The age-old problem of the derivation of a proper formula for the mechanica
l (or electrical) mobility of large, heavy (l.h.) particles in a simple neu
tral gas in any regime is carefully examined and solved under the usual hyp
otheses that the l.h. particles are subject to the action of a constant ext
ernal force and undergo only elastic collisions with the gas particles. By
a convenient procedure, a general mobility formula is obtained which not on
ly properly corrects the well-known result derived by Cunningham for an l.h
. hard sphere in a hard-sphere gas, but also applies to the general case in
which both the l.h.-particle-gas-particle and gas-particle-gas-particle in
teractions are arbitrary. In addition, on the basis of the new formula, the
fair success of the Cunningham formula (regarded as a semiempirical formul
a) in fitting the experimental results is explained. Other interesting aspe
cts of the new formula are also examined, and its limits of validity are br
iefly discussed. (C) 2000 Elsevier Science B.V. All rights reserved.