/*! 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 43 A 2-mm-diameter electrical wire ... [FREE SOLUTION] | 91Ó°ÊÓ

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A 2-mm-diameter electrical wire is insulated by a 2 -mm-thick rubberized sheath \((k=0.13 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\), and the wirc/sheath interface is characterized by a thermal contuct resistance of \(R_{t,}^{\prime \prime}=3 \times 10^{-4} \mathrm{~m}^{2} \cdot \mathrm{K} / \mathrm{W}\). The convection heat transfer coefficient at the outer surface of the sheath is \(10 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), and the tempenature of the ambient air is \(20^{\circ} \mathrm{C}\). If the temperature of the insulation may not exceed \(50^{\circ} \mathrm{C}\), what is the maximum allowable electrical power that may be dissipated per unit length of the conductor? What is the critical radius of the insulation?

Short Answer

Expert verified
Critical radius is 13 mm. Maximum power dissipation is 3769 W/m.

Step by step solution

01

Calculate the Critical Radius

The critical radius of insulation is determined using the formula \( r_c = \frac{k}{h} \), where \( k \) is the thermal conductivity of the insulation and \( h \) is the convection heat transfer coefficient. Given that \( k = 0.13 \mathrm{~W/m} \cdot \mathrm{K} \) and \( h = 10 \mathrm{~W/m}^2 \cdot \mathrm{K} \), we have:\[r_c = \frac{0.13}{10} = 0.013 \text{ m} = 13 \text{ mm}\]The critical radius is 13 mm.
02

Evaluate If Current Insulation Maintains Temperature Below 50°C

The current insulation radius (not including the wire) is 2 mm, which is less than the critical radius of 13 mm. Therefore, insulation will actually **reduce** the rate of heat loss rather than increase it, indicating it's on the proper side of the critical radius to maintain temperature limitations at maximum power.
03

Calculate Total Thermal Resistance

Total thermal resistance, \( R_t \), includes the conductive resistance of the wire/sheath interface and the convective resistance. - Conductive resistance \( R_{c}^{''} = R_{t}^{''} = 3 \times 10^{-4} \mathrm{~m^2K/W} \).- Convective resistance \( R_{b}^{''} = \frac{1}{hA} = \frac{1}{10 \times 4 \pi(0.002+0.002)\times L} = \frac{1}{10 \times 4\times \pi \times 0.004} \mathrm{~m^2K/W}\).Total resistance:\[R_t^{''} = 3 \times 10^{-4} + \frac{1}{10 \times 4 \pi \times 0.004} \approx 0.00796 \mathrm{~m^2K/W}\]
04

Calculate Maximum Allowable Power Dissipation

The temperature difference between the insulation surface and the ambient air is \( \Delta T = 50 - 20 = 30 \degree \mathrm{C} \). Using \( P = \frac{\Delta T}{R_t^{''}} \) to solve for maximum power:\[P = \frac{30}{0.00796} \approx 3769 \mathrm{~W/m}\]The maximum power dissipation per unit length is approximately 3769 W/m.

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Key Concepts

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

Thermal Resistance
Thermal resistance is a measure of a material's ability to resist heat flow. It is the inverse of thermal conductance, which represents how easily heat passes through a material. Imagine it like the insulation for heat, much like a thick winter jacket is for cold air. The higher the thermal resistance, the better it is at preventing heat from moving through.
In this particular insulation problem, the thermal resistance consists of two main parts:
  • The conductive resistance: This resistance is due to the wire/sheath interface, calculated as Rt', in this problem, it is given as 3 x 10-4 ³¾Â²°­/°Â.
  • The convective resistance: This is due to the heat being transferred from the surface of the sheath to the surrounding air. It can be calculated using the formula Rb' = 1/(hA) where h is the convection heat transfer coefficient and A is the surface area in contact with the air.
To find the total thermal resistance (Rt'), you combine both resistances, resulting in approximately 0.00796 ³¾Â²°­/°Â. This total thermal resistance helps us understand how much power can safely pass through the insulation without overheating.
Convection Heat Transfer Coefficient
The convection heat transfer coefficient, often denoted as h, quantifies how effectively heat is exchanged between a surface and the surrounding fluid, like air or water, in this case, air. It essentially tells us how well the sheath can give away heat to the ambient environment.
This coefficient depends on factors like the flow of the fluid, the surface area, and even the nature of the fluid itself. For this problem, it is noted as 10 W/m2K.
Think of it like blowing on hot soup to cool it down faster; a higher h means quicker cooling (or heat transfer) from the surface to the fluid.
  • Lower values of h indicate poor heat transfer, meaning the insulation holds onto the heat longer.
  • Higher values mean heat is carried away more rapidly by the surrounding air.
Balancing this coefficient is crucial in designing effective insulation systems, ensuring that the right amount is dissipated without overheating.
Thermal Conductivity
Thermal conductivity, denoted by k, is a material property indicating the ability to conduct heat. Materials with high thermal conductivity, like metals, transfer heat efficiently, while materials with low thermal conductivity, like rubber or wool, act as better insulators.
In this exercise, the sheath surrounding the wire has a thermal conductivity value of 0.13 W/mK. This relatively low value signifies the material's effectiveness at thermally insulating the wire.
The formula for thermal conductivity
  • conveys how well heat flows through the material: q = -k * (dT/dx), where q is the heat flux and dT/dx is the temperature gradient.
  • demonstrates that less conductive materials will require thicker layers to achieve the same insulation effect as more conductive ones.
Therefore, in designing electrical systems, choosing materials with the right thermal conductivity is key to managing heat effectively.
Critical Radius
The concept of the critical radius is linked to the effectiveness of cylindrical insulation, exploring how insulation thickness can sometimes adversely affect heat loss. The critical radius formula is given by \[ r_c = \frac{k}{h} \] where rc represents the critical radius, k is the thermal conductivity, and h is the convection heat transfer coefficient.
In this problem, the critical radius was found to be 13 mm. The idea here is counterintuitive: adding insulation does not always reduce heat loss.
If the insulation radius is less than the critical radius, adding thickness reduces heat loss. But if it's greater, additional insulation could increase the heat loss due to a larger surface area.
This is vital for determining whether or not added insulation is beneficial, particularly when managing the thermal needs of electrical wires. Here, with the sheath being only 2 mm, it's clear that additional insulation reduces heat loss, staying on the safer side of the critical radius.

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Most popular questions from this chapter

The energy transferred from the anterior chamber of the eye through the cornea varies considerably depending on whether a contact lens is worm. Treat the eye as a splerical system and assume the system to be at steady state. The convection coefficient \(h_{e}\) is unchanged with and without the contact lens in place. The cornea and the lens cover one-third of the spherical surface area. Values of the parameters representing this situation are as follows: \(\begin{array}{ll}r_{1}=10.2 \mathrm{~mm} & r_{2}=12.7 \mathrm{~mm} \\\ r_{3}=16.5 \mathrm{~mm} & T_{-a}=21^{\circ} \mathrm{C} \\ T_{s 1}=37^{\circ} \mathrm{C} & k_{2}=0.80 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K} \\\ k_{1}=0.35 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K} & h_{n}=6 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K} \\ h_{4}=12 \mathrm{~W} / \mathrm{m}^{2}-\mathrm{K} & \end{array}\) (a) Construct the thermal circuits, labeling all potentials and flows for the systems excluding the contact lens and including the contact lens. Write resistance elements in terms of appropriate parameters. (b) Determine the heat loss from the anterior chamber with and without the contact lens in place. (c) Discuss the implication of your results.

The wall of a drying oven is constructed by sandwiching an insulation material of thermal conductivity \(k=\) \(0.05 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) between thin metal shects. The oven air is at \(T_{s j}=300^{\circ} \mathrm{C}\), and the corresponding convection coefficient is \(h_{4}=30 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). The inner wall surface absorbs a radiant flux of \(q_{\text {iat }}^{\prime \prime}=100 \mathrm{~W} / \mathrm{m}^{2}\) from hotter objects within the oven. The room air is at \(T_{m e}=25^{\circ} \mathrm{C}\), and the overall coefficient for convection and radiation from the outer surface is \(h_{e}=10 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) Draw the thermal circuit for the wall and label all temperatures, heat rates, and thermal resistances. (b) What insulation thickness \(L\) is required to maintain the outer wall surface at a sofe-to-touch temperature of \(T_{e}=40^{\circ} \mathrm{C}\) ?

A hollow aluminem sphere, with an clectrical heater in the center, is used in tests to determine the thermal conductivity of insulating materials. The inner and outer radii of the sphere are \(0.15\) and \(0.18 \mathrm{~m}\), respectively. and testing is done under steady-state conditions with the inner surface of the aluminum maintained at \(250^{\circ} \mathrm{C}\). In a particular test, a spherical shell of insulation is cast on the outer surface of the sphere to a thickness of \(0.12 \mathrm{~m}\). The system is in a roorn for which the air temperature is \(20^{\circ} \mathrm{C}\) and the convection cocfficient at the outer surface of the insulation is \(30 \mathrm{~W} / \mathrm{m}^{2}+\mathrm{K}\). If \(80 \mathrm{~W}\) are dissipated by the heater under steady-state conditions, what is the thermal conductivity of the insulation?

A thin clectrical heater is inserted between a long circular rod and a concentric tube with inner and outer radii of 20 and \(40 \mathrm{~mm}\). The rod (A) has a thermal conductivity of \(k_{A}=0.15 \mathrm{~W} / \mathrm{m}+\mathrm{K}\). while the tube (B) has a thermal conductivity of \(k_{\mathrm{B}}=1.5 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and its cuter surface is subjected to convection with a fluid of temperature \(T_{w}=-15^{\circ} \mathrm{C}\) and heat transfer coefficient \(50 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). The thermal contact resistance betueen the cylinder surfaces and the heater is negligible. (a) Determine the electrical power per unit length of the cylinders (W/m) that is required to maintain the outer surface of eylinder \(\mathrm{B}\) at \(5^{\circ} \mathrm{C}\). (b) What is the temperature at the center of cylinder A?

Consider two long. slender rods of the same diameter but different materials. One end of each rod is attached to a base surface maintained at \(100^{\circ} \mathrm{C}\), while the surfaces of the rods are exposed to ambient air at \(20^{\circ} \mathrm{C}\). By traversing the length of each rod with a thermocoeple, it was observed that the temperatures of the rods were equal at the positions \(x_{A}=0.15 \mathrm{~m}\) and \(x_{\mathrm{A}}=\) \(0.075 \mathrm{~m}\), where \(x\) is measured from the base surface. If the thermal conductivity of rod \(A\) is known to be \(k_{A}=\) \(70 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\), determine the value of \(k_{\mathrm{m}}\) for rod \(\mathrm{B}\).

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