Question
A gas is taken through the cyclic process: A→B isobaric expansion, B→C isochoric pressure drop, C→A isothermal compression. Given K, L, atm, and L. Find , , and for the full cycle.
Solution — Step by Step
A: atm, L, K.
A→B is isobaric, so atm. L. By ideal gas law: K.
B→C is isochoric, so L. C→A is isothermal — meaning K. By ideal gas: atm.
A→B (isobaric): atm·L.
B→C (isochoric): .
C→A (isothermal): atm·L atm·L.
(using atm·L J)
for a cycle (state function returns to start).
By first law: J.
Final answer: , J, J.
Why This Works
Internal energy depends only on state, so any closed cycle has . The first law then gives for the cycle. The net work equals the area enclosed by the cycle on a - diagram.
This is true for any cycle, regardless of the working substance (ideal gas, real gas, refrigerant) — a powerful conceptual shortcut.
Alternative Method
Compute for each segment using and , then sum. Slower but useful when individual segment heats are asked.
The area enclosed by a cycle on a - diagram equals the net work done. Clockwise = positive (heat engine). Anticlockwise = negative (refrigerator). This visual shortcut beats algebra in MCQs.
Forgetting the sign of in the isothermal compression. Volume decreases, so , making — gas absorbs work, not delivers it. Sign comes naturally from , but only if you keep on top.