The Carnot Cycle in Thermodynamics

p
V
Isotherm, pV = constant = Nk
B
T
Adiabat, pV
 = constant
v = 10:1:100;
t = 100;
r = 8.314;
gamma = 1.67;
p = r*t./v;
k = (10^(gamma-1)).*r*t;
pa = k./v.^gamma;
plot(v,pa,v,p)
Carnot cycle
v = 10:1:100;
th = 100;
tl = 50;
r = 8.314;
gamma = 1.67;
p1 = r*th./v;
k1 = (30^(gamma-1)).*r*th;
pa1 = k1./v.^gamma;
p2 = r*tl./v;
k2 = (30^(gamma-1)).*r*tl;
pa2 = k2./v.^gamma;
plot(v,p1,v,pa1,v,p2,v,pa2)
Carnot cycle
p
V
 
Q
h
T
h
Isotherm 1
Adiabat 1
Adiabat 2
Isotherm 2
p
A
, V
A
, T
A
p
B
, V
B
, T
B
p
C
, V
C
, T
C
p
D
, V
D
, T
D
Carnot cycle
p
V
Q
h
p
A
, V
A
, T
A
p
B
, V
B
, T
B
p
C
, V
C
, T
C
p
D
, V
D
, T
D
T
h
Carnot cycle
Isotherm 1
Adiabat 1
Adiabat 2
Isotherm 2
p
V
Q
h
p
A
, V
A
, T
A
p
B
, V
B
, T
B
p
C
, V
C
, T
C
p
D
, V
D
, T
D
T
l
 
Q
l
Carnot cycle
Isotherm 1
Adiabat 1
Adiabat 2
Isotherm 2
p
V
Q
h
p
A
, V
A
, T
A
p
B
, V
B
, T
B
p
C
, V
C
, T
C
p
D
, V
D
, T
D
Q
l
T
l
Carnot cycle
Isotherm 1
Adiabat 1
Adiabat 2
Isotherm 2
Why such a strange engine?
Will discuss in class
p
V
Efficiency of a Carnot engine
 
Isotherm 1
 
Adiabat 1
Adiabat 2
 
Isotherm 2
Efficiency of a Carnot engine
p
V
Isotherm 1
Adiabat 1
Adiabat 2
Isotherm 2
Efficiency of a Carnot engine
(1) From isotherm 1
(3) From isotherm 2
(2) From adiabat 1
(4) From adiabat 2
 
From the first law of thermodynamics:
Efficiency of a Carnot engine
(1) From isotherm 1
(3) From isotherm 2
(2) From adiabat 1
(4) From adiabat 2
 
From the first law of thermodynamics:
 
From (1) and (3):
Efficiency of a Carnot engine
(1) From isotherm 1
(3) From isotherm 2
(2) From adiabat 1
(4) From adiabat 2
 
From (1) and (3):
 
Efficiency is defined as:
Efficiency of a Carnot engine
(1) From isotherm 1
(3) From isotherm 2
(2) From adiabat 1
(4) From adiabat 2
 
(from (1) and (3))
 
(2)
 
and (4)
Efficiency of a Carnot engine
 
0. There is a game
Laws of thermodynamics
 
1.
You can never win
 
2. You cannot break even, either
 
3. You cannot quit the game
Carnot
Carnot engine: Schematic representation
Carnot
Carnot engine: Schematic representation
Carnot
Carnot engine is reversible
Carnot
Carnot engine is reversible (refrigerator)
C
a
r
n
o
t
s
 
t
h
e
o
r
e
m
Of all heat engines working between two given
temperatures, none is more efficient than a Carnot engine
 
reversible
Carnot
Carnot engine is reversible (refrigerator)
R
Carnot
Carnot engine is reversible (refrigerator)
R
Carnot
Carnot engine is reversible (refrigerator)
R
 
If
 
Carnot
Is this possible?
 
R
The Second Law of Thermodynamics
The Second Law of Thermodynamics
Clausius’ statement: 
Clausius’ statement: 
It is impossible to construct a
It is impossible to construct a
device that operates in a cycle and whose sole effect is
device that operates in a cycle and whose sole effect is
to transfer heat from a cooler body to a hotter body.
to transfer heat from a cooler body to a hotter body.
C
a
r
n
o
t
s
 
t
h
e
o
r
e
m
Of all heat engines working between two given
temperatures, none is more efficient than a Carnot engine
 
reversible
Carnot
For reversible engines
R
C
a
r
n
o
t
s
 
t
h
e
o
r
e
m
Of all heat engines working between two given
temperatures, none is more efficient than a Carnot engine
The Second Law of Thermodynamics
The Second Law of Thermodynamics
Clausius’ statement: 
Clausius’ statement: 
It is impossible to construct a
It is impossible to construct a
device that operates in a cycle and whose sole effect is
device that operates in a cycle and whose sole effect is
to transfer heat from a cooler body to a hotter body.
to transfer heat from a cooler body to a hotter body.
 
Kelvin-Planck statement: 
Kelvin-Planck statement: 
It is impossible to construct a
It is impossible to construct a
device that operates in a cycle and produces no other
device that operates in a cycle and produces no other
effect than the performance of work and the exchange
effect than the performance of work and the exchange
of heat from a single reservoir.
of heat from a single reservoir.
Carnot
Carnot refrigerator and Kelvin violator
Kelvin
violator
Carnot
Carnot engine and Claussius violator
Claussius
violator
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Explore the principles of the Carnot cycle, efficiency of a Carnot engine, and the significance of isotherms and adiabats in thermodynamics. Gain insights into the working of such engines and their efficiency calculations through a series of informative visual representations.

  • Thermodynamics
  • Carnot Cycle
  • Efficiency
  • Isotherms
  • Adiabats

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  1. v = 10:1:100; t = 100; r = 8.314; gamma = 1.67; p = r*t./v; k = (10^(gamma-1)).*r*t; pa = k./v.^gamma; plot(v,pa,v,p) 90 80 70 60 50 p Isotherm, pV = constant = NkBT 40 30 20 10 Adiabat, pV = constant 0 10 20 30 40 50 60 70 80 90 100 V

  2. v = 10:1:100; th = 100; tl = 50; r = 8.314; gamma = 1.67; p1 = r*th./v; k1 = (30^(gamma-1)).*r*th; pa1 = k1./v.^gamma; p2 = r*tl./v; k2 = (30^(gamma-1)).*r*tl; pa2 = k2./v.^gamma; plot(v,p1,v,pa1,v,p2,v,pa2) Carnot cycle

  3. Carnot cycle

  4. Carnot cycle pA, VA, TA Isotherm 1 Th p Qh pB, VB, TB Adiabat 2 Adiabat 1 pD, VD, TD Isotherm 2 pC, VC, TC V

  5. Carnot cycle pA, VA, TA Isotherm 1 Th p Qh pB, VB, TB Adiabat 2 Adiabat 1 pD, VD, TD Isotherm 2 pC, VC, TC V

  6. Carnot cycle pA, VA, TA Isotherm 1 Tl p Qh pB, VB, TB Adiabat 2 Adiabat 1 pD, VD, TD Ql Isotherm 2 pC, VC, TC V

  7. Carnot cycle pA, VA, TA Isotherm 1 Tl p Qh pB, VB, TB Adiabat 2 Adiabat 1 pD, VD, TD Ql Isotherm 2 pC, VC, TC V

  8. Why such a strange engine? Will discuss in class

  9. Efficiency of a Carnot engine ??,??,?? Isotherm 1 ??= ??= ? p ??,??,?? Adiabat 2 Adiabat 1 ??,??,?? ??,??,?? Isotherm 2 ??= ??= ?? V

  10. Efficiency of a Carnot engine ??,??,? Isotherm 1 ? = ?? ln?? p ?? Adiabat 2 ??,??,? ? = 0 ???? ? 1= ? ?? ? 1 Adiabat 1 ? = 0 ? ?? ? 1= ???? ? 1 ??,??,?? ??,??,?? Isotherm 2 ??= ???ln?? ?? V

  11. Efficiency of a Carnot engine ? = ?? ln?? (1) From isotherm 1 ?? ? 1= ???? ? 1 (2) From adiabat 1 ? ?? ??= ???ln?? (3) From isotherm 2 ?? ? 1= ? ?? ? 1 ???? (4) From adiabat 2 From the first law of thermodynamics: ? = ? + ? For the complete Carnot cycle ? = 0 since ? is a state variable

  12. Efficiency of a Carnot engine ? = ?? ln?? (1) From isotherm 1 ?? ? 1= ???? ? 1 (2) From adiabat 1 ? ?? ??= ???ln?? (3) From isotherm 2 ?? ? 1= ? ?? ? 1 ???? (4) From adiabat 2 From the first law of thermodynamics: ? = ? + ? For the complete Carnot cycle ? = 0 since ? is a state variable ? = ? ?is the work done on the engine (system), let ? be the work done by the engine ? = ? = ? From (1) and (3): ? = ? + ??= ?? ln?? ??+ ???ln?? ??

  13. Efficiency of a Carnot engine ? = ?? ln?? (1) From isotherm 1 ?? ? 1= ???? ? 1 (2) From adiabat 1 ? ?? ??= ???ln?? (3) From isotherm 2 ?? ? 1= ? ?? ? 1 ???? (4) From adiabat 2 From (1) and (3): ? = ? + ??= ?? ln?? ??+ ???ln?? ??= ? Efficiency is defined as:Output Input Output is the work done by the engine i.e. ? and input is the heat absorbed by the engine i.e. ? ? ? ? = ? + ?? = 1 + ?? ? efficiency = ?

  14. Efficiency of a Carnot engine ? = ?? ln?? (1) From isotherm 1 ?? ? 1= ???? ? 1 (2) From adiabat 1 ? ?? ??= ???ln?? (3) From isotherm 2 ?? ? 1= ? ?? ? 1 ???? (4) From adiabat 2 = ? + ?? ? ? ? = 1 + ?? ? efficiency = ? ???ln?? ln?? = 1 ?? ?? ?? (from (1) and (3)) ? = 1 + ?? ln?? ln?? ? ?? ?? ? 1 ? 1 ?? =?? ?? =?? (2) ? ?? ?? ? ?? ?? and (4) = = ?? ?? ?? ?? ?? ??

  15. Efficiency of a Carnot engine ? = 1 ?? ?

  16. Laws of thermodynamics 0. There is a game 1.You can never win 2. You cannot break even, either 3. You cannot quit the game

  17. Carnot engine: Schematic representation ? ? = ? ? = ? + ??= ? ?? Carnot ??= ?? = ?? ??

  18. Carnot engine: Schematic representation ? ? ? = ? ?? Carnot ?? ??

  19. Carnot engine is reversible ? ? ? = ? ?? Carnot ?? ??

  20. Carnot engine is reversible (refrigerator) ? ? ? = ? ?? Carnot ?? ??

  21. Carnots theorem reversible Of all heat engines working between two given temperatures, none is more efficient than a Carnot engine

  22. Carnot engine is reversible (refrigerator) ? ? ? ?? ? = ? ? = ? ?? R Carnot ?? ?? ?? Adjust the cycles so that ? = ?

  23. Carnot engine is reversible (refrigerator) ? ? ? ?? ? = ? ??= ? R Carnot ?? ?? ??

  24. Carnot engine is reversible (refrigerator) ? ? ? If ? > ? then: ? ? >? ?? ? ? = ? ??= ? R Carnot < ? ? ? > 0 ? ?? Also: ? ??= ? ?? ?? = ?? ?? > 0 ? ? ??

  25. Is this possible? ? ? ? ? ? = ?? ?? > 0 ? ? ?? ? = ? ??= ? R Carnot ??? ??> ?? ? > ? ?? ?? ?? ?? ??

  26. The Second Law of Thermodynamics Clausius statement: It is impossible to construct a device that operates in a cycle and whose sole effect is to transfer heat from a cooler body to a hotter body. ? ?

  27. Carnots theorem reversible Of all heat engines working between two given temperatures, none is more efficient than a Carnot engine ????< ???? ????< ????

  28. For reversible engines ? ? ? ?? ? = ? ??= ? R Carnot ?? ?? ?? ? ? ??? ? ? ? = ?

  29. Carnots theorem Of all heat engines working between two given temperatures, none is more efficient than a Carnot engine All reversible engines working between two temperatures have the same efficiency as ?Carnot

  30. The Second Law of Thermodynamics Clausius statement: It is impossible to construct a device that operates in a cycle and whose sole effect is to transfer heat from a cooler body to a hotter body. Kelvin-Planck statement: It is impossible to construct a device that operates in a cycle and produces no other effect than the performance of work and the exchange of heat from a single reservoir.

  31. Carnot refrigerator and Kelvin violator ? ? ? ? ??= ? = ??> 0 = ? ?? ? ? ? = ? Kelvin violator Carnot ?? ??

  32. Carnot engine and Claussius violator ? ? ?? ? = ? ?? Claussius violator Carnot ?? ?? ??

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