The Jeans equations describe the motion of a collection of stars in a gravitational field.
If ν = ν(x,t) is the density of stars in space, as a function of position x = (x1, x2, x3) and time t, v = (v1, v2, v3) is the velocity, and Φ = Φ(x,t) is the gravitational potential, the Jeans equations may be written as
Here, the bar is used to take averages at a given point, so that, for example, is the average of component 1 of the velocity of the stars at a given point. The second set of equations may alternately be written as
where measures the velocity dispersion in components i and j at a given point.
The Jeans equations are analogous to the Euler equations for fluid flow and may be derived from the collisionless Boltzmann equation. They were originally derived by James Clerk Maxwell but were first applied to stellar dynamics by James Jeans.[1][2]