1975 Volume 39 Issue 1 Pages 261-262
Based on the microscopic theory of transport processes, the Buneman resistivity is calculated to be (4πα⁄\sqrt3ωp)(me⁄2mi)1⁄3, where ωp2=4πne2⁄me and α=〈δn2〉⁄n2. The saturation level of turbulence in the Hamberger-Jancarik experiment is inferred to be α\simeq0.35; a number of possible mechanisms for the saturation are discussed.
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