Joule- Kelvin effect
The Joule-Kelvin effect - the expansion of a real gas
This famous experiment performed in 1852 was a follow-up to those of Gay-Lussac (1807) and Joule (1845) and demonstrated that there were indeed attractive forces acting between gas molecules. In theory, if attractive forces do exist then when a gas expands its temperature should drop. The potential energy of the gas molecules has been increased and therefore in an isolated system its kinetic energy, and thus its temperature, should fall.
The apparatus used is shown in Figure 1. The experiment is often known as the porous plug experiment because gas at high pressure was allowed to expand through a cotton wool plug. The plug prevented eddies forming and the gas did not gain any kinetic energy in bulk. The initial temperature of the gas was maintained by the constant-temperature bath.
All gases showed a temperature change when passing through the plug but for some it was a cooling and for others a heating. The change in temperature was proportional to the pressure difference between the two sides of the plug: this can be understood if it is realised that work is done on the gas in forcing it through the plug and by the gas when it expands on emerging. For every gas there is an inversion temperature; if the initial temperature of the gas is above this then heating occurs and if it is below this cooling. For helium this inversion temperature is 30 K, for hydrogen 190 K and for most other gases it is well above room temperature.
The table below gives the temperature changes per atmosphere observed in the experiment.
Gas
Temperature change (oC atm-1)
Nitrogen
-0.249
Oxygen
-0.253
Air
-0.208
Carbon dioxide
-1.005
Hydrogen
-0.039
This famous experiment performed in 1852 was a follow-up to those of Gay-Lussac (1807) and Joule (1845) and demonstrated that there were indeed attractive forces acting between gas molecules. In theory, if attractive forces do exist then when a gas expands its temperature should drop. The potential energy of the gas molecules has been increased and therefore in an isolated system its kinetic energy, and thus its temperature, should fall.
The apparatus used is shown in Figure 1. The experiment is often known as the porous plug experiment because gas at high pressure was allowed to expand through a cotton wool plug. The plug prevented eddies forming and the gas did not gain any kinetic energy in bulk. The initial temperature of the gas was maintained by the constant-temperature bath.
All gases showed a temperature change when passing through the plug but for some it was a cooling and for others a heating. The change in temperature was proportional to the pressure difference between the two sides of the plug: this can be understood if it is realised that work is done on the gas in forcing it through the plug and by the gas when it expands on emerging. For every gas there is an inversion temperature; if the initial temperature of the gas is above this then heating occurs and if it is below this cooling. For helium this inversion temperature is 30 K, for hydrogen 190 K and for most other gases it is well above room temperature.
The table below gives the temperature changes per atmosphere observed in the experiment.
Gas
Temperature change (oC atm-1)
Nitrogen
-0.249
Oxygen
-0.253
Air
-0.208
Carbon dioxide
-1.005
Hydrogen
-0.039