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Home / Calculus III / Surface Integrals / Divergence Theorem
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August 27, 2020

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### Section 6-6 : Divergence Theorem

In this section we are going to relate surface integrals to triple integrals. We will do this with the Divergence Theorem.

#### Divergence Theorem

Let $$E$$ be a simple solid region and $$S$$ is the boundary surface of $$E$$ with positive orientation. Let $$\vec F$$ be a vector field whose components have continuous first order partial derivatives. Then,

$\iint\limits_{S}{{\vec F\centerdot d\vec S}} = \iiint\limits_{E}{{{\mathop{\rm div}\nolimits} \vec F\,dV}}$

Let’s see an example of how to use this theorem.

Example 1 Use the divergence theorem to evaluate $$\displaystyle \iint\limits_{S}{{\vec F\centerdot d\vec S}}$$ where $$\vec F = xy\,\vec i - \frac{1}{2}{y^2}\,\vec j + z\,\vec k$$ and the surface consists of the three surfaces, $$z = 4 - 3{x^2} - 3{y^2}$$, $$1 \le z \le 4$$ on the top, $${x^2} + {y^2} = 1$$, $$0 \le z \le 1$$ on the sides and $$z = 0$$ on the bottom.
Show Solution

Let’s start this off with a sketch of the surface.

The region $$E$$ for the triple integral is then the region enclosed by these surfaces. Note that cylindrical coordinates would be a perfect coordinate system for this region. If we do that here are the limits for the ranges.

$\begin{array}{c}0 \le z \le 4 - 3{r^2}\\ 0 \le r \le 1\\ 0 \le \theta \le 2\pi \end{array}$

We’ll also need the divergence of the vector field so let’s get that.

${\mathop{\rm div}\nolimits} \vec F = y - y + 1 = 1$

The integral is then,

\begin{align*}\iint\limits_{S}{{\vec F\centerdot d\vec S}} & = \iiint\limits_{E}{{{\mathop{\rm div}\nolimits} \vec F\,dV}}\\ & = \int_{{\,0}}^{{\,2\pi }}{{\int_{{\,0}}^{{\,1}}{{\int_{{\,0}}^{{4 - 3{r^2}}}{{r\,dz}}\,dr}}\,d\theta }}\\ & = \int_{{\,0}}^{{\,2\pi }}{{\int_{{\,0}}^{{\,1}}{{4r - 3{r^3}\,dr}}\,d\theta }}\\ & = \int_{{\,0}}^{{\,2\pi }}{{\left. {\left( {2{r^2} - \frac{3}{4}{r^4}} \right)} \right|_0^1\,d\theta }}\\ & = \int_{{\,0}}^{{\,2\pi }}{{\frac{5}{4}\,d\theta }}\\ & = \frac{5}{2}\pi \end{align*}
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