Heat Engines, Refrigerators and Carnot Engine
Class 11 Physics notes covering heat engines, efficiency, refrigerators, coefficient of performance, Carnot engine, Carnot cycle, Carnot efficiency, numericals and PYQs.
Heat engines and refrigerators are practical applications of thermodynamics. A heat engine converts part of heat into useful work, while a refrigerator uses work input to move heat from a colder region to a warmer region. Carnot engine gives the ideal upper limit of efficiency between two temperatures.
Introduction
Heat engines, refrigerators and Carnot engines connect thermodynamics with machines used in transport, homes, industries and power plants.
A heat engine works in a cycle. It absorbs heat from a high-temperature source, converts part of it into work, and rejects the remaining heat to a low-temperature sink. A refrigerator works in reverse: it takes heat from a cold chamber and rejects it to a warmer room by consuming external work. The Carnot engine is an ideal reversible engine that tells us the maximum possible efficiency for any engine operating between two reservoirs.
Heat Engine
Designed to produce work output from heat input.
Refrigerator
Designed to remove heat from a cold region using work input.
Carnot Engine
Ideal reversible heat engine with maximum theoretical efficiency.
Heat Engine
A heat engine is a device that converts heat energy into mechanical work by operating in a cycle.
The engine absorbs heat Qh from a hot source at temperature Th. A part of this heat is converted into useful work W. The remaining heat Qc is rejected to a cold sink at temperature Tc. The working substance may be steam, petrol-air mixture, diesel-air mixture or gas undergoing cyclic changes.
Working Principle
- Source supplies heat at high temperature.
- Working substance converts part of heat into work.
- Sink receives rejected heat at lower temperature.
- The working substance returns to its initial state after each cycle.
Examples
Steam engines, petrol engines, diesel engines, gas turbines and thermal power plants are heat-engine examples. Their real efficiency is limited by friction, heat losses, incomplete combustion and the second law of thermodynamics.
Efficiency of Heat Engine
Efficiency measures how much of the absorbed heat becomes useful work output.
Here Qh is heat absorbed from source, Qc is heat rejected to sink, and W is net work output. Since a cyclic engine must reject some heat to the sink, 100% efficiency is impossible for a real heat engine. This is not a technological weakness only; it is a fundamental thermodynamic limitation.
Memory Trick
Efficiency asks: out of the heat taken from the hot source, what fraction came out as useful work?
Refrigerator
A refrigerator is a reverse heat engine. It uses work input to remove heat from a cold space and reject heat to warmer surroundings.
Natural heat flow is from hot to cold. A refrigerator forces heat to move from cold to hot, so external work is needed. In a domestic refrigerator, the refrigerant evaporates inside the cold chamber, absorbs heat, is compressed by a compressor, rejects heat at the condenser coils and then expands through a valve.
Domestic Refrigerator Cycle
- Evaporator absorbs heat from the cold compartment.
- Compressor does work on the refrigerant.
- Condenser rejects heat to the room.
- Expansion valve reduces pressure and temperature of refrigerant.
Coefficient of Performance (COP)
COP measures the useful cooling obtained per unit work input.
For a refrigerator, Qc is the heat removed from the cold chamber and W is the work input. COP can be greater than one because the refrigerator is not converting work into cooling directly; it is using work to transfer a larger amount of heat.
| Quantity | Heat Engine | Refrigerator |
|---|---|---|
| Purpose | Produce work output | Remove heat from cold chamber |
| Performance measure | Efficiency η = W/Qh | COP = Qc/W |
| Input | Heat from hot source | Work supplied to compressor |
| Desired output | Work | Cooling effect Qc |
Carnot Engine
A Carnot engine is an ideal reversible heat engine operating between two heat reservoirs.
It uses reversible isothermal and adiabatic processes. It has no friction, no heat leakage through finite temperature difference and no dissipative losses. Although no real engine can be perfectly Carnot, the Carnot engine sets the maximum possible efficiency between a given source and sink.
Carnot Assumptions
- All processes are reversible.
- The working substance undergoes a complete cycle.
- Heat exchange with reservoirs occurs isothermally.
- Adiabatic processes connect the two reservoir temperatures.
- No engine between the same temperatures can be more efficient.
Carnot Cycle
The Carnot cycle has four reversible stages: two isothermal and two adiabatic.
1. Isothermal Expansion
Gas expands at Th, absorbs Qh, does work and internal energy remains constant for ideal gas.
2. Adiabatic Expansion
No heat exchange. Gas expands, does work, temperature falls from Th to Tc.
3. Isothermal Compression
Gas is compressed at Tc, rejects Qc, and internal energy remains constant for ideal gas.
4. Adiabatic Compression
No heat exchange. Work is done on gas, temperature rises from Tc to Th.
Carnot Efficiency
Carnot efficiency is the maximum possible efficiency of any heat engine operating between two reservoirs.
Temperatures must be in kelvin. The formula shows that efficiency increases when source temperature is increased or sink temperature is decreased. It also shows why 100% efficiency is impossible unless Tc is 0 K, which cannot be achieved in practice.
The derivation comes from the reversible Carnot cycle relation Qc/Qh = Tc/Th. Substituting this into η = 1 - Qc/Qh gives η = 1 - Tc/Th.
Diagrams
Corrected NCERT-style diagrams showing physically accurate heat-engine, refrigerator, Carnot-cycle, efficiency, COP and P-V energy-flow structures.
Heat Engine Block Diagram
Refrigerator Block Diagram
Carnot Engine Energy Flow
Carnot Cycle P-V Diagram
Efficiency Energy-Balance Diagram
COP Energy-Flow Diagram
General Heat Engine P-V Cycle
Heat Engine vs Refrigerator Direction
Applications
Automobile Engines
Petrol and diesel engines convert heat from combustion into mechanical work.
Diesel Engines
Use high compression; adiabatic compression raises air temperature before fuel injection.
Petrol Engines
Use spark ignition and cyclic expansion of hot gases to produce work.
Refrigerators
Use work input to remove heat from food chamber and reject it to the room.
Air Conditioners
Remove heat from indoor air and reject it outside using a refrigeration cycle.
Heat Pumps
Deliver heat to a warm space; useful output is Qh.
Power Plants
Convert heat from fuel or nuclear reactions into mechanical and electrical energy.
Formula Cards
Net work output of a heat engine per cycle.
Efficiency is useful work divided by heat absorbed.
Equivalent efficiency formula using rejected heat.
Refrigerator performance: cooling effect per work input.
Energy balance for refrigerator.
Maximum efficiency between two temperatures in kelvin.
Reversible Carnot relation.
Heat pump performance when heating is desired.
If Heat Engines, Refrigerators or Carnot Engine concepts are not clear and you are looking for a Physics Tutor, contact Kumar Sir.
50 Solved Numericals
Attempt each question before opening the solution.
Show Solution
Given: Qh = 1000 J, Qc = 600 J.
Formula: W = Qh - Qc, η = W/Qh.
Solution: W = 1000 - 600 = 400 J. η = 400/1000 = 0.40.
Final Answer: Work = 400 J; efficiency = 40%.
Show Solution
Given: Qc = 800 J, W = 200 J.
Formula: COP = Qc/W.
Solution: COP = 800/200 = 4.
Final Answer: COP = 4.
Show Solution
Given: Th = 600 K, Tc = 300 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 300/600 = 0.5.
Final Answer: Carnot efficiency = 50%.
Show Solution
Given: η = 0.25, Qh = 2000 J.
Formula: W = ηQh.
Solution: W = 0.25 × 2000 = 500 J.
Final Answer: Work output = 500 J.
Show Solution
Given: COP = 5, W = 300 J.
Formula: Qc = COP × W.
Solution: Qc = 5 × 300 = 1500 J.
Final Answer: Heat extracted = 1500 J.
Show Solution
Given: Qc = 900 J, W = 300 J.
Formula: Qh = W + Qc, η = W/Qh.
Solution: Qh = 1200 J. η = 300/1200 = 0.25.
Final Answer: Heat absorbed = 1200 J; efficiency = 25%.
Show Solution
Given: η = 0.40, Th = 500 K.
Formula: η = 1 - Tc/Th.
Solution: 0.40 = 1 - Tc/500. Tc = 300 K.
Final Answer: Sink temperature = 300 K.
Show Solution
Given: Qh = 1500 J, η = 0.30.
Formula: W = ηQh, Qc = Qh - W.
Solution: W = 450 J. Qc = 1500 - 450 = 1050 J.
Final Answer: Rejected heat = 1050 J.
Show Solution
Given: Qh = 2400 J, W = 400 J.
Formula: Qh = Qc + W, COP = Qc/W.
Solution: Qc = 2000 J. COP = 2000/400 = 5.
Final Answer: Qc = 2000 J; COP = 5.
Show Solution
Given: Th = 400 K, Tc = 320 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 320/400 = 0.20.
Final Answer: Efficiency = 20%.
Show Solution
Given: Qh = 1000 J, Qc = 600 J.
Formula: W = Qh - Qc, η = W/Qh.
Solution: W = 1000 - 600 = 400 J. η = 400/1000 = 0.40.
Final Answer: Work = 400 J; efficiency = 40%.
Show Solution
Given: Qc = 800 J, W = 200 J.
Formula: COP = Qc/W.
Solution: COP = 800/200 = 4.
Final Answer: COP = 4.
Show Solution
Given: Th = 600 K, Tc = 300 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 300/600 = 0.5.
Final Answer: Carnot efficiency = 50%.
Show Solution
Given: η = 0.25, Qh = 2000 J.
Formula: W = ηQh.
Solution: W = 0.25 × 2000 = 500 J.
Final Answer: Work output = 500 J.
Show Solution
Given: COP = 5, W = 300 J.
Formula: Qc = COP × W.
Solution: Qc = 5 × 300 = 1500 J.
Final Answer: Heat extracted = 1500 J.
Show Solution
Given: Qc = 900 J, W = 300 J.
Formula: Qh = W + Qc, η = W/Qh.
Solution: Qh = 1200 J. η = 300/1200 = 0.25.
Final Answer: Heat absorbed = 1200 J; efficiency = 25%.
Show Solution
Given: η = 0.40, Th = 500 K.
Formula: η = 1 - Tc/Th.
Solution: 0.40 = 1 - Tc/500. Tc = 300 K.
Final Answer: Sink temperature = 300 K.
Show Solution
Given: Qh = 1500 J, η = 0.30.
Formula: W = ηQh, Qc = Qh - W.
Solution: W = 450 J. Qc = 1500 - 450 = 1050 J.
Final Answer: Rejected heat = 1050 J.
Show Solution
Given: Qh = 2400 J, W = 400 J.
Formula: Qh = Qc + W, COP = Qc/W.
Solution: Qc = 2000 J. COP = 2000/400 = 5.
Final Answer: Qc = 2000 J; COP = 5.
Show Solution
Given: Th = 400 K, Tc = 320 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 320/400 = 0.20.
Final Answer: Efficiency = 20%.
Show Solution
Given: Qh = 1000 J, Qc = 600 J.
Formula: W = Qh - Qc, η = W/Qh.
Solution: W = 1000 - 600 = 400 J. η = 400/1000 = 0.40.
Final Answer: Work = 400 J; efficiency = 40%.
Show Solution
Given: Qc = 800 J, W = 200 J.
Formula: COP = Qc/W.
Solution: COP = 800/200 = 4.
Final Answer: COP = 4.
Show Solution
Given: Th = 600 K, Tc = 300 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 300/600 = 0.5.
Final Answer: Carnot efficiency = 50%.
Show Solution
Given: η = 0.25, Qh = 2000 J.
Formula: W = ηQh.
Solution: W = 0.25 × 2000 = 500 J.
Final Answer: Work output = 500 J.
Show Solution
Given: COP = 5, W = 300 J.
Formula: Qc = COP × W.
Solution: Qc = 5 × 300 = 1500 J.
Final Answer: Heat extracted = 1500 J.
Show Solution
Given: Qc = 900 J, W = 300 J.
Formula: Qh = W + Qc, η = W/Qh.
Solution: Qh = 1200 J. η = 300/1200 = 0.25.
Final Answer: Heat absorbed = 1200 J; efficiency = 25%.
Show Solution
Given: η = 0.40, Th = 500 K.
Formula: η = 1 - Tc/Th.
Solution: 0.40 = 1 - Tc/500. Tc = 300 K.
Final Answer: Sink temperature = 300 K.
Show Solution
Given: Qh = 1500 J, η = 0.30.
Formula: W = ηQh, Qc = Qh - W.
Solution: W = 450 J. Qc = 1500 - 450 = 1050 J.
Final Answer: Rejected heat = 1050 J.
Show Solution
Given: Qh = 2400 J, W = 400 J.
Formula: Qh = Qc + W, COP = Qc/W.
Solution: Qc = 2000 J. COP = 2000/400 = 5.
Final Answer: Qc = 2000 J; COP = 5.
Show Solution
Given: Th = 400 K, Tc = 320 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 320/400 = 0.20.
Final Answer: Efficiency = 20%.
Show Solution
Given: Qh = 1000 J, Qc = 600 J.
Formula: W = Qh - Qc, η = W/Qh.
Solution: W = 1000 - 600 = 400 J. η = 400/1000 = 0.40.
Final Answer: Work = 400 J; efficiency = 40%.
Show Solution
Given: Qc = 800 J, W = 200 J.
Formula: COP = Qc/W.
Solution: COP = 800/200 = 4.
Final Answer: COP = 4.
Show Solution
Given: Th = 600 K, Tc = 300 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 300/600 = 0.5.
Final Answer: Carnot efficiency = 50%.
Show Solution
Given: η = 0.25, Qh = 2000 J.
Formula: W = ηQh.
Solution: W = 0.25 × 2000 = 500 J.
Final Answer: Work output = 500 J.
Show Solution
Given: COP = 5, W = 300 J.
Formula: Qc = COP × W.
Solution: Qc = 5 × 300 = 1500 J.
Final Answer: Heat extracted = 1500 J.
Show Solution
Given: Qc = 900 J, W = 300 J.
Formula: Qh = W + Qc, η = W/Qh.
Solution: Qh = 1200 J. η = 300/1200 = 0.25.
Final Answer: Heat absorbed = 1200 J; efficiency = 25%.
Show Solution
Given: η = 0.40, Th = 500 K.
Formula: η = 1 - Tc/Th.
Solution: 0.40 = 1 - Tc/500. Tc = 300 K.
Final Answer: Sink temperature = 300 K.
Show Solution
Given: Qh = 1500 J, η = 0.30.
Formula: W = ηQh, Qc = Qh - W.
Solution: W = 450 J. Qc = 1500 - 450 = 1050 J.
Final Answer: Rejected heat = 1050 J.
Show Solution
Given: Qh = 2400 J, W = 400 J.
Formula: Qh = Qc + W, COP = Qc/W.
Solution: Qc = 2000 J. COP = 2000/400 = 5.
Final Answer: Qc = 2000 J; COP = 5.
Show Solution
Given: Th = 400 K, Tc = 320 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 320/400 = 0.20.
Final Answer: Efficiency = 20%.
Show Solution
Given: Qh = 1000 J, Qc = 600 J.
Formula: W = Qh - Qc, η = W/Qh.
Solution: W = 1000 - 600 = 400 J. η = 400/1000 = 0.40.
Final Answer: Work = 400 J; efficiency = 40%.
Show Solution
Given: Qc = 800 J, W = 200 J.
Formula: COP = Qc/W.
Solution: COP = 800/200 = 4.
Final Answer: COP = 4.
Show Solution
Given: Th = 600 K, Tc = 300 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 300/600 = 0.5.
Final Answer: Carnot efficiency = 50%.
Show Solution
Given: η = 0.25, Qh = 2000 J.
Formula: W = ηQh.
Solution: W = 0.25 × 2000 = 500 J.
Final Answer: Work output = 500 J.
Show Solution
Given: COP = 5, W = 300 J.
Formula: Qc = COP × W.
Solution: Qc = 5 × 300 = 1500 J.
Final Answer: Heat extracted = 1500 J.
Show Solution
Given: Qc = 900 J, W = 300 J.
Formula: Qh = W + Qc, η = W/Qh.
Solution: Qh = 1200 J. η = 300/1200 = 0.25.
Final Answer: Heat absorbed = 1200 J; efficiency = 25%.
Show Solution
Given: η = 0.40, Th = 500 K.
Formula: η = 1 - Tc/Th.
Solution: 0.40 = 1 - Tc/500. Tc = 300 K.
Final Answer: Sink temperature = 300 K.
Show Solution
Given: Qh = 1500 J, η = 0.30.
Formula: W = ηQh, Qc = Qh - W.
Solution: W = 450 J. Qc = 1500 - 450 = 1050 J.
Final Answer: Rejected heat = 1050 J.
Show Solution
Given: Qh = 2400 J, W = 400 J.
Formula: Qh = Qc + W, COP = Qc/W.
Solution: Qc = 2000 J. COP = 2000/400 = 5.
Final Answer: Qc = 2000 J; COP = 5.
Show Solution
Given: Th = 400 K, Tc = 320 K.
Formula: η = 1 - Tc/Th.
Solution: η = 1 - 320/400 = 0.20.
Final Answer: Efficiency = 20%.
50 PYQs and Exam Questions
Answers are hidden for practice.
Show Answer
Explanation: A heat engine is a device that converts part of heat absorbed from a hot source into work and rejects the remaining heat to a cold sink.
Answer: Device converting heat into work cyclically.
Show Answer
Explanation: Some heat must be rejected to a sink in a cyclic engine; complete conversion of heat into work violates the second law.
Answer: Because Qc cannot be zero for a real cyclic engine.
Show Answer
Explanation: Efficiency is useful work output divided by heat absorbed from the hot source.
Answer: η = W/Qh = 1 - Qc/Qh.
Show Answer
Explanation: COP is the heat removed from the cold chamber per unit work input.
Answer: COP = Qc/W.
Show Answer
Explanation: Carnot efficiency depends only on absolute temperatures of source and sink.
Answer: (B) Temperatures of reservoirs.
Show Answer
Explanation: A refrigerator uses work input to transfer heat from cold body to hot body.
Answer: (B) Reverse heat engine.
Show Answer
Explanation: Energy conservation gives work output as heat absorbed minus heat rejected.
Answer: W = Qh - Qc.
Show Answer
Explanation: Carnot efficiency uses kelvin temperatures.
Answer: η = 1 - Tc/Th.
Show Answer
Explanation: The enclosed area gives net work done per cycle.
Answer: Net work output.
Show Answer
Explanation: Carnot efficiency is based on thermodynamic absolute temperature.
Answer: Temperature must be absolute.
Show Answer
Explanation: It is fully reversible and has no dissipative losses, so it sets the maximum possible efficiency.
Answer: Reversible engine between two reservoirs.
Show Answer
Explanation: No engine operating between the same two reservoirs can exceed Carnot efficiency.
Answer: No.
Show Answer
Explanation: The source supplies heat at high temperature and the sink receives rejected heat at lower temperature.
Answer: Hot reservoir and cold reservoir.
Show Answer
Explanation: It is the material that undergoes cyclic changes and exchanges heat and work.
Answer: Gas or vapour inside engine cycle.
Show Answer
Explanation: It transfers heat from colder region to hotter surroundings, opposite natural heat flow.
Answer: Work input is required.
Show Answer
Explanation: The Carnot cycle contains two isothermal and two adiabatic reversible processes.
Answer: Isothermal expansion/compression and adiabatic expansion/compression.
Show Answer
Explanation: Both statements are true and reason explains assertion.
Answer: Both true; reason is correct.
Show Answer
Explanation: Both statements are true and the reason explains why COP is not efficiency.
Answer: Both true; reason is correct.
Show Answer
Explanation: False. It rejects some heat to sink.
Answer: False.
Show Answer
Explanation: From η = 1 - Tc/Th, decreasing Tc increases η.
Answer: True.
Show Answer
Explanation: COP compares desired heat transfer with work input and may exceed one, while efficiency is work output over heat input and is less than one.
Answer: COP is a performance ratio, not conversion efficiency.
Show Answer
Explanation: Both use work input to remove heat from a colder region and reject it to hotter surroundings.
Answer: Same reverse heat engine principle.
Show Answer
Explanation: η = 1 - 400/800 = 0.5.
Answer: 50%.
Show Answer
Explanation: Rapid compression is approximately adiabatic and raises temperature.
Answer: Adiabatic compression.
Show Answer
Explanation: For heat pump, desired output is heat delivered to the warm room.
Answer: Qh.
Show Answer
Explanation: A heat engine is a device that converts part of heat absorbed from a hot source into work and rejects the remaining heat to a cold sink.
Answer: Device converting heat into work cyclically.
Show Answer
Explanation: Some heat must be rejected to a sink in a cyclic engine; complete conversion of heat into work violates the second law.
Answer: Because Qc cannot be zero for a real cyclic engine.
Show Answer
Explanation: Efficiency is useful work output divided by heat absorbed from the hot source.
Answer: η = W/Qh = 1 - Qc/Qh.
Show Answer
Explanation: COP is the heat removed from the cold chamber per unit work input.
Answer: COP = Qc/W.
Show Answer
Explanation: Carnot efficiency depends only on absolute temperatures of source and sink.
Answer: (B) Temperatures of reservoirs.
Show Answer
Explanation: A refrigerator uses work input to transfer heat from cold body to hot body.
Answer: (B) Reverse heat engine.
Show Answer
Explanation: Energy conservation gives work output as heat absorbed minus heat rejected.
Answer: W = Qh - Qc.
Show Answer
Explanation: Carnot efficiency uses kelvin temperatures.
Answer: η = 1 - Tc/Th.
Show Answer
Explanation: The enclosed area gives net work done per cycle.
Answer: Net work output.
Show Answer
Explanation: Carnot efficiency is based on thermodynamic absolute temperature.
Answer: Temperature must be absolute.
Show Answer
Explanation: It is fully reversible and has no dissipative losses, so it sets the maximum possible efficiency.
Answer: Reversible engine between two reservoirs.
Show Answer
Explanation: No engine operating between the same two reservoirs can exceed Carnot efficiency.
Answer: No.
Show Answer
Explanation: The source supplies heat at high temperature and the sink receives rejected heat at lower temperature.
Answer: Hot reservoir and cold reservoir.
Show Answer
Explanation: It is the material that undergoes cyclic changes and exchanges heat and work.
Answer: Gas or vapour inside engine cycle.
Show Answer
Explanation: It transfers heat from colder region to hotter surroundings, opposite natural heat flow.
Answer: Work input is required.
Show Answer
Explanation: The Carnot cycle contains two isothermal and two adiabatic reversible processes.
Answer: Isothermal expansion/compression and adiabatic expansion/compression.
Show Answer
Explanation: Both statements are true and reason explains assertion.
Answer: Both true; reason is correct.
Show Answer
Explanation: Both statements are true and the reason explains why COP is not efficiency.
Answer: Both true; reason is correct.
Show Answer
Explanation: False. It rejects some heat to sink.
Answer: False.
Show Answer
Explanation: From η = 1 - Tc/Th, decreasing Tc increases η.
Answer: True.
Show Answer
Explanation: COP compares desired heat transfer with work input and may exceed one, while efficiency is work output over heat input and is less than one.
Answer: COP is a performance ratio, not conversion efficiency.
Show Answer
Explanation: Both use work input to remove heat from a colder region and reject it to hotter surroundings.
Answer: Same reverse heat engine principle.
Show Answer
Explanation: η = 1 - 400/800 = 0.5.
Answer: 50%.
Show Answer
Explanation: Rapid compression is approximately adiabatic and raises temperature.
Answer: Adiabatic compression.
Show Answer
Explanation: For heat pump, desired output is heat delivered to the warm room.
Answer: Qh.
Case Study Practice
Refrigerator
Questions focus on Qc, W, Qh, COP and why work input is necessary.
Air Conditioner
Same reverse heat engine principle; indoor heat is removed and rejected outdoors.
Diesel Engine
Rapid compression raises air temperature, helping fuel ignition.
Petrol Engine
Combustion gases expand and perform work on piston.
Thermal Power Plant
Heat from fuel produces steam, turbine work and rejected heat at condenser.
Heat Pump
Useful output is heat delivered to the warm region, so COP uses Qh/W.
Quick Revision Notes
Formula Sheet
- W = Qh - Qc
- η = W/Qh
- η = 1 - Qc/Qh
- COP = Qc/W
- Qh = Qc + W
- ηCarnot = 1 - Tc/Th
Most Common Mistakes
- Using Celsius in Carnot efficiency.
- Confusing efficiency with COP.
- Forgetting that a heat engine must reject heat.
- Thinking COP cannot exceed one.
- Mixing Qh and Qc in refrigerator questions.
- Calling real engines Carnot engines.
Exam Tips
- For heat engine, desired output is work.
- For refrigerator, desired output is heat removed from cold space.
- For heat pump, desired output is heat delivered to warm space.
- Use kelvin temperature in Carnot formula.
- Remember Carnot efficiency is maximum possible, not usually achieved.
If Heat Engines, Refrigerators or Carnot Engine concepts are not clear and you are looking for a Physics Tutor, contact Kumar Sir.
Phone: +91-9958461445 Email: kumarsirphysics@gmail.com
