A single electron of mass and charge orbits a fixed nucleus of charge

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Atomic, Molecular & Optical Physics · Origins of quantum theory

Quantum Mechanics: From the Photon to the Hydrogen Atom, Ch Line spectra, the Bohr atom and the old quantum theory

Problem

A single electron of mass mem_e and charge −e-e orbits a fixed nucleus of charge +Ze+Ze, the only force being the Coulomb attraction Ze2/4πϵ0r2Ze^2/4\pi\epsilon_0r^2. Bohr's rule is mevr=nℏm_evr = n\hbar, and light is emitted only in a jump with hν=En2−En1h\nu = E_{n_2} - E_{n_1}. Write ∣E1H∣=13.6|E_1^{\mathrm H}| = 13.6 eV for hydrogen's ground-state binding energy, and take h=6.626×10−34h = 6.626\times10^{-34} J s, 1 eV=1.602×10−191\ \mathrm{eV} = 1.602\times10^{-19} J. Use the binomial expansion (1−x)−2≈1+2x(1 - x)^{-2} \approx 1 + 2x for small xx where needed. ((a)) Show that rn=n2a0/Zr_n = n^2a_0/Z and En=−Z2∣E1H∣/n2E_n = -Z^2|E_1^{\mathrm H}|/n^2. ((b)) Show that for large nn the frequency of the n→n−1n \to n-1 line tends to 2Z2∣E1H∣/hn32Z^2|E_1^{\mathrm H}|/hn^3, and that this is also the classical orbital frequency vn/2πrnv_n/2\pi r_n of the nnth orbit. ((c)) For He+^+ (Z=2Z = 2) with n=200n = 200, compute the exact Bohr line frequency of the 200→199200 \to 199 jump and the classical orbital frequency of the n=200n = 200 orbit, both in GHz.

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