Cyclic Process: Why dU = 0 and Work = Area of Loop

Physics · Thermodynamics · NEET

A cyclic process is one where a gas returns to its exact starting state. Because internal energy U depends only on the state (mainly temperature), and the state is the same at the end as at the start, the change in internal energy is zero: dU = 0. By the first law, this means the net heat equals the net work: Q = W, and this net work equals the area enclosed by the loop on the P-V graph. Memory hook: "Same start, same finish, so U forgets the trip. What is left is the loop's area."
PVArea = net workW = Q (dU = 0)abcdClockwiseloop:W is positiveStart = endso dU = 0
A closed loop on the P-V graph: the gas returns to its start (a), so dU = 0 over the full cycle. The net work equals the shaded area enclosed by the loop, and since dU = 0 this also equals the net heat (Q = W). A clockwise loop gives positive work.

Your doubts, answered

Why is dU = 0 in a cyclic process?

Internal energy U is a state function. This means its value depends only on the current state of the gas (for an ideal gas, only on its temperature), not on the path taken. In a cyclic process the gas comes back to the same state it started from, so its temperature is the same and U is the same. The change is dU = U(final) - U(initial) = 0. It does not matter how curvy or complicated the path was in between.

If dU = 0, does that mean no work is done?

No. dU = 0 does NOT mean W = 0. From the first law Q = dU + W, setting dU = 0 gives Q = W. So the gas can absorb heat and do net work equal to that heat over the full cycle. Work is zero only for a special path (like a single isochoric line), not for a real loop that encloses an area.

Why is the work the area ENCLOSED by the loop, not the area under the curve?

Work done by a gas in one step is W = area under that part of the curve (W = integral of P dV). In a cycle the gas expands on one part (positive work, area under the upper path) and is compressed on the return part (negative work, area under the lower path). When you subtract the return work from the forward work, the areas below both paths cancel and only the area trapped inside the loop is left. So net work = area enclosed by the loop.

How do I know if the net work is positive or negative?

Look at the direction the loop is traced on the P-V graph. Clockwise loop means positive net work (the gas does work on the surroundings, like a heat engine). Anticlockwise loop means negative net work (work is done on the gas, like a refrigerator). The size of the work is the same area either way; only the sign flips with direction.

Does Q = W for every step of the cycle, or only for the whole cycle?

Only for the WHOLE cycle. For a single step, dU is usually not zero, so Q and W differ in that step. It is only when you add up the complete loop that dU cancels to zero and the totals satisfy Q(net) = W(net) = area of the loop.

⚠️ The NEET trap
Since dU = 0 in a cyclic process, the net heat Q is also 0.
dU = 0 makes Q = W, not Q = 0. The gas still exchanges net heat, which equals the net work, which equals the area enclosed by the loop.
🧠 dU = 0 links Q to W, it does not switch them off. Zero change in U means Q and W are equal, both equal to the loop area.

Real NEET questions

ReNEET 2026

One mole of an ideal monatomic gas undergoes a cyclic process (rectangle a to b to c to d in the P-V plane, with P between 100 and 300 N/m^2, and V between 2 and 5 m^3). The total heat supplied to the gas is:

A · 400 J
B · 500 J
C · 600 J
D · 800 J
Solution: Step 1: For a complete cycle the gas returns to its starting state, so the change in internal energy is dU = 0. Step 2: By the first law, Q = dU + W = 0 + W, so the total heat supplied equals the net work done. Step 3: For a rectangular loop the net work equals the area enclosed by the loop: W = (change in V) x (change in P) = (5 - 2) x (300 - 100) = 3 x 200 = 600 J. Step 4: Therefore Q = W = 600 J. Answer: C.
NEET 2024

A thermodynamic system is taken through the cycle abcda. The work done by the gas along the path bc is:

A · 30 J
B · -90 J
C · -60 J
D · Zero
Solution: Step 1: Work done by a gas is W = integral of P dV, which equals the area under that step. Step 2: On the P-V diagram the path bc is a vertical segment, meaning the volume does not change: dV = 0 (an isochoric step). Step 3: With dV = 0, W(bc) = integral of P dV over a fixed volume = 0. So no work is done along bc even though it is part of a cycle. Answer: D. (Tip: in any cycle, the vertical, constant-volume legs contribute zero work; all the net work comes from the enclosed area.)

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Frequently asked

What is a cyclic process in thermodynamics?

A cyclic process is a series of changes after which the gas returns to its exact initial state (same pressure, volume and temperature). On a P-V graph it appears as a closed loop.

Why is the change in internal energy zero in a cyclic process?

Internal energy is a state function, so it depends only on the state of the gas, not the path. Since the final state equals the initial state in a cycle, dU = U(final) - U(initial) = 0.

What does the area of the loop represent?

The area enclosed by the loop on a P-V diagram equals the net work done in one complete cycle, which also equals the net heat exchanged since Q = W when dU = 0.

What does a clockwise loop mean?

A clockwise loop means positive net work is done by the gas (it behaves like a heat engine, absorbing heat and doing work). An anticlockwise loop means net work is done on the gas (like a refrigerator).

Is efficiency related to the area of the loop?

Yes. For a heat engine running on a cycle, the useful work output equals the area of the loop. Efficiency is that work divided by the heat absorbed from the hot source.