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

The overall heat transfer coefficient (the \(U\)-value) of a wall under winter design conditions is \(U=2.25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Now a layer of \(100-\mathrm{mm}\) face brick is added to the outside, leaving a 20 -mm airspace between the wall and the bricks. Determine the new \(U\)-value of the wall. Also, determine the rate of heat transfer through a \(3-\mathrm{m}\)-high, 7-m-long section of the wall after modification when the indoor and outdoor temperatures are \(22^{\circ} \mathrm{C}\) and $-25^{\circ} \mathrm{C}$, respectively.

Short Answer

Expert verified
Answer: The new U-value of the wall is 0.731 W/m²⋅K and the rate of heat transfer through the modified wall section is 720.729 W.

Step by step solution

01

(Step 1: Determine the thermal resistance of the original wall)

To find the original thermal resistance of the wall, we use the formula: \(R = \frac{1}{U}\), where \(R\) is the thermal resistance and \(U\) is the overall heat transfer coefficient. Given, \(U = 2.25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), we can calculate the thermal resistance of the original wall. \(R_\text{original} = \frac{1}{2.25 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}} = 0.444~\mathrm{m}^{2} \cdot \mathrm{K} / \mathrm{W}\).
02

(Step 2: Determine the thermal resistance of the face brick layer and the airspace)

We're given that the added layer of face brick is 100 mm, and the airspace is 20 mm. To calculate the thermal resistance of both the face brick layer and the airspace, we will need their respective thermal conductivities. Commonly, the thermal conductivity of face brick(\(k_\text{brick}\)) is approximately \(0.81~\mathrm{W} / \mathrm{m} \cdot \mathrm{K}\), and for the airspace (\(k_\text{air}\)), it is \(0.025~\mathrm{W} / \mathrm{m} \cdot \mathrm{K}\). Now, we can calculate the thermal resistance using the formula: \( R_{i} = \frac{d_{i}}{k_{i}} \), where \(R_{i}\) is the thermal resistance of the ith layer, \(d_{i}\) is the layer thickness, and \(k_{i}\) is the layer thermal conductivity. \( R_\text{brick} = \frac{0.1 \mathrm{~m}}{0.81 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}} = 0.1235~\mathrm{m}^{2}\cdot \mathrm{K} / \mathrm{W} \) \( R_\text{air} = \frac{0.02 \mathrm{~m}}{0.025 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}} = 0.8~\mathrm{m}^{2}\cdot \mathrm{K} / \mathrm{W} \).
03

(Step 3: Calculate the new U-value of the wall)

After adding the face brick layer and the airspace, the overall thermal resistance of the modified wall is the sum of the thermal resistances of the original wall, face brick layer, and the airspace. Then, we can calculate the new U-value using the formula: \(U_\text{new} = \frac{1}{R_\text{total}}\). \( R_\text{total} = R_\text{original} + R_\text{brick} + R_\text{air} = 0.444 + 0.1235 + 0.8 = 1.3675~\mathrm{m}^{2} \cdot \mathrm{K} / \mathrm{W} \) \( U_\text{new} = \frac{1}{1.3675~\mathrm{m}^{2} \cdot \mathrm{K} / \mathrm{W}} = 0.731~\mathrm{W} / \mathrm{m}^{2} \cdot \mathrm{K} \).
04

(Step 4: Calculate the rate of heat transfer through the modified wall)

Now that we have the new U-value, we can calculate the rate of heat transfer through the modified wall using the formula: \(Q = U_\text{new} \cdot A \cdot \Delta T\), where \(Q\) is the rate of heat transfer, \(A\) is the area of the wall section, and \(\Delta T\) is the temperature difference. We're given that the wall section is 3 m high and 7 m long, so its area is: \(A = 3\,\mathrm{m} \times 7\,\mathrm{m} = 21\,\mathrm{m}^2\) Also, we're given that the indoor temperature is \(22^{\circ}\mathrm{C}\), and the outdoor temperature is \(-25^{\circ}\mathrm{C}\). Therefore, the temperature difference is: \(\Delta T = 22^{\circ}\mathrm{C} - (-25^{\circ}\mathrm{C})= 47\,\mathrm{K}\) Now, calculating the rate of heat transfer: \(Q = 0.731~\mathrm{W} / \mathrm{m}^{2} \cdot \mathrm{K} \times 21\,\mathrm{m}^2 \times 47\,\mathrm{K} = 720.729\,\mathrm{W}\). So, the new U-value of the wall is \(0.731 \,\mathrm{W} / \mathrm{m}^{2} \cdot \mathrm{K}\), and the rate of heat transfer through the modified wall section is \(720.729 \,\mathrm{W}\).

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 1-cm-diameter, 30-cm-long fin made of aluminum $(k=237 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\( is attached to a surface at \)80^{\circ} \mathrm{C}\(. The surface is exposed to ambient air at \)22^{\circ} \mathrm{C}$ with a heat transfer coefficient of $18 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$. If the fin can be assumed to be very long, the rate of heat transfer from the fin is (a) \(2.0 \mathrm{~W}\) (b) \(3.2 \mathrm{~W}\) (c) \(4.4 \mathrm{~W}\) (d) \(5.5 \mathrm{~W}\) (e) \(6.0 \mathrm{~W}\)

A 12 -m-long and 8-cm-diameter hot-water pipe of a district heating system is buried in the soil \(80 \mathrm{~cm}\) below the ground surface. The outer surface temperature of the pipe is \(60^{\circ} \mathrm{C}\). Taking the surface temperature of the earth to be \(2^{\circ} \mathrm{C}\) and the thermal conductivity of the soil at that location to be $0.9 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}$, determine the rate of heat loss from the pipe.

Consider a \(1.5-\mathrm{m}\)-high and 2 -m-wide triple pane window. The thickness of each glass layer $(k=0.80 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\( is \)0.5 \mathrm{~cm}$, and the thickness of each airspace \((k=0.025 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) is \(1.2 \mathrm{~cm}\). If the inner and outer surface temperatures of the window are $10^{\circ} \mathrm{C}\( and \)0^{\circ} \mathrm{C}$, respectively, the rate of heat loss through the window is (a) \(3.4 \mathrm{~W}\) (b) \(10.2 \mathrm{~W}\) (c) \(30.7 \mathrm{~W}\) (d) \(61.7 \mathrm{~W}\) (e) \(86.8 \mathrm{~W}\)

Consider a house with a flat roof whose outer dimensions are $12 \mathrm{~m} \times 12 \mathrm{~m}\(. The outer walls of the house are \)6 \mathrm{~m}$ high. The walls and the roof of the house are made of 20 -cm-thick concrete $(k=0.75 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})$. The temperatures of the inner and outer surfaces of the house are \(15^{\circ} \mathrm{C}\) and $3^{\circ} \mathrm{C}$, respectively. Accounting for the effects of the edges of adjoining surfaces, determine the rate of heat loss from the house through its walls and the roof. What is the error involved in ignoring the effects of the edges and corners and treating the roof as a $12-\mathrm{m} \times 12-\mathrm{m}\( surface and the walls as \)6-\mathrm{m} \times 12-\mathrm{m}$ surfaces for simplicity?

The heat transfer surface area of a fin is equal to the sum of all surfaces of the fin exposed to the surrounding medium, including the surface area of the fin tip. Under what conditions can we neglect heat transfer from the fin tip?

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