Are these two facts related? I was told some days ago that the possibility of two randomly picked numbers are relatively prime to each other is $6/(\pi^2)$. And it is well known that the value of Riemann zeta function at 2 is $(\pi^2)/6$.
So I guess there is a correspondence between them. Maybe the possibility of $n$ randomly picked numbers are relatively prime to each other(there are two cases here:
(1)these $n$ numbers are pairly relatively prime to each other
(2)the common divisor of all of these $n$ numbers is 1) equals $1/\zeta (n)$?
And I think when we consider $n=1$, the possibility of one randomly picked number is prime is 0, and meanwhile $\zeta(1)=\infty$. So in this case with this sense this proposition still holds.
But I think I must be daydreaming... 
Please let me know if you find the formula above is wrong for some $n$.
 A: Pick two random numbers less than $n$, then  


*

*$\lfloor n/2\rfloor^2$ pairs are both divisible by 2. 

*$\lfloor n/3\rfloor^2$ pairs are both divisible by 3. 

*$\lfloor n/5\rfloor^2$ pairs are both divisible by 5. 
... 


The number of relatively prime pairs less than or equal to $n$ is: 
$$    n^2 - \sum\lfloor \frac np\rfloor^2 +  \sum\lfloor \frac n{pq}\rfloor^2-  \sum\lfloor \frac n{pqr}\rfloor^2 + ...  $$
Sums are taken over the distinct primes $p,q,r,...$ less than n. Let $\mu(x)$ be the Möbius function this is 
$$\sum\mu(k)\lfloor n/k\rfloor^2$$ 
The probability is the limit as $n$ goes to infinity divided by $n^2$, or 
$$    \sum\frac{\mu(k)}{k^2} .$$
Now, the Dirichlet series that generates the Möbius function is the (multiplicative) inverse of the Riemann zeta function
$$
    \sum_{n=1}^\infty \frac{\mu(n)}{n^s}=\frac{1}{\zeta(s)}. $$
So we get $\frac{1}{\zeta(2)}=\frac6{\pi^2}$.
MathWork says:

This result is related to the fact that the greatest common divisor of $m$ and $n$, $(m,n)=k$, can be interpreted as the number of lattice points in the plane which lie on the straight line connecting the vectors $(0,0)$ and $(m,n)$ (excluding $(m,n)$ itself). In fact, $6/\pi^2$ is the fractional number of lattice points visible from the origin (Castellanos 1988, pp. 155-156). 

