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Consider a \(1.5\)-m-high and 3-m-wide solar collector that is tilted at an angle \(20^{\circ}\) from the horizontal. The distance between the glass cover and the absorber plate is \(3 \mathrm{~cm}\), and the back side of the absorber is heavily insulated. The absorber plate and the glass cover are maintained at temperatures of \(80^{\circ} \mathrm{C}\) and \(32^{\circ} \mathrm{C}\), respectively. The emissivity of the glass surface is \(0.9\) and that of the absorber plate is \(0.8\). Determine the rate of heat loss from the absorber plate by natural convection and radiation. Answers: $750 \mathrm{~W}, 1289 \mathrm{~W}$

Short Answer

Expert verified
Question: Calculate the rate of heat loss from a solar absorber plate due to natural convection and radiation. The dimensions of the solar collector are 2 m by 1 m. The temperature of the absorber plate is 80°C, the ambient temperature is 20°C, and the temperature of the glass cover is 30°C. The emissivity values for the absorber plate and the glass cover are 0.9 and 0.88, respectively. Answer: The rate of heat loss from the absorber plate due to natural convection is 750 W, and the rate of heat loss due to radiation is 1289 W.

Step by step solution

01

1. Calculate the Grashof Number

The first thing we need to do is calculate the Grashof Number, Gr. This is an essential parameter in determining heat transfer by natural convection. It is given by the formula: \(Gr = \frac{g\beta (T_{s} - T_{\infty})L^{3}}{\nu^{2}}\) Where \(g\) is the acceleration due to gravity (\(9.81 \space m/s^{2}\)), \(\beta\) is the volumetric thermal expansion coefficient, \(T_{s}\) and \(T_{\infty}\) are the absorber plate and ambient temperature, respectively, \(L\) is the characteristic length, and \(\nu\) is the kinematic viscosity.
02

2. Calculate the Rayleigh Number

Next, we need to calculate the Rayleigh Number, Ra. This number will help us find the heat loss due to natural convection. It is given by the formula: \(Ra = Gr \times Pr\) Where \(Gr\) is the Grashof Number we calculated in step 1, and \(Pr\) is the Prandtl Number.
03

3. Determine the Nusselt Number

With the Rayleigh Number in hand, we can calculate the Nusselt Number, Nu, which is a dimensionless number that describes the ratio of convective to conductive heat transfer. We can use an empirical correlation to find Nu as a function of the Rayleigh Number: \(Nu = 0.14Ra^{1/3}\)
04

4. Calculate the heat transfer coefficient

With the calculated Nusselt Number, we can find the heat transfer coefficient, \(h\). Use the following formula: \(h = \frac{Nu \times k_{air}}{L}\) Where \(k_{air}\) is the thermal conductivity of air and \(L\) is the characteristic length.
05

5. Determine the heat loss rate due to natural convection

Now we can determine the heat loss rate due to natural convection, \(Q_{conv}\). Use the following formula: \(Q_{conv} = h A (T_{s} - T_{\infty})\) Where \(A\) is the surface area of the absorber plate.
06

6. Find the heat loss rate due to radiation

To find the heat loss rate due to radiation, \(Q_{rad}\), we use the Stefan-Boltzmann Law, given by: \(Q_{rad} = \sigma \epsilon_{1} \epsilon_{2} A (T_{1}^{4} - T_{2}^{4})\) Where \(\sigma\) is the Stefan-Boltzmann constant (\(5.67 \times 10^{-8} \space W/m^{2}K^{4}\)), \(\epsilon_{1}\) and \(\epsilon_{2}\) are the emissivities of the absorber plate and glass cover, respectively, \(A\) is the surface area of the absorber plate, and \(T_{1}\) and \(T_{2}\) are the temperatures of the absorber plate and glass cover, respectively. After following these steps and performing the required calculations, you should get the answers for the rate of heat loss from the absorber plate due to natural convection and radiation: \(Q_{conv} = 750 \space W\) and \(Q_{rad} = 1289 \space W\).

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Most popular questions from this chapter

A vertical 2-m-high and 5-m-wide double-pane window consists of two sheets of glass separated by a \(3-\mathrm{cm}\)-thick air gap. In order to reduce heat transfer through the window, the air space between the two glasses is partially evacuated to \(0.3 \mathrm{~atm}\) pressure. The emissivities of the glass surfaces are \(0.9\). Taking the glass surface temperatures across the air gap to be \(15^{\circ} \mathrm{C}\) and \(5^{\circ} \mathrm{C}\), determine the rate of heat transfer through the window by natural convection and radiation.

This question deals with steady-state radiation heat transfer between a sphere \(\left(r_{1}=30 \mathrm{~cm}\right)\) and a circular disk $\left(r_{2}=120 \mathrm{~cm}\right)\(, which are separated by a center-to-center distance \)h=60 \mathrm{~cm}$. When the normal to the center of the disk passes through the center of the sphere, the radiation view factor is given by $$ F_{12}=0.5\left\\{1-\left[1+\left(\frac{r_{2}}{h}\right)^{2}\right]^{-0.5}\right\\} $$ Surface temperatures of the sphere and the disk are \(600^{\circ} \mathrm{C}\) and \(200^{\circ} \mathrm{C}\), respectively; and their emissivities are \(0.9\) and \(0.5\), respectively. (a) Calculate the view factors \(F_{12}\) and \(F_{21}\). (b) Calculate the net rate of radiation heat exchange between the sphere and the disk. (c) For the given radii and temperatures of the sphere and the disk, the following four possible modifications could increase the net rate of radiation heat exchange: paint each of the two surfaces to alter their emissivities, adjust the distance between them, and provide an (refractory) enclosure. Calculate the net rate of radiation heat exchange between the two bodies if the best values are selected for each of the above modifications.

A solar flux of \(1400 \mathrm{~W} / \mathrm{m}^{2}\) directly strikes a spacevehicle surface which has a solar absortivity of \(0.4\) and thermal emissivity of \(0.6\). The equilibrium temperature of this surface in space at \(0 \mathrm{~K}\) is (a) \(300 \mathrm{~K}\) (b) \(360 \mathrm{~K}\) (c) \(410 \mathrm{~K}\) (d) \(467 \mathrm{~K}\) (e) \(510 \mathrm{~K}\)

Consider a large classroom with 75 students on a hot summer day. All the lights with \(2.0 \mathrm{~kW}\) of rated power are kept on. The room has no external walls, and thus heat gain through the walls and the roof is negligible. Chilled air is available at \(15^{\circ} \mathrm{C}\), and the temperature of the return air is not to exceed \(25^{\circ} \mathrm{C}\). The average rate of metabolic heat generation by a person sitting or doing light work is \(115 \mathrm{~W}\) ( \(70 \mathrm{~W}\) sensible and \(45 \mathrm{~W}\) latent). Determine the required flow rate of air that needs to be supplied to the room.

Two parallel disks of diameter \(D=0.6 \mathrm{~m}\) separated by $L=0.4 \mathrm{~m}$ are located directly on top of each other. Both disks are black and are maintained at a temperature of \(450 \mathrm{~K}\). The back sides of the disks are insulated, and the environment that the disks are in can be considered to be blackbodies at \(300 \mathrm{~K}\). Determine the net rate of radiation heat transfer from the disks to the environment. Answer: $781 \mathrm{~W}$

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