Determining Intermolecular Potentials from Second Virial Coefficients

1996 ◽  
Vol 73 (7) ◽  
pp. 612
Author(s):  
Brian P. Reid
1976 ◽  
Vol 54 (16) ◽  
pp. 2617-2627 ◽  
Author(s):  
Vijay P. S. Nain ◽  
Ronald A. Aziz

The predictions of the Joule–Thomson coefficient for the inert gases on the basis of numerous intermolecular potentials are calculated and compared with directly measured experimental data and derived values from p–V–T measurements. For all Systems, the agreement is good except for TFD potentials derived by Gustafsson for He and Ne. We have also shown that the kinetic energy corrections in the low pressure region are not as high as those suggested by Gustafsson. Inversion temperatures are also calculated and recommended values are presented. Also presented are empirical relations which give as a function of temperature, second virial coefficients including the first two quantum corrections for many of the realistic potentials.


2011 ◽  
Vol 164 (1-2) ◽  
pp. 153-156 ◽  
Author(s):  
Francisco Gámez ◽  
Santiago Lago ◽  
Álvaro Plaza-Reyes ◽  
Alfredo González-Calderón

1955 ◽  
Vol 33 (4) ◽  
pp. 589-596 ◽  
Author(s):  
G. A. Nicholson ◽  
W. G. Schneider

The second virial coefficients of neon have been determined in the temperature range 0° to 700 °C. and the pressure range 10 to 80 atmospheres. These data were combined with published low temperature (−150° to 0 °C.) second virial data, to investigate the intermolecular potentials of neon using both a Lennard-Jones potential, with a 9th and 12th power repulsion term, and also a modified Buckingham exponential–six potential. The agreement between observed and calculated values of B(T) was excellent for both the exponential–six and the Lennard-Jones 12:6 potentials and slightly less satisfactory for the Lennard-Jones 9:6 potential.


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