results in considerable change of level between the separated portions. Erosion may then remove the beds on the higher side of the frac- ture, or subsequent deposition may introduce new deposits upon the beds on the lower side. These dislocations are known as faults, and may be displayed as small local dis- turbances or extend over many miles. A study of Fig. 4 will make it evident that faults may have a considerable bearing upon the quarrying of stone. A here shows the condition of the beds after dislocation, and B the section of the same beds after erosion. It will be observed that the building stone, which, from an examination of the beds on the left, might have been expected to be continuous, has disappeared on the right of the fault owing to erosion. A consideration of the above facts will make it evident that, although a certain deposit may originally have covered a wide area, it does not necessarily follow that it will always have a present existence over the whole of such area. OUTLINES OF GEOLOGY 99 Many upheavals and submergences of the land, and many wrinklings and breakages, have taken place during the formation of the great series of rocks which form the earth's outer crust, and in places exposure to erosion has continued sufficiently long to admit of the removal of the ElG. 4. — Eaults or dislocations in strata, showing how a building stone may suddenly terminate against worthless materials. whole of certain deposits, with a corresponding lack of con- tinuity in beds subsequently formed upon such eroded areas. III. Identification op Stkata. 1. Physical and Biological Characters. — On recalling the general characters of the land surface as now existing, laid out as most of it is in the service of agriculture, or for H 2 100 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS human habitation, it might appear hopeless to endeavour to trace the geological strata and identify the various beds in different places. It must be remembered, however, that the surface soil, which consists of the disintegrated beds below it mixed with the remains of decayed vegetation, is very superficial in character, usually not exceeding a depth of two or three feet, while in many places the natural rocky stratum is actually exposed. Aided by such exposures and natural sections obtained on cliffs and in quarries and by well-sinkings, geological maps have been constructed representing the country denuded of its superficial soil and artificial excrescences. Further, by noting where certain beds disappear beneath the surface and where they again reappear, and the angle at which they dip, tolerably accurate sections can be produced showing the form of the vertical exposure which would be obtained were the country cut into two between different points. It is true that the physical characters of a given layer of stratum often show considerable variation in different places, particularly in the case of gravelly beds formed in ancient river estuaries, while, again, subsequent local earth movements may have further modified their characteristics ; on the other hand, strata which have been formed in deep water, as for instance chalk, are very constant in their general characters and appear- ance, even in widely-separated districts. The geologist, however, possesses a most important aid to the identifica- tion of his deposits in the existence of the remains of plant and animal life found in them. These life remains are termed fossils, and their value lies in the fact that many of them are characteristic of the beds in which they occur. The fossils, again, differ in organisation : some have evi- dently a marine origin ; others, as proved by similar existing species, lived in fresh water ; and this offers a further means of distinguishing the surrounding strata. The oldest rocks contain only simple forms of life, later fishes are found, OUTLINES OF GEOLOGY 101 hen luxuriant plant life, reptiles, higher forms of shell fishes, then in more recent deposits mammals and birds, and quite in the latest beds remains of man himself occur. The whole series of formations thus exhibits the wonderful process of gradual evolution. 2. Names and Order of Strata. — Geologists have found it possible, by utilising the means of identification described, to classify and arrange the layers of the earth's crust in a tabular form in the order of their deposition — the main divisions of which are known as formations. The chief members of this table, arranged in descending order — that is, headed by the latest deposits — and the more important economic products derived from these layers, are appended (pages 102 and 103). Aided by such a table, geological maps showing in what part of the country the various strata are exposed may obviously be studied with advantage. IV. EOCKS NOT FOBMED UNDER WaTER. Although the preceding description has accounted for the formation of by far the greater part of the earth's crust, but little consideration is required to show that some of the rocks found in this country and elsewhere cannot be regarded as having been laid down under water by gradual deposition. Granite, for example, and rocks allied thereto, present no planes of bedding or stratification, contain no remains of animal life, and are found to occur in irregular masses, breaking through the water-formed strata, to which they bear no relation either in character or position. These rocks might represent the original and once molten crust of the earth, and such an origin has indeed been attributed to granite rocks in certain districts, as that of Malvern, in this country ; but their occurrence among strata of all ages calls for some wider explanation of their existence. The resemblance of these irfiegulsw: masses to rocks erupted 102 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS - CD 5^ ^ Q o o ^ CO CO ?-i a cS 3 ^ CO X • rt S CO >H o) a (In CO --s O) S =3 O g 0 o o 00 s o o -a Is < >i £3 § ? d o D CO O O OUTLINES OF GEOLOG-Y 103 pi o O o i rid 43 d 2 1-1 Ph >5 O 173 O! 02 " 5 g » <1 ^ rd S 5 O 5> ^ ^ oCd M « »H n3 O CQ 1 104 OHEMISTEY AND PHYSICS OF BUILDING MATEEIALS from or found solidified beneath ancient volcanoes leaves little room for doubt that they were similarly once molten, and were either poured out upon the land surface, or cooled very slowly, and gradually solidified and crystallised beneath the surface, which has been subsequently eroded away, and this has resulted in their exposure. Eocks possessing such an origin are known as igneous rocks. V. Conclusion. From this brief introduction to geology it will be evident that the value of this branch of science is not confined to mere localisation of surface exposures, but extends to actual predictions as to the extent of strata underground. In mining operations, in the search for coal, building- stones, and indeed any material characteristic of any given beds, a knowledge of the principles of geology is indis- pensable. For example, the dip or inclination of a bed of freestone must obviously have a direct bearing upon the quarrying and market price of such stone, and a slight variation in dip may easily convert an open quarry into a costly working underground. The investigation of faults, again, is of great importance, for if beds to be worked end abruptly against valueless rocks owing to dislocations, quarrying must necessarily cease in the working thus affected. The nature of the soil, and thus its suitability for agri- cultural products, depends largely upon the strata imme- diately beneath it. The rich plain land, the barren moor, the rounded chalk hill, all owe their characteristics to the rocks below them, while the desirability of a site for building purposes, the nature of the foundation requisite, and the quantity and character of water likely to be obtained thereon, are all matters ultimately connected with the study of geology. PAET II— BUILDING MATEEIALS INTEODUCTION In this section of the book it is proposed to deal with the applications of the foregoing principles to the materials used in building. In discussing so wide a subject wherein each class of product may form the basis for a small library of text- books, it is obviously impossible to do more than generalise on broad lines within the limits of what is essentially meant to be a small and readily assimilated work. Thus the object which will be kept in view is not that of enabling a mastery of the properties and means of identification of any individual stone, brick, or piece of timber, to be acquired, so much as to point out chemical and physical characteristics of these bodies as classes of materials, and to indicate from a consideration of the history of their formation, natural or artificial, and of the conditions surrounding their use, the nature and value of their structure, and of the tests whereby their properties may be assessed. For this reason accounts of manufacturing processes and manipulatory and statistical details of tests have been reduced as far as an intelligible presentation of the subject will allow. All these matters are readily accessible in many excellent text-books dealing with individual sub- stances, and it is by the further study of such books and 106 CHEMISTRY AND PHYSIOS OF BUILDING MATERIALS of the materials themselves in actual use, that a com- plete knowledge of their practical value can alone be acquired. If these few pages serve to show how such further study may be profitably undertaken, they will amply fulfil their intended purpose. Arrangement of Subjbct-Matter. This section of the book will be found divided up into chapters dealing with materials as ordinarily classified as Stones, Brick Clays, Limes and Cements, Metals, Timber and Paints ; but since the first three of these groups contain, or are derived from, a comparatively small number of com- pounds which occur naturally in the form of minerals, a general account of such minerals and the means employed for their identification will form the initial chapter, after which some account of the natural occurrence or pre- parative principles, properties and composition, tests upon, classification of, and defects arising in, the groups above cited, will be dealt with. CHAPTEK XI THE CONSTITUENTS OF STONES, CLAYS AND CEMENTING MATERIALS I. Mineral Constituents and their Characters. 1. Composition of Natnral Materials. — All the natural mineral materials employed in building — stones and slates, brick-clays, limes and similar substances — although they differ much in origin, physical structure and minor con- stituents, consist essentially of a comparatively small number of bases combined with an equally small number of acid-forming oxides. These bases are : potash (K2O), soda (Na20), lime (CaO), magnesia (MgO) , and the acid oxides are alumina ( AI2O3) and ferra^ (FeaOa) (which in the absence of the above bases act as bases themselves), silica (Si02) present alone or in silicates, carbon dioxide (CO2) in carbonates, sulphur trioxide (SO3) in sulphates. 2. Minerals defined. — The above acids and bases (generally in combination as salts), which constitute natural materials, are found as isolated chemical compounds, or, more usually, as several compounds mixed together. Such naturally occurring compounds are known as minerals.^ 1 The writer has ventured to coin the word " ferra," which is analogous to and consistent with the common designation of other oxides. The term oxide of iron, by which FcqOs is usually known, besides breaking up terminological continuity, is not always sufl&ciently definite, as there are several compounds of iron and oxygen. The name ferra will be confined to Fe^Og, and the oxide FeO will be referred to by its ordinary chemical name as ferrous oxide. ^ Minerals need not be compounds ; e.g., sulphur and gold are minerals, but no elements found naturally concern the present discussion. 108 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS Although minerals are thus defined as chemical com- pounds, from the nature of their formation it is hardly to be expected that they will be found in materials in a state of absolute purity. Small quantities of impurities are often mechanically included within them, and again, chemical reactions sometimes lead to the partial replacement of one base by another, resulting in groups of compounds somewhat difficult to define individually, and conveniently referred to under one designation, which is particularly the case with mineral silicates. Notwithstanding this, most minerals possess distinctive and definite properties whereby they may be recognised, as, for example, quartz and mica in granite. Some of these characteristics will now be referred to. 3. Characters of Minerals. — {a) Regularity of Shape. — The molecules of most compounds tend to arrange themselves in a regular manner when they can come together freely and they "grow" by the addition of successive layers derived from dissolved or melted material, and under favourable circumstances produce masses which have flat faces separated by definite angles. Such growths are known as " crystals," a term which is used quite irrespective of glassy appearance or transparency; for example, the yellow metallic mineral iron-pyrites and black opaque oxide of iron are found as crystals. Owing to the restrictions of surrounding bodies it is but seldom that characteristic crystal forms can be distinguished in building materials, but mere evidence of an attempt on the part of a mineral to crystallise as shown by the sparkling under light of a fractured surface, is of value, since crystalline materials have much more stability than those possessing an earthy structure. Marble and chalk, for example, are both composed of carbonate of lime, and the superior weathering power of marble is entirely due to its crystalline structure. (h) Cleavage. — Cleavage is the property in virtue of STONES, CLAYS AND CEMENTINa MATEEIALS 109 which bodies split along certain planes, and owes its origin to molecule arrangement. Slates and some stones possess this property, which is developed to a remarkable degree in such a mineral as mica. Cleavage takes places in minerals along definite planes, and often in more than one direction. Crystallised carbonate of lime can be readily distinguished from quartz by its cleavage, since the latter mineral does not cleave but breaks with an irregular fracture like a piece of glass. (c) Hardness. — The ease with which a mineral can be scratched forms a useful means of estabHshing its identity. In order to make comparisons of hardness, a scale has been agreed upon represented by minerals numbered from 1 to 10 in increasing order of hardness. These minerals are as follows : — 1 talc, 2 selenite, 3 calcite, 4 fluorspar, 5 apatite, 6 felspar, 7 quartz, 8 topaz, 9 corundum, 10 diamond. The statement, then, that the hardness of a mineral is, for example, 7, means that it has the hardness of quartz ; thus it will be scratched by a fragment of topaz but will itself scratch felspar. (d) Streak— T}he true colours of many minerals are often masked by surface oxidation, but may be revealed by scratching through the external layers with a pen- knife or any harder mineral fragment. The colour presented by the scratch is known as the streak of the mineral, and often aids identification. (e) Other Physical Properties. — Further distinctions lie in differences in specific gravity, colour, appearance (whether earthy, glassy, or metallic), and in differences of crystalline form, which study is a special branch of mineralogical science known as crystallography. (/) Chemical Analysis. — The ultimate composition of minerals as ascertained by chemical analysis gives a means of identification which requires the services of a chemical expert. Some account of the objects to be aimed at by llO CHEMISTRY AND PHYSIOS OF BUILDING MATERIALS such analyses and of a few simple tests for certain constituents will be found in subsequent pages. II. Use of the Miceoscopb in Examining Materials. 1. Principles of Construction. — The microscope provides such a rapid and effective means of obtaining an insight into the mineral and structural character of many materials that a short description of its use may profitably be given. When an object is viewed through any transparent sub- stance possessing curved faces — a lens — it appears altered in size. The rays of light from the object falling on the lens are bent in their passage through its substance, and if the surface is convex these rays converge to a point on the opposite side of the lens and subsequently diverge and form an image of the object at a definite position. If the matter be investigated by holding different " reading glasses " between a lighted candle and a vertical sheet of paper in a darkened room it will be observed that the size and clearness of the image of the flame formed upon the paper depends upon the distances of the candle and paper from the glass and upon the amount of curvature on the faces of the latter. In a microscope an image of the object to be examined is formed by a small lens at the bottom of the instru- ment, known as the " objective," and this image, which is produced in the tube of the microscope, is observed through another lens at the top, called the " eye-piece," which increases the magnification due to the objective in the same way as a simple image of a candle flame on a sheet of paper might be magnified by observing it through another lens held between this image and the eye. The position of the objective and eye-piece are adjustable by means of sliding tubes or rack and pinion motion to STONES, CLAYS AND CEMENTING MATEEIALS 111 admit of the use of different lenses and to allow for different foci of vision. The object to be viewed is placed on what is known as the " stage " of the instrument, which is perforated to allow a strong light, necessary to produce an enlarged image of sufficient brightness, to be thrown upon it from a mirror, sometimes supplied with a concentrating lens of its own below, or if the object is opaque arrangements must be made for throwing light on its upper surface and causing this to be reflected up to the objective. 2. Use of Polarised Light. — A valuable adjunct to a petrological (rock investigating) microscope consists of two specially constructed prisms known as " Nicols prisms," which are suitably mounted in frames, one below the object viewed, the other in the tube of the instrument above the objective. These prisms are capable of rotation about the axis of the tube of the microscope, and have the effect of filtering out the light so that instead of passing through the object and lenses in a bundle of rays, it is restricted to one plane, and is then said to be " polarised." If one of the prisms is rotated so that the plane along which it transmits light is at right angles to that for the other prism, all light will be cut off from the eye-piece and hence from the observer. It is found, however, that certain transparent minerals, if placed on the stage of the instrument, have the effect of allowing some light to pass when the prisms are placed with their transmitting planes at right angles as described, or, in scientific language, "between crossed Nicols." Further, when fragments of certain minerals so placed are rotated on the stage the colour of the light transmitted shows dis- tinct changes in tint, and minerals which possess this property are said to be dichroic (two-coloured) or to exhibit dichroism. It is obvious that a knowledge of these facts must be of 112 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS value in aiding identification. For example, a certain kind of mica often present in granite, and which does not weather very well, is strongly dichroic ; if, therefore, a thin section of the granite, mounted for convenience on a strip of glass, be rotated under polarised light, such change of colour in certain parts of the "field," i.e., the magnified image observed, may indicate the presence of this mineral. III. Individual Minerals connected with Materials. A short description will now be given of the chief minerals which compose the materials now under con- sideration. It will be found most convenient to classify these bodies according to their chemical composition, except in the case of the silicates, where each mineral will be dealt with separately. 1. Silica (Si02). — Forming as it does more than one half of the entire crust of the earth, silica is of immense importance, and not only do many sandstones consist almost entirely of this compound, but in combination with bases in the form of silicates (salts, described at the end of this chapter), it has a very wide distribution in such bodies as granitic rocks, clays, and slates. Silica, besides occurring in rounded or angular grains in sand and sandstone, is found associated with many minerals in rocks and metallic ores, as quartz. In this form it is sometimes milky in appearance, or coloured owing to the presence of oxides of iron or manganese, but generally, as in granites, it is glassy and colourless. Under favourable circumstances it forms six-sided, prismatic crystals with pointed pyramidal ends, as found in certain Cornish granitic stones. Common flint is a form of silica particularly associated with the chalk formation, while agate, jasper, and opal (the last containing water) are other less common varieties of the compound. STONES, CLAYS AND CEMENTINa MATEEIALS 113 Silica is exceedingly infusible and has a small co-efficient of expansion. When specially prepared from a molten condi- tion it stands sudden changes of temperature remarkably well, and is likely to replace glass for many special purposes. The absence of cleavage and the hardness (7) of mineral silica form useful characteristics for identification. Since the hardness of ordinary steel is below 7, quartz (or sand grains) cannot be scratched by a penknife. The specific gravity of silica is about 2" 6. It is insoluble in all ordinary acids and hence exceedingly durable. It, however, dissolves in alkaline solutions, combining readily with such bases as soda and potash. This solution is of importance and explains the formation of many silicate minerals. Quartz generally occurs in stones of the granite class as a transparent infilling between other minerals and shows no regularity of outline in rock sections viewed under the microscope. With high power objectives numerous minute inclusions arranged along definite planes may often be observed in transparent fragments. 2. Calcium Carbonate (CaCOa). — This compound is also very widely distributed and is known in several mineral forms. In a crystallised condition it occurs as calcite or calc-spar, commonly found in limestone districts. In this form it is usually white or colourless, and possesses a pearly lustre. Its excellent cleavage in two directions and its hardness (only 3) render it easily distinguishable from quartz. Its specific gravity is about 2*7. Other forms of calcium carbonate are marble, which shows a distinctly crystalline structure ; chalk, which is the remains of shell fragments, and is generally soft and amorphous (without form, i.e., not crystalline) ; and lime- stone, the commonest and least pure variety of this icompound. All forms of calcium carbonate are easily soluble in all (dilute mineral acids and even in many vegetable acids, such £.M. I 114 CHEMISTRY AND PHYSIOS OF BUILDINO MATERIALS as vinegar, and the effervescence produced by such action has already been cited as a useful means of identification. 3. Calcium Sulphate (CaSO^). — Combined with water of crystallisation this compound is found in flat-pointed crystals, possessing the formula CaS04.2H20 as the mineral selenite which is common in certain clays, and is known among workmen as "petrified water." It occurs in larger masses often possessing a fibrous and silky texture as gypsum or satin spar, which possesses the same composition as selenite and is used as a source of plaster of paris. 4. Alumina (AI2O3). — Next to silica, alumina is the most plentiful and widely distributed compound known. Ordinary clay contains more than 25 per cent, of this oxide. It is found associated with iron in the mineral Bauxite which forms a source of metallic aluminium, and it also occurs alone as corundum, which in an impure form is the emery of commerce, and owes its value to its great hardness, which is 9. In a mineral form aluminium oxide is quite insoluble in water and acids. Alumina, in the presence of bases such as lime, always occurs in combination in building materials as an acid, forming aluminates, but in the absence of other bases it itself acts as a base, forming salts with acid oxides such as silica, e.g., aluminium silicate. In this latter form it is found in clays. 6. Magnesium Carbonate (MgCOa). — All magnesium com- pounds bear a strong similarity, both chemically and physically, to those of calcium, but since magnesia (MgO) is a less powerful base than lime (CaO), magnesium com- pounds are less easily formed, and when formed are more easily decomposed. This carbonate is found to a limited extent alone as the mineral magnesite, but in larger quantity in dolomite, which is a limestone in which magnesium and calcium carbonates are mixed together. 6. Potash and Soda Compounds. — The compounds of these STONES, CLAYS AND CEMENTING MATEEIALS 115 two bases resemble one another in a very marked degree. Apart from certain silicates referred to in a later paragraph, all compounds of these bases are readily soluble in water, and are therefore seldom found in large quantities in the solid state. Sodium and potassium chlorides NaCl and KCl, the carbonates, NaaCOa and K2CO3 and the sulphates Na2S04 and K2SO4 are among the commonest compounds found, and of these the sodium compounds are much commoner than those of potassium. In the nature of things such bodies cannot enter largely into the composi- tion of stable materials. Eeference has already been made to eflflorescence and deliquescence due to these salts, which are further characterised by their comparatively ready fusibility. 7. Compounds of Iron. — Two common minerals, iron pyrites and marcasite compounds of iron and sulphur, have already been described in Chapter VIII. These minerals are readily recognised under the microscope as, since they are quite opaque, they always appear black when viewed by light transmitted from below them, but if light is reflected from their surfaces the yellow colour they possess becomes at once apparent. Two oxides of iron, ferrous oxide (FeO) and ferric oxide (Fe203), are of common occurrence in building materials, and account for nearly all the natural colours possessed by stones and clays. The former is always found in combina- tions, as for instance, in ferrous carbonate (FeCOa), and thus acts as a base resembling lime and magnesia. The latter is found as the valuable ore of iron haematite, or disseminated, often as a mere coating film (a rust), upon the grains of other materials. IV. Silicate Minbkals. 1. Constitution of Silicates. — The silicates may be regarded as salts of silicic acid. As, however, there are several silicic I 2 116 CHEMISTEY AND PHYSICS OF BUILDINO MATEEIALS acids there are several series of salts. These acids, them- selves unstable compounds, may be regarded as combina- tions of one, two or more molecules of water with one molecule of silica. The acid HaSiOs or H20.Si02 is known as metasilicic acid, and that having the formula HiSiOi or 2H20.Si02 is known as orthosilicic acid. The lime salts of those acids are respectively calcium metasilicate OaSiOs, and calcium orthosilicate CaaSiOi- Other bases, such as ferrous oxide and magnesia, form similar silicates, as do potash and soda, and as these silicates are often found in combination and also associated with alumina, a very complex series of minerals results therefrom. As the exact composition of many of these compounds is uncertain the bases and acids are usually written side by side in the more complex cases. Thus felspar may be represented as K2Al2Si60i6 ; it is, however, preferable to write the formula as K20.Al203.6Si02. 2. The Felspars. — The felspars are a group of minerals composed of the bases potash, soda, and lime combined with alumina and silica. They are usually of a dull opaque white or grey colour, but some varieties are pink or red and other colours are known. These minerals show a fairly good cleavage, have a specific gravity of about 2*5 and a hardness of 6 to 7. (a) Orthoclase Felspar (K20.Al203.6Si02).— This variety, also called potash felspar, is more often red in colour than the other varieties, and is found in certain stones, such as Shap granite, in large, well-defined, bluntly-pointed crystals often two or three inches long and interlocked in a charac- teristic manner. More frequently it occurs in smaller masses without any distinguishable outline. (&) Plagioclase Felspars. — In the minerals included under this title the bases soda and lime are present in place of potash shown in the formula given for orthoclase. The felspars, if not white or grey, are at least not strongly STONES, CLAYS AND CEMENTING MATEEIALS 117 coloured. Under the microscope they sometimes show a series of fine parallel lines, and these markings, if present, serve to distinguish them from orthoclase. When felspars decay the bases are removed in solution and the remaining aluminium silicate remains as kaolin or china clay. 3. Micas. — There are two micas commonly found in stones and clays — Muscovite or potash mica and biotite or magnesium mica, which are aluminates and silicates of the bases named. Micas are characterised by remarkably perfect cleavage ; this allows them to be split into exceed- ingly thin pieces which possess much elasticity and the faces of which have a pearly lustre. Under the microscope the fine parallel cleavage lines are readily seen, unless, of course, the piece of the mineral viewed is lying parallel to its cleavage plane. The specific gravity of the micas is about 3 and their hardness 2 to 3. Muscovite, the commonest variety, is silvery white or brownish in colour. In sections parallel to the cleavage plane it exhibits bright colours under polarised light. It is found in some quantity in granites and other stones, and weathers well. Biotite is usually brown or black and exhibits marked dichroism under polarised light. It weathers badly, assuming a greenish tint when partially decomposed, owing to the formation of chlorite. 4. Hornblende and Augite. — These two minerals are com- plex silicates and aluminates of iron, magnesium and calcium, and have a specific gravity of 2'9 to 3*5 and a hardness of 5 to 6. As found in rocks, such as granite, they are usually dark green or black in colour and occur in opaque irregular masses possessing fairly good weathering properties. Many varieties of the minerals showing very different physical characters are known, however ; the valuable silicate asbestos is, for example, a variety of hornblende. 118 CHEMISTEY AND PHYSICS OP BUILDINa MATEEIALS Hornblende is a frequent constituent of many granites and often presents under the microscope crystals showing a corroded outline, it is also strongly dichroic. 5. Chlorite. — This mineral, a hydrated silicate and aluminate of magnesium and iron, is essentially an altera- tion product, and its presence indicates decay. It occurs in scaly fragments possessing no elasticity and somewhat greasy to the touch. Under the microscope it presents a radiating fibrous or earthy structure, and under polarised light usually appears grey or dull blue in colour and exhibits dichroism if sufficiently transparent. 6. Serpentine. — This is another decomposition product formed from a mineral termed olivine, found in certain rocks rich in bases and sometimes also from augite or hornblende. Its specific gravity is 2*5 to 2*7 and its hardness 3 to 4. In colour it is dull green (though red varieties are known) and shows a mottled or interlaced structure under the micro- scope. This mineral readily decays on exposure to the weather and is found in large masses alone (when it is often erroneously termed "marble ") and also in certain granitic rocks. As a conclusion to this chapter, the following list of minerals, arranged according to chemical composition, show- ing their respective characters, may prove useful, and therein are included metallic ores and other minerals which concern materials dealt with in succeeding chapters. 119—120 COMMON MINERALS. Occurring in, or Uskd in the Production op, Building Materials. 02 o -2 cS o Name. Graphitk Sulphur Iron Ptritks Marcasite . Copper Pyrites Galena Blende . Bauxite Corundum Cassiterite LiMONITE H«MATITK Maqnetiie . Pyrolusite Quartz . Composition. FeS2 FeS.2 CuFeS2 PbS ZnS Specific Gravity 2—2-3 2-0 4-9— 5-2 4-6- -5'9 4 1— 4-3 7-2— 7-7 3-7— 4-2 Spathic Iron Ore Ca lcite Dolomite Calamine Witherite . Barytes Gypsum . % j Orthoclase . I I Oligoclases . Mica (Muscovite) AUGITE . horneblende Olivine Chlorite Asbestos Kaolin Al203.Pe203 AI2O3 SnOa 2 FeaOs.S H2O Fe208 FegO^ Mn02 Si02 FeCOs CaCOs CaCO;! and MgCO ZnCOs BaCOs 3-6—4 6-8—7 3- 4—3 4- 5—5 4-9—5 4-8 2-6 Hard- NESS. 1—2 1-5—2-5 6—6-5 6—6-5 3-5-4 2-5 3-5—4 naS04 CaSOi.2 H2O K2Al2 8ifi0i6 Ca, Na, Al, Si, O K, H, Al, Si, O Mg, Ca, Al, Fe, Si, O Mg, Ca, Al, Fe, Si, O Mg, Fo, Si, O Mg,Fe,H,Si,0 Mg.Ca, H, Si,0 Al, H, Si, O 3- 7- 3-9 2-6—2-8 2-8—2-9 4—4-5 4- 2—4-3 4-3— 4-7 2—2-4 2-5— 2-6 2-5— 2-7 2-9 2-9—8-5 2- 9— 3-5 3- 2-3-5 2-6—2-9 2-2—2-6 9 6—7 5 3—5 5-5- 6-5 1—2 7 Colour. Black Yellow Yellow Light yellow Yellow Lead grey Black Brown Violet Black Brown Red to black Black Black White, violet Appear- ance ON Fracture. Cleavage Irregular Conchoidal2 Irregular Conchoidal Good cleavage Good cleavage 3-5—4-5 3 3-5—4-5 5 3—3-5 3—3-5 1-5—2 2—3 5-6 6-7 Grey to brown Colourless or white White White White or colourless White or colourless White or colourless Irregular Irregular Irregular Irregular Irregular Cleavage fibrous Conchoidal Appearance. Massivel Massive and crystals Massive and crystals Massive and crystals Massive Massive and crystals Massive and crystals Cleavage Very good cleavage Irregular Irregular IiTegular Irregular and cleavage Cleavage White to red White to pale tints Colourless or brown Green or black Green or black Green or brown Light green to black White to grey White to Irregular Irregular Very perfect cleavage Irregular Irregular Irregular Cleavage Cleavage A clay Massive, granular Massive and crystals Massive and granular Massive and crystals Massive and granular Massive, earthy Massive and good crystals Metallic, scaly Resinous . Metallic Metallic, dull Metallic Metallic, light Resinous to metallic . Nodules (crys- tal masses) Massive and crystals Rock masses and crystals Rounded masses Compact masses Massive and crystals Fibrous masses Earthy Vitreous, translucent Vitreous, dull . Earthy, dull, fibrous . Metallic Metallic, dull . Semi-metallic . Vitreous, transparent Occurrence. Ceylon, Cumberland . Sicily and other vol- canic districts Very widely diffused Very widely diffused . Cornwall, Cape, Chili . Derbyshire, North Wales With ores of lead Pearly lustre Pearly, vitreous Pearly or stony . Vitreous or chalky . Greasy or vitreous lustre Interlocked crystals Crystalline masses Crystalline masses Massive and crystals Massive and crystals Granular masses Irregular masses Fibrous masses A olay Vitreous or granular . Silky lustre, vitreous Vitreous, opaque Vitreous, opaque Vitreous, transparent Vitreous, dull Vitreous, dull . Vitreous, translucent Soft scaly flakes Silky texture Earthy, greasy touch Aries (France) Widely distributed Cornwall, Straits Settle- ments Sweden, and many other countries Spain, Sweden, Cum- berland Norway, Sweden, Russia Spain .... Very widely di stributed Remarks . Also known as black lead, or plumbago. Marks paper. Melts easily and burns. Very brittle. Weathers well, unless finely Rather brittle, divided. Spear-like crystals ; often whitish or brown. Weathers b.adly. Chief ore of copper. Chief ore of lead. Crystals generally cubes. Chief ore of zinc. Sometimes yellow or red, and semi-transparent. Prussia, Staffordshire, Yorkshire In all limestone dis- tricts Sunderland, Permian formation Vieille Montague, Spain With lead ores With lead ores, Shrop- shire Bristol, Retford, Derby 1 Irregular masses, often 8 In this and The normal felspar of granite In granite and many rocks Siberia. Granites gener- ally In many igneous rocks In many igneous rocks In Basalts and Dolerites In many decomposing rocks Canada, Italy Cornwall, Dartmoor . Chief ore of aluminium. Water and other impurities i)resent. Impure as emery. Forms many gems : as ruby, sapphire. Chief ore of tin. Arsenic often associated. Streak white. An iron ore. With clay forms ochre, umber, and siliceous earths. Important iron ore. Rounded fibrous masses. Streak red. The richest iron ore, and most valuable when pure. Chief ore of manganese. Crystals six-sided pyramid-t ; varieties : avanturine, agate, jasper, flint .sand. Seldom pure ; sometimes with manganese. Clay ironstone common impure variety. Crystals in many forms, breaks into rhombs. Used as a building-stone. Crystals hare curved faces. A valuable zinc ore. Often formed from blende. Used in brick manufacture as a corrective. Known as heavy spar. Used in paints. Varieties : selenite (clear crystals), alabaster, satin spar. Crystals often large, flat and bluntly pointed at ends. Distinct crystals rare. Often popularly called talc. A good insu- lator. Granular masses, crystals columnar and short. Fibrous masses. Very similar to augite. Occurs in volcanic rocks. Changes into serpentine. Replaces other minerals in igneous rocks. Often laminated. A variety of hornblende. Very flexible. Also called china clay. Results from decomposition of felspars. of considerable size. the following minerals the elements present 2 Resembling the fracture shown by a lump of glass, are alone indicated, as the formulas are very complex. CHAPTER XII CLISSIFIOATION OF STONES I. Introductory. In Chapter X. it was shown that the majority of stones, or rocks as they are termed by the geologist, which compose the earth's crust, are the fragmental remains of older rocks which have been deposited under water, but that intruded among them are other rocks, such as granite, which have solidified from a molten condition, and which are easily distinguishable by the absence therein of planes of bedding, fossils, and by their general structure. The former class are called Sedimentary (also Stratified or Aqueous) rocks, and the latter, in reference to their origin. Igneous rocks. It has further been stated that earth movements and the earth's heat have in various localities caused great changes in many deposits subsequent to their formation, and rocks which have thus been altered may conveniently be relegated to a separate class, and are known as Metamorphic rocks (rocks of changed form). The only rocks not accounted for under the above headings are certain limestones which have been deposited from solution, that is chemically precipitated, but since such deposits resemble the sedimentary rocks in all but their mode of origin they are properly included in this group. This simple classification, which conforms both to the geological and utilitarian aspects of the subject, may be 122 CHEMISTRY AND PHYSICS OF BUILDINa MATERIALS conveniently adopted and the members of these groups discussed under the following headings : — Igneous Stones. Sedimentary Stones. Metamorphic Stones. Granites and Limestones Slates allied stones Sandstones Marbles. II. Igneous Stones. 1. Granites. — The name granite is popularly applied not only to most stones of igneous origin but often to hard sedimentary stones used for road coverings. Such ter- minology is very misleading. Granite is an igneous rock which has never flowed out upon the earth's surface as a lava but has consolidated slowly at some depth, hence it is always entirely crystalline in character. The normal constituents of granite are quartz, felspar, and micBi. Quartz is always present in quantity — in fact, the total amount of silica present as quartz and combined in the silicates felspar and mica often reaches 70 per cent, of the whole rock. The predominating felspar and mica are generally orthoclase and muscovite, but plagioclase and biotite are also generally present. The quartz and felspar are commonly found in about equal quantities, and the mica in smaller quantity than either of the above constituents. The minerals hornblende and augite are often associated with granites, and when present in quantity such rocks are known as hornblende or augite-granites. Again, numerous accessory minerals are common in small amounts. Those which are objectionable are referred to at the end of this section. The structure of granites varies very much on account of the different rates at which solidification has taken place in different examples. In Shap granite, for instance, large porphoritic crystals of orthoclase felspar several inches long CLASSIFICATION OF STONES 123 occur, while in some other stones of very similar chemical composition all the minerals are so finely divided that they are with difficulty distinguished. As a rule finely grained granites weather better than those of coarser structure, apart from questions of defects. 2. Elvans. — This name, of Cornish origin, is given to certain igneous rocks which much resemble granite in composition, but which present a very different structure and appearance. Finely grained granites which show no distinctive minerals are sometimes placed in this category. An important member of this group of stones is quartz- porphory, a rock containing well formed crystals of quartz (never found in distinguishable crystals in granite) in a fine ground mass of quartz and felspar. Sometimes crystals of felspar are also present. Very little mica is found in these stones. Some of the Cornish elvans have considerable local use, since they are comparatively easy to work and harden on exposure. 3. Syenites. — These rocks may be looked upon as granites without quartz, or at least as containing quartz only as a minor constituent. The name Syenite is properly confined to rocks in which the felspar present is orthoclase ; those which contain plagioclase felspars are called Diorites. Syenites are only found in England in Leicestershire, and their chief use from this locality is for road " metalling." Much syenite is imported into this country from Scan- dinavia, under the name of granite. The rock is usually of a mottled grey tint or almost black, due to the presence of large quantities of augite, and the variety of mica is chiefly biotite. Some of these syenites (or more correctly syenite-dioritee, since both felspars are present) display iridescence, due to the arrangement of the felspars in parallel layers, and are termed popularly Labradorite, though the particular felspar from which this name is derived is not really present. 124 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS The small proportion of quartz and the presence of biotite mica are features which render the weathering properties of these stones not likely to be so great as those of the granites. 4. Other Igneous Stones. — Few other stones of igneous origin are in general use, though many are employed for local purposes. Of these the most important are the Basalts, which are ancient lavas very rich in iron. The rapid cooling which necessarily takes place in rocks which have flowed out upon the earth's surface has resulted in the production of a very finely grained rock. Basalts are black or very dark in colour. Their high specific gravity and the six-sided columnar form assumed by the rock in certain localities render it valuable for such structures as sea walls. 5. Objectionable Minerals in Igneous Stones. — Iron pyrites as a constituent of igneous or any other stones is objection- able owing to its tendency to weather, when iron oxide is produced, which is accompanied by expansion. Evidences of rusty stains round pieces of this mineral indicate that its decay has already set in. Kaolin, the residue left after the removal of the bases from felspars, naturally indicates advanced decay, and will render the felspars soft and earthy in proportion to the amount present. A test for the hardness of the felspar is therefore valuable. Chlorite has been described as essentially a product of decay of several mineral constituents of igneous stones. Calcite — crystallised carbonate of lime — is, in igneous stones and in slates, the product of lime freed by decom- position of felspars and other lime minerals, with carbon dioxide obtained from air and water to which such rock may have been exposed. The presence of this easily recognised mineral, therefore, indicates that changes of an undesirable character have taken place in such stones. CLASSIFICATION OF STONES 125 Since decay invariably reduces the hardness of stones, it naturally increases the ease and cheapness with which they can be worked. It should be borne in mind, however, that many partially decayed stones, which usually con- tain much calcite, as, for example, serpentine, may prove perfectly satisfactory for internal work while decaying rapidly in external situations. III. Sbdimentaky Stones. Stratified rocks have not received, at the hands of petro- logists in this country, the attention which has been devoted to those of igneous origin although they are much more important commercially. The fragmental origin of these stones certainly renders their microscopic examination less interesting, but their structure and the cementing materials of which they are composed are of the highest importance, and not infrequently remains of many of the foregoing minerals which have escaped complete decom- position may be detected. 1. Limestones. — Under this heading are comprised all stones which consist essentially of calcium carbonate, except such metamorphic stones as the marbles. The variation in composition and structure of limestones is very great, while some consist of little else than calcium carbonate, others contain much silica (siliceous limestones) or clay (argillaceous limestones), some are associated with magnesia (dolomitic stones) or with iron (ferruginous stones), while those impregnated with organic matter are termed bituminous limestones. These stones may again be classified from a structural aspect as granular, oolitic, shelly, or crinoidal limestones. (a) Common Limestone. — Ordinary limestone is found in layers or beds, which are often of great thickness and cover large tracts of country, as in the North of England and 126 CHEMISTKT AND PHYSICS OF BUILDING MATEEIALS Ireland. The rocks of the carboniferous and Hassic for- mations belong largely to this class, and these stones usually possess a bluish grey colour, present a fine grain, and are often distinctly crystalline in structure. Many common limestones were probably originally deposited from solution, and since they are generally highly fossiliferous and often very argillaceous, they are more suited for the production of hydraulic limes than for use as building-stones. (b) Oolitic Limestones. — These stones have a chemical origin, their characteristic structure, which presents yery perfectly rounded grains connected by cementing material, is assumed to be due to the constant motion of such grains in shallow water during the deposition of coatings upon them. The oolites can be traced through this country continuously from Yorkshire to Dorset, and comprise such important building-stones as those of Portland, Bath, Ancaster, and Ketton. These stones are lighter in tint than the limestones found in the older rocks. The variation which they show in their weathering powers must be attributed to differences in structure since they vary very slightly among themselves in chemical composition, and consist of little else but calcium carbonate. (c) Dolomitic Limestones. — These stones, also called magnesian limestones, consist of calcium and magnesium carbonates mixed together, or possibly to some extent combined, in varying proportions. The stones designated by this name, however, are only such as contain an amount of magnesium carbonate comparable with that of the calcium carbonate present. As all the limestones (at least in this country) which contain any magnesium show either trifling or quite large percentages of magnesium carbonate, this definition of a dolomitic limestone is sufficiently deter- minate. These stones are characteristic of the Permian formation, which presents good exposures in the north of England. CLASSIFICATION OF STONES 127 Structurally the dolomites vary considerably : some are compact and crystalline and possess great durability, while others are porous and shelly and weather badly. A high percentage of magnesium is regarded as an indication of good quality. Anston stone and Woodhouse Mansfield stone are examples of building-stones which come under this category. (d) Other Limestones. — Other stones belonging to this class find a limited use as building-stones. Kentish rag is an example of a hard siliceous limestone which weathers well, but its use is generally confined to random work. Ham Hill stone is a shelly ferruginous limestone possessing a warm tint and very attractive appearance, but is some- what difficult to work. Chalk is a soft variety of stone, consisting almost entirely of minute shell fragments deposited in deep water, and its marine origin confers upon it great constancy of structure and composition, but owing to its porosity and the lack of cohesion between its particles it is not suitable for external work. 2. Sandstones. — Sandstones consist of fragments of quartz cemented together by silica deposited from solution, or by alumina, carbonate of lime or magnesia, or one of the oxides of iron. In some stones, however, no cementing material is discernible and the grains hold together as the result of partial vitrification. Since quartz is entirely unaltered by atmospheric agencies the weathering power of sandstones must depend upon the nature of the cementing materials, the shape of the quartz fragments, and the amount of porosity possessed by the stone. The commonest of these cementing materials consists of hydrated oxide of iron, which gives the yellow, brown or red tint so associated with these stones. If carbonates are present they may be either crystalline or amorphous, and if alumina, the material will usually be soft and clayey. 128 OHBMISTEY AND PHYSICS OF BUILDING- MATERIALS In the strongest and most durable stones the quartz grains are fritted together owing to partial fusion, as in the famous Craigleith sandstone. Such stones are, however, very hard and difficult to work, and if the fusion has taken place to any marked extent they are termed quartzites, and must be regarded as metamorphic stones. Some sandstones possess distinct planes of bedding, as, for instance, the well-known York stone. These bedding planes, which give the stone a cleavage, are generally due to the presence of mica, which forms layers between the quartz grains, and thus disturbs their continuity. In other varieties, such as the Bramley Fall stone of Leeds, these laminations are conspicuously absent. Finely grained sandstones stand sudden changes of temperature better than other natural stones, owing to their homogeneous structure. 3. Objectionable Minerals in Sedimentary Stones. — The remarks upon iron pyrites, made in connection with igneous stones, apply equally to those of sedimentary origin, and though, perhaps, seldom present in quantity, the sister mineral marcasite is not uncommon, disseminated between the planes of bedding. The oxidation of these sulphides of iron not only produces staining and disruption due to expansion, but also, owing to the formation of sulphuric acid, solution of any carbonate of lime or magnesia present with the production of sulphate of lime and a corresponding loss in cohesion. Other iron compounds, such as ferrous carbonate (FeCOa), if present in quantity are also objectionable owing to their tendency to oxidise, while alumina, the usual source of which is clay, by destroying the continuity of crystalline structure or of some cohesive cementing material may prove a source of great weakness. 4. Weathering. — The weathering of igneous and sedimen- tary stones differs in that, while the decomposed products CLASSIPIOATION OF STONES 129 remain in situ in the former they are generally removed by surface scaling in the latter, which renders an estima- tion of the process of decay in a stone of sedimentary origin not very amenable to microscopic investigation. No serious attempt, however, has yet been made to carry out micro- scopic examinations of weathered stones, and a most useful field in this direction awaits the labours of the petrologist. The chief product of the weathering of sedimentary stones, apart from iron compounds, is sulphate of lime resulting from the action of sulphuric acid upon carbonate of lime, and causing a surface efflorescence often of some thickness. Where such deposits are maintaining the stone in a damp condition and thus causing further damage they should be removed ; but in certain circumstances they may act as a protective coating, when their removal may be doubtful policy. IV. Metamoephic Stones. 1. Definition. — Eeference has been made to the crushing effects of earth shrinkage and the change produced by the heat from intruded rocks in explanation of the alteration in characters which make it desirable to include certain originally sedimentary deposits in a special category. So far has this baking action gone in many cases that all remains of original structure, planes of bedding and contained fossils have disappeared, but all stages of meta- morphosis are known down to the slightest alterations which have merely produced incipient crystallisation. Water also plays a large part as a metamorphic agent. Under the pressure of great rock masses confined water may reach a temperature far above its normal boiling point while still remaining liquid, and then possesses greatly enhanced solvent powers. When the pressure is released 130 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS through some earth movement this water will turn into steam and deposit its dissolved matter in a form which may be essentially different from that which it originally possessed. 2. Marbles. — The marbles are composed of carbonate of lime which, subsequent to its deposition, has been rendered entirely crystalline, thus giving the material a compact structure which enables it to take a high polish, and also confers upon it great strength and durability. Since, how- ever, acids attack all forms of carbonate of lime, no marble will withstand exposure to a town atmosphere without detriment, which, owing to the fine arrises and polished faces generally conferred upon marble, makes itself readily conspicuous. The colours of marbles are due to the presence of iron in various states of combination. Hydrated ferric oxide confers yellow or brown tints, and this oxide in an anhydrous state (without water) gives red markings. Iron combined with silica in the mineral glauconite accounts for green colourings, while black marbles generally owe their absence of colour to the presence of organic matter derived from bituminous limestones. Marbles sometimes contain finely disseminated sulphides of iron, which are particularly to be avoided in the white varieties, since on oxidation of the iron the stone will acquire a pink tint. Varieties. — No attempt can be made here to deal with the many varieties of marble used for decorative purposes, which range from the polished fossiliferous and only slightly altered limestones to the much-prized Greek and Italian marbles, which are wholly crystalline in character. The term "marble" should be confined to stones composed of carbonate of lime, and not applied to serpentines or similar stones. Some of the Irish Connemara marble, for CLASSIFICATION OF STONES 131 instance, is correctly so called since it is an altered dolo- mite, but other stones included under this designation are serpentines, and therefore of igneous origin. Alabaster is a variety of marble characterised by its transparency ; this statement, however, is only true of Oriental alabaster. The material produced in this country under the name of alabaster is not the carbonate but the sulphate of lime, and may be regarded as a variety of the mineral gypsum. 3. Slates. — (a) Formation. — The term "slate" is properly confined to metamorphic rocks derived from clays which, originally laid down as sedimentary deposits, have been subjected to the action of heat and great lateral pressure while still confined, by the vertical pressure of deposits above them. This has resulted in an alteration of the position of the particles forming the clay, which, originally deposited in horizontal layers — that is, with the longer axes of the particles lying flat — has been transformed into layers with such axes at right angles to the lateral pressure, the thrust upon the particles having turned them round until they occupy as little space from side to side as possible. As an analogy, a crowd of people standing side to side may be taken. If such persons were crushed laterally by crowds pressing upon them on either side they would tend to move individually through a right angle, as they would then, standing face to back, have more space in the direction of the pressure. An important effect of this change is the cleavage which is thereby induced in planes at right angles to the direction of the lateral pressure, since it is naturally easier to separate layers of particles lying side by side than to split the material in other directions, which would involve the fracture of individual particles ; and when thin platey minerals, such as mica, occur in the clay this induced cleavage may be developed in a very perfect degree. From the above considerations it will be obvious that all B.M K 132 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS traces of the original planes of bedding will generally be lost when slates are formed. (h) Composition. — Clays are decomposed felspars from which the bases have been removed, hence clays and slate formed from them are chiefly composed of silicate of alumina. Since, however, this felspathic decomposition has been seldom complete, and as quartz, mica, and other minerals originally associated with the felspar may have escaped complete removal, slates always contain small quantities of lime and other bases, and are often very rich in iron. Silica is usually present in amounts ranging from some 60 to 60 per cent., and alumina from some 10 to 20 per cent. The bases, lime and magnesia, together account- ing for some 3 to 12 per cent., and potash and soda 2 to 5 per cent., may be present as part of the original minerals, such as felspar and mica, or in the form of secondary minerals, chiefly as carbonates. In the former condition they are not likely to prove disadvantageous, but their presence as carbonates is, as previously explained, an indication that changes have taken place in the slate sub- sequent to its formation, and coupled with any sign of a soft and friable condition, may be taken as evidence of advanced decay. Iron occurs in a fully oxidised condition as Fe203, and also in larger amounts, reaching some 7 per cent, as ferrous oxide (FeO) in combination. In this form, unless combined with silica, it is liable to undergo further oxidation, with resulting expansion as previously explained, and unless well disseminated may cause local disruption. Iron pyrites and marcasite are often found in slates ; the former, when it occurs in crystals, so situated that they are not liable to fall out and leave holes in the slate, are not in the least liable to change, and form a charming feature. When occurring in veins or small grains pyrites is to be looked upon as objectionable. Marcasite, which may usually be CLASSIFICATION OF STONES 133 distinguished by its duller appearance and often by its earthy surroundings, should always cause the rejection of slate, as it decays very readily. The nature of the changes which occur when sulphides of iron decompose has already been discussed. (c) Occurrence. — Slates occur only in the older rocks, such as those of the Cambrian and Silurian formations. Since the metamorphic action which has produced them has seldom had a crisp termination in any locality, the quality of slates must be expected to rapidly deteriorate towards the borders of a slate-bearing district, and a gradual passage into shales and clays may in many places be looked for. Shales may always be distinguished from slates by their property of forming plastic clays when rubbed up with water. They also usually possess bedding planes and exhibit very poor cleavage. Poor slates smell earthy, fail to ring when struck, absorb water readily, and possess little crushing and transverse strength, properties developed in good slate to a very high degree. Artificial Stone. The principles involved in the production of artificial stone, and the methods employed for preserving stone, will be better understood after the discussion of the properties of limes and cements. A short article on this subject will be found in Chapter XIX. K 2 CHAPTEE XIII the examination and testing of stones 1. Introductory. The examination of stones may be approached from a purely scientific or from a commercial aspect ; but since the latter aspect necessarily calls upon information obtained from scientific investigation, it is very desirable that a complete knowledge of the chemical and physical proper- ties of all stones suitable for commercial use should be obtained. No organised comprehensive scheme for such investigation has yet been attempted in this country, although valuable work in this direction is extant for the building stones of America. Stone is a natural product, and, like all such products, it fails to comply with the rigid standard of constancy which may be demanded in a material made artificially. At the same time there are many building stones which are remarkably constant in composition and properties, and many interspersed beds among them which should be precluded from acceptance in the same category. More precise nomenclature in certain cases would undoubtedly benefit users and ultimately also vendors of stone. Scientific tests should be carried out with the greatest accuracy and refinement upon specimens of known origin, in order to serve as a collection of standard data in which every possible factor affecting any use of the stone should be taken into consideration. Commercial tests, the fair- ness of which can only be assessed with a knowledge of THE EXAMINATION AND TESTING OF STONES 135 such scientific data, may be of a simpler character, and need relate only to the particular calls which will be made upon the stone in use. Thus, for example, the elasticity, hardness and solubility of all building stones may be advantageously recorded, although a determination of the elasticity of a paving-stone, the hardness of a lintel, or the solubility of a marble for internal decoration, would have no value commercially when the use of the materials for these respective purposes was in question. The examination of stone may be conveniently discussed under the following headings : Specific gravity Hardness Porosity Crushing strength Elasticity Microscopic tests Adherence Chemical analysis Expansion Solubility Conductivity Characters in site. II. Individual Tests. 1. Specific Gravity. — The methods of determining specific gravity have been explained in Chapter II. In making such determinations in the case of stone, it must be reaHsed that this property as assessed for freshly-quarried, for dried stone and for the stone reduced to powder, will not be the same. No stone is entirely free from porosity, and when quarried the pores are always partially filled with water, which evaporates on exposure, when air takes its place and thus decreases the specific gravity. On account of porosity, again, many stones have a markedly higher specific gravity when this determination is made with the material in the state of a powder, for in this case the volume added by the intervening pores is excluded. When a stone is composed 136 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS of several mineral constituents it is obviously necessary that a sufficiently large specimen to form a fair sample of average composition must be dealt with if the result is to be of any value. Any statement of the value of specific gravity should therefore be accompanied by information as to the condi- tion of the stone at the time of its determination, but as ordinarily understood it refers to its weight per unit volume in bulk after exposure to air of ordinary dryness, and therefore the air-filled pores are included. The determination of this property seldom has any direct value, as, except in certain marine works, the stability of stones is seldom influenced by their relative weights. Since, however (at least among sedimentary examples), the individual minerals of which stones are composed differ themselves but slightly as regards this property, differences in specific gravity as determined when in bulk give valuable indications as to porosity. 2. Porosity. — Tests for porosity are usually made by immersing a given volume of the stone in water and observing the increase in weight of the specimen when no further absorption takes place, when, from a knowledge of the weight of unit volume of water, the volume absorbed by the stone is ascertained. The only means of ascertaining whether absorption has ceased, is to weigh the stone at intervals until no further increase in weight is observed. It is obvious that the absorption must be complete if the test is to be of any value, and the time taken to attain this will be partially governed by the configuration of the specimen; a thin slab, for example, will naturally reach saturation more rapidly than a cube of the same weight. Even made as suggested, the test is far from satisfactory, since it is almost impossible to remove all air, and thus to fully admit water to the pores of the material, though the THE EXAMINATION AND TESTING OF STONES 137 operation may be facilitated by placing the stone in a vessel connected to an exhausting pump. Further, any air remaining will be altered in volume quite precisely by barometric changes in pressure and by change in temperature. The water used may, with advan- tage, be previously boiled, as it will then be in a position to dissolve some of the air which it has failed to expel. Since porosity represents the ratio of interspaces to solid material, this quality may be assessed by comparing the specific gravity of the stone in bulk, i.e., including the pores, with that of the stone as powder ; but even in this case it is difficult to remove every particle of air from the powdered substance. A more satisfactory test for porosity is a practical one based on the rate of soakage, though in the absence of any standard yet agreed upon the results obtained can only have a comparative value, and for this reason, as in the case of many other tests, gives but little assistance in specifying requirements. Soakage tests are carried out by placing a piece of the stone of known area and thickness under a known and constant head of water at a constant temperature (hot water is more limpid than cold water), and weighing the water which soaks through in a given time, due precautions being taken to prevent loss by evaporation. 3. Elasticity.— Defined in a previous chapter, this property is an important one even in the case of stones, as when stones fail from mechanical causes it is generally through bending that fracture occurs. Elasticity in stones presents anomalies, and its determina- tion is beset with some difficulties, though these facts are hardly an excuse for the indifference to this property generally displayed in use. The difficulty of the test arises chiefly from the very small amount of deformation apparent under stress, and in obtaining uniformity in the specimens 138 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS to be experimented upon. Professor Unwind has given an interesting account of the investigations of Bauerehinger on this subject, and has himself confirmed the conclusions of this savant by his own experiments. The specimens under test were submitted to compression, and the deformations resulting in the stones were measured by optical magnification. A permanent "set" was found to take place in the materials when sustaining but quite light loads, and in the case of hard and dense stones the com- pression was observed to be proportional to the load right up to the final crushing of the test piece. In the case of the more porous stones, the compression at first increased more rapidly than the load, but finally, with heavy loads, less rapidly, as would be expected. Similar relations between force and deformation were obtained in a series of experiments upon stones under tensile and bending stresses. A stone, then, under stress takes a permanent set, and this process is repeated with each additional load right up to the breaking point. Stones, therefore, possess no elastic limit in the sense that up to a certain stress they will recover their original form on the removal of the force calling out this stress, as is found to be the case with the metals. Their limit of elasticity, if indeed it is wise to use the expression in a different sense, must be regarded as reached at the point of failure. ^ Hard stones appear to possess the greatest elasticity, and limestones as a class to have very similar elastic powers, which are greater than those of sandstones. In the case of stones used for lintels and arches, especially when called upon to bear variable loads, as in bridges, a knowledge of elasticity is of importance and can seldom 'be looked upon as useless, since this property is bound up with all causes of mechanical failure. » "The Testing of the Materials of Construction." Unwin. THE EXAMINATION AND TESTING OF STONES 139 4. Adherence. — Upon the power of the particles of a stone to hold together, the probability of disintegration by freezing water or expanding minerals to some extent depends. Power of adherence over a given sectional area of the stone is necessarily influenced by porosity, as air- or water- filled voids represent area which is a direct decrease in the effective points of contact. Adherence is usually tested by artificially freezing water contained in the pores of the material, and is assessed by the weight of the fragments, which are split off as the result of this internal expansion, when this process has been several times repeated. Such a test has little scientific value, but until more research is undertaken upon adherence and coherence it is impossible to formulate suggestions for a standard. Some further remarks on these properties occur in Chapter XVIII. 5. Expansion. — The co-efficient of linear expansion of a bar of stone may be determined as has already been described for the metals in Chapter V., but the result obtained will be found to depend largely upon the amount of moisture contained in the stone, which must therefore be ascertained. Owing, however, to the low conductivity and high specific heat of stones, expansion as thus measured is not of great importance. By an expansion test is more generally meant an investi- gation of the relation between temperature and disintegra- tion, and the factors mainly involved are the relative co-efficients of expansion of the different minerals com- prising the stone and the adherence and size of the particles. The behaviour of a stone under sudden increase in temperature can thus be to some extent predicted. A stone composed of very different ingredients, such as granite, must necessarily be subjected to enormous internal stresses when heated, owing to the unequal expansion of its various 140 CHEMISTEY AND PHYSICS OP BUILDING MATEEIALS constituents, and will fly to pieces in the heat of a burning building, whereas a sandstone composed almost wholly of one compound may resist the ordeal. The tests usually made from the above aspect are not of great scientific accuracy. The time during which the stone withstands a given temperature is naturally an important factor, and this will depend upon the configuration of the test piece, the rate of heating, and in a minor degree upon the specific heat and conductivity of the material. In this country such tests are of value in relation perhaps solely to fire risks, but in some climates where very rapid atmospheric changes of temperature occur, much shelling of stone surfaces may take place through consequent sudden expansion or contraction. 6. Conductivity. — All stones are bad conductors, and although they differ as regards this property the difference is not of great importance in practice. Some data on this subject have been obtained by finding the rates at which heat flows through plates of the same area and thickness of different stones when the two sides of the plate are kept at different known temperatures. 7. Hardness. — By the "hardness " of stone, resistance to abrasion is usually implied. Abrasion tests are naturally of most interest in connection with stones used for steps and pavements. A standard is again lacking in respect to this quality. Various forms of abrasion machines have been devised ; these usually consist of a weight attached to some gear by which it may be moved over the surface of the stone to be tested, and the actual abrasion is caused by emery fed on to the surface. Possibly a standard might be contrived by the use of a given weighted hemisphere of corundum made to pass at a given rate along a certain length of the specimen, with and across the grain (if any), a certain number of times, after which the abraded material would be weighed. THE EXAMINATION AND TESTINa OE STONES 141 The hardness of a stone generally increases considerably on exposure after quarrying, for the " quarry sap " or water in the stone evaporates upon the exposed surfaces and there deposits solids, such as silica, which are contained in the water in solution. The surface pores of the stone are then filled, and the face hardened. It should be remembered, however, that since the evaporation and deposition of solids only takes place on the surface, the interior of the stone does not benefit in the same manner, and that the process of face hardening is not repeated if this skin is removed — a fact which should cause reflection before the surface of old stone is submitted to dragging operations. It must be admitted, nevertheless, that this explanation of the hardening of stones leaves something to be desired, as some stones become hard in course of time to considerable depths beneath their surfaces. This might conceivably be due, in the case of limestones, to gradual solution in moisture charged with carbon dioxide and subsequent deposition of such dissolved material in a crystalline form in the pores of the stone. 8. Crushing Stress. — It is seldom that the snperincumbent pressure on stones used in buildings, or even the thrust upon such stones, exceeds a tenth of the load necessary to produce failure by crushing. The lightest building stones, for example, will sustain a pressure of some 250 tons per square foot, and even in columns about three quarters of this weight. Notwithstanding which fact this test is the one usually adduced before all others by merchants anxious to substantiate the good quality of a stone. A knowledge of crushing stress, however, has some indirect value as in- dicating the elastic and adherent properties of the material. Such tests as usually made, leave, nevertheless, something to be desired, for the cube, though generally used, has been shown to be less suitable for ascertaining the value of this property than a rectangular block half as great again 142 CHEMISTRY AND PHYSIOS OF BUILDING MATERIALS in the direction of the crushing pressure than in its other dimensions. The test is applied by submitting opposite and parallel faces of the block to compression in a hydraulic press. Eepresentative results are difficult to obtain without the use of a powerful machine, and since there are but few presses at disposal capable of dealing with specimens presenting a face area exceeding 6x6 inches, the actual load which can be carried by any area of jointed masonry is seldom really ascertained, for it is not probable that this can be correctly assessed from the proportionate area of a small specimen. For the reason given above this is perhaps not of much moment, and it would probably be more useful to utilise crushing tests as adjuncts to tests on elasticity and adherence instead of attempting to give them a direct significance. 9. Microscopic Tests.— The examination of thin slices of stone or rock sections,^ as they are termed, under the microscope gives more information as to the quality of the material than perhaps any other test, and can, moreover, be carried out with rapidity. In the nature of things, micro- scopic analysis must be of a qualitative rather than a quanti- tative character, and it requires an expert petrologist to elucidate the meaning of many of the features displayed by this instrument ; but much may be learnt even by the layman with a little practice. Anyone, for example, can gain some insight into the nature and proportion of the cementing material between the grains of a sandstone, determine whether such grains are rounded or angular, and detect certain minerals, such as iron pyrites, by the use of a ^ Rock section cutting forms a small distinct branch of lapidary work, and is accomplished by grinding chips of the stone until thin enough to transmit light when they are mounted on glass slides. Sections of ordinary building stones can be prepared for about Is. 6d. each. THE EXAMINATION AND TESTING OP STONES 143 simple instrument devoid of polarising prisms or^ other accessories. Again, incipient decay in igneous rocks as judged by earthy felspars, the presence of carbonates, chlorite and other minerals of secondary origin, is not usually a difficult matter to discover microscopically. The microscope has yet to be accorded its due place as a commercial instrument, and a great aid to its popularity would be the production of a standard set of rock sections of the commoner building stones fully identified and described, and a similar set showing the effects of weathering under defined and practical conditions. In the case of the sedimentary stones the preparation of sections showing weathering presents considerable difficulty, but a well-known geologist has expressed to the writer his belief that it is practicable. 10. Chemical Analysis. — Though a few simple tests which will indicate the presence of certain constituents in a stone may be undertaken by the layman, chemical analysis is essentially the work of an expert, and the preparation of a complete statement as to the nature and amounts of the constituents of any stone involves, except in the case of those of very simple composition, considerable skill and labour. Much misconception appears to exist upon the subject of analyses, which usually give the percentage of bases and acids present in the stone with little, if any, regard to their true relations. Such analyses may have some value as showing the presence and amounts of wholly undesirable constituents, and do not give rise to ambiguity in the case of stones of very simple composition. Generally speaking, however, a chemical analysis should be preceded as far as possible by a mineral analysis, for since many of the minerals present usually contain the same acids and bases, a mere statement of the total amounts of such components can give, in such cases, no conception of composition. 144 CHEMISTEY AND PHYSICS OP BUILDING MATEEIALS A complete separation of the minerals composing a stone is admittedly a matter of great difficulty, but, making full allowance for the complexity of the problem, the fact remains that much valuable work is thrown away by the stereotyped manner in which the analyst too often approaches his work. Different stones require different methods of procedure. As an illustration, the analysis of a calcareous sandstone and a granite may be considered. In the former stone the microscope has revealed grains of silica cemented by carbonate of lime. The chemist submits an analysis showing the percentage of silica (SiOa), lime (CaO) and carbon dioxide (CO2) which accounts for everything present. This is perfectly intelligible. The carbon dioxide could not have been combined with anything but the lime ; hence, since 44 parts (the molecular weight) of CO2 combine with 56 parts of CaO, 44 parts of CO2 must involve the presence of 100 parts (56 + 44) of calcareous matter, namely, CaCOs, and thus from the percentage of CO2 given, theCaCOa can be calculated by simple proportion. The analysis of the granitewhich will probably be presented in the same manner will show the percentage of siHca, alumina, lime, potash and soda. Now both felspar and mica are silicates and aluminates of potash ; in felspar, however, the ratio of alumina to potash is about 4 to and in mica this ratio is about 4 to 1. Suppose that an inspection of the analysis showed that the percentage of potash was low as compared with other analyses of good stones, this might indicate the presence of a large percentage of mica, but it might equally well imply that the felspar had lost much of its potash owing to decay, which would involve a very different conclusion as to the suitabiHty of the stone for use. Identical ultimate analyses are therefore possible for stones possessing wholly different structural values. What is wanted in the case of all heterogeneous rocks THE EXAMINATION AND TESTING OE STONES 145 is the composition of the individual minerals present. The amount of each mineral, which is not easily ascertained, may be often gauged with sufficient accuracy by microscopic investigation. Attempts at mineral separation have been made by crushing the stone and placing the powder in liquids of different specific gravities, so that one constituent of the stone may float while another will sink. This has not proved very satisfactory, and in the case of stones possessing minerals in distinguishable pieces a better plan would possibly be to fracture rock sections and remove the individual minerals while still in position by mechanical separation under the microscope. 11. Solubility. — Experiments upon the solubility of stones refer chiefly to the effects of acids, such as sulphuric acid present in town atmospheres. In the neighbourhood of certain industries hydrochloric acid is also often found in the air. Both these acids readily dissolve carbonate of lime, and therefore it is among the limestones and calcareous sandstones that their greatest ravages are to be looked for. The structure of the stone is found to influence its behaviour very materially in regard to solubility. As usually recommended, the test consists in immersing a known weight of the stone in a weak solution (about 1 per cent.) of sulphuric or hydrochloric acid and ascer- taining the amount dissolved after a given period. To obtain results of any accuracy specimens of the same size and configuration should be used, and these must be weighed in the same condition (say dried at 100° C.) before and after the experiment. In the case of stones to be placed under water it may occasionally be desirable to make other solubility tests if an analysis of the water indicates the probability of any solution taking place. 12. Characters in Situ. — The examination of stone by 146 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS actual inspection at the quarry is of great value. This has two objects : an inquiry into (1) Weathering qualities ; (2) The probability of obtaining uniformity in the material supplied. In the former investigation actual working faces which have been exposed to the weather should be examined, due allowance being made for weather stains produced by surrounding vegetation. It does not, however, follow that a stone which presents a satisfactory appearance in the quarry will weather equally well in the situation proposed for its use, and every advantage should be taken of possible investigations of the condition of buildings erected in the stone in the locality proposed. It is to be hoped that a register may some day be compiled showing the stone employed, age and locaHty of accessible buildings, with notes upon aspect, weathering and local conditions. This would be invaluable to stone users. The question of uniformity to be expected in the supply of stone is naturally of importance in proportion to the amount required, and though in the case of many well- known stones uniformity from reputable vendors may be expected without investigation, this matter assumes a different aspect in the case of stone supplied from new sources. A knowledge of local geology and of the investigations which have been undertaken by the quarry owners can alone answer such inquiry, and such owners would do much both for purchasers and themselves by strictly defining the beds of their quarries and publishing such evidence of probable uniformity as they have acquired. CHAPTEE XIV BRICK AND OTHER CLAYS I. Geological Formation. Clays are universally secondary deposits ; that is, they are the result of the decomposition of older rocks. They are found in all geological formations, though in the lower series of deposits earth movements and the compression due to overlying strata have usually converted clays into shales or slates. Clays owe their origin chiefly, but not entirely, to the decomposition of felspars contained in igneous rocks. Such disintegration may be due to ordinary weathering, but since masses of decomposed felspars some hundreds of feet in depth, evidently still situated in their original positions, are known, some further explanation of this decomposition seems to be called for, as it is not conceivable that weathering should have extended to so great a depth without the removal of the larger part of the friable materials so produced. It is believed that these deep clay deposits have been formed by the decomposing action of vapours penetrating the felspars from below, and particularly by the action of hydrofluoric acid, a gas which resembles hydrochloric acid, but which possesses greater chemical activity and can dissolve silica. The solution of part of the silica from the felspars sets free the bases, which are themselves then removed in solution, and leaves silicate of aluminium, which constitutes the clay. B.M. L 148 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS This theory of the formation of certain clays is borne out by the presence in them of secondary minerals, such as tourmaline, which contain the element fluorine as one of their constituents, and by the fact that hydrofluoric acid is producible from fluorides in the presence of superheated water, which is known to occur in the earth's crust at great depths. II. Varieties of Clay. Clays may be residual or transported, the latter being the more common. 1. Residual Clays. — Eesidual clays are those which have been left in situ after the decomposition of the rocks giving rise to them, and may be distinguished by the evident relation in character and composition which they bear to the rocks which they overlie. Such clays generally merge into the underlying rocks without any definite plane of separation. Kaolin or china clay belongs to this class. 2. Transported Clays. — Transported clays, among which all the ordinary brick clays must be included, form stratified deposits which resemble in their mode of deposition the sedimentary rocks ; that is to say, they have been laid down in beds under water and can be traced by their relations to neighbouring deposits and by their characteristic fossils. These facts, the wide areas often covered by such clays and the sharp line of demarcation between them and the strata on which they rest, to which they bear as a rule no relation in character, make transported clays easily distinguishable from those of residual origin. 3. Varieties of Transported Clays. — Transported clays present varieties in their mode of occurrence similar to those found among stones of sedimentary origin. Some — the marine clays — have been deposited in deep water, cover wide areas, and show great constancy in composition ; such BRICK AND OTHEE CLAYS 149 clays consist of fine particles, since only such material can be carried out from river courses or cliff erosion far into the ocean. Other clays less extensive and constant in character have been laid down in lakes ; the London clay is an example of this class. Finally, estuarine clays deposited at the mouths of rivers and streams are still more local in character and are often found in lenticular (lens-shaped) deposits which present marked physical variations at, it may be, distances of a few yards. Such clays are often mixed with, or broken up by, layers of sand and gravel. Another extensive clay deposit is the boulder clay, formed from detritus scraped up by the great ice sheet which once spread over the northern part of E urope. Such clay is found in the eastern counties of this country, but is too full of stones and boulders to admit of its being put to much practical use. III. Physical Propbetibs of Clay. The distinctive property of clay is its plasticity, and most of its uses depend upon this property and upon the fact that it is entirely lost when the material is heated to a certain temperature, when it acquires rigidity of form. Plasticity is usually attributed to the presence of kaolin, which is hydrated aluminium silicate ; but since the display of this property bears no relation to the amount of kaolin in a clay which may be exceedingly plastic while containing but 5 or 10 per cent, of this mineral, some further explana- tion seems to be called for. Any exceedingly finely grained substance which is wetted by a liquid may be expected to display some powers of being moulded, as, owing to what is called " surface tension," the liquid will tend to stick to the solid particles. Clays contain particles which are stated by Eies^ to be in many cases not 1 Eies, " Clays : their Occurrence, Properties, and Uses." John Wiley, 1906. L 2 150 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS more than i^j,^ou ^ millimetre in diameter, and the plas- ticity of the mass is found to increase with the fineness of the particles, though no direct relation between these properties appears to exist. In a valuable summary upon the theories put forward to explain plasticity, the above writer refers to that based on molecular attraction which, where such small bodies are in question, may not unreasonably be supposed to exercise some effect in holding the particles together while still allowing them to slide round one another. The effects of kaolin in producing this property are probably due to the colloidal (glue-like) nature of hydrated silica and alumina ; such bodies, to which must be added hydrated oxide of iron and organic matters frequently found in clays, undoubtedly exercise an important effect, on account of their jelly-like nature, which is largely due to their powers of absorbing large quantities of water mechanically. IV. Mineral Composition of Clay. Though clay results from the decomposition of felspars, it has naturally often happened that the weathering action has been arrested before such decomposition was completed. Hence clays are often very complex in character, and contain not only remains of felspar as such, but other constituents of igneous rocks, such as quartz and mica. The presence of such minerals, again, accounts for the existence in clays of further " secondary minerals," such as caicite and gypsum, formed by later chemical changes. The following may be regarded as the commonest con- stituents of clays : kaolin, quartz, mica, felspars, pyrites, iron oxides, gypsum, caicite, dolomite, carbonaceous matter, and water chemically combined and as mere moisture. Many other minerals are often present in small quantities. BEICK AND OTHEE CLAYS 151 The above-named minerals have already received con- sideration in Chapter XI., and the following account of them will therefore be confined to their effects upon the properties of clay and the ware made therefrom, while the behaviour of these constituents in the kiln when clays are " burnt " will form the subject of the succeeding chapter. 1. Kaolin. — This mineral is referred to as kaolinite by American writers, who confine the term " kaolin " to clays consisting largely of this substance in an impure condition. Kaolin, which is found crystallised in very minute hexagonal plates, has the composition Al2O3.2SiO2.2H2O, a specific gravity of 2*2 to 2*6, and a hardness of about 2. It results from the removal from orthoclase and other felspars of the whole of the bases potash, soda, and lime, and of about two-thirds of the silica, but it is never found in a pure condition. Chemically kaolin is usually dis- tinguished as that part of a clay which is soluble in hot sulphuric acid and also in a solution of sodium carbonate. 2. Felspars. — Felspars are occasionally present in a sufficiently undecomposed state to admit of their identifica- tion when much magnified under the microscope. Orthoclase, which is less liable to decomposition than the felspars possessing lime and soda as bases, is more frequently found than these latter varieties. 3. Mica. — Mica, particularly muscovite, which withstands much weathering action, is often found in clays, but is by no means universal. 4. Quartz. — Free quartz is often present in sufficient quantity to seriously decrease the plasticity of clays. As it does not absorb water, however, it decreases the shrinkage which occurs when clays are dried. 5. Iron Pyrites. — This mineral and also marcasite are fairly common in clays and are very objectionable. On weathering these sulphides of iron undergo oxidation, with 152 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS the eventual production of sulphuric acid, which leads to the formation of gypsum and other undesirable minerals. 6. Iron Oxides. — Ferra (Fe203) results from the final decomposition of most iron-bearing minerals, and it is to this oxide that the clays, particularly when burnt, owe their various colours. When hydrated, the oxide, then known as limonite, gives a yellow or brownish colour, and when anhydrous (without water), as haematite, it confers a red colour on the clay in its natural state. Iron is also found in a partially oxidised condition, as ferrous oxide (FeO). 7. Calcite. — Carbonate of lime in this form results from the action of carbon dioxide contained in percolating water upon lime freed by the weathering of plagioclase felspars. Carbonate of lime is also often present as intermixed chalk, or as the shells of fossil organisms. If finely disseminated through the clay it may be harmless or beneficial, but more usually it occurs in lumps, or nodules, which must be removed unless thoroughly crushed and intermixed. 8. Selenite. — Crystallised calcium sulphate, CaS04. 2H2O, which has already been referred to as the clay worker's " petrified water," results from the action of sulphuric acid on lime, or carbonate of lime. Its presence in the clay is objectionable for reasons given hereafter. 9. Dolomite. — Certain minerals containing magnesium, such as biotite mica, lead to the production of dolomite — calcium-magnesium carbonate — to which the remarks made upon the presence of calcite may be applied. In making certain bricks for furnace linings the presence of magnesia, properly disseminated, is of value. 10. Carbonaceous Matter. — Vegetable and animal remains are naturally not uncommon in clays, and often largely account for the natural colours they possess. Usually such matter is found in the form of leaves or twigs, or sometimes as peaty layers. In some clays the organic remains are BEICK AND OTHEE CLAYS 153 present in such quantity that the combustion of this material in the kiln is sufficient to provide the whole of the heat necessary after firing has been started. This is the case, for example, in the Oxford clay, as used at Peter- borough for the manufacture of Fletton bricks, where the material almost assumes the character of an oil shale. The effect of such matter on the plasticity of clay has been commented upon, but there are objections to, as well as advantages in, its presence in the case of clays of low fusibility, as will be shown. V. Drying of Clays. The drying of moulded clay as a preliminary to its treatment in the kiln is an operation which requires con- siderable care, as any defects there developed will probably be accentuated on burning. Drying is the removal of such water as will evaporate at ordinary air temperatures, and the rate at which this can be safely effected depends upon the size and configura- tion of the moulded material, the amount of water it con- tains, the quantity of colloidal constituents present, the power of adhesion possessed by the particles, and the porosity of the material. Clays in their natural state may contain, without any special appearance of wetness, as much as 30 per cent, of evaporable moisture, which increases with their porosity, and as far as composition is concerned., particularly with the amount of hydrated iron oxide and carbonaceous matter present. When this moisture is removed, a contraction, which may exceed 5 per cent, of the original volume of the clay, takes place, and since the exterior parts lose water more quickly than the interior, the clay must be submitted to some internal strain, and the rate of drying, which will be a measure of the internal stresses involved, must not 154 CHEMISTRY AND PHYSIOS OF BUILDING MATERIALS exceed the adhesive power of the particles, or rupture will result. For this reason tensile tests on dried unburnt clay are often made in order to gain an insight into the comparative power of different clays of resisting strains produced in drying. These tests are carried out in the same manner as similar tests upon cements, which will be referred to under this heading. The results of such tests show that the clays capable of resisting the largest strains are those which contain particles which vary in size. This is true generally of binding materials in which graded aggregates are found to be stronger than wholly j&ne or wholly coarse particles. Colloidal bodies part with water extremely slowly, as they form therewith a kind of emulsion. Their presence also, by decreasing the general porosity of the material, retards the evaporation of water not actually entangled in such bodies. The presence of large quantities of non- absorbent minerals, such as quartz, much increases the rate of loss of water on exposure, and though clays of this character possess low tensile strength, inasmuch as the shrinkage which they undergo is small, drying may be safely allowed to proceed in them with greater rapidity. Though the washing and subsequent drying of clays is necessary, generally speaking, certain clays which are quarried in a dry state may be reduced to powder and moulded directly in suitable machines. Pressed bricks, such as Flettons, are produced in this manner, which is obviously exceedingly economical when practicable. VI. Fusibility of Clays. The fusibility of a clay, upon a knowledge of which correct firing must be largely based, is dependent upon its composition and fineness of grain, and it is upon the BEIOK AND OTHER CLAYS 165 temperature of fusion, coupled with considerations of colour, that the acceptance or rejection of a clay for a particular purpose must chiefly rest. Clays for the pro- duction of china, terra cotta, earthenware, stoneware, fire- bricks, common bricks, slips for glazes, and other purposes naturally differ much in composition and mode of treat- ment. It is only possible here to present some general facts connected with the physical and chemical changes in clay burning, but since an endeavour will be made to deal with all the minerals of importance likely to be present, given the analysis of any particular clay, some knowledge as to its behaviour will, it is hoped, be obtainable. 1. Combinations Causing Fusion. — The melting point of a clay is determined by a very complex set of conditions. Certain compounds invariably confer this property and are known as fluxes, and the most important of these are the non-silicate compounds of the bases potash and soda. The chemical changes which occur in " burning " often result in the production of new substances which have lower melting points than the orignal constituents, and no doubt largely for this reason clays of fine grain melt more readily than those composed of coarse particles, for the smaller the particles the more readily will reaction take place between them. When the more infusible minerals unite to form com- pounds possessing lower melting points the proportions in which such minerals are present naturally influence the resulting temperature of fusion. Thus both lime and silica are individually quite infusible at any kiln temperature, but when heated together they form fusible silicates. In a certain proportion the most fusible silicate will be produced, but if either the amount of lime or silica be increased less fusible compounds or possibly uncombined lime or silica will result. It will thus be seen that the fluxing action of any ingredient is not by any means necessarily an 156 CHEMISTRY AND PHYSICS OE BUILDING MATEEIALS individual property to be assessed in proportion to the amount of such ingredient present. Similarly the oxides of iron, aluminium, and magnesium, and also the carbonates and sulphates of these metals, are all quite infusible individually, but in the presence of silica they may form fusible silicates. The amounts of lime, magnesia, and iron oxides are usually small as compared with silica, hence these compounds may be generally rightly regarded as fluxes, and since silicates of iron melt at a lower temperature than those of lime or magnesia, iron is a more powerful flux and its presence in quantity often precludes the use of clay for burning. 2. Mixtures of Fluxes. — When two substances are melted together the melting point of the mixture is usually much lower than that of either of the substances alone. Fluxes have thus the power not only to help the general fluidity of the material owing to their molten condition, but, as it were, to induce fusion in other bodies to some extent, and, further, by the increased freedom of molecular motion which they enjoy as liquids they promote chemical actions which in their absence might not be able to take place. 3. Molecular Proportion and Fusion. — Eichter^ has endea- voured to show that the molecules of all fluxes when present in small quantities have an equal effect in pro- ducing fusibility : that is, for example, that one molecule of lime (CaO), i.e., 56 parts of weight, would lower the melting point as much as one molecule of ferra (FeaOs), i.e., 160 parts by weight, or one molecule of potash (K2O), i.e., 94 parts by weight. It is known that the freezing and boiling points of solutions are equally altered by molecules of different compounds, and therefore this experimenter's conclusions are not unlikely to be well-founded. Assuming the truth of the above contention, the conver- sion of the iron in a clay from the ferric to the ferrous ^ Beferences will be found in Eies' book previously referred to. BEICK AND OTHEE CLAYS 157 condition, that is, from Fe203 to FeO, will, as pointed out by Eies, double its effective amount, since one moleeule of Fe203 will form two molecules of FeO. Such a change may be brought about by an undue exclusion of air from the kiln on burning owing to but partial combustion of the fuel resulting in the formation of carbon monoxide, thus : — FeaOg + CO = 2FeO + CO2 The above forms an interesting example of the direct practical bearing of what may appear a somewhat abstruse chemical consideration. 4. Stages of Fusion. — Ries classifies the stages of the melting of clays into: (1) Incipient fusion; (2) vitrification; (3) viscosity. The stage to be aimed at is to some extent dependent on the ware to be produced ; in common bricks, for example, incipient fusion is usually sufficient, but in the case of stoneware, vitrification must be attained. Viscosity is to be avoided, since the material naturally loses its shape when it reaches the temperature initial to liquefaction. Though no very definite line of demarcation can be drawn between these stages, their recognition is of value because upon the temperature intervals between them the ease or difficulty of burning a given clay depends. The above writer points out that in extreme cases incipient fusion and viscosity may be separated by so small an interval as 24° G. Such a condition, which might be expected in a clay very rich in potash and soda, iron or lime, would involve extreme difficulty in correct firing and almost certainly result in the production of under-burnt (slake-baked) materials in the endeavour to avoid the loss which attaining the viscosity temperature would involve. In good classes of ordinary clays three or foar times this range of temperature may be looked for, while in fireclays, though incipient fusion takes place at about 1,300° C.,the pro- duction of viscosity requires a temperature of over 1,600° C. CHAPTER XV CLAYS (continued). — kiln reactions and the properties OF BURNT CLAYS I. Kiln and Subsequent Behaviour of Minerals. An introduction to the problems connected with burning clay has formed the subject of the preceding section in Chapter XIV. The probable changes which take place in the various components of clay in the kiln must be also con- sidered, and such changes will be arranged as far as may be in the order in which they seem likely to occur, though it will be evident from the remarks upon fusibility that no definite lines of demarcation can be expected for such re-actions. 1. Compounds of Ammonia. — When nitrogenous organic matters decay out of contact with air, various salts of ammonia are formed on the application of heat. These compounds are, like those of potash and soda, powerful fluxes, but they are ail easily volatilised, and if present in clay they are expelled as gases before they can produce any effect in promoting fusion. 2. Water. — Dried clays often contain 10 per cent, of water chemically combined and, therefore, incapable of evapora- tion. Such water is contained in carbonaceous matter, limonite (hydrated ferric oxide), gypsum, kaolin, sodium sulphate and carbonate, mica, and sulphate of iron, pro- duced by decomposed pyrites. This water, which is all finally expelled, is liberated at very different temperatures. From carbonaceous matter and such compounds as limonite KILN EEACTIONS— PEOPERTIES OF BUENT CLAYS 159 and gypsum, it is evolved at temperatures not much exceeding 100° C, whereas kaolin and mica must be heated to redness (600° or 700° C.) before such expulsion occurs. Since this water is evolved as steam, firing must be con- ducted with special discretion through the ranges of its most abundant escape, as otherwise the ware may be injured in the same manner as by too rapid air-drying. During the escape of this steam it is very important that an efficient draught be maintained to prevent the forma- tion of sulphuric acid from the pyrites, as explained in Chapter VIII. 3. Carbonaceous Matter. — All organic matters in clay undergo in the kiln decomposition and distillation similar to that described as taking place when coal is heated, and an oxidising atmosphere, that is, efficient supply of air, is most necessary during such distillation. Carbon itself is quite non-volatile and infusible, and in the absence of air may be heated indefinitely without change ; hence even the highest temperatures will fail^ to remove it in a closed kiln, and the discolouration thus pro- duced in the ware might be very serious. Much greater evils, however, may result from such incomplete combus- tion. The tarry matters distilled from such sources may, if unoxidised, be unable to pass out through the pores of the clay before surface vitrification has taken place, par- ticularly in the case of clays possessing low melting points. Such matters will then become permanently enclosed, and from such ware used in a fractured condition (as, for instance in the case of half bricks in walling) these tarry substances will be likely to exude and to find their way through plaster and decorations. It is hardly necessary to point out the importance of attention to such considerations as these when mural painting or other elaborate forms of decorative treatment are in prospect. 4. Magnesium Carbonate. — Magnesium compounds are 160 CHEMISTHY AND PHYSICS OF BUILDING MATEEIALS not usually found in clays in quantities much exceeding 1 per cent., unless the material is distinctly dolomitic. Carbonate of magnesia decomposes into magnesia (MgO) and carbon dioxide at a much lower temperature than is necessary to effect a similar decomposition in carbonate of lime. Eecent experiments have shown that magnesia and lime are not at all similar in their effects upon burnt clays. Magnesia does not appear to exert the bleaching action upon the colour of the ware, nor to produce sudden vitrifi- cation characteristic of calcareous clays ; it seems rather to separate the points of incipient fusion and viscosity, and to counteract any tendency towards warping. No explanation of these characters seems to be forth- coming. Possibly they are due to the less basic character of magnesia, which should result in a lesser tendency to com- bine with silica than is displayed by lime. The observed effects of its presence are certainly such as would be expected if this base remained uncombined. 5. Magnesium Sulphate. — This salt, unlike calcium sul- phate, is very soluble in water and is, therefore, hardly likely to be found in washed clay. It may, however, be produced in the same manner as calcium sulphate (see p. 161). Its presence is likely to result in efflorescence. 6. Calcium Carbonate. — Ordinary clays seldom contain more than 3 or 4 per cent, of carbonate of lime, though in many marls the amount is much higher, and clays contain- ing as much as 20 per cent, have been successfully employed for brickmaking.^ The state of division of this compound is of vital import- ance in considering the percentage permissible. When heated, evolution of carbon dioxide begins at about 400° C, 1 "The Clays of Alabama." H. Ries. Geological State Bulletin, U.S.A. KILN REACTIONS— PEOPERTIES OF BURNT CLAYS 161 but the expulsion of this gas and the consequent con- version into free lime (CaO) is probably incomplete below 950° C. The objection to free lime in burnt clays is due to the great heat and consequent disruption caused when slaking occurs. In minute fragments partial combination with silica may occur, and the porosity of the ware is usually sufficient to admit of the expansion of the free lime with- out damage, while the local rise of temperature is too slight to be destructive ; but when particles of any size are present the heat and expansion resulting from the access of water in any moist situation have been known to cause disruption sufficient not only to split and shell brickwork, but to throw a wall built of such defective bricks out of the perpendicular. Lime has a bleaching effect on the colour of well-fired bricks. This is probably due to the withdrawal of some of the iron oxide with silica to form complex silicate minerals. 7. Calcium Sulphate. — This objectionable compound may be present in the original clay as a secondary mineral, as explained, or may be formed owing to the action of sul- phuric acid resulting from the weathering of pyrites or marcasite upon carbonate of lime. Another possible source of calcium sulphate is use of water possessing much permanent hardness for clay washing. Though clay may be absolutely free from sulphate of lime, this compound may yet be produced in the kiln, either due to the decomposition of iron pyrites contained in the clay, when the formation takes place in a similar manner to that which occurs on weathering, or due to the presence of sulphur compounds in the coal used for firing. This latter source of calcium sulphate often fails to receive the attention it deserves. Coal has been shown to contain varying amounts of sulphur, usually in the form of iron pyrites (Chapter IX.), and when burnt the sulphur 162 OHEMISTEY AND PHYSICS OF BUILDING MATEEIALS therein is converted into sulphur dioxide (SO2) gas. In the presence of air and moisture sulphuric acid is produced, which acts upon lime or carbonate of lime in the heated clay, as follows : — CaO + H2SO4 = CaSOi + H2O CaCOa + H2SO4 = CaS04 + H2O + CO2 In the absence of water it is doubtful whether any action between lime and oxidised sulphur takes place, hence the importance of guarding against a stagnant atmosphere in the kiln when water is being evolved. Coals used for firing should be submitted to an analysis for sulphur, and only such varieties used as contain but small quantities of this element. The objection to sulphate of lime lies in the fact that it produces efflorescence. Slightly soluble in water, it finds its way in solution to the surface of the material exposed to a moist atmosphere, and when evaporation takes place, owing to heat or dryness, it forms an unsightly salt-like incrustation, which constantly repeated removal can alone at last eradicate. 8. Ferrous Oxide and its Compounds. — Iron is found in clay partially oxidised, that is, in the ferrous condition, and also fully oxidised as ferric oxide. Ferrous oxide (FeO) never occurs uncombined, but is often found in small quantities in combination with carbon dioxide as carbonate of iron (FeCOs), which is decomposed at a low temperature with the momentary formation of FeO, which, in the presence of a good air supply in the kiln, is oxidised to Fe203 ; thus 2 FeO + 0 = Fe208. In the absence of sufficient air, however, its tendency will be to combine with silica to form ferrous silicate — FeO + SiOa = FeSiOa Since silicate of iron is easily fused, ferrous iron is especially liable to act as a flux in clays. KILN EEAOTIONS— PEOPEETIES OF BUENT CLAYS 163 An intermediate stage of oxidation between ferrous and ferric oxides is known, in which one molecule of each of these oxides is combined to form a compound FeO.Fe203 or FeaPi. This oxide is black and it may be produced in burnt clay by a premature cessation of the oxidising process due to rapid heating, if this causes incipient fusion of the outer layers of the material, while ferrous oxide still exists in the interior. The black cores often found in ill-burnt bricks are generally due to the presence of this inter- mediate oxide, though often erroneously attributed to carbon. As this oxide is quite insoluble no ill effects similar to those to be expected from enclosed tarry matters need be feared from it. The presence of carbonaceous matter naturally tends to keep the iron in the ferrous condition, as it itself absorbs the oxygen in the kiln atmosphere during its combustion. 9. Ferric Oxide. — Present in a hydrated state as limonite, or anhydrous, as haematite, this oxide (FeaOa) is often abundant in clays, and accounts almost entirely for the colour of the burnt ware. The colour increases in intensity in proportion to the amount of this oxide present ; 2 to 3 per cent, result in a yellow tint, 4 or 5 per cent, will pro- duce a red tint, but the actual colour obtained will be modified by the presence of other compounds, particularly by lime, and, in a lesser degree, by alumina, which, by forming with the iron oxide less highly coloured compounds, exert a bleaching action upon the ware. Iron in a fully oxidised state, as Fe203, does not combine directly with silica, and thus its fluxing power is negligible. This is only true, however, if it does not undergo reduction (de-oxidation), which may be brought about by insufficient air in the kiln atmosphere, as explained under the section on Fusibility of Clays in the last chapter. At a high temperature also decomposition may take place B.M. M 164 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS in the presence of silica, resulting in the liberation of oxygen, which may cause blistering, and the ferrous oxide which results then combines with the silica, forming a flux, as already explained — FeaOa + SiOa = SFeSiOa + 0 10. Iron Pyrites. — The sulphides of iron are, in the absence of oxygen, very stable, even when highly heated, but in an oxidising atmosphere they lose half their sulphur at a red heat and the remainder at a temperature approach- ing a white heat. The products of such decomposition are the oxides FeaOs and SOa. The conversion of the gas SOa into sulphuric acid, and its action upon lime, has already been explained. If iron pyrites occurs in the clay in pieces of any size its decomposition will be attended with disruption not only due to the evolution of gas but because the oxide of iron formed is greater in volume than the original pyrites. 11. Potash and Soda. — Potash and soda (KaO and NaaO) are, when present, always found in combination as silicates, chlorides, sulphates, carbonates, or phosphates. The silica compounds are very infusible. Orthoclase felspar, for example, melts at about 1,200° C, and mica remains unfused even at 1,400° C. Other compounds of these bases, however, have comparatively low melting points, and act as powerful fluxes, as already stated. Though the presence of such compounds in quantity precludes the use of clays for burn- ing, a small amount is often advantageous, since this, on melting, frits the less fusible minerals together. The molten salts of these bases are readily attacked by silica with the formation of silicates. Thus in the case of sodium carbonate the reaction may be given as : — NaaCOs + SiOa = NaaSiOs + COa If potash and soda are present as soluble (non-silicate) compounds, even in very minute quantities, it is most KILN EEACTIONS— PEOPEETIES OF BURNT CLAYS 165 necessary that they should be converted into silicates as above shown, since otherwise they will undoubtedly give rise to efflorescence, the formation of which has been referred to as also due to sulphate of lime. 12. Summary of Temperature Changes. — From the above attempted outline of the behaviour of compounds in the burning of clay it will be evident that many of the changes enumerated must go on simultaneously or be dependent upon the fulfilment of certain conditions. Under this reservation, and even then, doubtless, open to some criti- cism, the following changes may perhaps be considered to take place with advancing kiln temperature : — 100° C. Volatilisation of certain compounds of ammonia and expulsion of water from some sodium salts. 200° C. Loss of water by calcium sulphate, limonite, car- bonaceous matter, and in part from kaolin. 800° C. Carbonates of magnesium and iron begin to decompose. 400° C. Above decomposition complete. Calcium carbonate begins to decompose, evolution of water from kaolin and carbonaceous matter continues. 500° C. Ferrous oxide in presence of air oxidised to ferric oxide. SO2 from furnace gas acts on lime in presence of moisture and air. 600° C. Above changes continue. Organic matter under- goes combustion. 700° C. Iron pyrites decomposed with combustion of half its sulphur. Dehydration of kaolin complete. 800° C. Sodium chloride and sodium carbonate melt. 900° C. Potassium carbonate and sodium sulphate melt. Iron pyrites entirely burnt to Fe203. Expul- sion of CO2 from calcium carbonate complete. Carbon from carbonaceous matter burnt away. 1,000° C. Ferric oxide attacked by silica, forming ferrous silicate ? M 2 166 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS 1,100° C. Calcium and sodium sulphates decomposed into free bases and SO3. Melting point of ordinary brick-clays. 1,200° C. Orthoclase felspar melts. Vitrification of more refractory clays. II. — The Eemoval of Defects in Clays. Where clays of variable composition are to be found in one brick-field the proportions of certain constituents which may be unsuitable in a single clay may often be advan- tageously modified by making suitable mixtures with the clay from other workings. Excess of soluble salts of potash and soda may be some- times removed by prolonged weathering, though this is not an attractive process commercially. Eflorescence due to the presence of calcium or magnesium sulphate may be to some extent alleviated by the addition to. the clay of barium carbonate before burning. This compound is found as the mineral witherite (BaCOs), which much resembles calcium carbonate (CaCOa), but is not decomposed by heat. In the kiln it reacts with calcium sulphate (or magnesium sulphate) as follows : — CaS04 + BaCOa = BaS04 + CaCOg The barium sulphate (BaS04) thus formed is quite insoluble, and hence does not give rise to efflorescence in the finished ware. The amount of witherite necessary may be calculated from the amount of calcium sulphate which would otherwise be present, but excess must be used, as the whole does not come into contact with the calcium sulphate. Witherite further reacts with sulphur dioxide, air and moisture, forming sulphate BaSOi, and thus helps to prevent the action of kiln gases upon the lime compounds. Barium chloride (BaCl2) has been employed in place of KILN EEACTIONS— PEOPERTIES OF BUENT CLAYS 167 the carbonate because, being soluble, it is more easily disseminated through the clay ; but since it produces soluble deliquescent calcium chloride, which remains in the burnt material, it merely removes one objection to add another. Its reaction upon calcium sulphate is as follows : — BaCl2 + CaS04 = BaSO* + CaCl2 III. — Examination and Tests upon Clay Ware. Nearly all the tests described in Chapter XIII., in reference to building-stones, are also applicable to bricks and other materials composed of burnt clay ; but few of such tests are usually carried out, and some of them would have but little commercial value. Mechanical tests upon bricks are usually confined to the determination of crushing strength, but as bricks do not bear stresses individually but in connection with a vast number of interspaces more or less filled with mortar, the results of experiments upon single bricks do not give much indication of the strength of brickwork. The results of a series of tests upon the crushing strength of brick piers, carried out by the Eoyal Institute of British Architects,^ have shown that the quality of the workmanship in the building of brickwork is capable of producing the most marked differences in the strength of brick erections, so that a generous factor of safety or very rigid supervision in building must be allowed for. Many of the defects in bricks and tiles cited as possible owing to faulty composition or firing are open to visual detection, and enough has been said to show the value of chemical analysis or at least of the determination of the presence, amount, and dissemination of certain possible constituents. 1 R.I.B.A. Journal, April, 1896 ; December, 1896 ; December, 1897. CHAPTER XVI PLASTERS AND LIMES I. Binding Materials Classified. Under the title of " binding materials " are to be included some of the most important and interesting substances con- nected with building products, namely, the various limes, plasters, and cements which to so large an extent deter- mine the permanency of any structure. These substances, presented as they are to the user in the form of powder, do not admit of the direct judgment as to their characters which is possible in the case of stones and bricks; and it is, therefore, the more necessary to carefully consider their chemical compositions and reactions in preparation and use. Binding materials may be classified according to their composition, uses, and the strength they display as cement- ing media, and may be briefly described as follows : — (a) Plasters. — Though fat limes are used for plaster work, all plasters proper consist mainly of sulphate of lime in a dehydrated condition, and set owing to the absorption of water. (b) Limes. — All limes are characterised by containing free lime (calcium oxide), and slake on the addition of water. The non-hydraulic varieties contain little else, and harden largely by mere mechanical drying. The hydraulic limes contain in addition silicates which, when decomposed by water, set in a manner similar to that observed in cements. (c) Cements. — All cements are distinguished from limes PLASTEBS AND LIMES 169 by the fact that in them excess of lime is absent, and that since no slaking action takes place with water they must be finely ground before use. The most important cements are formed artificially by heating together chalk and clay. (d) Pozzuolanas. — These bodies are siliceous and argil- laceous materials which develop hydraulic properties when mixed with lime. They may be natural volcanic products, or slags produced in various industries. The following tabular arrangement will make the rela- tions between these materials clearer : — Binding Materials Plasters I Limes Cements Plaster Flooring of Paris Plaster Non-Hydraulic Natural Roman Natural Portland I Hydraulic Pozzuolanas Artificial Portland I I Natural Artificial III I I Fat Lean Dolomitic Feebly Strongly Hydraulic Hydraulic Selenitic Grappiers I I Clay Slag II. Plastees. Plasters are essentially composed of sulphate of lime, and are prepared from the mineral gypsum (GaS04.2H20) which is found in rocks of all ages, but in this country chiefly in the Triassic formation. Gypsum often occurs remarkably free 170 CHEMISTEY AND PHYSICS OP BUILDING MATEEIALS from impurities ; but is sometimes discoloured by iron which, in the form of oxide, remains in the plaster prepared, and thus decreases its value. 1. Plaster of Paris, — When gypsum is heated to a tem- perature between 120° and 130° C. it loses three-quarters of its water of crystallisation, and the partially dehydrated sul- phate formed is known as " plaster of paris," which, on the addition of water equivalent to that removed, re-crystallises as gypsum and thus " sets." Gypsum. Plaster of Paris. 2(CaS04.2H20) = 2CaS04.H20 + SHaO. 2. Flooring Plasters. — When gypsum is heated to 163° C. it loses, according to Le Chatelier, a further quantity of its water, and at 194° C. is completely dehydrated. If maintained for a long time above this temperature, or raised to a red heat, the plaster becomes incapable of absorbing water in, at least, any reasonable period, and is then said to be " dead burnt." The power of absorbing water and setting is not, however, lost after all water of crystallisation is expelled, if heating be continued for a limited time at not too high a temperature. Gypsum so treated and subsequently finely ground forms what is known as " flooring plaster," which sets slowly with water, producing a very hard material. 3. Keene's and Similar Cements. — Keene's, Parian and other plasters, which finish with a hard face, are made by heating very pure gypsum to redness and soaking the resulting dehydrated mineral in a solution of alum (for Keene's) borax, sodium or potassium sulphate, or potassium carbonate. The mineral is then heated a second time and finely ground. The quantity of alum or other salt taken up from the solution is quite small, often forming much less than one per cent, of the plaster, which is, therefore, essentially the PLASTERS AND LIMES 171 same in composition as flooring plaster. Some sugges- tions as to the action of the salts taken up from the solutions will be found in Chapter XIX. By far the greater number of the many patent plasters in use, such as Serapite and Asbestic plasters, owe their bind- ing power chiefly to the above derivatives of gypsum. III. Non-Hydraulic Limes. The limes which fall under this heading have been classified as fat limes, lean limes, and dolomitic limes. Though each of these groups shows in typical examples characteristic properties, it must be borne in mind that, as previously emphasised, all natural materials show gradations and merge one into the other ; but a study of typical examples will enable a judgment to be formed upon the qualities of such limes as may be found in practice to possess intermediate compositions. 1. Fat Limes. — Ideal fat lime consists solely of calcium oxide produced by the decomposition of calcium carbonate (chalk) by heat — CaCOg = CaO + GO, Although in practice pure calcium carbonate is unobtain- able in quantity, certain stones, such as those used for preparing lime used for the manufacture of calcium carbide, approach this ideal very closely. The usual impurities present consist of alumina, iron oxides, silica and magnesia, and a lime is classed in this group when such total impurities estimated after " burning " do not exceed 5 per cent, of the material. The specific gravity of pure lime, although it varies to the extent of about 0*06 per cent, according to condition of burning, may be taken as 3*1, to which the specific gravity of fat limes in the lump should therefore approximate. 172 CHEMISTEY AND PHYSIOS OF BUILDING MATEEIALS The chief characteristic of fat lime is the great develop- ment of heat which occurs when water is mixed with it, and the large expansion which the material undergoes on hydration. Indeed, before the discovery of gunpowder lime cartridges were used for blasting purposes on account of this property. This slaking action is represented as follows : — CaO + H2O = CaOaHa So sudden and violent is this action that the hydrated lime produced on the direct addition of water always forms a friable mass quite devoid of cohesion, but under suitable conditions this hydrate may crystallise, when its mechanical properties will be very different. Fat limes are only suitable for plastering, and their use for making mortar is quite inexcusable, since they possess no setting powers, and what hardening they undergo is due to mere mechanical drying, and in a very small degree to the formation of a thin surface layer of calcium carbonate owing to absorption of carbon dioxide from the air. Sand mixed with fat limes should always be clean and sharp, for the presence of clayey matters by decreasing porosity will prevent the progress of such mechanical hardening and carbonating as would otherwise take place. 2. Lean Limes. — Lean, or poor, limes are merely fat limes containing additional quantities of the impurities cited above, and show only some 80 per cent, of calcium oxide on analysis. Their use should therefore be restricted to the necessities of certain local conditions. These impurities, which, it will be seen later, must be regarded in another light in other classes of limes, are not in those under this heading sufficiently well distributed to admit of the develop- ment of any hydraulic properties therefrom, and for this reason are an actual objection in burning owing to the PLASTEES AND LIMES 173 danger of the production of inert material by local fusion. Lean limes are thus always liable to be underburnt, and therefore to contain inert carbonate of lime as an additional impurity. These limes are usually difficult to work, absorb water less violently than fat limes, and are greyish in colour, whereas good fat limes are white. 3. Dolomitic Limes. — Dolomitic or magnesian limes are those which contain a considerable proportion of magnesia. As has been pointed out, dolomitic stones usually contain large proportions of this base, and these limestones form the source of this group of materials. Magnesia is a much less active base than lime, hence dolomitic limes slake more slowly than fat limes, and they also increase less in bulk and are less workable and plastic than the latter. Although these limes acquire but little strength when used in mortars, they appear to be stronger than fat limes, probably owing to the lesser amount of mechanical disruption which takes place in the mass on slaking. The decomposition of magnesium carbonate in the pro- duction of these limes resembles that of calcium carbonate, but takes place at a much lower temperature. The equation is as follows : — MgCOa = MgO + CO2 Eckel ^ quotes tests which appear to show that, although dolomitic limes when mixed with sand as mortars are not at first superior in strength to ordinary fat limes, their strength increases with age till after one year they are twice as strong. Briquettes made up of 1 part of lime to 2 parts of sand showed a tensile strength after one year of 1 Eckel, " Cements, Limes, and Plasters." John Wiley & Sons, 1905. 174 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS 45 pounds for fat lime and 93 pounds for dolomitic lime per square inch. 4. Strength of Lime Mortars. — The strength of non- hydraulic limes in use depends much upon the character and proportion of the aggregate used with them, but by no means decreases in proportion to the aggregate added; in fact, tests are extant which show greater strengths for 1 to 3 than 1 to 2 mixtures, and in Sabin's results for 1 to 6 than 1 to 3 mixtures. Perhaps 30 pounds per square inch may be regarded as about the tensile strength of ordinary fat lime mortars, and the strength in compression as about 5 times as great. IV. Hydraulic Limes. 1. Characters. — The term "hydraulic" as applied to binding materials has lost much of its original significance which related to the power of setting under water, since such materials also set, and have a much more extensive use, in air. Hydraulic limes and cements owe their characters to the fact that silica and alumina, in the natural materials from which they are made, enter into chemical combina- tion with the lime formed on burning, which results in the production of silicates and aluminates of lime. On the addition of water these compounds are decomposed and their previous mechanical division, which is necessary for such decomposition, is effected by the free lime in the case of hydraulic limes, and by grinding in the case of cements. The theories advanced to explain the setting of these materials will be dealt with in Chapter XVIH. 2. Peehly Hydraulic Limes. — Limes under this heading include the many varieties of grey stone limes used for building work. They contain from 40 per cent, to as much PLASTEES AND LIMES 175 as 80 per cent, of uncombined lime, at which latter limit their hydraulic properties are of a very weak description. Chemical opinion is not unanimous as to the composition of the compounds of lime with silica and alumina, to the formation of which the subsequent development of hydraulic properties is due. In the strongest hydraulic compounds, lime, silica and alumina are present in such proportions as would form the silicate 3CaO.Si02 and the aluminate BCaO.AlaOa or 2CaO.Al203. The aluminate is generally present in comparatively small quantity, and is only necessary to admit, by its lower melting point, of the formation of the silicate. Neglecting the aluminate and calculating the proportion of silica and of lime in the silicate, it will be seen that in a hydraulic lime in which 80 per cent, of free calcium oxide exists only some 5 per cent, of silica present can be in combination. 3. Selenitic Limes. — Feebly hydraulic limes may be con- siderably increased in strength by the addition of small quantities of calcium sulphate. Limes so treated are said to be selenitised " and are referred to as selenitic limes, a designation derived from the mineral selenite, which is crystallised hydrated lime sulphate. The addition of this sulphate is usually made in the form of some 5 per cent, of plaster of paris, but the sulphate may be formed by the neutralisation of some of the free lime by sulphuric acid, thus : CaO + H2SO4 = CaSOi + H2O. The increase in strength produced by this treatment may be due to the retardation caused by a thin pelHcle of the but slowly soluble sulphate upon the lime particles, which thus obtain the water necessary for hydration much more slowly, and, therefore, with much less mechanical disruption when slaking takes place. This suggested explanation is due to Schott, but no evidence that this 176 CHEMISTEY AND PHYSIOS OF BUILDING MATERIALS coating action really takes place has yet been brought forward. Another explanation, based on the supersatura- tion theory of Le Chatelier (Chapter XIX.), may be possible. The actual increase in strength resulting from selenitising the poorer qualities of hydraulic limes is remarkable, and amply sufficient to repay such treatment. From experiments carried out by Grant, it would appear that the strength of mortars of lime and sand in various proportions is, on an average, doubled by such treatment, it has been shown, for example, that a mortar of 1 part untreated lime to 3 parts of sand has almost the same strength as one consisting of 1 part of the same lime selenitised with 5 parts of sand. Selenitic limes, or cements as they are often called, are employed chiefly for plastering, but there seems to be no reason why they should not be more extensively used for ordinary building mortars. The objection is often advanced that the sulphate of lime is soluble in water and thus unsuitable for exposure. One thousand parts of water at ordinary temperatures dissolve about 1| parts of slaked lime and about 2 parts of sulphate of lime. This difference in solubility is not great, and inasmuch as a selenitised lime still contains 10 to 16 times as much free lime as sulphate, such mortars would appear to be likely to lose more free lime than sulphate by solution due to atmospheric moisture. The process of selenitising is confined to the feebly- hydraulic limes, as the better classes of these limes and the cements do not show improvement on the addition of calcium sulphate, sufficient to Justify such treatment, and may indeed be injured thereby. 4. Eminently Hydraulic Limes. — This somewhat cumbrous title is applied to the better class of hydraulic limes which contain, after burning, some 60 to 75 per cent, of calcium oxide, partly in combination with silica and alumina. The PLASTEES AND LIMES 177 limestones from which such limes are prepared may be taken to contain some 70 to 80 per cent, of calcium car- bonate, some 13 to 17 per cent, of silica, and a variable percentage of alumina and ferra, say 1 to 6 per cent, in ordinary cases. The ideal hydraulic lime would be that in which the whole of the silica and alumina were in combination with calcium oxide, this base being present in excess just suffi- cient to cause complete disintegration of the silicate and aluminate formed in burning, by the disruption due to its slaking. In practice it is not found possible to bring the whole of the silica into combination, though such combination is considerably assisted by the alumina and ferra present. The best hydraulic limes thus contain a much larger percentage of free lime than would appear to be the case on the assumption that all the silica is present in the form of the compound 3CaO. Si02 after burning. Thus an analysis of blue lias lime, which belongs to this class, supplied by Messrs. Nelson, of Bugby, shows 61 per cent, of CaO and 20 per cent, of Si02. If the relative weights of lime and silica in the compound 3CaO.Si02 be calculated, it will be observed that 61 per cent, of CaO requires about 22 per cent, of SiOa for combination, which in the lime in question would leave no free lime over for slaking action ; and since this action does occur, a considerable percentage of the silica must, after burning, be present in an uncombined condition if the formula SCaO.SiOg is to be accepted. As will be seen, however, in Chapter XVIII., the base and acid oxide possibly form the compound 2CaO.Si02, and this view certainly accords better with the proportions of the constituents found in the best classes of hydraulic limes. The well-known lime from Lyme Regis contains some 24 per cent, of silica, while the famous limes from Teil (France) contain a similar quantity which, in the presence 178 CHEMISTEY AND PHYSICS OF BUILDINa MATERIALS of not too small a percentage of alumina, may therefore be regarded as an indication of a lime of high quality. The efficiency of the burning which such limes have undergone may be judged by freedom from carbonate which evolves the gas carbon dioxide when treated with an acid. 5. Grrappiers. — Although it would appear from the above remarks that hydraulic limes are completely disintegrated on slaking, this is not actually the case with the better class of such materials. The reactions between the lime, silica and alumina in the kiln result in the fusion of these materials, and owing to the imperfect distribution of these compounds, such fusion is found to vary much locally in its completeness. In places, silica and alumina are found combined with lime with but little intermixed free lime, and here fusion has been too far advanced to admit of the disintegration of such masses by the subsequent slaking of surrounding lime particles, hence such fused masses remain as lumps in the slaked product. These lumps, consisting as they do chiefly of calcium silicate, form a valuable cement when ground ; they are, therefore, separated and reduced to powder, in which form they are known as grappier cements. This material resembles natural cement in its formation and general characters, but as even the best varieties con- tain 3 or 4 per cent, of entangled limestone which has escaped decomposition, and as the grinding is not usually carried out to a great degree of fineness, the material is much inferior to Portland cement in strength. V. Testing op Hydraulic Limbs. 1. Chemical Analysis. — It is obvious that the analysis of limes from limestones which are natural products covering wide areas, must often differ in a marked degree even for products which may be placed in the same general category, PLASTEES AND LIMES 179 and further, that if comparable analyses are to be expected, these must be made under comparable conditions. Limes readily absorb water and carbon dioxide from the air when exposed ; hence, unless analysis is possible immediately the material is drawn from the kiln, the samples to be examined should be at once selected and kept in stoppered bottles. A great number of analyses of limes and limestones are recorded in works upon cementing materials, but the analysis of the stones is not of much interest to the user. In examining the analysis of limes the completeness of the burning may be judged by the amount of carbon dioxide remaining, and the hydraulicity may usually be assessed by the amount of silica present. The following table of limes from the kiln will serve to give an idea of the composition of the materials dealt with in this section : — (1) 1 Grey Stone Lime, Mersthara. Blue Lias, Eugby. (3) Lyme Regis Lime. (*) Typical Grappier Cement. Lime (CaO) 80-24 61-17 71-9 63-0 SUica (SiOi) 11-40 20-04 24-3 26-5 Alumina (AI2O3) . 4-97 3-7 2-5 Ferra (Fe^Os) . j 4-60 6-10 1-5 Magnesia (MgO) 0-5 0-95 1-0 Carbon dioxide (CO2) 2-0 4-03 0-0 60 and water (HgO) Alkalis (K2O and^NaaO) 1-25 1-08 CO 1 Authority : (1) Middleton ; (2) Messrs. Nelson ; (3) Blount and Bloxam • (4) Le Chatelier. ' 2. Mechanical and Other Tests. — No very strictly organised series of tests is demanded by users of hydraulic limes, who are often content to regard any lime which is not termed grey stone lime as necessarily eminently hydraulic. Owing to the variable amount of iron which these limes B.M. N 180 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS contain, no very satisfactory evidence of quality can be based upon colour, but specific gravity determination will serve to distinguish these materials from Portland cement. The average specific gravity for grappiers may be taken as about 2*7, and for hydraulic limes as about 2-9, whereas that of Portland cement is 3'1. (a) Tensile and Compression Strength— The determination of tensile strength as estimated by the force required to produce rupture by pulling, is always given so prominent a position among tests on binding materials that some comment upon its value is called for, inasmuch as such materials are never purposely submitted to tensile stresses but are always used in compression. Tests of materials under tension are always more reliable and more easily carried out than tests under compression. The apparatus necessary is less cumbrous and costly, and accurate results are obtainable with smaller specimens. These facts would, of course, not offer any excuse for making tests which bear no relation to the practical use of the materials. It has, however, been ascertained that a fairly constant ratio exists in limes and lime mortars between strength in tension and compression, and Eckel places the compressive strength of hydraulic limes at five to six times their tensile strength, in substantiation of which he quotes experiments by Schoch on mortars com- posed of 1 part of lime to 3 parts of sand. Average Strength of good Hydraulic Limb Mortars. Seven. Days. Twenty-eight Days. One Year. In tension In compression 64 356 100 683 299 1920 As an illustration of the strengths of feebly hydraulic and selenitic limes Kirkaldy's results, given in detail by PLASTEES AND LIMES 181 Eedgrave/ may be cited. An average of the results of experiments on common mortar in proportions of 1 to 2, 1 to 3, and 1 to 4 showed strengths of : in tension 24 pounds, in compression 122 pounds, and in tension as a joint between stock bricks 8 pounds, per square inch. In the case of selenitic lime mortars of 1 to 4, 1 to 5, and 1 to 6, the same lime selenitised showed, as an average of similar experiments, strengths of : in tension 64 pounds, in com- pression 285 pounds, in tension as a joint between stocks, 17 pounds per square inch. Some tests by McKenna, quoted by Eckel, place the tensile strength of certain grappier cements at about 650 pounds per square inch neat after one year, which appears to bring their strength nearly to full development. The addition of 2 parts of sand (1—2) seems to reduce the strength to a little more than one-half of this amount. I Redgrave, "Calcareous Cements: their Nature and Uses." 1 of lime to 2 of sand. N 2 CHAPTER XVII CEMENTS I. Relations between Limbs and Cements. Cements differ from limes in that they are "burnt" at a much higher temperature, which results in more effective chemical combination between the acids and bases and the production of semi-fused lumps. As a result, cements do not slake with water, and must be ground to extreme fineness in order to allow water to effect its full decom- position before the material sets, after which any further slaking action of water only takes place with extreme slow- ness, and tends not towards further strength but disruption. These building materials are very much superior to even the best hydraulic limes, but the special plant required for mixing, burning and grinding makes their cost considerable. Cements may be classified as natural and artificial. The former, of which Roman cement is the best known repre- sentative in this country,! ^re produced by^ the direct burning of natural argillaceous stones, which usually contain a considerable excess of the acid forming oxides, silica, alumina, and ferra. The latter are practically com- prised in Portland cement made from a mixture of chalk and clay so proportioned that acids and bases are present in quantities to admit of effective combination, in which circumstances the greatest strength is obtained. Chemically, then, the natural cements err in containing » Some of the so-caUed Uas limes are really natural cements. CEMENTS 183 excess of acids, just as the hydraulic limes err in excess of bases (free lime), and the relations between these three classes may be made clear thus : — ^^Geeatbst Stebngth.v^ Excess of Bases. Excess of Acids. Hydraulic Limes. Portland Cement. Natural Cements. II. Natubal Cements. 1. General Characters. — These cements are prepared by " burning " argillaceous limestones : that is, limestones con- taining a proportion of clayey matter. The process of burning is carried out at a much lower temperature than in the case of Portland cement, and the semi-fused product, or clinker, formed is much more friable and therefore more easily ground. These cements set very rapidly, owing to the large quantity of alumina which they contain. They may be further distinguished from Portland cement by their specific gravity, which seldom exceeds 2*8, and (unless this is artificially disguised) by their colour, since they are very ferruginous and thus possess a yellow or brown tint, very different from the blue-grey colour associated with the artificial product. Natural cements are not capable of bearing much dilution with sand when used as mortars, as great falling off of strength accompanies such additions. Though now little used in this country, where their employment is chiefly confined to repairs upon work where strength is of no importance, or for work exposed between tides when rapid setting is essential, these cements are extensively manufactured in America and other countries, where they largely take the place of our hydraulic limes. For general use, in order to decrease the rate of setting, plaster of Paris is often added, but it has been shown that this addition, in the case of cements, if made in any 184 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS quantity produces a considerable reduction in strength. The maximum amount allowable in natural cements is placed at about 1 per cent. The classification of the natural stones used in preparing these cements is not easy, as they present great variations in composition. Their products, however, may be regarded as represented by the following two groups. 2. Varieties of Natural Cements. — (a) Roman Cement. — This material is prepared from ferruginous nodules containing some 30 to 45 per cent, of clay, and is, perhaps, the best known natural cement used in this country. It is charac- terised by its rapidity in setting, and its brown colour. It rapidly deteriorates on exposure to the atmosphere, and is very liable to efflorescence after use. Medina, Whitby & Atkinson's cements resemble Roman cement and have similar uses. (b) Natural Portland Cement. — This somewhat unfor- tunate name is given to the product of certain natural stones, the ingredients of which resemble in composition those used in making Portland cement. Since, however, their composition varies considerably, and also because the " burning " is not effected in the complete manner adopted in the case of real Portland cement, this natural product is very inferior in strength to the artificial material. Eckel, quoting from a report on the Belgium cement industry, says in reference to such cement : " Cinders are often added, changing it to a grey colour resembling Portland. . . . This is the product which is purchased by unscrupu- lous exporters and sold by them marked as Portland cement." In fairness to the Belgian manufacturers, a further quotation from the report, pointing out that brand marks have been designed to protect purchasers who take the trouble to make their acquaintance, should be also cited. The low specific gravity and the large proportion of CEMENTS 185 calcium sulphate necessary to decrease the rate of setting should make cements of this character easily distinguishable from Portland. 3. Strength of Natural Cements. — The study of a large number of strength " curves " given in Johnson's " Materials of Construction " seems to indicate that natural cements rapidly increase in strength up to about six months, sub- sequent to which but little improvement is observable. The maximum tensile strength of neat American natural cements appears to range between 300 and 500 pounds per square inch, but it would not be advisable to adopt so high a standard as a safe guide for many natural cements used in this country. The ratio of compressive to tensile strength is naturally not easy to obtain satisfactorily in such variable materials, but the average results of twenty-nine experiments made by Sabin, on American cements, show a ratio very similar to that given in the case of hydraulic limes, namely, about 5 to 1. III. Portland Cement (Manufacture). 1. Introductory. — Not only is Portland cement the sole representative of any importance belonging to the group of materials known as artificial cements, but it far exceeds in quality and scale of production all other hydraulic materials. The cement, first manufactured in England and named from a fancied resemblance to Portland stone, is now made on a large scale in almost all civilised countries. The Portland cement industry, which must be placed only second to the iron and steel industry in respect to the application of scientific method and the attainment of accuracy and uniformity in production, owes its position to a great extent to the rigorous demands of engineers for material which shall comply with an exacting series of 186 CHEMISTRY AND PHYSICS OP BTJILDINa MATERIALS tests, and forms a useful object lesson as to what might be achieved in other directions for materials were the value of standardisation more widely appreciated. If materials were valued and sold on the basis of the characteristics which are sought for in them, such as strength, permanency and protective power, instead of by the more primitive standards of weight or bulk, very rapid industrial advances in many manufactures might be looked for. 2. Details of Mamifacture. — The object aimed at in the manufacture of Portland cement may be taken to be the production of material consisting, to as great an extent as is practically possible, of lime and silica in the propor- tion represented by the formula SCaO.SiOa. The manu- facture is carried out by the mixture and fusion of natural calcareous and siliceous materials. The substances employed to supply the lime are chalk and sometimes limestone or marl, and to supply the silica, clay and sometimes shale or even slate. These materials, besides lime and silica, which are the preponderating con- stituents, contain (1) alumina, which is a practical essential as a fluxing agent to admit of the combination of the lime and silica ; (2) magnesia and ferra, the influence of which in small quantities is not important ; (3) combined sulphur, which is not without its functions. The chalk and clay — the usual materials employed — in the proportion of about 3 to 1 are first mixed in mills containing water by the aid of rotating vanes carrying round iron drags, or in more modern practice when the ingredients are both found in a suitably dry and friable condition they are mixed in a dry state. The "slurry" obtained in the commoner wet process as a very liquid mud is kept in motion in large tanks or reservoirs, whence it is pumped into rotating cylindrical kilns slightly inclined from a horizontal position. These kilns, which are 60 to 130 feet in length and some 6 feet in diameter, are CEMENTS 187 lined with refractory firebrick and supplied with a blast of air and coal dust (or gas) at the opposite (lower) end to that at which the slurry is admitted. The burning of the coal dust produces an intense heat which evaporates the water from the slurry and drives off carbon dioxide from the chalk. The free lime thus formed combines with the silica and alumina in the clay at the high temperature attained in the lower part of the rotary kiln, which may exceed 1400° C. (a bright white heat). On leaving the kiln the semi-fused grey clinker " passes through rotating cylinders of very similar construction but supplied with internal vanes which, by alternately picking up and dropping the material, cause it to give up its heat to a natural current of air passing through this cooler. The air thus heated is supplied to the kilns in place of cold air with a proportionate saving in fuel. The cooled clinker is then ground to a state of extreme fineness by passage through other rotating cylinders half filled with rounded stones, during which process a small quantity of steam is admitted to ensure the complete slaking of any free lime which may have escaped combination. Portland cement is also made in stationary kilns which are developments of ordinary lime kilns, but owing to the increased output, powers of regulation and continuous working facilities possessed by the rotary kiln, this is rapidly supplanting the older forms of plant. IV. PoKTLAND Cement (Tests). 1. Introductory. — Some indication of the nature of the tests to which hydraulic materials are submitted has already been given, but only in the case of Portland cement have such tests been systematised. As pointed out in the case of stones, individual tests should have some bearing upon 188 CHEMISTEY AND PHYSICS OF BUILDINa MATEEIALS the use of the material. For example, though a knowledge of compressive strength is of value in the case of cement used for foundations, this has no interest when such material is required for lining a water tank. The usual tests by which the quality of a cement is judged are, how- ever, not as a rule differentiated according to the intended use of the material. These tests, which form the headings of the following paragraphs, are for : — 1. Fineness of grain ; 2. Specific gravity ; 3. Expansion ; 4. Tensile strength ; 5. Chemical composition ; 6. Eate of setting. 2. Fineness. — Fineness in cements is produced mechani- cally by continued grinding. The finer the material the greater the strength of the mortar produced from it, the more thorough is the action of water upon it, and the less is its porosity when set. Fineness is estimated by weighing the residue from a given weight of cement which fails to pass through a sieve containing a specified number of holes of given size per square inch. The meshes of such sieves are sometimes referred to by the number of holes in a row per linear inch, and sometimes by the total number of holes per square inch. Thus what is known as 180 X 180 sieve contains 180 holes per linear inch or 32,400 holes per square inch. This is the finest sieve in ordinary use,^ and so perfect is modern grinding that the higher grades of cement will leave considerably less than 10 per cent, of residue on such meshes. It is obvious that the gauge of the wire used in these sieves will materially affect the size of the holes. The wire employed for the sieve above referred to has a diameter of 0'002 inches. The strength developed by a cement depends not only upon its fineness but also on the size of the particles of sand or other inert aggregate with which it is mixed, and if the ^ A sieve possessing 200 holes per lineal inch, i.e., 40,000 holes per square inch, has recently been introduced from America. CEMENTS 189 full advantage of the fineness of high class cements is to be taken a suitable aggregate must be used. As grinding is a costly process, a limitation to the degree of subdivision economically obtainable would seem to exist, and some interesting " curves " showing such limit from relations between price and strength developed might be constructed. 3. Specific Gravity. — The determination of specific gravity, which has now taken the place of the measure- ment of weight per bushel, has no direct interest. Indirectly, however, it gives a valuable insight into the quality of the material, because the limes and lightly burnt natural cements never attain the density of Port- land cement, which may be taken as 3'10 to 3*15, whereas the former materials, as stated, range from about 2*7 to 2'9. The methods of determining specific gravity have been dealt with in Chapter II. In the case of cement the volume of the weighed quantity taken is ascertained by placing the material in a graduated vessel filled to a certain mark with paraffin oil and noting the rise in level produced. 4. Expansion. — No test on cement is more important than that for expansion, by which is meant the eventual increase in bulk which, possibly after a long interval, takes place in cement subsequent to use. All cements swell slowly after setting, and if such swelling, which is due to incomplete chemical action, is appreciable, great damage and disruption may result. Undue expansion is generally caused by excess of lime in the cement or by insufficient grinding or burning. By placing cement which has set, in hot water, evidence of expansion, which would normally be displayed only long after use, makes itself apparent in a few hours. A simple test is made by gauging with water on a plate of glass, and forming a thin pat of cement, which in shape should resemble a slice off a large sphere, and may be three or four inches in diameter and about half an inch 190 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS thick at the centre. This is allowed to set under cold water and is then placed for six hours in boiling water. If the cement neither leaves the glass nor shows cracks on its edges its soundness may be considered assured. A more accurate method, due to Le Chatelier, whereby the expansion may be measured, consists of filling a small split cylinder of sheet metal with cement gauged with water, and after allowing the mass to set and immersing it in boil- ing water as above, again measuring the distance between the adjoining edges of the metal which have by expansion been forced apart. To facilitate this measurement a long Fig. 6. — Le Cliatelier's split ring for measuring expansion in cements. prong is attached to each side of the opening, and the distance is actually measured between the ends of these prongs (Fig. 5). 5. Tensile Strength. — Some comments upon the reasons for making tensile tests upon cementing materials have been made on page 180, where it was stated that a relation between compressive and tensile strengths exists. This ratio is not the same as for hydraulic limes and natural cements, and may be taken in the case of Portland cement as 10 to 1, i.e., the results of tensile tests multiplied by ten give the approximate strength of the material under the same conditions and with the same amount of aggregate, under compression. Tensile tests are made by observing the force — the weight CEMENTS 191 in pounds — applied at the end of a lever, necessary to pull in halves a briquette of cement of dumb-bell shape of one square inch in sectional area in the middle. The briquette is fixed to a support below and gripped at the short end of the lever above, and the actual pull on the specimen is obtained by multiplying the force in pounds employed by the number of times the greater arm of the lever is longer than the lesser arm (Fig. 6). 10 WEIGHT / Fig. 6. -Principle of the lever as used in machines for tensile tests. 6. Chemical Composition. — Some account of the role played by the various compounds in cement will be found in Chapter XVIII. It may be said here that analysis is chiefly of value as showing {a) whether the bases and acids are present in proper proportion ; (&) proving the absence of inert and useless material ; and (c) as showing the amount of magnesia and combined sulphur present, which are prejudicial in excessive quantities. (a) Portland cement consists substantially of lime (CaO), silica (Si02) and alumina (AI2O3), and it may be taken that there should be three molecules of CaO to every molecule of SiOa, and also three molecules of lime to every molecule of AI2O3. To determine from the percentage of these com- pounds whether this is so merely involves a reference to atomic weights and the working out of a simple proportion 192 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS sum, as explained in Chapter VI. If the lime is found to be less in quantity than this amount a loss in strength in the cement may be looked for, while if the lime is greater in quantity, the cement will be liable to exhibit undue expansion after setting. (6) Portland cement should be entirely soluble in dilute hydrochloric acid. This may easily be ascertained without expert aid by placing a small quantity of the cement in powder, in excess (say, ten times its volume) of spirits of salt diluted with four or five times its bulk of water. If the mixture is gently warmed in a porcelain or glass vessel the whole of the cement should dissolve in a few minutes. Any residue is sand or other inert matter which has not entered into combination with bases on burning, and has no value in the process of setting. (c) The role played by magnesia in cements is still a matter of dispute, but in this country amounts much exceeding 2 per cent, are looked upon with suspicion, probably chiefly on account of the slow rate at which this base becomes hydrated and hence of the probability of expansion, due to such hydration, occurring after setting has taken place. A certain amount of combined sulphur in cement is probably advantageous, but its addition in the form of calcium sulphate with the object of retarding setting is considered to be prejudicial when the amount of this salt exceeds 2 per cent. Sulphur is generally stated in analyses as "sulphuric anhydride " (SO3) which may be looked upon as the acid- forming oxide which with lime forms CaSOi ; thus CaO + SO3 = CaSO^. Given the percentage of SO3, that of CaSOi is therefore readily calculated.-"^ » CaO + SOs = CaSOi, 80 - - 136, 136 1 = gQ- = 1'70, that is, 1 per cent, of SOs is equivalent to 1-7 per cent, of CaSOi. CEMENTS 193 7. Rate of Setting. — This test, which is of smaller import- ance than the foregoing, is useful as an indication of the suitability of a cement for a particular purpose. Rate of setting depends partly upon the amount of alumina present, partly upon fineness of grain which increases the speed of chemical action with water. The determination of the setting point is made by noting the period which elapses after gauging before a metal weight possessing a blunt point of given area fails to make an impression when placed on the cement. It is found that an initial set (due to the decomposition of aluminate) is first obtained, and that the final setting, which indicates real solidity, takes place subsequently. The test refers to the final stage of the process. 8. Use of the Microscope. — Le Chatelier has brought microscopic research to bear upon cements, and this method of investigation is likely to develop. If sections of cement clinker cut and mounted in the same manner as rock sections, be examined, several distinct minerals may be observed. This experimenter has given the names alit, belit, celit, and felit to these distinguishable constituents, but whether they are true chemical compounds or, as suggested by Eichardson, merely solutions of one mineral silicate or aluminate in another, has yet to be determined. Alit, according to Le Chatelier, appears to be the silicate 3CaO.Si02. It is colourless, and gives under polarised light but dull colours as distinguished from the deep brown tint and brilliant polarisation colours of certain other less valuable constituents. 9. Other Tests. — Tests for compressive strength, porosity, elasticity and behaviour under fire are not usually included in the ordinary examination of cement, but may be carried out in the manner described for stones. In the case of reinforced concrete structures, elasticity tests are of great importance and are usually carried out by 194 OHEMISTEY AND PHYSICS OP BUILDING MATEEIALS loading actual structures and measuring the deflection observed by the magnifying aid of a beam of light reflected from a mirror, and subsequently the recovery attained when the load is removed. 10. Actual Strength of Portland Cement.— The British standard specification requires a tensile strength test per square inch of 400 pounds in seven days and 500 pounds in 28 days for neat cement, and 120 pounds in seven days and 225 pounds in twenty-eight days for cement mortars composed of one part of cement to three parts of sand. This is for a cement which may leave a 22^ per cent, residue on a 180 X 180 sieve, hence greater strength may be demanded for many cements now prepared. From a table of tests given by Butler^ it would appear that the average strength per square inch in tension for neat cements leaving some 4 per cent, residue on 100 X 100 sieve is after seven days 740 pounds and after twenty-eight days 767 pounds and as 1 to 3 mortars, after seven days 265 pounds and after twenty-eight days 834 pounds. V. PozzuoLANA Cements. This name, derived from that of the village Pozzuoli, near Naples, is applied to natural and artificial siliceous materials which when ground and mixed with lime exhibit hydraulic properties without any kiln treatment. These products vary very widely in composition, and consist of some 30 to 70 per cent, of Si02, some 10 to 20 per cent, of AI2O3, and some 5 to 20 per cent, of Fe203. A small quantity of CaO and MgO, usually considerably less than 10 per cent., and variable amounts of K2O, Na20, and H2O are also present. 1. Natural Pozzuolanas. — The most important of the natural pozzuolanas are of volcanic origin, though certain clays and sands have a limited use under this designation. » Butler, " Portland Cement." CEMENTS 195 The former, derived from lavas, or volcanic cinders or mud, are represented by the famous Italian deposits which supplied material for mortar and concrete still in excellent preservation in many ancient buildings. These deposits still form the source of hydraulic material. Trass, a vol- canic mud, and santorin, an ash, also have an extensive use. These materials, quarried in open workings or some- times mined at considerable depths, are screened and ground, after which they are mixed with the requisite quantity of lime slaked so as to form a powder, that is, free from excess of water. The cement is then ready for use. 2. Artificial Pozzuolanas. — The most important materials classed under this heading are the slag cements, though burnt clays which have been employed in large under- takings remote from transit facilities must also be regarded as belonging to this group. Certain slags produced in various industries, particularly in the manufacture of iron and steel, possess a composition very similar to that of many natural pozzuolanas. The more basic varieties, i.e., those containing a fair proportion of lime, are employed to some extent in the manufacture of cements. The slag is granulated by causing it to flow in a molten condition straight from the furnace into water, which, besides producing great mechanical subdivision, removes a good deal of the sulphur present largely as calcium sulphide. It is then dried by hot air, ground, and mixed with dry slaked lime to which is often added a proportion of Portland cement, which is said to promote soundness in the resulting product. 3. Properties and Strength of Pozzuolana Cements. — In colour these cements vary much, owing to the great difference in the percentage of iron found among them ; but they are generally of light tint, as would be expected in materials partly composed of free lime. Their specific gravity is about 2'8. B.M. o 196 CHEMISTEY AND PHYSIOS OF BUILDING MATEEIALS Though inferior to Portland cement, the better ground and mixed varieties exhibit a remarkable degree of strength, and results are recorded of slag cements consisting of 3 parts of slag to 1 of lime which showed a tensile strength exceeding 600 pounds per square inch. Johnson^ quotes experiments which tend to show that the ratio of compressive to tensile strength is similar to that given for Portland cement, namely, about 10 to 1 ; but Eckel,^ citing fuller details, places this ratio at about 5 to 1, and gives tests which show a strength for these neat cements in tension at seven days as about 460 pounds and at twenty-eight days as 515 pounds per square inch, while with sand as 1 to 3 mortar such cements showed a strength of 157 pounds and 209 pounds respectively. The materials forming the pozzuolana group possess hydraulic properties apart from the addition of free lime, since they contain a certain proportion of bases, but these are usually small in quantity, except in the case of the slag cements, and the strength is always developed chiefly by the free lime subsequently added. Some views suggesting an explanation of this remarkable effect of the presence of lime will be given in the following chapter. One of the chief objections urged against slag cements is their liability to contain sulphur in the form of calcium sulphide,^ a substance which readily decomposes in the presence of moisture with the liberation of sulphuretted hydrogen. This compound (or these compounds, for there are several sulphides of calcium) on oxidation form calcium sulphate, with expansion. A greenish tint on fracture shown by briquettes kept under water, and the evolution of sulphuretted hydrogen, readily recognised by its smell, on the addition of dilute acids, enable the presence of sulphides to be detected. 1 Johnson, " The Materials of Construction." ' Eckel, " Cements, Limes, and Plasters." 8 The expansion observed in breeze concretes may possibly be due to this compound in coke. CHAPTER XVIII THEORIES UPON THE SETTING OF PLASTERS AND HYDRAULIC MATERIALS The great variations which occur in the strength and stabiHty of the binding materials dealt with in the previous chapters, and the importance of a true understanding of the conditions upon which these characters depend, render it necessary to deal with the views which have been put forward in explanation of these complex phenomena. Scientific opinion is by no means unanimous as to the explanation of setting and hardening, and much remains to be done in the realm of pure science on the subject of the cohesion and adhesion of bodies, and upon the exact nature of the chemical reactions which take place on the burning of hydraulic materials and on their subsequent treatment with water. I. Cohesion and Adhesion. The strength of any material is ultimately dependent upon the power possessed by its particles of sticking together when submitted to disruptive forces. This is due to cohesion and adhesion, the display of which vary very much with the area, closeness of contact and nature of the materials or molecules between which such forces are exerted. 1. Cohesion.— By cohesion is meant the power of resisting disruption possessed by individual chemical substances. Thus, if a crystal of selenite be pulled into halves, the force of cohesion has been overcome. This rupture is, therefore, 0 2 198 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS the overcoming of the actual molecular forces which confer upon the substance its rigidity. Cohesion is not only displayed in very different degrees by different bodies, but this property varies in the same body in different directions. It is less, for example, between cleavage planes, when such exist, than in other directions. 2. Adhesion. — Adhesion is the tendency displayed by different bodies to stick together. This is non-existent in the case of many bodies, but is sometimes greater than the force of cohesion, as when materials joined by a cement fracture individually rather than at the joint. Given com- plete contact, the force of adhesion usually increases with the roughness of the adjoining surfaces. This is no doubt due largely to the greater area of contact over any given section which is produced by the sinuosities of such surfaces and because the force tending to overcome the adhesion can- not act normally, that is, at right angles and with greatest effect upon the whole of this sinuous area at one time. 3. Effect of Inert Aggregates on Cementing Strength. — From the above considerations it will be obvious that problems connected with the setting and strength of cementing bodies will be very materially influenced if, as is usual, sand or other aggregate be mixed with such materials. Those aggregates should be chosen as intrin- sically adhere most strongly to the cementing material employed, upon which subject little information at present exists. The shape of the aggregate particles should be such as to produce the greatest total area across any given cross section, that is, to give the greatest interlocking effect consistent with the limits of size permissible for such particles. The aggregate should be graded in size to preclude the formation of voids in the material, which, whether they be filled with air or water, produce a decrease in adhesive power proportional to their combined area. In most aggregates in ordinary use the force of cohesion SETTING OF PLASTEES AND HYDEATJLIC MATEEIALS 199 is greater than that of adhesion to the cementing material. As this cohesive force is inherent, and therefore costs nothing, whereas the adherence as developed by the cement is expensive, as much value should be got out of the former as possible by the judicious use of angular aggregates, thoroughly cemented together, of as great a size as circum- stances will allow. Such thorough cementing demands the use of aggregates carefully graded so as to contain particles of sizes suitable for filling all voids, otherwise a wasteful amount of cementing material will have to be employed. Some opinion as to the voids presented by various aggre- gates may be obtained by a complete mixing and ramming of the aggregate alone in a vessel of known volume, when the amount of water which can then be added without increasing the apparent volume of the mass will represent the space which must be occupied by the cementing sub- stance when it reaches its final hardened condition. It seems probable that considerable economy might be effected in the use of cementing materials by greater attention to the nature, configuration, and grading of the aggregates mixed with them. II. Introductoey Kemarks on Setting. 1. General Causes. — It is now necessary to consider what explanations can be offered of the setting of cementing materials, and though the theories advanced on the subject naturally differ in the case of different substances, it will be observed that, whether plasters, limes, or cements be in question, the ingredients composing them have all been subjected to heat and have thus been rendered anhydrous, or nearly so. Further, setting power is only developed by the subsequent addition of water, which is absorbed, and thus becomes chemically combined, and this hydration takes place with considerable swelling during the setting process. 200 CHEMISTRY AND PHYSICS OF BUILDING- MATERIAL Setting is, therefore, the result of hydration ; cohesion is developed by the pull of the newly-formed hydrated mole- cules one upon another ; and adhesion, if inert aggregates or several cementing compounds are present, by the pressure of the boundary areas of the constituent substances against each other. The cohesion developed between the molecules of a given substance depends not only upon the chemical nature of the substance and the hydrate formed from it, but in a very high degree upon the physical conditions under which the hydration takes place, at least in the case of all compounds which endeavour to develop an orderly molecular arrange- ment: that is, which show any tendency to crystallise. Molecules in solution take time to group themselves when assuming the solid condition, and if disturbed during the process cohesion will be diminished or destroyed. The heat developed by the hydration of quicklime produces so much molecular disturbance that hydrated lime in a solid condition is produced long before molecular quiescence is possible, and a friable non-coherent mass is the result ; but by allowing the hydration to proceed slowly the same hydrate may be obtained in a crystallised condition, when it possesses considerable cohesive powers. The problem of setting is again further complicated by the fact that a given compound may assume several crystalline forms, according to the conditions under which crystallisation takes place- Gypsum, for example, formed on the setting of plaster of Paris, can crystallise in short columnar crystals or in masses of slender needle-shaped form. The force required to separate one crystal from another is less than that necessary to pull into two an individual crystal, hence the material in the latter form will show a much greater development of strength than in the former. 2. Crystalloid and Colloid Theories of Setting. — Hydraulic SETTING OF PLASTEES AND HYDRAULIC MATERIALS 201 materials, which form by far the most important class of bodies connected with this discussion, owe the strength which they develop to the presence of compounds of silica. These compounds break up on treatment with water, but the composition and nature of the resulting bodies is still a matter of dispute. While there are many individual opinions as to the rdle played by various chemical con- stituents two main schools of thought exist on the general subject of setting. (a) One view is that setting is due to crystallisation. In the case of wholly crystalline bodies, such as gypsum, this view is beyond contention, but is also held to explain the setting of hydraulic materials, in which process it is assumed that the silicates and aluminates of lime contained in such materials break up and combine with water to form crystal- line compounds, and that setting is due to the interlocking and adhesion of such crystals. This school is led by Le Chatelier. (b) The other view is that the hydration of hydraulic materials results in the production of colloidal (gelatinous) forms of hydrated silicates and aluminates of lime, and that it is the drying up of such gelatinous hydrates into hard and glue-like masses which accounts for setting. Further, that some inevitable crystallisation which takes place on account of the presence of non-gelatinous compounds such as hydrated lime resulting from chemical decomposition, is actually injurious to the strength of the material. This school is led by Michaelis. III. Theokibs on Setting Developed. 1. Crystalloid Theory of Setting. — The advocates of this theory believe that the main and only essential compound in hydraulic materials is tricalcium silicate 3CaO.Si02, and that the alumina always present in small quantity and 202 CHEMISTKY AND PHYSICS OF BUILDING MATEEIALS necessary in practice to admit of fusion in the kiln, is com- bined with lime as SCaO.AlaOs, according to Le Chatelier, and as SCaO.AlaOs according to the American view as represented by the researches of Newberry and Eichardson. On the addition of water the above silicate of lime is decom- posed into a similar compound which absorbs water as water of crystallisation, and to which the formula 2(CaOSi02).5H20 is given. In this process the rest of the lime from the sili- cate 3CaO.Si02is freed and forms calcium hydrate Ca(0H)2, which crystallises. The set cement is regarded as consisting of interlaced needle-shaped crystals of the hydrated silicate and hexagonal platey crystals of calcium hydrate embedded in them. The calcium aluminate is believed by Le Chatelier to combine with water to form 3CaO.Al2O3.10H2O.^ These views on the constitution of hydraulic materials are based partly on optical examination of Portland cement and partly on research, in which an attempt was made to prepare silicates and aluminates of limes artificially by fusion in various molecular proportions, and to determine the stability and characters of the resulting bodies. Le Chatelier in France, and Newberry in America (1897), have prepared a variety of such compounds, and the experiments of the latter were later confirmed by Clifford Richardson. Le Chatelier believes the setting to be due to the hydrated silicates and aluminates, but in the American view this is due to the crystallisation of calcium hydrate. More recently (1906) Messrs. Day and Shepherd, in America, have conducted experiments on the formation of lime silicates, and deny the existence of the trisilicate 3CaO.Si02. According to their view the hydraulic proper- ties are due to basic silicate of calcium 2CaO.Si02 formed by rearrangement or " inversion," at a high temperature, ^ The later view of this savant, kindly expressed in a letter to the writer, May, 1908. SETTING OF PLASTEES AND HYDEAUIJC MATEEIALS 203 of another silicate composed of lime and silica in the same proportions, a fact previously suggested by Zulkowski in 1899. The views of these experimenters are now accepted by Eichardson. The original papers^ must be consulted for a further pursuit of this subject. 2. Colloidal Theory of Setting. — This theory, which for many years has been advocated by Dr. W. Michaelis, in Germany, denies the value of crystallisation in the setting process.^ This experimenter contends that the combina- tions of lime and silica after the addition of water cannot be looked upon as definite compounds of precise compo- sition, but must be regarded as gelatinous hydrated sili- cates, which swell very greatly on formation. The water in such bodies cannot then be regarded as water of crystal- lisation, its amount is indefinite, and it is imbibed by a process of transpiration through the membrane-like walls of the colloidal compounds, which thus swell and even- tually stick together, and finally, on drying, harden, when they lose their powers of imbibing water. Portland cement is to be regarded as composed of silica combined with lime in such quantity that most of such lime is liberated on the addition of water, and this freed lime, when hydrated, results in the formation of colloidal silicate of lime, pro- bably, in the case of all hydraulic materials, CaOSi02 + water. The amount of lime, i.e., whether it is present in 1 Newberry, J. Soc. Chem. Industry, November, 1897, pp. 887 — 894. Richardson, Engineering News (U.S.A.), August, 1904, and January, 1905. H. Le Chatelier, " Le Constitution des Mortiers Hydraulic," Dunod, 2nd ed., 1904; Am. translation, 1st ed. H. Le Chatelier and others, L'Association Internationale pour I'essai des Materiaux de Construction, February, 1902 ; January, 1903 ; April, 1903 ; April, 1904 ; October, 1904. Day and Shepherd, J. Am. Chem. Soc, vol. xxviii. , September, 1906, pp. 1089 — 1114 ; also Day, Allen, and Iddings, Am. J. Sci., 19, 93 (1905). " " The Hardening Process of Hydraulic Cements," paper read in Berlin, February 21st, 1907, translated, published by Cement and Engineering News (U.S.A.). 204 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS such proportion that the compound 3CaO.Si02 could be formed or not, does not all affect the reaction, though this amount may affect the quality of the resulting material. Hence the fact that lime and silica are found to give the best results in cements in about the proportion of 3 CaO to 1 Si02 must be regarded as a more or less fortuitous circumstance depending on the usual method of employ- ing cements, and not as indicating the existence of the compound 3CaO.Si02. To substantiate his view that Portland cement ought to be regarded as a kind of desiccated jelly, Michaelis cites experiments showing that when cement is mixed with about fifty times its weight of water and thoroughly agitated, a gelatinous mass is formed, accompanied by swelling of the cement to from twenty to twenty- five times its original volume, and this, when kneaded into a dough, may even be rolled out into slabs without detriment to subsequent hardening. Such treatment would probably prevent any molecular arrangement such as is essential for development of cohesion by crystallisation. It would certainly seem that the development of hydraulic properties displayed by pozzuolanic materials on the addi- tion of lime is more readily explained by the adoption of the colloid theory of setting, since lime in solution has a remarkable power of causing the precipitation of gelatinous silica from bodies such as pozzuolanas which contain silica in a soluble form. In the case of slag cements, Le Chatelier attributes the display of hydraulicity to the decomposition of a double siHcate of lime and alumina owing to the solvent power of calcium hydrate in solution. 3. Views on the Effects of Magnesia and Iron Oxides. — Almost all hydrauUc materials contain small quantities of magnesia (MgO) and of ferra (Fe203), but the importance of these compounds is small as compared with the main con- stituents above discussed. SETTING OF PLASTEES AND HYDEAULIC MATEEIALS 205 Opinions as to whether these oxides enter into combina- tion or not are very much divided. If any combinations exist these are probably composed of magnesia and silica, and of lime and ferra, which last, in the presence of strong bases like lime, always acts as an acid-forming oxide. (a) Magnesia. — Magnesia is a much less powerful base than lime, hence it is less likely to combine with the acid- forming oxides, and its hydration takes place with com- parative slowness. It is generally regarded in this country as equivalent to lime in its action when present in small quantities, though there is little evidence for the basis of this assertion. Le Chatelier's experiments indicate that magnesia and silica enter into combination, but Newberry describes attempts to prepare silicates of magne- sium which led to no definite indication of the formation of compounds. Perhaps the chief authority on this subject is Dyckerhoff, who places the maximum safe limit of magnesia in cements at 4 per cent., and states that no tests on the properties of this base as affecting cements are of value if undertaken less than six months after setting.^ The safe limit is usually placed at 3 per cent, in this country, but cements are in use in America which contain much larger quanti- ties. Michaelis quotes an opinion that magnesia is an essential for the formation, by fusion, of certain silicates of lime, hence this oxide may yet be discovered to play some part in the formation of cements, (6) Ferra. — Le Chatelier's attempts to produce compounds of lime and ferra (calcium ferrites) led to the formation of bodies which merely displayed the properties of free lime on slaking. Newberry and Richardson, however, consider that ferra can enter into combination and display hydraulic properties, while both Le Chatelier and Michaelis are agreed as to its value as a component of cements for use in ' Dyckerhoff, J. Soc. Chem. Industry, 1890, p. 943. 206 CHEMISTRY AND PHYSICS OF BUILDING MATERIALS sea-water. The amount of this oxide present in ordinary cements is so small that further discussion on this subject is unnecessary here, but it seems likely that considerable advantage might be taken of the use of iron in cements for special purposes. Michaelis refers to an industry for the production of iron-ore cement which is developing in Germany, and bases his eulogies of this material upon the fact that calcium ferrites do not crystallise. 4. Summary of Views on Constitution and Setting. — The following attempt to summarise the diverse views on this subject may be found useful ■} — View held. Authority. That in the kiln treatment of hydraulic materials combination between lime and silica takes place, and that such combined silica is chemically active as distinct from free silica such as sand, which is inert. That the silicate of Hme formed is substantially SCaO.SiOa. That the silicates of lime formed can only be CaOSi02 and 2CaO.Si02. That the aluminate of lime formed is SCaO.AlaOs . ,, „ ,, J) )) >> 2CaO.Al203 . That magnesia appears to form silicates and aluminates. That magnesia does not seem to form silicates and aluminates. That hme and f erra do not appear to form hydraulic compounds. That lime and ferra enter into combination . All. Le Chatelier and Newberry. Day and Shepherd, Michaelis. Le Chatelier, Newberry and Richardson. Le Chatelier. Newberry and Richardson. Le Chatelier. Newberry. ^ A valuable historical summary on the subject will be found in a paper entitled " The Structure of Cementing Materials," by Prof. Anderson, of Glasgow, given in full in The Quarry, April, 1902, pp. 234 — 242. The author, however, entirely omits any reference to the colloid theories of setting. SETTING OF PLASTEES AND HYDEAULIC MATEEIALS 207 View held. Authority. That setting is due to hydration of lime silicates (and aluminates) accompanied by liberation of lime. That setting is due to crystallisation, the water added combining as water of crystallisation, That setting is due to the formation of the sihcate 2(CaOSi02)5H20, and in minor degree to the aluminate 3CaO.Al2O3.10H2O. That setting is due to the crystals of hydrated lime formed. That setting is due to colloidal silicate of lime CaOSi02 with an indefinite quantity of imbibed water. All. T 1^ n Q "foil Of Newberry (and Eichardson?). Le Chatelier. Eichardson (?). Michaelis. IV. Eate of Setting op Plasters and Cements. It has already been pointed out that the character of crystalline compounds formed during setting^ bears an important relation to the strength of the resulting material. Le Chatelier has carried out experiments upon which he has based an interesting theory in explanation of the effects of fineness of grain and of the presence of certain com- pounds occasionally added to cementing materials, as influencing the nature of the solids which result after gauging with water. This theory, known as the super- saturation theory, is developed in connection with plaster, but also gives an insight into the physical nature of setting in the case of hydraulic materials on the assumption that the crystalloid theory of setting is the correct one. This savant has developed his views on the fact that the solubility of a dehydrated or partially dehydrated compound is greater than that of the same compound combined with its full complement of water of crystallisation. Thus when ' Advocates of the colloid theory must admit that the liberated lime crystallises as hydrate of lime. 208 CHEMISTRY AND PHYSICS OF BUILDING MATEEIALS plaster of Paris is dissolved in water a saturated solution is produced which is, therefore, supersaturated for the resulting gypsum formed immediately on hydration. As a result part of the gypsum, the fully hydrated sulphate, is immediately deposited in the form of crystals. This with- drawal of matter from the solution leaves the remaining water free to dissolve more of the plaster of Paris, and thus the cycle is repeated until the whole of the water added (if not excessive) becomes combined as water of crystallisation. It is evident that the relative rates of solution of the plaster of Paris and crystallisation of the gypsum will fix the concentration, that is, the strength of the solution at any given stage in the process, and since it has been shown that the stronger the solution the greater is the tendency towards the production of needle-shaped and, therefore, firmly interlocked crystals, the rate of solution has a material effect upon the strength of the resulting material. This rate of solution will be dependent upon the surface exposed to the solvent action of the water, which explains the increased strength of finely ground cementing materials. It will also depend on the relative solubilities of the dehydrated and hydrated compounds concerned in the action, and this relation may be influenced by adding to the water used for gauging, bodies which increase the solubility of the dehydrated salt. This gives an explanation of the use of " accelerators," such as washing soda, some- times added to cements to hasten setting, and may also possibly explain the increased strength of Keene's and other special cements over ordinary plaster of Paris. Common salt is another instance of a compound which accelerates setting. Conversely, the use of certain bodies to retard setting, such as calcium sulphate in Portland cement, may possibly be explained by the decrease in solubility of the dehydrated SETTING OF PLASTEES AND HYDRAULIC MATERIALS 209 compounds produced by their presence. This gives an alternative to the theory of Schott in reference to the coating action of such compounds, which is supposed to decrease the rate at which water can reach the particles undergoing solution. Much more information, however, as to the actual solubilities of cementing constituents in solu- tions of salts used is required before any general statement can be made on this subject. The effect of such retarders as size or other colloid matter is probably to be explained on the assumption that their action is mechanical and decreases the rate of solution by adding to the viscosity of the liquid. Such substances, by preventing the interlocking of crystal masses, must be regarded as having a detrimental effect. V. — The Failure op Hydraulic Materials. 1. Expansion. — The commonest and most important cause of failure in hydraulic materials must be regarded as due to slow expansion after, and often long after, complete rigidity of the mass has been attained. This is caused by incomplete hydration before setting, which may be due to imperfect mixing of the cement and water, or to the presence of particles so large that the action of water upon them cannot immediately reach completion. Again, an excessive proportion of lime may produce expansion, and the use of insufficient water in gauging the cement might also produce similar results. This subsequent expansion is caused by the gradual hydration of cement which has escaped initial action of water, either by atmospheric moisture or by water entangled in the material on setting. Since the compounds formed on hydration all occupy a larger volume than the original constituents, such hydration results in immense internal strains in the rigid material, 210 CHEMISTEY AND PHYSICS OF BUILDING MATEEIALS which may thus undergo disruption, with disastrous results to surrounding structures in confined situations. The long intervals, which have been known to reach several years, before the expansion of unsound cement makes itself evident would seem to somewhat favour the colloid theory of setting, since the permeability of colloids approaching a state of dryness is exceedingly small, and once such colloidal films surround material unacted upon, the passage of water to such material must be a very gradual process. In cases in which disruptive effects make a sudden appearance, it is probable that slow hydration is still the cause, but that the material has previously withstood an accumulating internal pressure under which it has at length broken down. If lime is present in cement materials in excessive quantities, this will, after the high temperatures of burn- ing, be found as a comparatively dense material. In this form it may be assumed that immediate slaking, on the addition of water, will not take place, and that an outer layer of slaked lime may be formed upon such free-lime particles, which will protect the internal core of quick lime until setting is complete. Slow hydration of this Hme core will eventually result in expansion. The actual effects of the expansion of hydraulic materials will depend very largely on the situation in which they are used and on their own physical structure ; the more porous the cement, for example, the more internal apertures it will provide for expanding particles, hence the disruptive effects of expansion are less likely to make themselves evident in the case of lightly burnt natural cements or hydraulic limes than in the case of denser materials such as Portland cement. 2. Efflorescence and Solution. — The hydrated bodies formed when water is added to cement are not efflorescent SETTING OF PLASTERS AND HYDEAULIO MATERIALS 211 in the ordinary sense, but when cements are exposed to great heat or draught, or when subjected to the action of fire, loss of some combined water may occur, with con- sequent loss of crystalline form, and hence with the production of white powders which may make themselves evident on the surface of the material. The presence, how- ever, of sulphate of lime or of salts of potash or soda may result in efflorescence and staining of surrounding materials, as previously explained. Solution of the hydrated lime formed on the setting of cement is undoubtedly possible under ordinary atmospheric conditions of use, but such loss is largely counteracted by its compact and crystalline nature, and by the action of carbon dioxide, which gives it a surface covering of car- bonate of lime, and any loss of material from this cause is trifling, _ 3. Defects due to Sea Water.— In marine works the solu- tion of cement may occur with considerable rapidity, owing to the action of magnesium chloride in sea water upon the lime in the cement, which results in the production of soluble calcium chloride. Thus : MgCla + CaOaHa = CaCla + MgO + H2O Sea water also contains sulphate of lime and magnesia, which act upon the alumina in the cement and produce a compound known as sulph-aluminate of lime; and since this compound occupies more space than the original con- stituents, expansion and disruption of the cement may result from its formation. Le Chatelier and, more recently, Michaelis have carried out experiments which show that, if alumina in cements is replaced by ferra, this deleterious action of sea water is pre- vented. It is stated that the whole of the alumina may be replaced by ferra in manufacture without any detriment. Le Chatelier further states, however, that if the percentage of B.M. CHEMISTEY AND PHYSIOS OF BUILDING MATEEIALS lime in the cement be decreased, alumina may still be present without the formation of sulph-aluminate, the quantity of lime being then insufficient for its formation. Attempts which have been made to improve the resisting power of cements for marine purposes by the addition of fatty materials on gauging to prevent the entrance of sea water appear to show negative results. 4. Defects due to Aggregates.— The inert materials em- ployed in the production of concretes may occasionally play a part in the failure of hydraulic materials. Coke, clinker, and slag are all liable to contain sulphur, and when this is present in the form of sulphides, decomposi- tion of those compounds is Hable to occur with expansion, as has been already explained in the chapters dealing with Brick Clays. Again, defective bricks containing lumps of lime, if used as an aggregate, might lead to subsequent expansion. CHAPTEE XIX ARTIFICIAL STONE, OXYCHLORIDE CEMENT, ASPHALTB I. Artificial Stone. The cementing materials discussed in the previous chapters and the means whereby their constituents may be brought mto combination have been extensively utilised for the production of artificial stones and bricks. Some of these materials are mere concretes : that is, they consist of inert fragments of stone or other suitable mgredients cemented together by some hydraulic agent such as Portland cement. Such materials do not call for special discussion. 1. Ransome's Process. — The manufacture of artificial stone proper was first attempted by Eansome, and his pro- cess consists in the formation of calcium silicate, by means of a chemical reaction, as a binding agent between suitable inert fragments. This involves the preparation of sodium silicate, a soluble gelatinous substance made by dissolving silica, usually in the form of flmt, in caustic soda solution under pressure The sodium siHcate is mixed with sand or other clean aggregate which is to form the bulk of the finished material and the plastic mass which results is pressed into moulds of the required shape. When the blocks are dry they are placed in a solution of calcium chloride, which gradually acts upon the sodium silicate with the production of calcium silicate and sodium p 2 214 CHEMISTEY AND PHYSICS OF BUILDING MATERIALS chloride. The composition of sodium silicate is doubtful.^ If it be assumed for simplicity's sake to consist of one mole- cule of Na20 combined with one molecule of SiOa or to have the formula Na2Si08, the reaction may be stated as follows : — Sod. silicate. Cal. chloride. Cal. silicate. Salt. NaaSiOs + CaCla = CaSiOg + 2NaCl. This equation shows the inevitable production of salt in this process, and since salt produces efflorescence prolonged washing is necessary before the " stone " can be satisfactorily used. The presence of salt in such preparations may be easily detected by the production of a heavy^ white precipitate on the addition of a few drops of a solution of silver nitrate to distilled water with which some crushed fragments have been shaken, and by the fact that this precipitate is not dissolved on the addition of nitric acid. 2. Lime-Sand Bricks. — The most satisfactory artificial combination, certainly from a scientific and probably also from a practical standpoint, is that of lime and silica directly, which is brought about by the treatment of sand mixed with a small percentage of lime with steam under pressure. The invention of the first successful process for effecting this is claimed by Michaelis, but a great many patents now exist under which such combination of lime and sand is carried out. It has never been satisfactorily proved, however, that chemical union really takes place. Eckel, for example, considers that any chemical action is unlikely, and cites the fact that the lime in such materials only amounts to from 1 Na20.4Si02 or Na2Si409 represents the approximate proportion of soda to silica in the substance known as soluble glass. 2 This test is a very deUcate one, hence mere cloudiness in the water would not be sufficient evidence of incomplete washing. ABTIFICIAL STONE, OXYCHLOEIDE CEMENT, ETC. 215 5 to 10 per cent, of the whole mass, and hence is not at all in the proportion to form silicates ; but it should be remembered that a very small proportion of silicate formed would be sufficient, with the perfect dissemination attained, to cement a large quantity of inert sand," and lime, although it does not possess the combining power of soda, is still an exceed- ingly strong base, and hence its combination with silica under the favourable circumstances supplied by heat and pressure seems by no means impossible. These artificial stones or bricks, consisting as they do of some 90 per cent, of fragmentary stone material, may be made to resemble natural stones very closely. They possess the advantage of great homogeneity, and can be worked with tools like natural stones. II. Stone Preservation. Although the preservation of natural stone has no direct connection with the subject of this chapter, the processes adopted for this end so closely resemble the first of the two cited in the preceding section that a few words on this topic have been reserved for introduction here. The use of stone preservatives carries its own condemna- tion as showing that the stone has been employed in a situation for which its chemical or physical nature renders it unsuitable, and no process known can be looked upon as approaching perfection on account of the difficulty in securing effective penetration of the preservatives employed. The object in all cases is the same, namely, to close the pores of the stone by some insoluble and permanent solid, and thus to prevent further damage. The most favoured means of effecting this is to cause chemical precipitation in the pores of the stone by the infiltration of one solution and then another, which shall, by precipitation, react with the first. Calcium or barium 216 CHEMISTRY AND tHYSlCS OF BUILDING MATEEIAT.S silicate is the solid, the production of which is usually aimed at, and this is effected by brushing over the face of the stone a solution of sodium silicate, followed, after this has penetrated as far as possible, by a solution of calcium chloride. The reaction is precisely that described for the production of artificial stone in the preceding paragraph. In the case of barium chloride, barium silicate and salt are similarly produced — NaaSiOa + BaCla = BaSiOg + 2NaCl. The removal of the sodium chloride, which can only be effected by washing, is a grave objection to the process. Single fluid stone preservatives generally consist of silicates or other compounds which dry up, leaving colloidal solids in the pores of the stone. The deposition of pure silica in the pores of the stone would be perhaps the ideal method of effecting preserva- tion. Silica is by no means insoluble in water ; solutions containing five per cent, of SiOa can be readily obtained, and if such solution could be arranged to flow slowly over the face of the stone the silica would be deposited on evaporation of the water or precipitated by the presence of alkaline compounds. III. OXYCHLORIDE CeMENTS. When magnesium chloride and oxide are mixed in suit- able proportions in the presence of water these compounds combine and form a cement of great hardness. This is due to the formation of magnesium oxychloride, which may be regarded as magnesium hydroxide Mg(0H)2, in which one of the oxygen and hydrogen atoms has been replaced by chlorine, thus : Mg^^^ becomes Mg