Plane walls sometimes consist of several layers of different materials. The concept of thermal resistance can be used to determine the rate of steady heat transfer through such ‘composite walls’.
The thermal resistance is analogous to electrical resistance and follows the series and parallel law.
The convective resistance is used at the peripheries of the wall and conductive resistance is used between the walls of similar material.
The composite wall (consisting of two plane walls in series) and its thermal resistance network for heat transfer are as shown:
The formulae for thermal resistances are:
a. Convective resistance at wall 1:
Here, the area of cross section is A and the convective coefficient at wall 1 is .
b. Conductive resistance in wall 1:
Here, the length of wall 1 is and its thermal conductivity is .
c. Conductive resistance in wall 2:
Here, the length of wall 2 is and its thermal conductivity is .
d. Convective resistance at wall 2:
Here, the convective coefficient at wall 2 is .
The rate of heat transfer can be calculated as,
Draw the thermal circuit.
Obtain the thermal resistances per unit area.
Here, the convective coefficient is h.
Here, the length and thermal conductivity of wall A are and respectively.
Here, the length and thermal conductivity of wall B are and respectively.
Here, the length and thermal conductivity of wall C are and respectively.
Calculate the heat flux.
Here, the temperature of air is and the temperature of the inner wall is .
Substitute for , for , for h, and for .
Calculate the thermal conductivity of material B.
Here, the outer wall temperature is .
Substitute for , for , for , for , for , for , for , for , 0.3 m for , 0.15 m for , and 0.15 m for .
Ans:
The thermal conductivity of material B, is .
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