Strongly disordered ferromagnetic alloys which exhibit magnetic inhomo
geneities are described in the frame of the Ginzburg-Landau theory by
introducing local, spatially varying Curie temperatures. It is shown t
hat this leads to a smooth phase transition. Furthermore it is shown t
hat the maxima and minima of the specific heat, the volume thermal exp
ansion coefficient and of the compressibility deviate from the Curie t
emperature.