Part of JPH-02 — Atoms: Bohr Model & Hydrogen Spectrum

Excitation, Ionization, and Photon Interactions

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Ionization energy from ground state = 13.6 eV; from nth level = 13.6/n2n^2 eV. First excitation energy (n=1 to n=2) = 13.6 - 3.4 = 10.2 eV. Second excitation energy (n=1 to n=3) = 13.6 - 1.51 = 12.09 eV. A photon must have exactly the right energy to be absorbed (all-or-nothing quantum condition). If 10.2 eV photon hits ground-state hydrogen, the electron goes to n=2. A 10.5 eV photon cannot be absorbed because it matches no transition. If photon energy exceeds 13.6 eV, the electron is freed with KE = EphotonE_{photon} - 13.6 eV. Crucially, electron collisions are different: a free electron can transfer any fraction of its energy (not quantized), but at least 10.2 eV must be transferred for excitation. If the colliding electron has KE < 10.2 eV, only elastic collision occurs. Subtle point: due to momentum conservation, the available excitation energy from electron collision is KE * Mm+M\frac{M}{m+M}, which is slightly less than KE but almost equal for hydrogen.

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