drcrabs
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Why does U = (3/2)nRT?
The discussion revolves around the equation U = (3/2)nRT, exploring its applicability to different types of gases, particularly in the context of thermodynamics. Participants examine the degrees of freedom associated with monatomic and diatomic gases and the implications for internal energy calculations.
Participants express differing views on the applicability of the equation U = (3/2)nRT to various gases, with some agreeing on the role of degrees of freedom while others emphasize the limitations of this relationship for diatomic gases. The discussion remains unresolved regarding the contributions of vibrational energy at different temperatures.
Participants reference the equipartition theorem and degrees of freedom, but there are unresolved assumptions regarding the temperature dependence of vibrational contributions and the specific conditions under which the equations apply.