As the inversion temperature is increased, the inversion time decreases.
2.
For other gases this " Joule inversion temperature " appears to be extremely high.
3.
Therefore, our inversion temperature is given where the sign flips at zero, or
4.
A gas must be below its inversion temperature to be liquefied by the Linde cycle.
5.
This inversion can lead to cracking of ceramic ware if cooling occurs too quickly through the inversion temperature.
6.
Only below its Joule-Thomson inversion temperature ( of about 32 to 50 K at 1 atmosphere ) does it cool upon free expansion.
7.
The temperature of this point, the " Joule Thomson inversion temperature ", depends on the pressure of the gas before expansion.
8.
However, the Joule Thomson effect can be used to liquefy even helium, provided that the helium gas is first cooled below its inversion temperature of 40 K.
9.
Helium and hydrogen are two gases whose Joule Thomson inversion temperatures at a pressure of one atmosphere are very low ( e . g ., about 45 K ( " 228 �C ) for helium ).
10.
It shows that the Joule Thomson inversion temperature, at which \ mu _ { \ mathrm { JT } } is zero, occurs when the coefficient of thermal expansion is equal to the inverse of the temperature.
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