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Section 17.6 : Divergence Theorem

2. Use the Divergence Theorem to evaluate \( \displaystyle \iint\limits_{S}{{\vec F\centerdot d\vec S}}\) where \(\vec F = \sin \left( {\pi x} \right)\,\vec i + z{y^3}\,\vec j + \left( {{z^2} + 4x} \right)\,\vec k\) and \(S\) is the surface of the box with \( - 1 \le x \le 2\), \(0 \le y \le 1\) and \(1 \le z \le 4\). Note that all six sides of the box are included in \(S\).

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Let’s start off with a quick sketch of the surface we are working with in this problem.

A three dimensional sketch of the surface drawn with the traditional axes.  It is the box with \( - 1 \le x \le 2\), \(0 \le y \le 1\) and \(1 \le z \le 4\), a tall thin rectangular block, and all six faces are included. A three dimensional sketch of the same box, this time drawn with a “box frame” set of axes to make the surface easier to visualize.

We included a sketch with traditional axes and a sketch with a set of “box” axes to help visualize the surface.

Note as well here that because we are including all six sides of the box shown above that the surface does enclose (or is the boundary curve if you want to use that terminology) for the box.

Show Step 2

We are going to use the Divergence Theorem in the following direction.

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

where \(E\) is just the solid shown in the sketches from Step 1.

\(E\) is just a box and the limits defining it where given in the problem statement. The limits for our integral will then be,

\[\begin{array}{c} - 1 \le x \le 2\\ 0 \le y \le 1\\1 \le z \le 4\end{array}\]

We’ll also need the divergence of the vector field so here is that.

\[{\mathop{\rm div}\nolimits} \vec F = \frac{\partial }{{\partial x}}\left( {\sin \left( {\pi x} \right)} \right) + \frac{\partial }{{\partial y}}\left( {z{y^3}\,} \right) + \frac{\partial }{{\partial z}}\left( {{z^2} + 4x} \right) = \pi \cos \left( {\pi x} \right) + 3z{y^2} + 2z\]
Show Step 3

Now let’s apply the Divergence Theorem to the integral and get it converted to a triple integral.

\[\begin{align*}\iint\limits_{S}{{\vec F\centerdot d\vec S}} & = \iiint\limits_{E}{{{\mathop{\rm div}\nolimits} \vec F\,dV}}\\ & = \iiint\limits_{E}{{\pi \cos \left( {\pi x} \right) + 3z{y^2} + 2z\,dV}}\\ & = \int_{{ - 1}}^{2}{{\int_{0}^{1}{{\int_{1}^{4}{{\pi \cos \left( {\pi x} \right) + 3z{y^2} + 2z\,dz}}\,dy}}\,dx}}\end{align*}\]
Show Step 4

All we need to do then in evaluate the integral.

\[\begin{align*}\iint\limits_{S}{{\vec F\centerdot d\vec S}} & = \int_{{ - 1}}^{2}{{\int_{0}^{1}{{\int_{1}^{4}{{\pi \cos \left( {\pi x} \right) + 3z{y^2} + 2z\,dz}}\,dy}}\,dx}}\\ & = \int_{{ - 1}}^{2}{{\int_{0}^{1}{{\left. {\left( {\pi z\cos \left( {\pi x} \right) + \frac{3}{2}{z^2}{y^2} + {z^2}} \right)} \right|_1^4\,dy}}\,dx}}\\ & = \int_{{ - 1}}^{2}{{\int_{0}^{1}{{3\pi \cos \left( {\pi x} \right) + \frac{{45}}{2}{y^2} + 15\,dy}}\,dx}}\\ & = \int_{{ - 1}}^{2}{{\left. {\left( {3y\pi \cos \left( {\pi x} \right) + \frac{{15}}{2}{y^3} + 15y} \right)} \right|_0^1\,dx}}\\ & = \int_{{ - 1}}^{2}{{3\pi \cos \left( {\pi x} \right) + \frac{{45}}{2}\,dx}}\\ & = \left. {\left( {3\sin \left( {\pi x} \right) + \frac{{45}}{2}x} \right)} \right|_{ - 1 }^2 = \require{bbox} \bbox[2pt,border:1px solid black]{{\frac{{135}}{2}}}\end{align*}\]