When two bodies at different temperatures T1 and T2 are brought in thermal contact, heat energy flows from the body at higher temperature to the body at lower temperature till thermal equilibrium is attained.
Let m be the mass of both bodies and C1 and C2 be the specific heat capacities of bodies at temperatures T1 and T2 respectively. Also, assume that T1>T2. Since the body at lower temperature absorbs all the energy supplied by a hot body,
ΔQ1=−ΔQ2
∴mc1ΔT1=−mc2ΔT2 .........(1)
If 'T' is the equilibrium temperature
∴mc1(T1−t)=−mc2(T2−T) ...........(2)
Re-arranging equation (2), we get
T=c1T1+c2T2C1+C2
The equilibrium temperature depends on the specific heat capacities of the two bodies and hence cannot be (T1+T2)/2 in general.
(Note: The common temperature will be (T1+T2)/2 only if the specific heat capacities are the same, i.e., if C1=C2, then (T1+T2)/2.