An analytical method within the frame of linear stability theory is present
ed for the normal field instability in magnetic fluids. It allows us to cal
culate the maximal growth rate and the corresponding wave number for any co
mbination of thickness and viscosity of the fluid. Applying this method to
magnetic fluids of finite depth, these results are quantitatively compared
to the wave number of the transient pattern observed experimentally after a
jumplike increase of the field. The wave number grows linearly with increa
sing induction where the theoretical and the experimental data agree well.
Thereby, a long-standing controversy about the behavior of the wave number
above the critical magnetic held is tackled.