The expectation value for the radial part of the wavefunction of Hydrogen.

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SUMMARY

The expectation value for the radial part of the wavefunction of hydrogen is calculated by integrating the square of the wavefunction multiplied by r cubed, with r ranging from 0 to infinity. The additional factor of r squared arises from the spherical volume element, dV = r^2 sin(θ) dr dθ dφ. The factor of 4π is normalized away by the spherical harmonics, as the integration over the entire spherical shell results in a value of 1. This normalization is crucial for accurately determining the expectation value.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically wavefunctions
  • Familiarity with spherical coordinates and their application in integration
  • Knowledge of spherical harmonics and their normalization
  • Basic calculus skills, particularly in performing integrals
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  • Study the derivation of the hydrogen wavefunction, focusing on R_{nl}(r) and Y_{lm}(θ, φ)
  • Learn about spherical coordinates and their volume elements in detail
  • Explore the normalization of spherical harmonics and its implications in quantum mechanics
  • Practice calculating expectation values for other quantum systems
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mjordan2nd
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The wavefunction of hydrogen is given by

<br /> <br /> \psi_{nlm}(r, \theta, \phi) = R_{nl}(r)Y_{lm}(\theta, \phi)<br />

If I am only given the radial part, and asked to find the expectation value of the radial part I integrate the square of the wavefunction multiplied by r cubed allowing r to range from 0 to infinity. I don't understand where the extra factor of r squared comes from? I suspect it has something to do with multiplying by a volume element, but it is unclear to me why the factor of 4 pi that would normally come with spherical integration that depends on r alone disappears. I missed this on a test, recently, and was hoping someone could explain.

Thanks.
 
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You're integrating in spherical coordinates so the volume element is dV=r^2sin\theta dr d\theta d\phi
 
Last edited:
The 4pi is normalized away by the spherical harmonics. You essentially already integrated over a spherical shell, and over that entire spherical shell, you should get the integral to be 1.
 

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