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.
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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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For a CO 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 and then using the approximate formula .
The dissociation of molecular hydrogen into atomic hydrogen, can be treated as an ideal gas reaction using the techniques of Section 5.6. The equilibrium constant K for this reaction is defined as
whereis a reference pressure conventionally taken to beand the other P's are the partial pressures of the two species at equilibrium. Now, using the methods of Boltzmann statistics developed in this chapter, you are ready to calculate K from first principles. Do so. That is, derive a formula for K in terms of more basic quantities such as the energy needed to dissociate one molecule (see Problem 1.53) and the internal partition function for molecular hydrogen. This internal partition function is a product of rotational and vibrational contributions, which you can estimate using the methods and data in Section 6.2. (An molecule doesn't have any electronic spin degeneracy, but an H atom does-the electron can be in two different spin states. Neglect electronic excited states, which are important only at very high temperatures. The degeneracy due to nuclear spin alignments cancels, but include it if you wish.) Calculate K numerically at Discuss the implications, working out a couple of numerical examples to show when hydrogen is mostly dissociated and when it is not.
Imagine a world in which space is two-dimensional, but the laws of physics are otherwise the same. Derive the speed distribution formula for an ideal gas of nonrelativistic particles in this fictitious world, and sketch this distribution. Carefully explain the similarities and differences between the two-dimensional and three-dimensional cases. What is the most likely velocity vector? What is the most likely speed?
Prove that the probability of finding an atom in any particular energy level is , where and the "'entropy" of a level is k times the logarithm of the number of degenerate states for that level.
Some advances textbooks define entropy by the formula
where the sum runs over all microstates accessible to the system and is the probability of the system being in microstate .
(a) For an isolated system, role="math" localid="1647056883940" for all accessible states . Show that in this case the preceding formula reduces to our familiar definition of entropy.
(b) For a system in thermal equilibrium with a reservoir at temperature,role="math" localid="1647057328146" . Show that in this case as well, the preceding formula agrees with what we already know about entropy.
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