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A hot plane surface at \(100^{\circ} \mathrm{C}\) is exposed to air at \(25^{\circ} \mathrm{C}\) with a combined heat transfer coefficient of $20 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$. The heat loss from the surface is to be reduced by half by covering it with sufficient insulation with a thermal conductivity of \(0.10 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). Assuming the heat transfer coefficient to remain constant, the required thickness of insulation is (a) \(0.1 \mathrm{~cm}\) (b) \(0.5 \mathrm{~cm}\) (c) \(1.0 \mathrm{~cm}\) (d) \(2.0 \mathrm{~cm}\) (e) \(5 \mathrm{~cm}\)

Short Answer

Expert verified
Answer: 1 cm.

Step by step solution

01

Calculate initial heat loss

To calculate the initial heat loss (Q_initial), we can use the equation for heat loss by convection: Q_initial = hA(T_surface - T_ambient) where h is the heat transfer coefficient, A is the area of the surface, T_surface is the surface temperature, and T_ambient is the ambient temperature. Given h = 20 W/(m^2∙K), T_surface = 100°C, and T_ambient = 25°C, we can calculate Q_initial: Q_initial = 20 A (100 - 25) = 20A(75)
02

Calculate heat loss with insulation

To find the heat loss with insulation (Q_insulation), we simply divide the initial heat loss by 2: Q_insulation = Q_initial / 2 = (20A(75))/2
03

Use heat transfer by conduction to find insulation thickness

The equation for heat transfer by conduction is: Q_insulation = (kAΔT)/L where k is the thermal conductivity of insulation, ΔT is the temperature difference between the surface and ambient air, and L is the insulation thickness. Given k = 0.10 W/(m∙K), we can rearrange the equation to find L: L = (kAΔT)/Q_insulation L = (0.10A(75))/((20A(75))/2) We can see the terms A and 75 can be canceled out in both the numerator and the denominator: L = (0.10)/((20)/2) Now we can solve for the insulation thickness L: L = (0.10)/(10) = 0.01 m = 1 cm The required insulation thickness is 1 cm, which corresponds to option (c) in the multiple-choice question.

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Most popular questions from this chapter

Steam at \(260^{\circ} \mathrm{C}\) is flowing inside a steel pipe $(k=61 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})$ whose inner and outer diameters are \(10 \mathrm{~cm}\) and \(12 \mathrm{~cm}\), respectively, in an environment at \(20^{\circ} \mathrm{C}\). The heat transfer coefficients inside and outside the pipe are 120 \(\mathrm{W} / \mathrm{m}^{2}, \mathrm{~K}\) and $14 \mathrm{~W} / \mathrm{m}^{2}, \mathrm{~K}\(, respectively. Determine \)(a)$ the thickness of the insulation $(k=0.038 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\( needed to reduce the heat loss by 95 percent and \)(b)$ the thickness of the insulation needed to reduce the exposed surface temperature of insulated pipe to \(40^{\circ} \mathrm{C}\) for safety reasons.

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) \(221 \mathrm{~W}\)

A \(20-\mathrm{cm}\)-diameter hot sphere at \(120^{\circ} \mathrm{C}\) is buried in the ground with a thermal conductivity of $1.2 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}$. The distance between the center of the sphere and the ground surface is \(0.8 \mathrm{~m}\), and the ground surface temperature is \(15^{\circ} \mathrm{C}\). The rate of heat loss from the sphere is (a) \(169 \mathrm{~W}\) (b) \(20 \mathrm{~W}\) (c) \(217 \mathrm{~W}\) (d) \(312 \mathrm{~W}\) (e) \(1.8 \mathrm{~W}\)

Using a timer (or watch) and a thermometer, conduct this experiment to determine the rate of heat gain of your refrigerator. First, make sure that the door of the refrigerator is not opened for at least a few hours to make sure that steady operating conditions are established. Start the timer when the refrigerator stops running, and measure the time \(\Delta t_{1}\) it stays off before it kicks in. Then measure the time \(\Delta t_{2}\) it stays on. Noting that the heat removed during \(\Delta t_{2}\) is equal to the heat gain of the refrigerator during \(\Delta t_{1}+\Delta t_{2}\) and using the power consumed by the refrigerator when it is running, determine the average rate of heat gain for your refrigerator, in watts. Take the COP (coefficient of performance) of your refrigerator to be \(1.3\) if it is not available. Now, clean the condenser coils of the refrigerator and remove any obstacles in the way of airflow through the coils. Then determine the improvement in the COP of the refrigerator.

In a combined heat and power (CHP) generation process, by-product heat is used for domestic or industrial heating purposes. Hot steam is carried from a CHP generation plant by a tube with diameter of \(127 \mathrm{~mm}\) centered at a square crosssection solid bar made of concrete with thermal conductivity of \(1.7 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The surface temperature of the tube is constant at \(120^{\circ} \mathrm{C}\), while the square concrete bar is exposed to air with temperature of \(-5^{\circ} \mathrm{C}\) and convection heat transfer coefficient of \(20 \mathrm{~W} / \mathrm{m}^{2}\). \(\mathrm{K}\). If the temperature difference between the outer surface of the square concrete bar and the ambient air is to be maintained at $5^{\circ} \mathrm{C}$, determine the width of the square concrete bar and the rate of heat loss per meter length. Answers: $1.32 \mathrm{~m}, 530 \mathrm{~W} / \mathrm{m}$

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