2. Using the back of the envelope estimate that o,op position and momentum of the electron along the radial direction with respect to the proton in a hydrogen atom, where the proton is considered to be infinitely massive and stationary at the origin: Estimate the ground state energy of the hydrogen atom. Remember that in the ground state, there is no contribution to kinetic energy due to the angular momentum of the electron. = ħ for minimal simultaneous uncertainties in the

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= ħ for minimal simultaneous uncertainties in the
2. Using the back of the envelope estimate that o„0p
position and momentum of the electron along the radial direction with respect to the proton in a hydrogen
atom, where the proton is considered to be infinitely massive and stationary at the origin: Estimate the
ground state energy of the hydrogen atom. Remember that in the ground state, there is no contribution to
kinetic energy due to the angular momentum of the electron.
Transcribed Image Text:= ħ for minimal simultaneous uncertainties in the 2. Using the back of the envelope estimate that o„0p position and momentum of the electron along the radial direction with respect to the proton in a hydrogen atom, where the proton is considered to be infinitely massive and stationary at the origin: Estimate the ground state energy of the hydrogen atom. Remember that in the ground state, there is no contribution to kinetic energy due to the angular momentum of the electron.
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