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Consider a homogeneous spherical piece of radioactive material of radius \(r_{o}=0.04 \mathrm{~m}\) that is generating heat at a constant rate of \(\dot{e}_{\mathrm{gen}}=4 \times 10^{7} \mathrm{~W} / \mathrm{m}^{3}\). The heat generated is dissipated to the environment steadily. The outer surface of the sphere is maintained at a uniform temperature of \(80^{\circ} \mathrm{C}\), and the thermal conductivity of the sphere is $k=15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\(. Assuming steady one-dimensional heat transfer, \)(a)$ express the differential equation and the boundary conditions for heat conduction through the sphere, \((b)\) obtain a relation for the variation of temperature in the sphere by solving the differential equation, and \((c)\) determine the temperature at the center of the sphere.

Short Answer

Expert verified
Answer: The temperature at the center of the spherical piece of radioactive material is approximately \(188.16^{\circ} \mathrm{C}\).

Step by step solution

01

Recall heat conduction equation in spherical coordinates

The heat conduction equation in spherical coordinates is given by: \[\frac{1}{r^{2}}\frac{\partial}{\partial r}\left(r^{2} \frac{\partial T}{\partial r}\right) = \frac{\dot{e}_{\mathrm{gen}}}{k}\] Where \(T\) is the temperature, \(r\) is the radial coordinate, \(\dot{e}_{\mathrm{gen}}\) is the heat generation rate per unit volume, and \(k\) is the thermal conductivity.
02

Write down the given information and values

The given information and values are: - Sphere radius: \(r_{o} = 0.04\) m - Heat generation rate: \(\dot{e}_{\mathrm{gen}} = 4 \times 10^{7} \mathrm{~W} / \mathrm{m}^{3}\) - Outer surface temperature: \(80^{\circ} \mathrm{C}\) - Thermal conductivity: \(k = 15 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\)
03

Express the differential equation and boundary conditions

Using the heat conduction equation from Step 1, we have: \[\frac{1}{r^{2}}\frac{\partial}{\partial r}\left(r^{2} \frac{\partial T}{\partial r}\right) = \frac{4 \times 10^{7}}{15}\] Boundary conditions: 1. At the outer surface of the sphere (\(r = r_{o}\)), the temperature is maintained at \(80^{\circ} \mathrm{C}\): \(T(r_{o}) = 80^{\circ} \mathrm{C}\). 2. At the center of the sphere (\(r = 0\)), the temperature gradient is zero due to thermal symmetry: \(\frac{\partial T}{\partial r}(0) = 0\).
04

Solve the differential equation

Integrating the differential equation twice, we obtain: \[\frac{\partial T}{\partial r} = -\frac{4 \times 10^{7}}{15} \frac{r^{3}}{3} + C_{1}\] Applying boundary condition 2 (\(\frac{\partial T}{\partial r}(0) = 0\)), we find \(C_{1} = 0\). So, \[\frac{\partial T}{\partial r} = -\frac{4 \times 10^{7}}{15} \frac{r^{3}}{3}\] Integrating again, we obtain: \[T(r) = -\frac{4 \times 10^{7}}{15} \frac{r^{4}}{12} + C_{2}\] Now, applying boundary condition 1 (\(T(r_{o}) = 80^{\circ} \mathrm{C}\)), we find: \[C_{2} = 80 + \frac{4 \times 10^{7}}{15} \frac{(0.04)^{4}}{12}\] So, the temperature variation in the sphere is: \[T(r) = -\frac{4 \times 10^{7}}{15} \frac{r^{4}}{12} + 80 + \frac{4 \times 10^{7}}{15} \frac{(0.04)^{4}}{12}\]
05

Determine the temperature at the center of the sphere

To determine the temperature at the center of the sphere, set \(r = 0\) in the temperature variation equation: \[T(0) = -\frac{4 \times 10^{7}}{15} \frac{(0)^{4}}{12} + 80 + \frac{4 \times 10^{7}}{15} \frac{(0.04)^{4}}{12}\] \[T(0) = 80 + \frac{4 \times 10^{7}}{15} \frac{(0.04)^{4}}{12}\] Calculating this value, we get: \[T(0) \approx 188.16^\circ \mathrm{C}\] So, the temperature at the center of the sphere is approximately \(188.16^{\circ} \mathrm{C}\).

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Most popular questions from this chapter

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Consider steady one-dimensional heat conduction through a plane wall, a cylindrical shell, and a spherical shell of uniform thickness with constant thermophysical properties and no thermal energy generation. The geometry in which the variation of temperature in the direction of heat transfer will be linear is (a) plane wall (b) cylindrical shell (c) spherical shell (d) all of them (e) none of them

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A long homogeneous resistance wire of radius \(r_{o}=0.6 \mathrm{~cm}\) and thermal conductivity \(k=15.2 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) is being used to boil water at atmospheric pressure by the passage of electric current. Heat is generated in the wire uniformly as a result of resistance heating at a rate of \(16.4 \mathrm{~W} / \mathrm{cm}^{3}\). The heat generated is transferred to water at \(100^{\circ} \mathrm{C}\) by convection with an average heat transfer coefficient of $h=3200 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\(. Assuming steady one-dimensional heat transfer, \)(a)$ express the differential equation and the boundary conditions for heat conduction through the wire, \((b)\) obtain a relation for the variation of temperature in the wire by solving the differential equation, and \((c)\) determine the temperature at the centerline of the wire.

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