An elastic body moving in a quenched random force environment with a s
ingular force correlator experiences an additional friction force whic
h is inversely proportional to velocity. This dynamical friction mecha
nism is important, e.g., for a moving interface which is subjected to
quenched random pinning forces. For sufficiently strong pinning forces
, interface motion becomes unstable at values of driving force smaller
than some critical one and the interface velocity drops. We expect in
this case a first-order depinning transition with hysteresis in the d
ependence of the interface velocity on driving force. Instability in t
he interface motion remains under perturbations like an additional per
iodic driving force or thermal fluctuations. Interface motion instabil
ity can also take place in systems with small viscosity, when inertial
effects are important.