AN INTRODUCTION TO SATURATED VAPOUR PRESSURE

The origin of saturated vapour pressure The evaporation of a liquid
The average energy of the particles in a liquid is governed by the temperature. The higher the temperature, the higher the average energy. But within that average, some particles have energies higher than the average, and others have energies lower than the average.
Some of the more energetic particles on the surface of the liquid can be moving fast enough to escape from the attractive forces holding the liquid together. They evaporate.
The diagram shows a small region of a liquid near its surface.
Notice that evaporation only takes place on the surface of the liquid. That's quite different from boiling which happens when there is enough energy to disrupt the attractive forces throughout the liquid. That's why, if you look at boiling water, you see bubbles of gas being formed all the way through the liquid.
If you look at water which is just evaporating in the sun, you don't see any bubbles. Water molecules are simply breaking away from the surface layer.

Eventually, the water will all evaporate in this way. The energy which is lost as the particles evaporate is replaced from the surroundings. As the molecules in the water jostle with each other, new molecules will gain enough energy to escape from the surface.
The evaporation of a liquid in a closed container
Now imagine what happens if the liquid is in a closed container. Common sense tells you that water in a sealed bottle doesn't seem to evaporate - or at least, it doesn't disappear over time.
But there is constant evaporation from the surface. Particles continue to break away from the surface of the liquid - but this time they are trapped in the space above the liquid.
As the gaseous particles bounce around, some of them will hit the surface of the liquid again, and be trapped there. There will rapidly be an equilibrium set up in which the number of particles leaving the surface is exactly balanced by the number rejoining it.
In this equilibrium, there will be a fixed number of the gaseous particles in the space above the liquid.
When these particles hit the walls of the container, they exert a pressure. This pressure is called the saturated vapour pressure (also known as saturation vapour pressure) of the liquid.
Measuring the saturated vapour pressure
It isn't difficult to show the existence of this saturated vapour pressure (and to measure it) using a simple piece of apparatus.


Note:  This experiment is much easier to talk about than do, given the safety problems in handling mercury because of its poisonous vapour. This is particularly going to be a problem if you want to find the saturated vapour pressure of a liquid at a higher temperature. You would have to use a more complex bit of apparatus. That isn't a problem you need to worry about for UK A level purposes.


If you have a mercury barometer tube in a trough of mercury, at 1 atmosphere pressure the column will be 760 mm tall. 1 atmosphere is sometimes quoted as 760 mmHg ("millimetres of mercury").
If you squirt a few drops of liquid into the tube, it will rise to form a thin layer floating on top of the mercury. Some of the liquid will evaporate and you will get the equilibrium we've just been talking about - provided there is still some liquid on top of the mercury. It is only an equilibrium if both liquid and vapour are present.
The saturated vapour pressure of the liquid will force the mercury level down a bit. You can measure the drop - and this gives a value for the saturated vapour pressure of the liquid at this temperature. In this case, the mercury has been forced down by a distance of 760 - 630 mm. The saturated vapour pressure of this liquid at the temperature of the experiment is 130 mmHg.
You could convert this into proper SI units (pascals) if you wanted to. 760 mmHg is equivalent to 101325 Pa.
A value of 130 mmHg is quite a high vapour pressure if we are talking about room temperature. Water's saturated vapour pressure is about 20 mmHg at this temperature. A high vapour pressure means that the liquid must be volatile - molecules escape from its surface relatively easily, and aren't very good at sticking back on again either.
That will result in larger numbers of them in the gas state once equilibrium is reached.
The liquid in the example must have significantly weaker intermolecular forces than water.

The variation of saturated vapour pressure with temperature The effect of temperature on the equilibrium between liquid and vapour
You can look at this in two ways.
There is a common sense way. If you increase the temperature, you are increasing the average energy of the particles present. That means that more of them are likely to have enough energy to escape from the surface of the liquid. That will tend to increase the saturated vapour pressure.