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Zoil
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Homework Statement
Specifically, this question is about computing the expectation value of the Hamiltonian of a variational calculation of a hydrogen atom *neglecting the potential term. I'm assuming the trial wavefunction [tex]e^{-\alpha r}[/tex]. The question, however, is purely math based, not quantum mechanical.
I'm having trouble understanding how to properly convert an integral from Cartesian coordinates to spherical coordinates. I know that I must add a factor of [tex]r^2\sin\(\theta\)[/tex] when going from [tex]dxdydz[/tex] to [tex]dr d\theta d\varphi[/tex]. but what if the expression I am integrating has an operator (specifically, [tex]\nabla^2[/tex])? Do I need to account for [tex]r^2\sin\(\theta\)[/tex] when I am taking the derivatives?
Homework Equations
Trial Wavefunction:
[tex]\Psi = e^{-\alpha r}[/tex]
Laplacian in spherical coords:
[tex] \nabla^2 = {1 \over r^2} {\partial \over \partial r} \left( r^2 {\partial \over \partial r} \right) + {1 \over r^2 \sin \varphi} {\partial \over \partial \varphi} \left( \sin \varphi {\partial \over \partial \varphi} \right) + {1 \over r^2 \sin^2 \varphi} {\partial^2 \over \partial \theta^2}[/tex]
The Attempt at a Solution
Here's the equation:
[tex]\langle \psi | H | \psi \rangle [/tex]
and then when I plug in [tex]\psi and \nabla^2[/tex] and the integrals, I get:
[tex]
\frac{i\hbar}{2m} \iiint e^{-\alpha r} \left( \left({1 \over r^2} {\partial \over \partial r} \left( r^2 {\partial \over \partial r} \right) + {1 \over r^2 \sin \varphi} {\partial \over \partial \varphi} \left( \sin \varphi {\partial \over \partial \varphi} \right) + {1 \over r^2 \sin^2 \varphi} {\partial^2 \over \partial \theta^2}\right)+V(r)\right)e^{-\alpha r} r^2 \sin(\theta) \,dr\,d\theta\,d\varphi
[/tex]
Essentially my question boils down to this: Can I neglect the second two terms of [tex] \nabla^2 [/tex] that are nonzero when I convert to spherical coords?
P.S. Sorry if my LaTeX sucks, I just taught myself how to do it for this post.
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