One of my friends recently posed the problem of finding the expected number of uniform random variables needed to get a sum greater than $1$ without using calculus.
Even though I've seen this problem before, I was not able to recollect it and the calculus proof was all I could come up with until he eventually showed the me the solution. But this time, something different struck me.
The solution to this problem uses that fact that
$\displaystyle \mathbb{P}(N>n)=\frac{1}{n!}$
where $N$ is the random variable indicating the number of Uniform random variables needed. But given this, we could do more than the expected value. We know that,
$\displaystyle \mathbb{E}(N)=\sum_{n=0}^\infty\mathbb{P}(N>n)=\sum_{n=0}^\infty \frac{1}{n!}=e$
which follows from the definition of Euler's number.
But suppose, we don't know the exact value of $e$. With elementary methods, we can show that $2<e<3$.
In the problem that we were discussing, we can use the expression for probability to find $\mathbb{V}(N)$ as well. We know that
$\displaystyle \mathbb{E}(N^2)=\sum_{n=0}^\infty(2n+1)\mathbb{P}(N>n)=\sum_{n=0}^\infty \frac{2n+1}{n!}=3e$
Therefore, $\mathbb{V}(N)=\mathbb{E}(N^2)-\mathbb{E}(n)=e(e-3)$
As variance of any random variable $\geq 0$ and we know that $e>0$, this shows us that $e<3$ which is something we already know. But this gives us a nice idea.
Let $N_{(2)}$ be the random variable denoting the number of Uniform random variables needed to get a sum a sum greater than $2$. Uniform Sum Distribution shows us that,
$\displaystyle \mathbb{P}(N_{(2)}=n)=\frac{(n-2)(2^{n-1}-n)}{n!}$
With this, we can see that
$\displaystyle \mathbb{E}(N_{(2)})=e(e-1)$ and $\displaystyle \mathbb{E}(N_{(2)}^2)=5e(e-1)$
Therefore, $\displaystyle \mathbb{V}(N_{(2)})=e(e-1)(5-e^2+e)$
Using the same idea as before, we see that $5-e^2+e>0$ which shows us
$\displaystyle \frac{1}{2}(1-\sqrt{21}) \leq e \leq \frac{1}{2}(1+\sqrt{21})$
Numerically, this shows that $e \leq 2.791288$!!
As you may have already guessed, this could be extended for higher moments and / or sum-greater-than-3 and so on. But the resulting expressions gives higher degree polynomials which, even though gives better estimates for $e$, cannot be easily solved in closed form. For example, using
$\displaystyle \mathbb{E}(N_{(3)})=\frac{1}{2}(2e^3-4e^2+e)$ and $\displaystyle \mathbb{E}(N_{(3)}^2)=\frac{7}{2}(2e^3-4e^2+e)$
Solving the resulting expression for variance, we get to see that $2e^3-4e^2+e-14 \leq 0$. Solving this with WA, we see that
$\displaystyle e < \frac{1}{6}(4+\sqrt[3]{784+18\sqrt{1894}}+\sqrt[3]{784-18\sqrt{1894}}) \approx 2.74615$
Hope you enjoyed this. See ya soon.
Until then, Yours Aye
Me