MHD plasma stabilization in a chain of axisymmetric adiabatic open mirror cells

Abstract

Conditions for convective plasma instability in a chain of axisymmetric adiabatic mirror cells with different signs of magnetic field curvature are analyzed. The boundaries of the region that can be occupied by a stable hollow plasma in a system of two connected cells—a nonparaxial simple mirror cell and a semicusp—are determined, as well as the interval of allowed values of the ratio between the pressures in the cells. Because of the large magnetic field curvature in the component cells, the safety factor that is achieved at both—external and internal—plasma boundaries in accordance with the average min-B principle can be high. It is assumed that the unperturbed pressure in each cell is almost isotropic, in which case the mirror ratio should necessarily be large. A key role in the stability of the plasma is played by its compressibility. A comparison is made between the conditions for complete plasma stabilization against arbitrary perturbations and the conditions for stability of individual cells against the global mode. The stability of the cells against the global mode is sufficient, but not necessary, for stabilizing the chain. The analysis is done by using orthogonal coordinates associated with the unperturbed magnetic field (flux variables). Numerical simulations were carried out for nonparaxial cells from a certain three-parameter family.