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Virial Theorem


The virial theorem relates time-averaged kinetic energy to the forces in a mechanical system. For particles with positions r_i, momenta p_i=m_ir^._i, and differentiable potential energy V(r_1,...,r_n), define D=sum_(i)r_i·p_i and T=1/2sum_(i)m_i||r^._i||^2. Newton's equations give

 D^.=2T-sum_(i)r_i·del _iV.
(1)

If the time averages exist and [D(tau)-D(0)]/tau->0 as tau->infty, then

 2<T>=<sum_(i)r_i·del _iV>,
(2)

where <f>=lim_(tau->infty)tau^(-1)int_0^tauf(t)dt denotes a time average. Bounded D is a sufficient condition for the boundary term to vanish (Fowler).

If V is a homogeneous function of degree k, so that V(lambdar_1,...,lambdar_n)=lambda^kV(r_1,...,r_n) for lambda>0, differentiating with respect to lambda gives sum_(i)r_i·del _iV=kV. Consequently,

 2<T>=k<V>.
(3)

For Newtonian gravitational attraction, k=-1 and 2<T>+<V>=0. For a quadratic potential, k=2 and the time-averaged kinetic and potential energies are equal. These conclusions require the averaging and boundary-term hypotheses; they do not apply to an arbitrary instantaneous state.


See also

Hamiltonian System, Homogeneous Function, n-Body Problem

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References

Fowler, M. "Mechanical Similarity and the Virial Theorem." University of Virginia. https://galileoandeinstein.phys.virginia.edu/7010/CM_05_MechSim.html.

Cite this as:

Weisstein, Eric W. "Virial Theorem." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/VirialTheorem.html

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