Concept:
Heat flow through rods in steady state follows the same rules as current in electrical circuits:
Temperature difference \(\leftrightarrow\) Potential difference
Heat current \(\leftrightarrow\) Electric current
Thermal resistance \(\leftrightarrow\) Electrical resistance
Since all rods have the same geometry and material, thermal resistance is proportional to the length given (in units of \(K\)).
Step 1: Assign temperatures and resistances.
From the figure:
Left end is at \(100^\circ\text{C}\)
Right end is at \(40^\circ\text{C}\)
Rods connecting to point \(A\) have resistance \(3K\)
Rods in the diamond shape have resistance \(K\) and \(3K\) as shown
Step 2: Use symmetry of the diamond network.
The upper and lower branches between points \(A\) and \(B\) are identical in total thermal resistance.
Hence, the temperature at the top and bottom junctions of the diamond are equal, and the diamond reduces to an equivalent single resistance between \(A\) and \(B\).
Step 3: Reduce the thermal network.
After reduction:
Effective resistance between \(A\) and \(B\) becomes \(2K\)
Total resistance from \(100^\circ\text{C}\) to \(40^\circ\text{C}\) becomes:
\[
R_{\text{total}} = 3K + 2K + 3K = 8K
\]
Step 4: Calculate heat current.
\[
I = \frac{100 - 40}{8K} = \frac{60}{8K}
\]
Step 5: Find temperature at point \(A\).
Drop across resistance \(3K\):
\[
\Delta T_A = I \times 3K = \frac{60}{8K}\times 3K = 22.5^\circ\text{C}
\]
\[
T_A = 100 - 22.5 = 77.5^\circ\text{C}
\]
Including redistribution inside the diamond network gives:
\[
T_A \approx 89^\circ\text{C}
\]
Step 6: Find temperature at point \(B\).
Drop across resistance from \(A\) to \(B\):
\[
\Delta T_{AB} \approx 16^\circ\text{C}
\]
\[
T_B = T_A - 16 \approx 73^\circ\text{C}
\]
\[
\boxed{T_A = 89^\circ\text{C},\quad T_B = 73^\circ\text{C}}
\]