Rotational motion and torque

College Physics I. Also known as: phys 101, phys 1401, phys 2425, phys 1, college physics, college physics i, algebra-based physics, physics 1, general physics 1, general physics i, introductory physics i, phys 201

Angular velocity, centripetal acceleration, torque, moment of inertia and angular momentum.

Describing rotation

Rotation uses angular versions of the linear quantities. Angular position θ is measured in radians, where one full turn is 2π rad (about 6.28 rad). Angular velocity ω is the rate of change of angle, and angular acceleration α is the rate of change of ω. To convert revolutions per minute to rad/s, multiply by 2π and divide by 60. The constant-acceleration equations carry over: ω = ω₀ + α t and θ = ω₀ t + ½ α t².

Linking to linear motion

A point at distance r from the axis moves with speed v = ω r and tangential acceleration a = α r. If it moves in a circle at constant speed it still accelerates toward the centre: a_c = v² / r = ω² r. For rolling without slipping, the centre of the wheel moves at v = ω r.

Torque

Torque is the turning effect of a force: τ = r F sin θ, where r is the distance from the pivot to the point of application and θ is the angle between the force and the arm. Torque has units N·m. A force along the line through the pivot gives zero torque. A longer wrench makes the same push turn a bolt more easily. For static balance (no rotation), the clockwise torques equal the anticlockwise torques about any chosen pivot, as when two children balance on a seesaw.

Moment of inertia and Newton's second law for rotation

The moment of inertia I measures resistance to a change in rotation. It depends on how mass is spread out: mass far from the axis counts more. The rotational second law is Στ = I α. Rotational kinetic energy is KE = ½ I ω².

Angular momentum

Angular momentum is L = I ω. With no net external torque it is conserved. When a spinning skater pulls in her arms, I falls and so ω rises in proportion. Note that kinetic energy is not conserved here, because she does work pulling her arms in.

Worked example

A wheel of radius 0.30 m starts from rest with α = 2.0 rad/s² for 5.0 s.

  1. Final angular speed: ω = 2.0 × 5.0 = 10.0 rad/s.
  2. Rim speed: v = ω r = 3.0 m/s.
  3. Angle turned: θ = ½ × 2.0 × 5.0² = 25 rad, which is 3.98 revolutions.
  4. Centripetal acceleration at the rim: ω² r = 30.0 m/s².

Common mistakes

  • Using degrees or revolutions in formulas that need radians.
  • Forgetting the sine of the angle in the torque formula.
  • Using the total mass rather than the distribution of mass for I.
  • Mixing linear and angular quantities in one equation without the factor r.

Practice questions

  1. A fan turns at 120 revolutions per minute. What is its angular speed in radians per second?

  2. A wheel spins at 15 rad/s. What is the linear speed of a point on it 0.40 m from the axis?

  3. A car drives at a steady 20 m/s around a circular bend of radius 50 m. What is its centripetal acceleration?

  4. A 25 N force acts on a lever arm 0.30 m long, at 30 degrees to the arm. What is the torque about the pivot?

  5. A 30 kg child sits 1.5 m from the pivot of a balanced seesaw. Where must a 45 kg child sit on the other side to balance it?

  6. A wheel starting from rest reaches 40 rad/s after 8.0 s of constant angular acceleration. What is the angular acceleration?