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The state of an ideal gas changes (expands) from 232312) via different processes. Assuming n, P₁,V₁,T₁, P₂,V₁, T2, Cvm Cp.m are known, fill in the following table. Isothermal (against vacuum) T1=T2 processes AS AS sys AS. surr universe AG Isothermal (reversible) T₁=T2 Isobaric (reversible) P₁=P₂ - Sar Isochoric (reversible) V1=V2 X Adiabatic (reversible) nCp,m (T₂-T₁) - nS(T₂-T₁)

The state of an ideal gas changes (expands) from 232312) via different processes. Assuming n, P₁,V₁,T₁, P₂,V₁, T2, Cvm Cp.m are known, fill in the following table. Isothermal (against vacuum) T1=T2 processes AS AS sys AS. surr universe AG Isothermal (reversible) T₁=T2 Isobaric (reversible) P₁=P₂ - Sar Isochoric (reversible) V1=V2 X Adiabatic (reversible) nCp,m (T₂-T₁) - nS(T₂-T₁)

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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6. The state of an ideal gas changes (expands) from (P₁,V₁,T₁) to (P₂,V₂,T₂) via different processes. Assuming n, P₁,V₁T₁, P₂,V₁, T₂, Cm, Cp.m are known, fill in the following table. Isothermal (against vacuum) T₁=T₂ processes AS AS AS sys surr universe AG Isothermal (reversible) T1=T2 Isobaric (reversible) P₁=P₂ - Sa JT₁ Isochoric (reversible) V1=V2 X Explain why the isobaric and adiabatic AG are as filled in the table. Adiabatic (reversible) nCpm (T₂-T₁) P,m - nS(T₂-T₁)
Transcribed Image Text:6. The state of an ideal gas changes (expands) from (P₁,V₁,T₁) to (P₂,V₂,T₂) via different processes. Assuming n, P₁,V₁T₁, P₂,V₁, T₂, Cm, Cp.m are known, fill in the following table. Isothermal (against vacuum) T₁=T₂ processes AS AS AS sys surr universe AG Isothermal (reversible) T1=T2 Isobaric (reversible) P₁=P₂ - Sa JT₁ Isochoric (reversible) V1=V2 X Explain why the isobaric and adiabatic AG are as filled in the table. Adiabatic (reversible) nCpm (T₂-T₁) P,m - nS(T₂-T₁)
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