1.5Motion, Forces and Energy
Moments — Cambridge IGCSE Physics 0625 Revision Notes & Topical Questions
15 min read 23 parts Lesson 38 of 91 Unit quiz
Lesson summary
1.5 Moments (Part 1) — IGCSE PHYSICS notes: Calculate the moment of a force and use the principle of moments to find an unknown force or distance on a balanced object.Definition — the moment of a force is its turning effect about a pivot.A force can make an object rotate clockwis…
- Everyday examples
- Deciding the direction
- Greater distance, smaller force
- Door example
- Spanner example
- Several forces
Section 1 of 23Moment of a force
Definition
- Definition the moment of a force is its turning effect about a pivot.
- A force can make an object rotate clockwise or anticlockwise about a fixed pivot.
Everyday examples
- Everyday examples a child on a see-saw, turning a spanner, opening a door, a crane lifting supplies, a screwdriver opening a paint tin, a tap, a wheelbarrow and scissors.
Deciding the direction
- Deciding the direction imagine only that force acting on the object about the pivot.
- If the object turns like the hands of a clock the moment is clockwise.
Section 2 of 23The moment equation
Equation
- Equation moment = force × perpendicular distance from the pivot, or M = Fd.
- The distance must be measured at right angles to the line of the force.
- On a horizontal beam the forces that cause moments are the ones acting up or down.
Units
- Units newton metres (N m), or N cm if the distance is in centimetres.
- Convert distances to metres unless told otherwise.
- Avoid N/m, which suggests division, and joules, which are never accepted for a moment.
Section 3 of 23Why distance matters
Why distance matters
Greater distance, smaller force
- Greater distance, smaller force a larger distance from the pivot needs less force for the same moment.
Door example
- Door example pushing next to the hinge needs a large force, while pushing at the handle needs much less.
Spanner example
- Spanner example a longer spanner makes a stiff bolt easier to turn.
Section 4 of 23Principle of moments (core)
Statement
- Statement for a balanced object the total clockwise moment about a pivot equals the total anticlockwise moment about that pivot.
Core use
- Core use one force on each side of the pivot, so F1d1 = F2d2.
Section 5 of 23Principle of moments (extended)
Several forces
- Several forces add all the moments on each side separately.
- Sum of clockwise moments = sum of anticlockwise moments.
- For example F2d2 = F1d1 + F3d3.
Weight of the beam
- Weight of the beam a beam pivoted at its centre contributes no moment because its distance from the pivot is zero.
- If the pivot is off-centre, the beam's own weight must be included.
Section 6 of 23Method for balance problems
1
Draw the beam, the pivot and every force with its distance.
2
Label each moment clockwise or anticlockwise.
3
Convert all distances to the same unit, preferably metres.
4
Write the principle: total clockwise = total anticlockwise.
5
Substitute Fd for each force and solve for the unknown.
6
Check the answer is sensible, for example the lighter person sits further out.
Section 7 of 23Moments in everyday devices
Lever
- Lever a long handle gives a large moment from a small effort.
Wheelbarrow
- Wheelbarrow the load is close to the wheel pivot, so a small lifting force at the handles balances it.
Crane
- Crane a counterweight on the short arm balances the load on the long arm.
Door
- Door the handle is placed far from the hinges to give a large moment.
Section 8 of 23More from the specification
More from the specification
Static equilibrium in structural loops
- Static equilibrium in structural loops equating clockwise and anticlockwise turning moments prevents rotation and ensures static stability throughout closed structural loops.
Principle of Moments and Equilibrium
- An object is in rotational equilibrium when there is no resultant turning effect,
- meaning total clockwise moments equal total anticlockwise moments about any pivot (M = F * d).What the symbols mean: moment (N m) · F = force (N) · d = perpendicular distance from the pivot to the line of the force (m)
Locating Center of Gravity of a Plane Lamina
- In a laboratory experiment, an irregular plane lamina is suspended from a clamp;
- vertical lines drawn using a plumb line intersect to locate its center of gravity.
Balancing Masses on a Meter Ruler
- Suspending calibrated masses at various distances along a balanced meter ruler demonstrates how varying force and perpendicular distance maintains equilibrium.
Center of Gravity Position and Stability
- Lowering the position of the center of gravity and broadening the base of an object increases physical stability against toppling.
Gravity
- A force of attraction between objects with mass.
Lamina
- A thin flat sheet.
Equilibrium
- State with zero net force.
Position
- Location relative to a reference point.
Resultant
- Vector sum of two or more vectors.
Topple
- Tip over because the weight acts outside the base.
Section 9 of 23Several forces on a beam
Extended principle
- Extended principle sum of clockwise moments = sum of anticlockwise moments.
- For forces F1 and F3 anticlockwise and F2 clockwise: F2d2 = F1d1 + F3d3.
Beam weight
- Beam weight a uniform beam pivoted at its centre contributes no moment because its weight acts through the pivot.
- If the pivot is elsewhere, the beam's weight acts at its centre and gives a moment.
Direction of each moment
- Direction of each moment decide it by imagining that force alone turning the beam.
Section 10 of 23Conditions for equilibrium
Definition
- Definition an object is in equilibrium when there is no resultant force and no resultant moment.
Two conditions
- Two conditions both must be satisfied.
- The forces are balanced, so there is no resultant force.
- The clockwise moments equal the anticlockwise moments, so there is no resultant moment.
Common error
- Common error stating only that the forces are balanced and forgetting the moments.
Section 11 of 23Equipment for demonstrating equilibrium
| Equipment | Purpose |
|---|---|
| Metre ruler with a hole at the centre | Forms the beam |
| Optical pin and cork, clamp stand | Act as the pivot |
| Two 100 g hangers and eight 100 g masses | Provide the forces |
| Cotton loops | Attach the hangers to the ruler |
| Modelling clay | Makes the unloaded ruler balance horizontally |
Section 12 of 23Method
1
Secure the pin in the clamp stand and mount the ruler on it so that it sits horizontal.
2
Hang unequal loads on each side while a second person steadies the beam.
3
Adjust the distances of the masses until the beam balances horizontally.
4
Record each mass and its distance from the pivot.
5
Repeat with different loads.
Variables
- Variables mass and distance are the independent variables, and the moment is the dependent variable.
Control
- Control the loops must have equal lengths and the pivot must stay at the ruler's centre.
Section 13 of 23Analysis, errors and safety
Analysis, errors and safety
Calculations
- F = mg and M = Fd for each side, with grams converted to kilograms and cm to metres.
- The results should show the anticlockwise moment equals the clockwise moment, so there is no resultant moment.
Systematic errors
- Systematic errors view the loops straight on to avoid parallax, check the loops have equal length and ensure the pin has no friction.
Random errors
- Random errors work away from draughts, use a spirit level to confirm the beam is horizontal and repeat to take a mean.
Assumptions
- Assumptions the cotton has negligible mass and each mass plus hanger is 100 g, which can be checked on a balance.
Safety
- Safety wear goggles, clamp the stand with a G clamp, stand while working and place a soft mat below the masses.
Section 14 of 23More from the specification
More from the specification
Moment of a force definition
- The moment of a force is a measure of its turning effect about a pivot, calculated as moment = force * perpendicular distance to the line of action.
Principle of moments for equilibrium
- For an object in rotational equilibrium, the sum of clockwise moments about any pivot must equal the sum of anticlockwise moments.
Centre of gravity and stability
- The centre of gravity is the single point where the total weight of a body may be considered to act;
- low centres of gravity and wide base areas maximize stability.
Turning effect
- Moment that rotates the coil.
Gravity
- A force of attraction between objects with mass.
Lamina
- A thin flat sheet.
Position
- Location relative to a reference point.
Topple
- Tip over because the weight acts outside the base.
Perpendicular
- At right angles.
Section 15 of 23What the centre of gravity is
Definition
- Definition the centre of gravity is the point through which the weight of an object acts.
Regular objects
- Regular objects a symmetrical object of uniform density has its centre of gravity at its point of symmetry.
- A sphere has its centre of gravity at its centre.
Hypothetical point
- Hypothetical point it can lie inside or outside the body.
- It moves when the shape changes, so a person leaning forward has a lower centre of gravity.
Force diagrams
- Force diagrams always draw the weight force from the centre of gravity.
Section 16 of 23Stability
Stable object
- Stable object its centre of gravity lies above its base.
Toppling
- Toppling if the line of action of the weight falls outside the base, a resultant moment turns the object over.
More stable designs
- More stable designs a low centre of gravity and a wide base.
- Cars, high chairs and Bunsen burners have wide bases.
Less stable designs
- Less stable designs tall objects on a narrow base topple easily.
- Bowling pins are designed to topple and lorries are advised to avoid exposed bridges in high wind.
Section 17 of 23Comparing stable and unstable objects
| Feature | More stable | Less stable |
|---|---|---|
| Centre of gravity | Low | High |
| Base | Wide | Narrow |
| Tilt before toppling | Large angle | Small angle |
| Example | Racing car | Bus (topples at about 45°; a car tilts to about 60°) |
Section 18 of 23Finding the centre of gravity of a lamina
1
Punch three holes near the edge of the lamina in different places.
2
Hang a cork horizontally in a clamp and hang the lamina from a pin through one hole.
3
Check that the lamina swings freely and let it settle.
4
Hang a plumb line from the same pin and mark where it passes over the lamina.
5
Repeat with the other holes to draw three lines.
6
The centre of gravity is where the lines cross.
7
Check by balancing the lamina on a pin tip at that point.
Section 19 of 23Why the method works and its errors
Why the method works and its errors
Principle
- Principle a hanging object settles with its centre of gravity directly below the pivot, so the plumb line passes through it.
- Two lines are enough to locate the point, and the third checks the first two.
Systematic errors
- Systematic errors view the plumb line straight on, use a sharp pencil and mark dots then rule the lines after removing the lamina.
Random errors
- Random errors allow the lamina to settle and punch the holes before the investigation, since later holes change the centre of gravity.
Safety
- Safety secure the clamp stand and push the sharp pin into a cork when not in use.
Section 20 of 23More about centre of gravity
Weight arrow
- Weight arrow it starts at the centre of gravity and points straight down.
Symmetry rule
- Symmetry rule a uniform rectangle has its centre of gravity where its diagonals cross.
Tilting
- Tilting an object tilted until its centre of gravity is above the edge of the base is on the point of toppling.
Lowering it
- Lowering it adding weight at the bottom lowers the centre of gravity and makes an object more stable.
Section 21 of 23More from the specification
1Rotational moment balancing loops
- Rotational moment balancing loops evaluating clockwise and anticlockwise moments about pivots confirms mechanical equilibrium in articulated structural loops.
2Definition of the Moment of a Force
- The moment of a force measures its turning effect about a fixed pivot, calculated as the force multiplied by the perpendicular distance from the line of action of the force to the pivot: Moment = F * d.
- (measured in N m)
3Principle of Moments for Rotational Equilibrium
- When an object is in rotational equilibrium, the total sum of clockwise moments about any pivot must equal the total sum of anticlockwise moments.
- (such as a balanced meter ruler or a see-saw with an adult and child)
4Laboratory Balancing Experiment
- In an experiment using a uniform metre ruler suspended horizontally from a clamp, known weights are hung at varying positions until balance is achieved, confirming that F1 * d1 = F2 * d2.
5Conditions for Complete Static Equilibrium
- For a planar rigid body to remain in complete equilibrium, the net external forces in all directions must be zero and the net turning moments about any point must be zero.
- (translational equilibrium)
6Principle of moments equilibrium
- Principle of moments equilibrium for a balanced beam in rotational equilibrium, total clockwise moments equal total anticlockwise moments about the pivot.
7Moment calculation
- Moment calculation moment equals applied perpendicular force multiplied by perpendicular distance from the pivot to the line of action.
8Balancing experimental beam
- Balancing experimental beam adjusting the position of a known mass on a graduated metre ruler verifies equilibrium conditions.
9Turning effect
- Moment that rotates the coil.
10M = Fd
What the symbols mean: moment (N m) · F = force (N) · d = perpendicular distance from the pivot to the line of the force (m)
11Clockwise
- Turning in the direction of a clock's hands.
12Anticlockwise
- Turning against the direction of a clock's hands.
13Distance
- Total length of path travelled, a scalar.
14Equilibrium
- State with zero net force.
15Position
- Location relative to a reference point.
16Perpendicular
- At right angles.
Section 22 of 23Key terms
| Term | Meaning |
|---|---|
| Moment | The turning effect of a force about a pivot, force × perpendicular distance. |
| Pivot | The fixed point about which an object turns. |
| Principle of moments | For a balanced object, total clockwise moment equals total anticlockwise moment. |
| Clockwise | Turning in the direction of a clock's hands. |
| Anticlockwise | Turning against the direction of a clock's hands. |
| Newton metre | The unit of moment. |
| Term | Meaning |
|---|---|
| Equilibrium | No resultant force and no resultant moment. |
| Resultant moment | The net turning effect after clockwise and anticlockwise moments are combined. |
| Pivot | The point about which a beam can turn. |
| Parallax error | An error from viewing a scale at an angle. |
| Uniform beam | A beam whose weight acts at its centre. |
| Term | Meaning |
|---|---|
| Centre of gravity | The point through which the weight of an object acts. |
| Stability | The tendency of an object to stay upright without toppling. |
| Plumb line | A thread with a weight that hangs vertically. |
| Lamina | A thin flat sheet. |
| Line of action | The line along which a force acts. |
Section 23 of 23Exam technique
1
Measuring the distance along the force instead of perpendicular to it.
2
Leaving distances in centimetres in one moment and metres in another.
3
Stating the principle as "the moments are equal" with no clockwise or anticlockwise.
4
Giving the unit of a moment as N/m or J — use N m.
1
Stating only that forces are balanced when asked for the conditions for equilibrium.
2
Using the distance from the end of the beam instead of from the pivot.
3
Adding the weight of a uniform beam as a moment when the pivot is at its centre.
4
Leaving masses in grams in M = mgd.
1
Saying the centre of gravity must be inside the object.
2
Confusing stability with weight — it depends on the base and the height of the centre of gravity.
3
Punching extra holes in the lamina after finding the point.
4
Using only one suspension line.
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