Second Virial Coefficients of the Lennard-Jones (6,m) Gases.

1966 ◽  
Vol 11 (1) ◽  
pp. 77-80 ◽  
Author(s):  
M. M-n. Sze ◽  
H. W. Hsu





1971 ◽  
Vol 54 (9) ◽  
pp. 4139-4140
Author(s):  
R. E. Caligaris ◽  
C. F. Mosquera ◽  
A. E. Rodriguez




1999 ◽  
Vol 155 (1) ◽  
pp. 75-83 ◽  
Author(s):  
Y.C Chiew ◽  
V Sabesan


1977 ◽  
Vol 30 (8) ◽  
pp. 1645 ◽  
Author(s):  
GA Bottomley ◽  
DB Nairn

A constant-volume gas-thermometer technique has been used at sub- atmospheric pressure to provide second virial coefficients to above 500 K from initial values in the vicinity of 300 K. The results for three organic vapours, butane, tetramethylsilane, 1,2-dichloro-1,1,2,2- tetrafluoroethane, are provided and expressed in terms of the intermolecular parameters for the Lennard-Jones (12-6) potential and the De Rocco and Hoover spherical-shell potential.



1971 ◽  
Vol 24 (12) ◽  
pp. 2449 ◽  
Author(s):  
CHJ Johnson ◽  
TH Spurling

The Hamann-Lambert model for globular molecules using Lennard-Jones 12- 6 potential functions for the atomic interactions has been used to obtain second virial coefficients for CH4, CF4, SF6, SiF4, CMe4, SiMe4, and the mixtures CH4-CF4, CH4-SF6, CH4-CMe4, CH4-SiMe4, and CF4-SF6. Additive third virial coefficients have been computed where experimental data are available. Of the 18 parameter sets needed for the 12-6 interactions in the above molecules and their combinations ten were obtained by a least-squares fitting process using experimental values of second virial coefficients, five were obtained from combining rules, and the remaining three from sources independent of virial coefficient data. The computed values of the virial coefficients agree well with the experimental data although in the case of the third virial coefficients improved agreement would be obtained if some form of non-additivity could be allowed for.



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