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9, c o r r e s p o n d i n g t o F i g . 5, is c i r c u l a r in c r o s s s e c t i o n , b u t h a s suffered a helical F I G . 9. The plasma surface is represented by an interior surface of the mesh, as in Fig. 5, at a time corresponding to that drawn in Figs. 6b, 7b, and 8b. The helical distortion of the plasma c o l u m n characteristic of an m = 1 perturbation is clearly shown. 38 JEREMIAH U. BRACKBILL d i s p l a c e m e n t f r o m t h e g e o m e t r i c axis. T h e c o m p u t a t i o n m e s h in F i g .

C , a n d Mastin, C . W . (1974). / . Comput. Phys. 15, 299. Tuck, J. (1968). Eur. Conf. Controlled Fusion Plasma Phys. , 2nd, 1968 V o l . 2, p. 595. Wagner, C. E . , a n d Manheimer, W . M . (1973). Proc. Conf. Numer. Simul. Plasmas, 6th 1973 Lawrence Livermore L a b . Conf. R e p . 730804. , M o n t i c e l l o , D . , R o s e n b l u t h , Μ . N . , and Strauss, N . (1974). Plasma Phys. , 1974, V o l . 1 , p. 495. , Hicks, H . , a n d D o r y , R. A . (1974). "Preliminary Results o f the 3 D N o n l i n e a r Ideal M H D C o d e , " O R N L T M 4784.

T h e p l a s m a is infinitely c o n d u c t i n g , a n d fills t h e i n t e r i o r o f a c o n ­ d u c t i n g c y l i n d e r . T h e r a d i a l v a r i a t i o n o f t h e c u r r e n t d e n s i t y is w r i t t e n r > a (79) w h e r e

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A Textbook of Electrical Technology Volume 2 by B.L. THERAJA and A. K. THERAJA

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