Signs and Wonders in Experimental Mathematics :)

Signs and Wonders in Experimental Mathematics :)

Buffon’s Needle experiment, proposed by 18th-century mathematician Georges-Louis Leclerc, also known as the Count of Buffon, is a renowned thought experiment that reveals an unexpected link between randomness and the mathematical constant \pi.

The setup is simple: imagine a floor with equally spaced parallel lines and a needle whose length is equal to or less than the distance between these lines. When you drop the needle, it may land crossing a line or completely between the lines. By dropping the needle repeatedly and counting how often it crosses a line, you can approximate the value of π. The percentage of a crossing event is linked to \pi through a specific formula, and, remarkably, the more times you repeat the experiment, the closer your calculated value will approach \pi.

Fig. 1

Suppose a needle of length L is dropped at random onto a floor with parallel lines spaced a distance D apart. Let \theta represent the angle between the needle and the lines on the floor, and let y be the distance between the midpoint of the needle and the nearest line. For the needle to cross a line when L \le D, the following condition must hold:

\displaystyle y \le \frac{L}{2} \sin(\theta)\quad\quad\quad(*)

Due to symmetry, the constrains are 0 \le \theta \le \frac{\pi}{2} and 0 \le y \le \frac{D}{2}.

Fig. 2

Tossing a needle is equivalent to selecting a point within the rectangle shown in Fig. 2. When the needle crosses a line, by (*), the point falls under the curve y = \frac{L}{2}\sin(\theta).

Since the number of randomly chosen points within a region is approximately proportional to its area, select at random n points within the rectangle and let n_s represents the number of points that fall under the curve, we have

\displaystyle \frac{n_s}{n} \approx \frac{\text{area under } y = \frac{L}{2}\sin(\theta)}{\text{area of the rectangle}}

That is,

\displaystyle \frac{n_s}{n} \approx \frac{\int\limits_{0}^{\frac{\pi}{2}}\frac{L}{2}\sin(\theta) \; d\theta}{\frac{D}{2}\cdot\frac{\pi}{2}} = \frac{2 L}{\pi D}

Thus,

\displaystyle \frac{n_s}{n} \approx \frac{2 L}{\pi D}

which leads to an approximation for \pi as:

\displaystyle \pi \approx 2 \cdot \frac{L}{D} \cdot \frac{n}{n_s}

An actual experiment was carried out by a diligent Italian mathematician, Mario Lazzarini, who made 3408 needle tosses and recorded that 1808 of them intersected a boundary line. This experiment, documented in Periodico di Matematica per l’insegnamento secondario, Vol. 17 (1901), produced an approximation for \pi:

\displaystyle 2 \times \frac{2.5}{3}\times\frac{3408}{1808}

This value is accurate to six decimal places!

Excerpts from Lazzarini’s “Un’applicazione del calcolo della probabilita”

Inspired by Mario’s groundbreaking result, I recently embarked on conducting my own version of the experiment. To my delight, the outcomes were nothing short of a wonder:

Total n Intersected n_s 2 \cdot \frac{L}{D}\cdot\frac{n}{n_s}
198 105 3.142857142857143
2997 1590 3.141509433962264
3195 1695 3.141592920353983
311979 165510 3.141592653011902

L = 2.5, D = 3


Exercise-1 Explain:

Exercise-2 Explain:

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