## Estimating the Size of the Hydrogen Atom (i.e., Bohr's Radius) using Equipartition

*estimate*of the hydrogen atom.

One method which we don't follow here, is to estimate the size of the atom using

*dimensional analysis*. Instead, we shall do so using the principle of

*equipartition*.

The potential energy of a single electron is given by:

$$ U \approx - {e^2 \over a_0} $$ $a_0$ is Bohr’s radius which we are seeking.

On the other hand, one can place a limit on the kinetic energy using the uncertainty principle. The latter is: $$ \Delta p \Delta x \approx \hbar $$ Thus, the typical momentum that the electron will have, will be roughly $$ p \sim {\hbar \over \Delta x}. $$ The total energy is therefore $$ E_{total} = U + E_{kin} = U + {p^2 \over 2 m} \sim -{e^2 \over a_0} + {\hbar^2 \over a_0^2 m_e}. $$ The system will seek a minimum energy. So, in principle we can differentiate this expression with respect to $a_0$ to find the minimum. However, this is pointless because the expression itself is not accurate. Instead, we can ask the question when will the two terms be comparable. This is permissible because the terms do not have any typical length scale to them other than $a_0$, such that $dA/dx \sim A / a_0$. Thus, by comparing the terms we find: $$ {e^2 \over a_0} \sim {\hbar^2 \over a_0^2 m_e} ~~\Rightarrow~~ a_0 \sim {\hbar^2 \over m_e e^2}. $$ Fools are lucky. It turns out that this expression is not just approximate, but it actually has the correct prefactor. Another interesting point, we can write this expression as: $$ a_0 = {\alpha \lambda_e \over 2 \pi} $$ with $\alpha = e^2 / \hbar c$ being the fine structure constant, while $\lambda_e = h/mc$ is the Compton wavelength of the electron.

Using this result for $a_0$, we can calculate the energy associated with Bohr's radius, which is the Rydberg energy. We do so by plugging in the $a_0$ we have found to either $U$ or $E_{kin}$ (note that the two terms were assumed to be the same at $a_0$ !). Plugging into $U$ gives $$ E_1 \sim {e^2 \over a_0} \sim {m_e e^4 \over \hbar^2}. $$ where $E_1$ is the energy of the lowest state (i.e., 1 Rydberg).

We can immediately also find out how the result will change if we consider a high-Z hydrogen like atom (e.g., the radius of Fe ionized 25 times, leaving just one electron), or if we consider a positronum.

In the first case of a high-Z hydrogen like atom, all we have to realize is that here the potential energy has $Z e^2$ in it instead of $e^2$. By make this transformation, that $e^2 \rightarrow Z e^2$, we can therefore deduce that

$$ a_Z = { a_0\over Z}, ~~\mathrm{and}~~ E_Z = {E_1 Z^2}. $$ Similarly, if we consider a positronium (which is a positron-electron pair orbiting each other), all we have to do is remember our classical mechanics. The relevant quantity in a two body problem is not the mass, but instead the reduced mass $\mu = m_1 m_2 / (m_1 + m_2)$. For the positron+electron case, one has $\mu = m_e/2$. Hence, the radius of the lowest orbit of a positronium is obtained by $m_e \rightarrow m_e/2$, giving that $$ a_{ee} ={ 2 a_0}, ~~\mathrm{and}~~ E_{ee} = {E_1 \over 2}. $$ Clearly, equipartition can be a very useful tool to derive the approximate properties of atoms, and perhaps more impressively, derive how those properties scale between different systems.

View the discussion thread.