We investigate the magnetotransport behavior of ferromagnet ͑F͒/superconductor/ferromagnet trilayers made of ferromagnetic Ni 80 Fe 20 ͑Permalloy, Py͒ and superconducting Nb for temperatures both above and below the superconducting transition temperature T c . In such devices, and for weak ferromagnets, T c depends on the relative magnetization directions of the two F layers in such a way that T c P of the parallel ͑P͒ alignment is lower than T c AP of the antiparallel ͑AP͒ alignment ͑the so-called superconducting spin-valve effect͒. For strong magnets, the suppression of Andreev reflection may alter this picture, but also stray field effects become important, as is known from earlier work. We compare large-area samples with microstructured ones, and find blocklike switching in the latter. We show this not to be due to a switch between the P and AP states, but rather to dipolar coupling between domains which are forming in the two Py layers, making a stray-field scenario likely. We also present measurements of the depairing ͑critical͒ current I dp and show that a similar depression of superconductivity exists far below T c as is found around T c .