Three Dimensional Virial Theorem for the Hydrogen Atom | Quantum Science Philippines
Quantum Science Philippines

Three Dimensional Virial Theorem for the Hydrogen Atom

Catherine Therese J. Quiñones

The virial theorem is a general theorem relating the potential energy (V) and the kinetic energy (KE) in a bound system.  A simple physical example is a small object orbiting around another object  bound by a force. The virial theorem states that the potential energy is twice the kinetic energy thus,

<V>=2<T>                                                                                                                  (1)

Here, we will derive the expectation value of  1/r in the unperturbed state of the of a hydrogen atom. We can use the virial theorem to easily solve the expectation value since the system can be considered a bound system with the electron orbiting around the proton bound by the Coulombic force. Hence, the potential energy is

V=-\frac{e^2}{4\pi\epsilon_0}\frac{1}{r}                                                                                                                      (2)

where e is the charge of the electron and the proton, r represents the separation distance between the two charges and \epsilon_0 is the permittivity of free space . The negative sign indicates that the force is attractive. The total energy is given by

E_n = - \Big[\frac{m}{2\hbar^2}\Big(\frac{e^2}{4\pi\epsilon_0}\Big)^2\Big]\frac{1}{n^2}                                                                                                 (3)

where m is the mass of the particle, \hbar is Planck’s constant over 2\pi and n= 0,1,2,3,.. which indicates the quantization of the energy level. The solution is very straight forward. All we need is to plug in eqn (2) and (3) to eqn (1).  Hence,

<V>= 2E_n                                                                                                                       (4)

-\frac{e^2}{4\pi\epsilon_0}<\frac{1}{r}> = -2\Big[ \frac{m}{2\hbar^2}\Big(\frac{e^2}{4\pi\epsilon_0}\Big)^2\Big] \frac{1}{n^2}                                                                                                                                             (5)

<\frac{1}{r}>=\Big(\frac{me^2}{4\pi\epsilon_0\hbar^2}\Big)\frac{1}{n^2}                                                                                                          (6)

Note that the term inside the parenthesis is just \frac{1}{a_0}, where a_0 is the Bohr radius . Hence we can write the expectation value of 1/r as,

<\frac{1}{r}> = \frac{1}{a_0n^2}                                                                                                                        (7)

Thus we have derived the expectation value, <\frac{1}{r}>, of the hydrogen atom in the unperturbed state using the virial theorem.

Share and Enjoy: These icons link to social bookmarking sites where readers can share and discover new web pages.
  • bodytext
  • del.icio.us
  • Facebook
  • NewsVine
  • Reddit
  • StumbleUpon
  • Google
  • YahooBuzz
  • Twitter
  • Technorati
  • Live
  • LinkedIn
  • MySpace
  • Blogosphere News
  • Bumpzee
  • Sphinn
  • E-mail this story to a friend!
  • Ma.gnolia

2 Responses to “Three Dimensional Virial Theorem for the Hydrogen Atom”

  1. Gekko Says:

    In Eq (3), isn’t this the *total* energy (kinetic + potential) of an electron in the n-th energy level? It is negative, which doesn’t to make sense for a kinetic energy…

  2. admin Says:

    Gekko, definitely you’re right. Kinetic energy is definitely positive. Equation (3) actually refers to the total energy and this post has been updated accordingly.
    Thanks for pointing this out!

Leave a Reply