Mean Diagonals

Calculus Level 2

Diagonals of a regular 30-gon Diagonals of a regular 30-gon

Let M n M_n be the arithmetic mean of the lengths of all the diagonals of the regular n n -gon with a circumradius of π \pi .

Compute lim n M n \displaystyle \lim_{n \to \infty} M_n .


Image Credit: Graeme McRae .


The answer is 4.

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3 solutions

Kerry Soderdahl
Sep 11, 2016

Observe that the mean of the lengths of all the diagonals of the n n -gon is equal to the mean of the lengths of only the diagonals that are incident to a particular vertex of the n n -gon.

The diagonals of the n n -gon can be imagined as chords of its circumcircle, whose radius is π \pi .

The length of a chord with a subtended angle θ \theta and radius r r is given by 2 r sin θ 2 2r\sin{\frac{\theta}{2}} . (see the figure below)

[http://mathcentral.uregina.ca/QQ/database/QQ.09.05/bes1.html](http://mathcentral.uregina.ca/QQ/database/QQ.09.05/bes1.html) http://mathcentral.uregina.ca/QQ/database/QQ.09.05/bes1.html

The lengths of the n 3 n-3 diagonals of the n n -gon incident to one vertex are 2 π sin 2 π k 2 n = 2 π sin π k n 2\pi\sin{\frac{2\pi k}{2n}} = 2\pi\sin{\frac{\pi k}{n}} for integers k [ 2 , n 2 ] k \in [2,n-2] . Further, the mean of these lengths is 1 n 3 k = 2 n 2 2 π sin π k n \displaystyle\frac{1}{n-3}\sum_{k=2}^{n-2}2\pi\sin{\frac{\pi k}{n}} .

The limit of this expression is lim n 2 π k = 2 n 2 1 n 3 sin π k n \lim_{n \to \infty} 2\pi \sum_{k=2}^{n-2} \frac{1}{n-3} \sin{\frac{\pi k}{n}}

= 2 π lim n k = 0 n 1 n sin π k n =2\pi\lim_{n\to\infty}\sum_{k=0}^{n}\frac{1}{n}\sin{\frac{\pi k}{n}}

Notice that I can extend the index to ( 0 , n ) (0,n) because lim n 1 n sin π m n = 0 \lim_{n\to\infty}\frac{1}{n}\sin{\frac{\pi m}{n}} = 0 for all m { 0 , 1 , n 2 , n 1 } m \in \{0,1,n-2,n-1\} . I also replaced n 3 n-3 with n n because ( n 3 ) n (n-3) \sim n .

By definition as the limit of a Riemann sum , the limit is equal to the definite integral 2 π 0 1 sin π x d x \displaystyle 2\pi\int_{0}^{1}\sin{\pi x}\ dx

= 2 π 1 π ( cos π cos 0 ) ) = 4 = 2\pi\cdot\frac{1}{\pi}\cdot -\left(\cos{\pi} - \cos{0)}\right) = \boxed{4}

For completeness, the first sentence should be clarified. I agree with your analysis for the odd ( 2 n + 1 ) (2n+1) case.

However, in the even case, each diameter occurs n n times while every other diagonal occurs 2 n 3 2n-3 times. Hence, we still have to explain if/how this "under counting of the largest line" affects the final limit.

Calvin Lin Staff - 4 years, 9 months ago
Jordan Soh
Sep 27, 2016

Motivation: The problem is equivalent to finding the average chord length in a circle. We focus on a single point on the circle, specifically (as we will see) the origin.

Take the circle with radius 1 centered at (0,1), C. Parametrising C in terms of θ \theta , we need to find the intersection of y = x tan θ y = x\tan \theta and ( y 1 ) 2 + x 2 = 1 (y-1)^2 + x^2 = 1 . This occurs at x = sin 2 θ x = \sin 2\theta . Hence the length of the chord from the origin to a point on C is x 2 + y 2 = 2 y = 2 tan θ sin 2 θ = 2 sin θ \sqrt{x^2 + y^2} = \sqrt{2y} = \sqrt{2\tan\theta \sin 2\theta} = |2\sin \theta| .

Thus the average length of a chord is

1 π 0 π 2 sin θ d θ = 4 / π . \frac{1}{\pi} \int_0^\pi |2\sin \theta| \ d\theta = 4/\pi.

Scaling up by π \pi we see the average chord length is 4.

(Credit to @Jake Lai.)

Let w = e 2 π i / n w=e^{2\pi i/n} be a n-th primitive root of unity. Then, the vertices of the n-gon in the complex plane are given by P k = R w k P_k=Rw^k , where R R is the circumradius and 0 k n 1 0 \leq k \leq n-1 with k Z k \in \mathbb{Z} . First let's find the sum of the lengths of all the diagonals from P 0 P_0 to the other vertices: k = 2 n 2 P 0 P k = R k = 2 n 2 w k 1 = 2 R k = 2 n 2 sin ( π k n ) = 2 R k = 2 n 2 sin ( π k n ) \sum_{k=2}^{n-2} \overline{P_0 P_k}=R\sum_{k=2}^{n-2} \lvert w^k-1 \rvert=2R\sum_{k=2}^{n-2} \left\lvert \sin\left(\dfrac{\pi k}{n}\right) \right\rvert=2R\sum_{k=2}^{n-2} \sin\left(\dfrac{\pi k}{n}\right) Now we have to multiply that by n n to count all the diagonals from all vertices, but we have counted twice every diagonal, so the sum (say S S ) of the length of every diagonal is then: S = n R k = 2 n 2 sin ( π k n ) \displaystyle S=nR\sum_{k=2}^{n-2} \sin\left(\dfrac{\pi k}{n}\right) . Using the formula for the sum of sines of angles in A.P. we get: S = n R cos ( 3 π 2 n ) sin ( π 2 n ) S=\dfrac{nR\cos\left(\dfrac{3\pi}{2n}\right)}{\sin\left(\dfrac{\pi}{2n}\right)} .

We know that there are n ( n 3 ) / 2 n(n-3)/2 diagonals, so M n = S n ( n 3 ) / 2 = 2 R cos ( 3 π 2 n ) ( n 3 ) sin ( π 2 n ) M_n=\dfrac{S}{n(n-3)/2}=\dfrac{2R\cos\left(\dfrac{3\pi}{2n}\right)}{(n-3)\sin\left(\dfrac{\pi}{2n}\right)} .

Finally, L = lim n M n = ( lim n 2 R n 3 ) lim n cos ( 3 π 2 n ) lim n sin ( π 2 n ) = ( lim n 2 R n 3 ) 1 π 2 n = lim n 4 n R π ( n 3 ) = 4 R π L=\displaystyle \lim_{n \to \infty} M_n=\left(\displaystyle \lim_{n \to \infty} \dfrac{2R}{n-3}\right) \cdot \dfrac{\displaystyle \lim_{n \to \infty} \cos\left(\dfrac{3\pi}{2n}\right)}{\displaystyle \lim_{n \to \infty} \sin\left(\dfrac{\pi}{2n}\right)}=\left(\displaystyle \lim_{n \to \infty} \dfrac{2R}{n-3}\right) \cdot \dfrac{1}{\frac{\pi}{2n}}=\displaystyle \lim_{n \to \infty} \dfrac{4nR}{\pi(n-3)}=\dfrac{4R}{\pi} .

But R = π R=\pi , so L = 4 L=\boxed{4} .

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