REPORT OF COMMITTEE ON ATOMIC WEIGHTS, PUBLISHED

REPORT OF COMMITTEE ON ATOMIC WEIGHTS. 201. Specific. Gravity at. Specific. Gravity at. •. Percent-. Percent-. -c. -IU c. -Sic. age by ilc. - -c. Ac...
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REPORT O F COMMITTEE ON ATOMIC WEIGHTS.

-

SPECIFIC GRAVITYAT

__ 4' c. 4 O

0.8923 0.8946 039% 0.8992 0.9014 0.9037

;: c.

201

SPECIFIC GRAVITYAT

::

Percent.

25' c.

-c.

25O

0.8836 0.8756 0.8858 0.8779 0.8881 0.8803 0.8826 0.8904 0.8927 0.8850 0.895U 0.8874 0.8897 0.w 0.8973 0.9083 0.8996 0.8921 0.9106 0.9019 0.8944 0.9129 0.9041 0.8968 0.9151 0.944 0.8991 0.9174 0.9087 0.9015 IO 0.9197 0.91 0.9038 0.9220 0,9133 0.9062 0.9243 0.9156 0.9~86 0.9266 0.9179 0.9109 0.9289 0.9202 0.9133 0.931I 0.9224 0.9156 0.9334 0.9247 0.9180 0.9354 0.9268 0.9202 0.9373 0.9289 0.9223 0.9392 0.9309 0.9245 0.941I 0.9330 0.9267 0.9431 0.935' 0.9288 0.9450 0.937' 0.9310

68 67 66 65 64 63 62 61 60

59 58 57 56 55 54 53 52 51

50

49 48 47 46 45 44

0.9469 0.94% 0.9508 0.9527 0.9541 0.9554 0.9567 0.9580 0.9594 0.9607 0.9620 0.9634 0.9647 0.9660 0.9674 0.9687 0.9700 0.97=4 0.9727 0.9740 0.9754 0.9767 0.9780 0.9794

0.9392 0.9412 0.9433 0.9454 0.94% 0.9484 0.9499 0.9514 0.9529 0.9544 0.9559 0.9574 0.9589 0.9604 0.9619 0.9635 0.9650 0.9665 0.9680 0.9795 0.9710 0.9725 0.9740 0.9755

25' ,.( 2.5'

0.9332 0.9353 0.9375 0.9397 0.9413 0.9430 0.9446 0.9462 0.9479 0.9495 0.9j12 0.9528 0.9545 0.9561 0.9578 0.9594 0.9611 0.9627 0.9644 0.9660 0.9677 0.9693 0.9709 0.9726

Percentag: b y weight.

43 42

41 40 39 38 37 36 35 34 33 32 31

30 29

28 27 26 25 24 23

22 21 20

REPORT OF COllMlTTEE ON ATOlllC WEIGHTS, PUBLISHED DURING 1894.' BY F. W. CLARKE. Received January I, 1895.

To fhe Members of fhe American Chemical Son'ety: OUR committee upon atomic weights respectfully submits the following report, which suniinarizes the work done in this department of chemistry during 1894. Although the volume of completed determinations is not large, it is known that several important iiivestigations are in progress, from which valuable results may be expected in the near future. I t is in this cbuntry that the greatest activity exists, and that the greatest progress is being made at present; and the preparation of these reports is therefore a peculiarly appropriate function of the Society. T h e data for 1894 are as follows: The N:0 rafio.-An interesting atteinpt a t the indirect measurement of this ratio, which is the base line upon which our sys-

Y

'Read at the Boston Meeting, D e c e m b e r 28, 1%.

F . W. CLARKE.

202

R E P O R T OF COMMITTEE

tein of atomic weights depends, has been niade by Julius Thonisen.' His deterniiiiatioiis are really determinations of the ratio N H , : HCl, and were conducted thus : First, pure, dry, gaseous hydrochloric acid was passed into a weighed absorption apparatus containing pure distilled water. After noting the increase in weight, gaseous amtnotiia was passed through to slight excess, and the apparatus was weighed again. T h e excess of ammonia was then measured by titration with standard hydrochloric acid. I n weighing, the apparatus was tared by another as nearly like it as possible, containing the same amount of water. Three sets of weighings were made, with apparatus of different size, and these Thomsen considers separately, giving the greatest weight to the experiments involving the largest masses of material.

T h e data are as follows, with the ratio

in the third

column : FIRSTSERIES. Wt. HCI.

5.1624 3.9425 4.6544 3.9840 5.3295 4.2517 4.8287 6.4377 4.1804 5.0363 4.6408

Wt. NH,.

Ratio

2.4120 1.8409 2.1739 I A609 2.4898 I .9863

2.1405

2.2550

2.1414

3.0068 1.9528 2.3523 2.1685

2.1403 2.1416 2.1411 2.1409

2.1406

2.1411

2.1407 2.1410

2.141 I

SECOSD SERIES. Wt. HC1.

11.8418 14.3018

Wt.NH,.

5.5302

12.1502

6.6808 5.6759

'7.5443

5.3927

I 2.3617

5.7733

Ratio.

2.14130

THIRDSERIES. W t HCI.

'9.3455 19.4578 1IZtschv. phys. Chem., 13, 399.

Wt. NH,.

9.0360 9.0890

Ratio.

2.14094 2.14081

OX

ATOMIC WEIGHTS, PUBLISHED DURIXG 1894.

203

Froin the sums of the weights Thomsen finds the ratio to be 2.14087, or 2.13934 invacuo. From this, using Ostwald’s reduction of Stas’ data for the atomic weights of nitrogen and chlorine, he gets the ratio 0 : H : : 16 : 0.99946, or almost exactly 16 : I . In a later paper’ Thomsen himself recalculates Stas’ data, with O= 16 as the basis of computation, and derives from them the subjoined values for the elements which Stas studied : A g ....................

.................... R r .................... I .................... S .................... c1

107.9299 35.4494 79.9510 126.8556

32.0606

..................206.9042 K .................... 39. =5o7 N a .................... 23.0543 Li .................... 7.0307 N .................... 14.0396 Ph..

Combining these values for chlorine and nitrogen with his ratio HCl : N H , he gets 0 :H : : 16 : 0.9992. This, however, is only an apparent support of Prout’s hypothesis, for it depends upon the anti-Proutiaii determinations of Stas. If we calculate from Thomsen’s new ratio with X = 14 and C1= 3 5 . 5 , it gives H = I .0242 ; which is most unsatisfactory. In short, the method followed by Thoiiisen is too indirect and subject to too many possibilities of error to entitle it to much weight in fixing so important a constant as the atomic weight of oxygen. T h e direct processes, followed by several recent investigators, and giving O= I j.87 to I 5.89 are much more trustworthy. Meyer and Seubert’. i n their criticism of Thomsen’s work, have pointed out soiiie of its uncertainties. In this connection it may be noted that Scott’s research upon the coinposition of water by volunie, cited by abstract i n the report of last year, has been published in full i n the Philosopliical transaction^.^ Stronfizrm.-The atomic weight of strontium has been redetermined by Richards‘ from analyses of the bromide. T h e first ratio measured, after a careful preliminary study of materials 1 Zhchr. phys.

26’eYd. cJtem.

Chem.. rg, 7 2 6 . Ges., 2 7 * 2770. See also abstract by Ostwald in Z f d z r . j J i y A CJww.xs, . 70s.

1 8 4 543,1893, A mer. Acad. 1894. 369.

4 Pwc.

F. W. CLARKE.

204

REPORT O F COMMITTEE

and methods, was that between silver and strontium bromide. Of this ratio, three sets of determinations were made, all volunietric, but with differences of detail in the process. T h e weights are as follows, with the ratio Ag, : SrBr, : : 100: x i n the third column : FIRSTSERIES. Wt. .4g.

* ,30755 2.10351 2.23357 5.36840

-Sum,

I I .or303

Wt. SrBr,. I ,49962

2.41225 2.561 5 3 6.15663 I 2.63003

Ratio.

114.689 114.677 114.683 114.683 I

14.683

SECOND SERIES. Wt. A g .

Wt. SrBr,.

Ratio.

I .30762

1.49962

I 14.683

2.10322 4.57502 5.3-

2.41225

5.24727 6.15663

114.693 114.694 114.691

--

Sum, 13.35386

15.31577 THIRD SERIES. Wt. SrBr,.

Wt. A g .

--

114.692

Ratio.

-

2.9172 3.8946 4.5426 5.2473

-

114.692 114.695

s u m , 14.4748

16.6017

114.694

2.5434 3.3957 3.9607 4.5750

114.697 I 14.692

From these data we have, if Ag= 107.93, and B r = 79.955, ( 0= 16),the following results :

.. . . .. .. .. . .

From first series.. . . Sr = 87.644 " second series.. . . .. 87.663 " third series.. . .. . . . . 87.668

In two additional series, partly identical with the foregoing, the silver bromide thrown down was collected and weighed. I subjoin the weighings with the ratio sAgBr: SrBr, in the last column. FIRSTSERIES.

aAgBr.

SrBr,.

Ratio.

2.4415

I.W6

65.886

1.8817 4.5681 -

65.884 65.883 -

2.8561 6.9337 -Sum, 12.2313

8.0584

65.8834

ON ATOMIC WEIGHTS, PUBLISHED DURING 1894.

205

SECOND SERIES. sAgBr.

2.27625 3.66140 3.88776 9.34497

--

SrBr,.

1.49962 2.41225 2.56153 6.15663

Sum, 19.17038 12.63003 From the first series.. " '' second series..

Ratio.

65.881 65.883 65.887 65.882

--

.....- Sr =87.660 .. . 87.659

65.883

The average of all five series is S r = 87.659. Barium .-Richards has corroborated his earlier determitiations of the atomic weight of barium, which were made with the bromide, by means of additional series of experimetits upon the chloride.' The work was carried out in the most elaborate and thorough manner, and for details the original paper must be consulted. First, barium chloride was titrated with standard solutions of silver, and the several series represent different methods of ascertaining accurately the end point. T h e data are as follows, with the ratio Ag, :BaCl, : : 100 : x in the third column. FIRSTSERIES. Wt. A g . Wt. BaC1,. Ratio. 6.1872 5.6580 3.5ss8 9.4010 0.79

5.9717 5.4597 3.4728 9.0726

96.507

0.6950

96.541

96.517 96.495 96.499

Mean, 96.512

SECOND SERIES. Wt. A g .

6.59993 5.55229 4.6380

Wt. BaC1,.

6.36974 5.36010 3.92244

Ratio. 96.512

96.539 96.522

Mean, 96.524

THIRDSERIES. Wt. Ag.

4.4355 2.7440 6.1865 3.4023

Wt. BaC1,.

Ratio.

4.2815 2.6488 5.9712 3.2841

96.528 96.531 96.520 96.526 Mean, 96.526

1%.

A w . Acad., ag, 55.

206

F. W . CLARKE.

REPORT O F COMMITTEE

FOCRTH S H R I l i S . Wt. A g

Wt. BaCl,.

Ratio.

6.7342 10.6023

6.50022 10.23365

96.525 96.523 .Mean, 96.524

X11 the weights represent vacuum standards. From the four series the atomic weight of barium is deduced as follows ; when 0 = 16. F i r s t series Second Third " Fourth ' I

I'

.................. ..Ba .................... .................... ....................

' l

I'

I '

= 137,419 137.445 137.449 137,445

I n three more series of experiments Richards determined the ratio between 2AgCl and BaCl,. The data are subjoined, with the ratio zXgC1 : BaCl, IOO : x appended. FIRSTSERIES. \Vt, ARC1

W t . BaCI,.

Ratio.

8.7673 5.1979 4.9342 2.0765

6.3697 3.7765 3.5846 1.5"85 3.2163

72.653 72.654 72.648 72.646 j2.650

4.4271

Mean, 72.649

wt asci. 2.9750 7.37610 5.39906

SECOND SERIES. W t . BaCI,.

Ratio.

,52384 5.360 I O 3.92244

72.650 72.669 72.650

I

Mean, 72.6563

THIRDSERIES. Wt. A g C I .

Wt. BaCl,.

8.2189 4.5199

5.97'23 3.28410

Hence we have for Ba, F i r s t series.. .............. Ba = 137.428 Second " ................ " = 137.446 T h i r d " ................ " =I37.444

The mean of all is 137.440, as against 137.434 found in the work on the bromide. By combining the two chloride ratios,

ON ATOMIC WEIGHTS, PUBLISHED DURING

1894.

207

Ag, : BaCI, and 2AgCI : BaCI,, the ratio Ag : C1 can be computed. This gives A g = 107.930, a value identical with that of Stas. Cobalt and Nickel.-The atomic weights of these two metals have been redetermined by Winkler,' who adopts a radically new method, using the pure electrolytic elements as a startingpoint. I n each case, the weighed metal, deposited upon platinum, is treated with a weighed excess of iodine dissolved in potassium iodide. T h e metals are thus converted into iodides, and the excess of iodine is then measured by titration with thiosulphate solution. T h u s the direct ratios, C o : I , N i : I , are determined. Two series of estimations are given for each metal, with results as follows. The atomic weights used in calculation are H = I , I = 126.53. Wt.

co.

FIRSTSERIES-COBALT.

0.4999 0.5084 0.5290 0.6822

0.6715

Wt. I.

At. Wt. Co.

2.128837 2.166750 2.254335 2.908399 2.861617

59.4242 59.3772 59.3828 59.3582 59.3824 Mean, 59.3849

SECOND

0.5185 0.5267 0.53'9

SERIES-COBALT. 2.209694 2.246037 2.268736

59.3798 59 * 3430 59 * 3 294 Mean, 59.3507

Mean of all, C o = 59.3678.

FIRSTSERIES-NICKEL. Wt. Ni.

Wt. I.

At. Wt. Ni.

0.5144 0.4983 0.5265 0.6889 0.6876

2,217494 2.148502 2.268742 2.970709 2.9659 18

58.6702 58.69 I 8 58.7268 58.6828 58.6678 Mean, 58.6878

SECOND

0.5120 0.5200

0.5246

SERIES-NICKEL. 2.205627 2.204107 2.259925

58.7436 58.7432 58.7432 Mean, 58.7433

IZtschr. anorg. Chcm., 0. I.

208

F. W. C L A R K E .

REPORT OF COMMITTEE

Mean of all, Ni = 5 8 , 7 1 j 5 . For 0 = 16, these become c0=59.517 Xi = 58.863.

PaZladium--In I 889 Keiser published his determinations of the atomic weight of palladium, for which, since then, other investigators have found somewhat different values. H e has now, jointly with Mary B. Breed, given a new set of determinations, which confirm his former series.' As before, palladiammonium chloride was reduced in hydrogen, the salt being prepared by two methods and carefully examined as to purity. Two series of experiments are given, with the following weights of material : FIRSTSERIES. Yd( NH,CI),.

Pd.

At. Wt. Pd

I .60842

0.w97 I .04920 1.0'975 I . 28360 0.88410

106.271 106.325 106.334 106.342 106.341

2.08295 2.02440 2.548 IO 1.75505

From s u m of weights, 106.325 Reduced to vacuum, 106.246

SECOND SERIES. Pd(NH,Cl),

Pd.

I .50275

0.75685

I . 23672

0.62286

1.34470 1.49359

At. Wt. Pd.

106.297

106.296 0.67739 106.343 0.75095 106.353 -From s u m of weights, 106.322 Reduced to vacuum, 106.245

T h e atomic weight was computed with H = I , N = 1 4 . 0 1 ,and C1= 35.37. If O = 16 this becomes P d = 106.51. This is only 0.02 less than the value obtained in the earlier investigation. Tungsten.-A new determination of the atomic weight of tungsten, by Pennington and Smith,' leads to a much higher value than that commonly accepted. T h e older work seems very pro.bably to have been done upon material contaminated 1 A m . C h e m . j . , 16, M.

2 R e a d before t h e Ainer. Philos. Soc., Nov. z , 1894.

ON ATOMIC

WEIGHTS,PUBLISHED DURING 1894.

203

with molybdenum, an impurity which was eliminated in this investigation by Debray’s method,-that is, by volatilization by means of gaseous hydrochloric acid. The metal, carefully purified, was oxidized in porcelain crucibles, with all necessary precautions, and the following data are given : Wt. w. 0.862871 0.650700 0.597654

0.666820

0.428228 0.671920 0.590220 0.568654 1.080973

Wt. 0,. 0.22.1952

0.16-

0.155143 0.1 73103 0 . 1 1 1 168 0.I74406 0.I53 193 0.147588 0.280600

At. Wt. W

184.942 184.923 184.909 184.902 184.9”

184.925 184.933 184.943 184.913 Mean, 184.921

All weights are reduced to a vacuum, and 0 = 16 is taken as the standard of reference. Another paper, by Smith and Desi, was read at the same meeting with that just cited. I n this research, the tungstic oxide was purified in the same way, and reduced by heating in a stream of pure hydrogen. T h e water formed was weighed, and all weights reduced to a vacuum. Computed with 0 = 16 and H = I .008,the results are as follows : Wt. w o , .

0.983024 0.998424 1.008074 0.911974 0.997974 I .007024

Wt. H,O.

0.22834 0.23I 89 0.23409 0.21184 0.231 79 0.23389

At. Wt. W.

184.683 184.709 184.749 184.678 184 704 184.706 Mean, 184.704

Why this result should be lower than that previously found by Pennington and Smith remains to be explained. Thallium .--Two determinations of atomic weight were made by Wells and Penfield to ascertain the constancy of the element as such.’ T h e nitrate was fractionally crystallized until about one-twentieth remained in the mother-liquor, while another 1 A t n . j . Si.,[3], 47, 466.

2 IO

F . W. CLARKE.

REPORT O F C O M M I T T E E

twentieth had been subjected to repeated recrystallization. Both fractions were converted into thallium chloride, which was dried at roo*,and in both the chlorine mas estimated by weighing as silver chloride on a Gooch filter. T h e results were as follows :

.

1'1c1.

Crystals. . . . . . . . . . . . .3.9146 Mother-liquor.. . . . . . . .?.3415

AgC1.

A t . W t . T1.

2.3393 1.9968

203.47 204.47

Calculated with .4g= 107.92 and C1= 35.45. I n the report for 1893 Lepierre's work on thallium was given, and the last value cited was T1= 2 0 3 . 0 0 ~ varying widely from the rest of the series, and affecting the mean. The mean stated by Lepierre was 203.62, and as found by me was 203.57. Lepierre' now calls attention to the fact that his value 203.00 was a misprint for 203.60, and that his mean was therefore correctly given. H e also gives additional details relative to his work. Bismuth .--The long-standing controversy between Schneider and Classen over the atomic weight of bismuth, has led to a new set of determinations on the part of Schneider.' T h e old method was still used ; namely, of converting the metal into the trioxide by means of nitric acid and subsequent ignition of the nitrate ; but the metal itself was carefully purified. Results as follows : W t . Ili.

W t BipO,.

j.0092

5.5868 4.1016 8.08j4 IO. 3 I p 6.7979 13.5610

3.6770 7.2493 9.2479 6.0945

12.1588

I 'er ceiit. Bi i n Bi,O,

89.661 29.648 89.659 89.662 89.653 89.660

Mean, 89.657

If O = 16,Bi ranges from 207.94 to 208.15,or inmean 208.05, confirming the earlier determinations. Tin.-Incidentally to his paper on the white tin sulphide Schmidt gives one determination of the atomic weight of the ~iietal.~ 0.5243 gram Sn gave 0.6659 SnO,. Hence Sn= 118.48. 1 Rid[. SOC. Chim..[3], 11. 423

1.1.p r a k t . Chcm.. [ z ] . 50, 461. 8

R w d . clrrnr. Ges., 27. 2743.

ON .4TOMIC WEIGHTS, PUBLISHED DURING

1894.

21 I

Attomalous Nitrogot.--An important discovery has been made by Lord Rayleigh, who finds that nitrogen obtained by purely chemical methods is perceptibly lighter than that from atniospheric air.' Equal volumes of the gas, variously prepared, weighed as follows :

............. 2.30008 ..................2.29904 ...................... 2.29869

....

By passing NO over hot i r o n . . N,@ " " " " AmNO,

For nitrogen from air he found :

..

.............. 2.31003

F r o m air passed over hot iron. " t h r o u g h moist F e 0 2 H , . " "