TLDR; Geomtric way of representing a derivation of Viete's formula for pi that involves nested square roots of two
Let ( R = 2^n ) for some positive integer ( n ). Consider a circle of radius ( R ) centered at the origin. Divide the circle into ( 2R ) equal slices. The ( y )-coordinate of the first slice's intersection point above the ( x )-axis approaches ( \pi ) as ( n \rightarrow \infty ).
- Define ( R = 2^n ) where ( n ) is a positive integer.
- Consider a circle of radius ( R ) centered at the origin.
- Divide the circle into ( 2R ) equal slices.
- The angle for each slice is ( \theta = \frac{2\pi}{2R} = \frac{\pi}{R} ).
The ( y )-coordinate for the first slice's intersection point above the ( x )-axis in Cartesian coordinates is ( y = R \sin(\theta) ). Substituting ( \theta = \frac{\pi}{R} ) and ( R = 2^n ), we get ( y = 2^n \sin\left(\frac{\pi}{2^n}\right) ). -
We want to find ( \lim_{n \to \infty} 2^n \sin\left(\frac{\pi}{2^n}\right) ). -
Substitute ( u = \frac{\pi}{2^n} ) and ( 2^n = \frac{\pi}{u} ), so ( u \to 0 ) as ( n \to \infty ). The limit becomes ( \lim_{u \to 0} \frac{\pi}{u} \sin(u) ). Utilizing the limit identity ( \lim_{u \to 0} \frac{\sin(u)}{u} = 1 ), the limit is ( \pi ). -
Conclusion:
- Therefore, the ( y )-coordinate of the first slice's intersection point above the ( x )-axis approaches ( \pi ) as ( n \rightarrow \infty ).
Let ( R = 2^n ) for some positive integer ( n ). Consider a circle of radius ( R ) centered at the origin and divide it into ( 2R ) equal slices. The ( y )-coordinate of the ( k )-th slice's intersection point above the ( x )-axis approaches ( k\pi ) as ( n \rightarrow \infty ).
- Define ( R = 2^n ) where ( n ) is a positive integer.
- Consider a circle of radius ( R ) centered at the origin.
- Divide the circle into ( 2R ) equal slices.
- The angle for the ( k )-th slice is ( \theta_k = k \left( \frac{2\pi}{2R} \right) = k \left( \frac{\pi}{R} \right) ).
The ( y )-coordinate for the ( k )-th slice's intersection point above the ( x )-axis in Cartesian coordinates is ( y_k = R \sin(\theta_k) ).
Substituting ( \theta_k = k \frac{\pi}{R} ) and ( R = 2^n ), we get: [ y_k = 2^n \sin\left(k \frac{\pi}{2^n}\right) ]
We want to find ( \lim_{n \to \infty} 2^n \sin\left(k \frac{\pi}{2^n}\right) ).
Substitute ( u = k \frac{\pi}{2^n} ) and ( 2^n = \frac{k \pi}{u} ), so ( u \to 0 ) as ( n \to \infty ).
The limit becomes ( \lim_{u \to 0} \frac{k \pi}{u} \sin(u) ).
Utilizing the limit identity ( \lim_{u \to 0} \frac{\sin(u)}{u} = 1 ), the limit is ( k \pi ).
Therefore, as ( n \rightarrow \infty ), the ( y )-coordinate of the ( k )-th intersection point will approach ( k \pi ).
- Visualizations:
Each of these horizontal lines approaches a multiple of pi as R goes to infinity
As R increases, each 2nd node y coordinate moves towards 2pi, 3rd node 3pi, etc. How each point converges to these multiples of pi creates some extremely interesting fractals which are worthy of future research