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In Exercises \(5-16,\) use the Divergence Theorem to evaluate \(\int_{S} \int \mathbf{F} \cdot \mathbf{N} d S\) and find the outward flux of \(F\) through the surface of the solid bounded by the graphs of the equations. Use a computer algebra system to verify your results. $$ \begin{aligned} &\mathbf{F}(x, y, z)=\left(x y^{2}+\cos z\right) \mathbf{i}+\left(x^{2} y+\sin z\right) \mathbf{j}+e^{z} \mathbf{k}\\\ &S: z=\frac{1}{2} \sqrt{x^{2}+y^{2}}, z=8 \end{aligned} $$

Short Answer

Expert verified
To find the outward flux, calculate the given triple integral after converting everything to cylindrical coordinates.

Step by step solution

01

Identify the vector field and the solid region

We first identify the vector field \(\mathbf{F}(x, y, z) = \left(x y^{2}+\cos z\right) \mathbf{i}+\left(x^{2} y+\sin z\right) \mathbf{j}+e^{z} \mathbf{k}\) and the solid region \(D\) bounded by \(S_1: z=\frac{1}{2} \sqrt{x^{2}+y^{2}}\) and \(S_2: z=8\).
02

Write the divergence of the vector field

The divergence of \(\mathbf{F}\) is calculated using the formula \(\nabla \cdot \mathbf{F} = \frac{\partial F_1}{\partial x} + \frac{\partial F_2}{\partial y} + \frac{\partial F_3}{\partial z}\). This gives us \(\nabla \cdot \mathbf{F} = 2xy + x^{2} + e^{z}\).
03

Convert to cylindrical coordinates

We change to cylindrical coordinates to make the integral simpler. In cylindrical coordinates, \(x = r\cos\theta, y = r\sin\theta,\) and \(z = z\). Our divergence becomes \(\nabla \cdot \mathbf{F} = 2r^{2}\cos\theta\sin\theta + r^{2}\cos^{2}\theta + e^{z}\). The lower surface in cylindrical coordinates becomes \(z = \frac{1}{2}r\) and upper surface remains \(z = 8\). The region \(D\) in cylindrical coordinates is then \(0 \leq r \leq 16\), \(0 \leq \theta \leq 2\pi\), and \(\frac{1}{2}r \leq z \leq 8\).
04

Calculate the triple integral

With all the components in place, we can now evaluate the triple integral using the divergence theorem. The divergence theorem states that \(\iint_{S} \mathbf{F} \cdot d\mathbf{S} = \iiint_{D} \nabla \cdot \mathbf{F} \,dV\) which, in this case, yields the triple integral \(\iiint_{D} 2r^{2}\cos\theta\sin\theta + r^{2}\cos^{2}\theta + e^{z} \, dzdrd\theta\). Evaluating this integral should yield the outward flux through the solid surface.

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