Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 27 - Early Quantum Theory and Models of the Atom - Problems - Page 800: 49

Answer

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Work Step by Step

Equation 27-15b says that for hydrogen, the energy of a level is $E_n=\frac{-13.6eV}{n^2}$. a. This transition is an absorption, because the final state energy is higher. The energy of the photon involved is the higher energy minus the lower energy. $$E=-13.6eV(\frac{1}{3^2}-\frac{1}{1^2})=12.1eV$$ b. This transition is an emission, because the initial state energy is higher. The energy of the photon involved is the higher energy minus the lower energy. $$E=-13.6eV(\frac{1}{6^2}-\frac{1}{2^2})=3.0eV$$ c. This transition is an absorption, because the final state energy is higher. The energy of the photon involved is the higher energy minus the lower energy. $$E=-13.6eV(\frac{1}{5^2}-\frac{1}{4^2})=0.31eV$$ The photon involved in the transition from n = 1 to n’ = 3 has the largest energy.
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