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Some properties of the Fokker-Planck equation

Published online by Cambridge University Press:  13 March 2009

G. J. Lewak
Affiliation:
Electrical Engineering and Computer Science Department, U.C.S.D. La Jolla, CA. 92093
L. A. Soto
Affiliation:
Electrical Engineering and Computer Science Department, U.C.S.D. La Jolla, CA. 92093

Abstract

The solution of the Fokker-Planck equation for the distribution function of heavy ions in a background of electrons is studied. It is found that quite broad physical conditions on the distribution function (such as the positive requirement and the existence of all velocity moments) are sufficient to eliminate any ambiguity in the time-independent steady-state solutions and to determine a discrete spectrum of the time-dependent Fokker–Planck operator. The more physical case of a Maxwell-Boltzman electron distribution function is treated using the small mass ratio expansion. First-order mass ratio corrections are calculated. A plasma heating application-is suggested.

Type
Research Article
Copyright
Copyright © Cambridge University Press 1985

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References

REFERENCES

Montgomery, D. C. & Tidman, D. A. 1964 Plasma Kinetic Theory, p. 20. McGraw-Hill.Google Scholar
Morse, P. M. & Feshbach, H. 1953 Methods of Theoretical Physics, part 1, p. 611, McGraw-Hill.Google Scholar
Saito, H. et al. 1977 Nuclear Fusion Supp. Part 3, 337.Google Scholar
Tsuji, H. et al. 1976 Nucl. Fusion, 16. 2.CrossRefGoogle Scholar