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CARNOT ENGINE
AND THEOREM
NAME: ANILA HALEEM
GROUP: 3rd
DEPARTMENT: PHYSICS
SEMESTER: 3rd
OUTLINES:
● CARNOT ENGINE
● CARNOT CYCLE
● CALCULATION OF EFFICIENCY
● CARNOT THEOREM
HISTORY:
● Proposed by Nicolas Leonard Sadi Carnot in 1824
● He was a French Engineer
● Founder of the science of thermodynamics
● First one to recognize the relationship between work and heat
INTRODUCTION:
● The most powerful and efficient heat cycle consisting of two isothermal and
two adiabatic processes
● Carnot engine is an ideal heat engine whose efficiency is maximum
● In carnot engine, carnot cycle is used
● It is free from all the dissipative forces
CONSIDERATION:
1. A cylinder having a conducting base only
2. Two expansions and two compressions
3. Calculation of efficiency
CARNOT CYCLE:
It consist of four processes
1. ISOTHERMAL EXPANSION:
● Allowed to expand isothermally, at temperature T1
● Absorbing heat Q1 from Hot Reservoir.(curve AB)
● The volume increases but pressure decreases
CONTI:
2. ADIABATIC EXPANSION:
● Allowed to expand adiabatically until temperature drops to T2 ( curve BC)
● The volume increase and pressure decreases
CONTI:
3. ISOTHERMAL COMPRESSION:
● Compressed isothermally at T2, rejecting heat Q2 to cold reservoir (curve
CD)
● The volume decreases and pressure increases
CONTI:
4. ADIABATIC COMPRESSION:
Finally the gas is compressed Adiabatically to restore the initial temperature
(curve DA)
CALCULATION OF EFFICIENCY:
● During one cycle, Carnot heat engine performs a net amount of work delW
● The net amount of heat absorbed by the engine in one cycle is Q1-Q2
● Where Q1 is the heat absorbed during the isothermal expansion
● Where Q2 is the heat rejected during the isothermal compression
● Thermal efficiency is given by:
Efficiency=output/input
CARNOT THEOREM:
● No real engine can be more efficient than a Carnot Engine operating
between same two reservoirs
● All Carnot Engines operating between reservoirs at the same temperature
have the same efficiency
carnot engine and theorem
carnot engine and theorem

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carnot engine and theorem

  • 1. CARNOT ENGINE AND THEOREM NAME: ANILA HALEEM GROUP: 3rd DEPARTMENT: PHYSICS SEMESTER: 3rd
  • 2. OUTLINES: ● CARNOT ENGINE ● CARNOT CYCLE ● CALCULATION OF EFFICIENCY ● CARNOT THEOREM
  • 3. HISTORY: ● Proposed by Nicolas Leonard Sadi Carnot in 1824 ● He was a French Engineer ● Founder of the science of thermodynamics ● First one to recognize the relationship between work and heat
  • 4. INTRODUCTION: ● The most powerful and efficient heat cycle consisting of two isothermal and two adiabatic processes ● Carnot engine is an ideal heat engine whose efficiency is maximum ● In carnot engine, carnot cycle is used ● It is free from all the dissipative forces
  • 5. CONSIDERATION: 1. A cylinder having a conducting base only 2. Two expansions and two compressions 3. Calculation of efficiency
  • 6. CARNOT CYCLE: It consist of four processes 1. ISOTHERMAL EXPANSION: ● Allowed to expand isothermally, at temperature T1 ● Absorbing heat Q1 from Hot Reservoir.(curve AB) ● The volume increases but pressure decreases
  • 7.
  • 8. CONTI: 2. ADIABATIC EXPANSION: ● Allowed to expand adiabatically until temperature drops to T2 ( curve BC) ● The volume increase and pressure decreases
  • 9.
  • 10. CONTI: 3. ISOTHERMAL COMPRESSION: ● Compressed isothermally at T2, rejecting heat Q2 to cold reservoir (curve CD) ● The volume decreases and pressure increases
  • 11.
  • 12. CONTI: 4. ADIABATIC COMPRESSION: Finally the gas is compressed Adiabatically to restore the initial temperature (curve DA)
  • 13.
  • 14. CALCULATION OF EFFICIENCY: ● During one cycle, Carnot heat engine performs a net amount of work delW ● The net amount of heat absorbed by the engine in one cycle is Q1-Q2 ● Where Q1 is the heat absorbed during the isothermal expansion ● Where Q2 is the heat rejected during the isothermal compression ● Thermal efficiency is given by: Efficiency=output/input
  • 15.
  • 16. CARNOT THEOREM: ● No real engine can be more efficient than a Carnot Engine operating between same two reservoirs ● All Carnot Engines operating between reservoirs at the same temperature have the same efficiency