When the rank 2 tensor associated with this quantity is diagonalized, it can be shown that its intermediate eigenvalue leads to instability.
When the rank 2 tensor associated with this quantity is diagonalized, it can be shown that its intermediate eigenvalue leads to instability. Three different forms of this value must necessarily be in descending order for the tennis racket theorem to apply, and those values of this quantity are multiplied by angular velocity in the Euler equations. This quantity remains unchanged for a rigid body that is pulled according to the stretch rule. This quantity is in the numerator in the formula for radius of gyration where it is divided by cross-sectional area. If this value is known at the centre of mass, it can be calculated for any other point by the parallel axis theorem. For 10 points, name this quantity, the rotational analog of mass.
When the rank 2 tensor associated with this quantity is diagonalized, it can be shown that its intermediate eigenvalue leads to instability.
moment of inertia [prompt on \"I\"]