We report experimental tests of the present models of the peak effect in we
akly disordered type-II superconductors. Our results favour the scenario in
which the peak effect arises from a crossover between the Larkin pinning l
ength and a rapidly falling elastic length in a Vortex phase populated with
thermally excited topological defects. A thickness dependence study of the
onset of the peak effect at varying driving currents suggests that both sc
rew and edge dislocations are involved in the vortex lattice disordering. T
he driven dynamics in three-dimensional samples are drastically different f
rom those in two-dimensional samples. We suggest that this may be a consequ
ence of the absence of a Peierls potential for screw dislocations in a thre
e-dimensional vortex line lattice.