Work and Heat at Constant Volume (Isochoric): Why ΔU = qV

Chemistry · Thermodynamics · NEET

When volume does not change (isochoric process), the gas cannot push anything, so no expansion work is done: w = 0. Then the first law ΔU = q + w becomes ΔU = qV, meaning all the heat you add at constant volume goes straight into raising the internal energy. Memory hook: "No room to push, so heat stays in" — locked volume, locked-in energy.
Constant Volume (Isochoric): ΔU = qVrigid sealed wallsGASV fixedΔV = 0 → w = 0qFirst law: ΔU = q + wAt constant V: w = 0ΔU = q_Vall heat becomes internal energy(measured in a bomb calorimeter)
In a rigid, sealed container the volume cannot change (ΔV = 0), so no expansion work is done (w = 0). The first law ΔU = q + w then reduces to ΔU = qV — every joule of heat added at constant volume is stored as internal energy. This is exactly what a bomb calorimeter measures.

Your doubts, answered

Why is work zero when volume is constant?

Expansion work in chemistry is w = -p(external) × ΔV. If the volume does not change, ΔV = 0. Anything multiplied by zero is zero, so w = 0. The gas has no space to expand into and pushes nothing, so it cannot do or receive pressure-volume work. This is the whole reason ΔU = qV works.

What exactly does the subscript V in qV mean?

The small V just tells you the heat was measured while the volume was held constant. qV is not a new kind of heat; it is ordinary heat q, but with the condition 'volume fixed' attached. NCERT writes it this way so you never forget the condition that makes ΔU = qV true.

How do you get ΔU = qV from the first law?

Start with the first law: ΔU = q + w. At constant volume w = 0. Substitute: ΔU = q + 0 = q. Since this q was measured at constant volume we call it qV. So ΔU = qV. It is one substitution, nothing more.

Does ΔU = qV mean heat is a state function here?

No. Internal energy U is always a state function, but heat q is not. It only happens that at constant volume the value of qV becomes equal to ΔU, so qV takes a fixed value for given start and end states. The heat is still path-dependent in general; the constant-volume condition just pins it to ΔU.

When would I actually use ΔU = qV in a real experiment?

In a bomb calorimeter. The steel bomb is sealed, so its volume cannot change. Any heat released by a burning sample is measured at constant volume, so that heat equals ΔU directly. This is why bomb calorimeters give ΔU (internal energy change), not ΔH.

Why does constant pressure give ΔH but constant volume gives ΔU?

At constant pressure the gas can expand and do work, so some heat leaks out as work; that heat equals ΔH (enthalpy). At constant volume no work is done, so no heat leaks out as work; all of it stays as internal energy, giving ΔU. Different condition, different state function.

⚠️ The NEET trap
Students plug heat straight into ΔU = qV even for a gas expanding against pressure, or they forget that heat absorbed is +q and work done BY the system is -w.
ΔU = qV only when volume is constant (w = 0). If the system does work (expands), use the full ΔU = q + w with the correct signs: heat absorbed is positive, work done BY the system is negative.
🧠 In NEET 2026, q = +500 J absorbed and 200 J of work done BY the system gives ΔU = 500 + (-200) = 300 J — the trap answer 700 J comes from adding instead of subtracting the work.

Real NEET questions

NEET 2026

At a certain temperature T (K), during a process, 500 J is absorbed by the system and work of 200 J is done by the system. Then the change in internal energy of the system is:

A · 400 J
B · 300 J
C · 700 J
D · 500 J
Solution: First law: ΔU = q + w. Heat absorbed by the system is positive, so q = +500 J. Work done BY the system is negative, so w = -200 J. ΔU = 500 + (-200) = 300 J. (If volume were constant, w = 0 and ΔU = qV = 500 J — option D — but here the system does work, so 300 J is correct. Trap answer 700 J adds the work instead of subtracting it.)
NEET 2026

Consider the reaction 2A(g) + B(g) -> 2D(g), with ΔU° = -10 kJ/mol and ΔS° = -44 J/K at 298 K. Identify the correct ΔG° and the spontaneity at 298 K. (R = 8.31 J/mol/K)

A · -1.635 kJ/mol, spontaneous
B · -0.63568 kJ/mol, spontaneous
C · +0.63568 kJ/mol, non-spontaneous
D · +1.635 kJ/mol, non-spontaneous
Solution: The data gives ΔU° (heat at constant volume). Δn_g = 2 - (2+1) = -1. Convert to enthalpy: ΔH° = ΔU° + Δn_g RT = -10 + (-1)(8.31)(298)/1000 = -12.476 kJ/mol. Then ΔG° = ΔH° - TΔS° = -12.476 - 298(-44)/1000 = -12.476 + 13.112 = +0.636 kJ/mol. Since ΔG° > 0, the reaction is non-spontaneous. This shows why you must first turn constant-volume ΔU into ΔH.

Solved Thermodynamics NEET PYQs

Try the real previous-year questions from this chapter — each with the answer and a full solution.

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Frequently asked

Is ΔU = qV always true?

It is true only when the volume is held constant so that no pressure-volume work is done (w = 0). Change the condition and it no longer holds; at constant pressure you use ΔH = qP instead.

What is an isochoric process?

An isochoric (or isovolumetric) process is one that happens at constant volume. 'Iso' means same and 'choric' relates to volume. Because volume is fixed, no expansion work is done.

Does adding an inert gas at constant volume do work?

No. If total volume is fixed, ΔV = 0, so w = 0 regardless of what gas is added. NCERT notes that adding an inert gas at constant volume does not change partial pressures or the reaction, so no work is involved.

Why is qV useful for NEET numericals?

Because it links the measured heat directly to internal energy change with no work correction. In bomb-calorimeter problems, the heat you read off is ΔU. To get ΔH you then add Δn_g RT.

What is the sign rule for q and w in ΔU = q + w?

Heat absorbed by the system is +q; heat released is -q. Work done ON the system is +w; work done BY the system is -w. This IUPAC convention is what NEET expects.