Moment of Inertia

Mass distribution and resistance to change in rotational state. Covers: Definition of the Moment of Inertia and Standard Moments of Inertia.

General idea of the topic

The moment of inertia measures a body's resistance to changes in its angular velocity. It depends on the mass and also on how it is distributed relative to the axis: each particle contributes its mass times the square of its distance from the axis.

The topic defines the quantity by sum or integral, gathers the values for the usual shapes (rod, hoop, disk, cylinder, sphere), presents the parallel-axis theorem and points to the inertia tensor, needed when the axis is not a principal axis.

What you will truly understand

By the end you will be able to compute the moment of inertia of systems of particles and simple bodies, move it to a parallel axis and recognize why two bodies of equal mass can resist rotation differently.

You will also know when a single number is not enough and the tensor must be used.

Recommended learning route

  1. Definition of the Moment of Inertia: definition as a sum of m·r² or an integral of r² dm.
  2. Standard Moments of Inertia: tabulated values of the usual geometric shapes and which axis they refer to.
  3. Parallel-Axis Theorem: parallel-axis theorem, I = I_cm + Md².
  4. Inertia Tensor: inertia tensor and principal axes for general rotations.

Physical criterion you must acquire

The essential criterion is always to specify the axis: the same body has different moments of inertia depending on the axis. To check a value, remember that it grows with mass and with the square of distance, that a hoop has more than a disk of equal mass and radius, and that the minimum is always about the axis through the center of mass.

Connection with real problems

  • flywheels and rotors.
  • design of wheels, pulleys and gears.
  • sports with spins: skating and gymnastics.
  • dynamics of satellites and free bodies.

Final goal of the topic

The final goal is to compute or look up the appropriate moment of inertia for each axis and use it rigorously in the equations of rotation.

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