/*! 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 88 A vertical \(1.5\)-m-high, 2.8-m... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A vertical \(1.5\)-m-high, 2.8-m-wide double-pane window consists of two layers of glass separated by a \(2.0\)-cm air gap at atmospheric pressure. The room temperature is \(26^{\circ} \mathrm{C}\) while the inner glass temperature is \(18^{\circ} \mathrm{C}\). Disregarding radiation heat transfer, determine the temperature of the outer glass layer and the rate of heat loss through the window by natural convection.

Short Answer

Expert verified
Answer: The temperature of the outer glass layer is 16.42°C and the rate of heat loss through the window by natural convection is 124.53 W.

Step by step solution

01

Find Grashof Number

To find the Grashof number, we need to know the properties of the air at the average temperature between the inner and outer glass layers. We can find this average temperature as: $$T_{avg} = \frac{T_{room} + T_{inner}}{2}$$ Plugging in the given values, we find the average temperature: $$T_{avg} = \frac{26^{\circ} \mathrm{C} + 18^{\circ} \mathrm{C}}{2} = 22^{\circ} \mathrm{C}$$ At this temperature, we can look up the air properties of kinematic viscosity (\(\nu\)) and thermal expansion coefficient (\(\beta\)) from standard air tables. For this case, we can use: $$\beta = 3.39 \times 10^{-3} \,\mathrm{K}^{-1}$$ $$\nu = 15.89 \times 10^{-6} \,\mathrm{m}^{2}/\mathrm{s}$$ Now we can find the Grashof number using the formula: $$Gr = \frac{g \beta (T_{room} - T_{inner}) L^3}{\nu^2}$$ Plugging in the given values and the values we found for air properties: $$Gr = \frac{9.81 \, \mathrm{m/s^2} \cdot 3.39 \times 10^{-3} \,\mathrm{K}^{-1} \cdot (26 - 18) \,\mathrm{K} \cdot (0.02 \, \mathrm{m})^3}{(15.89 \times 10^{-6} \,\mathrm{m}^{2}/\mathrm{s})^2}$$ Calculating the Grashof number, we get: $$Gr = 192,165$$
02

Find Nusselt Number

Now we need to find the Nusselt number, which can be correlated as a function of the Grashof number and Prandtl number for natural convection. For a vertical air gap, we can use the following correlation: $$Nu = 0.138 \cdot (Gr \cdot Pr)^{1/3}$$ We need to find the Prandtl number, which is defined as the ratio of momentum diffusivity to thermal diffusivity: $$Pr = \frac{\nu}{\alpha}$$ For air at \(22^{\circ} \mathrm{C}\), we can find the thermal diffusivity (\(\alpha\)) from standard air tables. For this case, we can use: $$\alpha = 22.49\times 10^{-6} \,\mathrm{m}^{2}/\mathrm{s}$$ Plugging in the value for kinematic viscosity (\(\nu\)) found earlier, we can calculate the Prandtl number: $$Pr = \frac{15.89 \times 10^{-6} \, \mathrm{m}^{2}/\mathrm{s}}{22.49 \times 10^{-6} \, \mathrm{m}^{2}/\mathrm{s}}$$ $$Pr = 0.707$$ Now substituting Gr and Pr in the Nusselt number correlation: $$Nu = 0.138 \cdot (192,165 \cdot 0.707)^{1/3}$$ Calculating the Nusselt number, we get: $$Nu = 14.312$$
03

Find Heat Transfer Coefficient

Now that we have the Nusselt number, we can find the heat transfer coefficient (\(h\)) using the following formula: $$h = \frac{Nu \cdot k}{L}$$ At \(22^{\circ} \mathrm{C}\), we can find the thermal conductivity (\(k\)) of air from standard air tables: $$k = 0.026 \, \mathrm{W/m} \cdot \mathrm{K}$$ Plugging in the given air gap thickness (\(L\)) and the values for \(Nusselt \, number\) and \(thermal \, conductivity\), we can calculate the heat transfer coefficient: $$h = \frac{14.312 \cdot 0.026 \, \mathrm{W/m} \cdot \mathrm{K}}{0.02 \, \mathrm{m}}$$ $$h = 18.808 \, \mathrm{W/m}^2 \cdot \mathrm{K}$$
04

Find Temperature of the Outer Glass Layer and Heat Loss

Finally, we can find the temperature of the outer glass layer (\(T_{outer}\)) by rearranging the formula for heat transfer and solving for \(T_{outer}\): $$q = hA(T_{room} - T_{outer})$$ $$T_{outer} = T_{room} - \frac{q}{h \cdot A}$$ We can find the heat loss per unit area (\(q'\)) using the formula: $$q' = h(T_{inner} - T_{outer})$$ $$q = q' \cdot A$$ $$T_{outer} = T_{room} - \frac{h(T_{inner} - T_{outer}) \cdot A}{h \cdot A}$$ $$T_{outer} = T_{room} - h(T_{inner} - T_{outer})$$ Plugging in the given values and the values we found for \(h\) and \(T_{room}\), we can find the temperature of the outer glass layer: $$18^{\circ} \mathrm{C} = 26^{\circ} \mathrm{C} - 18.808 \, \mathrm{W/m}^2 \cdot \mathrm{K}(T_{outer} - 18^{\circ} \mathrm{C})$$ $$T_{outer} = 16.42^{\circ} \mathrm{C}$$ Next, we can find the heat loss per unit area (\(q'\)) from the heat transfer formula: $$q' = 18.808 \, \mathrm{W/m}^2 \cdot \mathrm{K}(18^{\circ} \mathrm{C} - 16.42^{\circ} \mathrm{C})$$ $$q' = 29.72 \, \mathrm{W/m}^2$$ Now, we can find the total heat loss (\(q\)) by multiplying the heat loss per unit area by the total area of the window: $$q = 29.72 \, \mathrm{W/m}^2 \times (1.5\,\mathrm{m} \times 2.8 \,\mathrm{m})$$ $$q = 124.53 \, \mathrm{W}$$ So, the temperature of the outer glass layer is \(16.42^{\circ} \mathrm{C}\) and the rate of heat loss through the window by natural convection is \(124.53 \mathrm{W}\).

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 91Ó°ÊÓ!

Key Concepts

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

Grashof number
When it comes to understanding natural convection heat transfer, the Grashof number is an indispensable dimensionless parameter. It represents the ratio of buoyancy to viscous forces in a fluid. In essence, the Grashof number gives us an idea of how significant natural convection will be for a given scenario.

To illustrate, let us tackle the scenario from the exercise. We know the Grashof number equation as:
\[Gr = \frac{g \beta (T_{room} - T_{inner}) L^3}{u^2}\]
Here, \(g\) stands for gravitational acceleration, \(\beta\) is the thermal expansion coefficient, indicating how much the fluid volume expands or contracts with temperature, \(u\) is kinematic viscosity, and \(L\) is a characteristic length, which is the air gap in our case.

Using the provided numbers for room and inner glass temperatures, as well as the air properties at the average temperature, we can calculate the Grashof number. A higher Grashof number suggests a stronger convection current due to the larger force of buoyancy compared to viscous forces. Consequently, this drives the heat transfer between the window panes.
Nusselt number
Moving forward, the Nusselt number emerges as another critical dimensionless quantity in the study of heat transfer. It correlates the convective to conductive heat transfer at a boundary in a fluid. In the context of our exercise, the Nusselt number helps us assess the effectiveness of convective heat transfer in comparison to conduction.

The Nusselt number can be determined through the correlation:
\[Nu = C \times (Gr \cdot Pr)^{1/n}\]
where \(C\) and \(n\) are empirical constants, and \(Pr\) represents the Prandtl number. This Prandtl number gives an idea of the fluid's viscosity relative to its thermal diffusivity.

In our exercise, we calculated the Nusselt number using the relationship for natural convection in a vertical plane. This is important because it influences the heat transfer coefficient, which we need for determining the heat loss rate through the window.
Heat transfer coefficient
The heat transfer coefficient, \(h\), is a key value in quantifying the rate of heat transfer between a solid surface and a fluid moving past it. In the scenario of the double-pane window, knowing the heat transfer coefficient allows us to figure out the amount of heat passing from the room through the window panes.

We utilize the Nusselt number to find \(h\) by the relationship:
\[h = \frac{Nu \cdot k}{L}\]
This equation ties together the convective heat transfer aspects captured by the Nusselt number with the material property of thermal conductivity, \(k\), over the characteristic length, \(L\). In our exercise, the result is a specific value of \(h\), which signifies the efficiency of heat transfer via natural convection within the air gap of the window.
Thermal conductivity
Lastly, thermal conductivity, denoted as \(k\), is an intrinsic property of a material that describes its ability to conduct heat. High thermal conductivity implies that the material is a good conductor of heat, and vice versa for a low value.

In our double-pane window scenario, the thermal conductivity of air plays a vital role. It factors into the heat transfer coefficient calculation and inherently affects how heat migrates through the air gap between the window panes. Materials selection for windows or any thermal insulation system often revolves around this property to ensure efficient thermal management.

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 room is to be heated by a coal-burning stove, which is a cylindrical cavity with an outer diameter of \(32 \mathrm{~cm}\) and a height of \(70 \mathrm{~cm}\). The rate of heat loss from the room is estimated to be \(1.5 \mathrm{~kW}\) when the air temperature in the room is maintained constant at \(24^{\circ} \mathrm{C}\). The emissivity of the stove surface is \(0.85\), and the average temperature of the surrounding wall surfaces is \(14^{\circ} \mathrm{C}\). Determine the surface temperature of the stove. Neglect the heat transfer from the bottom surface and take the heat transfer coefficient at the top surface to be the same as that on the side surface. The heating value of the coal is \(30,000 \mathrm{~kJ} / \mathrm{kg}\), and the combustion efficiency is 65 percent. Determine the amount of coal burned a day if the stove operates \(14 \mathrm{~h}\) a day. Evaluate air properties at a film temperature of \(77^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\) pressure. Is this a good assumption?

What does the effective conductivity of an enclosure represent? How is the ratio of the effective conductivity to thermal conductivity related to the Nusselt number?

The side surfaces of a 3-m-high cubic industrial (?) furnace burning natural gas are not insulated, and the temperature at the outer surface of this section is measured to be \(110^{\circ} \mathrm{C}\). The temperature of the furnace room, including its surfaces, is \(30^{\circ} \mathrm{C}\), and the emissivity of the outer surface of the furnace is 0.7. It is proposed that this section of the furnace wall be insulated with glass wool insulation \((k=0.038 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) wrapped by a reflective sheet \((\varepsilon=0.2)\) in order to reduce the heat loss by 90 percent. Assuming the outer surface temperature of the metal section still remains at about \(110^{\circ} \mathrm{C}\), determine the thickness of the insulation that needs to be used. The furnace operates continuously throughout the year and has an efficiency of 78 percent. The price of the natural gas is \(\$ 1.10 /\) therm ( 1 therm \(=105,500 \mathrm{~kJ}\) of energy content). If the installation of the insulation will cost \(\$ 550\) for materials and labor, determine how long it will take for the insulation to pay for itself from the energy it saves.

Determine the \(U\)-factor for the center-of-glass section of a double-pane window with a 13-mm air space for winter design conditions. The glazings are made of clear glass having an emissivity of \(0.84\). Take the average air space temperature at design conditions to be \(10^{\circ} \mathrm{C}\) and the temperature difference across the air space to be \(15^{\circ} \mathrm{C}\).

A hot object suspended by a string is to be cooled by natural convection in fluids whose volume changes differently with temperature at constant pressure. In which fluid will the rate of cooling be lowest? With increasing temperature, a fluid whose volume (a) increases a lot (b) increases slightly (c) does not change (d) decreases slightly (e) decreases a lot.

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.