Ion transport theory for a slightly ionized rarefied gas in a strong electric field. II.

J. H. Whealton, E. F. Jaeger, and D. S. Burch
Phys. Rev. A 15, 773 – Published 1 February 1977
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Abstract

Solutions to the initial-value problem of a weakly ionized rarefied gas in a uniform electrostatic field are found explicitly for the lowest three hydrodynamic levels indicated by a moment method previously described. The resulting sets of equations are solved by a completely implicit Crank-Nicholson scheme. For very light ions, or moderately inelastic electrons, a Monte Carlo solution is also found and compared to the moment solutions delineating their range of validity. The deviation of the higher-order theory from the diffusion theory is mapped on a parametric plane bounding the region of validity of the diffusion equation as derivable from the Boltzmann equation. The Hornbeck experiment is analyzed neglecting a cathode boundary, thus illustrating the effects of large initial density gradients on the transient current.

  • Received 15 September 1975

DOI:https://doi.org/10.1103/PhysRevA.15.773

©1977 American Physical Society

Authors & Affiliations

J. H. Whealton*, E. F. Jaeger*, and D. S. Burch

  • Joint Institute for Laboratory Astrophysics, University of Colorado and National Bureau of Standards, Boulder, Colorado 80302

  • *Now at Oak Ridge National Laboratory, Thermonuclear Division, Oak Ridge, Tenn. 37830.
  • JILA Visiting Fellow 1973-74, on leave from Dept. of Physics, Oregon State University, Corvallis, Ore. 97331.

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Vol. 15, Iss. 2 — February 1977

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