Moment of inertia is a measure of how strongly a body resists angular acceleration about a specified axis. It depends on both the body’s mass and how that mass is distributed relative to the axis of rotation.
This is an HL-only concept in A.4 Rigid body mechanics. For a system of point masses, moment of inertia is
where is each point mass and is its perpendicular distance from the axis. Its SI unit is .
Moment of inertia is often described as the rotational analogue of mass. However, unlike mass, it is not fixed for a body because choosing a different axis changes the distances of its particles from that axis.
The squared distance is crucial: moving mass farther from the axis increases substantially. Newton’s second law for rotation is
so, for the same resultant torque , a larger produces a smaller angular acceleration .
| Factor | Effect on moment of inertia |
|---|---|
| Total mass increases without changing its distribution | increases proportionally |
| Mass moves farther from the axis | increases according to |
| Axis of rotation changes | usually changes because the distances change |
For example, two point masses of are each from an axis:
If both are moved to , then
Doubling the distance makes the moment of inertia four times larger. This fourfold increase means that the same torque would produce only one-quarter of the original angular acceleration, since .
A common misconception is that moment of inertia is a property of the body alone. It is a property of the body and the chosen axis.
In an IB exam, identify the axis first, use perpendicular distances, and show each term in . For explanation questions, link greater mass distribution away from the axis to larger and therefore smaller for a fixed torque.
