Can someone provide some references on spherical wave analysis in spherical magnetized gravitating fluids?
Spherical waves are ubiquitous in astrophysical environments. Can someone provide some useful references on spherical wave analysis in spherical gravito-magnetized fluids?
NASA Goddard Space Flight Center, Greenbelt, MD, United States
What kind of system are you examining? Have you looked into how the magnetic field is treated in the solar corona and the solar p-modes? We investigated magnetic fields in white dwarf stars https://ui.adsabs.harvard.edu/#abs/1989ApJ...336..403J/abstract and much literature is devoted to the interaction of nonracial oscillations and magnetic fields in stars.
Thanks, anyway. I am rather interested in spherical wave analyses with and without approximations. The physical model may spherical stars, dust molecular clouds, etc.
NASA Goddard Space Flight Center, Greenbelt, MD, United States
The only approximation we make is linear wave theory. The system is very important. Waves inside stars tend to adiabatic because the material is optically thick. Waves in optically thin matter, such as the solar corona, have different characteristics. Waves in interstellar dust clouds aren't spherical when the cloud isn't self-gravitating. Although spherically symmetric waves were the first variable stars to be observed (radial oscillators such as Cepheids, RR Lyrae stars, and Mira stars), nonradial oscillations are far more common throughout the H-R diagram. Nonlinear calculations of Cepheids and RR Lyrae stars are easy to find in the literature (Christy and Cox are among the authors.)
NASA Goddard Space Flight Center, Greenbelt, MD, United States
J. P. Cox, Theory of Stellar Oscillations, is a good place to start. It's a little old but thorough in theory and observations. Additional references are difficult to provide without knowing your application. Cox is good for stars, but other systems have different approaches.
"If the bodies in question have spatial extent (rather than being theoretical point masses), then the gravitational force between them is calculated by summing the contributions of the notional point masses which constitute the bodies. In the limit, as the component point masses become "infinitely small", this entails integrating the force (in vector form, see below) over the extents of the two bodies.
"In this way it can be shown that an object with a spherically-symmetric distribution of mass exerts the same gravitational attraction on external bodies as if all the object's mass were concentrated at a point at its centre. (This is not generally true for non-spherically-symmetrical bodies.)"
This would seem to indicate that solutions to a representative distribution of point masses should be obtained, then combined by vector summation to determine a more representative result. This may be necessary because the inverse-square force contributed by millions of discrete masses, each with individual separation distances much less than the subject's radial distance from the galactic center, would exceed the force estimation using a single separation distance term.
It is shown that the assumed consistency equation of the self-consistent theory of spinning fluid puts severe restrictions on the fluid configurations. If one drops the consistency equation, the spin kinetic energy gives rise to some novel effects similar to that of an imperfect fluid. Following the analogy of the imperfect fluid the authors descri...
We study the longitudinal instabilities of two interpenetrating fluids interacting only through gravity. When one of the constituents is of relatively low density, it is possible to have a band of unstable wavenumbers well separated from those involved in the usual Jeans instability. If the initial streaming is large enough, and there is no linear...
We generalize the Raychaudhuri equation for the evolution of a self gravitating fluid to include an Abelian and non-Abelian hybrid magneto fluid at a finite temperature. The aim is to utilize this equation for investigating the dynamics of astrophysical high temperature Abelian and non-Abelian plasmas.