The model used for the galaxy cluster is the King model
(King 1966; Padmanabhan 2002), which was chosen because
it possesses a finite radial cut-off, and is therefore a well
defined problem for a code comparison. Its form is based on
the distribution function:
where &epsilon = &Psi - 1/2 v
2, is the coordinate change for the shifted
energy, &rho
c is the central density and &sigma is related to (but
not equal to) the velocity dispersion. The resulting density
distribution of this cluster vanishes at the tidal radius, r
t.Integrating over all velocities yields a density distribution:
Putting this into the Poisson equation results in a second order
ODE which can be solved numerically. A c code that does this can be found
[here]. This model has three independent parameters, the mass of the cluster, the
tidal radius and the concentration c = log
10(rt/r0), where
r
0 is the central or King radius. For this problem, we selected
a concentration of 3, r
t = 1Mpc and a cluster mass
of 1014 M
solar. This results in a King radius of 1 kpc. Therefore,
to successfully maintain hydrostatic equilibrium, the codes
must be able to model the cluster out to 1Mpc while resolving
the 1 kpc core. The profile of the cluster is analyzed at t = 1 Gyr.