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CARNOT CYCLE
By: Engr. Yuri G. Melliza
• Second Law of Thermodynamics
• Kelvin – Planck Statement
• Carnot engine
• Carnot Refrigerator
• Sample Problems
Second Law of Thermodynamics:
Whenever energy is transferred, the level of
energy cannot be conserved and some
energy must be permanently reduced to a
lower level.
When this is combined with the first law of
thermodynamics, the law of energy conservation, the
statement becomes:
Whenever energy is transferred, energy
must be conserved, but the level of energy
cannot be conserved and some energy must
be permanently reduced to a lower level.
Kelvin-Planck statement of the Second Law:
No cyclic process is possible whose sole result
is the flow of heat from a single heat reservoir
and the performance of an equivalent amount
of work.
For a system undergoing a cycle:
The net heat is equal to the net work.
Q
W 

 
 dW
dQ Where:
W - net work
Q - net heat
CARNOT CYCLE
Nicolas Leonard Sadi Carnot 1796-1832
1.Carnot Engine
Processes:
1 to 2 - Heat Addition (T = C)
2 to 3 - Expansion (S = C)
3 to 4 - Heat Rejection (T = C)
4 to 1 - Compression (S = C)
PV Diagram
TS Diagram
P
V
2
1
3
4
T = C
S = C
S = C
T = C
T
S
2
1
3
4
T H
T L
Q A
Q R
TH = T1 = T2
TL = T3 = T4
Heat Added (T = C)
QA = TH(S)  1
Heat Rejected (T = C)
QR = TL(S) 2
S = S2 - S1 = S3 – S4  3
Net Work
W = Q = QA - QR  4
W = (TH - TL)(S)  5
PV Diagram
TS Diagram
%
x
Q
Q
e
%
x
Q
Q
Q
e
%
x
Q
W
e
A
R
A
R
A
A
100
1
100
100




  6
 7
 8
PV Diagram
TS Diagram
Substituting eq.1 and eq. 5 to eq 6
%
x
T
T
e
%
x
T
T
T
e
H
L
H
L
H
100
1
100



  9
 10
PV Diagram
TS Diagram
TH
TL
W
QA
QR
E
Carnot Engine
2. Carnot Refrigerator: Reversed
Carnot Cycle
Processes:
1 to 2 - Compression (S =C)
2 to 3 - Heat Rejection (T = C)
3 to 4 - Expansion (S = C)
4 to 1 - Heat Addition (T = C)
TS Diagram
QR
QA
1
2
4
3
S
T
TH
TL
TH = T2 = T3
TL = T1 = T2
Heat Added (T = C)
QA = TL(S)  1
Heat Rejected (T = C)
QR = TH(S) 2
S = S1 - S4 = S2 - S3  3
Net Work
W = Q 4
W = QR - QA  5
W = (TH - TL)(S)  6
TS Diagram
Coefficient of Performance
(COP)
L
H
L
A
T
T
T
COP
W
Q
COP


  7
 8
TS Diagram
Tons of Refrigeration
211 KJ/min = 1 TR
3. Carnot Heat Pump:A heat pump
uses the same components as the
refrigerator but its purpose is
to reject heat at high energy
level.
Performance Factor
(PF)
A
R
R
R
Q
Q
Q
PF
W
Q
PF


  10
 11
13
1
12






COP
PF
L
T
H
T
H
T
PF
TH
TL
W
QA
QR
R
Carnot Refrigerator
A Carnot engine operating between 775 K and
305K produces 54 KJ of work. Determine the
change of entropy during heat addition.
TH = 775 K ; TL = 305 K
W = 54 KJ
TS Diagram
TH
TL
W
QA
QR
E
K
KJ
0.015
775
89.04
T
Q
S
-
S
)
S
-
(S
T
Q
KJ
89.04
0.606
54
e
W
Q
Q
W
e
0.606
775
305
775
T
T
T
e
H
A
1
2
1
2
H
A
A
A
H
L
H














A Carnot heat engine rejects 230 KJ of
heat at 25C. The net cycle work is 375 KJ.
Determine the cycle thermal efficiency and
the cycle high temperature .
Given:
QR = 230 KJ
TL = 25 + 273 = 298K
W = 375 KJ
TL = 298K
TH
W
E
QR = 230 KJ
QA
K
87
.
783
772
.
0
605
)
S
-
(S
Q
T
K
KJ/
-0.772
)
S
-
(S
K
KJ/
772
.
0
)
S
S
(
)
S
S
(
298
230
)
S
S
(
S
S
)
S
S
(
T
Q
)
S
S
(
T
Q
62
.
0
605
375
QA
W
e
KJ
605
QA
)
230
375
(
Q
W
Q
Q
Q
W
1
2
A
H
1
2
3
4
3
4
1
2
3
4
3
4
L
R
1
2
H
A
R
A
R
A





























Module 9 (second law & carnot cycle)
Module 9 (second law & carnot cycle)

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