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Parallel Axis Theorem Equation

Reference from the original Physics I textbook.

Parallel Axis Theorem Equation

Iz=Ic+mR2

I_z = inertia about the new axis; I_c = inertia about the parallel axis through the center of mass (kg·m²); m = mass (kg); R = perpendicular separation of the two parallel axes (m).

Figure6.2.2 — details in the accompanying text.

Related Glossary Terms

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

Index

Chapter 6 - Moment of Inertia

Chapter 6 - Moment of Inertia

Chapter 6 - FFR - Rotational Energy

Reviewed physics notes (1)

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

  • Parallel-axis theorem requires a center-of-mass reference axis. — 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.

  • 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 →

  • 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 →

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