Heat engines, refrigerators and the Carnot engine · Physics Class 11–12 | StemPy Lab
Course 11.3·Lesson 2 of 3
Heat engines, refrigerators and the Carnot engine
A heat engine takes heat Qh from a hot reservoir, does work W
Lesson 2 of 3Show all lessonsHide
Try the code and the simulations beside the lesson.
A heat engine
A car engine, a power station and a steam engine all do the same three things in each cycle:
take heat Qh from a hot reservoir at Th;
do work W;
give the rest, Qc, to a cold reservoir at Tc, usually the air or a river.
Over a cycle ΔU=0, so W=Qh−Qc, and the efficiency is
η=QhW=1−QhQc
Two block diagrams. On the left, a heat engine. A hot reservoir at the temperature T one gives the heat Q one to the engine. The engine does the work W and gives the heat Q two to a cold reservoir at the temperature T two. The efficiency is W over Q one, which is equal to 1 minus Q two over Q one. On the right, a refrigerator. Work W is put into the machine. It takes the heat Q two from the cold space and gives the heat Q one to the hot room. The coefficient of performance is Q two over W.
The picture labels the hot side T1, Q1 and the cold side T2, Q2, as NCERT does. We write h for hot and c for cold, which is easier to remember.
A refrigerator
A refrigerator is an engine run backwards. Work W moves heat Qc out of the cold inside and gives Qh=Qc+W to the warm kitchen. How well it works is its coefficient of performance:
COP=WQc
A good one has a COP of 3 to 6: it moves several joules of heat for each joule of work.
The Carnot engine
Carnot imagined an engine with no losses at all. Its gas goes round two isotherms and two adiabats, every step reversible.
A graph of pressure against volume for the Carnot cycle, a closed loop of four curves traced in the clockwise direction. A to B is an isothermal expansion at the higher temperature T one, and the gas takes the heat Q one. B to C is an adiabatic expansion, and the temperature falls to T two. C to D is an isothermal compression at the lower temperature T two, and the gas gives out the heat Q two. D to A is an adiabatic compression that brings the gas back to the start. The area inside the loop is the work done in one cycle.
For this engine QhQc=ThTc, so
ηCarnot=1−ThTc
Carnot's theorem says no engine working between the same two temperatures can do better. The best refrigerator between them has COP=Th−TcTc.
You should find that a hotter source helps an engine, while a small gap between the temperatures helps a refrigerator.
Watch out. Use kelvin. Between 100∘C and 0∘C the best efficiency is 1−373K273K, about 27%, not 100%.
A worked example
A Carnot engine works between 600K and 290K and takes in 1800J of heat per cycle. Find its efficiency, its work and the heat it gives to the sink. Then find the best COP for a freezer at 263K in a room at 303K.
Efficiency.η=1−600K290K=0.517, or 51.7%.
Work.W=0.517×1800J=930J, so Qc=1800J−930J=870J.
Freezer.COP=303K−263K263K=6.58.
Practise with new numbers
Try it in Python
The program works out the engine and the freezer of the example.
Remember these
Engine: W=Qh−Qc and η=QhW.
Refrigerator: COP=WQc and Qh=Qc+W.
Carnot, the best: η=1−ThTc, in kelvin.
Check yourself
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
An engine works between 457∘C and 37∘C. What is the best efficiency it could have?
An engine takes in 1700J per cycle and gives 1190J to its sink. Find its work and its efficiency.
Why can no real engine reach the Carnot efficiency?
A refrigerator with a COP of 3.5 uses 160J of work. How much heat does it take from its inside, and how much reaches the kitchen?
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