1.5.2 Turning Effect of Forces – Moment (Torque)
Quick‑scan of the Cambridge IGCSE Physics (0625) syllabus
| Syllabus requirement | Covered in these notes? |
|---|
| Definition of a moment (torque) | ✓ |
| Formula τ = F d sin θ and special case τ = F d | ✓ |
| Units (N·m) and distinction from energy (J) | ✓ |
| Sign convention for clockwise/anticlockwise moments | ✓ |
| Principle of moments (rotational equilibrium) | ✓ |
| Effect of changing force magnitude, lever arm, or angle | ✓ |
| Everyday examples illustrating the concept | ✓ |
| Worked example with a seesaw (balance of moments) | ✓ |
| Sample calculations (different angles, zero‑moment case) | ✓ |
| Practical activity to verify τ = F d | ✓ |
| Quick‑check questions & model answers | ✓ |
| Summary of key points | ✓ |
What is a Moment?
- A moment (or torque) measures a force’s ability to cause rotation about a pivot (fulcrum).
- It depends on:
- Force magnitude (F) – newtons (N)
- Perpendicular distance from the pivot to the line of action (lever arm, d) – metres (m)
- Angle (θ) between the force direction and the lever arm. Only the component of the force acting ⟂ to the lever arm contributes.
τ = F d sin θ
When the force is applied at right angles (θ = 90°), sin θ = 1 and the formula reduces to τ = F d.
Units
SI unit: newton‑metre (N·m). Although dimensionally equivalent to the joule, N·m is used for rotational effects, while J is used for energy.
Sign convention
| Direction | Sign |
|---|
| Clockwise | – (negative) |
| Anticlockwise | + (positive) |
Any consistent convention may be used; apply it throughout a problem.
Principle of Moments (Rotational Equilibrium)
An object will not rotate when the algebraic sum of all moments about any pivot is zero:
∑τ = 0 ⟹ ∑τclockwise = ∑τanticlockwise
Everyday Examples
- Opening a door – The handle is far from the hinges, giving a large lever arm and a large moment for a modest push.
- Using a wrench – Doubling the length of the wrench halves the required force for the same torque.
- Seesaw (teeter‑totter) – Balance is achieved when the clockwise and anticlockwise moments are equal.
- Steering wheel – Hands on the rim apply force at a large radius, producing a sizeable turning moment.
- Crowbar – A longer bar provides a greater lever arm, making it easier to lift or pry heavy objects.
- Cork‑screw – The spiral acts as a lever; a longer handle reduces the force needed to twist the cork.
Worked Example – Seesaw Balance
Problem: A seesaw is pivoted at its centre. Child A (weight = 300 N) sits 1.2 m to the left of the pivot. Child B (weight = 200 N) sits on the right. How far from the pivot must Child B sit to keep the seesaw level?
- Choose a sign convention (clockwise = –, anticlockwise = +).
- Write the equilibrium condition: ∑τ = 0.
- Calculate each moment:
- τA = –(300 N)(1.2 m) = –360 N·m
- τB = +(200 N)(d) (where d is the unknown distance)
- Set the sum to zero and solve:
–360 N·m + 200 N·d = 0 ⇒ d = 360 / 200 = 1.8 m
Child B must sit 1.8 m to the right of the pivot.
Sample Calculations
| Force F (N) | Lever arm d (m) | Angle θ (°) | Moment τ (N·m) |
|---|
| 30 | 0.50 | 90 | 30 × 0.50 × sin 90° = 15 |
| 50 | 0.20 | 30 | 50 × 0.20 × sin 30° = 5 |
| 80 | 0.40 | 0 | 80 × 0.40 × sin 0° = 0 (force acts through the pivot) |
Practical Activity – Verifying τ = F d
Objective: Demonstrate that the moment produced by a force applied at right angles equals the product of the force and its perpendicular distance.
- Set up a rigid board (≈1 m) on a low fulcrum (e.g., a wooden block).
- Attach a spring scale at one end; this will apply a known force F.
- Measure the distance d from the fulcrum to the point where the scale is attached.
- Place a known weight W on the opposite side of the fulcrum. Adjust its distance d′ until the board stays horizontal (rotational equilibrium).
- Using the principle of moments, calculate the experimental torque: τexp = W d′.
- Compare τexp with the calculated torque τ = F d. Discuss sources of error (friction at the fulcrum, non‑perpendicular force, scale calibration).
Safety: Secure the board, keep fingers away from the moving scale, and avoid over‑loading the fulcrum.
Quick‑Check Questions
- If you double the lever arm d while keeping the force unchanged, what happens to the moment?
- A 10 N force is applied at the end of a 0.30 m wrench at an angle of 60°. Calculate the moment.
- Explain why a longer crowbar makes it easier to lift a heavy object.
- In the seesaw example above, if Child A moves 0.30 m farther from the pivot, how must Child B’s distance change to keep balance?
Model Answers
- The moment doubles because τ = F d (τ ∝ d).
- τ = 10 N × 0.30 m × sin 60° = 10 × 0.30 × 0.866 ≈ 2.6 N·m.
- A longer crowbar increases the lever arm d, so for the same applied force the torque τ = F d is larger, reducing the effort needed.
- Original balance: 300 N × 1.2 m = 200 N × d → d = 1.8 m.
New left‑hand moment: 300 N × (1.2 + 0.3) = 300 × 1.5 = 450 N·m.
To balance: 200 N × d′ = 450 N·m → d′ = 2.25 m.
Child B must move 0.45 m farther from the pivot.
Summary of Key Points
- Moment (torque) quantifies a force’s turning effect: τ = F d sin θ.
- Both the magnitude of the force and its perpendicular distance from the pivot are crucial; the angle determines the effective component.
- Assign opposite signs to clockwise and anticlockwise moments; rotational equilibrium requires ∑τ = 0.
- Everyday tools (doors, wrenches, seesaws, steering wheels, crowbars, cork‑screws) illustrate how increasing the lever arm reduces the required effort.
- Practical investigations reinforce the concept and develop essential AO3 skills for the IGCSE exam.
Note to Teachers & Learners
These notes cover sub‑topic 1.5.2 in detail. They should be used alongside the full IGCSE Physics syllabus, which also includes motion, thermal physics, waves, electricity & magnetism, nuclear physics, space physics, and practical skills. Cross‑reference the relevant sections for a complete revision programme.