One form of this quantity is represented as the cross product of lambda times magnetization and the derivative of magnetization in the Landau- Lifshitz-Gilbert equation. For an electric dipole, this q
One form of this quantity is represented as the cross product of lambda times magnetization and the derivative of magnetization in the Landau- Lifshitz-Gilbert equation. For an electric dipole, this quantity with a "spin- transfer" variety is equal to the cross product of the dipole moment and the electric field, while for a rigid body, this quantity can be maximized by increasing the distance from the pivot point or increasing the tangential component of force. With units of newton-meters, it is the time derivative of angular momentum. For 10 points, name this quantity, the rotational analogue of force.
One form of this quantity is represented as the cross product of lambda times magnetization and the derivative of magnetization in the Landau- Lifshitz-Gilbert equation.
{torque} [or {moment}]