Complete question is missing, so i have attached it.
Answer:
ΔS = nC_p*In[(T1 + T2)²/4(T1•T2)]
Explanation:
Since the two blocks are kept in contact together, the final temperature will be given written as:
T_f = (T1 + T2)/2
Now, the entropy change of the system would be expressed as;
ΔS_sys = ∫(dq_rev)/T
This can be broken down into;
ΔS_sys = nC_p∫(1/T)dT
For the first block, when we integrate with boundaries of T_f and T1, we have;
ΔS1 = nC_p[In (T_f/T1)]
Similarly, for the second block, integrating with boundaries of T_f and T2, we have;
ΔS2 = nC_p[In (T_f/T2)]
Thus, total change in entropy will be;
ΔS = ΔS1 + ΔS2 = nC_p[In (T_f/T1)] + nC_p[In (T_f/T2)]
This gives;
ΔS = nC_p*In[T_f²/(T1•T2)]
Earlier, we saw that T_f = (T1 + T2)/2
Thus;
ΔS = nC_p*In[(T1 + T2)²/4(T1•T2)]