Consider two identical, finite, isolated systems of constant heat capacity \( C \) at temperatures \( T_1 \) and \( T_2 \) (\( T_1>T_2 \)). An engine works between them until their temperatures become equal. Taking into account that the work performed by the engine will be maximum (\( W_{\text{max}} \)) if the process is reversible (equivalently, the entropy change of the entire system is zero), the value of \( W_{\text{max}} \) is: