For the reversible isobaric expansion from V1 to V2 of an ideal gas inside a frictionless piston-cylinder system with heat-conductive walls: (AU)sys = q + w = CPAT – pAV. This process can be performed by slowly raising the temperature of the surroundings from T1 to T2 while holding the pressure of the surroundings constant. Show that for this type of process, AU can also be given as: (AU)sys=CVAT .
For the reversible isobaric expansion from V1 to V2 of an ideal gas inside a frictionless piston-cylinder system with heat-conductive walls: (AU)sys = q + w = CPAT – pAV. This process can be performed by slowly raising the temperature of the surroundings from T1 to T2 while holding the pressure of the surroundings constant. Show that for this type of process, AU can also be given as: (AU)sys=CVAT .
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For the reversible isobaric expansion from V, to V2 of an ideal gas inside a frictionless piston-cylinder
system with heat-conductive walls: (AU)sys = q + w = CPAT - pAV. This process can be performed by
slowly raising the temperature of the surroundings from T1 to T2 while holding the pressure of the
surroundings constant. Show that for this type of process, AU can also be given as: (AU)sys=CvAT."
Transcribed Image Text:2)
For the reversible isobaric expansion from V, to V2 of an ideal gas inside a frictionless piston-cylinder
system with heat-conductive walls: (AU)sys = q + w = CPAT - pAV. This process can be performed by
slowly raising the temperature of the surroundings from T1 to T2 while holding the pressure of the
surroundings constant. Show that for this type of process, AU can also be given as: (AU)sys=CvAT.
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