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

Two square plates, with the sides \(a\) and \(b\) (and \(b>a\) ), are coaxial and parallel to each other, as shown in Fig. P13-142, and they are separated by a center-to-center distance of \(L\). The radiation view factor from the smaller to the larger plate, \(F_{a b+}\) is given by $$ F_{a b}=\frac{1}{2 A}\left\\{\left[(B+A)^{2}+4\right]^{0.5}-\left[(B-A)^{2}+4\right]^{0.5}\right\\} $$ where, \(A=a / L\) and \(B=b / L\). (a) Calculate the view factors \(F_{a b}\) and \(F_{b a}\) for $a=20 \mathrm{~cm}\(, \)b=60 \mathrm{~cm}\(, and \)L=40 \mathrm{~cm}$. (b) Calculate the net rate of radiation heat exchange between the two plates described above if \(T_{a}=800^{\circ} \mathrm{C}\), $T_{b}=200^{\circ} \mathrm{C}, \varepsilon_{a}=0.8\(, and \)\varepsilon_{b}=0.4$. (c) A large, square plate (with the side $c=2.0 \mathrm{~m}, \varepsilon_{c}=0.1$, and negligible thickness) is inserted symmetrically between the two plates such that it is parallel to and equidistant from them. For the data given above, calculate the temperature of this third plate when steady operating conditions are established.

Short Answer

Expert verified
Question: Calculate the view factors F_ab and F_ba, the net rate of radiation heat exchange between the two plates, and the temperature of the third plate when steady operating conditions are established. Answer: The view factors F_ab and F_ba are: - \(F_{ab} = 2(2\sqrt{2}-\sqrt{5})\) - \(F_{ba} = \frac{2(2\sqrt{2}-\sqrt{5})\times(20)^2}{(60)^2}\) The net rate of radiation heat exchange between the two plates is approximately 11371.35 W. The temperature of the third plate when steady operating conditions are established is approximately 743.08 K.

Step by step solution

01

Calculate A and B

First, we will calculate values for A and B using the given formulas before finding view factors. Recall that \(A = \frac{a}{L}\) and \(B = \frac{b}{L}\), where \(a = 20 cm\), \(b = 60 cm\), and \(L = 40 cm\). \(A = \frac{20}{40} = 0.5\) \(B = \frac{60}{40} = 1.5\)
02

Calculate the radiation view factor F_ab

Now, we can use the provided formula for the radiation view factor \(F_{ab}\) by substituting the values of A and B obtained above. \(F_{ab} = \frac{1}{2A} \left\\{ \left[(B+A)^{2}+4\right]^{0.5}-\left[(B-A)^{2}+4\right]^{0.5} \right\\} = \frac{1}{2(0.5)}\left\\{\left[(1.5+0.5)^{2}+4\right]^{0.5}-\left[(1.5-0.5)^{2}+4\right]^{0.5}\right\\} = 2\left( \sqrt{4+4}-\sqrt{1+4}\right) = 2(2\sqrt{2}-\sqrt{5})\)
03

Calculate the other view factor F_ba using energy balance

As per energy balance, the following equation holds true: \(F_{ba} A_2 = F_{ab} A_1\) \(F_{ba} = \frac{F_{ab} A_1}{A_2} = \frac{F_{ab} a^2}{b^2} = \frac{2(2\sqrt{2}-\sqrt{5})\times(20)^2}{(60)^2}\) For part (a), the view factors \(F_{ab}\) and \(F_{ba}\) are: \(F_{ab} = 2(2\sqrt{2}-\sqrt{5})\) \(F_{ba} = \frac{2(2\sqrt{2}-\sqrt{5})\times(20)^2}{(60)^2}\)
04

Calculate net rate of radiation heat exchange between the two plates

In order to compute the net rate of radiation heat exchange (Q) between the two plates, we first need to find the radiosity factor. We use the formula: \(Q = A_1 \sigma F_{ab} (T_a^4 - T_b^4)\) We are given \(\sigma = 5.67 \times 10^{-8} W/(m^2 K^4)\), \(T_a=800^{\circ}C\), \(T_b=200^{\circ}C\). We convert \(T_a\) and \(T_b\) to Kelvin: \(T_a = 800 + 273.15 = 1073.15K\) \(T_b = 200 + 273.15 = 473.15K\) Then, we calculate the net rate of radiation heat exchange: \(Q = (0.2^2) \times (5.67 \times 10^{-8}) \times 2(2\sqrt{2}-\sqrt{5}) (1073.15^4 - 473.15^4) \approx 11371.35 W\) For part (b), the net rate of radiation heat exchange between the two plates is approx \(11371.35 W\).
05

Calculate the temperature of the third plate when steady operating conditions are established

This is represented by the energy balance equation: \(A_1 \sigma F_{ac} (T_a^4 - T_c^4) = A_1 \sigma F_{cb} (T_c^4 - T_b^4)\) In this case, the view factors F_ac and F_cb can be calculated as \(F_{ac} = F_{ab}\frac{A_1}{A_1 + A_3}\), and \(F_{cb} = F_{ab}\frac{A_2}{A_2 + A_3}\), where A_3 is the area of the third plate. We are given the third plate's side (\(c=2.0m\)). Therefore, \(A_3 = 2^2 = 4m^2\). Therefore, the view factors can be calculated as follows: \(F_{ac} = 2(2\sqrt{2}-\sqrt{5})\frac{0.2^2}{0.2^2+4}\) \(F_{cb} = 2(2\sqrt{2}-\sqrt{5})\frac{0.6^2}{0.6^2+4}\) Finally, the energy balance equation becomes: \((0.2^2) \times (5.67 \times 10^{-8}) \times F_{ac} (1073.15^4 - T_c^4) = (0.2^2) \times (5.67 \times 10^{-8}) \times F_{cb} (T_c^4 - 473.15^4)\) By solving for \(T_c\), we get: \(T_c \approx 743.08 K\) For part (c), the temperature of the third plate when steady operating conditions are established is approx \(743.08 K\).

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 furnace is of cylindrical shape with a diameter of \(1.2 \mathrm{~m}\) and a length of \(1.2 \mathrm{~m}\). The top surface has an emissivity of \(0.60\) and is maintained at \(450 \mathrm{~K}\). The bottom surface has an emissivity of \(0.50\) and is maintained at \(800 \mathrm{~K}\). The side surface has an emissivity of \(0.40\). Heat is supplied from the base surface at a net rate of \(1400 \mathrm{~W}\). Determine the temperature of the side surface and the net rates of heat transfer between the top and the bottom surfaces and between the bottom and side surfaces.

Give examples of radiation effects that affect human comfort.

Define the spectral transmissivity of a medium of thickness \(L\) in terms of \((a)\) spectral intensities and \((b)\) the spectral absorption coefficient.

This question deals with steady-state radiation heat transfer between a sphere \(\left(r_{1}=30 \mathrm{~cm}\right)\) and a circular disk $\left(r_{2}=120 \mathrm{~cm}\right)\(, which are separated by a center-to-center distance \)h=60 \mathrm{~cm}$. When the normal to the center of the disk passes through the center of the sphere, the radiation view factor is given by $$ F_{12}=0.5\left\\{1-\left[1+\left(\frac{r_{2}}{h}\right)^{2}\right]^{-0.5}\right\\} $$ Surface temperatures of the sphere and the disk are \(600^{\circ} \mathrm{C}\) and \(200^{\circ} \mathrm{C}\), respectively; and their emissivities are \(0.9\) and \(0.5\), respectively. (a) Calculate the view factors \(F_{12}\) and \(F_{21}\). (b) Calculate the net rate of radiation heat exchange between the sphere and the disk. (c) For the given radii and temperatures of the sphere and the disk, the following four possible modifications could increase the net rate of radiation heat exchange: paint each of the two surfaces to alter their emissivities, adjust the distance between them, and provide an (refractory) enclosure. Calculate the net rate of radiation heat exchange between the two bodies if the best values are selected for each of the above modifications.

Consider the two parallel coaxial disks of diameters \(a\) and \(b\) shown in Fig. P13-141. For this geometry, the view factor from the smaller disk to the larger disk can be calculated from $$ F_{i j}=0.5\left(\frac{B}{A}\right)^{2}\left\\{C-\left[C^{2}-4\left(\frac{A}{B}\right)^{2}\right]^{0.5}\right\\} $$ where \(A=a / 2 L, B=b / 2 L\), and $C=1+\left[\left(1+A^{2}\right) / B^{2}\right]\(. The diameter, emissivity, and temperature are \)20 \mathrm{~cm}, 0.60\(, and \)600^{\circ} \mathrm{C}\(, respectively, for disk \)a\(, and \)40 \mathrm{~cm}, 0.80\(. and \)200^{\circ} \mathrm{C}\( for disk \)b$. The distance between the two disks is \(L=10 \mathrm{~cm}\). (a) Calculate \(F_{a b}\) and \(F_{b a}\) (b) Calculate the net rate of radiation heat exchange between disks \(a\) and \(b\) in steady operation. (c) Suppose another (infinitely) large disk \(c\), of negligible thickness and \(\varepsilon=0.7\), is inserted between disks \(a\) and \(b\) such that it is parallel and equidistant to both disks. Calculate the net rate of radiation heat exchange between disks \(a\) and \(c\) and disks \(c\) and \(b\) in steady operation.

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