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Consider two walls, \(A\) and \(B\), with the same surface areas and the same temperature drops across their thicknesses. The ratio of thermal conductivities is \(k_{A} / k_{B}=4\) and the ratio of the wall thicknesses is \(L_{A} / L_{B}=2\). The ratio of heat transfer rates through the walls \(\dot{Q}_{A} / \dot{Q}_{B}\) is (a) \(0.5\) (b) 1 (c) 2 (d) 4 (e) 8

Short Answer

Expert verified
Answer: The ratio of heat transfer rates through the walls A and B is 2:1.

Step by step solution

01

Recall the formula for heat transfer rate

The formula for the heat transfer rate (Q) through a wall is given by: $$ \dot{Q} = \frac{k A \Delta T}{L} $$ Where \(\dot{Q}\) is the heat transfer rate, k is the thermal conductivity, A is the surface area, \(\Delta T\) is the temperature drop across the wall, and L is the wall thickness.
02

Write the equation for heat transfer rate ratio

We want to find the ratio of the heat transfer rates for wall A and wall B. Using the formula from Step 1, we can write the equation as follows: $$ \frac{\dot{Q}_{A}}{\dot{Q}_{B}} = \frac{\frac{k_{A} A \Delta T_{A}}{L_{A}}}{\frac{k_{B} A \Delta T_{B}}{L_{B}}} $$
03

Simplify the equation and plug the given ratios

Notice that the surface areas and temperature drops across both walls are the same, so those will cancel out. We can simplify the equation and insert the given ratios into the equation, such as: $$ \frac{\dot{Q}_{A}}{\dot{Q}_{B}} = \frac{k_{A} L_{B}}{k_{B} L_{A}} = \frac{\frac{k_{A}}{k_{B}}}{\frac{L_{A}}{L_{B}}} $$ We are given that \(\frac{k_{A}}{k_{B}} = 4\) and \(\frac{L_{A}}{L_{B}} = 2\). Plugging these values into the equation, we get: $$ \frac{\dot{Q}_{A}}{\dot{Q}_{B}} = \frac{4}{2} $$
04

Calculate the heat transfer rate ratio

Now we can simply calculate the heat transfer rate ratio from the equation: $$ \frac{\dot{Q}_{A}}{\dot{Q}_{B}} = \frac{4}{2} = 2 $$ So, the ratio of heat transfer rates through the walls is 2, which corresponds to option (c).

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Most popular questions from this chapter

The overall heat transfer coefficient (the \(U\)-value) of a wall under winter design conditions is \(U=1.40 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Determine the \(U\)-value of the wall under summer design conditions.

Consider a wall that consists of two layers, \(A\) and \(B\), with the following values: $k_{A}=1.2 \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) \(56.8 \mathrm{~W} / \mathrm{m}^{2}\) (b) \(72.1 \mathrm{~W} / \mathrm{m}^{2}\) (c) \(114 \mathrm{~W} / \mathrm{m}^{2}\) (d) \(201 \mathrm{~W} / \mathrm{m}^{2}\) (e) \(270 \mathrm{~W} / \mathrm{m}^{2}\)

Heat is lost at a rate of \(275 \mathrm{~W}\) per \(\mathrm{m}^{2}\) area of a 15 -cm-thick wall with a thermal conductivity of $k=1.1 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}$. The temperature drop across the wall is (a) \(37.5^{\circ} \mathrm{C}\) (b) \(27.5^{\circ} \mathrm{C}\) (c) \(16.0^{\circ} \mathrm{C}\) (d) \(8.0^{\circ} \mathrm{C}\) (e) \(4.0^{\circ} \mathrm{C}\)

Determine the winter \(R\)-value and the \(U\)-factor of a masonry cavity wall that consists of \(100-\mathrm{mm}\) common bricks, a \(90-\mathrm{mm}\) airspace, \(100-\mathrm{mm}\) concrete blocks made of lightweight aggregate, 20 -mm airspace, and \(13-\mathrm{mm}\) gypsum wallboard separated from the concrete block by \(20-\mathrm{mm}\)-thick (1-in \(\times 3\)-in nominal) vertical furring whose center-to-center distance is \(400 \mathrm{~mm}\). Neither side of the two airspaces is coated with any reflective films. When determining the \(R\)-value of the airspaces, the temperature difference across them can be taken to be \(16.7^{\circ} \mathrm{C}\) with a mean air temperature of $10^{\circ} \mathrm{C}$. The airspace constitutes 84 percent of the heat transmission area, while the vertical furring and similar structures constitute 16 percent.

A 2.2-mm-diameter and 14-m-long electric wire is tightly wrapped with a \(1-\mathrm{mm}\)-thick plastic cover whose thermal conductivity is $k=0.15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}$. Electrical measurements indicate that a current of \(13 \mathrm{~A}\) passes through the wire, and there is a voltage drop of \(8 \mathrm{~V}\) along the wire. If the insulated wire is exposed to a medium at \(T_{\infty}=30^{\circ} \mathrm{C}\) with a heat transfer coefficient of \(h=24 \mathrm{~W} / \mathrm{m}^{2}\), \(\mathrm{K}\), determine the temperature at the interface of the wire and the plastic cover in steady operation. Also determine if doubling the thickness of the plastic cover will increase or decrease this interface temperature.

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