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Reminimization of Energy Integral and Stability Limit for Non-Ideal MHD (Magnetohydrodynamic) Plasma

机译:非理想mHD(磁流体)等离子体能量积分和稳定极限的再极化

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The stability condition of relaxed states is derived from the energy principle for the non-ideal MHD plasma. An Euler equation for the reminimization of energy integral is derived and shown to give the marginal stable, non-singular perturbations for the stability condition. An extended stability limit for the beta = 0 relaxed states is derived from the stability condition, with use of the eigenvalue analysis for the Euler equation. By using the perturbation method, the extended stability limit is solved in the 1st order approximation to explain the deviation of the experimental stability limit from the idealized stability limit by Taylor. A procedure to get overall stability limit against both the non-singular and the singular perturbations is discussed. 25 refs. (ERA citation 13:038788)

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