The definition of heat capacity at constant area and the Maxwell relation give the entropy differential
For a reversible adiabatic process, . Hence
for positive heat capacity . Reversible adiabatic stretching cools the film. Reversibility, or negligible entropy production, is essential to this inference. Adiabatic isolation alone only sets the heat transfer to zero; an irreversible stretch can generate entropy, so its temperature change is not fixed by this isentropic derivative.

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