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Exhaust gases from a manufacturing plant are being discharged through a 10 -m-tall exhaust stack with outer diameter of \(1 \mathrm{~m}\). The exhaust gases are discharged at a rate of \(0.125 \mathrm{~kg} / \mathrm{s}\), while temperature drop between inlet and exit of the exhaust stack is $30^{\circ} \mathrm{C}$, and the constant pressure-specific heat of the exhaust gases is \(1600 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\). On a particular calm day, the surrounding quiescent air temperature is \(33^{\circ} \mathrm{C}\). Solar radiation is incident on the exhaust stack outer surface at a rate of $500 \mathrm{~W} / \mathrm{m}^{2}$, and both the emissivity and solar absorptivity of the outer surface are \(0.9\). Determine the exhaust stack outer surface temperature. Assume the film temperature is \(60^{\circ} \mathrm{C}\).

Short Answer

Expert verified
The outer surface temperature of the exhaust stack is approximately 210.73°C.

Step by step solution

01

Calculate the exhaust stack surface area

The exhaust stack is a cylinder with height of 10 m and diameter of 1 m. The surface area \(A\) of a cylinder is given by \(A=2\pi rh\), where \(r\) is the radius and \(h\) is the height. So, we have: \(A = 2\pi \times 0.5 \times 10 = 31.42 \mathrm{~m^2}\)
02

Determine the heat transfer rate due to convection

The temperature drop \(\Delta T\) between the inlet and exit of the exhaust stack is given: \(\Delta T = 30^{\circ} \mathrm{C}\) The heat transfer rate \(Q_\mathrm{conv}\) due to convection can be calculated by using the mass flow rate (\(\dot{m}\)), the specific heat of the exhaust gases (\(c_P\)), and temperature drop \(\Delta T\): \(Q_\mathrm{conv} = \dot{m} \times c_P \times \Delta T = 0.125\mathrm{~kg/s} \times 1600\mathrm{~J/(kg\cdot K)} \times 30^{\circ}\mathrm{C} = 6000\mathrm{~W}\)
03

Calculate the heat transfer rate due to radiation

We will use the energy balance equation to find the heat transfer rate due to radiation. The energy balance equation is: \(Q_\mathrm{conv} - Q_\mathrm{rad} = Q_\mathrm{abs}\) But first, we need to find the value for the emissivity \(\epsilon\) and the Stefan-Boltzmann constant \(\sigma\). We are given the emissivity of the outer surface as 0.9. The Stefan-Boltzmann constant value is: \(\sigma = 5.67\times10^{-8} \mathrm{~W/(m^{2}\cdot K^{4})}\) Next, we need to convert the film temperature to Kelvin, which is given as: \(T_\mathrm{film} = 60^{\circ}\mathrm{C} + 273.15 = 333.15\mathrm{~K}\) Now we can calculate the heat transfer rate due to radiation \(Q_\mathrm{rad}\) using the following formula: \(Q_\mathrm{rad} = \epsilon \sigma A(T_\mathrm{s}^{4} - T_\mathrm{film}^{4})\)
04

Compute the heat absorbed due to solar radiation

To calculate the heat absorbed by the exhaust stack due to solar radiation, we need the solar absorptivity \(\alpha\), which is given as 0.9. The heat absorbed per unit area can be calculated as: \(Q_\mathrm{abs,per\,unit\,area} = \alpha \cdot I = 0.9 \times 500\mathrm{~W/m^{2}} = 450\mathrm{~W/m^{2}}\) The total heat absorbed \(Q_\mathrm{abs}\) can be calculated by multiplying the heat absorbed per unit area with the total surface area of the exhaust stack: \(Q_\mathrm{abs} = Q_\mathrm{abs,per\,unit\,area} \times A = 450\mathrm{~W/m^{2}} \times 31.42\mathrm{~m^{2}} = 14,139\mathrm{~W}\)
05

Apply the energy balance equation to find the outer surface temperature

Now we can use the energy balance equation to find the outer surface temperature \(T_s\): \(Q_\mathrm{conv} - Q_\mathrm{rad} = Q_\mathrm{abs}\) Substituting values: \(6000\mathrm{~W} - 0.9 \times 5.67\times10^{-8}\mathrm{~W/(m^{2}\cdot K^{4})} \times 31.42\mathrm{~m^{2}} (T_\mathrm{s}^{4} - 333.15\mathrm{~K}^{4}) = 14,139\mathrm{~W}\) Solve for \(T_\mathrm{s}\): \((T_\mathrm{s}^{4} - 333.15\mathrm{~K}^{4}) = \frac{14,139\mathrm{~W} - 6000\mathrm{~W}}{0.9 \times 5.67\times10^{-8}\mathrm{~W/(m^{2}\cdot K^{4})} \times 31.42\mathrm{~m^{2}}} = 5.79\times10^{8}\mathrm{~K^{4}}\) \(T_\mathrm{s}^{4} = 5.79\times10^{8}\mathrm{~K^{4}} + 333.15\mathrm{~K}^{4} = 2.15\times10^{9}\mathrm{~K^{4}}\) \(T_\mathrm{s} = \sqrt[4]{2.15\times10^{9}\mathrm{~K^{4}}} = 483.88\mathrm{~K}\) Convert back to Celsius: \(T_\mathrm{s} = 483.88\mathrm{~K} - 273.15 = 210.73^{\circ}\mathrm{C}\) So, the exhaust stack outer surface temperature is approximately \(210.73^{\circ} \mathrm{C}\).

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Most popular questions from this chapter

A spherical tank \((k=15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) with an inner diameter of \(3 \mathrm{~m}\) and a wall thickness of \(10 \mathrm{~mm}\) is used for storing hot liquid. The hot liquid inside the tank causes the inner surface temperature to be as high as \(100^{\circ} \mathrm{C}\). To prevent thermal burns to the people working near the tank, the tank is covered with a \(7-\mathrm{cm}\)-thick layer of insulation $(k=0.15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})$, and the outer surface is painted to give an emissivity of \(0.35\). The tank is located in surroundings with air at $16^{\circ} \mathrm{C}$. Determine whether or not the insulation layer is sufficient to keep the outer surface temperature below \(45^{\circ} \mathrm{C}\) to prevent thermal burn hazards. Discuss ways to further decrease the outer surface temperature. Evaluate the air properties at \(30^{\circ} \mathrm{C}\) and $1 \mathrm{~atm}$ pressure. Is this a good assumption?

Consider an ordinary house with \(R-13\) walls (walls that have an \(R\)-value of $\left.13 \mathrm{~h} \cdot \mathrm{ft}^{2}{ }^{\circ} \mathrm{F} / \mathrm{B} t \mathrm{u}\right)\(. Compare this to the \)R$-value of the common double-door windows that are double pane with \(\frac{1}{4}\) in of airspace and have aluminum frames. If the windows occupy only 20 percent of the wall area, determine if more heat is lost through the windows or through the remaining 80 percent of the wall area. Disregard infiltration losses.

A hot fluid $\left(k_{\text {fluid }}=0.72 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right)$ is flowing as a laminar fully developed flow inside a pipe with an inner diameter of \(35 \mathrm{~mm}\) and a wall thickness of $5 \mathrm{~mm}\(. The pipe is \)10 \mathrm{~m}$ long, and the outer surface is exposed to air at \(10^{\circ} \mathrm{C}\). The average temperature difference between the hot fluid and the pipe inner surface is $\Delta T_{\text {avg }}=10^{\circ} \mathrm{C}$, and the inner and outer surface temperatures are constant. Determine the outer surface temperature of the pipe. Evaluate the air properties at \(50^{\circ} \mathrm{C}\). Is this a good assumption?

Consider a vertical plate with length \(L\), placed in quiescent air. If the film temperature is \(20^{\circ} \mathrm{C}\) and the average Nusselt number in natural convection is of the form \(\mathrm{Nu}=\mathrm{CRa}_{L}^{n}\), show that the average heat transfer coefficient can be expressed as $$ \begin{aligned} h &=1.51(\Delta T / L)^{1 / 4} \quad 10^{4}<\mathrm{Ra}_{L}<10^{9} \\ h &=1.19 \Delta T^{1 / 3} \quad 10^{10}<\mathrm{Ra}_{L}<10^{13} \end{aligned} $$

A vertical \(0.9\)-m-high and \(1.5\)-m-wide double-pane window consists of two sheets of glass separated by a \(2.0-\mathrm{cm}\) air gap at atmospheric pressure. If the glass surface temperatures across the air gap are measured to be \(20^{\circ} \mathrm{C}\) and \(30^{\circ} \mathrm{C}\), the rate of heat transfer through the window is (a) \(16.3 \mathrm{~W}\) (b) \(21.7 \mathrm{~W}\) (c) \(24.0 \mathrm{~W}\) $\begin{array}{ll}\text { (d) } 31.3 \mathrm{~W} & \text { (e) } 44.6 \mathrm{~W}\end{array}$ (For air, use $k=0.02551 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \quad \operatorname{Pr}=0.7296\(, \)\nu=1.562 \times 10^{-5} \mathrm{~m}^{2} / \mathrm{s}\(. Also, the applicable correlation is \)\left.\mathrm{Nu}=0.42 \mathrm{Ra}^{1 / 4} \operatorname{Pr}^{0.012}(H / L)^{-0.3} .\right)$

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