5.1.2Torque and Rotational Dynamics
Angular Displacement — AP PHYSICS 1 Revision Notes & Topical Questions
5 min read 10 parts Lesson 4 of 18 1 quiz
Lesson summary
5.1.2 Angular Displacement — AP PHYSICS 1 notes: Define angular displacement, convert between degrees, radians and revolutions and relate it to arc length.Angular position = the angle of a point on a rigid system relative to a reference line, measured about the axis of rotation.A…
- Not total rotation
- Directions
- Convention
- Dimensionless
- Calculator
- Degrees to radians
Section 1 of 10Angular position and displacement
Angular position
Angular position the angle of a point on a rigid system relative to a reference line, measured about the axis of rotation.
Angular displacement
- Δθ = θf − θ0, the change in angular position, in rad.
Reference line
- Reference line a coordinate axis or another position vector.
- (a point at 30° from the x-axis; a point rotated 75° clockwise from its start)
Not total rotation
- Not total rotation a wheel turning two revolutions forward and one backward has net displacement one revolution.
Section 2 of 10Direction and sign
Directions
- Directions clockwise or counterclockwise about the axis; both are vector-like.
Convention
- Convention either direction may be positive only if the other is negative;
- counterclockwise is usually positive.
Example
- Δθ = −3π rad is one and a half revolutions clockwise.
Size
- Size angular displacement can exceed 2π because the object may turn many times.
Section 3 of 10Radians
Radian
Radian the angle subtended at the centre of a circle by an arc equal in length to the radius.
θ = s/r
- θ = s/r arc length s = rθ with θ in radians.
Dimensionless
- Dimensionless a ratio of lengths, so the radian is not strictly a unit.
Calculator
- Calculator must be in radian mode for formulas with ω, α and arc length.
Section 4 of 10Conversions
| Angle | Degrees | Radians |
|---|---|---|
| Full revolution | 360° | 2π (about 6.28) |
| Three quarters | 270° | 3π/2 |
| Half | 180° | π |
| Quarter | 90° | π/2 (about 1.57) |
Degrees to radians
- θ(rad) = θ(°) × π/180°; 1 rad is about 57.3°.
Revolutions
- N = Δθ/2π; 25 rad is about 4.0 revolutions.
rev/s to rad/s
- rev/s to rad/s multiply by 2π.
Section 5 of 10Arc length
Arc length
Full revolution
- Full revolution s = 2πr, the circumference.
Part of a revolution
- Part of a revolution s = rθ.
Rolling without slipping
- Rolling without slipping the centre moves Δx = RΔθ when the wheel turns through Δθ.
Rigid body
- Rigid body all points share Δθ but points at larger r move through greater arc length.
Section 6 of 10Angular position–time graphs
Angular position–time graphs
Gradient
- Gradient is the angular velocity; a steeper line means faster rotation.
Straight line
- Straight line constant ω.
Curve concave upward
- ω increasing, so there is angular acceleration.
Flat line
- Flat line no rotation.
Displacement over an interval
- Displacement over an interval difference of the two vertical-axis values.
Section 7 of 10Benchmarks
Second hand
- 2π rad every 60 s, so 0.105 rad/s.
Minute hand
- 60 times slower, 1.7 × 10−3 rad/s.
Section 8 of 10More from the specification
More from the specification
Angular velocity and orbital motion
- Angular velocity and orbital motion rotating celestial bodies traversing orbital paths around Earth show linear gradient slope relationships on kinematics graphs.
Distance
- Total length of path travelled, a scalar.
Rotational kinematics
- Equations linking Δθ, ω0, ω, α and t.
Angular speed
- Magnitude of the angular velocity.
Linear
- A graph that is a straight line through the origin, so resistance is constant.
Section 9 of 10Key terms
| Term | Meaning |
|---|---|
| Angular displacement | Angle turned by an object, Δθ = θf − θi. |
| Radian | Angle for which arc length equals radius; 2π rad = 1 revolution. |
| Arc length | Distance along a circle, s = rθ. |
| Revolution | One complete turn, 2π rad. |
Section 10 of 10Exam technique
1
Using degrees in s = rθ.
2
Ignoring signs when a rotation reverses direction.
3
Treating a revolution as 1 radian rather than 2π.
4
Using the diameter instead of the radius for arc length.
5
Believing angular displacement is limited to 2π.
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