Centre Of Gravity (A Level)
Key idea: Use centre of gravity as the point where weight acts; optional sections extend to centre-of-mass calculations, laminas and stability.
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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. Centre of gravity (CoG)
The centre of gravity is the point through which the entire weight of an object may be considered to act.
In a uniform gravitational field, the centre of gravity coincides with the centre of mass.
For H2 Physics 9478, you must understand that a body’s weight may be taken to act at one point called its centre of gravity. Calculating centres of mass for particles or composite laminas, and detailed toppling geometry, are useful extensions rather than stated outcomes.
B. Centre of mass (CoM)
The centre of mass is the point that represents the average position of the mass distribution of a body.
C. Stability (idea)
Stability describes what happens after a small displacement:
- stable equilibrium: returns to its original position
- unstable equilibrium: moves further away
- neutral equilibrium: stays in its new position
2. Key ideas
- Centre of mass (discrete masses):
- x_CM = (∑ mᵢ xᵢ)/(∑ mᵢ), y_CM = (∑ mᵢ yᵢ)/(∑ mᵢ)
- For a uniform lamina (same thickness and density), mass ∝ area, so you can use area-weighting:
- x bar = (∑ Aᵢ xᵢ)/(∑ Aᵢ), y bar = (∑ Aᵢ yᵢ)/(∑ Aᵢ)
- Treat a hole/cut-out as a negative area (or negative mass).
- An object topples when the line of action of its weight falls outside its base of support.
- Lower CoG and wider base generally increase stability.
3. Detailed explanations
A. Centre of mass vs centre of gravity
- Centre of mass depends only on the mass distribution.
- Centre of gravity depends on the mass distribution and the gravitational field.
For most mechanics questions near Earth’s surface, we assume a uniform gravitational field, so the centre of gravity is at the same point as the centre of mass.
B. Optional extension: calculating a composite centre
If an object can be split into parts with known centres (e.g. rectangles, discs), you can find the overall centre using a weighted average.
Workflow:
- Choose axes and an origin.
- Split the object into parts and find each part’s centre coordinates (xᵢ, yᵢ).
- Use mass-weighting (or area-weighting for a uniform lamina) to find (x bar, y bar).
- For holes, use negative mass/area.
C. Optional extension: stability and toppling
An object is stable if, after a small tilt, there is a restoring moment that tends to return it to its original position.
A practical rule used in exam questions:
- draw the line of action of the weight (vertical line through the CoG),
- the object is stable as long as that line falls within the base of support,
- it topples once the line falls outside the base.
4. Common Mistakes
- Mixing up CoG (depends on the field) and CoM (depends only on mass distribution).
- Forgetting a hole is treated as negative mass/area in composite-shape questions.
- Using inconsistent axes/origin when combining parts.
- Assuming “low CoG” alone guarantees stability (base width matters too).
5. Exam Tips
- Use symmetry first (it often gives one coordinate immediately).
- Put the origin at a convenient corner/edge to reduce arithmetic.
- Keep work organised in a table: part, mass/area, (xᵢ,yᵢ), and mᵢxᵢ / Aᵢxᵢ.
- For stability questions, sketch the base and the weight line of action.
6. Worked Examples
Modelled example 1
Choosing the weight’s line of action
Problem
Study the worked solution
Replace the distributed weight
Method
Draw one downward force W = mg through the beam’s centre of gravity.Reason
In a uniform gravitational field, the whole body’s weight may be represented as acting at its centre of gravity.Working
W = mg vertically downward through the CoG.Use symmetry
Method
Place the force at the beam’s midpoint.Reason
A uniform beam has a symmetric mass distribution, so its centre of gravity lies halfway along it.Working
x_CoG = L/2 from either end.
Optional calculation practice
Guided practice 2
Two particles on a line
Optional extension
Try this before viewing the solution
Hints
Hint 1: set up the weighted mean
View solution step by step
Form the mass-weighted sum
Method
The position moment is 15 kg m.Reason
The 2.0 kg particle is at the origin, so only the second particle contributes.Working
(2.0)(0) + (3.0)(5.0) = 15 kg mDivide by total mass
Method
x_CM = 3.0 m.Reason
The centre-of-mass coordinate is the position moment per unit total mass.Working
x_CM = 15/(2.0 + 3.0) = 3.0 m
Common misconception 3
Three particles on a line
Learner claim
Try this before viewing the solution
View solution step by step
Identify the faulty assumption
Method
The three positions must not be weighted equally.Reason
Each particle’s contribution depends on both its mass and its position.Working
x_CM ≠ (0 + 2.0 + 5.0)/3 for unequal masses.Use mass weighting
Method
x_CM = 3.17 m.Reason
The largest mass at 5.0 m pulls the weighted mean toward that end.Working
x_CM = ((1.0)(0) + (2.0)(2.0) + (3.0)(5.0))/(1.0 + 2.0 + 3.0) = 19/6 = 3.17 m
Examiner practice 4
Centre of mass in 2D (point masses)
Optional examination-style extension
Try this before viewing the solution
View solution step by step
Find the total mass
1 markMethod
M = 6.0 kg.Reason
Both coordinate calculations use the same total mass.Working
M = 2.0 + 1.0 + 3.0 = 6.0 kgCalculate the x coordinate
2 marksMethod
x_CM = 0.667 coordinate units.Reason
Only the 1.0 kg mass has a non-zero x coordinate.Working
x_CM = (2.0(0) + 1.0(4.0) + 3.0(0))/6.0 = 0.667Calculate the y coordinate
2 marksMethod
y_CM = 1.00 coordinate units.Reason
Only the 3.0 kg mass has a non-zero y coordinate.Working
y_CM = (2.0(0) + 1.0(0) + 3.0(2.0))/6.0 = 1.00
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 the total mass and both weighted-coordinate calculations.
Challenge 5
Lamina with a square hole (negative area)
Optional extension
Try this before viewing the solution
Hints
Hint 1: represent the cut-out
View solution step by step
Represent the hole as negative area
Method
The remaining area is 20 cm².Reason
Removing material subtracts both area and its area moments.Working
A = 24-4 = 20 cm²Calculate the horizontal coordinate
Method
x bar = 2.6 cm.Reason
The removed top-right area shifts the centroid left.Working
x bar = (24(3.0)-4(5.0))/20 = 2.6 cmCalculate the vertical coordinate
Method
y bar = 1.8 cm.Reason
The removed top-right area also shifts the centroid downward.Working
y bar = (24(2.0)-4(3.0))/20 = 1.8 cm
Challenge 6
Toppling angle (stability rule)
Independent transfer
Try this before viewing the solution
Hints
Hint 1: draw the limiting triangle
View solution step by step
State the limiting condition
Method
The vertical line through the centre of mass passes through the pivot edge.Reason
Beyond this position, the weight produces a moment that continues the toppling motion.Working
weight line of action through pivotUse the centre geometry
Method
The horizontal and vertical offsets are 0.20 m and 0.40 m.Reason
A uniform rectangle’s centre is halfway across its width and height.Working
w/2 = 0.20 m, h/2 = 0.40 mCalculate the critical angle
Method
θ ≈ 26.6°.Reason
The limiting tilt rotates the centre until its horizontal offset from the pivot is zero.Working
tan θ = 0.20/0.40 = 0.5 ⇒ θ = 26.6°
7. Mind Stretchers
Mind stretcher 1: Does CoG always equal CoM?Extension
Explain why centre of gravity and centre of mass can differ in a non-uniform gravitational field (e.g. very far from Earth).
Click here to show/hide answer
Centre of mass depends only on how mass is distributed.
Centre of gravity depends on how gravitational field strength varies across the object. In a non-uniform field, different parts of the object experience different gravitational forces, so the single point where you can treat the weight as acting (CoG) may shift relative to the CoM.
Mind stretcher 2: Optional (Enrichment)Extension
A. Continuous mass distributions
For continuous mass distributions, the centre of mass can be found using integration.
This is beyond what most A Level exam questions require; composite shapes + symmetry is usually enough.
Mind stretcher 3: Why does lowering the centre of gravity increase stability?Extension
Explain why a lower CoG makes an object harder to topple, even if its base width stays the same.
Click here to show/hide answer
An object topples when the line of action of its weight falls outside the base.
With a lower CoG, you need a larger tilt angle before the vertical line through the CoG reaches the edge of the base. That means it is harder to reach the toppling condition, so stability increases.
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Course and syllabus information
- Course
- GCE A-Level H2 Physics
- Edition
- GCE A-Level H2 Physics 2027