The magnetic and mechanical finite element systems are combined into one ma
gnetomechanical system. Investigating the coupling terms results in a finit
e element expression ibr the magnetic forces (Lorentz force and reluctance
force) for both the linear and nonlinear case. The material deformation cau
sed by magnetostriction is represented by an equivalent set of mechanical f
orces, giving the same strain to the material as magnetostriction does. The
resulting magnetostriction force distribution is superposed onto other for
ce distributions (external mechanical forces, magnetic forces) before start
ing the mechanical deformation or vibration analysis. This procedure is inc
orporated into a weakly-coupled cascade solving of the magnetomechanical pr
oblem.