A well-insulated, rigid calorimeter contains two immiscible liquids that do not mix chemically but remain in good thermal contact through their interface. Liquid X has mass mX and specific heat cX and is initially at temperature TX0. Liquid Y has mass mY and specific heat cY and is initially at temperature TY0. Immediately after the liquids are poured into the calorimeter they form two horizontal layers with an interface area that is large compared with the thickness of either layer. Neglect any energy transfer to the calorimeter walls.
(a) Derive an algebraic expression for the common equilibrium temperature Teq of the two-liquid system in terms of mX,mY,cX,cY,TX0, and TY0. Clearly state the physical principle used.
(b) Explain why the net energy transfer across the interface must be zero once the temperature Teq you derived is achieved.
(c) Suppose a small electric heater supplies energy Qin uniformly to liquid X after equilibrium has been established. Determine the new equilibrium temperature Teq∗ that will eventually be reached, expressing your answer in terms of Qin and the other given variables. Neglect energy losses to the surroundings.
(d) Discuss qualitatively how the magnitude of the interface area influences the time required to reach the original equilibrium temperature Teq derived in part (a). Do not perform a numerical calculation; base your reasoning on molecular-level interactions and the macroscopic definition of thermal equilibrium.