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Plasma Transport in Toroidal Confinement Systems
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2.[L. A. Artsimovich, A. M. Anashin, E. P. Gorbunov, D. P. Ianov, M. P. Petrov, and V. S. Strelkov, JETP Letters 10, 82 (1969)].
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9.An analysis of this point, which however includes the effects of like species collisions only through a model collision operator, has been presented by P. H. Rutherford, L. M. Kovrizhnikh, M. N. Rosenbluth, and F. L. Hinton [Phys. Rev. Letters. 25, 1090 (1970)].
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17.Some terms in which relate that flux to the forces n′, and have been neglected in Eq. (173). (In this approximation, ) These terms may be significant, however, in the substitution of Eq. (173) into the ion heat balance Eq. (172). We therefore remark that the corrections to which can be calculated with some refinement of our procedures of Secs. III and IV, are proportional to г, and that results correct to may be obtained simply by replacing the left‐hand side of Eq. (173) by
18.Compare Ref. 9. The coefficient 1.6 in Eq. (9) of this reference results from a numerical error, and should be 1.46, as given in our Eq. (182).
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20.We are indebted to A. A. Ware (private communication) for pointing out this relation.
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