5.1Torque and Rotational Dynamics
Rotational Kinematics — AP PHYSICS 1 Revision Notes & Topical Questions
5 min read 8 parts Lesson 2 of 18 1 quiz
Lesson summary
5.1 Rotational Kinematics — AP PHYSICS 1 notes: Describe the rotation of a system over time using angular displacement, angular velocity and angular acceleration.Rigid system — a system that holds its shape although different points move in different directions and with different…
- Not a point object
- Centre of mass
- Rigid body
- Angular displacement Δθ
- Average angular velocity
- What the symbols mean
Part 1 of 6Rotating rigid systems
Rotating rigid systems
Rigid system
- Rigid system a system that holds its shape although different points move in different directions and with different speeds.
Not a point object
- Not a point object a rigid system cannot be modelled as a single object;
- its size and mass distribution matter.
Centre of mass
- Centre of mass if the rotation about an axis can be described by the centre of mass motion, the system may be treated as one object.
- (Earth's rotation is negligible for its orbit)
Rigid body
- Rigid body all points share the same θ, ω and α.
Part 2 of 6Angular variables
1Angular displacement Δθ
Angular displacement Δθ angle through which a point rotates about an axis, in radians; 1 rev = 2π rad; revolutions = Δθ/2π.
2Average angular velocity
- ωavg = Δθ/Δt in rad/s; ω = 2π/T.What the symbols mean: ω = angular frequency (rad s−1) · f = frequency (Hz) · T = period (s)
3Average angular acceleration
- αavg = Δω/Δt in rad/s2.
4Sign
- Sign counterclockwise is usually positive.
5Speeding up or slowing
- Speeding up or slowing same signs of ω and α speed it up; opposite signs slow it down.
6Conversion
- Conversion rev/min × 2π/60 = rad/s.
Part 3 of 6Constant angular acceleration equations
| Linear | Rotational |
|---|---|
| v = v0 + at | ω = ω0 + αt |
| x = v0t + ½at2 | θ = ω0t + ½αt2 |
| v2 = v02 + 2aΔx | ω2 = ω02 + 2αΔθ |
Validity
- Validity constant α only.
Analogy
- θ, ω, α correspond to x, v, a with the same mathematics.
Part 4 of 6Graphs
θ–t slope
- θ–t slope gives ω.
ω–t slope
- ω–t slope gives α.
ω–t area
- ω–t area gives Δθ.
α–t area
- α–t area gives Δω.
Part 5 of 6Solving rotational kinematics problems
1
Choose a positive rotation direction (usually counterclockwise).
2
Convert all angles to radians and speeds to rad/s.
3
List the known variables (θ, ω0, ω, α, t) and the unknown.
4
Choose the constant-α equation that omits the variable you do not need.
5
Solve and convert to revolutions if asked.
Part 6 of 6More from the specification
Vector
- Quantity with magnitude and direction.
Distance
- Total length of path travelled, a scalar.
Key terms
| Term | Meaning |
|---|---|
| Angular displacement | Angle turned, in radians. |
| Angular velocity | Δθ/Δt in rad/s. |
| Angular acceleration | Δω/Δt in rad/s2. |
| Radian | Arc length divided by radius; 2π rad = 360°. |
| Period | Time for one revolution; ω = 2π/T. |
| Rigid system | System that holds its shape while rotating. |
Avoid these mistakes
1
Using degrees or rpm directly in the equations.
2
Forgetting that the equations need constant α.
3
Mixing up revolutions and radians.
4
Ignoring the sign convention for direction.
Marked practiceQuizzes for this lesson
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