Given:
The temperature at point A \(T_A = 100^\circ C\),
The temperature at point B \(T_B = 100^\circ C\),
The temperature at point D \(T_D = 40^\circ C\),
The lengths, diameters, and thermal conductivities of the wires are identical.
Since the wires are connected in a steady-state condition, the heat flow through each wire must be the same due to the steady-state condition and no heat loss from the wires. We assume the heat flow is governed by Fourier’s Law of Heat Conduction, which is expressed as:
\[
Q = \frac{k A (T_1 - T_2)}{L}
\]
Where:
\(Q\) is the heat flow,
\(k\) is the thermal conductivity,
\(A\) is the cross-sectional area of the wire,
\(T_1\) and \(T_2\) are the temperatures at the two ends of the wire,
\(L\) is the length of the wire.
Since all the wires have the same length, cross-sectional area, and thermal conductivity, we can simplify the equation for the heat flow \(Q\) through each wire as:
\[
Q_{AC} = Q_{BC} = Q_{CD}
\]
The heat flow from A and B to C must be equal, and the heat flow from C to D must also be equal. Therefore, we have the following heat flow equations:
\[
Q_{AC} = \frac{k A (T_A - T_C)}{L}
\]
\[
Q_{BC} = \frac{k A (T_B - T_C)}{L}
\]
\[
Q_{CD} = \frac{k A (T_C - T_D)}{L}
\]
Since \(Q_{AC} = Q_{BC} = Q_{CD}\), we can equate the heat flows:
\[
\frac{k A (T_A - T_C)}{L} = \frac{k A (T_B - T_C)}{L} = \frac{k A (T_C - T_D)}{L}
\]
Simplifying the equations:
\[
(T_A - T_C) + (T_B - T_C) = (T_C - T_D)
\]
Substitute the given temperatures:
\[
(100 - T_C) + (100 - T_C) = (T_C - 40)
\]
Simplifying:
\[
200 - 2T_C = T_C - 40
\]
Solving for \(T_C\):
\[
200 + 40 = 2T_C + T_C
\]
\[
240 = 3T_C
\]
\[
T_C = \frac{240}{3} = 80^\circ C
\]
Thus, the temperature at point C is 80°C.