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 freeThis problem concerns a collection of N identical harmonic oscillators (perhaps an Einstein solid or the internal vibrations of gas molecules) at temperature T. As in Section 2.2, the allowed energies of each oscillator are 0, hf, 2hf, and so on. (
a) Prove by long division that
For what values of x does this series have a finite sum?
(b) Evaluate the partition function for a single harmonic oscillator. Use the result of part (a) to simplify your answer as much as possible.
(c) Use formula 6.25 to find an expression for the average energy of a single oscillator at temperature T. Simplify your answer as much as possible.
(d) What is the total energy of the system of N oscillators at temperature T? Your result should agree with what you found in Problem 3.25.
(e) If you haven't already done so in Problem 3.25, compute the heat capacity of this system and check t hat it has the expected limits as and .
Imagine a particle that can be in only three states, with energies -0.05 eV, 0, and 0.05 eV. This particle is in equilibrium with a reservoir at 300 K.
(a) Calculate the partition function for this particle.
(b) Calculate the probability for this particle to be in each of the three states.
(c) Because the zero point for measuring energies is arbitrary, we could just as well say that the energies of the three states are 0, +0.05 eV, and +0.10 eV, respectively. Repeat parts (a) and (b) using these numbers. Explain what changes and what doesn't.
Each of the hydrogen atom states shown in Figure 6.2 is actually twofold degenerate, because the electron can be in two independent spin states, both with essentially the same energy. Repeat the calculation given in the text for the relative probability of being in a first excited state, taking spin degeneracy into account. Show that the results are unaffected.
For a mole nitrogen gas at room temperature and atmospheric pressure, compute the following and . (The electronic ground state of nitrogen is not degenerate.)
The most common measure of the fluctuations of a set of numbers away from the average is the standard deviation, defined as follows.
(a) For each atom in the five-atom toy model of Figure 6.5, compute the deviation of the energy from the average energy, that is, . Call these deviations .
(b) Compute the average of the squares of the five deviations, that is, . Then compute the square root of this quantity, which is the root-mean- square (rms) deviation, or standard deviation. Call this number . Does give a reasonable measure of how far the individual values tend to stray from the average?
(c) Prove in general that
that is, the standard deviation squared is the average of the squares minus the square of the average. This formula usually gives the easier way of computing a standard deviation.
(d) Check the preceding formula for the five-atom toy model of Figure 6.5.
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