Bohr's hydrogen levels

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Quantum Mechanics · 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

Bohr's hydrogen levels, derived from mevr=nℏm_evr = n\hbar and the Coulomb force, are En=−∣E1∣/n2E_n = -|E_1|/n^2 with ∣E1∣=13.6|E_1| = 13.6 eV, and light is emitted only in a jump with hν=En2−En1h\nu = E_{n_2} - E_{n_1}. Use hc=1240hc = 1240 eV nm and the binomial expansion (1−x)−2≈1+2x(1 - x)^{-2} \approx 1 + 2x for small xx. ((a)) Show that for large nn the frequency of the n→n−1n \to n-1 line is ν≈2∣E1∣/hn3\nu \approx 2|E_1|/hn^3, and hence that its wavelength is λ≈hcn3/2∣E1∣\lambda \approx hcn^3/2|E_1|. ((b)) Use that approximation to find the wavelength of the 30→2930 \to 29 line of hydrogen, in mm. ((c)) Find the same wavelength exactly from ΔE=E30−E29\Delta E = E_{30} - E_{29}, in mm, and state the percentage by which the approximation is too large.

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