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Question: Two bars of thermal conductivities \[K\] and \[3K\] and lengths \[1{\text{ cm}}\] and \[{\text{2 cm}...

Two bars of thermal conductivities KK and 3K3K and lengths 1 cm1{\text{ cm}} and 2 cm{\text{2 cm}} respectively have equal cross-sectional area. They are joined lengthwise as shown in the figure. If the temperature of the ends of the composite bar is 0C{0^ \circ }C and 100C{100^ \circ }C respectively (see figure), then the temperature of the interface (φ)\left( \varphi \right) is
A. 50C{50^ \circ }C
B. 1003C{\dfrac{{100}}{3}^ \circ }C
C. 60C{60^ \circ }C
D. 2003C{\dfrac{{200}}{3}^ \circ }C

Explanation

Solution

In this question, we need to find the temperature of the interface of two composite slabs. As they are connected in series the heat current through both the slabs must be equal. Assume the temperature as TC{T^ \circ }C and write the heat current for both slabs and equate them as they must be equal. On solving, we get the temperature of interface

Formula used:
H=dQdt=KAdTdx=KA(T1T2)lH = \dfrac{{dQ}}{{dt}} = - KA\dfrac{{dT}}{{dx}} = KA\dfrac{{\left( {{T_1} - {T_2}} \right)}}{l}
Where HH is the heat current, KK is the thermal conductivity, dTdT is the temperature difference and ll is the length of the slab.

Complete step by step answer:
We are given two bars of thermal conductivities KK and 3K3K.
The Length of the first bar is, l1=1 cm{l_1} = 1{\text{ }}cm
The Length of the second bar is, l2=2 cm{l_2} = 2{\text{ }}cm
The Area of cross-section of both the bars is AA
T1=0C{T_1} = {0^ \circ }C
T2=100C\Rightarrow {T_2} = {100^ \circ }C
Let the temperature of the interface be TC{T^ \circ }C
Heat current through the first composite slab,
H=KA(T1T)1H = KA\dfrac{{\left( {{T_1} - T} \right)}}{1}
Heat current through the second composite slab,
H=3KA(TT2)2H = 3KA\dfrac{{\left( {T - {T_2}} \right)}}{2}

But heat current through both the slabs must be equal. Therefore,
KA(T1T)1=3KA(TT2)2KA\dfrac{{\left( {{T_1} - T} \right)}}{1} = 3KA\dfrac{{\left( {T - {T_2}} \right)}}{2}
Dividing both sides by KAKA we get,
T1T=32(TT2)\Rightarrow {T_1} - T = \dfrac{3}{2}\left( {T - {T_2}} \right)
Substituting T1=0C{T_1} = {0^ \circ }C and T2=100C{T_2} = {100^ \circ }C we get,
T=32(T100)\Rightarrow - T = \dfrac{3}{2}\left( {T - 100} \right)
52T=150\Rightarrow \dfrac{5}{2}T = 150
T=60C\therefore T = {60^ \circ }C
Hence, the temperature of the interference of the two composite blocks is60C{60^ \circ }C.

Therefore, the correct option is C.

Note: The negative signed use is H=dQdt=KAdTdxH = \dfrac{{dQ}}{{dt}} = - KA\dfrac{{dT}}{{dx}} is used to make dQdt\dfrac{{dQ}}{{dt}} a positive quantity since dTdx\dfrac{{dT}}{{dx}} is a negative quantity. The constant KK , called thermal conductivity, is the measure of the ability of the material to conduct heat. A substance with a large value of KK means it is a good conductor of heat. The value of KK depends on temperature but can be taken practically constant if the temperature difference between the two ends of the substance is not too great.