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Rotational kinematics equations
Intermediate
Analogues of linear equations with θ, ω, α.
ω = ω₀ + αtWith constant α the equations mirror the linear ones: ω = ω₀ + αt, θ = ω₀t + ½αt², ω² = ω₀² + 2αθ. Replace x→θ, v→ω, a→α.
A disc at 10 rad/s decelerates at 2 rad/s²: stops after 5 s turning 25 rad.
Use radians consistently.
In more detail
Rotational kinematics equations match the linear ones: ω = ω0 + αt, θ = ω0 t + ½αt², and ω² = ω0² + 2αθ, valid for constant angular acceleration.
Real-world uses
- Calculating how many turns a flywheel makes as it slows to a stop.
- Estimating the time for a spinning drill to reach operating speed.
- A flywheel in a motor slows down with constant angular deceleration, and the rotational equations predict how many turns it makes before stopping.
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Frequently asked questions
How do I convert between linear and angular quantities?
Use s = rθ, v = rω and a = rα.
Can I use these for variable angular acceleration?
Only over intervals where the angular acceleration is roughly constant.
How do I know which rotational equation to use?
Match the known quantities: angle, angular velocity, angular acceleration and time, just as with linear motion.
Related topics in Kinematics
Centripetal acceleration · Non-uniform circular motion · Angular acceleration · Motion in polar coordinates · Motion in three dimensions · Parametric motion