Principle of moments and centre of gravity

Key idea: In equilibrium, clockwise and anticlockwise moments about the same point balance. Include the object's weight acting through its centre of gravity.

Reading settings

On this page

Reading settings

Text size, line spacing and reading width for your lessons.

Text size
Line spacing
Reading width

Live preview

Take a moment to read at your own pace. Choose the text size and spacing that feel comfortable for you.

Pause after each idea, then explain it in your own words before moving on.

Narrower lines take effect when the screen has room.

Enlarged diagram

A heavy adult and a small child can balance on a seesaw if the adult sits closer to the middle. The seesaw stays level because the turning effects on it cancel: the child’s weight turns it one way and the adult’s turns it the other, equally. That balance, the principle of moments, lets you find an unknown force, distance or weight on any level beam, once you know where the beam’s own weight acts.

The principle of moments

A body is in equilibrium when the forces and the moments on it balance. A body at rest in equilibrium stays at rest: it does not start to turn and it does not start to move. A level seesaw with two children sitting still on it is in equilibrium.

For a body in equilibrium, the turning effects cancel. This is the principle of moments:

For a body in equilibrium, the sum of the clockwise moments about a pivot is equal to the sum of the anticlockwise moments about the same pivot.

sum of clockwise moments = sum of anticlockwise moments

For a body initially at rest and free to rotate about its pivot, a greater total clockwise moment makes it start to turn clockwise; a greater total anticlockwise moment makes it start to turn anticlockwise.

A balanced body still has forces acting on it. Balanced moments do not mean that individual forces disappear. The pivot also pushes up on the body, and for equilibrium the upward forces must equal the downward forces. The pivot’s force has no moment about the pivot, because its line of action passes through the pivot.

A balanced seesaw with two peopleA uniform 4.0 m seesaw plank is pivoted at its middle. A 400 N child sits 1.5 m to the left of the pivot. A 600 N adult sits an unknown distance d to the right of the pivot. The seesaw is level.pivot400 N600 N1.5 md
A balanced seesaw with two peopleA uniform 4.0 m seesaw plank is pivoted at its middle. A 400 N child sits 1.5 m to the left of the pivot. A 600 N adult sits an unknown distance d to the right of the pivot. The seesaw is level.pivot400 N600 N1.5 md
The child's weight turns the seesaw anticlockwise and the adult's weight turns it clockwise. It is level when the two moments are equal.

Worked example 1

Where must the adult sit?

Problem

In the seesaw above, the plank is uniform and pivoted at its middle. A 400 N child sits 1.5 m to the left of the pivot. How far to the right of the pivot must a 600 N adult sit for the seesaw to balance?

Show full solution
  1. Sort the moments

    Method

    The child’s weight is left of the pivot and the adult’s is right of it.

    Reason

    The plank’s own weight acts at its middle, through the pivot, so it has no moment about the pivot.

    Working

    Answer

    Anticlockwise: 400 × 1.5 = 600 N m. Clockwise: 600 × d.
  2. Apply the principle of moments

    Working

    Answer

    600 × d = 600, so d = 1.0 m to the right of the pivot.

Check your understanding 1 Apply the principle about one pivot

A uniform seesaw is pivoted at its middle. A 300 N child sits 2.0 m to the left of the pivot. Find that child’s moment, then the distance to the right where a 500 N child must sit for balance.

For equilibrium, which relation compares moments about the same pivot?
Unit: N m
Show the steps Optional working
Unit: N m
Unit: m

Show answer

The principle compares the sums of moments about the same pivot, for a body in equilibrium. It does not require equal forces on the two sides, or the absence of forces. For this uniform seesaw, the plank’s weight has zero moment about its midpoint pivot. The child’s anticlockwise moment is 300 × 2.0 = 600 N m. Set 500 × d = 600, giving d = 1.2 m to the right of the pivot.

Use the principle to solve problems

Follow the same steps for any balanced body:

  1. Choose one pivot. If a force you do not need acts at a point, taking moments about that point removes it, because its moment there is zero.
  2. For each force, find its perpendicular distance from that pivot, in metres. Measure from the pivot, not from the end of the beam.
  3. Label each moment clockwise or anticlockwise.
  4. Add up each side and write sum of clockwise moments = sum of anticlockwise moments.
  5. Solve for the unknown, then check the unit and whether the answer makes sense.

Worked example 2

An unknown force and the pivot’s force

Problem

A light horizontal beam is supported at a pivot O. A 36 N downward force acts 0.25 m to the left of O. An unknown downward force F acts 0.60 m to the right of O. The beam is in equilibrium. Find F and the upward force R from the pivot.

Show full solution
  1. Take moments about O

    Method

    Use O as the pivot.

    Reason

    R acts through O, so it has no moment about O and does not appear in the equation. “Light” means the beam’s weight can be ignored.

    Working

    Answer

    Clockwise: F × 0.60. Anticlockwise: 36 × 0.25 = 9.0 N m.
  2. Solve for F

    Method

    Apply the principle of moments.

    Reason

    The beam is in equilibrium.

    Working

    Answer

    0.60F = 9.0, so F = 15 N.
  3. Balance the forces

    Working

    Answer

    Upward force = total downward force: R = 36 + 15 = 51 N upward.

Check your understanding 2 A beam and its support

A 30 N load hangs 0.20 m to the left of a pivot on a light horizontal beam. Find the downward force needed 0.50 m to the right of the pivot for equilibrium, then the upward force from the pivot. Choose why the support has no moment about the pivot.

Show the steps Optional working
Unit: N m
Unit: N
Show the steps Optional working
Unit: N
Unit: N
Why is the support absent from the moment equation?

Show answer

30 × 0.20 = F × 0.50, so F = 12 N. The pivot pushes up with 30 + 12 = 42 N to balance the downward forces. Its line of action passes through the pivot, so its moment about that pivot is zero; this removes it from the moment equation, not from the forces on the beam.

Guided practice 3

Two loads on one side

About 6 min

Problem

A light beam is pivoted at its middle. A 20 N load hangs 0.50 m to the left of the pivot and a 10 N load hangs 0.20 m to the left of the pivot. A downward force F acts 0.40 m to the right of the pivot and the beam is level.

Try this before viewing the solution

Show the steps Optional working
Unit: N m
Unit: N m
Unit: N m
Show the steps Optional working
Unit: N m
Unit: N
Show the steps Optional working
Unit: N
Unit: N
Unit: N

Hints

Hint 1

one side

Both loads turn the beam the same way. Work out each moment, then add them.

Hint 2

the pivot force

The beam does not move up or down, so the upward force equals the total of the downward forces.

Show solution step by step
  1. Add the anticlockwise moments

    Method

    Both loads are left of the pivot.

    Reason

    Each has its own distance, so find each moment before adding.

    Working

    Answer

    20 × 0.50 + 10 × 0.20 = 12 N m
  2. Equate and solve

    Method

    F is the only clockwise moment.

    Reason

    The beam is in equilibrium, so the totals are equal.

    Working

    Answer

    0.40F = 12, so F = 30 N.
  3. Find the pivot force

    Working

    Answer

    R = 20 + 10 + 30 = 60 N upward.

Centre of gravity

Every part of an object has weight. You do not need to add up the moments of all those parts. The centre of gravity of an object is the single point at which its whole weight may be taken to act. When you take moments, draw one downward arrow for the object’s weight, through its centre of gravity.

  • A uniform beam or rule has the same weight in every equal length, so its centre of gravity is at its middle. For a metre rule, that is the 50 cm mark.
  • A non-uniform rod, such as a tapered rod, need not have its centre of gravity at its middle. Use the position given or measured, rather than assuming the midpoint.
  • If the pivot is at the centre of gravity, the weight acts through the pivot and has no moment. That is why a uniform plank balances on its own when pivoted at its middle, and why the balance point of a metre rule on a knife edge is its centre of gravity.

Check your understanding 3 A plank on its own

A uniform horizontal plank weighs 40 N and initially balances on a pivot at its middle. The pivot is moved 10 cm to the left of the middle, with the left end on your left. Find the moment of the plank’s weight about the new pivot and predict the direction it turns. Would doubling its weight restore balance?

Show the steps Optional working
Unit: m
Unit: N m
Turning direction
Would doubling the weight restore balance?

Show answer

The centre of gravity stays at the middle, now 0.10 m to the right of the pivot. The weight gives a moment of 40 × 0.10 = 4.0 N m clockwise, so the right side turns down. Doubling the weight would double this moment to 8.0 N m clockwise, not restore balance. The pivot’s own force still acts through the pivot and cannot balance that moment.

A metre rule pivoted away from its centre of gravityA uniform metre rule is pivoted at the 40 cm mark. Its 1.2 N weight acts downward at its centre of gravity, the 50 cm mark, 0.10 m to the right of the pivot. An unknown downward force F acts at the 10 cm mark, 0.30 m to the left of the pivot.0 cm100 cmpivotFweight 1.2 N0.30 m0.10 m
A metre rule pivoted away from its centre of gravityA uniform metre rule is pivoted at the 40 cm mark. Its 1.2 N weight acts downward at its centre of gravity, the 50 cm mark, 0.10 m to the right of the pivot. An unknown downward force F acts at the 10 cm mark, 0.30 m to the left of the pivot.0 cm100 cmpivotFweight 1.2 N0.30 m0.10 m
The rule's own weight acts at its centre of gravity, the 50 cm mark. Measure both distances from the pivot.

Worked example 4

Balancing a metre rule with its own weight

Problem

A uniform metre rule weighs 1.2 N and is pivoted at the 40 cm mark. What downward force F at the 10 cm mark keeps it level?

Show full solution
  1. Place the rule's weight

    Method

    The rule is uniform, so its centre of gravity is at the 50 cm mark.

    Reason

    The pivot is not at that point, so the rule’s weight has a moment and must be included.

    Working

    Answer

    The weight acts 50 - 40 = 10 cm = 0.10 m right of the pivot: clockwise.

  2. Measure F's distance from the pivot

    Method

    F acts at the 10 cm mark.

    Reason

    Distances are measured from the pivot, not from the end of the rule.

    Working

    Answer

    40 - 10 = 30 cm = 0.30 m left of the pivot: anticlockwise.

  3. Apply the principle of moments

    Working

    Answer

    F × 0.30 = 1.2 × 0.10, so F = 0.12/0.30 = 0.40 N downward.

Check your understanding 4 Where the weight acts

A uniform horizontal 1.5 m rod weighs 24 N and is pivoted 0.25 m from its left end. Where does its weight act, and what is the moment of the weight about the pivot, viewed with the left end on your left?

Unit: m
Show the steps Optional working
Unit: m
Unit: m
Unit: N m
Turning direction

Show answer

The rod is uniform, so its weight acts at its 0.75 m midpoint, 0.75 − 0.25 = 0.50 m right of the pivot. The moment is 24 × 0.50 = 12 N m clockwise.

A plank with a load, its own weight and an unknown forceA uniform 2.0 m plank is pivoted 0.75 m from its left end. A 200 N load hangs 0.20 m from the left end, which is 0.55 m left of the pivot. The plank's 120 N weight acts at its middle, 1.0 m from the left end and 0.25 m right of the pivot. An unknown downward force F acts at the right end, 1.25 m right of the pivot.pivot200 Nweight 120 NF0.55 m0.25 m1.25 m
A plank with a load, its own weight and an unknown forceA uniform 2.0 m plank is pivoted 0.75 m from its left end. A 200 N load hangs 0.20 m from the left end, which is 0.55 m left of the pivot. The plank's 120 N weight acts at its middle, 1.0 m from the left end and 0.25 m right of the pivot. An unknown downward force F acts at the right end, 1.25 m right of the pivot.pivot200 Nweight 120 NF0.55 m0.25 m1.25 m
Three forces have moments about the pivot. The plank's own weight is one of them.

Worked example 5

A plank that is not pivoted at its middle

Problem

A uniform 2.0 m plank weighs 120 N and is pivoted 0.75 m from its left end. A 200 N load hangs 0.20 m from the left end. Find the downward force F at the right end that keeps the plank level.

Show full solution
  1. Find each distance from the pivot

    Method

    Change each position along the plank into a distance from the pivot.

    Reason

    The plank is uniform, so its weight acts at its 1.0 m midpoint.

    Working

    Answer

    Load: 0.75 - 0.20 = 0.55 m left. Weight: 1.0 - 0.75 = 0.25 m right. F: 2.0 - 0.75 = 1.25 m right.

  2. Write the moment equation

    Method

    The load turns the plank anticlockwise; the weight and F turn it clockwise.

    Reason

    Both clockwise moments go on the same side.

    Working

    Answer

    200 × 0.55 = 120 × 0.25 + F × 1.25

  3. Solve

    Working

    Answer

    110 = 30 + 1.25F, so F = 80/1.25 = 64 N downward.

Check your understanding 5 Two errors

A uniform metre rule weighing 1.2 N is pivoted at the 30 cm mark. A 3.0 N load hangs at the 10 cm mark, and a downward force F at the 90 cm mark keeps the rule level. A learner writes 3.0 × 0.10 = F × 0.90. Find the load’s distance from the pivot, the rule’s weight moment and the correct force F.

Unit: m
Show the steps Optional working
Unit: m
Unit: N m
Show the steps Optional working
Unit: N m
Unit: N m
Unit: N m
Unit: m
Unit: N

Show answer

The learner used scale readings instead of distances from the pivot, and left out the rule’s weight. The load is 0.20 m left: 3.0 × 0.20 = 0.60 N m anticlockwise. The rule’s weight acts at 50 cm, 0.20 m right: 1.2 × 0.20 = 0.24 N m clockwise. F is 0.60 m right, so 0.60 = 0.24 + 0.60F and F = 0.36 ÷ 0.60 = 0.60 N.

Finding the weight of a stone with a metre ruleA uniform metre rule weighing 1.5 N is pivoted at the 40 cm mark. Its weight acts at the 50 cm mark, 0.10 m right of the pivot. A stone of unknown weight W hangs at the 15 cm mark, 0.25 m left of the pivot. The rule is level.0 cm100 cmpivotstone, Wweight 1.5 N0.25 m0.10 m
Finding the weight of a stone with a metre ruleA uniform metre rule weighing 1.5 N is pivoted at the 40 cm mark. Its weight acts at the 50 cm mark, 0.10 m right of the pivot. A stone of unknown weight W hangs at the 15 cm mark, 0.25 m left of the pivot. The rule is level.0 cm100 cmpivotstone, Wweight 1.5 N0.25 m0.10 m
With the rule level, the stone's moment balances the moment of the rule's own weight.

Guided practice 6

Weighing a stone with a metre rule

About 5 min

Problem

A uniform metre rule weighs 1.5 N. It is pivoted at the 40 cm mark, and a stone hangs from the 15 cm mark. The rule is level. Find the weight W of the stone.

Try this before viewing the solution

Show the steps Optional working
Unit: m
Unit: N m
Show the steps Optional working
Unit: N m
Unit: m
Unit: N

Hints

Hint 1

the rule's weight

The rule is the only other thing with a moment. Its weight acts at its centre of gravity.

Hint 2

distances

Measure both distances from the 40 cm mark, and change them to metres.

Show solution step by step
  1. Moment of the rule's weight

    Method

    The rule’s weight acts at the 50 cm mark.

    Reason

    A uniform rule’s centre of gravity is at its middle.

    Working

    Answer

    1.5 × 0.10 = 0.15 N m clockwise.
  2. Balance it with the stone

    Working

    Answer

    The stone is 40 - 15 = 25 cm = 0.25 m left of the pivot, so W × 0.25 = 0.15 and W = 0.60 N.

Check your understanding 6 A non-uniform rod

A horizontal non-uniform rod weighs 20 N. Positions in the table are measured from its left end.

Positions along a non-uniform rod
FeaturePosition / m
Left end0.00
Pivot0.50
Measured centre of gravity0.80
Right end1.20

A learner puts the rod’s weight at its 0.60 m midpoint. Correct the placement, then find the moment of the weight about the pivot.

Unit: m
Show the steps Optional working
Unit: m
Unit: N m
Turning direction

Show answer

The rod is not uniform, so its weight acts at the measured centre of gravity, 0.80 m, not the midpoint. That is 0.80 − 0.50 = 0.30 m right of the pivot, so the moment is 20 × 0.30 = 6.0 N m clockwise. The midpoint would give 20 × 0.10 = 2.0 N m, which is wrong for this rod.

Common mistakes

  • Saying a balanced beam has no forces on it. Several forces act; their moments cancel, and the pivot pushes up to balance the downward forces.
  • Leaving out the beam’s own weight. Unless the beam is light, its weight has a moment whenever the pivot is not at its centre of gravity.
  • Putting the weight of a non-uniform object at its middle. Use the centre of gravity that is given or measured.
  • Using scale readings as distances. A load at the 10 cm mark is 0.30 m from a pivot at the 40 cm mark.
  • Adding the loads on one side before multiplying. Loads at different distances have different moments, so find each moment and then add.
  • Taking some moments about one point and some about another. Measure every distance from the same pivot.

Spotted an error? Report a correction

Syllabus and review details

Last reviewed:

Back to top