Surface Integral

Motivation

KE, CC-BY, "torus".

Have you ever thought to yourself, "I wonder how much powdered sugar I could get on a donut?"
I would assume no but I can get you on the right track.

Vectors

Disclaimer: this page will be a little out there, even for me.

A vector is a combination of a scalar and a direction. Technically, that is. Less formally, we can say that a vector is the combination of a length and a direction. For example, an arrow pointing up with length 3 is a vector. There are many ways to notate a vector but for this we will use the standard $x$, $y$ ordered pair notation with angled brackets. A vector is assumed to have its tail at the origin and its head at the point shown in $\langle x, y\rangle$. Its length (by simple trigonometry) is $\sqrt{x^2 + y^2}$ and its direction (or angle) is $\tan^{-1}(\frac{y}{x})$.

Easy enough, right? Right, but now it gets worse.
To find the surface area of a donut (torus) we must realize that a donut is 3-dimensional.
That means that our vectors will be of the form $\vec{v} = \langle x,y,z\rangle$. Our length will be $\sqrt{x^2+y^2+z^2}$ and our direction will be a little bit (lotta bit) more complicated and unnecessary.

Operations

Let us notice that $a \cdot \langle x , y, z \rangle = \langle ax, ay, az \rangle$. Where $a$ is just a number.

Another property to notice is that $\langle x, y, z \rangle + \langle a, b, c \rangle = \langle x + a, y + b, z + c \rangle$.

Using $\hat{\imath} = \langle 1, 0, 0 \rangle$, $\hat{\jmath} = \langle 0, 1, 0 \rangle$, and $\hat{\mathcal{k}} = \langle 0, 0, 1 \rangle$, We can rewrite any vector $\langle x,y,z\rangle$ as $x\hat{\imath} + y\hat{\jmath} + z\hat{\mathcal{k}}$.

We define the cross product of two vectors to be the determinant of the matrix made up of the basis vectors and the two other vectors together, that is: for any two vectors, $\vec{u} = \langle x,y,z\rangle$ and $\vec{v} = \langle a,b,c \rangle$, $$ \vec{u} \times \vec{v} = \left| \begin{matrix} \hat{\imath} & \hat{\jmath} & \hat{\mathcal{k}} \\ x & y & z \\ a & b & c \\ \end{matrix} \right| = \hat{\imath}(yc - zb) + \hat{\jmath}(za - xc) + \hat{\mathcal{k}}(xb-ya) = \langle yc-zb,\; za - xc,\; xb-ya \rangle $$ Geometrically, the cross product gives us a new vector that is one of the vectors that is perpendicular to both.


Surface Integral

Consider that $\Omega$ is some surface (in our case, a donut) in 3 dimensions.
$\vec{v}(t,s)$ is a function that takes in two parameters and gives out a vector. Using the desired constrained inputs for the function, the function will map out $\Omega$.
Finally, consider $C$ being the space of the (constraint of $t$) $\times$ (the constraint of $s$).

In our case, $\Omega$ is a donut, $\vec{v}(t,s) = \langle (b+a\cos(t))\sin(s), \; (b+a\cos(t))\cos(s), \; a\sin(t) \rangle$, and our constraints are that $t$ and $s$ both go from $0$ to $2 \pi$ so $C = [0,2\pi] \times [0, 2\pi]$. Where $a$ is the radius of the loop and $b$ is the radius of the donut.

The formula for surface area is $$ \iint_C \left| \frac{\partial \vec{v}}{\partial t} \times \frac{\partial \vec{v}}{\partial s} \right| dt\,ds $$
Using our amazing calculus skills, we can rewrite this as $$ \int\limits_0^{2\pi}\int\limits_0^{2\pi} \left| \frac{\partial \vec{v}}{\partial t} \times \frac{\partial \vec{v}}{\partial s} \right| dt\,ds $$ Calculating the partial derivatives, we get: $$\frac{\partial \vec{v}}{\partial t} = \langle -a \sin(s) \sin(t), \; -a \cos(s) \sin(t), \; a\cos(t) \rangle$$ And calculating the other, we get: $$ \frac{\partial \vec{v}}{\partial s} = \langle (b + a\cos(t))\cos(s), \; -(b+a\cos(t)\sin(s)), \; 0 \rangle $$ Skipping most of the hard work, we find the determinant (which geometrically is the area of the parallelogram created by the two vectors' cross product): $$ \left| \frac{\partial \vec{v}}{\partial t} \times \frac{\partial \vec{v}}{\partial s} \right| = ab + a^2 \cos(t) $$ Now we can rewrite the integral and solve! $$ \int\limits_0^{2\pi}\int\limits_0^{2\pi} ab + a^2 \cos(t) dt ds = \int\limits_0^{2\pi} \left[ abt + a^2 \sin(t) \right]_0^{2\pi}ds \\ = \int\limits_0^{2\pi} 2\pi ab ds = \left[ 2\pi abs \right]_0^{2\pi} = 4\pi^2 ab $$ Wow. We found our answer. The surface area of a donut is $4\pi^2$ times its inner radius times its outer radius. We could have just looked that up but we didn't. Astounding.