Exercise 13.1.1 Derive Eqs. (13.1.11) and (13.1.14) starting from Eqs. (13.1.8)-(13.1.10).
Exercise 13.1.2 Derive the degeneracy formula, Eq. (13.1.18).
Exercise 13.1.3 Starting from the recursion relation, obtain (normalized).
Exercise 13.1.4 Recall from the last chapter [Eq. (12.6.19)] that as , in a Coulomb potential . Show that this agrees with Eq. (13.1.26).
Exercise 13.1.5 (Virial Theorem) Since is a stationary state, for any .\ Consider and use Ehrenfest's theorem to show that in the state .
Exercise 13.2.1 Let us see why the conservation of the Runge-Lenz vector implies closed orbits.
(1) Express in terms of and alone (get rid of ).
(2) Since the particle is bound, it cannot escape to infinity. So, as we follow it from some arbitrary time onward, it must reach a point where its distance from the origin stops growing. Show that
Exercise 13.3.1 The pion has a range of as a mediator of nuclear force. Estimate its rest energy.
Exercise 13.3.2 Estimate the de Broglie wavelength of an electron of kinetic energy . (Recall .)
Exercise 13.4.1 Show that if we ignore interelectron interactions, the energy levels of a multielectron atom go as . Since the Coulomb potential is , why is the energy ?
Exercise 13.4.2 Compare (roughly) the sizes of the uranium atom and the hydrogen atom. Assume levels fill in the order of increasing , and that the nonrelativistic description holds. Ignore interelectron effects.
Exercise 13.4.3 Visible light has a wavelength of approximately . Which of the series-Lyman, Balmer, Paschen-do you think was discovered first?
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