We consider a superconducting film supplied with a magnetic dot array. The
dot magnetization is random and oriented, perpendicular to the film. The co
ncentration of the superconducting vortices bound to the dots is a step-lik
e function of the dot magnetic flux. The concentration of the unbound vorti
ces is an oscillating function of the same variable. The resistivity is det
ermined by the thermal drift of the vortices through the corner points of a
checker-board formed by positive and negative unbound vortices.