During a visit to a plastic sheeting plant, it was observed that a 60 -m-long section of a 2 -in nominal \((6.03\)-cm-outerdiameter) steam pipe extended from one end of the plant to the other with no insulation on it. The temperature measurements at several locations revealed that the average temperature of the exposed surfaces of the steam pipe was \(170^{\circ} \mathrm{C}\), while the temperature of the surrounding air was \(20^{\circ} \mathrm{C}\). The outer surface of the pipe appeared to be oxidized, and its emissivity can be taken to be \(0.7\). Taking the temperature of the surrounding surfaces to be \(20^{\circ} \mathrm{C}\) also, determine the rate of heat loss from the steam pipe. Steam is generated in a gas furnace that has an efficiency of 78 percent, and the plant pays \(\$ 1.10\) per therm ( 1 therm \(=\) \(105,500 \mathrm{~kJ}\) ) of natural gas. The plant operates \(24 \mathrm{~h}\) a day 365 days a year, and thus \(8760 \mathrm{~h}\) a year. Determine the annual cost of the heat losses from the steam pipe for this facility.

Short Answer

Expert verified
Answer: The rate of heat loss for the steam pipe is 23,158 W, and the annual cost of heat losses is $2,710.12.

Step by step solution

01

Calculate convective heat loss

To calculate the convective heat loss, we can use the formula: \(Q_{conv} = h\cdot A\cdot (T_s - T_\infty)\) where: \(Q_{conv}\) = convective heat loss (W) \(h\) = convection heat transfer coefficient (W/m²°C) \(A\) = surface area (m²) \(T_s\) = steam pipe surface temperature (°C) \(T_\infty\) = surrounding air temperature (°C) For this exercise, we are not given the value of \(h\), so we will assume it to be an average value of 10 W/m²°C for free convection from a horizontal cylinder to air, as found in standard heat transfer texts. The steam pipe has a length of 60 m and an outer diameter of 6.03 cm. To calculate the surface area, we can use the formula: \(A = L \cdot D_\text{outer} \cdot \pi\) where: \(D_\text{outer}\) = outer diameter (m) \(L\) = length of the pipe (m) Calculating the surface area: \(A = 60 \cdot 0.0603 \cdot \pi = 11.36 \mathrm{~m^2}\) Now we can determine \(Q_{conv}\): \(Q_{conv} = 10 \cdot 11.36 \cdot (170 - 20) = 10 \cdot 11.36 \cdot 150 = 17,040 \mathrm{~W}\)
02

Calculate radiative heat loss

To calculate the radiative heat loss, we can use the formula: \(Q_{rad} = \epsilon \cdot \sigma \cdot A \cdot (T_s^4 - T_\infty^4)\) where: \(Q_{rad}\) = radiative heat loss (W) \(\epsilon\) = emissivity of the pipe surface (dimensionless) \(\sigma\) = Stefan-Boltzmann constant (\(5.67 \times 10^{-8} \mathrm{~W/m^2K^4}\)) \(T_s\) and \(T_\infty\) = temperature in Kelvin Now we can convert temperatures to Kelvin and determine \(Q_{rad}\): \(T_s = 170 + 273.15 = 443.15 \mathrm{~K}\) \(T_\infty = 20 + 273.15 = 293.15 \mathrm{~K}\) \(Q_{rad} = 0.7 \cdot 5.67 \times 10^{-8} \cdot 11.36 \cdot (443.15^4 - 293.15^4) = 6,118 \mathrm{~W}\)
03

Calculate total heat loss

The total heat loss is the sum of the convective and radiative heat losses: \(Q_\text{total} = Q_{conv} + Q_{rad} = 17,040 + 6,118 = 23,158 \mathrm{~W}\)
04

Calculate the annual cost of heat losses

We can now use the total heat loss rate to determine the annual cost of this heat loss. First, we need to find the energy loss per year: \(E_\text{loss} = Q_\text{total} \cdot t_\text{operating}\) where: \(t_\text{operating}\) = operating hours per year (8760 h) \(E_\text{loss} = 23,158 \mathrm{~W} \cdot 8,760 \mathrm{~h} = 202,944,880 \mathrm{~Wh} = 202,944.88 \mathrm{~kWh}\) Next, we can calculate the energy content of the fuel used per year: \(E_\text{fuel} = \frac{E_\text{loss}}{\eta}\) where: \(\eta\) = gas furnace efficiency (0.78) \(E_\text{fuel} = \frac{202,944.880 \mathrm{~kWh}}{0.78} = 260,187.282 \mathrm{~kWh}\) Finally, we can calculate the annual cost of heat losses: \(C_\text{annual} = \frac{E_\text{fuel}}{105.5 \mathrm{~kWh/therm}} \cdot \$1.10 \mathrm{/therm}\) \(C_\text{annual} = \frac{260,187.282 \mathrm{~kWh}}{105.5 \mathrm{~kWh/therm}} \cdot \$1.10 \mathrm{/therm} = \$2,710.12\) Therefore, the annual cost of the heat losses from the steam pipe for this facility is $2,710.12.

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Most popular questions from this chapter

A horizontal \(1.5\)-m-wide, \(4.5\)-m-long double-pane window consists of two sheets of glass separated by a \(3.5-\mathrm{cm}\) gap filled with water. If the glass surface temperatures at the bottom and the top are measured to be \(60^{\circ} \mathrm{C}\) and \(40^{\circ} \mathrm{C}\), respectively, the rate of heat transfer through the window is (a) \(27.6 \mathrm{~kW}\) (b) \(39.4 \mathrm{~kW}\) (c) \(59.6 \mathrm{~kW}\) (d) \(66.4 \mathrm{~kW} \quad(e) 75.5 \mathrm{~kW}\) (For water, use \(k=0.644 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \operatorname{Pr}=3.55, v=\) \(0.554 \times 10^{-6} \mathrm{~m}^{2} / \mathrm{s}, \beta=0.451 \times 10^{-3} \mathrm{~K}^{-1}\). Also, the applicable correlation is \(\mathrm{Nu}=0.069 \mathrm{Ra}^{1 / 3} \operatorname{Pr}^{0.074}\) ).

A 3 -mm-diameter and 12-m-long electric wire is tightly wrapped with a \(1.5-\mathrm{mm}\)-thick plastic cover whose thermal conductivity and emissivity are \(k=0.20 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and \(\varepsilon=0.9\). Electrical measurements indicate that a current of \(10 \mathrm{~A}\) passes through the wire and there is a voltage drop of \(7 \mathrm{~V}\) along the wire. If the insulated wire is exposed to calm atmospheric air at \(T_{\infty}=30^{\circ} \mathrm{C}\), determine the temperature at the interface of the wire and the plastic cover in steady operation. Take the surrounding surfaces to be at about the same temperature as the air. Evaluate air properties at a film temperature of \(40^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\) pressure. Is this a good assumption?

A vertical double-pane window consists of two sheets of glass separated by a \(1.5-\mathrm{cm}\) air gap at atmospheric pressure. The glass surface temperatures across the air gap are measured to be \(278 \mathrm{~K}\) and \(288 \mathrm{~K}\). If it is estimated that the heat transfer by convection through the enclosure is \(1.5\) times that by pure conduction and that the rate of heat transfer by radiation through the enclosure is about the same magnitude as the convection, the effective emissivity of the two glass surfaces is (a) \(0.47\) (b) \(0.53\) (c) \(0.61\) (d) \(0.65\) (e) \(0.72\)

When neither natural nor forced convection is negligible, is it correct to calculate each independently and add them to determine the total convection heat transfer?

A vertical \(0.9\)-m-high and \(1.8\)-m-wide double-pane window consists of two sheets of glass separated by a \(2.2-\mathrm{cm}\) 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) \(19.8 \mathrm{~W}\) (b) \(26.1 \mathrm{~W}\) (c) \(30.5 \mathrm{~W}\) (d) \(34.7 \mathrm{~W}\) (e) \(55.0 \mathrm{~W}\) (For air, use \(k=0.02551 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \operatorname{Pr}=0.7296, v=\) \(1.562 \times 10^{-5} \mathrm{~m}^{2} / \mathrm{s}\). Also, the applicable correlation is \(\mathrm{Nu}\) \(\left.=0.42 \mathrm{Ra}^{1 / 4} \mathrm{Pr}^{0.012}(H / L)^{-0.3}\right)\) (For air, use \(k=0.02588 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \operatorname{Pr}=0.7282, v=1.608 \times\) \(10^{-5} \mathrm{~m}^{2} / \mathrm{s}\) )

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