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Heat conduction in a nearly collisionless molecular gas

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  • Knaap, H.F.P.
  • Beenakker, J.J.M.
  • Kuščer, I.

Abstract

Transport phenomena in molecular gases and the respective field effects have so far been analyzed in the hydrodynamic and Knudsen regimes. In between there is a rather large gap covered by the transition regime. For the case of heat conduction through a diatomic diamagnetic gas between parallel plates an attempt is made to partially bridge the gap by the beginning of a density expansion derived through iteration of an integral form of the Boltzmann equation. Second-order perturbation in non-sphericity of both intermolecular and gas-wall interactions is applied to determine the effect of a magnetic field. Explicit expressions are derived for a simple model.

Suggested Citation

  • Knaap, H.F.P. & Beenakker, J.J.M. & Kuščer, I., 1982. "Heat conduction in a nearly collisionless molecular gas," Physica A: Statistical Mechanics and its Applications, Elsevier, vol. 112(1), pages 29-43.
    • Handle: RePEc:eee:phsmap:v:112:y:1982:i:1:p:29-43
    DOI: 10.1016/0378-4371(82)90206-0
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    References listed on IDEAS

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    1. Snider, Thomas E., 1972. "Branch Banking And Loan Portfolio Changes- The Virginia Experience," 1972 Annual Meeting, August 20-23, Gainesville, Florida 284611, American Agricultural Economics Association (New Name 2008: Agricultural and Applied Economics Association).
    2. Eggermont, G.E.J. & Vestner, H. & Knaap, H.F.P., 1976. "Influence of a magnetic field on diffusion and thermal diffusion in gaseous mixtures," Physica A: Statistical Mechanics and its Applications, Elsevier, vol. 82(1), pages 23-46.
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