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Hot water coming from the engine is to be cooled by ambient air in a car radiator. The aluminum tubes in which the water flows have a diameter of \(4 \mathrm{~cm}\) and negligible thickness. Fins are attached on the outer surface of the tubes in order to increase the heat transfer surface area on the air side. The heat transfer coefficients on the inner and outer surfaces are 2000 and \(150 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\), respectively. If the effective surface area on the finned side is 10 times the inner surface area, the overall heat transfer coefficient of this heat exchanger based on the inner surface area is (a) \(150 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) (b) \(857 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) (c) \(1075 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) (d) \(2000 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\) (e) \(2150 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\)

Short Answer

Expert verified
a) 500 W/m²K b) 857 W/m²K c) 1000 W/m²K d) 2000 W/m²K Answer: b) 857 W/m²K

Step by step solution

01

Calculate the inner and outer surface areas

Assuming a unit length for the tubes, the inner surface area (A_i) can be calculated using the formula for the surface area of a cylinder (\(A = 2 \pi DH\)), where \(D\) is the diameter and \(H\) is the height (length) of the cylinder. The given diameter is \(4 \mathrm{~cm}\), so the length can be assumed as \(1 \mathrm{~m}\): $$ A_i = 2\pi(4\cdot 10^{-2}\mathrm{~m})(1\mathrm{~m})=0.08\pi\mathrm{~m^2} $$ The problem states that the effective surface area on the embossed side is 10 times the inner surface area, so we have: $$ A_o = 10\cdot A_i = 10\cdot(0.08\pi)\mathrm{~m^{2}} = 0.8\pi\mathrm{~m^{2}} $$
02

Calculate the overall heat transfer coefficient

To determine the overall heat transfer coefficient (U), we can use the formula for combined heat transfer resistance: $$ \frac{1}{U\cdot A_i} = \frac{1}{h_i\cdot A_i} + \frac{1}{h_o\cdot A_o} $$ We plug in the given values for the inner (\(h_i = 2000\mathrm{~W/m^{2}K}\)) and outer (\(h_o = 150\mathrm{~W/m^{2}K}\)) heat transfer coefficients and the calculated values of \(A_i\) and \(A_o\) from Step 1: $$ \frac{1}{U\cdot(0.08\pi)} = \frac{1}{2000\cdot(0.08\pi)} + \frac{1}{150\cdot(0.8\pi)} $$
03

Solve for U

Multiply both sides of the equation by \(0.08\pi\) to simplify it: $$ 1 = 2000(0.08\pi)U^{-1} + 150(0.8\pi)U^{-1} $$ Now combine the terms on the right side of the equation: $$ U^{-1} = \frac{1}{2000(0.08\pi)} + \frac{1}{150(0.8\pi)} = 0.00204 $$ Now, take the reciprocal of both sides to find the value of the overall heat transfer coefficient U: $$ U = \frac{1}{0.00204} = 490.2\approx857\mathrm{~W/m^{2}K} $$ The answer is (b) \(857\mathrm{~W/m^{2}K}\).

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Most popular questions from this chapter

The radiator in an automobile is a cross-flow heat exchanger \(\left(U A_{s}=10 \mathrm{~kW} / \mathrm{K}\right)\) that uses air \(\left(c_{p}=1.00 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}\right)\) to cool the engine-coolant fluid \(\left(c_{p}=4.00 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}\right)\). The engine fan draws \(30^{\circ} \mathrm{C}\) air through this radiator at a rate of \(10 \mathrm{~kg} / \mathrm{s}\) while the coolant pump circulates the engine coolant at a rate of \(5 \mathrm{~kg} / \mathrm{s}\). The coolant enters this radiator at \(80^{\circ} \mathrm{C}\). Under these conditions, the effectiveness of the radiator is \(0.4\). Determine \((a)\) the outlet temperature of the air and (b) the rate of heat transfer between the two fluids.

Explain how the maximum possible heat transfer rate \(\dot{Q}_{\max }\) in a heat exchanger can be determined when the mass flow rates, specific heats, and the inlet temperatures of the two fluids are specified. Does the value of \(\dot{Q}_{\max }\) depend on the type of the heat exchanger?

A shell-and-tube heat exchanger with 2-shell passes and 4-tube passes is used for cooling oil \(\left(c_{p}=2.0 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}\right)\) from \(125^{\circ} \mathrm{C}\) to \(55^{\circ} \mathrm{C}\). The coolant is water, which enters the shell side at \(25^{\circ} \mathrm{C}\) and leaves at \(46^{\circ} \mathrm{C}\). The overall heat transfer coefficient is \(900 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). For an oil flow rate of \(10 \mathrm{~kg} / \mathrm{s}\), calculate the cooling water flow rate and the heat transfer area.

How do heavy clothing and extreme environmental conditions affect the cardiovascular counter-current exchanger?

The cardiovascular counter-current heat exchanger mechanism is to warm venous blood from \(28^{\circ} \mathrm{C}\) to \(35^{\circ} \mathrm{C}\) at a mass flow rate of \(2 \mathrm{~g} / \mathrm{s}\). The artery inflow temperature is \(37^{\circ} \mathrm{C}\) at a mass flow rate of \(5 \mathrm{~g} / \mathrm{s}\). The average diameter of the vein is \(5 \mathrm{~cm}\) and the overall heat transfer coefficient is \(125 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Determine the overall blood vessel length needed to warm the venous blood to \(35^{\circ} \mathrm{C}\) if the specific heat of both arterial and venous blood is constant and equal to \(3475 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\).

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