I'm currently trying to solve a problem that involves estimating the minimum energy of a particle in the potential:
$$ V(x) = \frac{-V_0a}{|{x}|} $$
I'm quite confused about how to handle the absolute value in the potential. So far I know that the total energy of the particle will be
$$ E = \frac{p^2}{2m} - \frac{V_0a}{|{x}|} $$
The expectation value of the energy is therefore
$$ \langle E\rangle = \frac{\langle p^2\rangle}{2m} - \frac{V_0a}{\langle|{x}|\rangle} $$
Now, can I use the fact that $$\frac{1}{|x|}=\frac{1}{\sqrt{x^2}}$$ and then $\langle|x|\rangle = \sqrt{\langle x^2\rangle} = \Delta x$? Then from the uncertainty principle we know that $\Delta p = \hbar/2\Delta x$ and $\Delta p^2 = \langle p^2\rangle$ ($\langle p\rangle = 0$ and $\langle x\rangle$ = 0 in a minimum energy state)
Plugging this back into the energy equation gives $$ \langle E\rangle = \frac{\hbar^2}{8m\Delta x^2} - \frac{V_0a}{\Delta x} $$
When minimising this I get
$$ E_{min} = \frac{-2mV_0^2a^2}{\hbar^2} $$
Now this doesn't look wildly wrong but I'm not sure if I've used the right approach with $\langle|x|\rangle = \sqrt{\langle x^2\rangle} = \Delta x$.