Wiedemann effect

The twisting of a ferromagnetic rod through which an electric current is flowing when the rod is placed in a longitudinal magnetic field. It was discovered by the German physicist Gustav Wiedemann in 1858 ^[1] . The Wiedemann effect is one of the manifestations of magnetostriction in a field formed by the combination of a longitudinal magnetic field and a circular magnetic field that is created by an electric current. If the electric current (or the magnetic field) is alternating, the rod will begin torsional oscillation.

In linear approach angle of rod torsion α does not depend on its cross-section form and is defined only by current density and magnetoelastic properties of the rod:^[2]

${\displaystyle \alpha =j{\frac {h_{15}}{2G}}}$,

where

• ${\displaystyle j}$ is current density;
• ${\displaystyle h_{15}}$ is magnetoelastic parameter, proportional to longitudinal magnetic field value;
• ${\displaystyle G}$ is the shear modulus.