If two rarefied masses of gas collide at a sufficiently high speed, their relative motion will be stopped by a collectlve plasma instability rather than by collisions of individual particles. The possible influence of magnetic fields is ignored for the most part, but a criterion is found to decide uader what conditions the collective interaction remains domiuant even when they cannot be ignored. (W.D.M.)
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F. D. Kahn (1958) studied this question.
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