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Question: A system consists of a cylinder surrounded by a cylindrical shell. A cylinder is a radius R and is m...

A system consists of a cylinder surrounded by a cylindrical shell. A cylinder is a radius R and is made of material of thermal conductivity K, whereas a cylindrical shell has an inner radius R and outer radius 2R and is made of material of thermal conductivity twice as that of cylinder. Assuming the system is in steady state and negligible heat loss across the cylindrical surface, find the effective thermal conductivity of the system, if the two ends of the combined system are maintained at two different temperatures.
A) 3K \\\
B) \dfrac{2}{3}K \\\
C) \dfrac{{7K}}{4} \\\
D) 5K4 \dfrac{{5K}}{4} \\\

Explanation

Solution

Whenever heat energy is transferred through conduction, due to the inherent property of the material, it offers obstruction to the flow of heat energy through it. This obstruction is called thermal energy.
The formula for the thermal resistance of a cylindrical surface is –
R=LK.A where  R = \dfrac{L}{{K.A}} \\\ where \\\
L = length of the cylinder
K = thermal conductivity
A = area of cross-section
The net-effective resistance for a parallel combination of individual bodies is given by the formula –
1Req=1R1+1R2\dfrac{1}{{{R_{eq}}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}}

Complete step by step answer:
Here is the diagram of the cylinder covered by the cylindrical shell.

The ends of the cylinders are maintained at the temperature T1{T_1} and T2{T_2}. Since, the heat flows through both the cylinders together at the same time, we need to use the condition of parallel combination.
The thermal resistance offered by the cylinder –
\Rightarrow R1=L1K1A1=LK(πR2){R_1} = \dfrac{{{L_1}}}{{{K_1}{A_1}}} = \dfrac{L}{{K\left( {\pi {R^2}} \right)}}
The thermal resistance offered by the cylindrical shell –
\Rightarrow R2=L2K2A2=LK(π(2R)2πR2)=LK(4πR2πR2)=LK(3πR2){R_2} = \dfrac{{{L_2}}}{{{K_2}{A_2}}} = \dfrac{L}{{K\left( {\pi {{\left( {2R} \right)}^2} - \pi {R^2}} \right)}} = \dfrac{L}{{K\left( {4\pi {R^2} - \pi {R^2}} \right)}} = \dfrac{L}{{K(3\pi {R^2})}}
Since, the heat flows through both the cylinders together at the same time, the net effective thermal resistance is equal to the parallel combination of the cylinders:
\Rightarrow 1Req=1R1+1R2\dfrac{1}{{{R_{eq}}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}}
On solving, we get:
\Rightarrow Req=R1R2R1+R2{R_{eq}} = \dfrac{{{R_1}{R_2}}}{{{R_1} + {R_2}}}
Substituting the values of the resistances, we get:

Req=R1R2R1+R2 Req=LK1(πR2).LK2(3πR2)LK1(πR2)+LK2(3πR2) Req=L23LK2πR2+LK1πR2 \Rightarrow {R_{eq}} = \dfrac{{{R_1}{R_2}}}{{{R_1} + {R_2}}} \\\ \Rightarrow {R_{eq}} = \dfrac{{\dfrac{L}{{{K_1}\left( {\pi {R^2}} \right)}}.\dfrac{L}{{{K_2}\left( {3\pi {R^2}} \right)}}}}{{\dfrac{L}{{{K_1}\left( {\pi {R^2}} \right)}} + \dfrac{L}{{{K_2}\left( {3\pi {R^2}} \right)}}}} \\\ \Rightarrow {R_{eq}} = \dfrac{{{L^2}}}{{3L{K_2}\pi {R^2} + L{K_1}\pi {R^2}}} \\\

Substituting
\Rightarrow Req=LKeqA=LKeq(2πR)2{R_{eq}} = \dfrac{L}{{{K_{eq}}A}} = \dfrac{L}{{{K_{eq}}{{\left( {2\pi R} \right)}^2}}}
Equating the values of Req{R_{eq}}, we get –
L4KeqπR2=L23LK2πR2+LK1πR2 L4KeqπR2=L2LπR2(3K2+K1) rearranging, 4Keq=K1+3K2  \Rightarrow \dfrac{L}{{4{K_{eq}}\pi {R^2}}} = \dfrac{{{L^2}}}{{3L{K_2}\pi {R^2} + L{K_1}\pi {R^2}}} \\\ \Rightarrow \dfrac{L}{{4{K_{eq}}\pi {R^2}}} = \dfrac{{{L^2}}}{{L\pi {R^2}\left( {3{K_2} + {K_1}} \right)}} \\\ rearranging, \\\ \Rightarrow 4{K_{eq}} = {K_1} + 3{K_2} \\\
As per the problem,
K1=K K2=2K  \Rightarrow {K_1} = K \\\ \Rightarrow {K_{_2}} = 2K \\\
Substituting these values in the above equation, we get –
4Keq=K1+3K2 4Keq=K+3(2K) 4Keq=7K Keq=74K  \Rightarrow 4{K_{eq}} = {K_1} + 3{K_2} \\\ \Rightarrow 4{K_{eq}} = K + 3\left( {2K} \right) \\\ \Rightarrow 4{K_{eq}} = 7K \\\ \Rightarrow {K_{eq}} = \dfrac{7}{4}K \\\
Hence, the correct option is Option C.

Note: The concept of thermal resistance is like that of electrical resistance. So, when in doubt, you can draw up the analogies between the two of them and compare the analogous quantities so that you have a better understanding of solving the problem.