It is the Boyle temperature $T_B.$ At Boyle temperature, the first virial coefficient (B) vanishes and real gas approaches ideal behaviour. $\, \, \, \, \, \, \, \, \, \, \, \, \, \, \, T_B=\frac{a}{Rb}$ Here, a and bare van der Waals' constants.
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The many forms of temperature listed above each have a special meaning. We must debate each one to determine which one best answers the issue. Important temperature: Each gas or vapor has the propensity to liquefy. The pressure and temperature of the vapor have a direct impact on the circumstances in which this liquefaction takes place. The different combinations of temperature and pressure allow for a wide range of liquefaction-friendly circumstances. However, regardless of changes in pressure, there is a specific temperature value over which liquefaction is not feasible due to physical limitations. Critical Temperature is the name given to the temperature. The temperature at which the sign of the Joule-Thomson effect changabout to gas is known as the inversion temperature. At this moment, neither cooling nor heating the gas expansion without using energy is permitted.