The Boltzmann collision integral, also called the Boltzmann collision operator, gives the change caused by binary elastic collisions in a nonnegative function
that describes particle density over velocity space.
For particles of equal mass, one common form is
Here
lies on the unit sphere, and the pairs of velocities
and
are related by
and
. The nonnegative function
weights collisions according to their relative velocity
and scattering direction. The first product in the integrand accounts for particles entering velocity
,
while the second product accounts for particles leaving
it.