Chapter 6: Q. 6.33 (page 246)
Calculate the most probable speed, average speed and rms speed for Oxygenmolecules at room temperature.
Short Answer
The most probable speed is, the average speed isand the rms speed is.
Chapter 6: Q. 6.33 (page 246)
Calculate the most probable speed, average speed and rms speed for Oxygenmolecules at room temperature.
The most probable speed is, the average speed isand the rms speed is.
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Get started for freeIn the low-temperature limit , each term in the rotational partition function is much smaller than the one before. Since the first term is independent of , cut off the sum after the second term and compute the average energy and the heat capacity in this approximation. Keep only the largest T-dependent term at each stage of the calculation. Is your result consistent with the third law of thermodynamics? Sketch the behavior of the heat capacity at all temperature, interpolating between the high-temperature and low- temperature expressions.
Derive equation 6.92 and 6.93 for the entropy and chemical potential of an ideal gas.
For a mole nitrogen gas at room temperature and atmospheric pressure, compute the following and . (The electronic ground state of nitrogen is not degenerate.)
In the numerical example in the text, I calculated only the ratio of the probabilities of a hydrogen atom being in two different states. At such a low temperature the absolute probability of being in a first excited state is essentially the same as the relative probability compared to the ground state. Proving this rigorously, however, is a bit problematic, because a hydrogen atom has infinitely many states.
(a) Estimate the partition function for a hydrogen atom at 5800 K, by adding the Boltzmann factors for all the states shown explicitly in Figure 6.2. (For simplicity you may wish to take the ground state energy to be zero, and shift the other energies according!y.)
(b) Show that if all bound states are included in the sum, then the partition function of a hydrogen atom is infinite, at any nonzero temperature. (See Appendix A for the full energy level structure of a hydrogen atom.)
(c) When a hydrogen atom is in energy level n, the approximate radius of the electron wavefunction is , where ao is the Bohr radius, about 5 x 10-11 m. Going back to equation 6.3, argue that the PdV term is Tot negligible for the very high-n states, and therefore that the result of part (a), not that of part (b), gives the physically relevant partition function for this problem. Discuss.
For a molecule, the constant is approximately .(This number is measured using microwave spectroscopy, that is, by measuring the microwave frequencies needed to excite the molecules into higher rotational states.) Calculate the rotational partition function for a molecule at room temperature , first using the exact formula 6.30 and then using the approximate formula 6.31
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