I am working through an explanation of the wave function of the Hydrogen atom.(adsbygoogle = window.adsbygoogle || []).push({});

I have got as far as deriving the version of Schrodinger's equation for the one-dimensional problem in which only the radial coordinate can vary:

##[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial^2 r}+\frac{\hbar^2 l (l+1)}{2mr^2}+V(r)]U_{El}(r)=EU_{El}(r)##

It is assumed that ##V(r)=-\frac{e^2}{r}##.

The presentation I am working through says:

'Find the asymptotic behavior of ##U_{El}(r)## as ##r\rightarrow 0##......

Solution: At ##r\rightarrow 0##, the first and second terms in the Hamiltonian will dominate, so [the above equation] becomes:

##\frac{\partial^2}{\partial^2 r}U_{El}(r)=\frac{l(l+1)}{r^2}EU_{El}(r)##'

I don't see why this follows. Certainly the second term in the square brackets will dominate the third term, which is only divided by ##r##, not ##r^2##, and the right-hand side of the equation, but why would it not also dominate the first term, which is not divided by ##r## at all?

Is it possible to derive the second equation above in a more convincing way?

Thank you.

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# Asymptotic properties of Hydrogen atom wave function

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