suppose we have the classic problem of buffon's needle , let $\ell$ be the length of the needle and $d$ the distance between the parallel lines . I have solved the case which $\ell \leq d$ and i understand why $P(\text{needle cross the line})= \frac{2\ell}{\pi d}$. I know this doesn't work for $\ell>d$ because we can have the last probability $> 1$ for $\ell>\frac{\pi d}{2}$. But i cannot understand what doesn't work geometrically.
2025-04-22 06:03:01.1745301781
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Buffon needle problem , scenario $\ell>d$
1.1k Views Asked by chaviaras michalis https://math.techqa.club/user/chaviaras-michalis/detail At
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One way you can think about this is in terms of the Buffon's noodle variant of the problem.
It turns out that the integral you wrote down for the $\ell < d$ case is always meaningful, no matter how big $\ell$ gets! It just doesn't always give the probability of a crossing. What it does give is the expected number of crossings.
When $\ell < d$, the only possible numbers of crossings are zero and one. So the expected number of crossings is equal to the probability. But when $\ell \geq d$, a single needle may cross more than one line, which means they need not be equal any more (as in fact they are not when $\ell > d$). So you need a more careful case analysis, such as the one given in the other answer.
This is not a full answer, but only an explanation of the integral appearing in the wikipedia article referenced above.
The integral must be slipt in two : $$p= \frac{4}{t\pi}\int_{\theta=0}^{\pi/2} \int_{x=0}^{m(\theta}dx\:d\theta$$
$$p= \frac{4}{t\pi}\int_{\theta=0}^{\pi/2} \int_{x=0}^{ \frac{l}{2} \sin^{-1}(t/l)}\sin(\theta)dx\:d\theta + \frac{4}{t\pi}\int_{\theta=0}^{\pi/2} \int_{x=\frac{l}{2}\sin^{-1}(t/l)}^{t/2}dx\:d\theta $$
$$p=\frac{2l}{t\pi}\left[-\cos(\theta)\right]_{0}^{\sin^{-1}(t/l)} +\frac{2}{\pi}\left(\frac{\pi}{2}-\sin^{-1}(t/l)\right)$$
$$p=\frac{2l}{t\pi}\left(1-\sqrt{1-\frac{t^2}{l^2}}\right) +1-\frac{2}{\pi}\sin^{-1}\left(\frac{t}{l}\right)$$