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Clausius-Clapeyron equation: vapor pressure and boiling point

Estimate the vapor pressure of a liquid at any temperature, or its boiling point at any pressure, from its enthalpy of vaporization and one known point.

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kJ/mol

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°C

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°C

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Results

Vapor pressure at this temperature

70.636

Assumes a constant ΔHvap: most accurate near the reference point

Boiling point at this pressure

89.8 °C

Boiling point in °F
193.6 °F
Boiling point in kelvins
362.91 K
Enthalpy of vaporization used
40.65 kJ/mol

Vapor pressure and temperature

Every liquid gives off vapor, and the pressure of that vapor in equilibrium with the liquid rises steeply with temperature. When it reaches the pressure of the surrounding air, the liquid boils. The Clausius-Clapeyron equation links the two, and lets you predict a vapor pressure or a boiling point from a single known point and the enthalpy of vaporization.

The equation

Assuming the enthalpy of vaporization ΔHvap is constant over the range:

ln(P2 ÷ P1) = −(ΔHvap ÷ R) × (1/T2 − 1/T1)

  • T1 and T2 are absolute temperatures in kelvins
  • P1 is the vapor pressure at T1; for a liquid at its normal boiling point, P1 = 101.325 kPa
  • R = 8.314 J/(mol·K)

Solved for the boiling point at a pressure P2:

1/T2 = 1/T1 − R × ln(P2 ÷ P1) ÷ ΔHvap

Example

For water, with ΔHvap = 40.65 kJ/mol and a normal boiling point of 100 °C:

  • Vapor pressure at 90 °C: about 70.6 kPa, close to the measured 70.1 kPa
  • Boiling point at 70 kPa, the air pressure around 10,000 ft: about 89.8 °C, or 193.6 °F

Built-in substances

The calculator includes water, ethanol, methanol, acetone, benzene, toluene and diethyl ether, each with its enthalpy of vaporization at the normal boiling point. Choose Other to enter any liquid’s ΔHvap and a known temperature and vapor pressure.

Limits of the approximation

ΔHvap decreases slowly as temperature rises and vanishes at the critical point. The equation is therefore most accurate within a few tens of degrees of the reference point. Far from it, the error grows: for water at 25 °C, starting from 100 °C, it predicts about 3.75 kPa while the measured value is 3.17 kPa. For precise work over wide ranges, chemists use the Antoine equation or tabulated data, which fit measured values with empirical constants.

Where it is used

  • Predicting boiling points at altitude, in vacuum distillation and in pressure cookers
  • Estimating the evaporation of solvents and fuels
  • Meteorology, where a version of the equation gives the saturation vapor pressure of water in air

Frequently asked questions

What does the Clausius-Clapeyron equation describe?

How the vapor pressure of a liquid changes with temperature. Integrated with a constant enthalpy of vaporization, it reads ln(P2/P1) = −ΔHvap/R × (1/T2 − 1/T1), with temperatures in kelvins and R = 8.314 J/(mol·K).

How accurate is it?

Very good close to the reference point, within a few percent over a few tens of degrees. Further away, ΔHvap changes with temperature and the error grows: for water at 25 °C, it gives about 3.75 kPa instead of the measured 3.17 kPa. The Antoine equation fits data more closely over wide ranges.

How do I find the boiling point at altitude?

Enter the atmospheric pressure at that altitude as the pressure. At about 70 kPa, roughly 10,000 ft, water boils at about 90 °C, or 194 °F, which is why cooking takes longer in the mountains.

Can I find ΔHvap from two measurements?

Yes, rearrange the equation: ΔHvap = R × ln(P2/P1) ÷ (1/T1 − 1/T2). Plotting ln P against 1/T for several points gives a straight line whose slope is −ΔHvap/R.

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Results are estimates provided for information purposes. They do not replace professional advice.