Let M n be the arithmetic mean of the lengths of all the diagonals of the regular n -gon with a circumradius of π .
Compute n → ∞ lim M n .
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For completeness, the first sentence should be clarified. I agree with your analysis for the odd ( 2 n + 1 ) case.
However, in the even case, each diameter occurs n times while every other diagonal occurs 2 n − 3 times. Hence, we still have to explain if/how this "under counting of the largest line" affects the final limit.
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 , we need to find the intersection of y = x tan θ and ( y − 1 ) 2 + x 2 = 1 . This occurs at x = sin 2 θ . 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 ∣ .
Thus the average length of a chord is
π 1 ∫ 0 π ∣ 2 sin θ ∣ d θ = 4 / π .
Scaling up by π we see the average chord length is 4.
(Credit to @Jake Lai.)
Let w = e 2 π 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 , where R is the circumradius and 0 ≤ k ≤ n − 1 with k ∈ Z . First let's find the sum of the lengths of all the diagonals from 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 ( n π k ) ∣ ∣ ∣ ∣ = 2 R k = 2 ∑ n − 2 sin ( n π k ) Now we have to multiply that by n to count all the diagonals from all vertices, but we have counted twice every diagonal, so the sum (say S ) of the length of every diagonal is then: S = n R k = 2 ∑ n − 2 sin ( n π k ) . Using the formula for the sum of sines of angles in A.P. we get: S = sin ( 2 n π ) n R cos ( 2 n 3 π ) .
We know that there are n ( n − 3 ) / 2 diagonals, so M n = n ( n − 3 ) / 2 S = ( n − 3 ) sin ( 2 n π ) 2 R cos ( 2 n 3 π ) .
Finally, L = n → ∞ lim M n = ( n → ∞ lim n − 3 2 R ) ⋅ n → ∞ lim sin ( 2 n π ) n → ∞ lim cos ( 2 n 3 π ) = ( n → ∞ lim n − 3 2 R ) ⋅ 2 n π 1 = n → ∞ lim π ( n − 3 ) 4 n R = π 4 R .
But R = π , so L = 4 .
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Observe that the mean of the lengths of all the diagonals of the n -gon is equal to the mean of the lengths of only the diagonals that are incident to a particular vertex of the n -gon.
The diagonals of the n -gon can be imagined as chords of its circumcircle, whose radius is π .
The length of a chord with a subtended angle θ and radius r is given by 2 r sin 2 θ . (see the figure below)
http://mathcentral.uregina.ca/QQ/database/QQ.09.05/bes1.html
The lengths of the n − 3 diagonals of the n -gon incident to one vertex are 2 π sin 2 n 2 π k = 2 π sin n π k for integers k ∈ [ 2 , n − 2 ] . Further, the mean of these lengths is n − 3 1 k = 2 ∑ n − 2 2 π sin n π k .
The limit of this expression is n → ∞ lim 2 π k = 2 ∑ n − 2 n − 3 1 sin n π k
= 2 π n → ∞ lim k = 0 ∑ n n 1 sin n π k
Notice that I can extend the index to ( 0 , n ) because lim n → ∞ n 1 sin n π m = 0 for all m ∈ { 0 , 1 , n − 2 , n − 1 } . I also replaced n − 3 with n because ( n − 3 ) ∼ 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
= 2 π ⋅ π 1 ⋅ − ( cos π − cos 0 ) ) = 4