Abstract
A quasi-linear prediction of the two-fluid dynamo effect is analyzed with the use of tearing eigenfunctions obtained for force-free equilibrium. In the range of parameters of practical interest, the basic shear Alfvén mode is decoupled from fast compressional Alfvén and slow magneto-acoustic modes. Kinetic Alfvén modification of the shear Alfvén wave drives an instability with a growth rate ∝δ1/3ρ 2/3s , where δ is the electron skin depth and ρs is the ion-sound gyroradius. A net dynamo effect parallel to the magnetic field is calculated at ρ s ≫δ for large values of the stability factor \(\Delta '\rho _s^{{1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}} \delta ^{{1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}} \gg 1\). The dynamo effect caused by the j×B Hall term dominates the contribution from the v×B term (the alpha effect) by a factor ∝(ρs/δ)2 in the narrow electron layer, while in the broader ion layer these contributions are comparable. The results are compared with the case of a strong guiding field where ρ s ≪δ and the tearing instability is described by resistive MHD.
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From Fizika Plazmy, Vol. 29, No. 7, 2003, pp. 612–617.
Original English Text Copyright © 2003 by Mirnov, Hegna, Prager.
This article was submitted by the authors in English.
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Mirnov, V.V., Hegna, C.C. & Prager, S.C. A hall dynamo effect driven by two-fluid tearing instability. Plasma Phys. Rep. 29, 566–570 (2003). https://doi.org/10.1134/1.1592555
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DOI: https://doi.org/10.1134/1.1592555