Equations describing the intergrain flux creep of ceramic superconduct
ors are derived. They are based on the behavior of small superconducti
ng loops closed by overdamped Josephson junctions. The elementary loop
s are formed around nonsuperconducting regions between the grains, the
loops acting as pinning centers. Despite different pinning mechanisms
the equations for the relaxation of the intergrain current density in
a static and a slowly varying external magnetic field are formally si
milar to those of the classical flux-creep theory based on volume pinn
ing.