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One wall of a refrigerated warehouse is \(10.0\)-m-high and \(5.0\)-m-wide. The wall is made of three layers: \(1.0\)-cm-thick aluminum \((k=200 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}), 8.0\)-cm-thick fibreglass \((k=\) \(0.038 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\), and \(3.0-\mathrm{cm}\) thick gypsum board \((k=\) \(0.48 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\). The warehouse inside and outside temperatures are \(-10^{\circ} \mathrm{C}\) and \(20^{\circ} \mathrm{C}\), respectively, and the average value of both inside and outside heat transfer coefficients is \(40 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). (a) Calculate the rate of heat transfer across the warehouse wall in steady operation. (b) Suppose that 400 metal bolts \((k=43 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\), each \(2.0 \mathrm{~cm}\) in diameter and \(12.0 \mathrm{~cm}\) long, are used to fasten (i.e., hold together) the three wall layers. Calculate the rate of heat transfer for the "bolted" wall. (c) What is the percent change in the rate of heat transfer across the wall due to metal bolts?

Short Answer

Expert verified
Answer: The percent change in the rate of heat transfer across the wall due to metal bolts is 60.2%.

Step by step solution

01

Calculate Heat Transfer Across Each Layer Without Metal Bolts

To find the rate of heat transfer across each wall layer, first calculate the cross-sectional area and temperature difference for each layer, then apply the formula for heat transfer q for each layer. Area \(A\) for every layer: \(A = 10.0\textrm{ m} \times 5.0\textrm{ m} = 50.0\textrm{ m}^2\) Temperature difference \(\Delta T = 20^{\circ}\mathrm{C} - (-10^{\circ}\mathrm{C}) = 30^{\circ}\mathrm{C}\) Now calculate \(q\) for each layer: Aluminum: \(q_{Al} = \frac{200\textrm{ W/m}\cdot\textrm{K} \times 50\textrm{ m}^2 \times 30\textrm{ K}}{0.01\textrm{ m}} = 300000\textrm{ W}\) Fiberglass: \(q_{fib} = \frac{0.038\textrm{ W/m}\cdot\textrm{K} \times 50\textrm{ m}^2 \times 30\textrm{ K}}{0.08\textrm{ m}} = 713.5\textrm{ W}\) Gypsum: \(q_{gypsum} = \frac{0.48\textrm{ W/m}\cdot\textrm{K} \times 50\textrm{ m}^2 \times 30\textrm{ K}}{0.03\textrm{ m}} = 24000\textrm{ W}\)
02

Calculate the Total Heat Transfer Across Layered Wall Without Metal Bolts

To find the total heat transfer for the wall without metal bolts, first find the total thermal resistance without metal bolts, \(R_{total} = \frac{\Delta T}{q}\), and then apply the formula \(\Delta T=qR_{total}\): \(R_{total} = R_{Al} + R_{fib} + R_{gypsum} = \frac{0.01\textrm{ m}}{200\textrm{ W/m}\cdot\textrm{K} \times 50\textrm{ m}^2} + \frac{0.08\textrm{ m}}{0.038\textrm{ W/m}\cdot\textrm{K} \times 50\textrm{ m}^2} + \frac{0.03\textrm{ m}}{0.48\textrm{ W/m}\cdot\textrm{K} \times 50\textrm{ m}^2} = 1.3417\textrm{ K/W} \) Now, calculate the total heat transfer for the unbolted layered wall: \(q_{total-unbolted} = \frac{\Delta T}{R_{total}} = \frac{30\textrm{ K}}{1.3417\textrm{ K/W}} = 2235.6\textrm{ W}\)
03

Calculate Heat Transfer Across Metal Bolts

To calculate heat transfer across metal bolts, first calculate the cross-sectional area of one bolt and then apply the formula for heat transfer q for the bolts: Area of one bolt \(A_{bolt} = \pi(\frac{0.02\textrm{ m}}{2})^2 = 3.14\times10^{-4}\textrm{ m}^2\) \(q_{bolt} = \frac{43\textrm{ W/m}\cdot\textrm{K} \times 3.14\times10^{-4}\textrm{ m}^2 \times 30\textrm{ K}}{0.12\textrm{ m}} = 3.36\textrm{ W}\) Now, calculate the total heat transfer for 400 bolts: \(q_{bolts-total} = 400 \times 3.36\textrm{ W} = 1344\textrm{ W}\)
04

Calculate the Total Heat Transfer Across the Bolted Wall

To find the total heat transfer for the bolted wall, add the total heat transfer for the unbolted layered wall from Step 2 to the total heat transfer for the 400 metal bolts from Step 3: \(q_{total-bolted} = q_{total-unbolted} + q_{bolts-total} = 2235.6\textrm{ W} + 1344\textrm{ W} = 3579.6\textrm{ W}\)
05

Calculate the Percent Change in the Rate of Heat Transfer

To find the percent change in the rate of heat transfer across the wall due to metal bolts, use the following formula: Percent change \(= \frac{q_{total-bolted} - q_{total-unbolted}}{q_{total-unbolted}} \times 100\) Percent change \(= \frac{3579.6\textrm{ W} - 2235.6\textrm{ W}}{2235.6\textrm{ W}} \times 100 = 60.2\%\) Thus, the percent change in the rate of heat transfer across the wall due to metal bolts is 60.2%.

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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 material property that measures a material's ability to conduct heat. Represented by the symbol 'k', it's quantified as the amount of heat, in watts, that passes through a meter-thick sample of the material when there's a temperature difference of one degree Celsius across the material. The higher the 'k' value, the better the material is at transferring heat. In the context of our problem, we see materials with a wide range of thermal conductivity; aluminum with a high 'k' rapidly transfers heat, while fiberglass with a low 'k' is much slower.
Steady State Heat Transfer
Steady state heat transfer refers to a condition where the temperature within each layer of the wall doesn't change with time, even though heat is constantly being transferred through the material. This implies that the rate at which heat enters a layer is equal to the rate at which it leaves, leading to a consistent temperature profile over time. In our problem, this principle enables us to calculate the heat transfer rate across different layers of the wall as if they were steady over time, simplifying the mathematical modeling of the process.
Thermal Resistance
Thermal resistance is the measure of a material's resistance to heat flow and is the reciprocal of thermal conductivity. High thermal resistance means the material is a good insulator, and it's measured in units of 'K/W' (Kelvin per Watt). In the given exercise, we add up the thermal resistances of each layer to find the total resistance, which then helps in determining the overall rate of heat transfer across the wall. Calculation of thermal resistance is key to designing insulating systems and for understanding how various construction materials will impact heat loss.
Conductance of Materials
Conductance, often denoted by 'C', is the reciprocal of resistance and is a measure of how easily heat flows through a material. Higher conductance values indicate that the material conducts heat more readily. In the context of our problem, the conductance of each material layer, and that added by the metal bolts, influences the overall rate of heat transfer. The bolts, acting as thermal bridges, considerably increase the total conductance and thus the rate of heat transfer, leading to the observed change in the insulation properties of the wall.

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Most popular questions from this chapter

The plumbing system of a house involves a \(0.5-\mathrm{m}\) section of a plastic pipe \((k=0.16 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) of inner diameter \(2 \mathrm{~cm}\) and outer diameter \(2.4 \mathrm{~cm}\) exposed to the ambient air. During a cold and windy night, the ambient air temperature remains at about \(-5^{\circ} \mathrm{C}\) for a period of \(14 \mathrm{~h}\). The combined convection and radiation heat transfer coefficient on the outer surface of the pipe is estimated to be \(40 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), and the heat of fusion of water is \(333.7 \mathrm{~kJ} / \mathrm{kg}\). Assuming the pipe to contain stationary water initially at \(0^{\circ} \mathrm{C}\), determine if the water in that section of the pipe will completely freeze that night.

Two flow passages with different cross-sectional shapes, one circular another square, are each centered in a square solid bar of the same dimension and thermal conductivity. Both configurations have the same length, \(T_{1}\), and \(T_{2}\). Determine which configuration has the higher rate of heat transfer through the square solid bar for \((a) a=1.2 b\) and \((b) a=2 b\).

Consider two metal plates pressed against each other. Other things being equal, which of the measures below will cause the thermal contact resistance to increase? (a) Cleaning the surfaces to make them shinier. (b) Pressing the plates against each other with a greater force. (c) Filling the gap with a conducting fluid. (d) Using softer metals. (e) Coating the contact surfaces with a thin layer of soft metal such as tin.

The unit thermal resistances ( \(R\)-values) of both 40-mm and 90-mm vertical air spaces are given in Table 3-9 to be \(0.22 \mathrm{~m}^{2} \cdot \mathrm{C} / \mathrm{W}\), which implies that more than doubling the thickness of air space in a wall has no effect on heat transfer through the wall. Do you think this is a typing error? Explain.

Exposure to high concentration of gaseous ammonia can cause lung damage. To prevent gaseous ammonia from leaking out, ammonia is transported in its liquid state through a pipe \(\left(k=25 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, D_{i}=2.5 \mathrm{~cm}\right.\), \(D_{o}=4 \mathrm{~cm}\), and \(L=10 \mathrm{~m}\) ). Since liquid ammonia has a normal boiling point of \(-33.3^{\circ} \mathrm{C}\), the pipe needs to be properly insulated to prevent the surrounding heat from causing the ammonia to boil. The pipe is situated in a laboratory, where the average ambient air temperature is \(20^{\circ} \mathrm{C}\). The convection heat transfer coefficients of the liquid hydrogen and the ambient air are \(100 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) and \(20 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), respectively. Determine the insulation thickness for the pipe using a material with \(k=\) \(0.75 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) to keep the liquid ammonia flowing at an average temperature of \(-35^{\circ} \mathrm{C}\), while maintaining the insulated pipe outer surface temperature at \(10^{\circ} \mathrm{C}\).

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