\\E UN!VER% * 3 5 S 3 OF-CAU \\E-UNIVER clOS-ANCElfT I S % ,55*' I i^ 1 ,OF-CAllf 5 6 .1 S i I x DESCRIPTION O F A GLASS APPARATUS, FOR MAKING MINERAL WATERS, LIKE THOSE opPYRMONT, SPA, SELTZER,&c, In a few Minutes, and with a very little Expence : TOGETHER WITH THE DESCRIPTION OF SOME NEW EUDIOMETERS, O R INSTRUMENTS forafcertainingtheWnoLSOMENEss of RESPIRABLE AIR; AND THE METHOD OF USING THESE INSTRUMENTS : IN A LETTER TO THE REV. DR. PRIESTLEY, LL.D. F.R.F; BY J. H. DE MAGELLAN, F. R. S. LONDON: PRINTED FOR W. PARKER, No. 69, FLEET-STREET, AND SOLD BY J. JOHNSON, No. ~2, ST. PAUL'S CHURCH-YARD, AND W. BROWN, THE CORNER OF 3^SSiX-STRT, IN THE SI RAND. MDCCLXXVII. Annex 5 oft ADVERTISEMENT OF THE E I> I T O R, RELATING TO THE USE OF THE SIM-- PLE GLASS MACHINES FOR MAKING MINERAL W A T E R S. A LTHOUGH the method of ufing jf~\. the fimple glafs machines of Mr. Parker, is minutely defcribed in the fol- lowing Letter, neverthelefs it may be more agreeable to find here diftincT: refer- ences to thofe articles, where it is parti- cularly contained ; as the Author feem- ingly could not help blending it with that- of his improved machines.- I. The defcription of the fimple Par- ker's machine is comprifed No. 5 and 6. II. The procefs to make ufe of the fame, is defcribed No. 9, 10 and 1 1. III. The manner of carrying on the production of fixed air^ is indicated No,. 14 and note ( and rife or lower the tube of the Eudiometer, fo as to fee the furface of the water, in the infide, even with that in the outfide ; which I mark by Hiding to it the brafs ring z. therwife I apply the ruler (fig. n, without making any ufe now of the brafs ring) to the fide of the Eudiometer, whilfl it is immerfed in the water of the trough : and there I fee the true di- inenfion of the remaining bulk of the two kinds of air, already diminimed. Perhaps the beft method for this obfervation would be to allow time enough that the mixed air may take its fettled bulk : but this requires fometimes twenty-four hours time. I leave, however, the choice of thefe two methods to the obferv- ing made a very great number of them with nice Eudio- meters, of the kind I am now defcribing. It certainly deferves the attention of Philofophers : and, although I have communicated it to fome of my acquaintance, none have as yet, in my humble opinion, given a fatisfa&ory fblution of this phenomenon. cr, ( 30 ) pr, who may ufe both if he pleafes, provided he keeps diftinctly the refult of each method in his account of the experiment. 30. The number marked about the middle of this ruler (fig. 1 i,) as for inftance, # #-96, means that the contents of both phials a and If are equal to ninety-fix divifions of the ruler, when put into the tube of that Eudiometer : that is to fay, they are equal to a folid cylin- der, as thick as thp infide of the glafs tube, and whofe length is ninety-fix divifions of the ruler, which has been divided into tenths of an Englilh inch,. 31. Now if, for inftance, this remaining bulk of mixed air correfponds to the 56th di- Tifion of the ruler, it (hews that, out of 9$ parts, only 40 (=96 56) have been loft or contracted : and, in this cale, the wholfome- nefs of that air, which I call A, will be . If another equal quantity of different air, which I mail call B 9 had alfo been tried by the fame Eudiometer, and its refiduum was equal to. <>o parts of the fame ruler, the refpective falubrity of the air B will then be to that of the air A* as 36 (-9660) to 40. 32. But if the air B had been tried by ano- ther Eudiometer, whofc proportional dimenfi- Oris, marked about the middle of its ruler^ were # * = 108, then the refpedive falu- brity of thefe two kinds of air A and J5, would be in the compound ratio of -^ to i| 56x06 to 4ox 108 " to 432 = 54 to 67, 5 : that is to fay, the wholfomenefs of the air B would be to that of the air A 9 as 54 to 33. Nearly the fame refults would be found, if the ruler (fig. 1 1,) was applied to the fide of the (I) It is fuppofed that the infide of the tube is of an uni- form diameter ; but it often happens, that there are fomc varieties in different parts of its whole length. When they are not very confiderable, we may neglect their influence in the refult of thefe Eudiometrical experiments ; but when the contrary happens, it will be very eafy to make a proper allowance for them in the calculation. It is for this reafon that I have always ordered that the contents of one fingle phial be marked alfo upon the fcale of each Eudiometer, as well as the contents of both phials ; for inftance as in. this manner: * # = 96 * =47 which means, firft, that the contents of both phials 6 and b are equal to a cylinder, whofe diameter is the fame as that of the infide bore of the tube d (fig. 16,) and whofe height is equal to 96 equal divifions of the ruler : fecondly, that the contents of a fingle phial are equal to 47 divifions in the upper part of the fame tube mud; and of the Eudiometer, as foon as the incbfed mix- ture of air came to its utmoft diminution, ai mentioned No. 28 : becaufe as much water muft fall in the tube n d^ as correfponds td the diminution fuffered by the two mixed airg in x. But there are fome varieties, which arife from the different prefTure of the column of water, which prefies more or lefs upon the air .at x (fig. 14,) as it is longer or fhorter : and thefe varieties ought not to -be overlooked iri nice experiments : they are avoided by the procefs already defcribed, No. 29 ; and majr otherwife be prevented by the method of which I will fpeak at the end of No. 39. 34. Whenever I have at hand a tall glafs receiver, like that reprefented fig. 14, the whole procefs is then more eafily performed ': for in this cafe I dip the Eudiometer, inverted as it appears fig. 12, into the water contained in the veflel V S q I : I then put the two kinds of air into the phials a and b as above faid, No. 26 and 27 : I turn the inftrument upright, as reprefented fig. 1 4. -, and finifh the procefs, as I have already defcribed. of courfe, to 49 divifions (=196 47) of its lower part. By this difference it appears that the tube of fuch Eudio- ineter is wider in the top than at the bottom, by & of the tthole. 35- t ( 33 ) 35- I mu ft> however, warn the operator that, unlefs every trial, and even almofl every part of the procefs, be made in the fame tempe- rature ; or, at leafl, unlefs the varieties arif- ing from this caufe be accounted for no re- liance can be had on the refult of fuch expe- riments : it being well known, that air is apt to increafe or diminifh very considerably in its bulk, by the influence of heat and cold. It is for this reafon that I conftantly keep a good thermometer K, which hangs by the wire y r, and is immerfed in the water of the glafs vefiel fig. 14, or in the trough fig. 17, whenever I make- .any of thefe experiments. For the fame reafon I take care to leave the Eudiometer and the veflcls of ai r , immerfed in water time enough, as above mentioned, to get the fame temperature : and I make ufe of the wooden tongs mentioned in note (), whenever I handle the phials c b filled with air, chiefly if they have not the folid lump at their bottoms, as reprefented in the plate ; unlefs I feel the heat of my hands to be the fame as that of the water, in the trough, I make ufe of. DESCRIPTION OF THE SECOND NEW EUDIOMETER. 36. The Eudiometer, reprefented fig. 15, confifts of a glafs tube / r, two or three feet F long. ( 34 ). long, and of an uniform diameter : the end c is bent forwards ; and the other end / is wide open, as a funnel, unlefs a feparate one is made ufe of : this tube is faftetied, by two loops, to the brafs fcale c w t V. There is a glafs phial , the neck y of which Is ground air-tight to the end / of the tube ; and contains only half of the whole infide capacity of the divided tube c t. It has, at the other end c, a large round phial a b c, containing three or four times the bulk of the phial n : its neck is alfo ground air-tight to the mouth c of the tube. The brafs fcale c w t Fis divided into 128 equal parts: this being a number that can be divided to unity in a fubduplicate ratio without fraction, by continual bilections -, on which account it is one of the numbers the late famous Mr. Bird had adopted for his di- viding mathematical inftruments with the ut- moft accuracy. Thefe numbers are fet out in the fcale from / towards c. The contents or capacity of the tube till the number 128 is the double of the capacity of the phial n. Befides this there is a tin veflel x s d t r o (fig. 15*}, which may ferve as a packing cafe for the whole inilrument, and its necefiary appen- dages ; and alfo as a trough, when experi- ments are made ; it being then filled with wa- ter. Both the glafs tube reprefented fig. 22, and the glafs floppier (fig, 15*), belong to this ( 35 ) jkis Eudiometer ; and both are fitted in, air- tight, to its mouth V. THE PROCESS. 37. Let the .inftrument be immerfed under the water zz of the tin veflel fig. 15*: and let the phial , filled with water, be put in the infide focket e e d of the tin veflel. Let it be filled with nitrous air, as above directed at the end of No. 27 : and let this quantity of air be thrown into the phial a b c (as directed No. 26 and No. 27), which I fix a little tight to the mouth c of the Eudiometer. I afterwards fill the fame phial n with the air I want to try : and, raifing the end c of the inftrument, I put it into its mouth V : when this is done, I fet the inftru- ment upright, as reprefented fig. 15, hanging it on the hook w ; and, as foon as this laft air goes up to the phial a b c , I take off the phial n, that the diminution of the two mixed airs may be fupplied from the water in the tin veffel ; which muft be the cafe, as the mouth ^"of the Eudiometer is then under the furface of the water. 38. I then put to the lower end V of the Eu- diometer, the bent tube ftg. 22, to which is fitted the brafs ring K, and is filled with F 2 WW water. It is by obferving the furface of the wa- ter in this fmall tube (which then forms a true fiphon with the tube of the inftrumer.t) and by means of the brafs ring X, that I can dif- tinguilh the ftationary date of the diminifhing bulk of the two mixed airs, above mentioned at the end of No-. 28 : which being perceived, I take off the fmall tube g h from the Eudio- meter, and lay down, for fome minutes, the whole inftrument, in an horizontal pofition, under the water of the tin veflel : I mut up the mouth V with the glafe ftopple m , and, reverfing the inftrument, I hang it up by the end V* on the hook w. By this pofition the whole diminiffced air of the veflel a b c goe$ up to the top, where its real bulk is fhewn by the number of the fcale, facing the infide fur- face of water. This number being deducted from 128, gives the comparative wholfome- nefs of the. air already tried, without any fur- ther calculation. 39. Biitthis procefs will be ftill eafier, when the laft 'diminution of the two mixed kinds of air, mentioned No. 29, is only required in the obfervation : becaufe no ufe will be then made of the fyphon, (fig. 22). In fuch a cafe the in- ftrument is left hanging, on the hook wfor 48 hours: after which it is laid down under the water of the trough (fig. 15*), in an horizon- tal ( 37 ) / tal pofition, for 8 or 12 minutes, in order to acquire the fame temperature of the water : the mouth F"is then fhut up with the ftopple m; the inftrument is hung by the end V in a con- trary pofition, and the Jail real bulk of the good mixed air will be then fhown by the number of the brafs fcale anfwering; to the in fide fur- face of the water. This number being fub- tracted from 128, will give the comparative fa- lubrity of the air employed in the trial, without any further calculation. I need not fay that all the circumftances already mentioned for the bet- ter obtaining exact refulcs in thefe experiments, are to be carefully obferved, when this fecond, or the third Eudiometers areufed: but chiefly that circumftance, mentioned No. 35, ought never to be omitted. The thermometer is to be kept dipped in the water of the tin vefiel ; and the Eudiometer mult be kept there im~ merfed fome minutes, as I have faid juft now, before it is railed for the laft time, to read off the quantity of the total diminution of the mix- ed air. As to the other circumftance, menti- oned No. 33, it has been rendered unneceflary by laying this Eudiometer in an horizontal pofition before the glafs ftopple was put in. The fame method muft be applied to the third new Eudiometer I am going to defcribe ; and even the firft Eudiometer, already defcribed, may be treated in the fame manner : for if it be laid ( 38 ) laid down in an horizontal pofition under the water in the tub, before it be (hut up with the ftopple, as directed No. 29, there) will be no variation produced by the expanfion of the air in the infide : becaufe the proper quantity of water is then fhut up within the glafs veffd c of the inftrument: fo that raifing it up, as it is, together with the veflel c, and its phials a I (fig. 1 4), the weight of the column of water will prefs totally upon them, without expanding the in- clofed air, or caufing any variation beyond the trifling one which may proceed from the natu- ral elafticity of the fides of the glafs tube and veflels. 40. I muft, however, acknowledge that, the long way through which the air pafTes, in going at firft to the large phial a b c in this fecond Eudiometer, muft leave fome doubt whether it has not then fuffered fome fenfible change in its quality, before it is mixed with the ni- trous air ; fince, as you have obferved, the air that has been long agitated in water, changes for the better from its bad qualities : and this objection muft be ftill greater in the ufe of the third Eudiometer. It is on this account that I have mentioned the firft Eudiometer, as the leaft exceptionable of all that we know till the prefent ; and perhaps the nature of the thing is not capable of a further perfection. Indeed 39 ) Indeed that inftrument, I mean my firft Eu- diometer, has not only the advantage of offer- ing a very fmall way through the water to the two kinds of air, on their going to mix at x in theveffcl c (fig. 14), but they are kept fepa- rated till that moment, in the two refpective phials a and , without any other contact with the water, but only in the narrow diameter of the necks of thefe phials. DESCRIPTION OF THE THIRD NEW EUDIOMETER. 41. This third Eudiometer is the neareft to your original one: and, was it not for the con- fideration I have mentioned in the preceding number (which, perhaps, will not weigh too much with fome philofophers) and few other circumflances which are obvious, I mould not doubt to pronounce this third inftrument to be the beft of all the three, as I have advanced in my laft letter to you of the 3Oth of November laft. This, however, I gladly fubmit to your fuperior judgment. 42. This third Eudiometer confifts- of a ftrait glafs tube e n (fig. 8), of an uniform diar meter, about two or three feet long, with a large ball j, and a glafs ftopple m, fitted air-tight to the ( 40 ) the mouth #, which ought to be wide open, as a funnel, unlefs a feparate one is made ufe of. There is alfo a fmall fiphon (fig. 23) with a brafs ring x: a fmall phial z (fig. 9), the contents of which may be received in the third part of the ball s : and, when put into the glafs tube n j, muft take there no more than the half of its length. ' Laftly, this in- liniment has a ruler (-fig. 13), which is divided and ftamped like that other already defcribed at the end of No. 24 ; and a glafs funnel, which is ground to the mouth n of the inftrument, when this is not wide t>pcn, as already faid. THE PROCESS. 43. The ufe of this inftrument is eafily un* derftood by what I have already faid of the tw* preceding ones. Firft, it is filled with water, and fet in a vertical pofition, with the mouth n under the furface of the water in a tub, or in a trough, Secondly, the phial 2 (fig. 9) is filled, as above, with nitrous air- 9 and thrown into the tube by means of the glafs funnel y (fig. 10), larhich is ground to the mouth of the Eudio- g meter, meter ; unlefs it be wide enough not to be in need of any funnel. Thirdly, the fame phial z is again filled With the air to be tried ; and thrown into the fame. Fourthly, .the fiphon (fig. 23) is added im- mediately to the mouth n of the Eudiometer, under the furface of the water ; fome of which is to be poured into it. Fifthly, the ftationary moment of the great- eft diminution of the mixed air at j,. is watched by means of the ring x, as mentioned No. 28 and 38. Sixthly, when that moment arrives, the fi- phon K I (fig. 23) is taken off; the Eudiome- ter is laid for fome minutes under the water, in an horizontal pofition, or nearly fo, but in fuch a manner that no part of the inclofed air may get out ; the rnouth n is mut up with the glafs ftopple , and theinftrument is inverted with the mouth n Upwards. Laflly, the fpace occupied by the refiduum.- of the diminimed air, is meafured by applying to its fide the divided ruler, or fcale (fig. 13), and the refuk is efnmated after the manner al- ready explained No. 31 and 32. G 44> ( 42 ) 44- Whenever I want only to know the laft diminution of the mixed air, mentioned No. 39, the procefs then becomes eafier, as no ufe is made of the fiphon (fig. 23). The method of conducting the procefs in fuch a cafe be- ing refpectively the fame as that already de- fcribed No. 39, it isunneceflary to defcribe it here again. The fame precautions I have fpo- ken of. No. 35 and 39, muft be obferved when this Eudiometer is made ufe of, in order to form a true judgment concerning thofe places, where people will be able to live without danger of hurting their conilitutions, by breathing and being continually 'furrounded by noxious air; which they have not yet been able to diftin- guilh from the moft wholfome, except by a long and too late experience. 45. The Eudiometers already defcribed are the fiteft inftruments for philofophical experi- ments, on the bulk of air and other fluids, when mixed together ; and even when mixed vith fome folid fubftances, which can be in- troduced into the lower veflel c of the firit of the three Eudiometers. It will be better, however, to have them made purpofely for fuch obje&s, with a tube two or three times longer than I have indicated above. When- ever dephlogifticated air is to be tried by thefe inftruments, proper care is to be taken to ob- ferve the precife point of its full faturation, 3 which ( 43 ) which is that of its greateft diminution by the addition of nitrous air. 46. In order to make this experiment with great accuracy, let a narrow glafs tube of an uniform diameter (fig. 24), be provided : let one of the two phials a or b (fig. 1 6) filled with qnickfilver, be thrown into it, and the tube cut exactly to thatfize, fo as to contain neither more nor lefs. Let its whole length be divided into fome number of equal parts, by which num- ber the value marked on the ruler (fig. u), of this Eudiometer, can be divided without any fraction : for inftance, the number % % ~ 108, marked in the ruler, means, that the contents of the two phials a and , of which I fpoke No. 32, are equal to a cylinder of 1 08 divifions long, as thofe of the ruler : and, of courfe, it mews that a fingle phial a or b contains but 54 of thefe parts. Jn this cafe this tube (fig. 24) may be divided either into 27 parts, each containing two of the ruler -, or into 54, into 108, &c. N. B. If the top of the tube is not very flat in the infide, it will be more exact to divide the weight of the quickfilver in two parts ; to put one of them into the tube ; to mark the fpace occupied by it ; to divide the pare pf it, which was empty, into half th? number G z i- ( 44 ) intended for this tube, and afterwards to di- vide the other half into fimilar equal parrs, as the firft half, carrying them towards the clofed end. 47. If the dephlogifticated air is very pure, it will require almoft double the quantity of nitrous air to be completely faturatcd. In orr der to do this without exceeding the neceflary quantity, I throw into the tube nd fig. 17) a fecond meafure b or a of nitrous rf/r, after I have brought the procefs to the moment men- tioned No. 29 : in this cafe the whole volume or bulk of the dephlogifticated and nitrous air will be 162 [=108 + 54:] I obferve where the furface of the infide water in the tube ftops, and I mark it by .the fliding brafs ring z. I then fill up the divided tube (fig. 24) with nitrous air : I throw a fmall quantity into the Eudiometer tube n d ; and, if it becomes of a redifh colour, the inclofed air will diminifh : I then pum up the ring z, and, by this means, I go on throwing in the nitrous air, by little and little, till I fee that the whole diminimes no more ; which mews me that it is fully fa- turated. 48. Let us fuppofe, for example, that the tube (fig. 24 ) was divided only into 27 equal parts i and that the faturation of the dephlo- gifticated ( 45 ) gifticated air was compleated at the eighth di- vifion of it : this fhews that 19 parts [27 8 19], equal to 38 of thofe marked in the ru- ler,- have been thrown into the Eudiometer ; that is to fay, that the whole bulk of both kinds of air is equal to 200 [ 162 + 38] meafures, as thofe marked by the ruler (rig. ii,) already explained No. 30. Now if the remaining quantity of air within the Eudio- metrical tube is only equal to two meafures or numbers of the ruler, it is clear that fuch de- phlogifticated air is ninety-nine times of an hundred rlHi = ii 8 = 39-1 pure air; L 200 200 IOO J fince its bulk is reduced, by the combination of nitrous air, to the -^-^ of the whole. 49. It is but three days ago (/) that you (hewed me fuch a wonderful kind of air, as I have exemplified in the preceding number. This air you have produced before my eyes, from a folution of quickfiher and nitrous acid 9 (/) This additional article to the prefent letter was wrote on the i6th of September, 1777; although the greateft part of it has been written many months before, and the firft twenty numbers were already printed : but fome cir- cumftances, the knowledge of which cannot intereft the public, have hindered the publication of the whole tilfe this prefent time. made ( 46 ) made many months before, and then diftilled in a long but narrow glafs retort, with a fand- heat. This is, perhaps, inleed, an extraor- dinary phenomenon, and feems to bring us a little nearer to the door of the fecret laboratory of Nature in the formation of air. 50. I cannot fay, but fo pure a dephlogijlica- ted air may flill be produced by this procefs ; that its whole bulk may be reduced to nothing by a proper combination with nitrous air. If fo, what fhali we then be able to think of a fluid fubftance, which is coercible in a glafs veflel, to which above the double quantity of another fubftance [VV 6 2 >7] likewife coerci- ble in a glafs veffel, being added j both thefe fubftances to appearance wholly vanifh 1 I JO" 7 ?' 51. This phenomenon certainly deferves the attention of philofophers : and I gladly leave to them the examination of it. I muft only add, for their information, that the nitrous acid is the thing chiefly concerned in its pro- duction : when this admirable fubftance acts on certain kinds of bodies, as quickfiher in the prefent cafe, its folution produces that elaftic^ but coercible fluid, which we call nitrous air : the refiduum, after a long while, being pro- perly urged by fire, gives at laft the other ici but likewife coercible fluid, which we call ( 47 . ) call depllogifticated air 5 and the combination of both, nearly in the above proportion, pro- duces the wonderful phenomenon I have fpo- ken of. 52. I mall fay no more on this matter; and leave it very willingly to be confidered and un- ravelled by abler philofophers than I can pre- tend to be : and conclude the fubject of this letter by alluring you, that I mall be very happy, if the things here treated of mould deferve your approbation : and ilill more fo, if they produce the defired effect I aim at, the general good of mankind. I am, with the utmoft regard and fmcere friendfhip, My dear Sir, Your moft obedient and Affectionate fervant, Bowood Park, j R ^ MAGELLAN. Januarys, 1777. - r Tf. ft* ^^^L & J3 =? % I/ I a 10S-ANGEI& -UBRARY I I 8 S s g I 1 f ^ > I I .^lOS ANGELA ^ t>^-^^ <-S ^- I I It -n V f fc ^ g I 1 ^W IW3-JO^ ^avuan-^ 3 wnw 4>mmw ^fliwsov I I ^1 \ .% ft 3' 1 1 I 1 vsov