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A new method of solution for one-dimensional quasi-neutral bounded plasmas

Published online by Cambridge University Press:  22 January 2010

M. KAMRAN
Affiliation:
Association Euratom-ÖAW, Institute for Theoretical Physics, University of Innsbruck, Technikerstrasse 25, A-6020 Innsbruck, Austria (muhammad.kamran@uibk.ac.at)
S. KUHN
Affiliation:
Association Euratom-ÖAW, Institute for Theoretical Physics, University of Innsbruck, Technikerstrasse 25, A-6020 Innsbruck, Austria (muhammad.kamran@uibk.ac.at)

Abstract

A new method is proposed for calculating the potential distribution Φ(z) in a one-dimensional quasi-neutral bounded plasma; Φ(z) is assumed to satisfy a quasi-neutrality condition (plasma equation) of the form ni{Φ(z)} = ne(Φ), where the electron density ne is a given function of Φ and the ion density ni is expressed in terms of trajectory integrals of the ion kinetic equation. While previous methods relied on formally solving a global integral equation (Riemann, Phys. Plasmas, vol. 13, 2006, paper no. 013503; Kos et al., Phys. Plasmas, vol. 16, 2009, paper no. 093503), the present method is characterized by piecewise analytic solution of the plasma equation in reasonably small intervals of z. As a first concrete application, Φ(z) is found analytically through order z4 near the center of a collisionless Tonks–Langmuir discharge with a cold-ion source.

Type
Papers
Copyright
Copyright © Cambridge University Press 2010

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References

[1]Lieberman, M. A. and Lichtenberg, A.. 1994. Principles of Plasma Discharges and Materials Processing. New York: Wiley.Google Scholar
[2]Hutchinson, I. H.. 2002. Principles of Plasma Diagnostics, 2nd edn.Cambridge: Cambridge University Press.CrossRefGoogle Scholar
[3]Stangeby, P. C.. 2000. The Plasma Boundary of Fusion Devices. Bristol, UK: Institute of Physics Publishing.CrossRefGoogle Scholar
[4]Tonks, L. and Langmuir, I.. 1929. A general theory of the plasma of an arc. Phys. Rev. 34, 876.CrossRefGoogle Scholar
[5]Harrison, E. R. and Thompson, W. B.. 1959. The low pressure plane symmetric discharge. Proc. Phys. Soc. Lond. 74, 145.CrossRefGoogle Scholar
[6]Riemann, K.-U., Seebacher, J., Tskhakaya, D. D. Sr, and Kuhn, S.. 2005. The plasma-sheath matching problem. Plasma Phys. Control. Fusion 47, 1949.CrossRefGoogle Scholar
[7]Riemann, K.-U. 2006 Plasma-sheath transition in the kinetic Tonks–Langmuir model. Phys. Plasmas 13, 063508.CrossRefGoogle Scholar
[8]Kos, L., Jelić, N., Kuhn, S., and Duhovnik, J.. 2009. Extension of the Bissell–Johnson plasma-sheath model for application to fusion-relevant and general plasmas. Phys. Plasmas 16, 093503.CrossRefGoogle Scholar
[9]Kamran, M. 2010 Correct fluid treatment of the collisionless Tonks-Langmuir model with a cold ion source. PhD thesis, Institute for Theoretical Physics, University of Innsbruck.Google Scholar
[10]Riemann, K.-U. 1991 The Bohm criterion and sheath formation. J. Phys. D: Appl. Phys. 24, 493.CrossRefGoogle Scholar