Uniform internal heat generation at (dot{q}=6 times 10^{7} mathrm{~W} / mathrm{m}^{3}) is occurring in a cylindrical nuclear

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Uniform internal heat generation at \(\dot{q}=6 \times 10^{7} \mathrm{~W} / \mathrm{m}^{3}\) is occurring in a cylindrical nuclear reactor fuel rod of \(60-\mathrm{mm}\) diameter, and under steady-state conditions


the temperature distribution is of the form \(T(r)=a+\) \(b r^{2}\), where \(T\) is in degrees Celsius and \(r\) is in meters, while \(a=900^{\circ} \mathrm{C}\) and \(b=-5.26 \times 10^{5}{ }^{\circ} \mathrm{C} / \mathrm{m}^{2}\). The fuel rod properties are \(k=30 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, ho=1100 \mathrm{~kg} / \mathrm{m}^{3}\), and \(c_{p}=800 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\).

(a) What is the rate of heat transfer per unit length of the rod at \(r=0\) (the centerline) and at \(r=30 \mathrm{~mm}\) (the surface)?

(b) If the reactor power level is suddenly increased to \(\dot{q}_{2}=10^{8} \mathrm{~W} / \mathrm{m}^{3}\), what is the initial time rate of temperature change at \(r=0\) and \(r=30 \mathrm{~mm}\) ?

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Fundamentals Of Heat And Mass Transfer

ISBN: 9781119220442

8th Edition

Authors: Theodore L. Bergman, Adrienne S. Lavine

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