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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) \(4.0^{\circ} \mathrm{C}\)

Short Answer

Expert verified
Answer: (a) 37.5°C

Step by step solution

01

Write down the Fourier's law of conductive heat transfer formula

The formula for Fourier's law of conductive heat transfer is: \(Q = -kA \frac{dT}{dx}\), where \(Q\) is the heat transfer rate, \(k\) is the thermal conductivity, \(A\) is the area of the wall, \(dT\) is the temperature difference across the wall (temperature drop), \(dx\) is the thickness of the wall. Since we already know the heat transfer rate per unit area (Q/A), we can rewrite the formula as: \(\frac{Q}{A} = -k \frac{dT}{dx}\)
02

Convert all units to SI units

To make all the calculations easier, convert the thickness of the wall from centimeters to meters: Thickness of the wall in meters: \(15 \mathrm{~cm} \times \frac{1 \mathrm{~m}}{100 \mathrm{~cm}} = 0.15 \mathrm{~m}\)
03

Plug in the given values into the formula

Now, we can plug the given values to the equation: \(\frac{275 \mathrm{~W}}{\mathrm{m^2}} = 1.1 \mathrm{~W/(m \cdot K)} \frac{dT}{0.15 \mathrm{~m}}\)
04

Solve for the temperature drop (ΔT)

Now, let's solve the equation for the temperature drop, \(dT\): \(dT = \frac{275 \mathrm{~W} \cdot 0.15 \mathrm{~m}}{1.1 \mathrm{~W/(m \cdot K)} \cdot \mathrm{m^2}}\) \(dT \approx 37.5 \mathrm{~K}\) Since we can interpret a temperature difference in Kelvins as the same temperature difference in Celsius, we can also write the temperature drop as \(37.5^{\circ} \mathrm{C}\). So, the correct answer is (a) \(37.5^{\circ} \mathrm{C}\).

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Most popular questions from this chapter

The walls of a food storage facility are made of a 2 -cm-thick layer of wood \((k=0.1 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) in contact with a 5 -cm- thick layer of polyurethane foam $(k=0.03 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\(. If the temperature of the surface of the wood is \)-10^{\circ} \mathrm{C}$ and the temperature of the surface of the polyurethane foam is \(20^{\circ} \mathrm{C}\), the temperature of the surface where the two layers are in contact is (a) \(-7^{\circ} \mathrm{C}\) (b) \(-2^{\circ} \mathrm{C}\) (c) \(3^{\circ} \mathrm{C}\) (d) \(8^{\circ} \mathrm{C}\) (e) \(11^{\circ} \mathrm{C}\)

A \(0.083\)-in-diameter electrical wire at \(90^{\circ} \mathrm{F}\) is covered by \(0.02\)-in-thick plastic insulation $\left(k=0.075 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft} \cdot{ }^{\circ} \mathrm{F}\right)$. The wire is exposed to a medium at \(50^{\circ} \mathrm{F}\), with a combined convection and radiation heat transfer coefficient of $2.5 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft}^{2} \cdot{ }^{\circ} \mathrm{F}$. Determine if the plastic insulation on the wire will increase or decrease heat transfer from the wire. Answer: It helps

A 1-m-inner-diameter liquid-oxygen storage tank at a hospital keeps the liquid oxygen at \(90 \mathrm{~K}\). The tank consists of a \(0.5\)-cm-thick aluminum \((k=170 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) shell whose exterior is covered with a 10 -cm-thick layer of insulation \((k=0.02\) $\mathrm{W} / \mathrm{m} \cdot \mathrm{K})$. The insulation is exposed to the ambient air at \(20^{\circ} \mathrm{C}\), and the heat transfer coefficient on the exterior side of the insulation is \(5 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). The rate at which the liquid oxygen gains heat is (a) \(141 \mathrm{~W}\) (b) \(176 \mathrm{~W}\) (c) \(181 \mathrm{~W}\) (d) \(201 \mathrm{~W}\) (e) \(221 \mathrm{~W}\)

The fin efficiency is defined as the ratio of the actual heat transfer from the fin to (a) The heat transfer from the same fin with an adiabatic tip (b) The heat transfer from an equivalent fin which is infinitely long (c) The heat transfer from the same fin if the temperature along the entire length of the fin is the same as the base temperature (d) The heat transfer through the base area of the same fin (e) None of the above

The heat transfer surface area of a fin is equal to the sum of all surfaces of the fin exposed to the surrounding medium, including the surface area of the fin tip. Under what conditions can we neglect heat transfer from the fin tip?

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