Chapter 5: Q31P (page 245)
Derive the Stefan-Boltzmann formula for the total energy density in blackbody radiation
Short Answer
Deriving the Stefan-Boltzmann formula for the total energy density in the blackbody radiation is
Chapter 5: Q31P (page 245)
Derive the Stefan-Boltzmann formula for the total energy density in blackbody radiation
Deriving the Stefan-Boltzmann formula for the total energy density in the blackbody radiation is
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Thebulk modulus of a substance is the ratio of a small decrease in pressure to the resulting fractional increase in volume:
Show that, in the free electron gas model, and use your result in Problem 5.16(d) to estimate the bulk modulus of copper. Comment: The observed value is , but don’t expect perfect agreement—after all, we’re neglecting all electron–nucleus and electron–electron forces! Actually, it is rather surprising that this calculation comes as close as it does.
Use the method of Lagrange multipliers to find the rectangle of largest area, with sides parallel to the axes that can be inscribed in the ellipse. What is the maximum area?
Suppose you had three particles, one in state, one in state, and one in state. Assuming , and are orthonormal, construct the three-particle states (analogous to Equations 5.15,5.16, and 5.17) representing
(a) distinguishable particles,
(b) identical bosons, and
(c) identical fermions.
Keep in mind that (b) must be completely symmetric, under interchange of any pair of particles, and (c) must be completely antisymmetric, in the same sense. Comment: There's a cute trick for constructing completely antisymmetric wave functions: Form the Slater determinant, whose first row is , etc., whese second row is , etc., and so on (this device works for any number of particles).
Calculate the Fermi energy for noninteracting electrons in a two-dimensional infinite square well. Let σ be the number of free electrons per unit area.
Chlorine has two naturally occurring isotopes,and . Show that
the vibrational spectrum of HCIshould consist of closely spaced doublets,
with a splitting given by , where v is the frequency of the
emitted photon. Hint: Think of it as a harmonic oscillator, with , where
is the reduced mass (Equation 5.8 ) and k is presumably the same for both isotopes.
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