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A 2.1-m-long, 0.2-cm-diameter electrical wire extends across a room that is maintained at \(20^{\circ} \mathrm{C}\). Heat is generated in the wire as a result of resistance heating, and the surface temperature of the wire is measured to be \(180^{\circ} \mathrm{C}\) in steady operation. Also, the voltage drop and electric current through the wire are measured to be \(110 \mathrm{~V}\) and \(3 \mathrm{~A}\), respectively. Disregarding any heat transfer by radiation, determine the convection heat transfer coefficient for heat transfer between the outer surface of the wire and the air in the room. Answer: \(156 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\)

Short Answer

Expert verified
Based on the given step by step solution, the convection heat transfer coefficient for heat transfer between the outer surface of the wire and the air in the room is calculated to be 156 W/m²·K.

Step by step solution

01

Calculate the power generated by resistance heating

To calculate the power generated by resistance heating, we can use the following formula: \(P = VI\) where P is the power, V is the voltage drop, and I is the electric current. In this case, V = 110 V, and I = 3 A. Therefore, the power generated is: \(P = (110 \mathrm{~V})(3 \mathrm{~A}) = 330 \mathrm{~W}\)
02

Calculate the surface area of the wire

The surface area (A) of a cylinder can be calculated using the following formula: \(A = 2 \pi rL\), where r is the radius, and L is the length of the wire. In this case, the diameter of the wire is 0.2 cm, which means the radius is 0.1 cm or 0.001 m, and the length is 2.1 m. Therefore, the surface area of the wire is: \(A = 2\pi(0.001\mathrm{~m})(2.1\mathrm{~m})=0.0132\mathrm{~m}^2\)
03

Calculate total heat transfer by convection

Now that we have the power generated (P) and the surface area of the wire (A), we can calculate the total heat transfer (Q) by convection using the following formula: \(Q = P - Q_{rad}\) Since we're disregarding any heat transfer by radiation (Q_rad = 0), the total heat transfer by convection (Q) is equal to the power generated (P): \(Q = 330 \mathrm{~W}\)
04

Calculate the convection heat transfer coefficient

Finally, we can calculate the convection heat transfer coefficient (h) using the following formula: \(h = \frac{Q}{A(T_s - T_{room})}\) where \(T_s\) is the surface temperature of the wire, and \(T_{room}\) is the room temperature. In this case, T_s = 180°C, and T_room = 20°C, so \(T_s - T_{room} = 180 - 20 = 160 \mathrm{~K}\). Therefore, the convection heat transfer coefficient is: \(h = \frac{330 \mathrm{~W}}{(0.0132\mathrm{~m}^2)(160\mathrm{~K})}=156\mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) The convection heat transfer coefficient for heat transfer between the outer surface of the wire and the air in the room is 156 W/m²·K.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Resistance Heating
Resistance heating is a process where electrical energy is converted into heat as an electrical current passes through a resistant material. In the context of our exercise, an electrical wire acts as the resistor. When current flows through the wire, the electrical resistance of the wire causes it to heat up.

The power generated can be calculated using the formula:
\(P = VI\), where \(P\) is the power in watts (W), \(V\) is the voltage in volts (V), and \(I\) is the current in amperes (A). To put this into perspective, if a wire in our exercise has a voltage drop of 110 V and carries a current of 3 A, the power generated by resistance heating is \(P = 110 V \times 3 A = 330 W\). This amount of power consequently raises the wire's temperature, which can be observed by its surface temperature.
Heat Transfer by Convection
Heat transfer by convection occurs when heat is carried away from the surface of an object by a fluid such as air or water. In our exercise, the wire is surrounded by air at a lower temperature, and heat flows from the wire into the air.

To describe this process quantitatively, we introduce the convection heat transfer coefficient (\(h\)), which is measured in watts per square meter per kelvin (\(W/m^2\cdot K\)). The coefficient represents the efficiency of heat transfer from the wire's surface to the surrounding air.

Our goal is to determine the value of \(h\) for our specific setup. We already know that radiation is disregarded, simplifying our calculation. We use the formula:
\(h = \frac{Q}{A(T_s - T_{\text{room}})}\), where \(A\) is the wire's surface area, \(T_s\) is the wire's surface temperature, and \(T_{\text{room}}\) is the room's air temperature. By calculating the values of \(A\) and \(Q\) from the wire's dimensions and power generated, we can solve for \(h\). In the given problem, the convection heat transfer coefficient is found to be 156 \(W/m^2\cdot K\), indicating the rate of heat loss per unit area per degree of temperature difference between the wire and the surrounding air.
Thermal Analysis of Electrical Wire
The thermal analysis of electrical wire involves understanding how the wire's temperature changes under the influence of current flow and the subsequent heat transfer to its surroundings. Our thermal analysis is crucial for determining the safe operating conditions of the wire and ensuring it does not overheat and cause damage or fire.

Such an analysis will consider factors such as the wire's material, its physical dimensions (diameter and length, which determine the surface area), the ambient temperature, and the properties of the surrounding medium (usually air). In the context of the given exercise, the wire attains a steady-state temperature of \(180^\circ C\) because the generated heat by resistance heating is balanced by the heat lost through convection.

The thermal analysis allows us to calculate essential parameters, like the convection heat transfer coefficient (\(h\)), which serves as an indicator of the wire's ability to dissipate heat into the environment. Ensuring the wire does not exceed certain temperature thresholds is vital for safety and maintaining the integrity of electrical systems.

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Most popular questions from this chapter

Heat is lost steadily through a \(0.5-\mathrm{cm}\) thick \(2 \mathrm{~m} \times 3 \mathrm{~m}\) window glass whose thermal conductivity is \(0.7 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The inner and outer surface temperatures of the glass are measured to be \(12^{\circ} \mathrm{C}\) to \(9^{\circ} \mathrm{C}\). The rate of heat loss by conduction through the glass is (a) \(420 \mathrm{~W}\) (b) \(5040 \mathrm{~W}\) (c) \(17,600 \mathrm{~W}\) (d) \(1256 \mathrm{~W}\) (e) \(2520 \mathrm{~W}\)

Solar radiation is incident on a \(5 \mathrm{~m}^{2}\) solar absorber plate surface at a rate of \(800 \mathrm{~W} / \mathrm{m}^{2}\). Ninety-three percent of the solar radiation is absorbed by the absorber plate, while the remaining 7 percent is reflected away. The solar absorber plate has a surface temperature of \(40^{\circ} \mathrm{C}\) with an emissivity of \(0.9\) that experiences radiation exchange with the surrounding temperature of \(-5^{\circ} \mathrm{C}\). In addition, convective heat transfer occurs between the absorber plate surface and the ambient air of \(20^{\circ} \mathrm{C}\) with a convection heat transfer coefficient of \(7 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Determine the efficiency of the solar absorber, which is defined as the ratio of the usable heat collected by the absorber to the incident solar radiation on the absorber.

A 2-kW electric resistance heater submerged in 30-kg water is turned on and kept on for \(10 \mathrm{~min}\). During the process, \(500 \mathrm{~kJ}\) of heat is lost from the water. The temperature rise of water is (a) \(5.6^{\circ} \mathrm{C}\) (b) \(9.6^{\circ} \mathrm{C}\) (c) \(13.6^{\circ} \mathrm{C}\) (d) \(23.3^{\circ} \mathrm{C}\) (e) \(42.5^{\circ} \mathrm{C}\)

Four power transistors, each dissipating \(12 \mathrm{~W}\), are mounted on a thin vertical aluminum plate \(22 \mathrm{~cm} \times 22 \mathrm{~cm}\) in size. The heat generated by the transistors is to be dissipated by both surfaces of the plate to the surrounding air at \(25^{\circ} \mathrm{C}\), which is blown over the plate by a fan. The entire plate can be assumed to be nearly isothermal, and the exposed surface area of the transistor can be taken to be equal to its base area. If the average convection heat transfer coefficient is \(25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), determine the temperature of the aluminum plate. Disregard any radiation effects.

The inner and outer surfaces of a \(25-\mathrm{cm}\)-thick wall in summer are at \(27^{\circ} \mathrm{C}\) and \(44^{\circ} \mathrm{C}\), respectively. The outer surface of the wall exchanges heat by radiation with surrounding surfaces at \(40^{\circ} \mathrm{C}\), and convection with ambient air also at \(40^{\circ} \mathrm{C}\) with a convection heat transfer coefficient of \(8 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Solar radiation is incident on the surface at a rate of \(150 \mathrm{~W} / \mathrm{m}^{2}\). If both the emissivity and the solar absorptivity of the outer surface are \(0.8\), determine the effective thermal conductivity of the wall.

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