Magnetohydrodynamic Equilibrium with Spheroidal Plasma-Vacuum Interface : Compact Toroid without Toroidal Magnetic Field
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概要
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The Grad-Shafranov equations for an oblate and a prolate spheroidal plasmasare solved analytically under the assumptions, 7l?.=0 and dp/d*=constant.Here B. is the toroidal magnetic field, p is the kinetic pressure, and p is themagnetic flux function. The plasmas in magnetohydrodynamic equilibrium areshown to be toroidal. The equilibrium magnetic-field configurations outside thespheroidal plasmas are considerably different from that of a spherical plasma.A line cusp or two point cusps appear outside the oblate or the prolate spheroidalplasma, respectively.
- 社団法人日本物理学会の論文
- 1983-06-15
著者
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KANEKO Shobu
Department of Applied Physics,Faculty of Engineering The University of Tokyo
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Kaneko S
Univ. Tokyo
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Kaneko Shobu
Department Of Applied Physics Faculty Of Engineering The University Of Tokyo
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HIROTA Isao
Energy Technology Division, Electrotechnical Laboratory, AIST, MITI
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CHIYODA Katsuji
Department of Applied Physics,Faculty of Engineering,The University of Tokyo
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HIROTA Isao
Department of Applied Physics,Faculty of Engineering,The University of Tokyo
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Hirota Isao
Department Of Applied Physics Faculty Of Engineering The University Of Tokyo:electrotechnical Labora
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Chiyoda Katsuji
Department Of Applied Physics Faculty Of Engineering The University Of Tokyo:electrotechnical Labora
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