Chapter 38: Problem 58
What is the energy of a transition capable of producing light of wavelength \(10.6 \mu \mathrm{m} ?\) (This is the wavelength of light associated with a commonly available infrared laser.)
Chapter 38: Problem 58
What is the energy of a transition capable of producing light of wavelength \(10.6 \mu \mathrm{m} ?\) (This is the wavelength of light associated with a commonly available infrared laser.)
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Get started for freeWhich model of the hydrogen atom-the Bohr model or the quantum mechanical model-predicts that the electron spends more time near the nucleus?
A muon is a particle very similar to an electron. It has the same charge but its mass is \(1.88 \cdot 10^{-28} \mathrm{~kg}\). a) Calculate the reduced mass for a hydrogen-like muonic atom consisting of a single proton and a muon. b) Calculate the ionization energy for such an atom, assuming that the muon is initially in its ground state.
The hydrogen atom wave function \(\psi_{200}\) is zero when \(r=2 a_{0}\). Does this mean that the electron in that state can never be observed at a distance of \(2 a_{0}\) from the nucleus or that the electron can never be observed passing through the spherical surface defined by \(r=2 a_{0} ?\) Is there a difference between those two descriptions?
What are the largest and smallest possible values for the angular momentum \(L\) of an electron in the \(n=5\) shell?
An electron in a hydrogen atom is in the ground state (1s). Calculate the probability of finding the electron within a Bohr radius \(\left(a_{0}=0.05295 \mathrm{nm}\right)\) of the proton. The ground-state wave function for hydrogen is $$ \psi_{1 s}(r)=A_{1 s} e^{-r / a_{0}}=e^{-r / a_{0}} / \sqrt{\pi a_{0}^{3}} $$
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