Page 1 4784 c. R. .4DAMS, JR., H. L. JOHNSTON AKD E. c. KERR I

Oct 3, 2014 - BY GEORGE B. Lb.\MS, JR., I ~ E R R ~ C K. 1,. JOI1NSTON .4ND EUGENIC c. KERR. RECEIVED FERRI.ARY 1, 1OtX. A gram atom of gallium ...
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c.R. .4DAMS,

4784 /CONTRIBUlION FROM

TIXE

JR.,

H. L.

JOHNSTON AKD

E.

c. KERR

I-01. 7 I

CRYOGENIC LABORATORY, DEPARTMENT O F CHEMISTRY, THEOHIO STATE

UXIVERSITY

]'

The Heat Capacity of Gallium from 15 to 320°K. The Heat of Fusion at the Melting Point BY GEORGE B.

Lb.\MS,

JR.,

I ~ E R R ~1,. CK JOI1NSTON

.4ND EUGENIC

c. K E R R

RECEIVED FERRI.ARY 1, 1OtX

A gram atom of gallium (99.99% purity) was preparctl, ~ n t iiieasurenients l were taken with this sample and with four other gallium samples, over the range 15 t o 300"K., t o obtain the heat capacity of the solid. The heat capacity of liquid gallium was measured from 303 t o 322"K., and was found to decrease with increasing temperature over this range. The heat of fusion of a sample of pure gallium was measured in a calorimeter designed specifically for the purpose and was found to be 1335 i 1.0 cal./g. atom. The entropy of fusion is 4.407 i 0.004 e.u. a t the melting point. A lambda point in the heat capacity curve for the solid observed at 292.4"K.,was shown t o have been caused by eutectic xneltitig of tin, present as an impurity in those gallium samples for which the anomaly was observed. A table of thermodynamic functions has been prepared for gallium at smoothed values of the temperatures. The entropies a t 298.1B°K., and at the melting point, 302.9>'K., are 9.82 i 0.05 e.u. and 9.92 i 0.05 e.u. (entropy of fusion not included), respectively, of which 0.15 e.u. was contributed by extrapolation below 16°K.

Introduction Clusius and Harteck2measured the heat capacity of solid gallium between 15 and 200'K. and Roth, Meyer and Zeumer, reported empirical equations for the heat capacities of the solid and liquid, as a function of temperature, near the melting point. These data were obtained as a part of their work on the calorimetric determination of the heat of fusion. The work done by Clusius and Harteck is incomplete and admittedly inaccurate because of the large heat transfer corrections required, and because less than a tenth of a gram atom uf galliuni was available. The heat of fusion of gallium has been measured calorimetrically by B e r t h e l ~ t , and ~ by Koth, Meyer and Zeumer,3 and piezometrically by Richards and B ~ y e r . ~ I t appeared desirable to redetermine the low tem/-CAP

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(1) This work w a s supported in part by the Office of Naval Research under contract with The Ohio State University Research Foundation. ( 2 ) K. Clusius and P. IIarteck, Z . piirrih. Ckem., 134, 243 (1928). (3) W. A . Koth, I. Meycr nod Ii. Zeumei-, %. uizo~g.allgcm. Chem., 214, 300 (1933). ( 2 ) X l . Berthelot, A n n . c h i m . pkys., 5, 242 ( 1 S i 8 ) . (.