We have studied the unsteady spreading of a liquid on a solid surface by ob
serving the liquid-air meniscus shape and analyzing it with the hydrodynami
c theory for Stokes' flow. The unsteady spreading process exhibits both qua
si-steady and unsteady regimes. The unsteadiness in our moderately high vis
cosity system arises from temporal relaxation of the contact angle rather t
han inertial effects or momentum diffusion. The quasi-steady regime can be
accurately described by a model that ascribes a steady-state flow near the
contact line. "Spontaneous" spreading, i.e., spreading to final state of ze
ro contact line speed, is recognized as a special case of the general unste
ady spreading process with the commonly used power laws for spreading occur
ring only under special conditions.