Parallel-Axis Theorem

The moment of inertia is minimal when the rotation axis passes through the center-of-mass and increases as the rotation axis is moved further from the center-of-mass.

I = Icm + Mh2

Here M is the mass, h is the distance from the center-of-mass to the parallel axis of rotation, and Icm is the moment of inertia about the center of mass parallel to the current axis.

Example:

What is the moment of inertia Icm for a uniform rod of length L and mass M rotating about an axis through the center, perpendicular to the rod?

I = Icm + Mh2   →   Icm = I - Mh2

Now the moment of inertia about the end of the rod is:   I = ML2/3.

The distance from the end of the rod to the center is h = L/2. Therefore:

Icm   = 
1
3
ML2   -   M (
L
2
) 2   = 
1
3
ML2  -  
1
4
ML2  = 
1
12
ML2