How to Derive the Hydrogen Atom Hamiltonian in Spherical Coordinates?

FloridaGators
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The Hamiltonian for a Hydrogen atom in Cartesian Coordinates (is this right?):
\hat{H} = - \frac{\bar{h}^2}{2m_p}\nabla ^2_p - \frac{\bar{h}^2}{2m_e}\nabla ^2_e - \frac{e^2}{4\pi\epsilon _0r}
In Spherical Coordinates do I just use:
x=r sin θ cos φ, y = r sin θ sin φ, and z = r cos θ?
 
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It is \hbar instead of h. But that is essentially correct. You might want to convert it to the center of mass reference frame before you do any work on it though. There are tons of sites out there that solve it as well and show all the work.
 
FloridaGators said:
The Hamiltonian for a Hydrogen atom in Cartesian Coordinates (is this right?):
\hat{H} = - \frac{h^2}{2m_p}\nabla ^2_p - \frac{h^2}{2m_e}\nabla ^2_e - \frac{e^2}{4\pi\epsilon _0r}

First, this form has no explicit reference to Cartesian coordinates.

Second, this is only correct if you define r to be the separation between the proton and the electron; not the distance from the origin.

In Spherical Coordinates do I just use:
x=r sin θ cos φ, y = r sin θ sin φ, and z = r cos θ?

There are many sites and texts that derive expressions for \nabla^2 in Spherical coordinates.
 
Thank you for helping. Do you mind my asking what your search inquiry in google was to find that?
 
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To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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