/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 47 An electrical current of 700 A f... [FREE SOLUTION] | 91Ó°ÊÓ

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An electrical current of 700 A flows through a stainless steel cable having a diameter of \(5 \mathrm{~mm}\) and an electrical resistance of \(6 \times 10^{-4} \mathrm{\Omega} / \mathrm{m}\) (i.e., per meter of cable length). The cable is in environment having a temperature of \(30^{\circ} \mathrm{C}\), and the total coefficient associated with convection and radiation between the cable and the environment is approximately \(25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) If the cable is bare, what is its surface temperature? (b) If a very thin coating of electrical insulation is applied to the cable, with a contact resistance of \(0.02 \mathrm{~m}^{2}+\mathrm{K} / \mathrm{W}\), what are the insulation and cable surface temperatures? (c) There is some concern about the ability of the insulation to withstand elevated temperatures. What thickness of this insulation \((k=0.5 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) will yield the lowest value of the maximum insulation temperature? What is the valie of the maximum temperature when the thickness is used?

Short Answer

Expert verified
(a) Cable surface temperature is 66.9°C. (b) With insulation, cable is 73.4°C, insulation surface is 60.1°C. (c) Critical thickness is 0.02 m, maximum temperature is 37.3°C.

Step by step solution

01

Determine Heat Generated in the Cable

The heat generated in the cable due to electrical resistance can be determined using the formula for power loss in a resistor: \[ P = I^2 imes R \]where:- \( I = 700 \) A is the current,- \( R = 6 \times 10^{-4} \) Ω/m is the resistance per meter.Substituting the values, the power loss per meter of cable is:\[ P = (700)^2 \times (6 \times 10^{-4}) = 294 \text{ W/m} \]
02

Calculate Surface Temperature without Insulation

The surface temperature of the cable can be found using the equation for heat transfer by convection and radiation: \[ P = h A (T_s - T_{ ext{env}}) \]where:- \( P = 294 \text{ W/m} \) is the power loss,- \( h = 25 \, \text{W/m}^2 \cdot K \) is the heat transfer coefficient,- \( A = \pi d \) is the surface area of the cable per unit length with \( d = 5 \times 10^{-3} \) m (diameter),- \( T_s \) is the surface temperature,- \( T_{\text{env}} = 30^{\circ} C \) is the environment temperature.First, calculate \( A \): \[ A = \pi \times 5 \times 10^{-3} = 0.0157 \text{ m}^2 \text{/m} \]Substitute values into the heat transfer equation and solve for \( T_s \): \[ 294 = 25 \times 0.0157 \times (T_s - 30) \]\[ T_s = \frac{294}{0.0157 \times 25} + 30 \approx 66.9^{\circ} C \]
03

Calculate Surface Temperature with Insulation

With a thin coating of insulation, the heat transfer equation is modified to account for the contact resistance:\[ P = \frac{T_{ ext{cable}} - T_{ ext{env}}}{R_c + \frac{1}{h A}} \]where:- \( R_c = 0.02 \text{ m}^2 K/W \) is the contact resistance.Rearranging for \( T_{\text{cable}} \):\[ T_{\text{cable}} = P \bigg(R_c + \frac{1}{h A}\bigg) + T_{\text{env}} \]Substituting known values:\[ T_{\text{cable}} = 294 \times (0.02 + \frac{1}{25 \times 0.0157}) + 30 \approx 73.4^{\circ} C \]
04

Calculate Insulation Surface Temperature

The surface temperature of the insulation can be found similar to the surface temperature of cable:\[ P = h A (T_{\text{insulation}} - T_{env}) \]And we have:\[ T_{\text{insulation}} = \frac{P}{h A} + T_{\text{env}} \]Using the value for surface area and power loss calculated earlier:\[ T_{\text{insulation}} = \frac{294}{25 \times 0.0157} + 30 \approx 60.1^{\circ} C \]
05

Find Insulation Thickness for Minimum Temperature

The critical thickness of insulation can be determined using:\[ r_{\text{crit}} = \frac{k}{h} \]where:- \( k = 0.5 \text{ W/m} \cdot K \) is the thermal conductivity of the insulation.Substitute the given values:\[ r_{\text{crit}} = \frac{0.5}{25} \approx 0.02 \text{ m} \]Thus, the critical thickness for minimum surface temperature is roughly 20 mm or 0.02 m.
06

Calculate Maximum Temperature with Critical Thickness

Now calculate the maximum insulation temperature using the critical thickness. The formula for the temperature at the inner surface of insulation is the same as previously used:\[ T_{\text{max}} = \frac{P}{h ( \pi (d+2r_{\text{crit}}))} + T_{\text{env}} \]Replacing \( d + 2r_{\text{crit}} \) with \( 0.05 + 2 \times 0.02 = 0.09 \text{ m} \):\[ T_{\text{max}} = \frac{294}{25 \times \pi \times 0.09} + 30 \approx 37.3^{\circ} C \]

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Key Concepts

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

Electrical Resistance
Electrical resistance is a measure of how much an object opposes the flow of electric current. It is expressed in ohms (Ω). In this exercise, the stainless steel cable has a resistance of \(6 \times 10^{-4}\ \text{Ω/m}\). This resistance causes electrical energy to be converted into heat, which is also known as Joule heating or resistive heating.
  • The power loss due to this resistance can be calculated using the formula \( P = I^2 \times R \).
  • In the case of the cable, with a current \( I = 700 \text{ A} \), the power loss per meter is \( 294 \text{ W/m} \).
This power loss is significant because it determines how much heat the cable generates, affecting the cable's temperature.
Thermal Insulation
Thermal insulation is used to reduce heat transfer between objects or environments with different temperatures. In this exercise, thin electrical insulation is applied to the cable. This insulation adds a layer of resistance to heat flow, expressed here as a contact resistance \( R_c = 0.02 \ \text{m}^2 \cdot \text{K/W} \).
  • When insulation is applied, the heat transfer equation must be modified to account for this additional thermal resistance.
  • The equation used is \( P = \frac{T_{\text{cable}} - T_{\text{env}}}{R_c + \frac{1}{h A}} \), where \( h \) is the heat transfer coefficient.
Thus, the insulation significantly affects both the cable's exterior temperature and the overall thermal resistance.
Critical Thickness
The concept of critical thickness of insulation is important when discussing thermal insulation. It refers to the thickness where additional insulation starts to result in an increase in heat loss due to increased surface area outweighing the resistance provided by the insulation.
The formula used for critical thickness \( r_{\text{crit}} \) is \( r_{\text{crit}} = \frac{k}{h} \), where \( k \) is the thermal conductivity of the material.
  • For this exercise, \( k = 0.5 \ \text{W/m} \cdot \text{K} \) and the heat transfer coefficient \( h = 25 \ \text{W/m}^2 \cdot \text{K} \).
  • Substituting these gives a critical thickness of approximately 0.02 m or 20 mm.
Understanding this aspect is crucial in insulation design, ensuring that insulation reduces heat loss efficiently without inadvertently causing a temperature rise.
Surface Temperature Calculation
Surface temperature calculation involves determining the temperature of an object's surface when it is subjected to heat transfer. It considers both convective and radiative heat losses.
To calculate the surface temperature of the cable, the equation \( P = h A (T_s - T_{\text{env}}) \) is used. Here's a breakdown:
  • \( P \) is the power loss per meter due to resistance, which is 294 W/m.
  • \( h \) is the heat transfer coefficient.
  • \( A \) represents the surface area per meter of the cable.
  • \( T_s \) is the surface temperature we aim to find, while \( T_{\text{env}} \) is the surrounding environment's temperature.
For the bare cable, applying rearrangement of the formula yields a surface temperature \( T_s \) of about 66.9°C. When insulated, similar calculations help find the temperatures accounting for different thermal resistances. Understanding this allows for precise control of temperatures in systems subject to heat transfer.

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Most popular questions from this chapter

Radinactive wastes \(\left(k_{1 w}=20 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right)\) are stored in a spherical, stainless steel \(\left(k_{\mathrm{m}}=15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right)\) container of inner and outer radii equal to \(r_{i}=0.5 \mathrm{~m}\) and \(r_{e}=0.6 \mathrm{~m}\). Heat is genersed volumetrically within the wastes at a unifom rate of \(\hat{q}=10^{8} \mathrm{~W} / \mathrm{m}^{3}\), and the outer surface of the container is exposed to a water flow for which \(h=\) \(1000 \mathrm{~W} / \mathrm{m}^{2}-\mathrm{K}\) and \(T_{\mathrm{s}}=25^{\circ} \mathrm{C}\).

Consider a plane composite wall that is composed of two naterials of thermal conductivities \(k_{A}=0.1 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and \(k_{B}=0.04 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and thicknesses \(L_{A}=10 \mathrm{~mm}\) and \(L_{\mathrm{B}}=20 \mathrm{~mm}\). The contact resistance at the interface between the two materials is known to be \(0.30 \mathrm{~m}^{2} \cdot \mathrm{K} / \mathrm{W}\). Material A adjoins a fluid at \(200^{\circ} \mathrm{C}\) for which \(h=10\) W/m² \(\cdot \mathrm{K}\), and material B adjoins a fluid at \(40^{\circ} \mathrm{C}\) for which \(h=20 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) What is the rate of heat transfer through a wall that is \(2 \mathrm{~m}\) high by \(2.5 \mathrm{~m}\) wide? (b) Sketch the temperature distribution.

Turbine blades mounted to a rotating dise in a gas turbine engine are cxposed to a gas stream that is at \(T_{a}=1200^{\circ} \mathrm{C}\) and maintains al convection coefficicnt of \(h=250 \mathrm{~W} / \mathrm{m}^{2}\) - K over the blade. The blades, which are fabricated from Inconel, \(k=20 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\), have a length of \(L=50 \mathrm{~mm}\). The blade profile has a uniform cross-sectional area of \(A_{c}=6 \times 10^{-4} \mathrm{~m}^{2}\) and a perimeter of \(P=110 \mathrm{~mm}\). A proposed blade- cooling scheme, which involves routing air through the supporting dise, is able to maintain the base of each blade at a temperature of \(T_{b}=300^{\circ} \mathrm{C}\). (a) If the maximum allowable blade temperature is \(1050^{\circ} \mathrm{C}\) and the blade tip may be assumed to be adiabatic, is the proposed cooling scheme satisfactory? (b) For the proposed cooling seheme, what is the rate at which heat is transferred from each blade to the coolant?

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An air heater may be fabricated by coiling Nichfome wire and passing air in cross flow over the wire. Consider a heater fabricated from wire of diameter \(D=\) \(1 \mathrm{~mm}\), electrical resistivity \(p_{e}=10^{-6} \mathrm{n} \cdot \mathrm{m}\), thernal conductivity \(k=25 \mathrm{~W} / \mathrm{m}=\mathrm{K}\), and emissivity \(\varepsilon=0.2\). The heater is designed to deliver air at a temperatiue of \(T_{m}=50^{\circ} \mathrm{C}\) under flow conditions that provide a convection coefficient of \(h=250 \mathrm{~W} / \mathrm{m}^{2}\). \(\mathrm{K}\) for the wire. The temperature of the housing that encloses the wire and through which the air flows is \(T_{\text {er }}=50^{\circ} \mathrm{C}\). If the maximum allowable temperature of the wire is \(T_{\max }=1200^{\circ} \mathrm{C}\), what is the maximum allowable clextric current \(n\) ? If the maximum available voltage is \(\Delta E=110 \mathrm{~V}\), what is the corresponding length \(L\) of wire that may be used in the heater and the power raing of the heater? Himt: In your solution, assume negligible temperature variations within the wire, but after obtaining the desired results, assess the validity of this arsumption.

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