The Plummer 3-dimensional density profile is given by
where is the total mass of the cluster, and a is the Plummer radius, a scale parameter that sets the size of the cluster core. The corresponding potential is
where G is Newton's gravitational constant. The velocity dispersion is
The isotropic distribution function reads
if , and otherwise, where is the specific energy.
The 2D surface density is:
and hence the 2D projected mass profile is:
In astronomy, it is convenient to define 2D half-mass radius which is the radius where the 2D projected mass profile is half of the total mass: .
For the Plummer profile: .
The escape velocity at any point is
For bound orbits, the radial turning points of the orbit is characterized by specific energy and specific angular momentum are given by the positive roots of the cubic equation
where , so that . This equation has three real roots for : two positive and one negative, given that , where is the specific angular momentum for a circular orbit for the same energy. Here can be calculated from single real root of the discriminant of the cubic equation, which is itself another cubic equation
where underlined parameters are dimensionless in Henon units defined as , , and .
The Plummer model comes closest to representing the observed density profiles of star clusters[citation needed], although the rapid falloff of the density at large radii () is not a good description of these systems.
The behavior of the density near the center does not match observations of elliptical galaxies, which typically exhibit a diverging central density.
The ease with which the Plummer sphere can be realized as a Monte-Carlo model has made it a favorite choice of N-body experimenters, in spite of the model's lack of realism.[3]