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A wall has two layers A and B, each made...

A wall has two layers A and B, each made of different material. Both the layers have the same thickness. The thermal conductivity of the material of A is twice that of B . Under thermal equilibrium, the temperature difference across the wall is `36^@C.` The temperature difference across the layer A is

A

`12 .^(@)C`

B

`18 .^(@)C`

C

`6.^(@)C`

D

`24 .^(@)C`

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The correct Answer is:
To solve the problem step by step, we will analyze the thermal properties of the two layers A and B of the wall. ### Step 1: Define the Variables Let: - \( k \) = thermal conductivity of material B - \( 2k \) = thermal conductivity of material A (since it is twice that of B) - \( T_A \) = temperature at the left side of layer A - \( T_B \) = temperature at the right side of layer B - \( T \) = temperature at the junction between layers A and B - The thickness of both layers = \( t \) - The total temperature difference across the wall = \( T_B - T_A = 36^\circ C \) ### Step 2: Write the Heat Flow Equations According to Fourier's law of heat conduction, the heat flow \( Q \) through each layer can be expressed as: \[ Q = \frac{k \cdot A \cdot (T_A - T)}{t} \quad \text{(for layer A)} \] \[ Q = \frac{2k \cdot A \cdot (T - T_B)}{t} \quad \text{(for layer B)} \] Since the heat flow is constant in steady state, we can set the two equations equal to each other: \[ \frac{2k \cdot A \cdot (T_A - T)}{t} = \frac{k \cdot A \cdot (T - T_B)}{t} \] ### Step 3: Simplify the Equation We can cancel out \( k \), \( A \), and \( t \) from both sides: \[ 2(T_A - T) = (T - T_B) \] This simplifies to: \[ 2T_A - 2T = T - T_B \] Rearranging gives: \[ 3T = T_B + 2T_A \] ### Step 4: Use the Total Temperature Difference We know from the problem statement that: \[ T_B - T_A = 36^\circ C \] We can express \( T_B \) in terms of \( T_A \): \[ T_B = T_A + 36 \] ### Step 5: Substitute and Solve for \( T_A \) Substituting \( T_B \) into the equation \( 3T = T_B + 2T_A \): \[ 3T = (T_A + 36) + 2T_A \] This simplifies to: \[ 3T = 3T_A + 36 \] Thus, we can express \( T \) in terms of \( T_A \): \[ T = T_A + 12 \] ### Step 6: Find the Temperature Difference Across Layer A Now, we can find the temperature difference across layer A: \[ \Delta T_A = T_A - T = T_A - (T_A + 12) = -12^\circ C \] This means the temperature difference across layer A is: \[ \Delta T_A = 12^\circ C \] ### Final Answer The temperature difference across layer A is \( 12^\circ C \).

To solve the problem step by step, we will analyze the thermal properties of the two layers A and B of the wall. ### Step 1: Define the Variables Let: - \( k \) = thermal conductivity of material B - \( 2k \) = thermal conductivity of material A (since it is twice that of B) - \( T_A \) = temperature at the left side of layer A - \( T_B \) = temperature at the right side of layer B ...
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