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 iner
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.