Chapter 10: Q27E (page 467)
Section 10.2 gives the energy and approximate proton separation of the molecule. What is the energy of the electron alone?
Short Answer
The energy of the electron in is .
Chapter 10: Q27E (page 467)
Section 10.2 gives the energy and approximate proton separation of the molecule. What is the energy of the electron alone?
The energy of the electron in is .
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Get started for freeThe effective force constant of the molecular “spring” in HCL is , and the bond length is .
(a) Determine the energies of the two lowest-energy vibrational states.
(b) For these energies, determine the amplitude of vibration if the atoms could be treated as oscillating classical particles.
(c) For these energies, by what percentages does the atomic separation fluctuate?
(d) Calculate the classical vibrational frequencyand rotational frequency for the rotational frequency, assume that L is the its lowest non zero value, and that the moment of inertia is .
(e) Is is valid to treat the atomic separation as fixed for rotational motion while changing for vibrational?
Question:If electrical conductivity were determined by the mere static presence of positive ions rather than by their motion the collision time would be inversely proportional to the electron's average speed. If however, it were dominated by the motion of the ions, it should be inversely proportional to the “area" presented by a jiggling ion, which is in turn proportional to the square of its amplitude as an oscillator. Argue that only the latter view gives the correct temperature dependence in conductors of . Use the equipartition theorem (usually covered in introductory thermodynamics and also discussed in Section 9.9).
Of , and , none has an electric dipole moment, but one does have a magnetic dipole moment, which one, and why?
(Refer to figure 10.10)
Show that for a room-temperature semiconductor with a band gap of , a temperature rise of 4K would raise the conductivity by about 30%.
Assuming an interatomic spacing of 0.15 nm, obtain a rough value for the width (in eV) of the band in a one-dimensional crystal.
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