Liquid mercury at \(250^{\circ} \mathrm{C}\) is flowing in parallel over a flat plate at a velocity of \(0.3 \mathrm{~m} / \mathrm{s}\). Surface temperature of the \(0.1-\mathrm{m}\)-long flat plate is constant at \(50^{\circ} \mathrm{C}\). Determine \((a)\) the local convection heat transfer coefficient at \(5 \mathrm{~cm}\) from the leading edge and \((b)\) the average convection heat transfer coefficient over the entire plate.

Short Answer

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Question: Determine the local convection heat transfer coefficient at a specific position 5 cm from the leading edge and the average convection heat transfer coefficient over the entire plate. Answer: (a) The local convection heat transfer coefficient at 5 cm from the leading edge is approximately 241048 W/(m^2 ⋅ K). (b) The average convection heat transfer coefficient over the entire plate is approximately 1712950 W/(m^2 ⋅ K).

Step by step solution

01

Obtain given information

We are given the following information: Temperature of liquid mercury, \(T_L = 250^\circ C\) Velocity of liquid mercury, \(u = 0.3 m/s\) Surface temperature of the flat plate, \(T_P = 50^\circ C\) Length of the flat plate, \(L = 0.1 m\) Position we would like to compute local (convection) heat transfer coefficient, \(x = 0.05 m\)
02

Calculate Reynolds number

To make use of the Nusselt number and heat transfer coefficient formulas, first, we need to calculate the Reynolds number at the position \(x = 5 cm\). Reynolds number, \(Re_x = \frac{u x}{\nu}\) where, \(\nu\) is the kinematic viscosity of liquid mercury. Based on the provided information, you can look up the kinematic viscosity of liquid mercury at \(250^\circ C\) in a reference table. For instance, \(\nu \approx 1.125 \times 10^{-7} m^2/s\). Now we can calculate the Reynolds number at \(x = 0.05 m\): \(Re_x = \frac{0.3 \times 0.05}{1.125 \times 10^{-7}} \approx 133333\)
03

Calculate Prandtl number

Next, we need to calculate the Prandtl number, which characterizes the relative thickness of the momentum and thermal boundary layers. Prandtl number, \(Pr = \frac{\nu}{\alpha}\) where, \(\alpha\) is the thermal diffusivity of liquid mercury. You can look up the thermal diffusivity of liquid mercury at \(250^\circ C\) in a reference table. For instance, \(\alpha \approx 1.0 \times 10^{-7} m^2/s\). Now we can calculate the Prandtl number: \(Pr = \frac{1.125 \times 10^{-7}}{1.0 \times 10^{-7}} \approx 1.125\)
04

Calculate local Nusselt number and Local convection heat transfer coefficient

Now that we have the Reynolds and Prandtl numbers, we can determine the local Nusselt number using the following formula: Local Nusselt number, \(Nu_x = C \cdot Re_x^m \cdot Pr^n\) Here, \(C\), \(m\), and \(n\) are empirical constants, typical values are \(C = 0.332\), \(m = 0.5\), and \(n = 1/3\) for laminar flow over a flat plate. Therefore, \(Nu_x = 0.332 \cdot (133333)^{0.5} \cdot (1.125)^{1/3} \approx 4598\) Now, we can determine the local convection heat transfer coefficient at \(x = 0.05 m\) by using the following formula: Local convection heat transfer coefficient, \(h_x = \frac{k \cdot Nu_x}{x}\) where, \(k\) is the thermal conductivity of liquid mercury. You can look up the thermal conductivity of liquid mercury at \(250^\circ C\) in a reference table. For instance, \(k \approx 26.3 W/(m \cdot K)\). Now we can calculate the local convection heat transfer coefficient: \(h_x = \frac{26.3 \times 4598}{0.05} \approx 241048 W/(m^2 \cdot K)\) The local convection heat transfer coefficient at \(5 cm\) from the leading edge is approximately \(241048 W/(m^2 \cdot K)\)
05

Calculate the average convection heat transfer coefficient

Next, we will determine the average convection heat transfer coefficient over the entire plate. First, we need to calculate the average Nusselt number with the following formula: Average Nusselt number, \( \overline{Nu}_L = C \cdot Re_L^m \cdot Pr^n\) Here, \(Re_L\) is the Reynolds number at the end of the plate, \(L = 0.1 m\): \(Re_L = \frac{0.3 \times 0.1}{1.125 \times 10^{-7}} \approx 266667\) Now, we can calculate the average Nusselt number: \( \overline{Nu}_L = 0.332 \cdot (266667)^{0.5} \cdot (1.125)^{1/3} \approx 6515\) Finally, we can determine the average convection heat transfer coefficient over the entire plate using the following formula: Average convection heat transfer coefficient, \(\overline{h}_L = \frac{k \cdot \overline{Nu}_L}{L}\) Now we can calculate the average convection heat transfer coefficient: \(\overline{h}_L = \frac{26.3 \times 6515}{0.1} \approx 1712950 W/(m^2 \cdot K)\) The average convection heat transfer coefficient over the entire plate is approximately \(1712950 W/(m^2 \cdot K)\). Answer: (a) The local convection heat transfer coefficient at \(5 cm\) from the leading edge is approximately \(241048 W/(m^2 \cdot K)\). (b) The average convection heat transfer coefficient over the entire plate is approximately \(1712950 W/(m^2 \cdot K)\).

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In flow across tube banks, how does the heat transfer coefficient vary with the row number in the flow direction? How does it vary with in the transverse direction for a given row number?

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Warm air is blown over the inner surface of an automobile windshield to defrost ice accumulated on the outer surface of the windshield. Consider an automobile windshield \(\left(k_{w}=\right.\) \(0.8 \mathrm{Btu} / \mathrm{h} \cdot \mathrm{ft} \cdot \mathrm{R})\) with an overall height of 20 in and thickness of \(0.2\) in. The outside air ( \(1 \mathrm{~atm})\) ambient temperature is \(8^{\circ} \mathrm{F}\) and the average airflow velocity over the outer windshield surface is \(50 \mathrm{mph}\), while the ambient temperature inside the automobile is \(77^{\circ} \mathrm{F}\). Determine the value of the convection heat transfer coefficient for the warm air blowing over the inner surface of the windshield, necessary to cause the accumulated ice to begin melting. Assume the windshield surface can be treated as a flat plate surface.

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