Quantum Mechanics and the Hydrogen Atom

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SUMMARY

The expectation value of the potential energy for an electron in a 1s orbital of a hydrogen atom is calculated using the potential energy operator V = -e²/(4πε₀r) and the wave function ψ = √(1/πa₀³)e^(-r/a₀). The integral for the expectation value is evaluated over the specified limits, resulting in = -e²/(4πε₀a₀), which is half of the ground state energy as per the virial theorem. This calculation demonstrates the application of quantum mechanics principles to atomic structure.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically wave functions and operators.
  • Familiarity with the hydrogen atom model and its 1s orbital characteristics.
  • Knowledge of integral calculus, particularly in three dimensions.
  • Experience with the virial theorem and its implications in quantum systems.
NEXT STEPS
  • Study the derivation of the Schrödinger equation for hydrogen-like atoms.
  • Explore the implications of the virial theorem in quantum mechanics.
  • Learn about the normalization of wave functions in quantum systems.
  • Investigate the significance of expectation values in quantum mechanics.
USEFUL FOR

Students and professionals in physics, particularly those focusing on quantum mechanics, atomic physics, and anyone interested in the mathematical foundations of the hydrogen atom model.

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Calculate the expectation value of the potential energy for an electron in a 1s orbital for a hydrogen atom





Ive determined the potential energy operator to be V=-e2/4∏ε0r
and a wave function of

ψ= (1/4∏)1/2

therefore i get
<V> = ∫∫∫ψ*Vψr2sin∅drd∅dphi
integrals from 0 to r, 0 to pi, 0 to 2pi


not sure where to go from here.
 
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Nevermind, i got it.

but if anyone is interested ill explain.

For a 1s orbital of a hydrogen the wavefunction is ψ=root(1/∏ao3 e-r/ao)

this gives
∫∫∫ψVψr2sinθdrdθd∅
integrals are zero to 2pi, zero to pi, and zero to infinity.

then factor out any terms that are not a function of r,θ, or∅.
This gives several terms outside of the integral: ∫∫∫e-2r/aorsinθdrdθd∅

then you can separate the integrals and evaluate. they were pretty easy to do.

the final answer was <v> = -e2/4∏εoao
 
You can use the virial theorem. The expectation value you're looking for is then half the ground state energy.
 

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