The heat transfer through the plate is governed by Fourier's law of heat conduction:
\[
Q = \frac{k A \Delta T}{d}
\]
Where:
- \( Q \) is the heat transferred per second (42 J),
- \( k \) is the thermal conductivity (which we need to find),
- \( A \) is the area of the cross-section of the plate (3750 cm\(^2\) = \( 3750 \times 10^{-4} \) m\(^2\)),
- \( \Delta T \) is the temperature difference between the two surfaces (14°C),
- \( d \) is the thickness of the plate (5 mm = 5 × 10\(^{-3}\) m).
Rearranging the equation to solve for \( k \):
\[
k = \frac{Q \cdot d}{A \cdot \Delta T}
\]
Substitute the known values:
\[
k = \frac{42 \cdot (5 \times 10^{-3})}{3750 \times 10^{-4} \cdot 14}
\]
Thus, the thermal conductivity of the metal is \( 30 \, \text{Wm}^{-1}\text{K}^{-1} \).