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Three rods of material X and three rods of material Y are connected as shown in the figure. All the rods are of identical length and cross-sectional area. If the end A is maintained at `60^@C` and the junction E at `10^@C`. Calculate the temperature of the junction B, C and D. The thermal conductivity of X is `0.92cal//sec-cm^@C` and that of Y is `0.46cal//sec-cm-^@C`.
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Let `K_(x)` and `K_(y)` be the thermal conductivites of X and Y respectively, and let `T_(B), T_(C)` and `T_(D)` be the temperature of junctions B,C and D, respectively Given `T_(A)=60^(@)C` and `T_(E)=10^(@)C`. In order to solve this problem, we will apply the principle that, in the steady state, the rate at which heat enters a junction is equal to the rate at which heat leaves that junction. In Fig. 1.63, the direction of flow of heat is given by arrows.
For junction B, we have
image
`(K_(y)A(T_(A)-T_(B)))/(d)=(K_(x)A(T_(B)-T_(C)))/(d)+(K_(y)A(T_(B)-T_(C)))/(d)`
or `K_(y)(T_(A)-T_(B))=Kx(T_(B)-T_(C))+K_(y)(T_(B)-T_(D))`
or `(T_(A)-T_(B))=(K_(x))/(K_(y))(T_(B)-T_(C))+K_(y)(T_(B)-T_(D))`
Given `(K_(x))/(K_(y))=(9.2xx10^(-2))/(4.6xx10^(-2))=2` and `T_(A)=60^(@)C`. Therefore
`(60-T_(B))=2(T_(B)-T_(C))+(T_(B)-T_(C))+(T_(B)-T_(D))`
or `4T_(B)-2T_(C)-T_(D)=60` (i)
For junction C, we have
`(K_(x)A(T_(B)-T_(C)))/(d)=(K_(x)A(T_(C)-T_(D)))/(d)+(K_(x)A(T_(C)-T_(B)))/(d)`
Solving we get
`-T_(B)+3T_(C)-T_(D)=10 ["At" T_(E)=10^(@)C]` (ii)
For junction D, we have
or `(K_(y)A(T_(B)-T_(D)))/(d)+(K_(x)A(T_(C)-T_(D)))/(d)=(K_(y)A(T_(D)-T_(E)))/(d)`
or `(T_(B)-T_(D))+(K_(x))/(K_(y))=2` and `T_(E)=10^(@)C`. In this equation, we have
`(T_(B)-T_(D))+2(T_(C)-T_(D))=(T_(D)-10)`
`T_(B)+2T_(C)-4T_(D)=-10` (iii)
Solving Eqs. (i),(ii) and (iii), we get
`T_(B)=30^(@)C` and `T_(C)=T_(D)=20^(@)C`

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