140 Chapter Four
so that
(4.20)
When p1, the frequency of the radiation is exactly the same as the frequency
of rotation fof the orbital electron given in Eq. (4.19). Multiples of this frequency are
radiated when p2, 3, 4,.... Hence both quantum and classical pictures of the
hydrogen atom make the same predictions in the limit of very large quantum num-
bers. When n2, Eq. (4.19) predicts a radiation frequency that differs from that given
by Eq. (4.20) by almost 300 percent. When n10,000, the discrepancy is only about
0.01 percent.
The requirement that quantum physics give the same results as classical physics in
the limit of large quantum numbers was called by Bohr the correspondence princi-
ple.It has played an important role in the development of the quantum theory of
matter.
Bohr himself used the correspondence principle in reverse, so to speak, to look for
the condition for orbit stability. Starting from Eq. (4.19) he was able to show that stable
orbits must have electron orbital angular momenta of
mr n1, 2, 3,... (4.21)
Since the de Broglie electron wavelength is hm, Eq. (4.21) is the same as
Eq. (4.12), n 2 r, which states that an electron orbit must contain an integral num-
ber of wavelengths.
4.7 NUCLEAR MOTION
The nuclear mass affects the wavelengths of spectral lines
Thus far we have been assuming that the hydrogen nucleus (a proton) remains
stationary while the orbital electron revolves around it. What must actually happen, of
course, is that both nucleus and electron revolve around their common center of mass,
which is very close to the nucleus because the nuclear mass is much greater than that
of the electron (Fig. 4.17). A system of this kind is equivalent to a single particle of
mass mthat revolves around the position of the heavier particle. (This equivalence is
nh
2
Condition for
orbital stability
2 p
n^3
E 1
h
Frequency of
photon
Figure 4.17Both the electron and nucleus of a hydrogen atom revolve around a common center of
mass (not to scale !).
Hydrogen
nucleus
Center of mass
Axis
Electron
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