The problem asks for the thickness of an aluminium plate ($L_2$) whose thermal resistance is equal to the thermal resistance of an interface between two aluminium plates.
The thermal resistance of an interface is inversely proportional to the thermal contact conductance ($h_c$). We consider the resistance per unit area ($R''_{interface}$):
$ R''_{interface} = \frac{1}{h_c} $
Given $h_c = 10000\ W/m^2\ ^\circ C$, the interface resistance per unit area is:
$ R''_{interface} = \frac{1}{10000\ W/m^2\ ^\circ C} = 0.0001\ m^2\ ^\circ C/W $
The thermal resistance of a plate (per unit area, $R''_{plate}$) is given by its thickness ($L$) divided by its thermal conductivity ($k$):
$ R''_{plate} = \frac{L}{k} $
We need to find the thickness $L_2$ for a second aluminium plate such that its resistance equals the interface resistance:
$ R''_{plate2} = R''_{interface} $
$ \frac{L_2}{k} = \frac{1}{h_c} $
Substitute the known values for the thermal conductivity of aluminium ($k = 237\ W/m\ ^\circ C$) and the thermal contact conductance ($h_c = 10000\ W/m^2\ ^\circ C$):
$ L_2 = \frac{k}{h_c} $
$ L_2 = \frac{237\ W/m\ ^\circ C}{10000\ W/m^2\ ^\circ C} $
$ L_2 = 0.0237\ m $
Convert the thickness from meters to centimeters:
$ L_2 = 0.0237\ m \times \frac{100\ cm}{1\ m} = 2.37\ cm $
Therefore, the thickness of the aluminium plate whose thermal resistance is equal to the thermal resistance of the interface is 2.37 cm.
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