Access this content offline
Omniguides
Skip to reading

Moment of Inertia

Reference from the original Physics I textbook.

Moment of Inertia

Moment of inertia measures how mass is distributed relative to a chosen rotation axis: I = Σmᵢrᵢ² or I = ∫r_⊥² dm. It has units kg·m².

Figure6.2.1 1 — details in the accompanying text.

 

Related Glossary Terms

Moment of Inertia Equation, Parallel Axis Theorem Equation, Parallel-Axis Theoremⓘ

Index

Chapter 6 - Moment of Inertia

Chapter 6 - Angular Forces

Chapter 6 - Angular Momentum

Chapter 6 - Angular Momentum

Reviewed physics notes (1)

These corrections keep the original lesson’s purpose while fixing errors in the source edition.

  • Original definition confuses inertia with forces causing rotation. — Reference 1

About this edition and its source ↗

Glossary and deeper reading · 2 refreshers

These editorial refreshers supplement the reading. Definitions and examples are added guidance; original source wording and recorded answers remain in their original context.

  • Rotational inertia

    Rotational inertia measures how strongly a mass distribution resists a change in angular velocity about a specified axis. Mass farther from that axis contributes more strongly because each contribution depends on squared distance. For example, moving small masses outward along a rotating rod increases its rotational inertia without changing its total mass.

    Read more: Rotational inertia →

  • Parallel-axis theorem

    The parallel-axis theorem relates rotational inertia about a center-of-mass axis to inertia about a parallel displaced axis. The displaced-axis value is the center-of-mass value plus total mass times the squared separation of the axes. For example, a uniform rod has greater rotational inertia about one end than about a parallel axis through its middle.

    Read more: Parallel-axis theorem →

Search lessons, terms and problems