The drawing (not to scale) shows the way in which the pressure and volume change for an ideal gas that is used as the working substance in a Carnot engine. The gas begins at point A (pressure = PA, volume = VA) and expands isothermally at temperature T until point B (pressure = PB, volume = VB) is reached. During this expansion, the input heat of magnitude Qn enters the gas from the hot reservoir of the engine. Then, from point B to point C (pressure Pc.volume Vc), the gas expands adiabatically. Next, the gas is compressed isothermally at temperature T. from point C to point D (pressure = PD, volume = VD). During this compression, heat of magnitude Q. is rejected to the cold reservoir of the engine. Finally, the gas is compressed adiabatically from point D to point A, where the gas is back in its initial state. The overall process A to B to C to D to A is called a Carnot cycle. Prove for this cycle that od = Te The work done during the cycle equals the area enclosed by the path on the PV diagram. %3D A %3D B Weng - Th Th Show that the for the whole process, AUA-A = 0 the energy is conserved. Note: AUA-A = AUA-B + AUB-c+ AUC-D + AUp-A
The drawing (not to scale) shows the way in which the pressure and volume change for an ideal gas that is used as the working substance in a Carnot engine. The gas begins at point A (pressure = PA, volume = VA) and expands isothermally at temperature T until point B (pressure = PB, volume = VB) is reached. During this expansion, the input heat of magnitude Qn enters the gas from the hot reservoir of the engine. Then, from point B to point C (pressure Pc.volume Vc), the gas expands adiabatically. Next, the gas is compressed isothermally at temperature T. from point C to point D (pressure = PD, volume = VD). During this compression, heat of magnitude Q. is rejected to the cold reservoir of the engine. Finally, the gas is compressed adiabatically from point D to point A, where the gas is back in its initial state. The overall process A to B to C to D to A is called a Carnot cycle. Prove for this cycle that od = Te The work done during the cycle equals the area enclosed by the path on the PV diagram. %3D A %3D B Weng - Th Th Show that the for the whole process, AUA-A = 0 the energy is conserved. Note: AUA-A = AUA-B + AUB-c+ AUC-D + AUp-A
Refrigeration and Air Conditioning Technology (MindTap Course List)
8th Edition
ISBN:9781305578296
Author:John Tomczyk, Eugene Silberstein, Bill Whitman, Bill Johnson
Publisher:John Tomczyk, Eugene Silberstein, Bill Whitman, Bill Johnson
Chapter2: Matter And Energy
Section: Chapter Questions
Problem 30RQ: A gas is compressed inside a compressor's cylinder. When the piston is at its bottom dead center,...
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![Problem:
The drawing (not to scale) shows the way in which the
pressure and volume change for an ideal gas that is used as
the working substance in a Carnot engine. The gas begins at
point A (pressure = PA, volume = VA) and expands
isothermally at temperature T until point B (pressure =
PB, volume = V B) is reached. During this expansion, the
input heat of magnitude Qn enters the gas from the hot
reservoir of the engine. Then, from point B to point C
(pressure Pc. volume = Vc), the gas expands
adiabatically. Next, the gas is compressed isothermally at
temperature T. from point C to point D (pressure =
PD, volume = VD). During this compression, heat of
magnitude Q. is rejected to the cold reservoir of the engine.
Finally, the gas is compressed adiabatically from point D to
point A, where the gas is back in its initial state. The overall
process A to B to C to D to A is called a Carnot cycle. Prove
The work done
during the cycle
equals the area
enclosed by the path
on the PV diagram.
B
Weng
T
Te
for this cycle that Od T
IQnl Th
V
Show that the for the whole process, AUA¬A = 0 the energy is conserved.
Note: AUA-A = AUA-B +AUB-c+AUC¬D + AUp¬A](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F213f7beb-e1a0-4798-85e1-b8d9fb0abe63%2Ff97b8031-3918-4278-8a89-8ea1b77f5b7f%2Fnk2yyqti_processed.jpeg&w=3840&q=75)
Transcribed Image Text:Problem:
The drawing (not to scale) shows the way in which the
pressure and volume change for an ideal gas that is used as
the working substance in a Carnot engine. The gas begins at
point A (pressure = PA, volume = VA) and expands
isothermally at temperature T until point B (pressure =
PB, volume = V B) is reached. During this expansion, the
input heat of magnitude Qn enters the gas from the hot
reservoir of the engine. Then, from point B to point C
(pressure Pc. volume = Vc), the gas expands
adiabatically. Next, the gas is compressed isothermally at
temperature T. from point C to point D (pressure =
PD, volume = VD). During this compression, heat of
magnitude Q. is rejected to the cold reservoir of the engine.
Finally, the gas is compressed adiabatically from point D to
point A, where the gas is back in its initial state. The overall
process A to B to C to D to A is called a Carnot cycle. Prove
The work done
during the cycle
equals the area
enclosed by the path
on the PV diagram.
B
Weng
T
Te
for this cycle that Od T
IQnl Th
V
Show that the for the whole process, AUA¬A = 0 the energy is conserved.
Note: AUA-A = AUA-B +AUB-c+AUC¬D + AUp¬A
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