5.3 Torque

Syllabus
2024
Topic
5.3
Level

Learning objectives

Identify torque from force geometry

Locate the rotational effect

A force exerts torque about a specified axis only through the component perpendicular to the position vector from that axis to the force's application point. Torque describes the force's rotational effect about that axis.

1

Trace the geometry

Identify each torque in this order:

  1. Name the axis of rotation.
  2. Mark where the force is applied and its direction.
  3. Extend the force's line of action.
  4. Measure the lever arm: the perpendicular distance from the axis to that line.

Recognize zero and nonzero torque

Force geometry about the chosen axis Lever arm Torque?
Line of action passes through the axis Zero None
Force is parallel to the position vector Zero None
Force has a perpendicular component away from the axis Nonzero Yes

Apply the geometry to a door

Door comparison: for an axis through the hinges, a push at the handle perpendicular to the door has a large lever arm and produces torque. A push directed along the door toward the hinges has a line of action through the axis, so its lever arm and torque are zero.

Measure the correct distance

The lever arm is not automatically the distance from the axis to the application point. It is the perpendicular distance to the line of action. Also, only the force component perpendicular to the position vector contributes to torque.

Calculate torque from a force diagram

Preserve force location

A torque force diagram must show each force's relative magnitude and direction and where it acts relative to the chosen axis. That location information is what an ordinary free-body diagram may omit.

Use either torque form

τ=rF=rFsinθ\tau=r_{\perp}F=rF\sin\theta

Symbol Meaning
rr Distance from axis to application point
θ\theta Angle between r\vec r and F\vec F
r=rsinθr_\perp=r\sin\theta Perpendicular lever arm
FF Force magnitude

Calculate an angled force

Angled force: a 30N30\,\text{N} force acts 0.40m0.40\,\text{m} from an axis at 6060^\circ to the position vector.

τ=rFsinθ=(0.40m)(30N)sin60=10.4Nm\tau=rF\sin\theta=(0.40\,\text{m})(30\,\text{N})\sin60^\circ=10.4\,\text{N}\,\text{m}.

Equivalently, r=(0.40m)sin60=0.346mr_\perp=(0.40\,\text{m})\sin60^\circ=0.346\,\text{m} and τ=rF\tau=r_\perp F gives the same result.

Keep angle, direction, and units bounded

The angle is between the position vector and force vector, not automatically the angle drawn against a surface. AP Physics 1 requires manipulation of torque magnitude but not the vector direction of torque. Torque uses N·m; do not relabel it as joules.