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On the definition of Pfirsch–Schlüter and bootstrap currents in toroidal systems
1.For reference to the original report by D. Pfirsch and A. Schlüter see, for example, the bibliography in our Re£ 2 or 3.
2.F. L. Hinton and R. D. Hazeltine, Rev. Mod. Phys. 48, 239 (1976).
3.S. P. Hirshman and D. J. Sigmar, Nucl. Fusion 21, 1079 (1981).
4.K. C. Shaing and J. D. Callen, Phys. Fluids 26, 3315 (1983).
5.M. Coronado and H. Wobig, Phys. Fluids 30, 3171 (1987).
6.L. S. Solov’ev and V. D. Shafranov, Review of Plasma Physics, edited by M. A. Leontovich (Consultants Bureau, New York 1970), Vol. 5, and references therein.
7.G. Bateman, MHDInstabilities (MIT Press, Cambridge, 1980), p. 125.
8.J. W. Connor and J. B. Taylor, Comments Plasma Phys. Controlled Fusion 11, 37 (1987).
9.Notice, however, that the dependence of Eq. (28) on appears through and Since it results that both and have only a weak dependence on because they are mainly determined externally by the current in the toroidal coils. Thus, to lowest order in the quantities and do not depend on
10.M. Coronado and J. Galindo Trejo, Phys. Fluids B 2, 530 (1990).
11.R. Balescu, Transport Processes in Plasmas (North-Holland, Amsterdam, 1988), Part I, Chap. 12.
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