2. Let A = A(T,V) and G = G(T,p) be thermodynamic state functions with total differentials dA = -SdT – pdV and dG = -SdT+V dp, where p, V, T, and S are, respectively, pressure, volume, temperature and entropy. a) Use dA and suitable relationships between partial derivatives to show that Cv dT + ()av dS (2) T av av as ƏT where a 1 1 and Cy = T K = V ƏT V
2. Let A = A(T,V) and G = G(T,p) be thermodynamic state functions with total differentials dA = -SdT – pdV and dG = -SdT+V dp, where p, V, T, and S are, respectively, pressure, volume, temperature and entropy. a) Use dA and suitable relationships between partial derivatives to show that Cv dT + ()av dS (2) T av av as ƏT where a 1 1 and Cy = T K = V ƏT V
Physics for Scientists and Engineers
10th Edition
ISBN:9781337553278
Author:Raymond A. Serway, John W. Jewett
Publisher:Raymond A. Serway, John W. Jewett
Chapter20: The Kinetic Theory Of Gases
Section: Chapter Questions
Problem 45CP
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