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Neoclassical diffusion of a finite-β, tokamak plasma

Published online by Cambridge University Press:  13 March 2009

Aldo Nocentini
Affiliation:
Istituto di Meccanica, Università degli Studi, Trieste

Abstract

The neoclassical diffusion in a tokamak is calculated for a finite-β plasma. The flux of the particles is shown to be substantially unchanged, with respect to the low-β case. The ‘equilibrium’ equation is derived. From it the magnetic surfaces can be obtained, once the external electromagnetic field and the density and temperature profiles are given. The case of magnetic surfaces with circular cross-section, in the small aspect ratio limit, is considered in detail.

Type
Research Article
Copyright
Copyright © Cambridge University Press 1972

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References

REFERENCES

Adam, J. C. & Mercier, C. 1969 Proc. Conf. Novosibirsk 1968, vol. 1, p. 199. Vienna: IAEA.Google Scholar
Frieman, E. A. 1970 Phys. Fluids, 13, 490.CrossRefGoogle Scholar
Galeev, A. A. & Sagdeev, R. Z. 1968 Soviet Phys. JETP, 26, 233.Google Scholar
Kovrizhnikh, L. M. 1969 Soviet Phys. JETP, 29, 475.Google Scholar
Rutherford, P. H. 1970 Phys. Fluids, 13, 482.CrossRefGoogle Scholar
Rutherford, P. H., Kovrizhnikh, L. M., Rosenbluth, M. N. & Hinton, F. L. 1970 Phys. Rev. Letters 25, 1090.CrossRefGoogle Scholar
Spitzer, L. 1962 Physics of Fully Ionized Gases, ch. 5. New York: Interscience.Google Scholar
Ware, A. A. 1970 Phys. Rev. Lett. 25, 916.CrossRefGoogle Scholar