Torque & Couples (A Level)
Key idea: Define moment (torque), apply the principle of moments, and solve equilibrium problems involving couples (A Level Physics).
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The core idea
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Learning objectives
- Apply moments, couples and force-and-torque equilibrium using free-body diagrams and vector triangles.
- show an understanding that the weight of a body may be taken as acting at a single point known as its centre of gravity
- apply the principle of moments to new situations or to solve related problems
- Explain inertia and momentum, then apply Newton's laws using free-body diagrams.
1. Definitions (Must Know)
A. Moment (torque) of a force, τ
The moment (torque), τ, of a force about a point (pivot) is:
τ = Fd_⊥
where d_⊥ is the perpendicular distance from the pivot to the force’s line of action.
Unit: N m.
B. Couple
A couple is a pair of forces that are:
- equal in magnitude,
- opposite in direction,
- parallel, but with different lines of action (separated by a distance).
A couple produces a turning effect with zero resultant force.
C. Equilibrium (force + moment)
A rigid body is in equilibrium when:
∑ vector F = 0 and ∑ τ = 0
2. Key Ideas (What Earns Marks)
- Use perpendicular distance to the line of action (not the slanted length).
- Choose a sign convention (e.g. anticlockwise +, clockwise −) and stick to it.
- For equilibrium, use:
- ∑ Fₓ = 0 and ∑ F_y = 0 (if needed),
- ∑ τ = 0 about a convenient pivot.
- The moment of a couple is: τ = Fs where s is the perpendicular separation of the forces; the torque of a couple does not depend on the pivot.
- The weight of a body can be taken as acting at its centre of gravity: Centre of Gravity.
Moment is force multiplied by the perpendicular distance to the line of action. Using the slanted length directly is one of the most common setup errors.
3. Detailed Explanations
A. Finding d_⊥ (the common trap)
d_⊥ is the shortest distance from the pivot to the force’s line of action.
If the force acts at an angle, you usually need:
- d_⊥ = r sin θ (if r is the distance from pivot to point of application, and θ is the angle between vector r and vector F).
B. Choosing the pivot smartly
You can take moments about any point. Choose a pivot that removes unknown forces from the moment equation.
Example: if a beam is supported at a hinge, taking moments about the hinge eliminates the hinge reaction.
C. Why a couple gives “pure rotation”
For a couple:
- resultant force is zero (forces cancel),
- but there is still a net turning effect because the forces act at different lines of action.
That is why a steering wheel can be turned without translating.
D. Principle of moments (equilibrium condition)
If a body is in equilibrium, the sum of clockwise moments equals the sum of anticlockwise moments (about any point):
∑ τ_clockwise = ∑ τ_anticlockwise
This is just another way to say ∑ τ = 0.
4. Common Mistakes
- Using the distance to the point of application instead of the perpendicular distance.
- Swapping clockwise/anticlockwise signs halfway through.
- Forgetting a force’s line of action (e.g. weight acts through the centre of gravity).
- Assuming “balanced forces” implies “no rotation” (you also need ∑ τ = 0).
5. Exam Tips
- Draw a clear diagram with the pivot marked and the line of action of each force.
- State your sign convention explicitly.
- In equilibrium problems, try moments about a point that eliminates an unknown.
- If you get a negative value for a reaction force, your assumed direction is wrong.
6. Worked Examples
Modelled example 1
Simple torque calculation
Problem
Study the worked solution
Identify the lever arm
Method
d_⊥ = 0.20 m.Reason
The force is perpendicular to the spanner, so the stated radius is already the perpendicular distance to its line of action.Working
d_⊥ = 0.20 mCalculate the moment
Method
τ = 10 N m.Reason
Moment magnitude is force times perpendicular distance.Working
τ = Fd_⊥ = 50(0.20) = 10 N m
Guided practice 2
Beam in equilibrium (principle of moments)
Problem
Try this before viewing the solution
Hints
Hint 1: balance vertical forces
View solution step by step
List the vertical forces
Method
The fixed support reaction acts upward; beam weight and load act downward.Reason
The beam is in translational equilibrium.Working
∑ F_y = R-40-60Apply vertical equilibrium
Method
R = 100 N upward.Reason
Zero vertical resultant requires the support force to balance both downward loads.Working
R-40-60 = 0 ⇒ R = 100 NKeep rotational equilibrium distinct
Method
The fixed support must also provide a reaction moment.Reason
A single upward force at the left end cannot by itself balance the clockwise moments of the two loads.Working
Mₛᵤₚₚₒᵣₜ = 40(1.0) + 60(2.0) = 160 N m anticlockwise.
Common misconception 3
Torque of a couple
Learner claim
Try this before viewing the solution
View solution step by step
Interpret the separation
Method
s = 0.30 m is the full perpendicular distance between the forces.Reason
Each force’s moment about a midpoint would use half this distance.Working
s/2 = 0.15 mAdd the two force moments
Method
The moments reinforce to 3.6 N m.Reason
Using the midpoint gives two terms F(s/2), equivalent to one Fs.Working
2(12)(0.15) = 12(0.30) = 3.6 N m
Examiner practice 4
Beam supported at both ends (find reactions)
Examination question
Try this before viewing the solution
View solution step by step
Write vertical force equilibrium
1 markMethod
R_A + R_B = 90 N.Reason
The reactions balance the beam and added-load weights.Working
R_A + R_B = 30 + 60Take moments about the left support
2 marksMethod
3.0R_B = 165 N m.Reason
The left reaction has zero lever arm; the uniform beam’s weight acts at 1.5 m.Working
R_B(3.0) = 30(1.5) + 60(2.0) = 165Calculate the right reaction
1 markMethod
R_B = 55 N.Reason
Divide the balancing moment by the 3.0 m support separation.Working
R_B = 165/3.0 = 55 NCalculate the left reaction
1 markMethod
R_A = 35 N.Reason
The two reactions must sum to 90 N.Working
R_A = 90-55 = 35 N
Self-mark with the mark scheme
Compare your response with each mark point. Select a point only when your response contains that evidence.
Self-mark force balance, moment setup and both reactions.
Challenge 5
Torque when the force is at an angle
Independent transfer
Try this before viewing the solution
Hints
Hint 1: extract the perpendicular contribution
View solution step by step
Find the perpendicular factor
Method
The moment uses rF sin θ.Reason
θ is the angle between the position vector along the spanner and the force.Working
d_⊥ = r sin θCalculate torque
Method
τ = 5.0 N m.Reason
The parallel component of force produces no moment about the bolt.Working
τ = (0.25)(40) sin 30° = 5.0 N m
7. Mind Stretchers
Mind stretcher 1: “Net force zero” does not guarantee equilibriumExtension
Give an example where the resultant force is zero but the object still rotates. Explain using moments.
Click here to show/hide answer
A couple: two equal and opposite forces separated by a distance.
Resultant force is zero, but there is a non-zero turning effect (τ = Fs), so it rotates unless an opposing moment balances it.
Mind stretcher 2: Pivot choice checkExtension
In a beam problem, explain why you can take moments about a point where an unknown reaction acts, and why that helps.
Click here to show/hide answer
If you take moments about the point where the unknown reaction acts, its moment is zero because d_⊥ = 0.
This removes that unknown from the moment equation, making the algebra simpler.
Mind stretcher 3: Optional (Enrichment)Extension
A. Torque as a vector (right-hand rule)
At a more advanced level, torque is treated as a vector vector τ = vector r × vector F (direction by right-hand rule).
For most A Level exam questions, clockwise/anticlockwise moments about a pivot are sufficient.
B. Three-force equilibrium (concurrency idea)
For a rigid body in equilibrium under three non-parallel forces, the lines of action are concurrent (they meet at one point). This is useful but not always required.
O Level refresher on moments: Moment Of A Force.
Continue with the next resource in this course.
Course and syllabus information
- Course
- GCE A-Level H2 Physics
- Edition
- GCE A-Level H2 Physics 2027