Answer: P(V 2 -V 1 ).
- A P(V<sub>2</sub>-V<sub>1</sub>)
- B (V<sub>2</sub>-V<sub>1</sub>)/P
- C P(V<sub>2</sub>+V<sub>1</sub>)
- D PV<sub>2</sub>/V<sub>1</sub>
Correct answer: A. P(V<sub>2</sub>-V<sub>1</sub>)
Explanation: W = P x delta V = P(V<sub>2</sub> - V<sub>1</sub>) for isobaric (constant pressure) process.
The Carnot cycle alternates two isothermal steps (heat absorbed at TH, released at TC) with two adiabatic steps (no heat exchange); the enclosed loop area equals the net work output, and η = 1−TC/TH is the maximum possible efficiency between those two temperatures.
Concept context
Laws of thermodynamics, heat engines, entropy, and gas processes.