The quantum mechanical operator for this quantity 
The quantum mechanical operator for this quantity is negative h-bar divided by twice the mass times the Laplacian, and the virial theorem calculates the total amount of this quantity for a system of particles. By the equipartition theorem, it is equal to three halves Boltzmann constant times temperature. This quantity's rotational analogue is proportional to moment of inertia times angular (*) velocity squared, and the change in this quantity is equal to the total work. Its linear form is equal to one-half mass times velocity squared. For ten points, identify this energy of objects in motion.
The quantum mechanical operator for this quantity is negative h-bar divided by twice the mass times the Laplacian, and the virial theorem calculates the total amount of this quantity for a system of particles.