/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 91 A rectangular cavity consists of... [FREE SOLUTION] | 91Ó°ÊÓ

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A rectangular cavity consists of two parallel, \(0.5-\mathrm{m}-\) square plates separated by a distance of \(50 \mathrm{~mm}\), with the lateral boundaries insulated. The heated plate is maintained at \(325 \mathrm{~K}\) and the cooled plate at \(275 \mathrm{~K}\). Estimate the heat flux between the surfaces for three orientations of the cavity using the notation of Figure 9.6: vertical with \(\tau=90^{\circ}\), horizontal with \(\tau=0^{\circ}\), and horizontal with \(\tau=180^{\circ}\).

Short Answer

Expert verified
In conclusion, the heat flux between the surfaces for the different cavity orientations are: - Vertical orientation: \(q = 61.07\, \textnormal{W}\) - Horizontal orientation with heated plate on top: \(q_{top} = 28.10\, \textnormal{W}\), \(q_{bottom} = 60.60\, \textnormal{W}\) - Horizontal orientation with heated plate on the bottom: \(q_{top} = 60.60\, \textnormal{W}\), \(q_{bottom} = 28.10\, \textnormal{W}\)

Step by step solution

01

Define the parameters and constants

First, list all the given values and dimensions of our rectangular cavity: - Heated plate temperature: \(T_H = 325\,\textnormal{K}\) - Cooled plate temperature: \(T_C = 275\,\textnormal{K}\) - Plate dimensions: \(0.5\, \textnormal{m} \times 0.5\,\textnormal{m}\) - Distance between the plates: \(L = 50\,\textnormal{mm} = 0.05\, \textnormal{m}\) - Gravitational acceleration: \(g = 9.81\, \textnormal{m/s}^2\) We also need to determine the fluid properties since we're dealing with natural convection. Assuming the fluid is air, we'll take average properties at the film temperature, which is the arithmetic mean of the heated and cooled plate temperatures: $$T_f = \frac{T_H + T_C}{2} = \frac{325+275}{2}\, \textnormal{K} = 300\, \textnormal{K}$$ At \(T_f = 300\,\textnormal{K}\), we have the following air properties: - Density, \(\rho = 1.177\,\textnormal{kg/m}^3\) - Specific heat, \(c_p = 1005\,\textnormal{J/(kg K)}\) - Thermal conductivity, \(k = 0.0262\,\textnormal{W/(m K)}\) - Dynamic viscosity, \(\mu = 1.846 \times 10^{-5}\,\textnormal{kg/(m s)}\) - Kinematic viscosity, \(\nu = \frac{\mu}{\rho} = 1.568 \times 10^{-5}\,\textnormal{m}^2/\textnormal{s}\) - Coefficient of Thermal Expansion, \(\beta = \frac{1}{T_f} = 3.333 \times 10^{-3}\,\textnormal{K}^{-1}\) (ideal gas approximation) Now that we have all the necessary parameters, we can proceed to estimate the heat flux for the three orientations.
02

Calculate the Rayleigh Number

For each orientation, we will first calculate the Rayleigh number, which is defined as: $$Ra_L = \frac{g \beta (T_H - T_C)L^3}{\nu \alpha}$$ where \(\alpha\) is the thermal diffusivity, which can be calculated as \(\alpha = \frac{k}{\rho c_p}\). In our case, \(\alpha = \frac{0.0262}{1.177 \times 1005} = 2.236 \times 10^{-5}\, \textnormal{m}^2/\textnormal{s}\). Now we can calculate the Rayleigh number: $$Ra_L = \frac{9.81 \times 3.333 \times 10^{-3} \times (325 - 275) \times 0.05^3}{1.568 \times 10^{-5} \times 2.236 \times 10^{-5}} = 1.697 \times10^7$$
03

Determine the Nusselt Number

Next, we need to determine the Nusselt number, \(Nu_L\), based on the different orientations. Use the following correlations: 1. For the vertical orientation (\(\tau=90^{\circ}\)): $$Nu_L = 0.589 Ra_L^{1/4}\,\, (\textnormal{for} \,\, 10^4 \leq Ra_L \leq 10^9)$$ 2. For the horizontal orientation with heated plate on top (\(\tau=0^{\circ}\)): Top Plate: $$Nu_L = 0.069 Ra_L^{1/3}\,\, (\textnormal{for} \,\, 10^4 \leq Ra_L \leq 10^{10})$$ Bottom Plate: $$Nu_L = 0.15 Ra_L^{1/3}\,\, (\textnormal{for} \,\, 10^4 \leq Ra_L \leq 10^{10})$$ 3. For the horizontal orientation with heated plate on the bottom (\(\tau=180^{\circ}\)): Top Plate: $$Nu_L = 0.15 Ra_L^{1/3}\,\, (\textnormal{for} \,\, 10^4 \leq Ra_L \leq 10^{10})$$ Bottom Plate: $$Nu_L = 0.069 Ra_L^{1/3}\,\, (\textnormal{for} \,\, 10^4 \leq Ra_L \leq 10^{10})$$ Calculate the Nusselt numbers for each orientation: 1. Vertical orientation: $$Nu_L = 0.589 \times (1.697 \times10^7)^{1/4} = 37.25$$ 2. Horizontal orientation with heated plate on top: Top Plate: $$Nu_L = 0.069 \times (1.697 \times10^7)^{1/3} = 17.16$$ Bottom Plate: $$Nu_L = 0.15 \times (1.697 \times10^7)^{1/3} = 37.05$$ 3. Horizontal orientation with heated plate on the bottom: Top Plate: $$Nu_L = 0.15 \times (1.697 \times10^7)^{1/3} = 37.05$$ Bottom Plate: $$Nu_L = 0.069 \times (1.697 \times10^7)^{1/3} = 17.16$$
04

Calculate Heat Transfer Coefficient and Heat Flux

Finally, use the Nusselt number to calculate the heat transfer coefficient, \(h\), and then the heat flux, \(q\): $$h = \frac{Nu_L \times k}{L}$$ $$q = h \times A \times (T_H - T_C)$$ where \(A\) is the surface area of the plates. For all three orientations, we have \(A = 0.5 \times 0.5 = 0.25\,\textnormal{m}^2.\) 1. Vertical orientation: $$h = \frac{37.25 \times 0.0262}{0.05} = 19.48\, \textnormal{W/(m}^2\textnormal{K)}$$ $$q = 19.48 \times 0.25 \times (325 - 275) = 61.07\, \textnormal{W}$$ 2. Horizontal orientation with heated plate on top: Top Plate: $$h = \frac{17.16 \times 0.0262}{0.05} = 8.976\, \textnormal{W/(m}^2\textnormal{K)}$$ $$q = 8.976 \times 0.25 \times (325 - 275) = 28.10\, \textnormal{W}$$ Bottom Plate: $$h = \frac{37.05 \times 0.0262}{0.05} = 19.36\, \textnormal{W/(m}^2\textnormal{K)}$$ $$q = 19.36 \times 0.25 \times (325 - 275) = 60.60\, \textnormal{W}$$ 3. Horizontal orientation with heated plate on the bottom: Top Plate: $$h = \frac{37.05 \times 0.0262}{0.05} = 19.36\, \textnormal{W/(m}^2\textnormal{K)}$$ $$q = 19.36 \times 0.25 \times (325 - 275) = 60.60\, \textnormal{W}$$ Bottom Plate: $$h = \frac{17.16 \times 0.0262}{0.05} = 8.976\, \textnormal{W/(m}^2\textnormal{K)}$$ $$q = 8.976 \times 0.25 \times (325 - 275) = 28.10\, \textnormal{W}$$ In conclusion, the heat flux between the surfaces for the different cavity orientations are: - Vertical orientation: \(q = 61.07\, \textnormal{W}\) - Horizontal orientation with heated plate on top: \(q_{top} = 28.10\, \textnormal{W}\), \(q_{bottom} = 60.60\, \textnormal{W}\) - Horizontal orientation with heated plate on the bottom: \(q_{top} = 60.60\, \textnormal{W}\), \(q_{bottom} = 28.10\, \textnormal{W}\)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Heat Transfer
Heat transfer involves the movement of thermal energy from a hotter region to a cooler one. In the context of natural convection in a rectangular cavity, it's interesting because it does not rely on fans or pumps to facilitate the movement of heat. Instead, heat transfer in this setup occurs naturally due to the temperature difference between the heated and cooled plates.

  • Conduction: This is the transfer of heat through a solid material, from the hot plate to the cool plate, typically occurring at the contact surfaces.
  • Convection: In our scenario, air serves as the medium for heat transfer. When the air near the heated plate warms up, it becomes lighter and rises, displacing cooler air that moves down to be warmed. This cycle forms what we call convection currents.
Understanding heat transfer in such a setup allows us to predict how efficiently a space can be heated or cooled.
Rayleigh Number
The Rayleigh Number, denoted as \( Ra_L \), plays a crucial role in natural convection heat transfer. It is a dimensionless number that provides insight into the flow regime of the convection.

In the exercise, it is calculated using the formula:\[Ra_L = \frac{g \beta (T_H - T_C)L^3}{u \alpha}\]where:
  • \(g\) is the gravitational acceleration.
  • \(\beta\) is the coefficient of thermal expansion.
  • \(T_H\) and \(T_C\) are the temperatures of the heated and cooled plates.
  • \(L\) is the characteristic length between plates.
  • \(u\) is the kinematic viscosity.
  • \(\alpha\) is the thermal diffusivity.
The value of the Rayleigh number helps in determining whether the flow is laminar or turbulent. For higher Rayleigh numbers, the flow tends to be more turbulent, enhancing heat transfer.
Nusselt Number
The Nusselt Number, \( Nu_L \), is another dimensionless number used in assessing heat transfer efficiency, indicating how much heat is transferred due to convection relative to conduction.

In the given cavity orientations, it is calculated differently depending on the configuration:
  • For vertical heated plates, \( Nu_L = 0.589 Ra_L^{1/4} \)
  • For horizontal plates, it varies whether the heated plate is on top or bottom, as the physical behavior of air changes. The formulas slightly differ, indicating a larger interface heat exchange when buoyant forces either aid or oppose the convection currents.
A higher Nusselt number suggests improved convective heat transfer, signifying a more effective heat removal by the fluid from the hot to the cool surfaces.
Thermal Diffusivity
Thermal diffusivity, \( \alpha \), is an important property of materials that influences how quickly heat spreads through a substance. It is defined as the ratio of thermal conductivity to the product of density and specific heat capacity:\[\alpha = \frac{k}{\rho c_p}\]where:
  • \(k\) is thermal conductivity.
  • \(\rho\) is the density of the fluid.
  • \(c_p\) is the specific heat capacity.
In the context of the problem, knowing the thermal diffusivity of air helps in calculating the Rayleigh number, which is essential for understanding the natural convection process. High thermal diffusivity means the material is quick to respond to changes in temperature, impacting how efficiently heat can be transferred in the cavity setup.

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Most popular questions from this chapter

Free convection occurs between concentric spheres. The inner sphere is of diameter \(D_{i}=50 \mathrm{~mm}\) and temperature \(T_{i}=50^{\circ} \mathrm{C}\), while the outer sphere is maintained at \(T_{o}=20^{\circ} \mathrm{C}\). Air is in the gap between the spheres. What outer sphere diameter is required so that the convection heat transfer from the inner sphere is the same as if it were placed in a large, quiescent environment with air at \(T_{\infty}=20^{\circ} \mathrm{C}\) ?

A refrigerator door has a height and width of \(H=1 \mathrm{~m}\) and \(W=0.65 \mathrm{~m}\), respectively, and is situated in a large room for which the air and walls are at \(T_{\infty}=T_{\text {sur }}=25^{\circ} \mathrm{C}\). The door consists of a layer of polystyrene insulation \((k=0.03 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) sandwiched between thin sheets of steel \((\varepsilon=0.6)\) and polypropylene. Under normal operating conditions, the inner surface of the door is maintained at a fixed temperature of \(T_{s, i}=5^{\circ} \mathrm{C}\). (a) Estimate the heat gain through the door for the worst case condition corresponding to no insulation \((L=0)\). (b) Compute and plot the heat gain and the outer surface temperature \(T_{s, o}\) as a function of insulation thickness for \(0 \leq L \leq 25 \mathrm{~mm}\).

Square panels \((250 \mathrm{~mm} \times 250 \mathrm{~mm}\) ) with a decorative, highly reflective plastic finish are cured in an oven at \(125^{\circ} \mathrm{C}\) and cooled in quiescent air at \(29^{\circ} \mathrm{C}\). Quality considerations dictate that the panels remain horizontal and that the cooling rate be controlled. To increase productivity in the plant, it is proposed to replace the batch cooling method with a conveyor system having a velocity of \(0.5 \mathrm{~m} / \mathrm{s}\).

According to experimental results for parallel airflow over a uniform temperature, heated vertical plate, the effect of free convection on the heat transfer convection coefficient will be \(5 \%\) when \(G r_{L} / R e_{L}^{2}=0.08\). Consider a heated vertical plate \(0.3 \mathrm{~m}\) long, maintained at a surface temperature of \(60^{\circ} \mathrm{C}\) in atmospheric air at \(25^{\circ} \mathrm{C}\). What is the minimum vertical velocity required of the airflow such that free convection effects will be less than \(5 \%\) of the heat transfer rate?

\(\mathbf{9 . 1 0 3}\) It has been proposed to use large banks of rechargeable, lithium ion batteries to power electric vehicles. The cylindrical batteries, each of which is of radius \(r_{i}=9 \mathrm{~mm}\) and length \(L=65 \mathrm{~mm}\), undergo exothermic electrochemical reactions while being discharged. Since excessively high temperatures damage the batteries, it is proposed to encase them in a phase change material that melts when the batteries discharge (and resolidifies when the batteries are charged; charging is associated with an endothermic electrochemical reaction). Consider the paraffin of Problems \(8.47\) and \(9.57\). (a) At an instant in time during the discharge of a battery, liquid paraffin occupies an annular region of outer radius \(r_{o}=19 \mathrm{~mm}\) around the battery, which is generating \(\dot{E}_{g}=1 \mathrm{~W}\) of thermal energy. Determine the surface temperature of the battery. (b) At the time of interest in part (a), what is the rate at which the liquid annulus radius is increasing? (c) Plot the battery surface temperature versus the outer radius of the liquid-filled annulus. Explain the relative insensitivity of the battery surface temperature to the size of the annulus for \(15 \mathrm{~mm} \leq\) \(r_{o} \leq 30 \mathrm{~mm}\).

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