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Water enters a 5-mm-diameter and 13 -m-long tube at \(15^{\circ} \mathrm{C}\) with a velocity of \(0.3 \mathrm{~m} / \mathrm{s}\) and leaves at $45^{\circ} \mathrm{C}\(. The tube is subjected to a uniform heat flux of \)2000 \mathrm{~W} / \mathrm{m}^{2}$ on its surface. The temperature of the tube surface at the exit is (a) \(48.7^{\circ} \mathrm{C}\) (b) \(49.4^{\circ} \mathrm{C}\) (c) \(51.1^{\circ} \mathrm{C}\) (d) \(53.7^{\circ} \mathrm{C}\) (e) \(55.2^{\circ} \mathrm{C}\) (For water, use $k=0.615 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \operatorname{Pr}=5.42, \nu=0.801 \times\( \)10^{-6} \mathrm{~m}^{2} / \mathrm{s}$.)

Short Answer

Expert verified
Answer: (c) 51.1 °C

Step by step solution

01

Determine the Reynolds number

To determine the heat transfer coefficient, we first need to find the Reynolds number (Re). The Reynolds number is calculated using the equation: \(Re = \frac{VD}{\nu}\) Where: \(V = 0.3\ m/s\) (velocity), \(D = 0.005\ m\) (diameter, converted from 5 mm), \(\nu = 0.801 \times 10^{-6}\ m^2/s\) (kinematic viscosity)
02

Calculate the Reynolds number

Now, plug the given values into the formula: \(Re = \frac{0.3 \times 0.005}{0.801 \times 10^{-6}}\) \(Re \approx 1869\)
03

Determine the Nusselt number

For laminar flow, as the Reynolds number is less than \(2300\), we can use the Sieder-Tate correlation to calculate the Nusselt number (Nu). The Sieder-Tate correlation is given as follows: \(Nu = 1.86 \times Re^{1/3} \times Pr^{1/3} \times \frac{L}{D}\) Where: \(L = 13\ m\) (length of the tube) and \(Pr = 5.42\) (Prandtl number)
04

Calculate the Nusselt number

Now, plug the given values into the formula: \(Nu \approx 1.86 \times 1869^{1/3} \times 5.42^{1/3} \times \frac{13}{0.005}\) \(Nu \approx 3127\)
05

Determine the heat transfer coefficient (h)

We can now use the Nusselt number to calculate the heat transfer coefficient as follows: \(h = \frac{Nu \times k}{D}\) Where: \(k = 0.615\ W/m\cdot K\) (thermal conductivity)
06

Calculate the heat transfer coefficient

Plug the given values into the formula: \(h \approx \frac{3127 \times 0.615}{0.005}\) \(h \approx 385\xa0W/m^2 \cdot K\)
07

Calculate the surface temperature at the exit

Now, using the heat flux (\(q''\)) given, let's find the temperature difference (\(\Delta T\)) between the water and tube surface at the exit: \(\Delta T = \frac{q''}{h}\) Where: \(q'' = 2000\ W/m^2\) (heat flux) Plug the given values into the formula: \(\Delta T \approx \frac{2000}{385}\) \(\Delta T \approx 5.2 \ ^\circ C\) Finally, add the temperature difference to the water temperature at the exit (\(45\ ^\circ C\)) to find the tube surface temperature: \(T_{surface} = T_{water} + \Delta T\) \(T_{surface} = 45 + 5.2\) \(T_{surface} \approx 50.2\ ^\circ C\) Based on the given options, the closest answer is (c) \(51.1\ ^\circ C\).

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Most popular questions from this chapter

Air flows in an isothermal tube under fully developed conditions. The inlet temperature is \(60^{\circ} \mathrm{F}\) and the tube surface temperature is \(120^{\circ} \mathrm{F}\). The tube is \(10 \mathrm{ft}\) long, and the inner diameter is 2 in. The air mass flow rate is \(18.2 \mathrm{lbm} / \mathrm{h}\). Calculate the exit temperature of the air and the total rate of heat transfer from the tube wall to the air. Evaluate the air properties at a temperature \(80^{\circ} \mathrm{F}\). Is this a good assumption?

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What does the logarithmic mean temperature difference represent for flow in a tube whose surface temperature is constant? Why do we use the logarithmic mean temperature instead of the arithmetic mean temperature?

Someone claims that in fully developed turbulent flow in a tube, the shear stress is a maximum at the tube surface. Do you agree with this claim? Explain.

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