Starting from a covariant cycle-averaged Lagrangian the relativistic o
scillation center equation of motion of a point charge is deduced, and
analytical formulas for the ponderomotive force in a traveling wave o
f arbitrary strength are presented. It is further shown that the ponde
rmotive forces for transverse and longitudinal waves are different; in
the latter, uphill acceleration can occur. In a standing wave there e
xists a threshold intensity above which, owing to transition to chaos,
the secular motion can no longer be described by a regular ponderomot
ive force.