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The Electron Temperature of a Partially Ionized Gas in an Electric Field

Abstract

The electron temperature of a partially ionized gas in an electric field can be determined by the collision rate for momentum transfer and the collision rate for energy transfer. Mean values of these rates are defined such that a simple expression for the electron temperature is obtained, and which depends, among other things, on the ratio of these mean rates. This ratio is calculated in the Lorentz approximation for power law cross sections, and also as a function of the degree of ionization for a helium plasma. It is pointed out that the complete results of refined transport theory can be used in calculating electron mobility and electron temperature in a multicomponent plasma without undue difficulty.
Authors:
Publication Date:
Mar 15, 1968
Product Type:
Technical Report
Report Number:
AE-313
Resource Relation:
Other Information: 19 refs., 2 figs.
Subject:
70 PLASMA PHYSICS AND FUSION TECHNOLOGY; ELECTRON TEMPERATURE; ELECTRIC FIELDS; WEAKLY IONIZED GASES; ELECTRON MOBILITY; COLLISIONS; ENERGY TRANSFER; MOMENTUM TRANSFER
OSTI ID:
20956283
Research Organizations:
AB Atomenergi, Nykoeping (Sweden)
Country of Origin:
Sweden
Language:
English
Other Identifying Numbers:
TRN: SE0708717
Availability:
Commercial reproduction prohibited; OSTI as DE20956283
Submitting Site:
SWDN
Size:
20 pages
Announcement Date:
Dec 31, 2007

Citation Formats

Robben, F. The Electron Temperature of a Partially Ionized Gas in an Electric Field. Sweden: N. p., 1968. Web.
Robben, F. The Electron Temperature of a Partially Ionized Gas in an Electric Field. Sweden.
Robben, F. 1968. "The Electron Temperature of a Partially Ionized Gas in an Electric Field." Sweden.
@misc{etde_20956283,
title = {The Electron Temperature of a Partially Ionized Gas in an Electric Field}
author = {Robben, F}
abstractNote = {The electron temperature of a partially ionized gas in an electric field can be determined by the collision rate for momentum transfer and the collision rate for energy transfer. Mean values of these rates are defined such that a simple expression for the electron temperature is obtained, and which depends, among other things, on the ratio of these mean rates. This ratio is calculated in the Lorentz approximation for power law cross sections, and also as a function of the degree of ionization for a helium plasma. It is pointed out that the complete results of refined transport theory can be used in calculating electron mobility and electron temperature in a multicomponent plasma without undue difficulty.}
place = {Sweden}
year = {1968}
month = {Mar}
}