5.1 Rotational Kinematics
- Syllabus
- 2024
- Topic
- 5.1
- Level
- —
Angular displacement measures rotation about a specified axis in radians. Choose either clockwise or counterclockwise as positive; the opposite direction is negative.
Δθωavgαavg=θ−θ0=ΔtΔθ=ΔtΔω
Units are rad, rad/s, and rad/s².
| One-dimensional linear motion | Rotation about one axis |
|---|---|
| Position x | Angular position θ |
| Velocity v | Angular velocity ω |
| Acceleration a | Angular acceleration α |
ωθω2=ω0+αt=θ0+ω0t+21αt2=ω02+2α(θ−θ0)
| Graph | Slope gives | Signed area gives |
|---|---|---|
| θ versus t | ω | — |
| ω versus t | α | Δθ |
| α versus t | Rate of change of α | Δω |
Constant-α example: choose counterclockwise as positive. A wheel has ω0=+2.0rad/s and α=−0.50rad/s2 for 4.0s.
ω=ω0+αt=2.0+(−0.50)(4.0)=0rad/s,
Δθ=ω0t+21αt2=(2.0)(4.0)+21(−0.50)(4.0)2=4.0rad.
The wheel slows to rest but still turns 4.0 rad counterclockwise during the interval.
A rigid system keeps its shape, but different points move in different directions during rotation, so it is not generally a point object. Treat it as a single object only when its rotation is negligible for the motion being analyzed. Direction descriptions here are limited to clockwise and counterclockwise about the stated axis.