Effects of Hall Currents on the Self-Gravitational Instability of a Finitely Conducting Plasma of Variable Density
β Scribed by P. K. Bhatia; P. N. Gupta
- Publisher
- John Wiley and Sons
- Year
- 1976
- Tongue
- English
- Weight
- 427 KB
- Volume
- 16
- Category
- Article
- ISSN
- 0005-8025
No coin nor oath required. For personal study only.
β¦ Synopsis
Abstract
The effects of Hall currents have been studied on the hydromagnetic stability of a selfβgravitating, incompressible, viscous and finitely conducting plasma of variable density. For a uniform and horizontal magnetic field which is present, it is shown that the problem is characterized by a variational principle. Making use of this, proper solutions have been obtained for a semiβinfinite plasma in which the density varies oneβdimensionally (exponentially) along the vertical. The dispersion relation has been solved numerically for the different values of the parameters involved. It is found that the growth rate increases with both the Hall currents and resistivity, showing thereby the destabilizing character of these effects. However, the influence of viscosity is found to be stabilizing as the growth rate decreases with viscosity.
π SIMILAR VOLUMES
The magneto-gravitational instability of an infinite homogeneous, finitely conducting, viscous rotating plasma through porous medium is investignted in view of its relevance to certain stellar atmospheres. The dispersion relation has been obtained from the relevant linearized perturbntion equations
We have studied the effect of rotation on the development of Ragleigh-Taylor instability of an incompressible, viscous, Hall, finitely conducting plasma of variable density. The solution is developed, through variational methods, for n semi-infinite pliisma in which the density varies exponentially
The self-gravitational instability of an infinite homogeneous magnetised and finitely conducting gas-particle medium is considered to include the finite Larmor radius effect in the presence of suspended particles. The equations of the problem are linearized and from linearized equations a general di