We derive an equation of motion for the dynamics of a ferromagnetic do
main wall driven by an external magnetic field through a disordered me
dium, and we study the associated depinning transition. The long-range
dipolar interactions set the upper critical dimension to be d(c) = 3,
so we suggest that mean-field exponents describe the Barkhausen effec
t for three-dimensional soft ferromagnetic materials. We analyze the s
caling of the Barkhausen jumps as a function of the field driving rate
and the intensity of the demagnetizing field, and find results in qua
ntitative agreement with experiments on crystalline and amorphous soft
ferromagnetic alloys.