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FractionRush AQA A-Level Physics 4

Scalars, Vectors & Moments

Master vector resolution, calculate moments and couples, apply equilibrium conditions, and locate the centre of mass of objects.

AQA A-Level Physics · Unit 4: Mechanics
➡️Scalars vs vectors
Distinguish between scalar and vector quantities with examples
📐Vector resolution
Resolve any vector into perpendicular components using trigonometry
🔄Moments
Calculate the turning effect of a force: M = Fd
⚖️Couples
Understand and calculate the torque of a couple
🏋️Equilibrium
Apply the conditions for static equilibrium to solve problems
Centre of mass
Define centre of mass and locate it for uniform and composite objects

Scalars and Vectors

Physical quantities are classified as either scalars or vectors.

Scalar: A quantity that has magnitude only. Examples: mass (kg), temperature (°C), speed (m s⁻¹), energy (J), time (s), distance (m).
Vector: A quantity that has both magnitude and direction. Examples: displacement (m), velocity (m s⁻¹), acceleration (m s⁻²), force (N), momentum (kg m s⁻¹).

Vectors are added using the triangle rule (tip-to-tail) or the parallelogram rule. The resultant is the single vector that has the same effect as all the original vectors combined.

For two vectors at right angles, the magnitude of the resultant R is found using Pythagoras: R = √(A² + B²), and the direction is θ = tan⁻¹(B/A).

The opposite of vector addition is resolution: splitting a single vector into two perpendicular components. This is almost always done horizontally (x) and vertically (y):

Fₓ = F cosθ     Fᵧ = F sinθ

where θ is the angle between the vector and the horizontal. Resolution into components makes all subsequent calculations far simpler, especially in mechanics problems.

Always draw a diagram before resolving vectors. Identify clearly which angle θ refers to — angles measured from different reference directions give different component expressions.

Moments of a Force

A moment is the turning effect of a force about a pivot point. It depends on both the size of the force and its perpendicular distance from the pivot.

Moment = F × d
SymbolQuantityUnit
MMoment (torque)N m
FForceN
dPerpendicular distance from pivot to line of action of forcem

The critical word is perpendicular: d must be the shortest distance from the pivot to the line of action of the force — not just the straight-line distance to where the force is applied. If the force is applied at an angle, you must find the perpendicular component or the perpendicular distance.

Moment = F × (perpendicular distance from pivot to line of action). Units: N m (not the same as joules, even though the dimensions are the same).

Moments are described as clockwise or anticlockwise. By convention, anticlockwise is usually taken as positive.

Couples and Equilibrium

A couple is a pair of equal and opposite forces that are not acting through the same point. A couple produces a pure turning effect (torque) with no resultant force.

Torque of a couple = F × d

where F is the magnitude of one force and d is the perpendicular distance between the two forces (not the distance from one force to a pivot).

Examples of couples: turning a steering wheel, using a spanner with two hands, the forces on a compass needle in a magnetic field.

For an object to be in static equilibrium, two conditions must both be satisfied:

Condition 1 (Force equilibrium): The resultant force in every direction is zero. (ΣF = 0 in both x and y directions)

Condition 2 (Moment equilibrium — Principle of Moments): The sum of clockwise moments about any point equals the sum of anticlockwise moments about the same point.

The Principle of Moments states: for a body in equilibrium, the sum of clockwise moments about any pivot equals the sum of anticlockwise moments about the same pivot.

Σ(clockwise moments) = Σ(anticlockwise moments)

Centre of Mass

The centre of mass (CoM) of an object is the single point at which the entire weight of the object appears to act. For a uniform object, the centre of mass is at its geometric centre (midpoint for a rod, centre of a circle, etc.).

Centre of mass: The point through which the resultant gravitational force (weight) acts on an object, regardless of the object's orientation.

For a composite object made of several uniform parts, the position of the overall CoM is found by taking moments of weight:

x̄ = (m₁x₁ + m₂x₂ + m₃x₃ + …) ÷ (m₁ + m₂ + m₃ + …)

where x₁, x₂, … are the distances of each component's own CoM from a chosen reference point.

Experimental method to find the CoM of an irregular lamina: suspend the object freely from different points — the CoM lies along the vertical through the suspension point. The intersection of two such vertical lines gives the CoM location.

A body is stable if a vertical line through its CoM passes within its base of support. Wider bases and lower centres of mass give greater stability.

An object will topple when its CoM moves beyond the edge of its base of support. Racing cars are wide and low for this reason.
A force of 50 N acts at 40° above the horizontal. Find its horizontal and vertical components.
1Horizontal component: Fₓ = F cosθ = 50 × cos(40°)
2Fₓ = 50 × 0.766 = 38.3 N
3Vertical component: Fᵧ = F sinθ = 50 × sin(40°)
4Fᵧ = 50 × 0.643 = 32.1 N
Fₓ = 38.3 N (horizontal), Fᵧ = 32.1 N (vertical)
A uniform beam of weight 200 N and length 4.0 m is supported at both ends. A 500 N load is placed 1.5 m from the left end. Find the reaction forces at each support.
1Let R_L = left reaction, R_R = right reaction. Condition 1: R_L + R_R = 200 + 500 = 700 N
2Take moments about the left end (eliminates R_L): R_R × 4.0 = 200 × 2.0 + 500 × 1.5
34 R_R = 400 + 750 = 1150, so R_R = 287.5 N
4R_L = 700 − 287.5 = 412.5 N
R_L = 412.5 N, R_R = 287.5 N
Two hands grip a steering wheel of diameter 0.35 m, each applying a force of 15 N tangentially in opposite directions. Calculate the torque of the couple.
1Perpendicular distance between the two forces = diameter = 0.35 m
2Torque = F × d = 15 × 0.35
Torque = 5.25 N m
A uniform rod AB of mass 2.0 kg and length 1.2 m has a 5.0 kg mass attached at end B. Find the position of the centre of mass from end A.
1Rod's CoM is at 0.6 m from A; mass 5.0 kg is at 1.2 m from A
2x̄ = (m₁x₁ + m₂x₂) ÷ (m₁ + m₂)
3x̄ = (2.0 × 0.6 + 5.0 × 1.2) ÷ (2.0 + 5.0) = (1.2 + 6.0) ÷ 7.0 = 7.2 ÷ 7.0
Centre of mass is 1.03 m from end A

Q1. Which of the following is a vector quantity?

Q2. A force of 30 N acts at 60° to the horizontal. What is the vertical component of this force?

Q3. State both conditions for a rigid body to be in static equilibrium.

Q4. A spanner applies a force of 25 N at a perpendicular distance of 0.18 m from a nut. What is the moment applied?

Q5. A uniform plank of length 3.0 m and mass 4.0 kg sits on a pivot at its centre. A 6.0 kg mass is placed 1.0 m from the left end. How far from the right end must a 3.0 kg mass be placed to achieve balance?

Challenge Q1. A ladder of mass 20 kg and length 5.0 m leans against a smooth vertical wall at 70° to the horizontal. A person of mass 70 kg stands 2.0 m up the ladder. Calculate the reaction forces at the wall and ground, assuming the ground is rough.

Challenge Q2. A composite object consists of a solid uniform square plate (side 0.4 m, mass 3.0 kg) with a solid uniform circle (radius 0.1 m, mass 1.5 kg) attached at its top-right corner. Taking the bottom-left corner of the square as origin, find the x and y coordinates of the overall centre of mass.

Challenge Q3. Explain why a racing car has a very wide wheelbase and very low centre of mass. Use the concept of centre of mass and toppling to justify your answer.