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av dH dP dU = cydT + dP és - ar - , av av ds dT dP Using these equations in combination with the ideal gas law, show that for an ideal gas: dH = cpdT dU = c,dT , In(T2/T) + R ln(V2/V1) AS = Cp In(T2/T1) – R In(P,/P)

av dH dP dU = cydT + dP és - ar - , av av ds dT dP Using these equations in combination with the ideal gas law, show that for an ideal gas: dH = cpdT dU = c,dT , In(T2/T) + R ln(V2/V1) AS = Cp In(T2/T1) – R In(P,/P)

Introduction to Chemical Engineering Thermodynamics
Introduction to Chemical Engineering Thermodynamics
8th Edition
ISBN:9781259696527
Author:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Publisher:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Chapter1: Introduction
Section: Chapter Questions
Problem 1.1P
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Maxwell Relations
dH = cpdT + V dP - T dU = cydT + dP - V Cy ds = di dv V ar - ), dT dP Using these equations in combination with the ideal gas law, show that for an ideal gas: dH = CpdT dU = c,dT Cy In(T2 /T1) + RlIn(V2/V1) Cp In(T2/T1) – R In(P2/P) AS =
Transcribed Image Text:dH = cpdT + V dP - T dU = cydT + dP - V Cy ds = di dv V ar - ), dT dP Using these equations in combination with the ideal gas law, show that for an ideal gas: dH = CpdT dU = c,dT Cy In(T2 /T1) + RlIn(V2/V1) Cp In(T2/T1) – R In(P2/P) AS =
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