The cooling that results when a highly compressed gas is allowed to expand adiabatically into a region of low pressure such that no work is done. The cooling effect occurs because as the molecules of the real gas separate during expansion, internal work is done in overcoming the attractive forces between them. A perfect gas, with no attractive forces between the molecules, shows no Joule–Thomson effect. The Joule–Thomson effect is more marked at lower temperatures and was used in the Linde process for the liquefaction of air. The phenomenon was discovered by James Joule working with William Thomson (later Lord Kelvin). Hydrogen is anomalous to the Joule–Thomson effect, by showing a rise in temperature at ambient temperature. This effect continues down to 193 K whereupon it cools under expansion. This is called the inversion temperature. Hydrogen was liquefied by Dewar in 1898, who cooled the gas below the inversion temperature by liquid air, and then used the principle of the Linde process. Helium, like hydrogen, is also anomalous, with an inversion temperature of 33 K.