Another Thermodynamics Question

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The equation U = (3/2)nRT applies specifically to monatomic ideal gases, as they possess only three degrees of freedom related to translational motion. For diatomic gases, the internal energy equation becomes U = (5/2)nRT due to the addition of rotational degrees of freedom. The equi-partition theorem explains that each degree of freedom contributes 1/2kT to the energy, with vibrational modes contributing an additional kT. In practice, for diatomic gases like hydrogen at room temperature, vibrational contributions are negligible, leading to U = (5/2)nRT rather than the expected (7/2)nRT. Consequently, the ratio of specific heats, γ, is calculated as 7/5 at room temperature.
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Why does U = (3/2)nRT?
 
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Thats not true in all cases. Its onlytrue for , if I remember correctly, monatomic ideal gases. The reason why its true has to do with the "degrees of freedom" of the gas. Monoatomic gaese have only 3 degrees of freedom(they can only move in the x, y and z directions and cannot rotate) For diatomic gases, it would be U = 5/2 nRT since we added two more degrees of freedom(two planes of rotation)
 
Yes i understand. I should have asked why

U=(f/2)nRT
where f = degrees of freedom
 
This is done by the equi partition theorem.
It states that we add 1/2KT per degree of freedom and 1KT per degree of Vibrational freedom.
An interesting case is when we consider a diatomic gas like Hyrdogen gas.
We expect U to be
N_a[ \frac{3}{2}KT + \frac{2}{2}KT + 1KT]

from velocities in x,y,z directions, the rotation about x,y and vibrational (1/2mv^2 and 1/2kx^2) respectivley
ie,
= \frac{7}{2}RT


But experimentally we find that
U= \frac{5}{2}RT

This is because at room temperature vibration does not seem to contribute

Therefore \gamma = \frac{7}{5} at room temperature
 
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