SB ID CALIFORWJA EAHTH SCIENCE* UBRARY THE CAUSE OF EARTHQUAKES, MOUNTAIN FORMATION AND KINDRED PHENOMENA CONNECTED WITH THE PHYSICS OF THE EARTH BY T. J. J. SEE, A.M., Lx.M., Sc.M. (Missou.), A.M., Pn.D. (BEROL.) Reprinted from PROCEEDINGS OF THE AMERICAN PHILOSOPHICAL SOCIETY VOL. XLV. 1907 ; THE CAUSE OF EARTHQUAKES, MOUNTAIN FORMA- TION AND KINDRED PHENOMENA CONNECTED WITH THE PHYSICS OF THE EARTH. BY T. J. J. SEE, A.M., Lx.M., Sc.M. (Missou.), A.M., PH.D. (BEROL.), PROFESSOR OF MATHEMATICS, U. S. NAVY, IN CHARGE OF THE NAVAL OBSERVATORY, MARE ISLAND, CALIFORNIA. Reprinted from Proceedings American Philosophical Society, Vol. xlv,^ 1906. THE CAUSE OF EARTHQUAKES, MOUNTAIN FORMA- TION AND KINDRED PHENOMENA CONNECTED WITH THE PHYSICS OF THE EARTH. BY T. J. J. SEE, A.M., Lx.M., Sc.M. (Missou.), A.M., PH.D. (BEROL.), PROFESSOR OF MATHEMATICS, U. S. NAVY, IN CHARGE OF THE NAVAL OBSERVATORY, MARE ISLAND, CALIFORNIA. (Read October 19, 1906.} I. GENERAL CONSIDERATIONS ON THE CAUSE OF EARTHQUAKES. i. Introduction. The great San Francisco earthquake of April 18, 1906, presented certain remarkable characteristics which immediately became a sub- ject of investigation on the part of men of science resident in this part of the United States. One very striking feature of this earth- quake was the conspicuous rotatory motion of the earth particle; and another was the long duration of the disturbance. The rotatory motion appeared so remarkable and so difficult to reconcile with theories very generally held by geologists and seismologists that it seemed worth while to make a somewhat comprehensive survey of the general subject of earthquakes, in the hope of reaching a better understanding of the cause of these phenomena. And as the details of this particular earthquake will be fully treated by others, 1 the result of the present inquiry 2 into the physical cause of earthquakes 1 The Committee of Investigation appointed by the Governor of Cali- fornia: Professors A. C. Lawson, George Davidson, A. O. Leuschner, G. K. Gilbert, W. W. Campbell, H. F. Ried, J. C. Branner, Chas. Burkhalter. Investigations are being made also by Professor Omori of the Imperial University of Tokio, Messrs. Otto Von Geldern, Luther Wagoner, and Mr. Hoehl of the American Society of Civil Engineers, and perhaps by others. 2 Rear Admiral H. H. Rousseau, U. S. Navy, Chief of the Bureau of Yards and Docks, has read this paper throughout, and made a number of suggestions which proved valuable. The independent judgment of an experi- enced engineer was felt to be no inconsiderable advantage in weighing some of the difficult questions here treated, and my most cordial acknowledgements are due to Rear Admiral Rousseau for his great kindness. 274 I9 o6.] SEE THE CAUSE OF EARTHQUAKES. 275 and other related phenomena may not be without interest to investi- gators of the physics of the earth. Almost exactly four months after the earthquake of April 18, namely, August 16, 1906, another, much more terrible, laid waste Valparaiso and the surrounding cities of Chili, producing scenes of desolation which are rare even in South America. The scientific need and the humanitarian demand for an investigation of the cause of these disturbances could, therefore, hardly be greater than it is at the present time. But if it be said that the researches of science are powerless to stay the hand of the destroyer, and only the laws of these terrible phenomena can be discovered, yet even the intelli- gent appreciation of natural laws may greatly mitigate the extent of the disaster and suffering which follow ; and on both humane and scientific grounds, the prospects of extending the domain of useful knowledge furnish a high inspiration for earnest endeavor to pene- trate the mystery of these hidden forces of nature, which so long have baffled the skill of philosophers. \Earthquakes and volcanoes were among the earliest physical phenomena to receive the attention of the ancients, and they have always occupied a prominent place in natural philosophy. Although the importance of the subject was derived originally from the ter- rible disasters which these mysterious agencies of unknown forces occasionally inflict upon large portions of mankind, in more recent times earthquakes have been studied also as about the only available means of throwing light upon the physics of the globe. No arti- ficial forces at the command of the experimenter are great enough to produce vibrations of the earth's crust or to transmit them through the body of the planet when once established in the surface layers. But notwithstanding all the labor and research which has been bestowed upon the subject, it can hardly be said that we yet have any satisfactory theory of the cause of these phenomena. This is the more regrettable, because, on the one hand, it places it beyond the power of science to predict earthquakes, or even to foretell the regions of their occurrence, which might afford some measure of security to life and property; while, on the other, it leaves many men of science without adequate hope that the true cause of these phenomena will ever be discovered, and at the same time so 276 SEE THE CAUSE OF EARTHQUAKES. [October 19, completely bewildered by a multitude of unsatisfactory theories that the progress of discovery itself is seriously embarrassed. There will naturally be those who doubt the existence of one common and universal cause of earthquake and volcanic phenomena. Nevertheless, difficult as the subject is, we believe that such a cause exists, and that it is capable of demonstration, if not with mathematical rigor at least with such high degree of probability 1 as to render the resulting theory practically useful, and we ask nothing of the reader except a careful examination of the facts as interpreted in the light of the cause assigned in this paper. If such a view, associating the varied phenomena of earthquakes and volcanoes, with mountain formation and the development of great sea waves, under one common cause, renders them more intel- ligible, and enables us to see the relations of all the observed phe- nomena in a clearer and simpler light, there will be presumptive evidence of the truth of the proposed theory ; and the probability of its correctness will increase with the harmony existing among all the known facts, and the effectiveness with which contradictions of other theories may be established. The final test of the theory will depend upon its usefulness in the advancement of discovery, so as to harmonize the whole body of earthquake and volcanic phenomena, including those associated with the origin and structure of mountains, the observations of geodesy, and of great sea waves, in their mutual relations, and in respect to the undisturbed parts of our globe. If the theory shall meet this test satisfactorily, we may feel confident that it assigns the true cause of the phenomena, and within certain limits the resulting laws of nature may be used to foretell events which will contribute to the repose and safety of mankind, and to the progress and usefulness of discovery in this interesting branch of natural philosophy. j 2.. The dynamical cause of earthquakes and volcanoes probably ^he unequivocal proof of the elevation of the coast at Yakutat Bay, Alaska, Sept. 10-15, 1899, seems to remove the last trace of uncertainty re- garding the chief function of earthquakes, and makes the demonstration as rigorous as that of any theorem in geometry. See the important memoir of Tarr and Martin, Bulletin of the Geological Society of America, vol. 17, May, 1906. Professor Georee Davidson, President of the Seismological Society of America, kindly called my attention to this classic work after the present investigation was finished. Note added December 12, 1906. Igo6 . SEE -THE CAUSE OF EARTHQUAKES. 277 depends upon the explosive pozver of steam formed within or just beneath the heated rocks of the earth's crust chiefly by the leakage of the ocean beds. Some of the most complicated phenomena in nature depend upon the simplest and most obvious of causes, but there are several reasons why the true cause often proves very difficult to discover. On the one hand our mental operations are not infrequently thwarted by conflicting prejudices and contradictory theories, so that attention is diverted from the real questions ; and, on the other, our clearness of vision and power of intuition are blinded by the very closeness and familiarity of the true cause, which is least sus- pected. Success in interpreting nature depends upon a combination of the proper elements of thought into one simple connected view which deals not with details but with the general tendencies. In the case of earthquakes and volcanoes this general view has been very difficult to obtain ; and with the growth of elaborate scientific inves- tigation and classification of earthquakes the difficulty has increased rather than diminished. For attention has been given to the attainment of high accuracy in the measurement of tremors by seismographs and other apparatus, and investigators have been oc- cupied with the registration and discussion of the details of phe- nomena rather than with the general underlying causes. We shall hereafter examine the porosity of matter and the prob- lem of the penetration of water into the rocks of the earth's crust, both from the experimental and historical standpoints, but let us first consider the probable state of the internal heat of the earth. In Astron. Nach., No. 4053, the writer has shown that when we consider the force of gravity alone, and suppose a body to be made up of gas reduced to the state of single atoms, over one-half of the primordial supply of heat is stored up within the condensing mass, while still in the gaseous stage ; and in a later paper on the rigidity of the heavenly bodies (A. N., 4104), it is shown that circulation and radiation become retarded and greatly restricted with increasing density, so that in the later stages of the development of a mass like the earth, much more than one-half of the heat generated is retained within the mass for raising the temperature. It is shown that all the heat of our earth depending on gravitation would raise the 278 SEE THE CAUSE OF EARTHQUAKES. [October 19, temperature of an equal mass of water 9954 C. ; and as decidedly more than half of it is still retained in the globe, we may conclude that the internal heat of the earth "is ample to raise the whole globe to a temperature of something like 20,000 or 25,000 C., accord- ing to the average specific heat of the earth's matter. If radium and other related elements exist within the earth in appreciable quan- tities, the amount of heat stored up, as Sir G. H. Darwin and others 1 have remarked, may be vastly greater yet. Now it is recog- nized that the crust or cooled layer on the outside of our planet is extremely thin, and we know that the temperature increases down- ward at an average rate of something like i C. for each 30 metres of descent. This accords also with Lord Kelvin's calculations on the cooling of a molten globe, carried out in conformity with Fourier's Analytical Theory of the propagation of heat in solid bodies. 2 From this we may infer, as geologists have long since remarked, that, even without the penetration of steam, molten rock would be encountered at a depth of decidedly less than 30 kilometres. As the percolation of hot water and steam appreciably lowers the melting point of silicious and perhaps other rocks (the lavas are mainly silicates), and itself develops at the very low temperature of only 100 C. under atmospheric pressure, we may infer that it would form in the earth at a depth much smaller than 30 kms. At no more than 10 or 15 kms. under the ocean beds large quantities of it might be produced and give rise to imprisoned forces of tremendous power. Besides it would rapidly absorb and spread in the hotter layers of rock beneath, just as in the case of gases absorbed in hot steel, cited by Tait and quoted in 5. That this absorption actually takes place is proved by the vast clouds of steam given off by melted lava after it pours from a volcano, such as Vesuvius. We are thus confronted with the following situation : \ The internal temperature of the earth is extremely high, with 1 Presidential address to the British Association for the Advancement of Science, Capetown, 1905; also a very recent paper presented to the Royal Society, April 5, 1906, by the Hon. R. J. Strutt, F.R.S., reported in Nature of May 17, 1906. 2 "The Secular Cooling of the Earth," Appendix D, Thomson and Tait's "Nat. Phil." I 9 o6j SEE THE CAUSE OF EARTHQUAKES. FIG. i. 279 Mt. Pelee. The burning cloud of December 16, 1902, seen from the sea. (From the Belgian Astronomical Society, tenth year. Plate V.) heated rocks quite near the surface, while the crust is fractured and leaky everywhere, and especially where the depth of the sea is greatest. The sea covers three-fourths of the earth's surface, and earthquakes are found to be most violent -where the sea is deepest, v PROC. AMER. PHIL. SOC., XLV. <8 4 R, PRINTED FEBRUARY I 9 , I 9 O 7 . 280 SEE THE CAUSE OF EARTHQUAKES. [October 19, , and volcanoes most numerous on the adjacent shores.^ Could then anything be more probable than to suppose that both of these great natural phenomena depend simply and wholly upon the explosive power of steam which has developed in the heated rock of the earth's crust ? The mere statement of the facts seems almost enough to con- vince one of the truth of this theory. But in view of the wide differences of opinion heretofore prevailing we shall examine it in detail, and we believe it will be possible to show that no contradiction can be established, and that it probably is the correct explanation of the mysterious forces which have so long baffled investigators and wrought such havoc in numerous places throughout the world. It would seem that the obvious fact of the leaky character of the sea bottom, covering three-fourth's of the earth, with great in- ternal heat everywhere so close beneath and volcanoes not only abundant on the shores adjacent to the deepest seas, but pouring forth vast quantities of steam when in eruption long ago suggested and apparently ought to have convinced investigators of the validity of this natural and simple explanation. But it appears to have been generally rejected, owing to several circumstances which did not enable investigators to obtain the proper point of view. On the one hand there were traditional theories of volcanoes and their relations to a supposed liquid or molten globe; and on the other little or no adequate knowledge of the enormous number and great violence of submarine earthquakes, which have recently been shown, mainly through the important researches of Professor Milne, to be the most powerful in the deepest oceans. While volcanoes and earthquakes have been associated from the time of Aristotle and Pliny, and we think justly so, and some'mutual connection could hardly be denied ; yet even after this relation was especially affirmed by great original investigators like Humboldt and Charles Darwin, it has unfortunately become customary of late years to class earthquakes as volcanic and tectonic or structural. Instead of viewing volcanoes as outlets of pent-up-steam, which blows out if possible the molten rock in which it develops a clear indication of every great eruption an effort was made to explain earthquakes as volcanic, with only partial success, whereas both I9o6 .] SEE THE CAUSE OF EARTHQUAKES. 281 phenomena depend upon the common cause of steam pressure formed deep in the earth's crust, principally by the leakage of waters from the sea. This highly explosive agency is developed so abun- dantly in the infinitely thin crust between the underlying molten globe, and the overlying oceans, the outcome of a fire beneath and of water above, as in a boiler, that one should not wonder at ter- rible explosive or eruptive phenomena appearing upon our planet. Considering the vast extent of the oceans it would be strange indeed if something like volcanoes and earthquakes were not inseparably, associated with the very nature of the terrestrial spheroid. If we consider with attention the various causes which might be assigned to explain earthquakes and volcanoes, taking into account their recognized geographical distribution and relation, the relative situation of the inner globe of fire and the overlying layer of water separated from it only by the thin and leaky bottom of the sea, and remembering that both phenomena are augmented to the maximum in regions characterized by high mountains near the deepest oceans, as on the west coast of South and Central America, the Aleutian and Kurile Islands, Japan, Sumatra, Java and other islands of the East Indies, bordering on the deep waters of the Indian Ocean, New Zealand, and the Lesser Antilles in the West Indies, Iceland, Italy, Greece, etc., we shall find the probabilities that steam pressure developing in the earth's crust is the true and common cause both of earthquakes and volcanoes, are as infinity to one against any other conceivable cause, or all other causes combined. The widely ex- tended relationship here pointed out is so intimate and everywhere so confirmatory of the theory that we cannot suppose it to be due to chance. 3. Views of Professor Milne and his methods of analysis. It has been justly remarked by many seismologists that the greatest belt of earthquakes surrounds the Pacific Ocean. Now each part of this great " fire girdle of volcanoes " with innumerable earthquake disturbances has been studied with care by one or more investigators. Without going into the detailed methods of record- ing and charting developed by Professor Milne, Professor Ewing, Dr. Davidson, Major De Montessus de Ballore, Dr. Agamennone, Dr. Cancani, Dr. Vicentini, Grablowitz, Omori, Koto, Nagaoka, and 282 SEE THE CAUSE OF EARTHQUAKES. [October , 9 , others, which are of. great value for the close study of particular regions, we may call attention to the conclusions of Milne, and Montessus de Ballore regarding the slope of the seashores as im- portant factors in the development of earthquakes. As a result of careful study of Japanese earthquakes covering eight years, Professor Milne found that "the central portions of Japan where there are a considerable number of active volcanoes are singularly free from earthquakes. The greater number of dis- turbances originate along the eastern coast of the Empire and many of them have a submarine origin." " Lines 120 geographical miles in extent in running in an easterly or southeasterly direction from the highlands of Japan into the Pacific Ocean, like similar lines drawn from the Andes westwards into the same ocean, have a slope of I in 20, or I in 30, and in both of these districts earthquakes are frequent. On the contrary, along the faces of flexures which are comparatively gentle, being less than half of these amounts, which may be seen along the borders of most of the continents and islands of the world, earthquakes are comparatively rare. The inference is that where there is the greatest bending it is there that sudden yielding is most frequent." 1 It seems advisable to quote more at length the full line of thought laid down by Professor Milne in his classic work on " Seismology " (London, 1898). On page 31 Professor Milne says: \ "A very much more serious objection to the volcanic origin of the majority of earthquakes is the fact that these disturbances are common in the Himalaya, Switzerland, and other non-volcanic regions. The destructive earthquake in 1891 in Mino and Owari occurred in a region of metamor- phic and stratified rocks. Again, an analysis of some ten thousand earth- quake observations of Japan shows that there have been but comparatively few which had their origin near to the volcanoes in the country. The greater number of this series originated beneath the ocean or along the seaboard, and as they radiated inland they became more and more feeble, until, on reaching the backbone of the country, which is drilled by numerous volcanic vents, they were almost imperceptible. Beyond this central range of mountains, earthquakes are only rarely experienced, and what is true of Japan seems to be generally true for the coasts of North and South America/'^ " Throughout the world we find that seismic energy is most marked along the steeper flexures in the earth's crust, in localities where there is evidence of secular movement, and in mountains which are geologically new 1 Cf. Scismological Journal of Japan, 1895, p. xv ; and Dutton, " Earth- quakes in the Light of the New Seismology," chapter III. I9 o 5 ] SEE THE CAUSE OF EARTHQUAKES. 283 and where we have no reason for supposing that brady-seismic movements have yet ceased. " As examples of the flexures to which reference is here made, we may take sections running at right angles to the coast lines of the various conti- nents. The unit of distance over which such slopes have been measured is taken at two degrees, or one hundred and twenty geographical miles. "The following are a few of such slopes:' West Coast, South America, near Aconcagua i in 20.2 "1 The Kurils from Urup I in 22.1 Seismic in 30.4 | districts, in 23.5 in J 91 ] 158 in 158 I Non-seismic 73 r districts, in 243 J in Japan, east coast of Nipon Sandwich Islands, northwards Australia generally Scotland from Ben Nevis South Norway South America, eastwards " The conclusion derived from this is that if we find slopes of consid- erable length extending downwards beneath the ocean steeper than I in 35, at such places submarine earthquakes, and their accompanying landslips may be expected. On the summit of these slopes, whether they terminate in a plateau or as a range of mountains, volcanic action is frequent, while the earthquakes originate on the lower portions of the face and base of these declivities. Districts where earthquakes, often followed by submarine disturbances, are most frequent are regions like the northeast portion of Japan and the South American coast between Valparaiso and Iquique. Here we have a double folding. The sea bed, as it approaches the shore line, instead of rising gradually, sinks downward to form a trough parallel to the coast, after which it rises to culminate in mountain ranges. The South American trough which lies within fifty or sixty miles off the coast, like the Tuscarora deep off Japan, attains depths of over four thousand fathoms, and the bottoms of these double folds are well known origins of earthquakes and sea wavesjj Professor Milne then goes on to show that where secular move- ments are active, " the forces which have brought these mighty folds (mountains) into existence have not yet ceased to act." The most important question of all, however, is what are these forces ? He says they appear where " mountain formation is geologically of recent origin," and adds i 1 "The conclusion to which such observations lead is that wherever we find in progress those secular movements which result in the building up of countries or mountain ranges, there we should expect also to find a pro- nounced seismic activity. Thus, while admitting a few small earthquakes to be volcanic in their origin, we recognize the majority of these disturb- ances as the result of the sudden fracturing of the rocky crust under the 1 " Seismology," by John Milne, F.R.S., p. 33. 284 SEE THE CAUSE OF EARTHQUAKES. [October x 9 , influence of bending. The after-shocks which so frequently follow large earthquakes announce that the disturbed strata are gradually accommodating themselves to their new position."l Professor Milne's statement that " the greater number of this series (10,000 Japanese earthquakes) originated beneath the ocean or along the seaboard, and as they radiated inward they became more and more feeble, until, on reaching the backbone of the country, which is drilled by numerous volcanic vents, they were almost imperceptible " seems to point directly to the cause set forth in this paper. If earthquakes depend upon the explosive power of steam, they ought not to be numerous near the volcanoes (unless these vents get stopped up), but they ought to be very numerous under the sea in the deep trough just east of Japan, which he says is found to be true by laborious and extensive observations covering a vast number of these phenomena. In order to leave no doubt as to the significance of these results we shall consider also the other lines of thought which he has worked out with so much care. 4. Inadequacy of the tectonic theory based on slipping and bending, and dislocational and fault movements. At present we shall not touch upon all the questions discussed by Professor Milne, but we may remark that slopes of I in 20 given above probably are not great enough to produce the least slipping, or fracturing or bending of rocks. The most effectual way to convince ourselves of the truth of this view is by an appeal to the cones of actual volcanoes. Take Mount Cotopaxi, for example. It is one of the tallest active volcanoes in the world, and the most regularly built of all the large volcanoes. The slope is 30, the angle of the apex being 120. A slope of 30 corresponds to I in 1.732; and thus Professor Milne's ratio of I in 20 is less than one- tenth that required to produce stability; and it has escaped his notice that slopes steeper than I in 35 are not such that the steepness could give rise to submarine earthquakes and their accompanying landslips. If the cones of volcanoes like Cotopaxi do not slip, when they are more than ten times steeper than the steepest sea slopes, and over twenty times that mentioned as unstable by Professor Milne, why should slips occur under the sea? Obviously the steep- ness, though no doubt considerable in certain places, is not the cause 19 o6.] SEE THE CAUSE OF EARTHQUAKES. 285 of earthquakes. Rains, snows and glaciers on Mount Cotopaxi ought to produce slipping of rocks, if anywhere, because the angle is steep and the material loose and unsettled. We are not aware that the slipping of any volcanic cone or other similar mountain has ever been observed to produce a real earthquake ; and if slipping were the order of nature, we should expect some enormous slips with corre- sponding tremors due to this cause near Cotopaxi, Aconcagua, and other great volcanoes (especially when these mountains are shaken at the times of eruption), which are not observed. We seem compelled therefore to abandon the theory of slipping and bending of rocks 1 except as producing all the time infinitesimal tremors called microseisms, which very likely depend to a con- siderable extent on this cause. Glaciers are known to be fluid masses, and they move accordingly, though very slowly. It has been shown by the writer (in Nature, 1902) that a rock such as marble undergoes secular bending, and is therefore fluid; and we take it that all large rock masses are very similar in their behavior, though their viscosity may be and generally is greater than that of marble; and hence if movement of mountain masses or other large rocks take place, it would seem that, wherever possible, it should be by a very gradual yielding. The cases in which very large masses of rock, like the sides of a mountain, acquire such unstable positions as to fall, do not seem to be very numerous. 2 Accordingly, it is difficult to believe that this cause is very effective in producing earthquakes ; for such shocks as might result from it would be rare, small and unimportant. And moreover they could never occur where the average slope is anything like so small as I in 20. Be- sides the arguments here outlined there is another hardly less effec- tive which we shall merely mention, namely : That the forces which may shake an entire continent and send waves of compression and 1 This hypothesis was originally proposed by Boussingault, from observa- tions made on earthquakes noticed in the Andes remote from known vol- canoes, and has at length developed into the tectonic theory now widely held by seismologists and geologists. 2 The movement by sliding of one or two mountains in the Alps is recorded within the historical period. Among the Andes the most noted change is the collapse of the crater of Carihuairazo, adjacent to Chimborazo, during a violent earthquake on the night of 19-20 of June, 1698. Before this disaster Carihuairazo is said to have been taller than Chimborazo. 286 SEE THE CAUSE OF EARTHQUAKES. [October 19 distortion through all the rocks between the two oceans, and disturb the whole earth, are not produced by so small a cause as the slipping and bending of ledges of rock. Humboldt and Charles Darwin long ago associated earthquakes with secular elevations and depressions, and it is noticeable that Professor Milne likewise thinks these disturbances occur with in- creased frequency in regions where such changes are still in progress. Montessus de Ballore concluded from his elaborate study of sta- tistical data that in adjacent seismic regions, instability of the earth is increased by differences of topographic relief; and that the unstable regions are associated with the greatest lines of corrugation of the earth's crust. Like Professor Milne, he observes that rapidly deepening shores which slope gently, especially if they are the con- tinuations of flat or moderately falling coast plains, are stable. His results are illustrated by steep regions of the seashore in South America, Japan, and other parts of the world, and by other regions where the slope into the sea is more gradual. These views and others of similar tenor by several investigators have led some geologists and seismologists to conclude that many of the earthquakes noticed along shores which are steep are due to the sliding of unstable deposits of sediment settling on the rock slopes. But if we recall, as above, the smallness of these slopes, even where the descent is most rapid it never exceeds that of our mountains upon the land, and is seldom as steep, and observe that the surrounding sea water is quiescent and would both greatly buoy up and resist the motion of any supposed sliding deposit, so that it is doubtful if appreciable sliding really takes place, and certain that if it does occur the effect in disturbing the earth would be very slight, we shall find it difficult to believe that the theory is well founded. It appears that such a deposit, resisted by the surrounding water, would slide with extreme slowness, and settle gently without any appreciable jar, and consequently no earthquake of importance could be produced in this way. I9o6 .| SEE THE CAUSE OF EARTHQUAKES. 287 II. ON THE POROSITY OF MATTER AND ON THE LEAKAGE OF THE OCEAN BOTTOMS. 5. On the porosity and penetrability of matter under the enor- mous fluid pressure operating in the deepest oceans, and the under- lying crust of the earth. Somewhat extensive researches on the internal pressures, con- stitution, and rigidities of the sun and planets, carried out during the past two years and published in the Astronomische Nachrichten, have led the writer to the conviction that many of the laws of matter depending on molecular forces, such as impenetrability and solidity, are quite inapplicable to the conditions prevailing in the interior of the earth and other bodies of our solar system; that under the immense pressures there operating, whatever be the temperatures, but especially under the high temperatures known to prevail in the interior of these masses, the hardest natural bodies would yield like sponges, and admit of the most perfect interpenetrability of all the elements. The conclusion was reached from the study of forces of somewhat impressive magnitude that all matter is enor- mously porous, and quite leaky under forces much smaller even than those operating in the interior of the earth; so that solidity and impenetrability, long held to be among the most universal properties of matter, far from being absolute, appeared to be very relative properties, appropriate to very small, but wholly inappropriate to large, forces, and sometimes set aside by the direct evidence of our senses in common laboratory experiments. There doubtless are many experiments which would enable us to appreciate the significance of these general principles in specific cases, but it will suffice to recall one close at hand, and directly connected with the question under discussion. In the series of soundings of the depths of the sea carried out some years ago by certain officers of the United States navy occupied with hydrographic and ocean surveys it was found that hollow glass balls with walls several centimetres thick, when subjected to increasing pressure at various depths, came up more and more completely filled with water, in proportion as the depth increased, though no fracture of the glass had occurred, and no holes in it could be discovered by ex- amination of the surface under the highest microscopic power. 288 SEE THE CAUSE OF EARTHQUAKES. [October 19, After a careful inquiry by many experienced physicists the conclu- sion was reached that the water had been forced slowly but bodily through the thick walls of the glass under a pressure of less than 1,000 atmospheres, in an interval of less than an hour's time. In the year 1661 a well-known 'experiment was made by the Florentine academicians who forced water through the solid walls of a sealed hollow sphere of gold, and other metals, by changing the shape of the sphere under mechanical applications of pressure, so as to diminish the volume. The present case of the porosity of glass was thus verified from the opposite point of view, by the steady application of external fluid pressure, on the spherical surfaces of glass balls sent down in modern soundings of the ocean depths. The great porosity of all matter has of course long been recog- nized by physicists, but we are so accustomed to dealing with small forces and the resulting doctrine of the impenetrability of matter that it is doubtful whether our appreciation of this fact has yet passed beyond the academic stage. In his well-known " Properties of Matter," fourth edition, p. 87, Tait says : " The porosity of wood, necessary for the circulation of sap, is beauti- fully shown by the fact that, from microscopic examination of a thin slice of fossil tree, a botanist can tell at once the species to which it belonged. The greater part of the material of the wood has disappeared for it may be millions of years, but its microscopic structure has been preserved by the infiltration of silicious or calcareous materials which, hardening in the pores, have thus preserved a perfect copy of the original. The rapid passage of gases through unglazed pottery, iron and (hot) steel, etc., shows the porosity of these bodies in a very remarkable manner. So does the strange absorp- tion of hydrogen by a mass of palladium. The porosity of steel has recently been shown in a most remarkable manner by Amagat, who forced mercury through a thickness of more than three inches under a presure of at least four thousand atmospheres. The metal was quite impervious to glycerine under the same pressure." At the time this passage was written, some twenty years ago, Tait remarked that decisive proof of the porosity of vitreous bodies, such as glass, had not yet been obtained, but added " that they form almost a solitary class of exceptions to an otherwise general rule seems highly improbable." He then proceeded to show that all bodies whatsoever must necessarily be porous and leaky when sub- jected to great fluid pressure, and he pointed out that the penetra- bility depended greatly on the character of the fluid, thus indicating the great influence of molecular and atomic forces. 19 o6] SEE THE CAUSE OF EARTHQUAKES. 289 To make a practical application of these principles, what shall we now say with respect to the ocean bottoms? In deep places the pressure of the sea water upon them is very great, sufficient to force the water through walls of solid glass several centimeters thick in a short time, and the bed itself in general no tighter than that of a pond in a common field. Obviously, most of these bot- toms will leak, and leak at a rapid rate under the enormous pres- sure operating in the greatest depths of the sea. The bed of the ocean will not leak with equal rapidity in all places, but almost universal leakage will certainly develop; and the water will be driven down into the earth at various rates depending upon the fluid pressure and temperature and the physical character of the sea bottom. Where the rock is volcanic, and badly fractured, or sandy, the leakage will be most rapid, and where the bed is made of fine clay or unbroken granite, the leakage will be much more gradual. It will also depend directly on the depth of the sea, being a maximum where the ocean is deepest, and generally quite insig- nificant in shallow water. The amount of water leaking through any square meter of the sea bottom will be given by an expression of the form w=P.p.f(t).4>(T), where P is the fluid pressure in the bed of the sea, and thus directly proportional to the depth ; p the average porosity of the ocean bot- tom, and thus depending on the kind of ooze, dust, sediment and rocks underlying the sea and their state of compression; and f(t) is some function of the time, depending on the average rate of leakage through the successive strata; and (f>(T) is a function of the temperature, and thus -increasing with the descent into the rocks of the earth's crust. As water is almost incompressible for small or moderate forces, its escape downward would depend upon the continued descent of that which first entered the bed of the ocean, the rate of which would be diminished under the increasing pressure and density encountered in the lower strata, but on the other hand increased by the rising temperature which makes the rocks more penetrable and also augments their power of absorption. Various values of these quantities, P, p, /(/), <1>(T), would give the 290 SEE THE CAUSE OF EARTHQUAKES. [October 19, several rates of leakage for the corresponding areas of the bottom of the sea. In general it is obvious that the leakage will be most rapid where the sea bottom is fractured or porous, the underlying temperature high, and the depth very great. A rapid rate of leakage would imply that large quantities of water quickly come in contact with the heated rock and develop correspondingly great steam pres- sure in the crust which underlies that part of the ocean. Tait's remark about the rapid passage of gases through hot steel ob- viously applies to the absorption and diffusion of steam in hot rock; for this is found by experiment to be quite general for many of the metals. And in the case of lava as it pours from a volcano, it is observed that the molten rock emits vast quantities of vapor, of which, according to Sir Archibald Geikie, 999 parts in 1,000 is steam. This fact in itself is extremely impressive; for it indicates that the remaining thousandth part of the gases emitted, including vapors of sulphur, hydrogen sulphide, hydrochloric and carbonic acid, are derived from the rocks of the earth's crust under the action of steam and the high temperature. We may therefore consider that steam is the only original vapor operating in the crust of the earth. 6. Daubree's experiments on the effects of capillarity. After this paper was fully outlined and some references were being verified, the author had the good fortune to notice the fol- lowing significant statement in Sir Archibald Geikie's admirable " Text Book of Geology," fourth edition, 1903, p. 354: "An obvious objection to this explanation is the difficulty of conceiving that water should descend at all against the expansive force within. But Daubree's experiments have shown that, owing to capillarity, water may permeate rocks against a high counter pressure of steam on the further side, and that so long as the water is supplied, whether by minute fissures or through pores of the rocks, it may, under pressure of its own superincumbent column, make its way to highly heated regions. Experience in deep mines rather goes to show that the permeation of water through the pores of the rocks gets feebler as we descend." In his " Physics of the Earth's Crust," second edition, p. 144, Rev. O. Fisher also makes some interesting remarks on Daubree's ex- periments, which are included in his " Rapport sur les progres de la Geologic experimentale,-" Paris, 1867. After describing Daubree's experiment, Rev. Fisher remarks : r 9 o6.] SEE THE CAUSE OF EARTHQUAKES. 291 M. Daubree conceives that if the layer of rock were of great thickness, and a very high temperature maintained in the cavity, a correspondingly high steam pressure would result, which would be sufficient to raise lava in the vent of a volcano, and to produce earthquakes; while the force so obtained might after expenditure be again and again renewed. "This theory requires the occurrence of cavities at great depth (' sup- posons une cavite separee des eaux de la surface') communicating with the volcanic vents. But the only argument in favor of cavities existing seems to be that the requisite mechanical force is obtainable by means of them; but it seems a priori impossible that there should be such cavities." These passages are of interest in connection with Part VIII. of this paper, where it is shown that such cavities or partial cavities develop from the expulsion of lava from under the bed of the sea, and the resulting subsidence of the bottom causes the great sea waves which so frequently follow violent earthquakes. 7. Historical development of the theory of the penetration of sea water. Although these passages were found too late to have influenced the theory developed in this paper, they are cited here for conveni- ence, and to show some of the historical aspects of the problem of the penetration of sea water. It was much discussed also in Hum- boldt's time, as we learn from his remarks in the Cosmos: " The geographical distribution of the volcanoes which have been in a state of activity during historical time, the great number of insular and lit- toral volcanic mountains, and the occasional, although ephemeral, eruptions in the bottom of the sea, early led to the belief that volcanic activity was connected with the neighborhood of the sea, and was dependent upon it for its continuance." "For many hundred years," says Justinian, or rather Trogus Pompeius, whom we follow, " Etna and the Eolian islands have been burning, and how could this have continued so long, if the fire had not been fed by the neighboring sea?" In order to explain the necessity of the vicinity of the sea, recourse has been had even in modern times, to the hypothesis of the penetration of sea-water into the foci of volcanic agency, that is to say, into deep-seated terrestrial strata. When I collect together all the facts that may be derived from my own observations and the laborious researches of others, it appears to me that everything in this involved investigation depends upon the questions whether the great quantity of aqueous vapours, which are unquestionably exhaled from volcanoes even when in a state of rest, be derived from sea-water impregnated with salt, or rather, perhaps, with fresh meteoric water; or whether the expansive vapours (which at a depth of nearly 94,000 feet is equal to 2,800 atmospheres) would be able at 292 SEE THE CAUSE OF EARTHQUAKES. [October 1 8, different depths to counterbalance the hydrostatic pressure of the sea, and thus afford them under certain conditions a free access to the focus." * Again : 2 " The great number of volcanoes on the islands and on the shores of continents must have early led to the investigation by geologists of the causes of this phenomenon. I have already, in another place (Cosmos, Vol. I, p. 242), mentioned the confused theory of Trogus Pompeius under Augus- tus, who supposed that the sea-water excited the volcanic fire. Chemical and mechanical reasons for this supposed effect of the sea have been adduced to the latest times. The old hypothesis of the sea-water penetrating into the volcanic focus seemed to acquire a firmer foundation at the time of the discovery of the metals of the earth by Davy, but the great discoverer himself soon abandoned the theory to which even Gay-Lussac inclined, in spite of the rare occurrence or total absence of hydrogen gas. Mechanical, or rather dynamical causes, whether sought for in the contraction of the upper crust of the earth and the rising of continents, or in the locally dimin- ished thickness of the inflexible portion of the earth's crust, might, in my opinion, offer a greater appearance of probability. It is not difficult to imagine that at the margins of the up-heaving continents which now form the more or less precipitous littoral boundary visible over the surface of the sea, fissures have been produced by the simultaneous sinking of the adjoin- ing bottom of the sea, through which the communication with the molten interior is promoted. On the ridge of the elevations, far from that area of depression in the oceanic basin, the same occasion for the existence of such vents does not exist. Volcanoes follow the present sea-shores in single, sometimes double, and sometimes even triple parallel rows. These are con- nected by short chains of mountains, raised on transverse fissures, and form- ing mountain-nodes. The range nearest to the shore is frequently (but by no means always) the most active, while the more distant, those more in the interior of the country, appear to be extinct or approaching extinction. It is sometimes thought that, in a particular direction in one and the same range of volcanoes, an increase or diminution in the frequency of the erup- tions may be perceived, but the phenomena of renewed activity after long intervals of rest render this perception very uncertain." 8. Views of Lucretius on the penetration of sea water into Mtna. We have quote the above passage because of Humboldt's saga- cious remarks, some of which deal with the theory of the penetra- tion of sea water as held by the ancients. He mentions Trogus Pompeius under Augustus as the author of the theory, but it is remarkable that the same views were held by the poet Lucretius more than half a century before. 1 Cosmos, Vol. I, p. 242. Bohn's translation. 2 Cosmos, Vol. V, pp. 431-2. All the citations of Humboldt's works are from the Bohn translations. i 9 o6.] SEE THE CAUSE OF EARTHQUAKES. 293 In " De Rerum Natura," Lib. VI, 680 et seq., we read, accord- ing to Munro's translation : " And now at last I will explain in what ways yon flame roused to fury in a moment blazes forth from the huge furnaces of ^Etna. And first the nature of the whole mountain is hollow underneath, underpropped through- out with caverns of basaltic rocks. Furthermore, in all caves are wind and air; for wind is produced when the air has been stirred and put in motion. When this air has been thoroughly heated and raging about has imparted its heat to all the rocks round, wherever it comes in contact with them, and to the earth, and has struck out from them fire burning with swift flames, it rises up and then forces itself out on high, straight through the gorges ; and so carries its heat far and scatters far its ashes and rolls on smoke of a thick pitchy blackness and flings out at the same time stones of prodigious weight; leaving no doubt that this is the stormy force of air. Again the sea to a great extent breaks its waves and sucks back its surf at the roots of that mountain. Caverns reach from this sea as far as the deep gorges of the mountain below. Through these you must admit (that air mixed up in water passes; and) the nature of the case compels (this air to enter in from that) open sea and pass right within and then go out in blasts and so lift up flame and throw out stones and raise clouds of sand; for on the summit are craters, as they name them in their own language ; what we call gorges and mouths." In one important part of this passage, the text is corrupt and the context, therefore, supplied; yet there is absolutely no doubt, from preceding passages stating that the sea penetrates the land, that Lucretius held that the mountain is hollow, the water filters through the crevices and cracks in the rocks, until it comes into con- tact with the subterranean fires which convert it into vapors that give rise to the explosive violence witnessed in the eruptions of We shall see hereafter that Aristotle describes a volcanic eruption as due to the urging blast of pent-up vapor, but it does not seem that he gave any satisfactory explanation of how the vapor developed within the earth's crust. 9. Lucretius' views on earthquakes, " Now mark and learn what the law of earthquakes is. And first of all take for granted that the earth below us as well as above is filled in all parts with windy caverns and bears within its bosom many lakes and many chasms, cliffs and craggy rocks; and you must suppose that many rivers hidden beneath the crust of the earth roll on with violence waves and submerged stones; for the very nature of the case requires it to be throughout like to itself. With such things then attached and placed below, the earth quakes above from the shock of great falling masses, when under- 294 SEE THE CAUSE OF EARTHQUAKES. [October 19, neath time has undermined vast caverns; whole mountains indeed fall in, and in an instant from the mighty shock tremblings spread themselves far and wide from that centre. And with good cause, since buildings beside a road tremble throughout when shaken by a waggon of not such very great weight; and they rock no less, where any sharp pebble on the road jolts up the iron tires of the wheels on both sides. Sometimes, too, when an enormous mass of soil through age rolls down from the land into great and extensive pools of water, the earth rocks and sways with the undula- tion of the water just as a vessel at times cannot rest, until the liquid within has ceased to sway about in unsteady undulations. . . . " The same great quaking likewise arises from this cause, when on a sudden the wind and some enormous force of air gathering either from without or within the earth have flung themselves into the hollows of the earth, and there chafe at first with much uproar among the great caverns and are carried on with a whirling motion, and when their force afterwards stirred and lashed into fury bursts abroad and at the same moment cleaves the deep earth and opens up a great yawning chasm. This fell out in Syrian Sidon and took place at JEg'mm in the Peloponnese, two towns which an outbreak of wind of this sort and! the ensuing earthquake threw down. And many walled places besides fell down by great commotions on land and many towns sank down engulphed in the sea together with their burghers. And if they do not break out, still the impetuous fury of the air and the fierce violence of the wind spread over the numerous passages of the earth like a shivering-fit and thereby cause a trembling" (" De Rerum Natura," Lib. VI, Munro's translation). III. THE GEOGRAPHICAL DISTRIBUTION OF VOLCANOES AND THEIR RELATION TO EARTHQUAKE PHENOMENA. 10. Four fundamental facts to be explained by a theory of volcanoes. A satisfactory theory of the cause of volcanic action must account for the following phenomena : 1. The distribution of some 400 active volcanoes about the mar- gins of the sea, and the numerous eruptions which take place in the sea or on islands, while none at all occur inland at distances exceed- ing about 100 miles from the ocean or equivalent large bodies of water. 2. The fact that 999 in 1,000 parts of the vapors emitted by volcanoes is steam, as if produced by the leakage of the oceans, near which the volcanic vents always are situated. 3. Volcanoes are particular mountains, and all mountains follow the seashore as if formed in some way by the action of the sea upon the adjacent land. I 9 o6] SEE THE CAUSE OF EARTHQUAKES. 295 r ^VT( '.'; i- ? f r.ff- < f i i *Y i >\K 1'ROC. AMER. PHIL. SOC. , XI.V. 184 S, PRINTED FEBRUARY 19, 296 SEE THE CAUSE OF EARTHQUAKES. [October 19, 4. The close geographical relationship existing between vol- canoes and earthquakes throughout the world, and the part played by earthquakes in mountain formation, and the eruption of volcanoes. These four fundamental facts seem to admit of easy and natural explanation on the hypothesis that the penetration of sea water develops steam just under the crust of the earth, and the result is the upheaval of mountains and the eruption of volcanoes^ ii. Professor Milne's researches on the distribution of earth- quakes. H)ne of the most remarkable results of recent research is the discovery of numerous regions greatly affected by submarine earth- quakes, so that it is now known that these phenomena occur not only on land, but more especially under the sea. As we shall treat of this remarkable result hereafter, we shall at present confine our attention to the relations of earthquakes and volcanoes as observed upon the continents. It has long been recognized that both groups of phenomena occur in a series of belts, which follow the same gen- eral regions of the world, along certain so-called lines of weakness in the earth's crust. 1 In a recent review of earthquakes published in the British As- sociation Report for 1902, Professor John Milne has outlined twelve principal seismic regions, some of them of great extent. These several belts include the wide boundaries of the Pacific Ocean, the Antilles and Caribbean Sea region, and the great belt beginning at the Azores, and extending through the Mediterranean to the Hima- layas and India. This last great belt is the only one in which the sea does not predominate over the land, and even here, the sea is paramount over a large part of the area included, while the rest includes or lies adjacent to the highest mountain range in the world^ As Major Button has remarked, it may be doubted whether all of this last region should be included in one area, except, perhaps, as an outline to aid the memory ; but at all events, the Azores and southern 1 Cf. Professor Milne's work on " Earthquakes," edition 1903, which includes an excellent map of the world giving the distribution of both earth- quakes and volcanoes. As -earthquakes in the interior of the oceans until recently were seldom recorded, unless of great violence, the earthquakes charted on the map are chiefly those observed on the land, so that the centres of the oceans appear unduly vacant. I 9 o6] SEE THE CAUSE OF EARTHQUAKES. 297 Europe, made up throughout of broken mountainous regions ex- tending into the Mediterranean, with the Black Sea and Caspian on the east, are not essentially different from the earthquake regions surrounding the Pacific Ocean. In his recent Bakerian Lecture at the Royal Society, March 12, 1906, Professor Milne explains his latest classification of seismic regions as follows : " Regions which lie on the western suboceanic frontier of the American and the eastern frontier of the Asiatic continents, and regions which lie on a band passing from the West Indies through the Mediterranean to the Himalayas. " In addition to these there are two minor regions, one following the eastern suboceanic frontier of the African continent, which I have called the Malagassy region, and an Antarctic region which lies to the southwest of New Zealand. " The following table gives the number of large earthquakes or mass displacements which have occurred in the subdivisions of these regions since 1899- 1899 1900 1901 1902 1903 ii 6 i 3 2 22 3 [902, ind s 1904 Total. Region of the Pacific Ocean. Western Atlantic and Eurasian regions. I. East Indian Archi- pelago ii 19 H 6 9 6 13 4 9 B her, ance 17 5 ii 4 o 7 6 2 4 etwee 1903 s wet 13 5 i 4 2 3 3 8 4 :n MJ ,751 e rec 14 9 i 8 6 o 22 I irch, arge orded 9 14 o o I 4 and mall 75 59 3o 28 16 25 25 62 21 S"ovem- disturb- 2. The coast of Japan... 3 Alaskan coast . .. 4. Central America 5. West of South Amer- ica 6. Antillian region. ... 7. Azores 8. Alpine, Balkan, Cau- casian, Himalayan region 9. Malagassy district 10. Antarctic district .Totals... Oi 56 4r1 64. 1 *8 20 341 " Many of the disturbances included in this table are known to have been followed by hundreds and even thousands of after-shocks. The most active district is at present that of the East Indies, which might well be consid- ered as an eastern prolongation of the Himalayan region. The scene of this activity it may be noticed, is at the junction of two lines of rock folding, which meet almost at right angles. Whether the Antillean and Central American region should be separated is open to question. If we unite their registers as belonging to two comparatively near and parallel earth ridges, the movements of one influencing those 'of the other, we have a region of hypogenic activity approximate to that of the Japan seas. 298 SEE THE CAUSE OF EARTHQUAKES. [October 18, " Generally it would appear that these regions of instability are to be found along the margins of continents or tablelands, which rise suddenly to considerable heights above oceanic or other plains. " At the present time we may, therefore, say that megaseismic disturb- ances do not occur anywhere, but only in districts with similar contours. Are we dealing with primitive troughs and ridges which are simply altering their dimensions under the continued influence of secular contraction, or do these reliefs of seismic strain represent isostatic adjustments which denuda- tion and sedimentation demand ? " Professor Milne then discusses other possible causes, such as the effects of ocean currents and the seasons, including * meteoro- logical causes, such as accumulations of ice and snow at the poles, and finally the motion of the pole in the body of the earth ; and he says that in about thirteen years between 1892 and 1904, he " finds records for at least 750 world-shaking earthquakes," which affords one an impressive idea of the extent of his researches, and of the importance of the subject. \ In general the "geographical distribution of volcanoes is closely similar to that of the earthquakes, but the latter are the more general and widely extended phenomena, while the former are more special. It is remarkable that the volcanoes break out in the centers of the earthquake belts. This relation can not be accidental, but points to a common cause underlying both phenomena^] Besides the active volcanoes near the seashore, and on islands, many of which were heaved up originally by submarine eruptions, nearly every country has a long list of extinct volcanoes. The islands in which volcanic eruptions have ceased, may also be viewed as extinct volcanoes in the sea. In this respect the southern and central Pacific Ocean is particularly rich in extinct volcanoes, and there also, a great many submarine earthquakes are supposed to occur. But the greatest breeding ground for world-shaking earth- quakes, as Professor Milne says, are the deep troughs along the continents, near which many volcanoes usually are burning. As volcanic regions, we may mention, especially, the west coast of South and Central America, the Aleutian and Kurile Islands, Japan, the Philippines, Sumatra, Java, and adjacent islands of the East Indies, New Zealand, the region of Erebus and Terror in the Antarctic, and Iceland, the Caribbean Sea, with the Azores and Canaries, the region of the Mediterranean and Central Asia, west of I9o6 .] SEE THE CAUSE OF EARTHQUAKES. 299 the Himalayas. In such of these regions as fall far within the con- tinents, the volcanoes have in all cases died out for lack of water, but the earthquakes still exist as a survival of former conditions. This is true, for example, in the regions of Central Asia, which no longer has any active volcanoes, though some were active there not very long ago geologically, and thus exhibit still a fresh and even sulphurous appearance. 12. The outbreak of new volcanoes within the historical period. It may be mentioned here that within historical times the follow- ing new volcanoes have broken forth : 1. Monte Nuovo, eight miles from Naples,. September 28, 1538. 2. Jorullo, in Mexico, September 29, 1759. 3. Izalco, San Salvador, February 23, 1770, 5,000 feet high, thrown up on what was formerly a cattle farm. 4. Las Pilas, on the Plains of Leon, Nicaragua, April n, 1850, a small volcano. 5. Ilopango, Nicaragua, January 20, 1880, a small volcano, thrown up in a lake 600 feet deep. 6. Fusiyama, Japan, 12,365 feet high, which tradition says was thrown up in a single night, about 300 B. C. 7. Tarewera, New Zealand, January 10, 1886, a mountain with a flat top, which previously had given no volcanic indications. There are perhaps other volcanoes, some of them mentioned by Strabo, which have broken forth on land ; and a good many more which have been upheaved in the sea. Many old volcanes long extinct have burst forth into renewed activity, generally with terrible violence. Any volcano may become extinct or dormant, and then again break forth. In his work, on " Volcanoes," Professor Bonney often speaks of a mountain as having lost its crater ; and mentions in this class Ixtaccihuatl and Chimborazo ; but although it is probable, it is not certain that either of these has ever been active. 1 Yet according to the view developed 1 In his two ascents of Chimborazo, Whymper found lava and other volcanic indications, which had escaped the notice of Humboldt and Bous- singault, who did not regard the mountain as volcanic. The adjacent moun- tain of Carihuairazo, said to have been higher than Chimborazo before the crater collapsed, June 19-20, 1698, might have ejected the volcanic products noticed by Whymper on Chimborazo, though it seems improbable. 300 SEE THE CAUSE OF EARTHQUAKES. |p c tob r , 9 , in this paper any mountain may become a volcano, on short notice, if the internal violence is sufficient to break open an outlet for the vapors which always slumber beneath. We shall see, hereafter, that the mountains are all filled with volcanic materials, and an explosion is all that is required to set them going, and this is usually effected by the throes of an earthquake. All new volcanoes, and old ones when they burst forth into renewed activity, do so with violent earthquake shocks. The shocks of an earthquake almost always have some effect on a burning volcano, and in earthquakes remote from erupting centers, the breaking out of a volcano causes the shocks to cease, as was long ago noticed by Strabo. Since this intimate connection has been observed again and again, and the volcanic and earthquake belts are generally similar, though not strictly identical, throughout the world, there is a very strong indication that both depend upon a common cause, and that cause is nothing else than ordinary steam. It is worth while to notice that as Central America is a narrow country, with fairly deep seas on both sides, it is exactly where we should expect volcanic forces to have great sway, and observation shows that this is true for earthquakes as w r ell as volcanoes. The recurrence of frightful earthquakes in that region, and the upheaval of three new volcanoes within historical times speaks for itself, and shows that all the mountains are not yet finished ; and that some of the land in Central America is being elevated by forces depending on the influence of the sea, whether volcanic or seismic. As the result of his observa- tions Darwin held that volcanoes break out in rising areas, most likely because an outlet is easily established when the outer layers are cracked open to a great depth. 13. The relation of earthquakes to volcanoes. . In his interesting work on " Earthquakes in the Light of the New Seismology," p. 43, Major Dutton follows Professor Milne in his classifications, and remarks : " Though it is possible to indicate regions which present both volcanoes and earthquakes, there is no proof of interdependence between seismicity and vulcanicity in general. While there are earthquakes which are certainly of volcanic origin, the one phenomenon does not necessarily imply the other." Professor Milne, Omori, Dutton, and others have recently at- tempted to disprove the relationship of earthquakes and volcanoes i9o6.] SEE THE CAUSE OF EARTHQUAKES. 301 exhibited by the shores of the Pacific Ocean, and their" mode of at- tack has been to show that the volcanoes around the Pacific are not a continuous " girdle of fire," but are bunched here and there, with large spaces between; and that while the earthquakes are also dis- tributed with some irregularity, there is no visible connection be- tween them and the volcanoes. But if steam forming in the earth's crust from sea water leaking down is the common cause of both earthquakes and volcanoes, should there really be any immediate connection between the two classes of phenomena? Would not volcanoes develop chiefly where the force of the steam was sufficiently powerful and suddenly exerted to break through the crust or mountains, and therefore chiefly in the mountains along the seashore, where the crust is greatly frac- tured, and enables the violent explosions of steam to blow open an outlet by raising a mountain which would burst into a volcano? It is along such shores also that the leakage would be greatest and most volcanoes should exist, provided the crust becomes badly fractured. If, on the other hand, the crust is not much broken and ex- plosions of steam cannot break through, would there not result a great many earthquakes of the class now called tectonic because not visibly connected with volcanoes and supposed to be due to slipping of rocks or faults? When the crust is wholly unbroken, it would naturally be very difficult, even for deep-seated forces of enormous magnitude, to raise up a mountain that would become a volcano, because all the overlying strata would have to be violently broken in such a way as to radiate from a point like a star, and ordinarily the strain of the imprisoned steam is much more easily released by an earthquake which merely shakes up the crust in such a way that a neighboring fault moves and the internal pressure is relieved and equalized by scattering, without breaking through all the overlying strata at one time. This indeed appears to be the process of nature, and if we consider it in relation to volcanoes and earthquakes we shall per- ceive, in accordance with observation, that the former should be the more special, the latter the more general phenomena. Also both phenomena should occur under the sea, and along the shores of the 302 SEE-THE CAUSE OF EARTHQUAKES. [Octob.r 19. deepest oceans ; but volcanoes would develop chiefly in certain regions where the rocks are already broken in the uplift of moun- tains and therefore easily burst open, whereas earthquakes might occur in any locality where the leakage of the sea developed suffi- cient steam. It is undeniable that this is in accordance with obser- vation on our actual earth ; and it shows that while both volcanoes and earthquakes should surround the Pacific Ocean, earthquakes are much more widely and uniformly distributed than volcanoes. Also in those regions near actual volcanoes, where the imprisoned steam has a vent, violent earthquakes should not occur; but if the activity of the volcano ceases, the danger of earthquakes would be increased. Humboldt remarks that this opinion was widely spread among the people of the Andes, and it would be difficult to deny that this result of their long experience was well founded, though confessedly they did not know upon what principle the dreaded explosions depended. If the leakage from the sea has moderate uniformity with respect to the time, it is clear that the cessation of the smoke of a volcano is really one of nature's danger signals, since the pressure within the subterranean reservoirs of the mountain and adjacent regions may then increase to such a degree as to become extremely dan- gerous. Neither Krakatoa nor Pelee had been active for long periods before the fearful explosions of 1883 and 1902. Krakatoa had been practically dormant for two hundred years, and while Pelee had experienced an eruption in 1851, it was small, and no Important explosion had occurred since I7&2. 1 In the case of Ve- suvius the general experience is the same the longer the eruptions are delayed the more violent they become. For it appears that in 79 A. D. no eruption had occurred for about six centuries, and Pliny's description of that outbreak shows that it was more violent than any that has occurred since. The volcano of Conseguina in Central America illustrates the same principle by the long repose preceding the frightful eruption of 1835, which spread devastation far and wide, and in many ways resembled the terrible outbreak of 1 Cf. Heilprin, " Mont Pelee and the Tragedy of Martinique," pp. 61-187, 188. a9 o6 ] SEE THE CAUSE OF EARTHQUAKES. 303 Krakatoa. 1 It has so often been observed that the earthquakes ceased on the eruption of a neighboring volcano, that one cannot doubt that direct relief was afforded by the eruption. Viewing the relation of earthquakes and volcanoes in this light, we can easily understand why many of the so-called tectonic earth- quakes are doubly severe much more violent than those closely connected with volcanoes because where no volcanic outlet has been available, the explosive strain increases to an enormous extent before it can obtain any relief whatever ; and when the yielding does occur the shock is one of appalling violence, and does great damage causing the slipping of rocks, faults and subsidences, and is felt over a very large area, because the explosive strain has become deep- seated and intense. The great depth at which many of the so-called tectonic earth- quakes have been proved to occur, is at once an argument against the dislocational or faulting theory, and a convincing proof that shocks of this type are due to the explosive power of superheated steam. These shocks are obviously too deep-seated to be accounted for by subsidences, and moreover the resulting vibrations are too complex to be due to mere slipping of a ledge of rock, as will be more fully explained hereafter. It may be shown that no possible subsidence of rock faults could produce a conspicuously rotatory earthquake like that which destroyed San Francisco. IV. THE GENERAL CAUSE OF THE FORMATION OF MOUNTAINS AND THEIR GEOGRAPHICAL DISTRIBUTION. 14. On the formation of mountains and Cordilleras, as illus- trated by the Andes. If we consider the deep trough running for a great distance parallel to the coast line of the western shore of South America 2 and recall that other deep troughs of the same kind exist parallel 1 In chapter XVI of his valuable work on " Earthquakes," edition of 1903, Professor .Milne cites several other eruptions of fearful violence accom- panied in each case by terrible earthquakes. 2 The trough is not of uniform depth throughout its course, but the depression is always conspicuous, so that everywhere the earth's crust is arched downward. 304 SEE THE CAUSE OF EARTHQUAKES. [October 19, to the Aleutian and Kurile Islands, the east shore of Japan, the west shore of Sumatra and Java ; also near New Zealand and vari- ous islands in the deepest oceans, as Guam, the Bahamas and other West Indian Islands, we shall perceive that this arrangement is not by chance. The South American trough always appears parallel to the great mountain ranges of the Andes, and the fact that it is FIG. 3. Outline Map of South America, showing the great Ocean Trough parallel to the Andes. of about the same volume as the matter included in the Cordilleras appeared to be a suspicious circumstance. The relation above cited for Japan, Java, and other islands is similar, but in the case of oval islands the adjacent depression may not be a trough, but rather a hole of somewhat oval or elliptical figure. Some years ago the writer noticed these remarkable sinks while I 9 o6.] SEE THE CAUSE OF EARTHQUAKES. 305 examining a relief cast of the Atlantic Ocean exhibited in the office of the United States Coast and Geodetic Survey at Washington, and remarked that it seemed as if the volumes of the upraised islands were not very much larger than those of the adjacent depressions. Why should depressions exist so near these elevations above the sea, and, in the case of mountain ranges, so nearly parallel to them for long distances? Is there not obviously a direct connection be- tween the elevated land and the unusual depression in the adjacent sea bottom ? To understand just what this connection is, we may recall that after the great eruption of Mt. Pelee in 1902, it was found by actual measurement that a considerable portion of the adjacent sea bottom FIG. 4. Vertical Section perpendicular to the Andes and Andean trough, drawn to natural scale, and showing the mode of operation of the trough in the formation of mountain and cordilleras. had sunk down hundreds of fathoms. 1 It is impossible to be- lieve that this settling of the bottom of the sea could be due to the 1 This statement is perhaps somewhat too positive, for Dr. O .H. Titt- man, superintendent of the U. S. Coast Survey, informs me that reliable determinations of depth before the eruption of Pelee seems to have been insufficient to decide the question satisfactorily. The cables were broken, and the subject investigated by the French Commission (Lacroix, Alf, La Montagne Pelee et ses eruptions, Paris, 1904), which includes M. Rollet de 1'Isle's investigation of the reported changes of depth in the vicinity of Mar- tinique. The French commission was inclined to ascribe the disturbances to submarine volcanic action, rather than to subsidences. This, however, is not a matter of great importance ; for in his work on " Seismology," p. 35-36, Professor Milne mentions several well established cases of subsidences in the Mediterranean and in the Pacific Ocean off the Esmeralda River in , Ecuador. He points out that " disturbances originating beneath the sea, which are much more numerous than those originating beneath the land, likewise emanate from a region of strain. Mr. W. G. Forster, who has paid so much attention to the earthquakes of the Mediterranean, tells us that they have been accompanied by great subsidences of the sea bottom." 306 SEE THE CAUSE OF EARTHQUAKES. [October i 9 mere shaking of the earthquakes accompanying that eruption; and we must, therefore, suppose that after matter had been expelled by the dreadful explosions which destroyed St. Pierre and devastated Mar- tinique, or in earlier eruptions, a subsidence near the roots of the mountain actually took place. Again, in 1835, Captain Fitzroy and Charles Darwin observed that after the violent earthquake which destroyed Conception, the Chilian coast line in that region had been elevated from three to five feet for several hundred miles. Not only the coast but also the whole country back to the Andes was raised. This could only be explained by the injection or forcing in of a corresponding bulk of lava under the land ; and this lava could come from nowhere except from under the bed of the great trough in the adjacent sea. The ultimate effect would be to cause the trough of the ocean to deepen correspondingly. And, moreover, such peri- odic injections from under the sea trough would not only push along the ejected stream of lava, step by step, until the end of the column reached the mountains, but the forces thus arising would supply the " lateral thrusts " which are said to be much needed for the explanation of the upheavals, the tipping of the strata, the inclina- tions and sometimes reversed positions of the rocks, and other geo- logical phenomena observed in mountains like the Andes. Hereto- fore the abundant phenomena of this kind noticed in all high moun- tains have not been satisfactorily explained. A correct theory must account for the inclinations seen in the mountains as well as the rising of the coast, and such submarine earthquakes as Darwin observed to precede the uplift of the beach at Conception. The present theory seems to be capable of meeting this severe test, and it requires us to make no assumption except that molten lava may be forced from under the bed of the trough, and pushed along its course beneath the crust by the throes of successive earthquakes. It is recorded that a great sea wave followed the Chilian earth- quake of 1835, and such waves are very frequent along the Chilian and Peruvian coasts. They almost always follow an earthquake, and begin by a recession of the sea from the shore, which then returns as a great wave, carrying everything before it. Some have supposed the sea bottom to subside, thus withdrawing the water toward the sink, till it flows in on all sides to fill up the depression, and then I90 6.] SEE THE CAUSE OF EARTHQUAKES. 307 piles up and returns as a great wave which continues to oscillate furiously, sometimes for days after the earthquake. We shall con- sider these waves more fully hereafter, and at present it is sufficient to remark that this explanation is satisfactory for the kind of waves usually observed along the west coast of South America. We may then suppose that in such earthquakes a very large mass of lava is forced from under the sea, which then settles below its former level, and the great wave follows. If the lava is forced toward the land, the coast or mountains are upraised ; if towards the ocean, a ridge may be upheaved there, or possibly a submarine vol- cano of large extent. In either case the trough of the sea bottom parallel to the coast eventually becomes less stable, and, at certain intervals, settles little by little, when the consistency of underlying FIG. 5. lava has been thinned by successive ejections ; and thus with the settling stability is again restored. As the trough is arched downwards towards thfe exploding lava the steam pressure from beneath cannot force it upward ; and the strain is necessarily relieved by motion of the lava towards the Andes or the ocean usually towards the mountains till the trough gets broad and deep and the mountains very far away and so high that the movement of the column offers unprecedentedly great re- sistance, when the release will at length become easier towards the ocean by the forcing up of ridges or volcanoes along the other margin of the trough. Ridges with peaks in them will usually re- sult, and this is the beginning of the new Andes or Cordilleras, which are destined to rise slowly from the sea, leaving a deep valley towards the ancient shore, to be drained and filled in by erosion. Thus we explain some of the remarkable parallel ridges of 308 SEE- THE CAUSE OF EARTHQUAKES. [October i 9 | the Cordilleras. And it is natural that in this upheaval of the crust, release of strain due to subterranean steam pressure should occasionally come by the throwing up of cross ridges, sometimes enclosing undrained areas, and thus lakes like Titicaca are formed. Proceeding upon this simple and natural principle, we may easily explain all the chief characteristics of the Andes. It is impossible to doubt that these mountains have been formed by the very forces which we see still at work there. The upheavals have been step by step, and earthquakes forcing up the mountains have at the same time caused the ejection, by the pushing along of a column or rather a layer, of the necessary matter from under the sea, thus sinking the bottom into a permanent trough, while the subsidences accompany- ing some of the earthquakes have produced enormous sea waves. Countless thousands and perhaps millions of these earthquakes ancl sea waves have occurred throughout past geological ages. The trough parallel to the coast and the upheavals and sea waves now observed are a survival to show us just how the moun- tains have been formed, and where the next mountain range will form in the sea. We can predict the formation of the new Andes as confidently as we can an eclipse, though it will be a much longer time before the new mountains develop ; for we recognize the cause to be a true one, and see just how it works by a kind of self-regulating automatic process. The working of the cause has been observed near Mt. Pelee, and the operation of the same process along the South American coast is proved by the observations of Charles Dar- win and by the great sea waves frequently observed within historical times. 15. Investigation of the significance of the observed lay of mountain chains by means of the theory of probability. In their new work on " Geology," Vol. I (p. 543), Chamberlin and Salisbury remark that the relationship between the direction of folded ranges of mountains and the adjacent seacoast is " a coinci- dence that is only in part causal.'' There are, doubtless, many ways in which this problem could be treated by the methods employed in theory of probability. Without claiming to exhaust the various lines along which the discussion might be developed, we believe the fol- lowing method rests on equitable considerations. I 9 o6.] SEE THE CAUSE OF EARTHQUAKES. 309 Imagine a mountain chain like the Andes which runs near the shore cut up into pieces each long enough to reach the sea. If there is no physical cause why the chain should be parallel to the seashore, some of the pieces might be expected to lie at all angles with respect to the shore line of the coast from o to 90, and thus the chain's most probable form is that of a zig-zag line made up of FIG. 6. short pieces lying at all angles. Take the intervals of angular dis- tribution of the pieces of the chain at 9 ; then, excluding the exis- tence of physical causes, any angle from the first interval, o to 9, to the last of these subdivisions, 81 to 90, must be held to be equally probable. At any place there are ten divisions of the quad- rant, all equally available for the mountain chain to follow. The 310 SEE THE CAUSE OF EARTHQUAKES. [October , 9 , probability that the direction of a piece of the chain will fall in any one of these divisions of the right angle is one-tenth ; and the prob- ability that all the n pieces throughout the whole chain will fall in the same angular division is (i/io)". When n is a large number, or the chain is long and close to the sea, this probability becomes prac- tically zero. In such a range as the Andes it is observed that all the pieces of the chain do fall in the first division of the angle, between o and 9; and, hence, in general, the probability is (io) n : i that the observed lay of the chain so exactly parallel to the shore of the sea is not the result of mere chance, but depends directly on some physical cause which has made the chain essentially straight as well as laid out the general course parallel to the sea coast. If the chain had the short bends in it here assumed to be pos- sible, the total length would be greater than that of the existing chain, and n would be correspondingly increased. The data used, therefore, make n a minimum, and P = i/(io) n a maximum for the given chain everywhere so closely following the seashore. Thus the calculated value of P is too large rather than too small, with the existing lay of the chain. Another way of reaching analogous results is to consider what the deviation from strict parallelism is in so long a chain, and the probability that the coincidence would be so exact throughout, when all angles between i" and 324,000" (the equivalent of 90) are equally probable. If no physical cause is involved depending on the sea, there is no reason why the chain should not run at any angle across the shore line. Now, the Andes are made up on the average of at least two parallel chains, and, the probability of this double parallel trend throughout would be only 324,000 324,000 114,976,000,000 In any case, we see that for the double chain, the chances are hun- dreds of billions to one against strict parallelism to the seashore. In the first method of treatment each part of the chain is con- sidered, without regard to the rest ; in the second method, the chain is viewed more as a whole, and the individual parts neglected. In respect to the first method, it might be claimed that as mountains 19 o6.] SEE THE CAUSE OF EARTHQUAKES. 311 arise from foldings of the crust, and as the earth's crust is thick, a zig-zag form with many bends in it would be improbable, because a crack started in the rocks anywhere would be likely to run in. a straight line. There may be some justice in this criticism, but it seems quite fully compensated for by the fact that the chain actually bends wherever the coast line alters it's course. Thus in practice the chain is shown to be capable of flexure wherever the shore line changes its direction, and there does not seem anything improbable in many short bends, unless the trend has some connection with the coast. Whether the chain could fairly be conceived as bending at such short intervals is a question we need not enter into, for we may observe that short bends actually appear in certain chains, and thus the hypothesis is not contrary to nature under certain conditions. In the present case we have made no assumption as to causes, except that the lay of the chain is independent of the seacoast, and hence the hypothesis postulates nothing improbable. To reduce the first method to numbers, we may observe that the length of the chain of the Andes is 4,400 miles and the average distance from the sea about 66 miles. Thus 4,400 i n= - = 66^ or P= - = i : (decillion) 2 If other parallel ranges be included, this divisor would be much increased, perhaps nearly squared. On the other hand, the method of viewing the chain as a whole makes the divisor a quantity of the order of one hundred billions. The truth must, I think, lie somewhere between these extremes. If we were to take account also of the mountains parallel to the Atlantic coast, it would certainly be moderate to conclude that the parallelism to the seashore noticed in the whole of South America, so far as it depends on chance, would be less than i : (decillion) 2 . Thus it is clear that the probability of a physical cause connect- ing the mountains with the parallel shore of the sea is probably more than a decillion decillions to unity, and certainly more than one hundred billions to unity. The parallelism noticed in North America along the Pacific and Atlantic coasts, is not less pronounced, nor is there less extent of PROC. AMER. PHIL. SOC., XLV. 184 T, PRINTED FEBRUARY 2O, 1907. 312 SEE THE CAUSE OF EARTHQUAKES. [October 19, mountains involved. On the contrary, the ranges of North America exceed in length those of South America. The Rocky Mountains are indeed farther from the coast than the Andes, but the shore line has receded since they were formed; while the Sierra Nevada and Coast Ranges are nearer the present shore. When one considers all these circumstances, including the greater length of the chains, FIG. 7. and the greater number of parallel ranges, notwithstanding their distance from the seacoast, it will be found that in North America P' is certainly not larger than P as found for South America. Thus we may put them approximately equal to each other, and write P. P'=-r- r ' 7 ^= l ' (decillion) 4 (io) 66 (io) b6 t In Africa the mountain ranges are not high, but they run quite 19o6 .] SEE THE CAUSE OF EARTHQUAKES. 313 parallel to the shore. We may, therefore, without appreciable error put P>=- (io) 66 and p. P'. P" = i: (decillion) 6 In the other three continents, Europe, Asia, Australia, the lay FIG. 8. of the mountains is such as to justify us in taking P'" . P iv . P v P. P'. P". And, therefore, for the whole world, we may safely take P. P f . P". P'". P iv . P v =i: (decillion) 12 This number is so infmitesimally small, or the divisor is so fabulously large, that it becomes an absolute certainty that the paral- lelism of the mountains to the seashore depends on a true physical cause, and that cause can be nothing but the action of the sea itself. Since the mountains always wall in the land, it follows that they are erected by the sea, through injection of the coast by lava ex- pelled from under the ocean bed. Accordingly, it follows that the crust is bent parallel to the seashore by a true physical cause. 314 SEE-THE CAUSE OF EARTHQUAKES. [October 19, If instead of putting P = i : (decillion) 2 we had used P = i: (100 billion), the final result would have been P. P'. P" . P'". P*. PV. = I : (100 billion) 6 . Even this divisor is so infinitely large that the fraction totally disappears, and it becomes an absolute certainty that the lay of the mountains depends on the action of the sea as a physical cause ; and that action can be nothing else than the injection of the coast with lava. By this process the mountains were upheaved. The lay of the FIG. 9. mountains parallel to the sea is, therefore, no " coincidence that is only in part causal," but the direct outcome of a general law of nature. How universal this law is may be inferred from the unerr- ing precision with which it is exemplified in a region such as that about the Bay of San Francisco. Here the mountains line the shores on all sides, and change their course in such a way as to enclose the bay with walls so close by and well fitting as to leave no doubt about the origin of the surrounding mountains. A deceptive way of viewing such an argument as the foregoing I 9 o6.] SEE THE CAUSE OF EARTHQUAKES. 315 is to claim that the sea, because of its fluid nature, flows into the depressions in the earth's crust, which are due to subsidence or collapse; and when these depressions are filled up they are bound to be surrounded by higher regions of hills or mountains, due to wrinkles in the crust. This method of reasoning ignores the exact FIG. 10. parallelism to the seashore, which held for every mountain chain in the world at the time of its formation, and still holds for nearly all the principal ranges, though in a few cases the lapse of ages has modified the direction of the shore of the adjacent sea. The result here established is, therefore, a fundamental law of nature, and it gives the key to the leading phenomena of the earth's surface. 316 SEE THE CAUSE OF EARTHQUAKES. [October 19, 1 6. Hozv a sea valley develops and gives rise to parallel moun- tain chains, as illustrated in the San Joaquin, between the Sierra Nevada and Coast Range, in California. We have already seen that mountains are raised by the injection of the coast by steam-saturated lava exploding beneath the earth's crust. To understand the entire working of this process under good conditions, we might study the different sea valleys now existing in various parts of the world, or take one which shows the characteris- tic features of the process. If we could find one in which the process is complete, but of recent date geologically, its present form would, no doubt, enable us to make out the transformation which is under- gone at different stages. The Sierra Nevada mountains, with the adjacent San Joaquin valley, appear to be an ideal case to illustrate the process in question. A study of the Sierras in California shows that the western slopes of these gigantic mountains are very gradual less than one in fifty and braced by many spurs, with deep intervening canons, of which Yosemite is the most famous. The eastern slopes of the Sierras are about ten times steeper than the western, and the jutting spurs are largely wanting. This shows that the injecting forces which raised these mountains came almost entirely from the west ; and they continued so long that they finally gave the range an unsymmetrical form 1 gently sloping and deeply corrugated with canons on the west, and steep and precipitous on the east. The form thus taken by the Sierras would indicate that at a late stage in their history the San Joaquin valley took the form shown in the accompanying figure, long and sloping on the east and 1 The more gradual slope of a mountain range toward the sea is due to two causes more or less distinct: (i) The vertical upheaval of the chain, with the successive horizontal thrusts which push it little by little from the sea, thus naturally making the farther slope the steeper; (2) the subse- quent elevation of the shore, by injections under the crust, which tips the range still further over, by raising the base of an incline that is already gradual. These two causes combined will be found to explain the principal inequalities in the slopes of mountain ranges as observed in different parts of the world. When the range is being first upheaved, the injections give a nearly vertical uplift; as the range gets older the injections come more and more from the seaward side; when the range itself is finished, the injections only tip its base upward, and make the seaward slope more and more gradual. I 9 o6.] SEE THE CAUSE OF EARTHQUAKES. 317 steep and precipitous on the west. And when this form was once attained the upheaval of the Coast Range became inevitable. The present position of the San Joaquin river near the western side of the valley still shows this form of the valley, and enables us to see the precise process of transformation. It is, perhaps, doubtful whether the elevation of these mountains has yet ceased; the earthquakes in California and the low level of the valleys would seem to show that the whole state is still rising, FIG. ii. a. Mountain formation just beginning. Mountain formation in the middle stages. c. Mountain formation in the later stages. d. New range rising from the sea. and I am told that this is also shown by beaches and shells at many places along the coast. The same principles which are here applied to the Californian mountains can be applied to other mountain ranges throughout the world. 17. Significance of the asymmetry of a mountain chain with respect to its principal axis. It is generally noticed that most mountains are unsymmetrical on the two sides ; one side has a gradual slope, while the other is steep and precipitous. Moreover, the spurs jutting out from the range are unequally divided between the two sides, the larger number of 318 SEE THE CAUSE OF EARTHQUAKES. [October*,, spurs being on the side where the slope is gradual,- which is always turned toward the sea. Let us now examine the meaning of this arrangement. In the new work on Geology by Chamberlin and Salisbury (Vol. I, p. 542-3) we read: " Mountain- forming Movements. Along certain tracts, usually near the borders of the continents, and at certain times, usually separated by long intervals, the crust was folded into gigantic wrinkles, and these constitute the chief type of mountains, though not the only type. The characteristic force in this folding was lateral thrust. The strata were not only arched, but often closely folded, and sometimes intensely crumpled. In extreme cases, like the Alps, the folds flared out above, giving overturn dips and reverse strata, as illustrated in the chapter on " Structural Geology," pp. 501-511. In these cases there was an upward as well as a horizontal move- ment, for the folds themselves were lifted; but the more horizontal thrust so much preponderated, and was so much the more remarkable, that the upward movement was overshadowed. It is well to note, however, that these mountain ranges are crumpled outward and not inward, as might be expected if they resulted simply from the shrinkage of the under side of a thin shell. The folds are sometimes nearly upright and symmetrical, and sometimes inclined and asymmetrical, as illustrated in the chapter referred to. Where the folds lean, the inference has been drawn that the active thrust came from the side of the gentler slope, the folds being pushed over toward the resisting side, and this seems to be commonly true." Thus we have good authority for the statement that the lateral thrust came from the side of the gentler slope. It is well known that the gentler slope is turned towards the sea, and thus we realize that the forces which pushed the mountains horizontally was directed from the adjacent ocean. In his great work on " Face of the Earth," * Professor Suess records the following facts, all bearing on the above view : 1. In Vol. I, p. 452, Suess shows that the tangential movement in the Himalayas and Burmese Mountains on the opposite sides of the Bramaputra are in opposite directions, each being directed from the center of the river exactly what the present theory requires, and not explainable on any other hypothesis. 2. In Vol. II, p. 34, Suess shows that the mountain folds in the eastern part of the United States " have been produced by a tan- gential movement directed from the existing Atlantic Ocean toward the mainland." On page 139 he shows that the same principle holds for South America. 1 Oxford Translation by Dr. Hertha Sollas. I9o6 | SEE THE CAUSE OF EARTHQUAKES. 31i) 3. In Vol. II, p. 121, Suess shows that the " prevailing tangential movement in the Alps and Pyrenees " is toward the north. Thus for the Alps, Lombardy is the most active ancient sea trough ; and in the case of the Pyrenees, Suess shows that most of Spain was then in the bed of the sea, and has since arisen (pp. 123-128). 4. That the Sierra Nevada folds were produced by tangential movement from the side of the Pacific is generally recognized by geologists. Dana and others long ago have remarked the same thing about the Andes (Suess, Vol. I, p. 539), and recently, Cham- berlin has written me that most of the mountains give evidence of having been upheaved by lateral thrusts from the direction of the sea. In view of these facts is not the significance of the asymmetry of mountain chains perfectly plain? The unsymmetrical build of the chains shows that the forces by which they were formed were di- rected from the sea. And, as these forces could not have been subaerial, they must have been subterranean, working just under the earth's crust, and identical with those observed in earthquakes, when lava is expelled from the sea and pushed under the adjacent coast, along which the mountains always run so exactly parallel. By no possibility could any supposed contraction of the earth have given rise to these features in mountain structure, since in that case it would be impossible for the shape of the ranges and tilting of the strata, pointing to lateral thrust, to be always directed from the sea. The arrangement and structure of mountains thus contradicts the contraction theory of the globe, and shows that any supposed effect of contraction was insensible. 1 8. Criticism of the contraction theory of the formation of a range such as the Alps. In addition to the considerations advanced by Fisher, as ex- plained elsewhere in this paper, to show that mountains formed by wrinkles in the crust would in no case exceed a very small height, and should, moreover, be distributed with some uniformity over the globe, we may here consider some objections to the view that a chain such as the Alps has been produced by shrinkage. To get Elie de Beaumont's theory clearly before us, we quote it as given by Lyell, " Principles of Geology," I2th ed., Vol. I, p. 119: " The origin of these chains depends not on partial volcanic action or a 320 SEE THE CAUSE OF EARTHQUAKES. [October*,, reiteration of ordinary earthquakes, but on the secular refrigeration of the entire planet. For the whole globe, with the exception of a thin envelope, much thinner in proportion than the shell to an egg, is a fused mass, kept fluid by heat, but constantly cooling and contracting its dimensions. The external crust does not gradually collapse and accommodate itself century after century to the shrunken nucleus, subsiding as often as there is a slight failure of support, but it is sustained throughout whole geological periods, so as to become partially separated from the nucleus until at last it gives way suddenly, cracking and falling in along determinate lines of fracture. During such a crisis the rocks are subjected to great lateral pres- sure, the unyielding ones are crushed, and the pliant strata bent, and are forced to pack themselves more closely into a smaller space, having no longer the same room to spread themselves out horizontally. At the same time, a large portion of the mass is squeezed upwards, because it is in the upward direction only that the excess in size of the envelope, as compared to the contracted nucleus can find relief' This excess produces one or more of those folds or wrinkles in the earth's crust which we call mountain-chains." It is unnecessary to dwell on the violence of the hypothesis that the nucleus has shrunk away from the crust, as here outlined. So far as one can see, no such result is possible, nor is the shrinkage ever appreciable. But we may here remark that a radial shrinkage of one mile will give a shrinkage in the semi-circumference amounting to 3.14 miles. Whether correctly or not, it has been estimated by geologists that the amount of folding in the Alps exceeds one-third of the whole space now occupied by these mountains, the shortening of the original crust being placed by Heim at 74 miles. Analogous results have been reached by Claypole and others regarding the mountain ranges of America. It should be observed that to afford a slack for folds amounting to 74 miles, a radial shrinkage of about 12 miles is required, even when all of the tangential movement is carried round to one point. To carry all the tangential movement round to one point would imply one of two things : ( i ) That the crust is loose from the globe it surrounds, and thus can be carried around to one point from a whole semi-circumference, which seems altogether improb- able; (2) that if the crust is thus shrunk up without being carried around loose from the globe, the matter underlying it must be condensed to about three-halves its former density. The cone of matter underlying the Alps, and extending to the center of the earth would thus have a density 50 per cent, greater than that i 9 o6.] SEE THE CAUSE OF EARTHQUAKES. 321 occurring under neighboring areas. This latter result is impossible, since observations show that the matter under mountains not only is not denser than the average, but actually lighter by an appreciable quantity. We know, therefore, that the wrinkling has not con- densed the matter underlying the mountains. On the other hand, it seems equally incredible that the shrink- age of the whole globe should be brought forward to one point, as if the crust were loose from the globe it covers. No part of the theory of mountains formed by wrinkles of the crust is to be seri- ously entertained. Besides the difficulties just mentioned, the postulated radial shrinkage of 12 miles is too great. It may well be doubted whether a shrinkage of one mile in the radius has taken place since the continents began to emerge from the oceans. Professor Suess (Vol. II, p. 552) says: "As a result of tangential thrusts, the sediment of this (Mediterranean) Sea were folded together and driven upwards as a great mountain range, and the Alps have, therefore, been described as a compressed sea." We must, therefore, seek the explanation of the formation of the Alps in some process by which this folding can have taken place in the sea, or along its borders, and thus we reach the theory outlined in this paper. 19. Why ive abandon the contraction theory of mountain for- mation. While the considerations here adduced for the origin of moun- tains seem conclusive, it may not be wholly without interest to point out some difficulties which are not satisfactorily met by the con- traction theory, which is the only one now in general use. It is usually stated that mountains result from a crumpling of the earth's crust, and that the crumpling takes place along the principal lines of weakness. This theory fails to explain the origin of isolated peaks or associated groups of peaks which sometimes rise like cones or groups of cones, often more or less intersecting, in the midst of comparatively regular plains. A theory w r ith this serious defect is highly unsatisfactory. If then the contraction theory fails to explain isolated peaks and groups, which are sometimes pushed up in comparatively level plains, and fails to explain the conspicuous parallelism to the sea- 322 SEE THE CAUSE OF EARTHQUAKES. [October 19 shores, while the account given of cross ranges and parallel ranges standing in isolation is unsatisfactory, it must be admitted that the theory itself is not well founded. The assumption that since the continents began to rise from the oceans the earth has shrunk enough to produce great wrinkles in the crust comparable with our high mountains is undeniably a violent hypothesis. For in the writer's paper on the rigidity of the heavenly bodies (A. N. t 4104), it is shown that no circulation of currents within the earth has been possible since the globe became encrusted. If there are no currents within, the propagation of heat outward could take place only by conduction; and from Fourier's analytical theory of heat we know that the loss of heat would be extremely slow, and confined almost wholly to a shallow layer near the surface. Indeed it seems probable that the shrinkage of the entire globe is barely comparable to the secular contraction of the cooling crust alone. The approximate accuracy of this view is confirmed by the fact that the crust has not cracked open by pulling apart, as it would do if the crust shrank much more rapidly than the globe as a whole. The fact that the interior of the globe lost very little heat, while the crust cooled all the time, would lead one to think that so far from wrinkling by contraction, the crust ought to have cracked open by the shrinkage of the shell over a nearly unyielding nucleus; but no doubt the process was too slow and the rocks too plastic to give rise to actual rupture of the earth's crust. Moreover, if the globe shrank, it is inconceivable that this shrink- age could fail to be fairly uniform in the different equal areas of the surface, and thus we should expect the resulting wrinkles to be distributed over the globe with . moderate equality and uniformity. Instead of this, we find the mountains, heretofore assumed to be wrinkles, bunched into congested systems, and almost always paral- lel to the seashore, and larger in proportion to the depth of the adjacent ocean. Is it therefore at all credible that the mountains have really been formed by the shrinkage of the earth ? Would it be going too far to say that the whole theory of secular contraction as applied to our encrusted planet is a misconception dating from a time when currents were supposed to circulate freely throughout a liquid globe ? 19o6 .] SEE THE CAUSE OF EARTHQUAKES. 323 After a careful consideration of the whole question, including all the forces at work, one may well doubt whether the radius of the earth -has shrunk a mile since the continents began to emerge from the oceans. The crust could easily accommodate itself to such a small shrinkage as one part in 4,000, without producing any wrink- ling whatever. This subject of planetary wrinkles has been treated mathe- matically by Professor Sir G. H. Darwin, in his researches on the "Tides of a Viscous Spheroid" (Phil. Trans. Roy. Soc., Part n, 1879, P- 588)- And while his results are recognized to be correct, on the hypothesis, they seem to me to be inapplicable to the remote history of the earth, because I believe the shrinkage to have been nearly insensible, and certainly much less effective than has been gen- erally supposed. In his " Physics of the Earth's Crust," page 118, Rev. O. Fisher has discussed Darwin's theory thus : " It may be replied to this theory, that the formation of the existing continents cannot be looked at apart from their geological history, and that they are evidently dependent on, and as it were, gathered round, the great mountain ranges in which they culminate. Although these ranges primarily originated long ago in very early geological times, their present loftiness is due to quite late movements ; and, if these had not subsequently occurred, they would before now have probably have been razed to the sea-level and have disappeared, so that, whatever cause it was which wrinkled the conti- nents, seems to have continued active to times comparatively, if not quite, recent; and the moon is too far off now. The occurrence of great changes of level at no very distant geological period are manifest from such instances as that related by the elder Darwin." It has always been extremely difficult to show how contraction could produce elevation of ranges, and the mechanical explanations which have been put forward are admittedly unsatisfactory. 1 The spurs which so often jut out from the main ranges do not look like wrinkles in the crust ; for they are too numerous and terminate too suddenly at their extreme ends. The isolated parallel ranges so often met with in Nevada and Southern California also terminate too suddenly to be explained by shrinkage, or by lines of weakness. In his work on the " Physics of the Earth's Crust," second edition, the Rev. O. Fisher has discussed with much care the inade- 1 Fisher's " Physics of the Earth's Crust," second edition, p. 123. 324 SEE THE CAUSE OF EARTHQUAKES. | October 19,. quacy of the contraction theory to account for the elevations of mountains actually observed upon the earth. In the case of a solid globe, he finds (p. 122) that the average height of the elevations would be only six and one-third feet. By the theory of probability we easily see that this would absolutely prevent individual elevations, even when exceptionally favored by circumstances, from attaining any considerable height. In the appendix to the second edition, page 58, he examines the mean elevations which will result from the hypothesis of a liquid substratum, and finds that when the radial contraction is 12 miles, "the mean height of all the elevations, due to the corresponding corrugation of the matter above the level owing to secular cooling, is about 44 feet." " It appears," he adds, " there- fore as the result of the investigations in this chapter, that the hypothesis of a liquid substratum does not afford such an increased amount of compression as to render it possible to attribute the elevation of mountains to contraction through cooling in that case,, any more than in the case of solidity." When one recalls that our actual mountains are many hundreds' and even thousands of times higher than the mean elevations re- sulting from the contraction theory, it is readily seen how utterly devoid of foundation that theory really is. Considerations adduced in the writer's paper on the rigidity of the heavenly bodies show that the radial contraction of twelve miles used by the Rev. O. Fisher is probably at least twelve times too large; so that the highest ad- missible mean elevations due to shrinkage would be only a very few feet. It need scarcely be added that the Rev. O. Fisher must be given the chief credit for showing by long and patient research the inadequacy of this time-honored theory, which was originally suggested by Elie de Beaumont in 1829, and was no doubt a direct outgrowth of Laplace's nebular hypothesis. We thus seem compelled to abandon the contraction theory en- tirely, and to explain both peaks and ranges with their striking parallelism to the coast by upheavals occurring near the sea, due to the explosive power of steam, which has heaved up the mountains from beneath. The mountains apparently show this mode of forma- tion, and it explains with equal satisfaction cordilleras and ranges,. I 9 o6.j SEE THE CAUSE OF EARTHQUAKES. 325 whether of continued or isolated character, with their numerous jutting spurs and cross ranges, and isolated peaks, which are well- nigh unintelligible on any other hypothesis. And lastly it shows that all mountains are alike inside, whether they burst open and become volcanoes or remain intact. A theory presenting so many desirable points should have a strong claim to acceptance. In this connection one geological term in extensive use might perhaps be explained. We refer to the phrase Line of Weakness of the earth's crust, which was employed by Leopold von Buch to explain the arrangement of volcanoes along the seashore. It .forms wherever the sea stands some time, especially if the sea is deep, because the explosive paroxysms of steam work under the edge of the sea, but not under the land, and, therefore, " lateral thrusts " from the sea begin, while they cease on the land; the result is an injection of the coast line from the direction of the sea, and moun- tains and volcanoes are upraised, according to the intensity and especially the difference of these forces, from the sea and land, and their duration. It is not without significance that the height of the mountains are in general proportional to the depth of the adjacent sea, because the forces of injection depend upon the depth, and the elevations produced are proportional to the intensity of these forces. When the sea recedes, however, the extent of the land gained is propor- tional to the shallowness of the water, and hence arise the large flat plains in many countries. This explains the arrangement of moun- tains and volcanoes along the sea coast, which has, therefore, been called a line of weakness in the earth's crust. As a matter of fact, any line will prove to be weak where the sea stands for a long time, for mountains and volcanoes will be upheaved there. Thus I con- ceive that there is originally no such thing as a line of weakness in the crust, and we may with advantage dispense with that unfortu- nate term. This seems the more advisable, since the earth behaves as a solid, and local weakness developed in the formation of moun- tains has little effect at a distance, except in volcanic regions or ocean troughs, which act together sometimes throughout their whole extent. 326 SEE THE CAUSE OF EARTHQUAKES. [October 19, It is shown in the paper on the rigidity of the heavenly bodies that the strength of a planet like the earth is not appreciably de- pendent upon the crust, but arises primarily from the great pressure acting throughout the body, which itself in turn depends upon the mass and density of the globe. The earth's crust, therefore, has little importance in the theory of the eartji, except in our treatment of surface phenomena. 20. Is there a creeping movement of the fluid substratum be- neath the crust? The existence of such a powerful seismic zone around the Pacific Ocean, which is surrounded by unfinished mountains and a * fire girdle of volcanoes ' leads one to inquire whether there may not be throughout this vast ocean, as well as in smaller seas, a tendency for the explosive stresses to find relief at the margins, by a slow creeping movement of the particles of the substratum towards the periphery, where the chief relief is afforded. For those stresses arising under the crust in the middle of such an ocean, some relief would be afforded by the rising and sink- ing of certain oceanic islands ; but a greater relief would be afforded around the periphery of the sea, where the great moun- tain chains are in process of formation. As the crust under the sea is incessantly strained by the heaving of subterranean forces, some parts rising and others sinking, a slow creeping movement of the fluid substratum towards the periphery seems not only possible, but perhaps probable. Such a final movement would be the result of the countless earthquakes which disturb the sea bottom, and in any given earthquake the motion would be extremely slight. The creeping fluid would tend towards the avenues of escape in islands and on the margins of the sea, as well as towards areas still sub- merged but rising; and thus we recognize forces which under cer- tain conditions may both elevate and depress islands in the sea ; but in the long run the sinking tendency will predominate where there is water, and the rising tendency where there is land. All along the west coast of South America Charles Darwin found conspicuous evidence of elevation within recent geological times ; and at Valparaiso the amount was no less than 1 ,300 feet. The periodic subsidences indicated in certain places by beds of ma- i9o6.] SEE THE CAUSE OF EARTHQUAKES. 327 rine fossils of past geological ages, could, I think, be explained by tendencies developed under the crust, according to which the fluid substratum is alternately thickened and thinned, owing to the con- currence or non-concurrence of the subterranean forces. When they work towards a point the result is elevation, and when they tend to diverge from a point the result is depression, and the elevation is transferred to neighboring areas. This is a modern view of the periodic movement of the earth's crust so clearly foreseen by Strabo nearly 2,000 years ago. According to this view the sea bottoms may oscillate, but on the whole tend to subside, not on account of the shrinkage of the globe, but by virtue of the gradual working out of the underlying fluid substratum, which in the long run pushes up the land. In his " Principles of Geology," I2th edition, Vol. II, page 155, Lyell discusses with characteristic fairness the historical cases of elevation of coasts noticed in different parts of the world. We shall content ourselves with citing a very few cases of this type :. 1. Islands in the sea innumerable, both volcanic and non-volcanic (apparently, though all are raised by volcanic forces). 2. The southwestern end of the Island of Crete, which even Professor Suess admits to have experienced undeniable secular elevation within the historical period. 3. The region about Pozzuoli and the Bay of Naples. This is shown by the famous temple of Jupiter Serapis, and by the eleva- tion of the coast actually witnessed at the time of the eruption of Monte Nuovo in 1538. This raising of the land was confirmed on a larger scale for the whole Bay of Naples during the Vesuvian eruption of April, 1906 (cf. Quarterly Journal of the Geological Society, No. 247, 1906), by Professor Lorenzo, who found the ele- vation of the land at Pozzuoli to be six inches, and at Portici one foot. 4. The foundations of both ^Etna and Vesuvius were laid in the sea. 5. Professor Suess cites the most ample evidence of raised beaches and other sea marks high above the present strand in almost all parts of the world. As these heights are very unequal, they can- not be explained by a simple sinking of the sea level, but there must PROC. AMER. PHIL. SOC., XLV. 184 U, PRINTED FEBRUARY 2O, 1907. 328 SEE THE CAUSE OF EARTHQUAKES. [October 19, have been undeniable oscillations of the land, similar to, but on a larger scale, than those observed during the historical period. 6. Conclusive proofs of the upheavals of the Chilian coast during the earthquakes of 1822, 1835, etc., have been given by Lyell, and will not be repeated here. We content ourselves, therefore, with the following account of the Valparaiso earthquake of August 16, 1906, which speaks for itself: THE GREAT EARTHQUAKE AT VALPARAISO, AUGUST 16, 1906. A special copyrighted cablegram to the San Francisco Examiner of August 23, dated Valparaiso, Chili, August 22, says : " The recent seismic disturbances in this region have thrown up several new islands in Valparaiso Bay. These islands are of various dimensions, some being very extensive while others appear to be mere cone-like rocks jutting above the waters. It is reported that islands have appeared at dif- ferent points along the coast of Chili. . . . " The wrenching given the earth's surface is still showing more and more day by day. In sections of the harbor and on the coast, the shore line has been materially changed. Promontories have slid bodily into the sea and in other places strips of coast line have been completely submerged. The theory is that there has been a great uplift of the Andes so as to change almost entirely the contour of the hilly region of the republic. Landslides are everywhere in evidence. Mountain sides have been stripped away and chasms in the hills filled up. " Persons who have arrived here on horseback from points along the coast say that they witnessed nothing but devastation. Whole villages were wiped out." * 1 Since this paper was finished, Professor H. D. Curtis, in charge of the D. O. Mills Expedition of the Lick Observatory, at Santiago, Chili, has written an interesting letter to Professor Kroeck of the Pacific University at San Jose, which is published in the San Francisco Argonaut of November 3. Professor Curtis says: " A Commission has been appointed to study the shock and its causes. I published a statement that the primary cause was doubtless the same as at San Francisco, the slipping or sliding of one stratum past another, due to the well-known geological fact that the Coast of Chili is very slowly rising. I learn since that the Bay of Valparaiso is now ten feet shallower. So I think the displacement in this shock will prove to be mainly vertical. It may be that the centre of disturbance was under the sea, as Valparaiso suf- fered much more than Santiago." Professor George Davidson, President of the Seismological Society of America, informs me that during the great earthquake at Yakutat Bay, near Mt. St. Elias, Alaska, September 3-20, 1899, the land at the head of Yakutat Bay was raised 47% feet. In the Bulletin of the Geological Society of America, vol. 17, May, 1906, will be found a careful investigation by Tarr I9o6 .] SEE THE CAUSE OF EARTHQUAKES. 329 21. Avicenna's views on mountain formation. Lyell .justly remarks that it is surprising to find among the extant fragments of Avicenna, Arabian physician and astronomer of the tenth century, a treatise on the " Formation and Classification of Minerals," characterized by considerable merit, the second chap- ter of which is " On the Cause of Mountains." Mountains, accord- ing to Avicenna, are formed, some by essential, others by accidental causes. And in illustration of the essential causes, he cites " a violent earthquake, by which land is elevated, and becomes a moun- tain." In regard to the accidental causes he mentions excavation by water or erosion, which produces cavities, such that adjoining land is made to stand out and form eminences. The theory of mountain formation adopted in this paper was therefore foreshadowed by Avicenna in the tenth century of our era. It is extremely remarkable that so simple an explanation should have been allowed to slumber for so many centuries, while artificial and highly unsatisfactory hypotheses were in use. V. EXPLANATION OF THE ELEVATION OF PARTICULAR MOUNTAIN RANGES AND PLATEAUS. 22. On the uplifting of the Andes. We have already seen that the Andes have been uplifted by the injection of lava beneath the crust in the earthquakes incident to the heaving of the Andean Valley in the adjacent sea. This has been the chief cause of the original uplift of these great mountains, and the resulting explanation suffices to account for all the principal phenomena. Thus we explain the gentle slope of the mountains and Martin, who show that the coast was elevated for more than a hundred miles, though slight depressions also occurred in a few places. Elevations of 7 to 20 feet were common, and so little change had occurred in 1905 that Tarr and Martin were able to illustrate their memoir by photographs of the most convincing character. The barnacles and other marine animals were still adhering to the rocks, and there could be no possible doubt about the fact of the elevation. The depression of some areas was made equally clear by the encroachment of the salt water upon forests, which were thus killed. Two of the shocks at this great earthquake (September 10-15) were particularly terrible, the motions recorded in Tokio, 3,300 miles away, being ^ and y% inch respectively. Note added December 3, 1906. 330 SEE THE CAUSE OF EARTHQUAKES. [October^, on the west and the extreme steepness of the descent on the east; 1 and we also account for the more numerous jutting spurs on the west. On the whole side spurs are much less conspicuous on the east, where descent is more rapid. These characteristics are prob- ably the leading features of the Andes, but there are others deserv- ing of attention, among which we may mention the following : 1. Very great volcanic violence throughout the whole range, and in the peaks of the eastern as well as of the western cordillera. 2. Enormous vertical uplifts, or fault movements, often amount- ing to thousands of feet, occurring throughout the cordillera, but be- coming especially predominant on the eastern side. 3. The vertical uplifting of enormous plateaus such as those of Quito, Caxamarca, Cuzco and Titicaca, the latter being 12,500 feet above the sea. The heaving of the Andean Valley in the sea seems to be the principal cause of the original elevation of the mountains, but it appears probable that after the mountains were raised to great height another secondary cause contributed to the forces operative in producing the present enormous elevation. This secondary force was nothing else than the soaking tropical rains constantly drench- ing the eastern slope of the mountains. As the earth's crust was already broken and faulted, the leakage of the water downward would be facilitated, while the ceaseless character of the rainfall would make the eastern slope of the Andes to all essential purposes an inland sea. Effectively, therefore, this great range of mountains is built upon a narrow strip of land with seas on both sides like the mountains in Central America, and hence, the violence of th*e vol- canoes and earthquakes becomes more easily intelligible. To make this theory more specific we may recall that all the principal peaks about Quito have been volcanic, and three or four volcanoes are still terribly active there now. Just east of Quito, at the head of the Amazon Valley, are the most terrible rainfalls on 1 Professor Solon I. Bailey, of Harvard Observatory, who crossed the Andes twice, once near Sorata, Bolivia, and again at the Aricoma Pass, and traversed the eastern ran