Abstract
In this paper, magnetic field generation in a fully ionized plasma is discussed both in the presence and absence of an external constant magnetic field. Considering the dependence of the transfer coefficients on the magnetic field, Braginsky's equations are applied to describe collective processes in plasma. Criteria for the formation of instabilities and, consequently, the generation of magnetic fields are obtained, taking into account convective heat transfer and thermomagnetic phenomena. We derive expressions for the growth rate of perturbations in the magnetic field and the temperature in the short-wave range.
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