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To defrost ice accumulated on the outer surface of an automobile windshield, warm air is blown over the inner surface of the windshield. Consider an automobile windshield with thickness of \(5 \mathrm{~mm}\) and thermal conductivity of \(1.4 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The outside ambient temperature is \(-10^{\circ} \mathrm{C}\) and the convection heat transfer coefficient is \(200 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), while the ambient temperature inside the automobile is $25^{\circ} \mathrm{C}$. Determine the value of the convection heat transfer coefficient for the warm air blowing over the inner surface of the windshield necessary to cause the accumulated ice to begin melting.

Short Answer

Expert verified
Short Answer: The convection heat transfer coefficient for the warm air blowing over the inner surface of the windshield necessary to cause the accumulated ice to begin melting is \(0.007 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\).

Step by step solution

01

Calculate the heat transfer through the windshield

First, let's determine the heat transfer through the windshield using the equation mentioned above. We are given \(Q_{conv}\) and we have provided the values for thermal conductivity \((k)\), the density difference \((T_{hot} - T_{cold})\), and thickness \((L)\). Therefore, we can set up the following equation: \(Q_{conv} = k\frac{A(T_{hot} - T_{cold})}{L}\)
02

Substitute the values

Plug in the given values: $$Q_{conv} = 1.4\frac{A(25-(-10))}{0.005}$$ $$Q_{conv} = 9.8A$$
03

Calculate the heat transfer at the outer surface of the windshield

Now, let's find \(Q_{conv}\) from the outer surface's convection heat transfer coefficient \((h_{out})\) and temperature difference: $$Q_{conv} = 200A(-10-T_0)$$ Divide \(9.8A\) by \(200A\) $$\frac{9.8}{200} = \frac{Q_{conv}}{200A} = \frac{-10-T_0}{-10}$$ Now we can find \(T_0\): $$T_0 = -10 - \frac{9.8}{200}(10)$$
04

Calculate the temperature at the outer surface of the windshield, \(T_0\)

Solve for \(T_0\) $$T_0 = -10 - \frac{49}{10} = -14.9^{\circ}C$$
05

Set up the equation for the heat transfer rate by convection inside the car

Now, we will find the heat transfer rate by convection inside the car using the following relationship: \(Q_{conv_{in}} = h_{in}A(T_{in} - T_1)\) Since we have determined \(Q_{conv}\) (the heat transfer through the windshield), we can equate it with \(Q_{conv_{in}}\): $$9.8A = h_{in}A(25 - T_1)$$
06

Calculate the temperature at the inner surface of the windshield, \(T_1\)

From the equation in Step 1, we have: $$9.8A = 1.4\frac{A(25-T_1)}{0.005}$$ Divide \(1.4A\) by \(0.005A\): $$\frac{9.8}{0.007} = 25 - T_1$$ Now we can find \(T_1\): $$T_1 = 25 - \frac{9.8}{0.007}$$
07

Solve for \(T_1\)#

Calculate \(T_1\): $$T_1 = 25 - 1400 = -1375^{\circ}C$$
08

Calculate the convection heat transfer coefficient for the warm air, \(h_{in}\)

Now, we can find \(h_{in}\) by plugging in the values of \(T_{in}\) and \(T_1\) in the equation from Step 5: $$9.8A = h_{in}A(25 - (-1375))$$ Divide \(9.8A\) by \(1400A\): $$h_{in} = \frac{9.8A}{1400A}$$
09

Solve for \(h_{in}\)

Calculate the convection heat transfer coefficient, \(h_{in}\): $$h_{in} = \frac{9.8}{1400} = 0.007 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$$ The convection heat transfer coefficient for the warm air blowing over the inner surface of the windshield necessary to cause the accumulated ice to begin melting is \(0.007 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\).

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Most popular questions from this chapter

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?

A cylindrical pin fin of diameter \(0.6 \mathrm{~cm}\) and length of $3 \mathrm{~cm}$ with negligible heat loss from the tip has an efficiency of 0.7. The effectiveness of this fin is (a) \(0.3\) (b) \(0.7\) (c) 2 (d) 8 (e) 14

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.

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