The general trends exhibited in the variation of the inelastic form factor
in collisional transitions nl --> n'l', when l' is changed and n, l, and n'
are kept fixed, are explained solely in terms of classical mechanics. Prev
ious quantal results are reproduced from purely classical mechanics princip
les. Our conclusions are valid not only for large quantum numbers (which pr
ovide the usual classical correspondence) but also for other cases, which,
up to now have been described only by quantal or semiclassical methods. The
interesting trends exhibited in the form factor are directly reflected in
experimental and theoretical treatments of collisions involving excited ato
ms.