Kinetic Theory of Loaded Spheres. IV. Thermal Diffusion in a Dilute‐Gas Mixture of D2and HT

1967 ◽  
Vol 47 (8) ◽  
pp. 2621-2630 ◽  
Author(s):  
Stanley I. Sandler ◽  
John S. Dahler
1973 ◽  
Vol 57 (1) ◽  
pp. 103-110 ◽  
Author(s):  
M. L. Lawson ◽  
Wen-Jei Yang

This paper investigates the Bénard problem in a binary mixture of dilute gases in which an imposed vertical temperature gradient induces a concentration gradient owing to the thermal diffusion effect. The transfer equations are derived by first-order perturbation theory which leads to instability criteria. Numerical results indicate that instability will set in only as stationary convection. This is distinctly different from the cases of liquids and concentrated gases, in which the thermal diffusion (or Soret) effect gives rise to oscillatory instability. It is disclosed in the study that the destabilization of the dilute gas-mixture layer is enhanced by an increase in the thermal diffusion ratio and/or the molecular weight ratio of the species.


Author(s):  
Sauro Succi

Kinetic theory is the branch of statistical physics dealing with the dynamics of non-equilibrium processes and their relaxation to thermodynamic equilibrium. Established by Ludwig Boltzmann (1844–1906) in 1872, his eponymous equation stands as its mathematical cornerstone. Originally developed in the framework of dilute gas systems, the Boltzmann equation has spread its wings across many areas of modern statistical physics, including electron transport in semiconductors, neutron transport, quantum-relativistic fluids in condensed matter and even subnuclear plasmas. In this Chapter, a basic introduction to the Boltzmann equation in the context of classical statistical mechanics shall be provided.


1975 ◽  
Vol 1 (1) ◽  
pp. 20-26
Author(s):  
Takao Kokugan ◽  
Masaru Shimizu

2000 ◽  
Vol 37 (4) ◽  
pp. 397-404 ◽  
Author(s):  
Hiroshi YAMAKAWA ◽  
Noboru KOBAYASHI ◽  
Youichi ENOKIDA ◽  
Ichiro YAMAMOTO

1962 ◽  
Vol 40 (11) ◽  
pp. 1608-1613 ◽  
Author(s):  
S. C. Saxena ◽  
S. M. Dave ◽  
P. A. Pardeshi

Simpler formulae for the second approximation to the thermal diffusion factor of a binary gas mixture are derived according to both the approximation procedures of Chapman and Cowling, and Kihara. These formulae are much simpler than the rigorous theoretical formulae from the view point of computational labor. These new formulae are derived by expanding the rigorous expressions in powers of the molecular weight ratio, M, and deleting all those terms which contain explicitly the power of M higher than two. The accuracies of these simpler formulae are demonstrated by numerical calculations on gas systems as a function of both temperature as well as composition.


1976 ◽  
Vol 9 (5) ◽  
pp. 411-413
Author(s):  
TAKAO KOKUGAN ◽  
HITOSHI YOSHIDA ◽  
MASARU SHIMIZU

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