When this quantity is known about the center of mass, the parallel axis theorem gives this quantity for different axes. This quantity for a solid sphere has a coefficient of two-fifths. It is equal to torque over angular acceleration, and for a point mass, it is equal to mass times the square of the (*) distance from the axis of rotation. For 10 points, name this rotational analogue of mass that indicates an object's resistance to rotational acceleration.
When this quantity is known about the center of mass, the parallel axis theorem gives this quantity for different axes. This quantity for a solid sphere has a coefficient of two-fifths. It is equal to torque over angular acceleration, and for a point mass, it is equal to mass times the square of the (*) distance from the axis of rotation. For 10 points, name this rotational analogue of mass that indicates an object's resistance to rotational acceleration.
When this quantity is known about the center of mass, the parallel axis theorem gives this quantity for different axes.
moment of inertia (prompt on "I;" do not prompt or accept "inertia")