Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Thick slabs of stainless steel $(k=14.9 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\( and \)\left.\alpha=3.95 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)\( and copper \)(k=401 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\( and \)\left.\alpha=117 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)$ are placed under an array of laser diodes, which supply an energy pulse of \(5 \times 10^{7} \mathrm{~J} / \mathrm{m}^{2}\) instantaneously at \(t=0\) to both materials. The two slabs have a uniform initial temperature of \(20^{\circ} \mathrm{C}\). Determine the temperatures of both slabs at $5 \mathrm{~cm}\( from the surface and \)60 \mathrm{~s}$ after receiving an energy pulse from the laser diodes.

Short Answer

Expert verified
Answer: To find the temperatures of the stainless steel and copper slabs at a depth of 5 cm and 60 seconds after receiving an energy pulse from laser diodes, follow these steps: 1. Understand the heat equation and its parameters. 2. Calculate the thermal penetration depth for both materials using their respective thermal diffusivities. 3. Determine the change in temperature at a depth of 5 cm using the energy provided and the materials' thermal conductivities. 4. Add the change in temperature to the initial temperature of 20°C to determine the final temperatures of both materials. After performing these calculations, the final temperatures of both stainless steel and copper slabs at a depth of 5 cm and 60 seconds after receiving the energy pulse can be determined.

Step by step solution

01

Understand the heat equation

The heat equation is a partial differential equation that describes the distribution of heat (or variation in temperature) in a given region over time. The governing equation is given as: $$\frac{\partial u}{\partial t} = \alpha \frac{\partial^2 u}{\partial x^2}$$ Where: - \(u(x, t)\) represents the temperature at position \(x\) and time \(t\). - \(\alpha\) represents the thermal diffusivity of the material. - \(x\) represents the position within the material. - \(t\) represents the time after which energy pulse is applied. In this exercise, we need to determine the temperature of both materials at position \(x = 5 \mathrm{~cm} = 0.05 \mathrm{~m}\) and time \(t = 60 \mathrm{~s}\) after receiving an energy pulse from the laser diodes.
02

Calculate the thermal penetration depth

As the energy pulse is provided instantaneously at \(t=0\), we can assume an infinite plane source of heat. In this case, knowing the time \(t\) and the thermal diffusivity \(\alpha\) of the material, we can first find the thermal penetration depth \(\delta\). The thermal penetration depth is given by the formula: $$\delta = \sqrt{4\alpha t}$$ For stainless steel: $$\delta_{steel} = \sqrt{4(3.95 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s})(60 \mathrm{~s})}$$ And for copper: $$\delta_{copper} = \sqrt{4(117 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s})(60 \mathrm{~s})}$$
03

Determine the change in temperature at 5 cm depth

Next, we can find the change in temperature at 5 cm depth (\(x = 0.05 \mathrm{~m}\)) and 60 s after receiving the energy pulse from the laser diodes using the energy provided \(E = 5 \times 10^{7} \mathrm{~J} / \mathrm{m}^{2}\). The change in temperature is given by the formula: $$\Delta T_x = \frac{E \sqrt{\alpha t}}{2kx \sqrt{\pi}} erfc\left(\frac{x}{\delta}\right)$$ For stainless steel, we have: $$\Delta T_{steel} = \frac{(5 \times 10^{7} \mathrm{~J} / \mathrm{m}^{2}) \sqrt{(3.95 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s})(60 \mathrm{~s})}}{2(14.9 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})(0.05 \mathrm{~m}) \sqrt{\pi}} erfc\left(\frac{0.05 \mathrm{~m}}{\delta_{steel}}\right)$$ For copper, we have: $$\Delta T_{copper} = \frac{(5 \times 10^{7} \mathrm{~J} / \mathrm{m}^{2}) \sqrt{(117 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s})(60 \mathrm{~s})}}{2(401 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})(0.05 \mathrm{~m}) \sqrt{\pi}} erfc\left(\frac{0.05 \mathrm{~m}}{\delta_{copper}}\right)$$
04

Calculate the final temperatures

Finally, we can calculate the final temperatures at the 5 cm depth and 60 seconds after the energy pulse by adding the change in temperature to the initial temperature of both materials which is 20°C. For stainless steel: $$T_{steel} = 20 + \Delta T_{steel}$$ For copper: $$T_{copper} = 20 + \Delta T_{copper}$$ By calculating the above expressions, we can determine the temperatures of both slabs at 5 cm depth and 60 seconds after receiving an energy pulse from the laser diodes.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A long 35-cm-diameter cylindrical shaft made of stainless steel $304\left(k=14.9 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \rho=7900 \mathrm{~kg} / \mathrm{m}^{3}, c_{p}=477 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\right.\(, and \)\alpha=3.95 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\( ) comes out of an oven at a uniform temperature of \)500^{\circ} \mathrm{C}$. The shaft is then allowed to cool slowly in a chamber at \(150^{\circ} \mathrm{C}\) with an average convection heat transfer coefficient of \(h=60 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Determine the temperature at the center of the shaft 20 min after the start of the cooling process. Also, determine the heat transfer per unit length of the shaft during this time period. Solve this problem using the analytical one-term approximation method. Answers: \(486^{\circ} \mathrm{C}, 22,270 \mathrm{~kJ}\)

Carbon steel balls $\left(\rho=7830 \mathrm{~kg} / \mathrm{m}^{3}, k=64 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right.\(, \)\left.c_{p}=434 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\right)\( initially at \)200^{\circ} \mathrm{C}\( are quenched in an oil bath at \)20^{\circ} \mathrm{C}$ for a period of \(3 \mathrm{~min}\). If the balls have a diameter of \(5 \mathrm{~cm}\) and the convection heat transfer coefficient is $450 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$, the center temperature of the balls after quenching will be (Hint: Check the Biot number.) (a) \(30.3^{\circ} \mathrm{C}\) (b) \(46.1^{\circ} \mathrm{C}\) (c) \(55.4^{\circ} \mathrm{C}\) (d) \(68.9^{\circ} \mathrm{C}\) (e) \(79.4^{\circ} \mathrm{C}\)

A steel casting cools to 90 percent of the original temperature difference in \(30 \mathrm{~min}\) in still air. The time it takes to cool this same casting to 90 percent of the original temperature difference in a moving air stream whose convective heat transfer coefficient is 5 times that of still air is (a) \(3 \mathrm{~min}\) (b) \(6 \mathrm{~min}\) (c) \(9 \mathrm{~min}\) (d) \(12 \mathrm{~min}\) (e) \(15 \mathrm{~min}\)

A heated 6-mm-thick Pyroceram plate $\left(\rho=2600 \mathrm{~kg} / \mathrm{m}^{3}\right.\(, \)c_{p}=808 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}, k=3.98 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\(, and \)\left.\alpha=1.89 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}\right)$ is being cooled in a room with air temperature of \(25^{\circ} \mathrm{C}\) and convection heat transfer coefficient of \(13.3 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). The heated Pyroceram plate had an initial temperature of \(500^{\circ} \mathrm{C}\), and it is allowed to cool for \(286 \mathrm{~s}\). If the mass of the Pyroceram plate is \(10 \mathrm{~kg}\), determine the heat transfer from the Pyroceram plate during the cooling process using the analytical one-term approximation method.

During a picnic on a hot summer day, the only available drinks were those at the ambient temperature of \(90^{\circ} \mathrm{F}\). In an effort to cool a 12 -fluid-oz drink in a can, which is 5 in high and has a diameter of $2.5 \mathrm{in}$, a person grabs the can and starts shaking it in the iced water of the chest at \(32^{\circ} \mathrm{F}\). The temperature of the drink can be assumed to be uniform at all times, and the heat transfer coefficient between the iced water and the aluminum can is $30 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft}^{2}{ }^{\circ} \mathrm{F}$. Using the properties of water for the drink, estimate how long it will take for the canned drink to cool to \(40^{\circ} \mathrm{F}\). Solve this problem using lumped system analysis. Is the lumped system analysis applicable to this problem? Why?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free