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Rotational kinematics

Beginner

Constant-α equations mirror linear ones.

Key relationθ = ω₀t + ½αt²

With constant α: ω = ω₀ + αt, θ = ω₀t + ½αt², ω² = ω₀² + 2αθ. They are used the same way as linear equations.

Worked example

A wheel stops from 10 rad/s with α = −2: turns 25 rad.

Common mistake

Check signs of α and ω.

In more detail

Rotational kinematics uses the same equations as linear kinematics with angular quantities: ω = ω0 + αt, θ = ω0 t + ½αt², and ω² = ω0² + 2αθ, for constant angular acceleration.

Real-world uses

Open the interactive lesson, with simulation and quiz →

Frequently asked questions

Can I use these for any rotation?

Only for constant angular acceleration.

What is the angular analogue of mass?

The moment of inertia.

How do I know which equation to use?

Use the same approach as linear motion, substituting angle for displacement, angular velocity for velocity and angular acceleration for acceleration.

Related topics in Rotational Motion

Angular acceleration · Radians and degrees · Relation between linear and angular quantities · Torque · Lever arm and moment · Equilibrium of a rigid body

← All Rotational Motion topics