Geometry and the Discrete Fourier Transform
We'll show a relationship between some elementary geometry of the plane and the Discrete Fourier Transform, that is a starting point for ramifications for polynomials, circulant matrices and interpolation, and even sculpture. We employ some recent technology to do this. ...
Patrick D. F. Ion
Mathematical Reviews
ion at ams.org
Introduction
Many of the most curious and popular theorems of plane geometry are those of Coincidence, Collinearity, and Equilateralness (also sometimes called Equilaterality): a certain collection of lines all intersect in a single point, or a collection of points in the plane lies on a line, or a certain triple of points forms an equilateral triangle.
The Discrete Fourier Transform is a tool used to efficiently and accurately approximate the Fourier Transform. It is applied in electrical engineering to analyze a signal into its components at various frequencies, and in mechanical engineering to analyze vibrations of a system.
There is a surprising connection between these two topics.
The starting point is to consider points in the plane as complex numbers $z = x+\ii y\in\cplx.$
To see a note on new technology behind this document, and explanation of the buttons above, click on the following uparrow; to hide it again click on the corresponding downarrow when it is shown .
This pairing of up and downarrows is used to Show or Hide asides or details of equations throughout this month's column.
Part I. The theorems
Theorems of Coincidence: Triangle Medians
The median lines of a triangle are the lines drawn from each vertex to the midpoint of the opposite side. The simplest Coincidence Theorem asserts that these three lines meet in a single point (which happens to be the center of gravity or centroid of the triangle).
There are other well known examples: the angle bisectors all intersect at the point $I$, the center of the inscribed circle (called the incenter), the perpendicular bisectors of the sides intersect at the circumcenter $C$, the altitudes intersect at the orthocenter $O$.
Collinearity theorems
The prime example of a collinearity theorem is that the circumcenter $C$, the centroid $G$ and the orthocenter $O$ are collinear. Below the altitudes are in black, medians are in green and perpendicular bisectors in blue. The line through their coincidence is shown in orange.
Equilateralness  Napoleon's Theorem
Napoleon's Theorem, though probably not directly due to the emperor himself, has long borne his name.
Its simplest form says that if one constructs an equilateral triangle external to each side of a nondegenerate plane triangle, and takes the three centroids of the resulting triangles, then these points form an equilateral triangle. A similar construction using internal triangles also leads to another equilateral triangle.
The most famous equilaterality theorem is Morley's Miracle from about 1901 which states that the pairwise intersections of adjacent internal angle trisectors are the vertices of an equilateral triangle.
In the case shown there is the equilateral triangle from the internal trisectors, and another one from external trisectors is show as well. The internal trisectors are shown in green, the external trisectors are shown in lilac.
A pentagon construction
A relatively recent construction was discovered by the Fields Medalist Jesse Douglas. It was devised probably around 1940, but only published in 1960, in a piece written in honor of a colleague Jekuthiel Ginsburg. He specifies a fixed construction that from any pentagon derives an associated convex pentagon and pentagram.
Consider a pentagon in the plane. Suppose the five vertex points are $ p_0, p_1, p_3 p_3, p_4$, taken to be numbers in $\cplx$. So we are given a complex vector in $\cplx^5$, which is to say an array of complex numbers $$ p=(p_0,p_1,p_2,p_3,p_4).$$ No one point of the five is to be distinguished. What is important is the cyclic order, so we shall consider the indices $i$ of $p_i$ modulo $5$. Sums in the index are cyclic, so that, for instance, $p_{3+4} = p_2$.
Douglas tells us: Join each vertex $p_i$ to the midpoint of the edge opposite between the points $p_{i+2}$ and $p_{i+3}$; then extend that line by an extra $(1/\sqrt{5})$ of its length to create a new vertex $q_i$. The new pentagon $(q_0,q_1, q_2, q_3, q_4)$ is always the affine image of a convex regular pentagon. Also, if the lines to the opposite midpoints are shortened by a similar decrement of $(1/\sqrt{5})$ to give new vertices $r_i$, then $(r_0, r_1, r_2, r_3, r_4)$ is the affine image of a regular star pentagon, commonly called a pentagram.
We plot a chosen example of $p=(p_0,p_1,p_2,p_3,p_4)$ but, as usual, the vertices can be dragged about in the interactive popup figures.
We see $$ q_i = p_i + \left(1+{\textstyle\sfrac1{\sqrt{5}}}\right) \left({{\textstyle\sfrac12}}(p_{i+2}+p_{i+3})  p_i\right) , $$ outlined in green in the figure.
and similarly $$ r_i = p_i + \left(1{\textstyle\sfrac11{\sqrt{5}}}\right)\left({\textstyle\sfrac12}(p_{i+2}+p_{i+3})  p_i\right) , $$ outlined in red.
One may put all this in a diagram with evrything drawn, which it is amusing to pull about to see the effect of the construction.
We see that starting from an arbitrary pentagon, a list of five points, we get by a fixed construction two new pentagons, which are, respectively, an affine image of a standard convex pentagon and an affine image of a standard pentagram.
Aside: affine transformations
Affine transformations
The general form of an affine transformation of the plane with coordinates $x$ and $y$, can be written $$\left(\begin{array}{c}x\\ y\\ \end{array}\right) \mapsto \left(\begin{array}{cc}a&b\\ c&d\\ \end{array}\right) \left(\begin{array}{c}x\\ y\end{array}\right) + \left(\begin{array}{c}e\\ f\end{array}\right) .$$ If we view the $(x,y)$plane as the complex plane $\cplx$, thus in terms of $z=x+\ii y$ with $\ii = \sqrt{1}$, we have to translate the above into complex language. We see the general plane affine transformation written in complex coordinates is $$ z \mapsto \lambda z + \mu \overline z + \nu $$ with $2 \lambda=(a+d)+(cb)\ii,\ 2 \mu=(ad)+(c+b)\ii,\ \nu\in\cplx$.
The addition of a constant term can be realized by the addition of a complex number: $$z = x + \ii y \mapsto x + \ii y + (e + \ii f)$$ so we are left with the matrix to deal with.
Since in the above affine transformation $x$ and $y$ are not coupled, a moment's reflection reveals that the expression using complex coordinates for an affine transformation will have to involve both $z$ and $\overline z$, the complex conjugate, so as to provide access to the real and imaginary parts of $z$. But then we just need to equate the general forms $$(\alpha + \ii \beta) (x + \ii y) + (\gamma + \ii \delta) (x  \ii y) = (ax + by) + \ii (cx + dy) .$$ The solution is $$\left(\begin{array}\alpha\\ \beta\\ \gamma\\ \delta\\\end{array}\right) = {1\over2} \left(\begin{array}{c}a+d\\ cb\\ ad\\ c+b\\\end{array}\right) ={1\over2} \left(\begin{array}{cccc}1&0&0&1\\ 0&1&1&0\\ 1&0&0&1\\ 0&1&1&0\end{array}\right) \left(\begin{array}{c}a\\ b\\ c\\ d\\\end{array}\right). $$ So we see the general plane affine transformation written in complex coordinates is $$ z \mapsto \lambda z + \mu \overline z + \nu $$ with $2 \lambda=(a+d)+(cb)\ii,\ 2 \mu=(ad)+(c+b)\ii,\ \nu\in\cplx$.
Another way of seeing this is just to note that the change from real to complex coordinates is \begin{eqnarray*} \left(\begin{array}{c} x\\ y\\ \end{array}\right) &=& \left(\begin{array}{c} (z+\zbar)/2\\ (z\zbar)/2\ii\\ \end{array}\right) =\frac12 \left(\begin{array}{cc} \ \ 1&\ 1\\ \ii&\ii\\ \end{array}\right) \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right) \\ &\mapsto&\frac12 \left(\begin{array}{cc} a&b\\ c&d\\ \end{array}\right) \left(\begin{array}{cc} \ 1&\ 1\\ \ii&\ii\\ \end{array}\right) \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right) =\frac12 \left(\begin{array}{cc} a\ii b& a+\ii b\\ c\ii d& c+\ii d\\ \end{array}\right) \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right). \\ \end{eqnarray*} In other words \begin{eqnarray*} \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right) = &\mapsto&\frac12 \left(\begin{array}{cc} \ 1& +\ii\\ \ 1&\ii\\ \end{array}\right) \left(\begin{array}{cc} a&b\\ c&d\\ \end{array}\right) \left(\begin{array}{cc} \ 1&\ 1\\ \ii& +\ii\\ \end{array}\right) \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right) \\ & =& \frac12 \left(\begin{array}{cc} \ 1& +\ii \\ \ 1& \ii \\ \end{array}\right) \left(\begin{array}{cc} a\ii b& a+\ii b\\ c\ii d&c+\ii d\\ \end{array}\right) \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right) \\ & =& \frac12 \left(\begin{array}{cc} (a+d)(bc)\ii & (ad)+(b+c)\ii\\ (ad)(b+c)\ii & (a+d)+(bc)\ii\\ \end{array}\right) \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right),\\ & =& \left(\begin{array}{cc} \lambda & \mu\\ \overline{\lambda} & \overline{\mu}\\ \end{array}\right) \left(\begin{array}{c} z\\ \zbar\\ \end{array}\right),\\ \end{eqnarray*} since $$ \frac12 \left(\begin{array}{cc} \ 1&+\ii \\ \ 1&\ii \\ \end{array}\right) \left(\begin{array}{cc} \ 1&\ 1\\ \ii&+\ii\\ \end{array}\right) = \left(\begin{array}{c} \ 1&\ 0\\ \ 0&\ 1\\ \end{array}\right). $$
Now consider the case of a linear sum of a regular $n$gon and its opposite, say the case of the convex pentagon where we had $n=5$. The points are of the form $A \omega^k + B \omega^{k}$. But $\omega^{1}=\bar \omega$, so these points are affine images of the points of the standard convex pentagon with parameters $$ (\lambda,\mu,\nu) = (A, B, 0). $$ That's what we have above as the result of Douglas's construction with a similar consideration for the affine image of a standard pentagram.
Part II. Geometry with the Discrete Fourier Transform
The Discrete Fourier Transform
A polygon with $N$ sides is a sequence of vertices $p_{0}$, $p_{1}$, ... , $p_{N1}$. None of the vertices is particularly more important than the others, so all that really matters is the cyclic order. In other words, what we have at hand is a complexvalued function $p_{j}$ on the cyclic group $\intg/N$ (short for $\intg/N\intg$.
The vector space $\cplx[\intg/N]$ of all complexvalued functions on $\intg/N$ has dimension $N$, and the natural coordinate system on this space assigns to a function $f$ the array $(f_{0}, \dots , f_{N1})$ in $\cplx^{N}$. But there is another useful coordinate system as well. To tell you what this is, we need to specify a new basis of the vector space. Let $\omega_{N} = \ee^{2 \pi \ii/N}$, and for each $a$ in $\intg$, let $\chi_{a}$ (more precisely $\chi_{N,a}$) be the function taking $j$ to $\omega_{N}^{aj}$. This is a function on $\intg/N$, since $\omega_{N}^{N} = 1$, that is $\omega_{N}$ is an $N$th root of unity. Furthermore, $\chi_{a}$ only depends on $a$ modulo $N$, so there are $N$ of these functions.
We assign to the complex vector space of complexvalued functions on $\intg/N$ a a Hermitian inner product: $$ p \Dot q = { 1 \over N} \sum_{j=0}^{N1} p_{j}\bar{q}_{j} = (1/N)(p_{0}\bar{q}_{0} + \cdots + p_{N1}\bar{q}_{N1}) . $$ The function $\chi_{0}$ is just the constant function taking all $j$ to $1$. We have $$ \chi_{a} \Dot \chi_{0} = \begin{cases} 1 \text{ if } a=0 \cr 0 \text{ otherwise} \cr \end{cases} $$ and hence $$ \chi_{a} \Dot \chi_{b} = \begin{cases} 1 \text{ if } a=b \cr 0 \text{ otherwise.}\cr \end{cases} $$ This means that the functions $\chi_{a}$ for $a$ in $\intg/N$ are an orthonormal basis for the space of functions on $\intg/N$. If $f$ is any such function, we may therefore write $$ f = \sum_{a=0}^{N1} \hat{f}_{a} \chi_{a} \quad \text{ where } \quad \hat{f}_{a} = f \Dot \chi_{a} $$ In particular, $\hat f_{0}$ is the center of gravity (a.k.a. centroid, barycenter or mean) of the values of $f$, $$ \hat{f}_{0} = \frac{1}{N} (f_0 + \cdots + f_{N1}) $$ and $\hat{f}_{0},\dots,\hat{f}_{N1}$ are the coefficients in the expression of the arbitrary function $f$, an $N$gon, as a linear sum of standard ones.
For example, the function $f_{j} = \chi_{1}(j)$ lists the vertices of the symmetric regular polygon of $N$ sides inscribed in the unit circle. Similarly $g_{j} = \chi_{N1}(j)$ gives the standard negatively oriented unit $N$gon. The combination $\lambda \chi_{1} +\mu \chi_{N1}$ with $\lambda$, $\mu$ in $\cplx$ then gives a general affine convex $N$gon.
Triangle geometry
The claim is that much classical plane geometry has a natural expression from the point of view outlined above. Start by looking at the standard types of triangles. For that we'll take $\omega := \omega_3^{\strut} = \frac12(1 + \ii \sqrt3)$ until further notice. The standard triangles are $\chi_0=(1,1,1)$, the degenerate one with 3 points at 1, the unit equilateral triangle $\chi_1=(1,\omega,\omega^2)$, and its reverse $\chi_2=(1,\omega^2,\omega)$.
The picture below shows the simple average of a standard equilateral triangle and its reverse, namely $\sfrac12(\chi_1+\chi_2)$. It is a digon (a segment) with a double point at the lefthand end.
We consider only triangles whose centroids are at the origin; after all, it is easy enough to move any triangle into this simplifying position by a translation, and all interesting theorems of plane geometry are invariant under translations.
If we separate the two triangles by making the standard one larger, say lying on a circle of radius $\lambda>1$ then we get
which shows the triangle is an isosceles one with height $\sfrac34(\lambda+1)$ lying along the real axis.
The slider labelled $\lambda$ controls the radius of the outer circle. The green isosceles triangle in the middle is the average of the two triangles with labelled vertices. Note the opposite orientations of the two triangles being averaged.
If we separate the two basic triangles $\chi_1$ and $\chi_2$ by turning them in opposite directions by a turn $\ee^{\ii \alpha}$ (in the attractive terminology of Frank Morley for complex numbers of modulus 1) to make $$ \begin{eqnarray} {\textstyle\sfrac12}(\ee^{\ii \alpha}\chi_1+\ee^{\ii \alpha}\chi_2)&=& {\textstyle\sfrac12}\left\{\ee^{\ii \alpha}(1,{\textstyle\sfrac12}+{\textstyle\sfrac{\sqrt3}2}\ii, {\textstyle\sfrac12}{\textstyle\sfrac{\sqrt3}2}\ii) +\ee^{\ii \alpha}(1,{\textstyle\sfrac12}{\textstyle\sfrac{\sqrt3}2}\ii, {\textstyle\sfrac12}+{\textstyle\sfrac{\sqrt3}2}\ii)\right\}\cr &=& \left({\textstyle\sfrac12}(\ee^{\ii \alpha}+\ee^{\ii \alpha}), {\textstyle\sfrac14}(\ee^{\ii \alpha}+\ee^{\ii \alpha})+ {\textstyle\sfrac{\sqrt3}4}\ii(\ee^{\ii \alpha}\ee^{\ii \alpha}) ,{\textstyle\sfrac14}(\ee^{\ii \alpha}+\ee^{\ii \alpha}) {\textstyle\sfrac{\sqrt3}4}\ii(\ee^{\ii \alpha}\ee^{\ii \alpha})\right)\cr &=&(\cos \alpha, {\textstyle\sfrac12}\cos \alpha{\textstyle\sfrac{\sqrt3}2}\sin \alpha, {\textstyle\sfrac12}\cos \alpha+{\textstyle\sfrac{\sqrt3}2}\sin \alpha) ) \end{eqnarray} $$ $$ \begin{eqnarray} {\textstyle\sfrac12}(\ee^{\ii \alpha}\chi_1+\ee^{\ii \alpha}\chi_2)= (\cos \alpha, {\textstyle\sfrac12}\cos \alpha{\textstyle\sfrac{\sqrt3}2}\sin \alpha, {\textstyle\sfrac12}\cos \alpha+{\textstyle\sfrac{\sqrt3}2}\sin \alpha) ) \end{eqnarray} $$ then we have achieved a splitting of the double point at $\sfrac12$ in $\sfrac12(\chi_1+\chi_2)$ but still have a degenerate triangle on the real axis, with the second vertex at $z_1=\sfrac12\cos \alpha\sfrac{\sqrt3}2\sin \alpha$ and the third symmetrically placed about $\frac12\cos\alpha$ at $z_2=\sfrac12\cos \alpha+\sfrac{\sqrt3}2\sin \alpha$.
The green slider $\alpha$ controls the angle away from the $x$axis that the triangles are rotated; it goes from $0$ to $2 \pi$. The linear green triangle is the average of the triangles with vertices on the unit circle. Note that the cycle $\ee^{\ii\alpha}$, $\ee^{\ii\alpha}\omega$ and $\ee^{\ii\alpha}\omega^2$ is positively oriented (counterclockwise) and $\ee^{\ii\alpha}$, $\ee^{\ii\alpha}\omega^2$ and $\ee^{\ii\alpha}\omega$ is negatively oriented.
The fully general case is then the addition of two arbitrarily sized and rotated standard triangles. This is a case where the interactive form of the diagram can be quite helpful.
The triangle $C$ is the average of triangles $A$ and $B$ so $C_i$ is midway between $A_i$ abd $B_i$. That is, $C$ is the triangle ${\scriptstyle\frac12}(\lambda \ee^{\ii \alpha}\chi_1 +\mu \ee^{\ii \beta}\chi_2)$.
The red sliders are $\lambda$ controlling the size of the red image of the standard triangle and $\alpha$ controlling its angle of rotation. Then the blue $\mu$ and $\beta$ are the corresponding controls for the blue image of the reversed standard triangle.
The general sum of this form, with six real parameters $\lambda,\mu,\nu,\alpha,\beta,\gamma\in \reals$, is $$ \lambda \ee^{\ii \alpha}\chi_1 +\mu \ee^{\ii \beta}\chi_2 + \nu \ee^{\ii \gamma}\chi_0 $$ and can represent any triangle in the plane; the centre of gravity is $\nu \ee^{\ii \gamma}\chi_0$.
One can spend quite some time playing with the interactive figures for polygon superpositions.
Proof of Median Coincidence
If the vertices of a triangle are $z=(z_0,z_1,z_2)$, the midpoints of the sides are $$ $$ where $I$ is the identity and $J$ is the cyclic permutation $$ J: (z_0,z_1,z_2) \mapsto (z_1,z_2,z_0) . $$ The points on the line from $z_0$ to $\sfrac12(z_2+z_1)$ are of the form, for some $\lambda \in \reals$ $$ (1\lambda)z_0 + \lambda {\textstyle\sfrac12}(z_2+z_1) $$ and similarly on the line from $z_1$ to $\sfrac12(z_0+z_2)$ we have, for some $\mu \in \reals$ $$ (1\mu)z_1 + \mu {\textstyle\sfrac12}(z_0+z_2). $$ The only solution for a point that lies on both lines is $$ (1{\textstyle\sfrac23})z_1 + {\textstyle\sfrac23}{\textstyle\sfrac12}(z_0+z_2) = {\textstyle\sfrac13}(z_0 + z_1 + z_2) = \chi_0 \Dot z. $$ The common intersection point of medians as the centre of gravity has become obvious.▓
Proof of other coincidences and collinearity
Other coincidence cases can be a bit more tricky but fundamentally proceed in a similar way. We need to show the Fourier transform coefficients of $\chi_1$ and $\chi_2$ both vanish. For collinearity we only need to show that $ \chi_1 \Dot x$ and $ \chi_2 \Dot x $ have the same absolute value.
Pentagon geometry and Jesse Douglas' pentagon construction explained
Let $\omega$ be the simplest primitive $5$th root of unity, with $\ii := \sqrt{1}$: $$ \omega = \cos\frac {2\pi}{5} + \ii \sin\frac {2\pi}{5}. $$ Note that complex conjugation acts as $\bar{\omega}_5^j = \omega_5^{5j}$.
These are the 5 standard vectors $$ \chi_0=( 1, 1, 1, 1, 1 ) \quad;\quad \chi_1=( 1, \omega_5^\strut, \omega_5^2, \omega_5^3, \omega_5^4 ) \quad;\quad \chi_2=( 1, \omega_5^2, \omega_5^4, \omega_5^\strut, \omega_5^3 ) \quad;\quad \chi_3=( 1, \omega_5^3, \omega_5^\strut, \omega_5^4, \omega_5^2 ) \quad;\quad \chi_4=( 1, \omega_5^4, \omega_5^3, \omega_5^2, \omega_5^\strut ). $$ which form a basis for $\cplx^5$.
Remark also that $$\cos\frac{2}{\pi}5 = \cos 72^\circ = \frac{1}{4} (1+\sqrt5)\simeq 0.309, \quad \sin\frac{2}{\pi} 5 =\cos 18^\circ = \frac{1}{4}\sqrt{10+2\sqrt5} \simeq 0.951 . $$ In fact, in terms of square roots, $$ \left( \begin{array}{c} 1\\ \omega_5^{\phantom{1}}\\ \omega_5^2\\ \omega_5^3\\ \omega_5^4 \end{array}\right) = \frac{1}{4} \left( \begin{array}{c} 4\\ 1+\sqrt5 + \ii \sqrt{10+2\sqrt5}\\ 1\sqrt5 + \ii \sqrt{102\sqrt5}\\ 1\sqrt5  \ii \sqrt{102\sqrt5}\\ 1+\sqrt5  \ii \sqrt{10+2\sqrt5} \end{array} \right) $$ $$= \frac{1}{4} \left\{\, \left[ \left( \begin{array}{c} 1\\ 1\\ 1\\ 1\\ 1 \end{array} \right) +\sqrt5\, \left( \begin{array}{c} \sqrt5\\ +1\\ 1\\ 1\\ +1 \end{array} \right) \,\right] + \frac{\ii}{2} \sqrt{10+2\sqrt5}\, \left[\,\, \left( \begin{array}{c} 0\\ 2\\ 1\\ 1\\ 2 \end{array} \right) +\sqrt5\, \left( \begin{array}{c} 0\\ 0\\ 1\\ 1\\ 0 \end{array} \right) \, \right]\, \right\} $$ which seems complicated enough.
Going back to examine the coordinates for $q_i$, the point obtained by extending a line from a vertex to an opposite midpoint by an extra $\frac1{\sqrt5}$, we see $$q_i = \frac{\sqrt5}5 p_i + \frac{5+\sqrt5}{10} p_{i+2}+ \frac{5+\sqrt5}{10} p_{i+3}.$$ To establish properties, see what components of the various standard types it has. The function $q=(q_0,q_1,q_2,q_3,q_4))\in{\cplx}[{\intg}/5]$ has the harmonic expansion q = \sum_{k=0}^{4} (\chi_k \Dot q) \chi_k = \sum_{k=0}^{4}\hat q_k \chi_k. $$ The character $\chi_0$ is the trivial (or degenerate) character of the trivial representation, and $\hat f_{0}$ is the center of gravity of the values of $f$. The other $\hat f_{1},\hat f_{2},\hat f_{3},\hat f_{4}$ are the harmonic components of $f$.
The center of gravity is just an expression of where the geometric object is located, so we don't expect any special properties for it. But look at $\hat q_2$; we find by calcualtion
$$ \begin{eqnarray} 5\hat {q_2}=5 \chi_2 \Dot q = 0\end{eqnarray} $$
$$ \begin{eqnarray} 5\hat {q_2} &=&5 \langle \chi_2  q\rangle \\ &=& 1\cdot q_1 + \overline{ \omega_5^{2}}\cdot q_2 + \overline{ \omega_5^{4}}\cdot q_3 + \overline{ \omega_5^{1}}\cdot q_4 + \overline{ \omega_5^{3}}\cdot q_5\\ &=& q_1 +\omega_5^{3} q_2 + \omega_5^{1} q_3 + \omega_5^{4} q_4 + \omega_5^{2} q_5\\ &=& \frac{\sqrt5}5( p_1 +\omega_5^{3} p_2 + \omega_5^{1} p_3 + \omega_5^{4} p_4 + \omega_5^{2} p_5) +\\ & & \frac{5+\sqrt5}{10}( p_3 +\omega_5^{3} p_4 + \omega_5^{1} p_5 + \omega_5^{4} p_1 + \omega_5^{2} p_2) +\\ & & \frac{5+\sqrt5}{10}( p_4 +\omega_5^{3} p_5 + \omega_5^{1} p_1 + \omega_5^{4} p_2 + \omega_5^{2} p_3)\\ &=& (\frac{\sqrt5}5\cdot1 + \frac{5+\sqrt5}{10} \omega_5^{4} + \frac{5+\sqrt5}{10} \omega_5^{1})p_1 +\\ & & (\frac{\sqrt5}5 \omega_5^{3} + \frac{5+\sqrt5}{10} \omega_5^{2} + \frac{5+\sqrt5}{10} \omega_5^{4})p_2 +\\ & & (\frac{\sqrt5}5 \omega_5^{1} + \frac{5+\sqrt5}{10} \cdot1 + \frac{5+\sqrt5}{10} \omega_5^{2})p_3 +\\ & & (\frac{\sqrt5}5 \omega_5^{4} + \frac{5+\sqrt5}{10} \omega_5^{3} + \frac{5+\sqrt5}{10} \cdot1)p_4 +\\ & & (\frac{\sqrt5}5 \omega_5^{2} + \frac{5+\sqrt5}{10} \omega_5^{1} + \frac{5+\sqrt5}{10} \omega_5^{3})p_5 . \end{eqnarray} $$
The thing to note is that the coefficients of the points $p_i$ are all multiples by powers of $\omega_5$ of the coefficient of $p_1$. Furthermore the coefficient of $p_1$ is a real number since $\overline{\omega_5^{4}} = \omega_5^{1}$. But
$$ \begin{eqnarray}  \frac{\sqrt5}5\cdot1 + \frac{5+\sqrt5}{10} \omega_5^{4} + \frac{1+\sqrt5}{2}\omega_5^{1} = \frac{\sqrt5}5 + \frac{5+\sqrt5}{10}\left(\omega_5^{4} + \omega_5^{1}\right) = 0 . \end{eqnarray} $$
$$ \begin{eqnarray}  \frac{\sqrt5}5\cdot1 + \frac{5+\sqrt5}{10} \omega_5^{4} + \frac{1+\sqrt5}{2}\omega_5^{1} &=& \frac{\sqrt5}5 + \frac{5+\sqrt5}{10}\left(\omega_5^{4} + \omega_5^{1}\right) \\ &=& \frac{\sqrt5}5 + \frac{5+\sqrt5}{10} 2 \Re{ \omega_5^{1}} \\ &=& \frac{\sqrt5}5 + \frac{(5+\sqrt5)(1+\sqrt5)}{10\times 2} \\ &=& \frac{\sqrt5}5 + \frac{5+5\sqrt5+5\sqrt5}{10\times 2} \\ &=& \frac{\sqrt5}5 + \frac{4\sqrt5}{20} = 0 . \end{eqnarray} $$
So $\hat q_2$ vanishes identically. Thus there is no regular pentagram component of the polygon $q$. Similarly look at $\hat q_3$, or at
$$ \begin{eqnarray} 5\hat { q_3} = 5\ \chi_3 \Dot q = 5\ \overline{ \overline q\Dot\chi_2} = 0 . \end{eqnarray} $$
$$ \begin{eqnarray} 5\hat { q_3} &=& 5\ \langle \chi_3  q\rangle \\ &=& 1\cdot q_1 + \overline{ \omega_5^{3}}\cdot q_2 + \overline{ \omega_5^{1}}\cdot q_3 + \overline{ \omega_5^{4}}\cdot q_4 + \overline{ \omega_5^{2}}\cdot q_5\\ &=& q_1 +\omega_5^{2} q_2 + \omega_5^{4} q_3 + \omega_5^{1} q_4 + \omega_5^{3} q_5\\ &=& 5\ \overline{\chi_2} \Dot q \\ &=& 5\ \overline{ \overline q\Dot\chi_2} \\ &=& 0 . \end{eqnarray} $$ This is because the reason that $\chi_3 \Dot q = 0$ has little to do with the properties of the $q_i$ as complex numbers, but was entirely the result of the interaction between the $5$th roots of unity, and the real coefficients in the specific makeup of the $q_i$ starting from arbitrary complex numbers $p_i$. If this is unconvincing, then a similar argument to the previous one goes through but involves the verification $$  \frac{\sqrt5}5\cdot1 + \frac{5+\sqrt5}{10} \omega_5^{1} + \frac{5+\sqrt5}{10}\omega_5^{4} = 0. $$
We have thus shown that $q = {\hat q}_0 + {\hat q}_1 \chi_1 + {\hat q}_4\chi_4={\hat q}_0 + {\hat q}_1 \chi_1 + {\hat q}_4 \overline{\chi_1}$. This means that $q$ is an affine image of the regular convex pentagon.
Similarly the polygon $r$ constructed is the affine image of a regular pentagram, for like reasons.
The pentagon $r$ has points given by $$ r_i = \frac{\sqrt5}5 p_i + \frac{5\sqrt5}{10} p_{i+2}+ \frac{5\sqrt5}{10} p_{i+3}. $$ For this case we examine correspondingly the components ${\hat r}_1$ and ${\hat r}_4$. Again we can group the coefficients of the points $p_i$, and see that they are all multiples of any one of them. For instance, the coefficient of $p_1$ is $$ \frac{\sqrt5}5\cdot1 + \frac{5\sqrt5}{10} \omega_5^{2} + \frac{5\sqrt5}{10} \omega_5^{3}= \frac{\sqrt5}5 + \frac{5\sqrt5}{10}\frac{1\sqrt5}{2} = 0, $$ just as before, up to a couple of sign changes. Also as before, we can conclude that ${\hat r}_1 = {\hat r}_4 = 0$, and say that the polygon $r$ is the affine image of a regular pentagram. ▓
Proof of Napoleon's Theorem
Again take $\omega := \omega_3^{\strut} = \frac12(1 + \ii \sqrt3)$ until further notice, so $\omega^3  1 = 0 = 1 + \omega + \omega^2.$ Start by expressing the construction steps in the Napoleon theorem with the help of the characters we introduced. We need to specify an equilateral triangle constructed positively on an oriented segment. The standard unit equilateral triangle is $\chi_{3,1}=:\chi_1$. Its righthand vertex is at the point $1\in\cplx$; we see that $\chi_1\chi_0$ is a similar triangle shifted so that its righthand vertex is at the origin. A diagram may help.
To shift it so that its first side is aligned positively along the horizontal $x$axis we multiply the whole by $(\omega1)^{1}=3^{1}(\omega^21)$ to get $3^{1}(\omega^21)(\chi_1\chi_0)$. This is clear because we want to move the vertex after the base at $0$, namely at $\omega1$, to the point $1$, and $$ (\omega 1)(\omega^21)=\omega^3\omega^2\omega+1=3. $$ Alternatively, we see immediately that $\overline{\omega1}=\omega^21$ and $\omega1=3$. The triangular building block we need is thus $$ 3^{1}(\omega^21)(\chi_1\chi_0). $$ There is an important thing to note about the constructed triangle: it is positively oriented with respect to the base interval from $0$ to $1$. It is on the left as we go from $0$ to $1$. To get the negatively oriented block on the right as we go from $0$ to $1$ we need $$ 3^{1}(\omega1)(\chi_2\chi_0). $$
In general, to translate a whole triangular figure by a vector $z$ we have to add $z\chi_0$ to it. To rotate by a angle $\alpha$ we have to multiply by the scalar turn $\ee^{\ii\alpha}$, and to scale by a homothety $\lambda > 0$ we have to multiply by the scalar $\lambda$. For instance, if we had not multiplied by $(\omega1)^{1}$ just a moment ago, but only used the rotation effected by the unit vector $\{3^{1/2}(\omega1)\}^{1}=3^{1/2}(\omega^21)$ then we would have had to scale the buildingblock triangle to unit sidelength by multiplying with $3^{1/2}$.
If the segment on which we need to erect a triangle is from $z_j$ to $z_k$, then it is of length $z_kz_j$ and in the direction $\arg(z_kz_j)$ from the starting point $z_j$. Thus the triangle on the left side of the interval which is to be constructed is $$ 3^{1}(\omega^21)(z_kz_j)(\chi_1\chi_0) + z_j\chi_0, $$ and the triangle on the right side is $$ 3^{1}(\omega1)(z_kz_j)(\chi_2\chi_0) + z_j\chi_0. $$
Finally, to find the centroid of a triangle $z=(z_0,z_1,z_2)$ we just have to take the inner product with $\chi_0$, namely $\chi_0 \Dot z$. So the centroid of the leftside resulting triangle in the last paragraph is, using the fact that the basis vectors $\chi_j$ are orthonormal, \begin{eqnarray*} \chi_0 \Dot( 3^{1}(\omega^21)(z_kz_j)(\chi_1\chi_0) + z_j\chi_0) &=& 3^{1}(\omega^21)(z_kz_j) + z_j\\ &=& 3^{1}\{(\omega^21)z_k(\omega^21)z_j3z_j\}\\ &=& 3^{1}\{(\omega^21)z_k(\omega^2+2)z_j\} . \end{eqnarray*}
Theorem 1 (Napoleon) For any nondegenerate triangle in the plane the result of constructing the centroids of equilateral triangles erected externally on the sides of the triangle is three points at the vertices of an equilateral triangle.
Proof. Let the initial triangle be $z=(z_0,z_1,z_2)$, and suppose it positively oriented. Start with externally constructed equilateral triangles. That means we need rightside building blocks. By the above remarks the externally constructed vertices are $$ ( 3^{1}\{(\omega1)z_{j+1}(\omega+2)z_j\} , j\in \{0,1,2\}), $$ so the triangle is $$3 ^{1}\{(1\omega)J z+ (\omega+2)z\}. $$ To show that this is an equilateral triangle we take the inner product with $\chi_2$. We know that the original triangle has its Fourier decomposition $z=\hat z_0\chi_0+\hat z_1\chi_1+\hat z_2\chi_2$, and the basis $(\chi_j,j\in\{0,1,2\})$ is orthonormal. Now we see quickly that the $\chi_j$ are eigenvectors of $J$, namely $J\chi_j = \omega^j\chi_J$. Therefore $Jz=\hat z_0\chi_0+\omega \hat z_1\chi_1+\omega^2 \hat z_2\chi_2$. Thus \begin{eqnarray*} \langle\chi_2\Dot3^{1}\{(1\omega)J z+ (\omega+2)z\}\rangle &=&3^{1}\{(1\omega)\omega^2 \hat z_2+ (\omega+2)\hat z_2\}\\ &=&3^{1}\{\omega^21+\omega +2\}\hat z_2 \\ &=&3^{1}\{\omega^2+\omega +1\}\hat z_2 \\ &=& 0. \end{eqnarray*} We have shown that constructing the centroids of equilateral triangles externally to the positively oriented initial triangle yields a sequence of points making up the vertices of a positively oriented equilateral triangle.
To deal with lefthand side, i.e. , ‘internal’ equilateral triangles, we just have to do a similar calculation.
Since we may suspect that the resulting vertices will have the reverse orientation we will take the inner product with $\chi_1$. As suspected, they are the vertices of a reverse equilateral triangle. ▓
Since we may suspect that the resulting vertices will have the reverse orientation we will take the inner product with $\chi_1$. By remarks above the internally constructed vertices are $$ ( 3^{1}\{(\omega^21)z_{j+1}(\omega^2+2)z_j\} , j\in 0..2), $$ so the triangle is $$ 3^{1}\{(1\omega^2)J z+ (\omega^2+2)z\}. $$ Thus \begin{eqnarray*} \langle\chi_13^{1}\{(1\omega^2)J z+ (\omega^2+2)z\}\rangle &=&3^{1}\{(1\omega^2)\omega \hat z_1+ (\omega^2+2)\hat z_1\}\\ &=&3^{1}\{\omega1+\omega^2 +2\}\hat z_1 \\ &=& 0, \end{eqnarray*} as suspected. We have the vertices of a reverse equilateral triangle. ▓
Corollary The Napoleon construction provides a geometrical way to find the discrete Fourier transform of a triangle.
Proof. First for the external triangles \begin{eqnarray*} \chi_1\Dot(3^{1}\{(1\omega)J z+ (\omega+2)z\}) &=&3^{1}\{(1\omega)\omega \hat z_1+ (\omega+2)\hat z_1\}\\ &=&3^{1}\{\omega\omega^2 +\omega +2\}\hat z_1 \\ &=&3^{1}\{\omega^2+2\omega +2\}\hat z_1 \\ &=&3^{1}\{3\omega^2\}\hat z_1\\ &=& \omega^2 \hat z_1, \end{eqnarray*} and \begin{eqnarray*} \langle\chi_03^{1}\{(1\omega)J z+ (\omega+2)z\}\rangle &=&3^{1}\{(1\omega) \hat z_0+ (\omega+2)\hat z_0\}\\ &=&\hat z_0 \end{eqnarray*} (which last we really already knew). Geometrically this means that the external Napoleon triangle has equal sides of lengths $\sqrt3\hat z_1$, and if we want to work out the argument of $\hat z_1$ then all we have to do is to rotate the first side of it back by $2\pi/3$ and flip.
From the internal Napoleon triangle we get similarly \begin{eqnarray*} \langle\chi_23^{1}\{(1\omega^2)J z+ (\omega^2+2)z\}\rangle &=&3^{1}\{(1\omega^2)\omega^2 \hat z_2+ (\omega^2+2)\hat z_2\}\\ &=&3^{1}\{\omega^2\omega +\omega^2 +2\}\hat z_2 \\ &=& \omega \hat z_2, \end{eqnarray*} giving us the value for $\hat z_2$. ▓
A generalization of this results from noticing that one could just as well use $N$ as $3$ above for the number of sides, $\chi_{N,k}$ for the initial $N$gon and some other $\chi_{N,l}$gon for the constructed figure on each side and still get the same results with careful manipulation of the indices. It is probably helpful to remark that the $N=4$ case says that constructing squares on the sides of a parallelogram gives four centers of gravity which are the vertices of a square, before the general formulation that follows. Let this theorem indicate that one can go a lot further with these methods.
Theorem 2 (Generalized Napoleon) Let $N$ be an integer greater than $2$, and $k$ and $l$ be integers between $1$ and $N1$. For any nondegenerate affine image of a regular $(N,k)$gon in the plane, the result of constructing the centroids of regular $(N,l)$gons externally upon the sides of the initial $(N,k)$gon is the set of vertices of a regular $(N,k)$gon if $k^2=l \pmod N$; if the additional figures are constructed internally then a regular $(N,Nk)$gon results.
Summary
We have seen that there's a relationship between some elementary geometry of the plane and the Discrete Fourier Transform: Assertions of triangle geometry are statements about the harmonics that remain after a prescribed construction, and Napoleon's Theorem gives a geometrical way of constructing a Discrete Fourier Transform of order $3$. This is just a suggestion of some ramifications of this which include relationships to polynomials, circulant matrices, interpolation and splines, Siebeck's and Marden's theorems on polynomial zeroes, and the HeisenbergWeyl group as it occurs in signal processing.
Acknowledgements
I would like to thank Bill Casselman and David Austin for many improvements to the exposition, Davide Cervone and Robert Miner for the excellent tool MathJax, and Markus Hohenwarter and his team for the valuable Geogebra package. Mathematical Reviews and the University of Michigan have provided unparalleled access to the literature of mathematics.
References

Douglas, Jesse

Geometry of polygons in the complex plane. J. Math. Phys. Mass. Inst. Tech. 19 (1940), 93.130. MR 0001574 (1,261f)

On linear polygon transformations. Bull. Amer. Math. Soc. 46 (1940), 551.560. MR 0002178 (2,9i)

A theorem on skew pentagons. Scripta Math. 25 1960 5.9. MR 0117643 (22 #8419)
The early papers on the whole approach to geometry through the Discrete Fourier Transform are items 1 and 2. The third introduces the pentagon construction discussed above, and is dedicated to a longtime colleague geometer, Jekuthiel Ginsburg. Douglas was awarded one of the first two Fields medals in 1936.

Schoenberg, I. J.

The finite Fourier series and elementary geometry. Amer. Math. Monthly 57 (1950), 390.404. MR 0036332 (12,92f)

Mathematical time exposures. Mathematical Association of America, Washington, DC, 1982. ix+270 pp. ISBN: 0883854384. MR 0711022 (85b:00001)

The harmonic analysis of skew polygons as a source of outdoor sculptures. The geometric vein, pp. 165.176, Springer, New YorkBerlin, 1981. MR 0661776 (84d:52011)
Article 1 discusses these matters very clearly, as do several chapters in the book 2. Schoenberg actually did make a sculpture based on Douglas's construction described in 3.

Andreescu, Titu; Andrica, Dorin, Complex numbers from A to... Z. Translated and revised from the 2001 Romanian original. Birkh.user Boston, Inc., Boston, MA, 2006. xiv+321 pp. ISBN: 9780817643263; 0817643265. MR 2168182
An introductory text using complex coordinate methods with an eye toward mathematical Olympiad problems.

Web sites:
Cut the Knot: Interactive Mathematics Miscellany and Puzzles, http://www.cuttheknot.org/
An excellent source for interactive geometry and, in particular, proofs of Morley's theorem.

http://wwwpersonal.umich.edu/~pion/WebGeom/
The author's personal site where more related material is to be posted.