/*! 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 103 The structural components of mod... [FREE SOLUTION] | 91Ó°ÊÓ

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The structural components of modern aircraft are commonly fabricated of high- performance composite materials. These materials are fabricated by impregnating mats of extremely strong fibers that are held within a form with an epoxy or thermoplastic liquid. After the liquid cures or cools, the resulting component is of extremely high strength and low weight. Periodically, these components must be inspected to ensure that the fiber mats and bonding material do not become delaminated and, in turn, the component loses its airworthiness. One inspection method involves application of a uniform, constant radiation heat flux to the surface being inspected. The thermal response of the surface is measured with an infrared imaging system, which captures the emission from the surface and converts it to a colorcoded map of the surface temperature distribution. Consider the case where a uniform flux of \(5 \mathrm{~kW} / \mathrm{m}^{2}\) is applied to the top skin of an airplane wing initially at \(20^{\circ} \mathrm{C}\). The opposite side of the 15 -mm-thick skin is adjacent to stagnant air and can be treated as well insulated. The density and specific heat of the skin material are \(1200 \mathrm{~kg} / \mathrm{m}^{3}\) and \(1200 \mathrm{~J} / \mathrm{kg}+\mathrm{K}\), respectively. The effective thermal conductivity of the intact skin material is \(k_{1}=1.6 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). Contact resistances develop internal to the structure as a result of delamination between the fiber mats and the bonding material, leading to a reduced effective thermal conductivity of \(k_{2}=1.1 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). Determine the surface temperature of the component after 10 and \(100 \mathrm{~s}\) of irradiation for (i) an area where the material is structurally intact and (ii) an adjacent area where delamination has occurred within the wing.

Short Answer

Expert verified
(i) For the intact skin material: - After 10 s of irradiation, the surface temperature is \(T_s(t = 10) = 20 + 5000\sqrt{\frac{4\alpha_1 \cdot 10}{\pi}}\) - After 100 s of irradiation, the surface temperature is \(T_s(t = 100) = 20 + 5000\sqrt{\frac{4\alpha_1 \cdot 100}{\pi}}\) (ii) For the delaminated skin material: - After 10 s of irradiation, the surface temperature is \(T_s(t = 10) = 20 + 5000\sqrt{\frac{4\alpha_2 \cdot 10}{\pi}}\) - After 100 s of irradiation, the surface temperature is \(T_s(t = 100) = 20 + 5000\sqrt{\frac{4\alpha_2 \cdot 100}{\pi}}\)

Step by step solution

01

Define known variables

The initial temperature: \(T_i = 20^{\circ}\mathrm{C}\) The applied heat flux at the surface: \(q'' = 5\,\mathrm{kW/m^2}\) Density of skin material: \(\rho = 1200\,\mathrm{kg/m^3}\) Specific heat capacity of skin material: \(c_p = 1200\,\mathrm{J/(kg\cdot K)}\) Thermal conductivity of intact skin material: \(k_1 = 1.6\,\mathrm{W/(m\cdot K)}\) Thermal conductivity of delaminated skin material: \(k_2 = 1.1\,\mathrm{W/(m\cdot K)}\) Time of inspection: \(t = 10\,\mathrm{s}\) and \(t = 100\,\mathrm{s}\).
02

Compute the thermal diffusivity for both cases

- For intact skin material: \[\alpha_{1} = \frac{k_1}{\rho c_p} = \frac{1.6}{1200 \cdot 1200}\,\mathrm{m^2/s}\] - For delaminated skin material: \[\alpha_{2} = \frac{k_2}{\rho c_p} = \frac{1.1}{1200 \cdot 1200}\,\mathrm{m^2/s}\]
03

Calculate the surface temperature after 10 and 100 seconds for the intact skin material

Recall the temperature distribution formula for a semi-infinite solid: \[ T(x,t) = T_i + q''\sqrt{\frac{4\alpha t}{\pi}}\exp(-\frac{x^2}{4\alpha t}) - q''x\,\mathrm{erf}(\frac{x}{2\sqrt{\alpha t}}) \] At the surface, \(x=0\) and we get: \[T_s(t) = T_i + q''\sqrt{\frac{4\alpha t}{\pi}}\] For the intact skin material (\(\alpha_1\)): - At \(t=1\)s (converting \(q''\) to W): \[T_s(t = 10) = 20 + 5000\sqrt{\frac{4\alpha_1 \cdot 10}{\pi}}\] - At \(t=100\)s: \[T_s(t = 100) = 20 + 5000\sqrt{\frac{4\alpha_1 \cdot 100}{\pi}}\] Calculate the surface temperatures for the intact skin material using the obtained expressions.
04

Calculate the surface temperature after 10 and 100 seconds for the delaminated skin material

For the delaminated skin material (\(\alpha_2\)): - At \(t=10\)s (converting \(q''\) to W): \[T_s(t = 10) = 20 + 5000\sqrt{\frac{4\alpha_2 \cdot 10}{\pi}}\] - At \(t=100\)s: \[T_s(t = 100) = 20 + 5000\sqrt{\frac{4\alpha_2 \cdot 100}{\pi}}\] Calculate the surface temperatures for the delaminated skin material using the obtained expressions.
05

Present the results

Finally, present the calculated surface temperatures after 10 and 100 seconds for both the intact and delaminated skin material cases.

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Key Concepts

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

Thermal Conductivity
Thermal conductivity is a crucial property in understanding how materials transfer heat. It tells us how easily heat can flow through a material over a certain distance. The higher the thermal conductivity, the better the material is at conducting heat. This is essential in applications where uniform temperature distribution is key, such as in heat exchangers or building insulation.
For our exercise, the intact aircraft wing skin has a thermal conductivity of 1.6 W/(m·K), meaning it efficiently transfers heat. When delamination occurs, this value drops to 1.1 W/(m·K). This reduction indicates a poorer heat flow capability due to potential gaps or voids between the layers. These internal resistances disrupt the heat flow, potentially affecting the wing's structural integrity.
Understanding thermal conductivity helps in predicting how materials will behave under different heating conditions and is essential in engineering reliable components, especially in safety-critical applications.
Composite Materials
Composite materials are engineered by combining two or more distinct materials to create a new material with enhanced properties. Typically, they consist of a matrix and a reinforcement. The matrix, often a thermoset resin or thermoplastic, supports the reinforcement, which might be fibers like carbon or glass, in maintaining the composite material's overall structure.
One big advantage of composites is their high strength-to-weight ratio, which makes them ideal for aerospace applications. In our exercise, the aircraft's skin is a composite, offering lightweight yet robust protection.
However, composites can face challenges such as delamination, where layers separate due to impacts or stress over time. This not only weakens the material but also alters its thermal properties, as seen with the reduced thermal conductivity in our delaminated wing scenario. Proper inspection and maintenance of composite materials are therefore crucial to ensure their longevity and performance.
Infrared Thermography
Infrared thermography is a non-destructive inspection technique used to measure and visualize temperature distribution across surfaces. This tool is handy for identifying issues like the delamination in composites. By detecting heat emitted in the infrared spectrum, thermography cameras provide thermal images or thermograms without the need for physical contact.
The principle behind this method is quite simple: all objects emit infrared radiation as a function of their temperature. Infrared thermography captures this radiation and converts it into temperature data. During inspections, engineers apply a known heat flux to the surface and capture the thermal response.
In the exercise, infrared thermography helps detect irregularities due to changes in heat transfer properties. For instance, areas with delamination would show a different thermal profile compared to intact areas. This technique is non-invasive, making it perfect for ongoing monitoring of high-value components like airplane wings, ensuring safety without dismantling the structure.

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Most popular questions from this chapter

Consider the thick slab of copper in Example 5.12, which is initially at a uniform temperature of \(20^{\circ} \mathrm{C}\) and is suddenly exposed to a net radiant flux of \(3 \times 10^{5} \mathrm{~W} / \mathrm{m}^{2}\). Use the Finite-Difference Equations/ One-Dimensional/Transient conduction model builder of \(I H T\) to obtain the implicit form of the finite-difference equations for the interior nodes. In your analysis, use a space increment of \(\Delta x=37.5 \mathrm{~mm}\) with a total of 17 nodes (00-16), and a time increment of \(\Delta t=1.2 \mathrm{~s}\). For the surface node 00 , use the finite-difference equation derived in Section 2 of the Example. (a) Calculate the 00 and 04 nodal temperatures at \(t=120 \mathrm{~s}\), that is, \(T(0,120 \mathrm{~s})\) and \(T(0.15 \mathrm{~m}, 120 \mathrm{~s})\), and compare the results with those given in Comment 1 for the exact solution. Will a time increment of \(0.12 \mathrm{~s}\) provide more accurate results? (b) Plot temperature histories for \(x=0,150\), and \(600 \mathrm{~mm}\), and explain key features of your results.

A long rod of \(60-\mathrm{mm}\) diameter and thermophysical properties \(\rho=8000 \mathrm{~kg} / \mathrm{m}^{3}, \quad c=500 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\), and \(k=50 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) is initially at a uniform temperature and is heated in a forced convection furnace maintained at \(750 \mathrm{~K}\). The convection coefficient is estimated to be \(1000 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) What is the centerline temperature of the rod when the surface temperature is \(550 \mathrm{~K}\) ? (b) In a heat-treating process, the centerline temperature of the rod must be increased from \(T_{i}=300 \mathrm{~K}\) to \(T=500 \mathrm{~K}\). Compute and plot the centerline temperature histories for \(h=100,500\), and \(1000 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). In each case the calculation may be terminated when \(T=500 \mathrm{~K}\).

During transient operation, the steel nozzle of a rocket engine must not exceed a maximum allowable operating temperature of \(1500 \mathrm{~K}\) when exposed to combustion gases characterized by a temperature of \(2300 \mathrm{~K}\) and a convection coefficient of \(5000 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). To extend the duration of engine operation, it is proposed that a ceramic thermal barrier coating \((k=10 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\), \(\alpha=6 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\) ) be applied to the interior surface of the nozzle. (a) If the ceramic coating is \(10 \mathrm{~mm}\) thick and at initial temperature of \(300 \mathrm{~K}\), obtain a conservative estimate of the maximum allowable duration of engine operation. The nozzle radius is much larger than the combined wall and coating thickness. (b) Compute and plot the inner and outer surface temperatures of the coating as a function of time for \(0 \leq t \leq 150 \mathrm{~s}\). Repeat the calculations for a coating thickness of \(40 \mathrm{~mm}\).

A soda lime glass sphere of diameter \(D_{1}=25 \mathrm{~mm}\) is encased in a bakelite spherical shell of thickness \(L=\) \(10 \mathrm{~mm}\). The composite sphere is initially at a uniform temperature, \(T_{i}=40^{\circ} \mathrm{C}\), and is exposed to a fluid at \(T_{\infty}=10^{\circ} \mathrm{C}\) with \(h=30 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Determine the center temperature of the glass at \(t=200 \mathrm{~s}\). Neglect the thermal contact resistance at the interface between the two materials.

The 150 -mm-thick wall of a gas-fired furnace is constructed of fireclay brick \((k=1.5 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \rho=2600\) \(\left.\mathrm{kg} / \mathrm{m}^{3}, c_{p}=1000 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\right)\) and is well insulated at its outer surface. The wall is at a uniform initial temperature of \(20^{\circ} \mathrm{C}\), when the burners are fired and the inner surface is exposed to products of combustion for which \(T_{\infty}=950^{\circ} \mathrm{C}\) and \(h=100 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) How long does it take for the outer surface of the wall to reach a temperature of \(750^{\circ} \mathrm{C}\) ? (b) Plot the temperature distribution in the wall at the foregoing time, as well as at several intermediate times.

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