Account for the temperature and volume dependence of the entropy of a perfect gas in terms of Boltzmann distributions.
A molecule moving through a gas collides with other molecules in a random fashion
This behavior is sometimes referred to as a random-walk process
The mean free path increases as the number of molecules per unit volume decreases
The mean free path, l , equals the average distance vt traveled in a time interval t divided by the number of collisions that occur in that time interval: The number of collisions per unit time is the collision frequency: The inverse of the collision frequency is the collision mean free time l = vt d2 ( ) vt nv = 1 d2N/V
The distribution of molecular speeds depends both on the mass and on temperature
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