Latent Heat in the First Law: Change in Internal Energy During Phase Change

Physics · Thermodynamics · NEET

During a phase change, all the added heat is latent heat Q = mL, but this heat does two jobs: some goes into work W = P times delta V (the gas pushes back the atmosphere as it expands) and the rest becomes the change in internal energy, delta U = Q minus W. So delta U during boiling is always a bit LESS than the latent heat supplied. Memory hook: "Latent heat pays two bills - a rent bill (work) and a savings bill (internal energy)."
Latent Heat Splits: Q = delta U + W (Phase Change)Heat suppliedQ = mLStays insidedelta U (internal energy)Leaves as workW = P x delta V1 g water to steam2256 = 2086.8 + 169.2 J(T constant, 100 C)
The latent heat Q = mL supplied during boiling does not all become internal energy. Part becomes expansion work W = P times delta V, so delta U = Q minus W. Example: for 1 g of water boiling at 100 degree C, 2256 J splits into 2086.8 J of internal energy and 169.2 J of work.

Your doubts, answered

Is the latent heat supplied equal to the change in internal energy?

No. This is the most common mistake. The latent heat Q = mL is the total heat you supply. But by the first law, Q = delta U + W. During boiling the substance expands a lot (liquid to vapour), so it does work W = P times delta V on the surroundings. Only the leftover, delta U = Q minus W, stays inside as internal energy. So delta U is always LESS than mL for boiling. For 1 g of water: Q = 2256 J, W = 169.2 J, delta U = 2086.8 J.

Why does delta U come out less than the latent heat when water turns to steam?

Because vapour takes up far more volume than liquid. 1 g of water is about 1 cubic cm as liquid but about 1671 cubic cm as steam. This huge expansion pushes against the atmosphere (constant pressure), so the gas spends some energy as work W = P times delta V. That work energy leaves the system, so what remains as internal energy is smaller than the total heat you put in.

Does temperature change during a phase change?

No. During melting or boiling the temperature stays constant (for example water boils at 100 degree C the whole time). The heat does not raise temperature; it breaks the bonds between molecules. That is exactly why this heat is called latent (hidden) heat - you add heat but the thermometer does not move.

How do I calculate the work done during melting or freezing?

Use W = P times delta V, where delta V is the volume change. For melting ice, the volume change is tiny (ice and water have almost the same volume), so W is nearly zero and delta U is almost equal to Q. For boiling, delta V is huge, so W matters a lot. Always convert cubic cm to cubic metre: 1 cc = 10 to the power minus 6 cubic metre.

Which sign does W take when a liquid boils into vapour?

Positive. The system (the substance) expands and does work ON the surroundings, so W is positive in the convention W = P times delta V (work done BY the gas). That makes delta U = Q minus W smaller than Q. If instead vapour condenses to liquid, the volume shrinks, work is done on the system, and W is negative.

⚠️ The NEET trap
When 0.1 g of water becomes steam using 54 cal, the change in internal energy equals the heat supplied, delta U = 54 cal = 226.8 J.
You must subtract the expansion work. delta U = Q minus P delta V = 226.8 minus 16.9 = about 209 J (option 208.7 J). The heat mL is NOT the internal energy change.
🧠 During boiling, NTA hides the trap in the words change of state. If the volume of steam is given, they want delta U = Q minus P delta V, not just Q. The given volume is your clue to compute work.

Real NEET questions

2018

0.1 g of water at 100 degree C and normal pressure (1.013 x 10^5 N/m^2) requires 54 cal to convert into steam at 100 degree C. If the volume of the steam produced is 167.1 cc, the change in internal energy is

A · 42.2 J
B · 208.7 J
C · 104.3 J
D · 84.5 J
Solution: By the first law, delta U = Q minus W, where W = P times delta V. Step 1 (heat): Q = 54 cal x 4.18 J/cal = 225.7 J (using 4.2 gives 226.8 J). Step 2 (work): the steam expands against constant pressure. Neglect the tiny liquid volume, so delta V = 167.1 cc = 167.1 x 10^-6 cubic metre. W = P delta V = (1.013 x 10^5)(167.1 x 10^-6) = 16.9 J. Step 3: delta U = Q minus W = 225.7 minus 16.9 = about 208.7 J. Answer (B). Note delta U is less than the latent heat supplied, because part of the heat became expansion work.

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Frequently asked

What is the formula linking latent heat and the first law?

Start with Q = mL for the heat during a phase change. Then apply the first law Q = delta U + W. So delta U = mL minus P times delta V. Temperature is constant, but internal energy still changes because bonds break and the substance expands.

Why is latent heat called hidden heat?

Because you add heat but the temperature does not rise. The heat is hidden inside as increased potential energy of the molecules (bonds broken) plus a small amount of work done in expanding, instead of showing up as a temperature increase.

For melting ice, is delta U approximately equal to Q?

Yes. When ice melts to water the volume change is very small, so the work W = P delta V is almost zero. Therefore delta U is nearly equal to the latent heat Q = mL. The big difference appears only during boiling, where the expansion is large.

What are the standard latent heat values NEET uses?

Latent heat of fusion of ice is about 3.34 x 10^5 J/kg (about 80 cal/g), and latent heat of vaporisation of water is about 2.256 x 10^6 J/kg (about 540 cal/g, or 2256 J/g). Learn both in SI and cal units.

Does internal energy include the work done during expansion?

No. Internal energy delta U is only the energy stored inside the substance. The work W = P delta V leaves the system to push back the surroundings, so it is counted separately. That is why delta U = Q minus W.