Deep-MOND polytropes

From WebRef.org
Jump to navigationJump to searchFrameist Custom Picture Frames

Mordehai Milgrom

Working in the deep-MOND limit (DML), I describe spherical, self-gravitating polytropes (equation of state P=Kργ), which can serve as heuristic models for astronomical systems, such as dwarf spheroidal galaxies, low-surface-density elliptical galaxies and star clusters, and diffuse galaxy groups. They can also serve as testing ground for various theoretical MOND inferences. In dimensionless form, the equation satisfied by the radial density profile ζ(y) is (for γ>1) [∫y0ζy¯2dy¯]1/2=−yd(ζγ−1)/dy. Or, θn(y)=y−2[(yθ′)2]′, where θ=ζγ−1, and n≡(γ−1)−1. I discuss general properties of the solutions, contrasting them with those of their Newtonian analogues -- the Lane-Emden polytropes. Due to the stronger MOND gravity, all DML polytropes have a finite mass, and for n<∞ (γ>1) all have a finite radius. (Lane-Emden spheres have a finite mass only for n≤5.) I use the DML polytropes to study DML scaling relations. For example, they satisfy a universal relation (for all K and γ) between the total mass, M, and the mass-average velocity dispersion σ: MGa0=(9/4)σ4. However, the relation between M and other measures of the velocity dispersion, such as the central, projected one, σ¯, does depend on n (but not K), defining a `fundamental surface' in the [M, σ¯, n] space. Another DML relation that the polytropes can model is that between the baryonic and the dynamical central surface densities. I also describe the generalization to anisotropic polytropes, which also all have a finite radius (for γ>1), and all satisfy the above universal M−σ relation.

https://arxiv.org/abs/2012.11412


Sponsor: Rexing W1 Multimedia Receiver

Auto Europe Car Rentals