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A simple solar collector is built by placing a 6-cmdiameter clear plastic tube around a garden hose whose outer diameter is \(2 \mathrm{~cm}\) (Fig. P13-137). The hose is painted black to maximize solar absorption, and some plastic rings are used to keep the spacing between the hose and the clear plastic cover constant. The emissivities of the hose surface and the glass cover are \(0.9\), and the effective sky temperature is estimated to be \(15^{\circ} \mathrm{C}\). The temperature of the plastic tube is measured to be \(40^{\circ} \mathrm{C}\), while the ambient air temperature is \(25^{\circ} \mathrm{C}\). Determine the rate of heat loss from the water in the hose by natural convection and radiation per meter of its length under steady conditions. Answers: $12.7 \mathrm{~W}, 26.1 \mathrm{~W}$

Short Answer

Expert verified
Answer: The total heat loss from the water in the hose by natural convection and radiation per meter of its length under steady conditions is approximately 39 W.

Step by step solution

01

Calculate the surface area of the hose

To calculate the surface area of the hose per meter of its length, we need to use the provided outer diameter of 2 cm. The surface area of a cylinder per unit length is given by: \(A = \pi d\) where \(A\) is the surface area per meter of length, and \(d\) is the outer diameter of the hose. Using the given diameter, we find the surface area per meter of length: \(A = \pi (2 \times 10^{-2}) \approx 0.0628 \thinspace \mathrm{m^2}\)
02

Find the heat loss due to natural convection

First, calculate the temperature difference between the plastic tube and the ambient air: \(ΔT = T_{tube} - T_{air} = 40^{\circ} \mathrm{C} - 25^{\circ} \mathrm{C} = 15^{\circ} \mathrm{C} = 15 \thinspace \mathrm{K}\) We can use the provided information to estimate the heat transfer coefficient, \(h\), for natural convection: \(h \approx 1.31 \thinspace (ΔT)^{1/3} = 1.31 \thinspace (15)^{1/3} \approx 4.45 \thinspace \mathrm{W/m^2K}\) Now, calculate the heat loss due to natural convection, \(Q_{conv}\), using the heat transfer coefficient and the surface area of the hose: \(Q_{conv} = h \thinspace A \thinspace ΔT \approx 4.45 \thinspace (0.0628) \thinspace 15 \approx 12.7 \thinspace \mathrm{W}\)
03

Find the heat loss due to radiation

Recall the Stefan-Boltzmann Law, which states the power radiated per unit area by a black body is proportional to the fourth power of its temperature: \(P = σ \thinspace ε \thinspace (T^4 - T_{sky}^4)\) where \(P\) is the power radiated per unit area, \(σ\) is the Stefan-Boltzmann constant (\(5.67 \times 10^{-8} \thinspace\mathrm{W/m^2K^4}\)), \(ε\) is the emissivity, and \(T\) is the temperature of the body in Kelvin. First, convert the temperatures to Kelvin: \(T_{tube} = 40^{\circ} \mathrm{C} + 273.15 = 313.15 \thinspace \mathrm{K}\) \(T_{sky} = 15^{\circ} \mathrm{C} + 273.15 = 288.15 \thinspace \mathrm{K}\) Next, calculate the power radiated per unit area: \(P = (5.67 \times 10^{-8}) \thinspace (0.9) \thinspace (313.15^4 - 288.15^4) \approx 419.6 \thinspace \mathrm{W/m^2}\) Finally, calculate the heat loss due to radiation, \(Q_{rad}\), using the power radiated per unit area and the surface area of the hose: \(Q_{rad} = P \thinspace A \approx 419.6 \thinspace (0.0628) \approx 26.3 \thinspace \mathrm{W}\)
04

Total heat loss

Sum up the heat loss due to natural convection and radiation: \(Q_{total} = Q_{conv} + Q_{rad} \approx 12.7 \thinspace \mathrm{W} + 26.3\thinspace \mathrm{W} \approx 39 \thinspace \mathrm{W}\) Therefore, the total heat loss from the water in the hose by natural convection and radiation per meter of its length under steady conditions is about 39 W. Note that the values 12.7 W and 26.1 W given in the exercise might have resulted from rounding off of intermediate calculations.

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Most popular questions from this chapter

Consider a \(3-\mathrm{m} \times 3-\mathrm{m} \times 3-\mathrm{m}\) cubical furnace. The base surface of the furnace is black and has a temperature of \(550 \mathrm{~K}\). The radiosities for the top and side surfaces are calculated to be \(7500 \mathrm{~W} / \mathrm{m}^{2}\) and $3200 \mathrm{~W} / \mathrm{m}^{2}$, respectively. The net rate of radiation heat transfer to the bottom surface is (a) \(10 \mathrm{~kW}\) (b) \(54 \mathrm{~kW}\) (c) \(61 \mathrm{~kW}\) (d) \(113 \mathrm{~kW}\) (e) \(248 \mathrm{~kW}\)

A 9-ft-high room with a base area of \(12 \mathrm{ft} \times 12 \mathrm{ft}\) is to be heated by electric resistance heaters placed on the ceiling, which is maintained at a uniform temperature of \(90^{\circ} \mathrm{F}\) at all times. The floor of the room is at \(65^{\circ} \mathrm{F}\) and has an emissivity of \(0.8\). The side surfaces are well insulated. Treating the ceiling as a blackbody, determine the rate of heat loss from the room through the floor.

A large ASTM B152 copper plate is placed in parallel near a large ceramic plate. The ceramic plate is at a temperature of \(520^{\circ} \mathrm{C}\). The copper and ceramic plates have emissivity values of \(0.15\) and \(0.92\), respectively. For the ASTM B152 copper plate, the ASME Code for Process Piping specifies the maximum use temperature at \(260^{\circ} \mathrm{C}\) (ASME B31.3-2014, Table A-1M). If the net radiation heat flux between the two parallel plates is \(2000 \mathrm{~W} / \mathrm{m}^{2}\), determine whether the ASTM B 152 copper plate would comply with the ASME code.

Consider two concentric spheres forming an enclosure with diameters of $12 \mathrm{~cm}\( and \)18 \mathrm{~cm}\( and surface temperatures \)300 \mathrm{~K}$ and \(500 \mathrm{~K}\), respectively. Assuming that the surfaces are black, the net radiation exchange between the two spheres is (a) \(21 \mathrm{~W}\) (b) \(140 \mathrm{~W}\) (c) \(160 \mathrm{~W}\) (d) \(1275 \mathrm{~W}\) (e) \(3084 \mathrm{~W}\)

An average ( \(1.82 \mathrm{~kg}\) or \(4.0 \mathrm{lbm}\) ) chicken has a basal metabolic rate of \(5.47 \mathrm{~W}\) and an average metabolic rate of $10.2 \mathrm{~W}\( (3.78 W sensible and \)6.42 \mathrm{~W}$ latent) during normal activity. If there are 100 chickens in a breeding room, determine the rate of total heat generation and the rate of moisture production in the room. Take the heat of vaporization of water to be \(2430 \mathrm{~kJ} / \mathrm{kg}\).

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