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A semi-infinite aluminum cylinder $(k=237 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\(, \)\alpha=9.71 \times 10^{-5} \mathrm{~m}^{2} / \mathrm{s}$ ) of diameter \(D=15 \mathrm{~cm}\) is initially at a uniform temperature of \(T_{i}=115^{\circ} \mathrm{C}\). The cylinder is now placed in water at \(10^{\circ} \mathrm{C}\), where heat transfer takes place by convection with a heat transfer coefficient of $h=140 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\(. Determine the temperature at the center of the cylinder \)5 \mathrm{~cm}$ from the end surface 8 min after the start of cooling. Solve this problem using the analytical one-term approximation method.

Short Answer

Expert verified
The temperature at the center of the cylinder 5 cm from the end surface 8 minutes after the start of cooling is 59.2°C.

Step by step solution

01

List down known values

First, let's write down the values we know: 1. Cylinder properties: \(k = 237 \frac{W}{m \cdot K}\) , \(\alpha = 9.71 \times 10^{-5} \frac{m^2}{s} \) 2. Cylinder diameter: \(D = 15 cm = 0.15 m\) 3. Initial temperature: \(T_i = 115^{\circ}/℃\) 4. Water temperature: \(T_\infty = 10^{\circ}/℃\) 5. Heat transfer coefficient: \(h = 140 \frac{W}{m^2 \cdot K}\) 6. Time: \(t = 8\) min \(= 480\) s 7. Position from the end surface: \(x = 5\) cm = 0.05 m
02

Calculate the Biot number, Fourier number, and variables for the one-term approximation

To use the one-term approximation method, we first need to find the Biot number (\(Bi\)), Fourier number (\(Fo\)), and other variables that will be used for calculations. 1. Biot number: \(Bi = \frac{hL_c}{k}\), where \(L_c\) is the characteristic length and it is equal to \(\frac{D}{4}\) for a cylinder. 2. Fourier number: \(Fo = \frac{\alpha \cdot t}{L_c^2}\) Calculate \(L_c\), \(Bi\), and \(Fo\): \(L_c = \frac{0.15}{4} = 0.0375m\) \(Bi = \frac{140 \times 0.0375}{237} = 0.0221\) \(Fo = \frac{9.71 \times 10^{-5} \times 480}{0.0375^2} = 4.20\)
03

Determine λ₀ and η₀

Recall that the one-term approximation equation requires us to find the λ₀ and η₀ values, which are defined as follows: \(λ₀^2 + η₀^2 Bi^2 = 1\) \(η₀ λ₀ Bi = 1\) Solve the simultaneous equations to find \(λ₀\) and \(η₀\) values: \(λ₀ = 1.20\) \(η₀ = 0.823\)
04

Calculate the temperature at the desired location and time

Now, we can use the one-term approximation formula to find the temperature at the desired location and time: \(T(x, t) - T_\infty = \left( T_i - T_\infty \right) \cdot \frac{4e^{-λ₀^2 \cdot Fo}cos(η₀ \frac{x}{L_c})}{πλ₀\tanh(η₀)}\) Plug in the values we found previously: \(T(0.05, 480) - 10 = \left( 115 - 10 \right) \cdot \frac{4e^{-1.20^2 \cdot 4.20}cos(0.823 \cdot \frac{0.05}{0.0375})}{π \cdot 1.20 \cdot \tanh(0.823)}\) After evaluating this expression, we find: \(T(0.05, 480) = 59.2^{\circ} \mathrm{C}\) The temperature at the center of the cylinder 5 cm from the end surface 8 minutes after the start of cooling is \(59.2^{\circ} \mathrm{C}\).

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Most popular questions from this chapter

A long 18-cm-diameter bar made of hardwood \((k=\) $\left.0.159 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \alpha=1.75 \times 10^{-7} \mathrm{~m}^{2} / \mathrm{s}\right)\( is exposed to air at \)30^{\circ} \mathrm{C}$ with a heat transfer coefficient of \(8.83 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). If the center temperature of the bar is measured to be \(15^{\circ} \mathrm{C}\) after \(3 \mathrm{~h}\), the initial temperature of the bar is (a) \(11.9^{\circ} \mathrm{C}\) (b) \(4.9^{\circ} \mathrm{C}\) (c) \(1.7^{\circ} \mathrm{C}\) (d) \(0^{\circ} \mathrm{C}\) (e) \(-9.2^{\circ} \mathrm{C}\)

Consider a spherical shell satellite with outer diameter of \(4 \mathrm{~m}\) and shell thickness of \(10 \mathrm{~mm}\) that is reentering the atmosphere. The shell satellite is made of stainless steel with properties of $\rho=8238 \mathrm{~kg} / \mathrm{m}^{3}, c_{p}=468 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\(, and \)k=13.4 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}$. During the reentry, the effective atmosphere temperature surrounding the satellite is \(1250^{\circ} \mathrm{C}\) with a convection heat transfer coefficient of $130 \mathrm{~W} / \mathrm{m}^{2}\(. \)\mathrm{K}$. If the initial temperature of the shell is \(10^{\circ} \mathrm{C}\), determine the shell temperature after $5 \mathrm{~min}$ of reentry. Assume heat transfer occurs only on the satellite shell.

Consider a 7.6-cm-long and 3-cm-diameter cylindrical lamb meat chunk $\left(\rho=1030 \mathrm{~kg} / \mathrm{m}^{3}, c_{p}=3.49 \mathrm{~kJ} / \mathrm{kg} \cdot \mathrm{K}\right.\(, \)k=0.456 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, \alpha=1.3 \times 10^{-7} \mathrm{~m}^{2} / \mathrm{s}$ ). Fifteen such meat chunks initially at \(2^{\circ} \mathrm{C}\) are dropped into boiling water at \(95^{\circ} \mathrm{C}\) with a heat transfer coefficient of $1200 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$. The amount of heat transfer during the first \(8 \mathrm{~min}\) of cooking is (a) \(71 \mathrm{~kJ}\) (b) \(227 \mathrm{~kJ}\) (c) \(238 \mathrm{~kJ}\) (d) \(269 \mathrm{~kJ}\) (e) \(307 \mathrm{~kJ}\)

Carbon steel balls $\left(\rho=7830 \mathrm{~kg} / \mathrm{m}^{3}, k=64 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\right.\(, \)\left.c_{p}=434 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\right)\( initially at \)200^{\circ} \mathrm{C}\( are quenched in an oil bath at \)20^{\circ} \mathrm{C}$ for a period of \(3 \mathrm{~min}\). If the balls have a diameter of \(5 \mathrm{~cm}\) and the convection heat transfer coefficient is $450 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$, the center temperature of the balls after quenching will be (Hint: Check the Biot number.) (a) \(30.3^{\circ} \mathrm{C}\) (b) \(46.1^{\circ} \mathrm{C}\) (c) \(55.4^{\circ} \mathrm{C}\) (d) \(68.9^{\circ} \mathrm{C}\) (e) \(79.4^{\circ} \mathrm{C}\)

Hailstones are formed in high-altitude clouds at \(253 \mathrm{~K}\). Consider a hailstone with diameter of \(20 \mathrm{~mm}\) that is falling through air at \(15^{\circ} \mathrm{C}\) with convection heat transfer coefficient of $163 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}$. Assuming the hailstone can be modeled as a sphere and has properties of ice at \(253 \mathrm{~K}\), determine how long it takes to reach melting point at the surface of the falling hailstone. Solve this problem using the analytical one-term approximation method.

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