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AP® Physics C: Mechanics · Unit 5 · Topic 5.3

Torque: Revision Notes (Physics C: Mechanics 5.3)

One-page recap of torque for the calculus-based course: rF sin θ, lever arms, force diagrams, τ = r × F with the right-hand rule, and signed net torque about one stated axis.

Short on time? This is the recap for the calculus-based course, which treats torque as a vector (Physics 1 uses only its size). For diagrams and worked examples, use the full study guide.

Recap

  • Torque is the turning effect of a force about a chosen axis. State the axis first.
  • r runs from the axis to the point where the force acts. θ is the angle between r and F, tail to tail.
  • Only the component of F perpendicular to r turns the object. The component along r gives no torque.
  • The lever arm r⊥ is the perpendicular distance from the axis to the line of action of the force.
  • A force diagram shows each force starting at the point where it acts, with distances from the axis.
  • Weight acts at the centre of mass (uniform g).
  • Net torque is the signed sum of torques about one axis.

Key relationships

Relationship Units Meaning
τ = r × F N·m vector, perpendicular to the plane of r and F
|τ| = rF sin θ N·m size from r, F and the angle between them
τ = rF⊥, F⊥ = F sin θ N·m perpendicular component × distance
τ = r⊥F, r⊥ = r sin θ N·m lever arm × force
τ_z = xF_y − yF_x N·m component form for forces in the xy-plane
î × ĵ = k̂, ĵ × î = −k̂ — order matters: B × A = −(A × B)
τ_net = Στ (one axis) N·m counterclockwise +, clockwise −

Right-hand rule

Fingers along r, curl towards F through the smaller angle: your thumb gives τ. For forces in the page, thumb out = counterclockwise, thumb in = clockwise.

Assumptions

  • The system is rigid: every part turns through the same angle.
  • Forces and r lie in one plane unless stated, so τ is along ±z.
  • g = 9.8 m/s², uniform, so weight acts at the centre of mass.

Mistakes to avoid

  1. τ = rF for any angle. Include sin θ.
  2. Lever arm = distance to the point of application. It is the distance to the line of action.
  3. F × r instead of r × F. The sign flips.
  4. Hinge forces in the torque sum about the hinge. They give zero torque there.
  5. Adding torques about different axes.
  6. Dropping the minus sign on clockwise torques.
  7. Using the obtuse angle wrongly. sin(180° − θ) = sin θ, so both give the same size; the direction comes from the right-hand rule.

Quick self-check

  1. A 60 N force acts 0.25 m from an axis at 40° to r. Size of torque? (0.25 × 60 × sin 40° = 9.6 N·m)
  2. r = 0.30î m, F = −20ĵ N. Find τ. (τ_z = (0.30)(−20) − 0 = −6.0 N·m, so −6.0k̂ N·m, clockwise)
  3. A 45 N force acts 0.80 m from an axis; its line of action makes 30° with r. Lever arm and torque? (r⊥ = 0.80 sin 30° = 0.40 m; τ = 18 N·m)

Next: practice questions.

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