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This value is exactly the Rydberg constant in the Rydberg heuristic formula [link] . In fact, [link] is identical to the Rydberg formula, because for a given m , we have In this way, the Bohr quantum model of the hydrogen atom allows us to derive the experimental Rydberg constant from first principles and to express it in terms of fundamental constants. Transitions between the allowed electron orbits are illustrated in [link] .
We can repeat the same steps that led to [link] to obtain the wavelength of the absorbed radiation; this again gives [link] but this time for the positions of absorption lines in the absorption spectrum of hydrogen. The only difference is that for absorption, the quantum number m is the index of the orbit occupied by the electron before the transition (lower-energy orbit) and the quantum number n is the index of the orbit to which the electron makes the transition (higher-energy orbit). The difference between the electron energies in these two orbits is the energy of the absorbed photon.
The radius of the orbit is
Thus, after absorbing the 93.7-nm photon, the size of the hydrogen atom in the excited state is 36 times larger than before the absorption, when the atom was in the ground state. The energy of the fifth excited state ( ) is:
After absorbing the 93.7-nm photon, the energy of the hydrogen atom is larger than it was before the absorption. Ionization of the atom when it is in the fifth excited state ( ) requites 36 times less energy than is needed when the atom is in the ground state:
Check Your Understanding When an electron in a hydrogen atom is in the first excited state, what prediction does the Bohr model give about its orbital speed and kinetic energy? What is the magnitude of its orbital angular momentum?
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