Light-induced drift of optically active atoms in a buffer gas is a conseque
nce of the unequal diffusive frictions suffered by the excited and the grou
nd-state atoms. This drift can be used to create an "optical piston." in wh
ich the active atoms are pushed forward by light through the semipermeable
membrane of the buffer gas. Normally, optical piston effect is studied when
the active atoms are neutral in a confined one-dimensional situation. We p
resent a detailed theory of this phenomenon when the active atoms are charg
ed and a magnetic held is applied for "timing" the direction as well as the
magnitude of the drift. thus removing the necessity of confinement. Our st
udy is in different geometries of the light beam and the magnetic field, fi
rst in the weak collision model. and then for the strong collision and the
Boltzmann-Lorentz models,