To solve for the temperature of the surface of contact in steady state, we need to apply the concept of thermal resistance in a series circuit. Given the thermal conductivities \(k_A = 84 \, Wm^{-1}K^{-1}\) and \(k_B = 126 \, Wm^{-1}K^{-1}\), and the fact that both plates have the same area \(A\) and thickness \(d\), we can define the thermal resistances as follows:
Resistance of plate A: \(R_A = \frac{d}{k_A \cdot A}\)
Resistance of plate B: \(R_B = \frac{d}{k_B \cdot A}\)
The total thermal resistance \(R_{total} = R_A + R_B = \frac{d}{A}\left(\frac{1}{k_A} + \frac{1}{k_B}\right)\)
In steady state, the heat flow \(Q\) through both plates is constant: \(Q = \frac{\Delta T}{R_{total}}\)
Let \(T\) be the temperature at the contact surface. The temperature drop across plate A is \((100 - T)\), and across plate B is \((T - 0)\). Therefore, we have:
For plate A: \(Q = \frac{(100 - T) \cdot A}{R_A} = \frac{(100 - T) \cdot k_A \cdot A}{d}\)
For plate B: \(Q = \frac{T \cdot A}{R_B} = \frac{T \cdot k_B \cdot A}{d}\)
Equating \(Q_A\) and \(Q_B\):
\(\frac{(100 - T) \cdot k_A}{d} = \frac{T \cdot k_B}{d}\)
Cancel \(d\) and simplify:
\((100 - T) \cdot k_A = T \cdot k_B\)
Substituting the known values:
\((100 - T) \cdot 84 = T \cdot 126\)
Expanding and rearranging terms:
\(8400 - 84T = 126T\)
\(8400 = 210T\)
Solving for \(T\):
\(T = \frac{8400}{210} = 40°C\)
The temperature of the contact surface is precisely 40°C, which fits within the given range (40,40).