Abstract
Considering the nonlinearity of the Yang Mills charge, we investigate the Joule–Thomson expansion for the Einstein–Power–Yang–Mills AdS black holes in the context of the gauge-gravity duality. Under this framework, we calculate the Joule–Thomson coefficient, describe all relevant inversion and isenthalpic curves in the temperature-pressure plane that determining in this manner the corresponding cooling and heating regions. Finally we analyze the effect of the charge nonlinearity on the Joule–Thomson expansion.
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