AP® Physics 2: Algebra-Based · Unit 9 · Topic 9.4
Heat Engines and Cyclic Processes
A heat engine repeats a cycle that takes in heat, converts part of it to work, and dumps the rest to a colder place. Its efficiency is e = 1 - Qc/Qh, and that leftover exhaust can never be zero.
Picture a gas trapped in a piston, run through a cycle on a PV diagram: it expands, maybe cools, compresses back, and returns to its starting point. Because it returns to the same state, its internal energy doesn't change over one full lap. But the path it takes matters: on a PV plot, a clockwise loop encloses an area, and that area is the net work the gas does on its surroundings in one cycle. Heat goes in at the hot parts of the cycle, heat comes out at the cold parts, and the difference between those two is exactly the work you get out.
That outgoing heat is not a flaw you can engineer away. The second law of thermodynamics says a gas can't just absorb heat and convert all of it to work in a repeating cycle, because that would leave the gas permanently more ordered with no offsetting disorder dumped elsewhere. So every real cycle has to exhaust some heat to a cold reservoir, which is why efficiency e = 1 - Qc/Qh is always less than 1, even for an engine with zero friction. Friction just makes things worse; removing it only gets you to the theoretical ceiling, not past it.
Run the exact same cycle backward, counterclockwise on the PV plot, and the engine becomes a refrigerator: now you put work in to drag heat from a cold space to a hot one, since heat won't flow that direction on its own. This backward cycle is the bridge from engines to refrigerators and heat pumps, same loop, same areas, just the arrows reversed.
Key terms
- Heat engine
- A device that converts heat into work by repeating a cycle and returning to its starting state.
- Efficiency
- The fraction of input heat converted to net work, e = 1 - Qc/Qh.
- Cyclic process
- A sequence of changes that returns a gas to its original pressure, volume, and temperature.
- Hot and cold reservoirs
- The high temperature source that supplies heat and the low temperature sink that absorbs exhausted heat.
- Second law of thermodynamics
- A principle stating no cyclic engine can convert all absorbed heat into work; some must be exhausted.
Watch it explained
- How it worksWalk me through one full clockwise cycle on a PV plot and where the net work shows up.
- Worked exampleFind the efficiency of an engine that takes in 800 J and exhausts 600 J every cycle.
- Common mistakeWhy isn't a perfectly frictionless engine able to reach 100 percent efficiency?
- Going furtherWhat happens to the cycle when you drive it backward and turn the engine into a refrigerator?
Check yourself
End of topic.