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Angular Momentum of a Rigid Body Equation

Reference from the original Physics I textbook.

Angular Momentum of a Rigid Body Equation

About a principal axis, H⃗_O = Iω⃗. For general rigid-body rotation, angular momentum and angular velocity need not be parallel.

H→0=Angular Momentum(N⋅m⋅s)​
I=Moment of Inertia(kg⋅m2)​
ω→=Angular Velocity(rad/s)

Gallery6.4.1.2 — details in the accompanying text.

Related Glossary Terms

Angular Momentum, Conservation of Angular Momentum (Inertia Definition)

Index

Chapter 6 - Angular Momentum

Chapter 6 - Angular Momentum

Chapter 6 - FFR - Rotational Energy

Reviewed physics notes (1)

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

  • Scalar I times ω⃗ is restricted to a principal axis. — Reference 1

About this edition and its source ↗

Glossary and deeper reading · 1 refreshers

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

  • Angular momentum

    Angular momentum describes motion about a specified point or axis. For rigid rotation about a fixed principal axis it can be written as rotational inertia times angular velocity; a translating particle can also have angular momentum about a point. For example, a ball moving past a pole has angular momentum about the pole even though the ball’s path is straight.

    Read more: Angular momentum →

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