Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 38 - Quantization - Exercises and Problems - Page 1153: 32

Answer

$\lambda_{41} = 97.4~ nm$ $\lambda_{42} = 487~nm$ $\lambda_{43} = 1.88~\mu m$

Work Step by Step

We can find the energy when $n = 1$: $E_1 = -\frac{13.6~eV}{1^2} = -13.6~eV$ We can find the energy when $n = 2$: $E_2 = -\frac{13.6~eV}{2^2} = -3.4~eV$ We can find the energy when $n = 3$: $E_3 = -\frac{13.6~eV}{3^2} = -1.51~eV$ We can find the energy when $n = 4$: $E_4 = -\frac{13.6~eV}{4^2} = -0.85~eV$ One wavelength is associated with the jump from $n = 4$ to $n = 1$. In this case, the energy difference is: $~~\Delta E = (-0.85~eV)-(-13.6~eV) = 12.75~eV$ We can find the wavelength $\lambda_{41}$: $E = \frac{h~c}{\lambda}$ $\lambda_{41} = \frac{h~c}{E}$ $\lambda_{41} = \frac{(6.626\times 10^{-34}~J~s)(3.0\times 10^8~m/s)}{(12.75~eV)(1.6\times 10^{-19}~J/eV)}$ $\lambda _{41}= 9.74\times 10^{-8}~m$ $\lambda_{41} = 97.4~ nm$ One wavelength is associated with the jump from $n = 4$ to $n = 2$. In this case, the energy difference is: $~~\Delta E = (-0.85~eV)-(-3.4~eV) = 2.55~eV$ We can find the wavelength $\lambda_{42}$: $E = \frac{h~c}{\lambda}$ $\lambda_{42} = \frac{h~c}{E}$ $\lambda_{42} = \frac{(6.626\times 10^{-34}~J~s)(3.0\times 10^8~m/s)}{(2.55~eV)(1.6\times 10^{-19}~J/eV)}$ $\lambda _{42}= 4.87\times 10^{-7}~m$ $\lambda_{42} = 487~nm$ One wavelength is associated with the jump from $n = 4$ to $n = 3$. In this case, the energy difference is: $~~\Delta E = (-0.85~eV)-(-1.51~eV) = 0.66~eV$ We can find the wavelength $\lambda_{43}$: $E = \frac{h~c}{\lambda}$ $\lambda_{43} = \frac{h~c}{E}$ $\lambda_{43} = \frac{(6.626\times 10^{-34}~J~s)(3.0\times 10^8~m/s)}{(0.66~eV)(1.6\times 10^{-19}~J/eV)}$ $\lambda _{43}= 1.88\times 10^{-6}~m$ $\lambda_{43} = 1.88~\mu m$
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