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Physics of Plasmas -- November 1994 -- Volume 1, Issue 11, pp. 3570-3576

Electron heat transport with non-Maxwellian distributions

J. M. Liu and J. S. De Groot
Plasma Research Group, Department of Applied Science, University of California, Davis, California 95616
J. P. Matte and T. W. Johnston
INRS-Énergie et Matériaux, C.P. 1020, Varennes, Québec, J3X 1S2 Canada
R. P. Drake
Plasma Physics Research Institute, Lawrence Livermore National Laboratory, L-418, P.O. Box 808, Livermore, California 94551

 

(Received 8 March 1994; accepted 14 July 1994)

Measurements are presented of electron heat transport with non-Maxwellian (flattopped) distributions due to inverse bremsstrahlung absorption of intense microwaves in the University of California at Davis Aurora II device [Rogers et al., Phys. Fluids B 1, 741 (1989)]. The plasma is created by pulsed discharge in a cylindrical vacuum chamber with surface magnets arranged to create a density gradient. The ionization fraction (~1%) is high enough that charged particle collisions are strongly dominant in the afterglow plasma. A short microwave pulse (~2 µs) heats a region of the afterglow plasma (ne/ncr<=0.5) creating a steep axial (LT~1–10lambdaei) temperature gradient. Langmuir probes are used to measure the relaxation of the heat front after the microwave pulse. Time and space resolved measurements show that the isotropic component of the electron velocity distribution is flat topped (~exp[–(v/vm)m], m>~2) in agreement with Fokker–Planck calculations using the measured density profile. Classical heat transport theory is not valid both because the isotropic component of the electron velocity distribution is flattopped and the temperature gradients are very steep. Physics of Plasmas is copyrighted by The American Institute of Physics.

 

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Electron heat transport with non-Maxwellian distributions

Electron heat transport with non-Maxwellian distributions