# Virial theorem

In mechanics, a **virial** of a stable system of *n* particles is a quantity proposed by Rudolf Clausius in 1870.^{[1]}
The virial (from the Latin *vis*, force) is defined by

where **F**_{i} is the total force acting on the *i* th particle and **r**_{i} is the position of the *i* th particle; the dot stands for an inner product between the two 3-vectors. Indicate long-time averages by angular brackets. The importance of the virial arises from the **virial theorem**, which connects the long-time average of the virial to the long-time average 〈 *T* 〉 of the total kinetic energy *T* of the *n*-particle system,^{[2]}

## Proof of the virial theorem

Consider the quantity *G* defined by

The vector **p**_{i} is the momentum of particle *i*. Differentiate *G* with respect to time:

Use Newtons's second law and the definition of kinetic energy:

and it follows that

Averaging over time gives:

If the system is stable, *G*(*t*) at time *t* = 0 and at time *t* = *T* is finite. Hence, if *T* goes to infinity, the quantity on the right hand side, being divided by infinite *T*, goes to zero. Alternatively, if the system is periodic with period *T*, *G*(*T*) = *G*(0) and the right hand side will also vanish. Whatever the cause, we assume that the time average of the time derivative of *G* is zero, and hence

which proves the virial theorem.

## Application

An interesting application arises when the potential *V* is of the form

where *a*_{i} is some constant (independent of space and time).

An example of such potential is given by Hooke's law with *k* = 2 and Coulomb's law with *k* = −1.
The force derived from a potential is

Consider

Hence

Then applying this for *i* = 1, … *n*,

For instance, for a system of charged particles interacting through a Coulomb interaction:

## Quantum mechanics

The virial theorem holds also in quantum mechanics. Quantum mechanically the angular brackets do not indicate a time-average, but an expectation value with respect to an exact stationary eigenstate of the Hamiltonian of the system. First the theorem will be proved and then it is applied to the special case of a potential that has a *r*^{k}-like dependence. Everywhere Planck's constant ℏ is taken to be one.

Let us consider a *n*-particle Hamiltonian of the form

where *m*_{j} is the mass of the *j*-th particle. The momentum operator is

Using the self-adjointness of *H* and the definition of a commutator one has for an arbitrary operator *G*,

In order to obtain the virial theorem, we consider

Use

Define

Use

and we find

The quantum mechanical virial theorem follows

where 〈 … 〉 stands for an expectation value with respect to the exact eigenfunction Ψ of *H*.

If *V* is of the form

it follows that

From this:

For instance, for a stable atom (consisting of charged particles with Coulomb interaction): *k* = −1, and hence 2〈*T* 〉 = −〈*V* 〉.

## Reference

- ↑ R. Clausius,
*On a Mechanical Theorem applicable to Heat*, The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, vol.**40**, 4th series, pp. 122 – 127 (1870). Google books. Note that Clausius still uses the term*vis viva*for kinetic energy, but does include the factor ½ in its definition, following Coriolis. - ↑ Clausius states this result as:
*the mean vis viva of the system is equal to its virial.*