Module 7 : Thermodynamic Relations
Lecture 33 : Clapeyron Equations
 



Clapeyron Equations

Let us study v−T diagram of a system. The system consists of a liquid phase at state A and a vapour phase at state B (figure 33.1)

FIGURE 33.1

The line AB corresponds to the pressure P and temperature T. Gibbs free energy can be conveniently used in analyzing the problem. Using Gibbs equation we can write

(33.1)

Along AB both dP and dT vanish; therefore dg=0

Hence, Gibbs function at a given pressure and temp has the same value for the saturated liquid and the saturated vapour.

The same result holds good for solid-liquid transition.

Next, consider a neighbouring line corresponding to pressure and temperature The value of the specific Gibbs function on the line may be denoted by Then assuming etc to be small, the change along is given by

(33.2)

While the same along is given by

(33.3)

Hence form (33.2) and (33.3) we get,

(33.5)

Diving by and proceeding to the limit

(33.5)

 

As transition from A to B is a constant pressure and constant temperature process, we get

(33.6)

Where L or is the latent heat of evaporation at temperature T

Hence

(33.7)

This is known as Clapeyron Equation. Also valid for solid - liquid transition.

  • is always positive so will depend on
  • Liquid vapour: is always positive.
    At higher pressure, boiling point is higher.
  • But for solid liquid: sometimes is negative; Notably for water: Melting is accompanied by contraction. A rise is pressure will lower down the melting point. (figure 33.2) This explains the phenomenon of relegation.

FIGURE 33.2

The Clapeyron equation can be put in a simple form if we make certain approximations. Let us consider the liquid – vapour phase transition at low pressures. Then the vapour phase may be approximated as an ideal gas. Moreover the volume if the liquid phase is negligible compared to the volume of the vapour phase

Hence

(33.8)

Using these condition, Clapeyron equation becomes

(33.9)

or

(33.10)

Which is known as Clausius – Clapeyron equation further, if we assume that is constant over a small temperature range, the above equation may be integrated to get

(33.11)

or

Constant (33.12)

Therefore a plot of InP versus 1/T yields a straight line the slope of which is equal to

The vapour pressure of most the substances agree fairly well with this equation.