Chapter 6: Q. 6.38 (page 246)
At room temperature, what fraction of the nitrogen molecules in the air are moving at less than?
Short Answer
The required fraction is .
Chapter 6: Q. 6.38 (page 246)
At room temperature, what fraction of the nitrogen molecules in the air are moving at less than?
The required fraction is .
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Get started for freeAlthough an ordinary H2 molecule consists of two identical atoms, this is not the case for the molecule HD, with one atom of deuterium (i.e., heavy hydrogen, 2H). Because of its small moment of inertia, the HD molecule has a relatively large value of At approximately what temperature would you expect the rotational heat capacity of a gas of HD molecules to "freeze out," that is, to fall significantly below the constant value predicted by the equipartition theorem?
In problem 6.20 you computed the partition function for a quantum harmonic oscillator :, where is the spacing between energy levels.
(a) Find an expression for the Helmholtz free energy of a system of harmonic oscillators.
(b) Find an expression for the entropy of this system as a function of temperature. (Don't worry, the result is fairly complicated.)
Consider an ideal gas of highly relativistic particles ( such as photons or fast-moving electrons) whose energy-momentum relation is instead of . Assume that these particles live in a one-dimensional universe. By following the same logic as above, derive a formula for the single particle partition function,, for one particle in the gas.
Consider a large system of indistinguishable, noninteracting molecules (perhaps an ideal gas or a dilute solution). Find an expression for the Helmholtz free energy of this system, in terms of , the partition function for a single molecule. (Use Stirling's approximation to eliminate the .) Then use your result to find the chemical potential, again in terms of.
Consider a classical "degree of freedom" that is linear rather than quadratic for some constant . (As example would be the kinetic energy of a highly relativistic particle in one dimension, written in terms of its momentum.) Repeat derivation of the equipartition theorem for this system, and show that the average energy isrole="math" localid="1646903677918" .
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