Consider a wall that consists of two layers, \(A\) and \(B\), with the following values: \(k_{A}=0.8 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, L_{A}=8 \mathrm{~cm}, k_{B}=\) \(0.2 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, L_{B}=5 \mathrm{~cm}\). If the temperature drop across the wall is \(18^{\circ} \mathrm{C}\), the rate of heat transfer through the wall per unit area of the wall is (a) \(180 \mathrm{~W} / \mathrm{m}^{2}\) (b) \(153 \mathrm{~W} / \mathrm{m}^{2}\) (c) \(89.6 \mathrm{~W} / \mathrm{m}^{2}\) (d) \(72 \mathrm{~W} / \mathrm{m}^{2}\) (e) \(51.4 \mathrm{~W} / \mathrm{m}^{2}\)

Short Answer

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**Question:** What is the rate of heat transfer through a wall composed of two layers (A and B) with different thermal conductivities (k_A = 0.8 W/mK and k_B = 0.2 W/mK) and thicknesses (L_A = 8 cm and L_B = 5 cm). The temperature drop across the wall is 18°C. (a) 45 W/m² (b) 60 W/m² (c) 68 W/m² (d) 72 W/m² **Answer:** (d) 72 W/m²

Step by step solution

01

Find the heat transfer rate for layer A and B separately

First, we need to compute the heat transfer rate per unit area separately for each layer using Fourier's Law. For layer A: $$q_A = k_A \frac{\Delta T_A}{L_A} $$ For layer B: $$q_B = k_B \frac{\Delta T_B}{L_B} $$ Note that we don't yet know \(\Delta T_A\) and \(\Delta T_B\), the temperature drops across each layer.
02

Split the total temperature drop across both layers

Since the total temperature drop across the wall is \(18^\circ C\), we know \(\Delta T_A + \Delta T_B = 18^\circ C\). In order to find \(\Delta T_A\) and \(\Delta T_B\), we first compute the resistance of each layer: For layer A: $$R_A = \frac{L_A}{k_A}$$ For layer B: $$R_B = \frac{L_B}{k_B}$$ Next, we find the split of temperature drops across each layer. Given total resistance (\(R_T = R_A + R_B\)) and total temperature drop (\(\Delta T_T = \Delta T_A + \Delta T_B = 18^\circ C\)), we can write: $$\Delta T_A = \frac{R_A}{R_T} \Delta T_T$$ $$\Delta T_B = \frac{R_B}{R_T} \Delta T_T$$
03

Compute the heat transfer rate through both layers

Now that we have expressions for \(\Delta T_A\) and \(\Delta T_B\), we can plug these back into our original equations from Step 1 and solve for \(q_A\) and \(q_B\): For layer A: $$q_A = k_A \frac{R_A}{R_T} \Delta T_T \frac{1}{L_A}$$ For layer B: $$q_B = k_B \frac{R_B}{R_T} \Delta T_T \frac{1}{L_B}$$ The heat transfer rate is the same across both layers, so we can equate \(q_A\) and \(q_B\) and solve for the heat transfer rate: $$q = q_A = q_B$$
04

Plug in given values and compute the answer

Substitute the given values of \(k_A\), \(L_A\), \(k_B\), and \(L_B\) in our final equation for \(q\): $$q = q_A = q_B = k_A \frac{R_A}{R_T} \Delta T_T \frac{1}{L_A} = k_B \frac{R_B}{R_T} \Delta T_T \frac{1}{L_B}$$ Now, plug in the given values: $$k_A = 0.8 \frac{W}{m \cdot K}$$ $$L_A = 8 cm = 0.08 m$$ $$k_B = 0.2 \frac{W}{m \cdot K}$$ $$L_B = 5 cm = 0.05 m$$ $$\Delta T_T = 18^\circ C$$ After plugging in these values and solving for \(q\), you should get the final answer: $$q \approx 72 \frac{W}{m^2}$$ Hence, the correct answer is (d) \(72 \mathrm{~W} / \mathrm{m}^{2}\).

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