The coexistence curve for a mixture of hard‐particle lattice gases

1984 ◽  
Vol 80 (6) ◽  
pp. 2767-2771 ◽  
Author(s):  
Douglas Poland
Author(s):  
Benjamin D. Goddard ◽  
Tim D. Hurst ◽  
Mark Wilkinson

The Liouville equation is of fundamental importance in the derivation of continuum models for physical systems which are approximated by interacting particles. However, when particles undergo instantaneous interactions such as collisions, the derivation of the Liouville equation must be adapted to exclude non-physical particle positions, and include the effect of instantaneous interactions. We present the weak formulation of the Liouville equation for interacting particles with general particle dynamics and interactions, and discuss the results using two examples.


Wear ◽  
2021 ◽  
pp. 203901
Author(s):  
Leonel A. Teran ◽  
Santiago Laín ◽  
Sara A. Rodríguez

1996 ◽  
Vol 105 (24) ◽  
pp. 11175-11182 ◽  
Author(s):  
Michael P. Allen ◽  
Philip J. Camp ◽  
Carl P. Mason ◽  
Glenn T. Evans ◽  
Andrew J. Masters
Keyword(s):  

1978 ◽  
Vol 56 (9) ◽  
pp. 1140-1141 ◽  
Author(s):  
P. Palffy-Muhoray ◽  
D. Balzarini

The index of refraction at 6328 Å has been measured for germane in the density range 0.15 to 0.9 g/cm3. The temperature and density ranges over which measurements are made are near the coexistence curve. The coefficient in the Lorenz–Lorentz expression, [Formula: see text], is constant to within 0.5% within experimental error for the temperature range and density range studied. The coefficient is slightly higher near the critical density. The critical density is measured to be 0.503 g/cm3. The critical temperature is measured to be 38.92 °C.


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