Magnetostriction and its inverse effect in Tb0.3Dy0.7Fe2 alloy

Magnetostriction and its inverse effect (also referred to as a magnetomechanical effect) in the Tb0.3Dy0.7Fe2 alloy have been investigated based on the three dimensional Stoner–Wohlfarth model in this paper. The solutions of direction cosines of magnetization under a compressive stress and a field both applied along the [112] axis have been obtained by following a conventional minimization procedure in which the nonlinear equations for equilibrium conditions have been solved numerically. With a more accurate computation presented here, some new theoretical results have been achieved. These results are in good agreement with experimental observations reported previously. In the demagnetized state the resultant anisotropy for the alloy is determined by the combination of the magnetocrystalline and stress-induced anisotropy energies, and degenerates from cubic into uniaxial at a critical stress. When a field is applied to the alloy along the [112] axis, the alloy under the compressive stress is more difficult to magnetize and can attain a maximum change in bulk magnetostriction at the critical stress. The main reason for the large bulk magnetostriction is that the fractional occupancy of the [1¯1¯1] or [111¯]-oriented domains increases from 1/8 to 1/2 with the stress. This more accurate computation has been proposed for similar investigations and the results will also be helpful for a better understanding of the magnetostriction in materials such as the FeGa alloys.