The magnetic material's deformation caused by magnetostriction is represent
ed by an equivalent set of mechanical forces, giving the same deformation t
o the material as magnetostriction does. This is done in a way similar to h
ow thermal stresses are usually incorporated. The resulting magnetostrictio
n force distribution is summed to other force distributions (external mecha
nical forces, magnetic forces) before starting the mechanical deformation o
r vibration analysis. This procedure is incorporated into a weakly coupled
cascade solving of the magnetomechanical problem.