From the thermodynamic identity at constant number of particles we have Show by integration that for an
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From the thermodynamic identity at constant number of particles we have
Show by integration that for an ideal gas the entropy is
σ = Cv log τ + N log V + σ1,
where σ1 is constant, independent of τ and V.
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From U 3N2 U V 3N2 C V UV 0 I...View the full answer
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