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AP® Physics 1: Algebra-Based · Unit 6 · Topic 6.2

Torque and Work: Revision Notes (Physics 1 6.2)

One-page recap of work done by torques for the algebra-based course: W = τΔθ in radians, signs of work, area under a torque–angle graph, the link to rotational kinetic energy and common slips.

Short on time? This page is the recap. For the derivation, diagrams and worked examples, use the full study guide. This is the algebra-based course: no calculus is needed.

Recap

  • A torque transfers energy into or out of a rigid system only when the system turns while the torque acts.
  • A tangential force F at radius r moves its point of application along an arc s = rΔθ, so W = Fs = (rF)Δθ = τΔθ.
  • A torque in the same sense as the rotation does positive work (energy in). An opposing torque, such as axle friction, does negative work (energy out).
  • A force through the axle exerts no torque and does no work on the rotation.
  • The net work done by all torques equals the change in rotational kinetic energy.

Key relationships

Relationship Symbols and units Use it to
W = τΔθ τ in N·m, Δθ in rad, W in J work by a constant torque
s = rΔθ s, r in m arc length moved by the point where a force acts
τ = rF⊥ N·m torque from the perpendicular force component
W = area under τ–θ graph J work by a changing torque
W_net = ½Iω² − ½Iω₀² J find a final angular velocity, or a stopping angle
1 rev = 2π rad; 90° = π/2 rad rad convert angles first

Factors of change: τ × 2 at the same Δθ → W × 2. From rest, W × 2 → ω × √2. A stopping angle against a constant friction torque grows with ω₀², so doubling ω₀ multiplies it by 4.

Assumptions behind the numbers

  • The object is rigid and turns about a fixed axis in one plane.
  • W = τΔθ needs a constant torque; otherwise use the graph area.
  • Friction torques are treated as constant unless a graph says otherwise.

Mistakes to avoid

  1. Degrees or revolutions in W = τΔθ. Convert to radians.
  2. Calling torque “energy” because both use N·m. Write work in J.
  3. Positive work for friction. It opposes the rotation, so its work is negative.
  4. Largest torque × whole angle for a changing torque. Use the area.
  5. Work done by a torque that does not turn anything. It is zero.
  6. Forgetting the starting kinetic energy when the object is already spinning: W_net is the change in K.

Quick self-check

  1. A constant torque of 5.0 N·m turns a wheel through 4.0 rad. How much work is done? (20 J)
  2. A constant torque of 2.0 N·m acts through 3.0 revolutions. How much work is done? (3.0 × 2π = 18.8 rad, so 37.7 J)
  3. Torque rises steadily from 0 to 4.0 N·m as a wheel turns from 0 to 3.0 rad. How much work is done? (Triangle: ½ × 3.0 × 4.0 = 6.0 J)

Next: practice questions.

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