amiras, now you need to explain the 1/12th for moment around center.
destroyer, imagine I replace the rod by N+1 point masses located at distance r
n=n(R/N) from the end, where n runs from 0 to N. The mass of each is m=M/(N+1), of course, to give you total mass of M. Moment of inertia for a point mass is mr
n². So we need to add these up.
[tex]I = \sum_{n=0}^{N} m r_n^2 = \frac{m R^2}{N^2} \sum_{n=0}^{N} n^2[/tex]
Sum of squares of consecutive integers is known as
square pyramidal number.
[tex]\sum_{n=0}^{N} n^2 = \frac{2N^3 + 3N^2 + N}{6}[/tex]
Putting it all together.
[tex]I = MR^2 \frac{2N^3 + 3N^2 + N}{6 N^2 (N+1)}[/tex]
That looks ugly, but if N is large enough, only the N³ terms are important in that fraction. Since we want the rod to be broken into infinitely many point masses, the square and linear terms can be dropped. (In other words, take limit as N goes to infinity.)
[tex]I = MR^2 \frac{2N^3}{6N^3} = \frac{1}{3}MR^2[/tex]
This isn't the cleanest way to derive moment of inertia, and it gets even worse for more complex shapes, but it shows where the 1/3 comes from without any advanced mathematics.