o:I m3 of an ideal gas f 360 k and I bar is compressed adiabatıcally to8 bar. It is then cooled at censtant velume dnd Purthev expanded isothermally so as to reach the conditions frem where it started. CaIculate d - pressure at the e nd of constant Volume cooling b- change in interna( energy during coustant uolume process C- Net work done and net heet t ransferred d uri the fotal process- given that the ídeal gas is div.

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
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Q2:
o:1 m3 of an ideal 19s of 360 k and I bar is compressed
ddiabatıcall to 8 bar. It is then cooled ot censtant Uelume
cdnd Purthe expanded is ofthermally so as to reach the
conditions frem where it started. cr lculate
d-pressure at the end of constant volume cooling
b- change in infernal energy durin coustant volume
process
c- Net work done and net heet transferred during
the fotal process-
given that the icdeal gas is dir.
Transcribed Image Text:Q2: o:1 m3 of an ideal 19s of 360 k and I bar is compressed ddiabatıcall to 8 bar. It is then cooled ot censtant Uelume cdnd Purthe expanded is ofthermally so as to reach the conditions frem where it started. cr lculate d-pressure at the end of constant volume cooling b- change in infernal energy durin coustant volume process c- Net work done and net heet transferred during the fotal process- given that the icdeal gas is dir.
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