A cylinder of radius R made of a material of thermal conductivity K1 is surrounded by a cylindrical shell of inner radiusRand outer radius 2Rmade of material of thermal conductivity K2. The two ends of the combined system are maintained at two different temperatures. There is no loss of heat across the cylindrical surface and the system is in steady state. The effective thermal conductivity of the system is
Both the cylinders are in parallel, for the heat flow from one end as shown.
Hence Keq = K1A1 + K2A2A1 + A2 ; where A1 = Area of
cross-section of inner cylinder = πR2 and
A2 = Area of cross-section of cylindrical shell
= π {(2R)2 − (R)2} = 3 π R2
⇒Keq = K1(πR2) + K2(3πR2)πR2 + 3πR2 = K1 + 3K24