Chapter 11: Problem 7
Interpret physically the Fermi energy \(\mathscr{E}_{F}\).
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Chapter 11: Problem 7
Interpret physically the Fermi energy \(\mathscr{E}_{F}\).
These are the key concepts you need to understand to accurately answer the question.
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What is the basic reason why the quantum distributions merge with the classical distribution at energies much larger than \(k T\) ?
In Debye's model of a solid, the maximum frequency \(v_{m}\) corresponds to a minimum wavelength. Because of the discrete nature of a solid this minimum wavelength corresponds to a vibration in which adjacent atoms move \(180^{\circ}\) out of phase with one another; that is, the interatomic spacing is half a wavelength. Is this plausible? Explain.
How can the ordered state of the He II explain its lack of resistance to heat conduction?
In a one-dimensional system the number of energy states per unit energy is \((l / h) \sqrt{2 m / \mathscr{E}}\), where \(l\) is the length of the sample and \(m\) is the mass of the electron. There are \(\mathcal{N}\) electrons in the sample and each state can be occupied by two electrons. (a) Determine the Fermi energy at \(0^{\circ} \mathrm{K}\). (b) Find the average energy per electron at \(0^{\circ} \mathrm{K}\).
The equilibrium state is one of maximum entropy \(S\) in thermodynamics and one of maximum probability \(P\) in statistics. Assuming then that \(S\) is a function of \(P\), show that we should expect \(S=k \ln P\), where \(k\) is a universal constant. This relation is sometimes called the Boltzmann postulate. (Hint: Consider the effect on \(S\) and \(P\) of combining two systems.)
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