Abstract
The total cross section for the collision of an atom and a diatomic molecule (rigid rotor) initially in rotational state (Ja, Ma) is computed to first order in the anisotropic part of the potential. The dependence of the cross section on the quantum number Ma is examined, and it is seen that the anisotropy of the long‐range attractive part of the potential can be determined from the Ma dependence of the average (average over glory oscillations) cross section, whereas the anisotropy of the short‐range repulsive part of the potential can be determined from the Ma dependence of the glory oscillations.