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AQA 6.5 / PHYSICS

Forces

Explore pushes and pulls, springs, motion and stopping safely. Use diagrams, worked examples and practical evidence to explain how forces change motion. Higher-only ideas are clearly labelled.

Supported GCSE version · Clear examples, worked calculations and optional challenges.

Foundation & Higher78 main + 6 challenge questionsSave and return any time

Understand the science

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YOUR TOPIC GUIDE

Forces

Work through one section at a time. Higher-only material is labelled explicitly; optional challenges can also use Foundation content.

Words to know

Scalar

A quantity with size only, such as mass or time.

Vector

A quantity with both size and direction, such as force or velocity.

Resultant force

The single force with the same effect as all the forces together.

Weight

The gravitational force on an object, measured in newtons.

Mass

The amount of matter in an object, measured in kilograms.

Centre of mass

The point through which the weight can be considered to act.

Displacement

Distance in a stated direction from start to finish.

Velocity

Speed in a stated direction.

Acceleration

Change in velocity per second, measured in m/s².

Work done

Energy transferred by a force acting through a distance.

Extension

Increase in length compared with the unloaded length.

Elastic deformation

A change of shape that is reversed when forces are removed.

Inelastic deformation

A change of shape that remains after forces are removed.

Spring constant

Force needed per metre of extension within the proportional range; measured in N/m.

Limit of proportionality

The point beyond which force and extension are no longer directly proportional.

Terminal velocity

Constant velocity reached when resistance balances weight during a fall.

Inertia (Higher only)

The tendency to stay at rest or at constant velocity.

Inertial mass (Higher only)

A measure of how difficult velocity is to change; resultant force divided by acceleration.

Thinking distance

Distance travelled during the driver’s reaction time.

Braking distance

Distance travelled from the brakes acting until the vehicle stops.

Momentum (Higher only)

Mass multiplied by velocity, measured in kg m/s.

Closed system (momentum)

A system with no resultant external force, so its total momentum is conserved.

1. Meet the main forces

A force is a push or pull caused by objects interacting. Forces can change an object’s motion or shape. We measure them in newtons (N).

Contact: objects must touch, including contact with air or water. Non-contact: the force can act across a gap.

On the ground: weight, support and friction

A supported book with upward normal contact force and downward weight; a box sliding right with friction left.
Always name the force and the object it acts on. “Normal” means at right angles to the surface.
ForceWhat it doesDirection or example
Weight (gravity)
Non-contact
The gravitational pull on an object.Towards the centre of Earth — usually drawn downwards. Mass is measured in kg; weight is a force in N.
Normal contact force
Contact
A surface pushes back on an object pressing against it. Also called the support force or normal reaction.A table pushes up on a book, at right angles to the tabletop.
Friction
Contact
Opposes sliding, or the tendency to slide, between surfaces.Acts along the surfaces. It can also provide grip: the road pushes a driven tyre forwards.

Moving through air or water

Aircraft with forward thrust and backward air resistance; floating boat with upward upthrust and downward weight.
Air and water are fluids. Their forces count as contact forces even when you cannot see the contact.
ForceWhat it doesDirection or example
Air resistance / water resistance (drag)
Contact
A fluid resists an object moving through it.Opposes motion relative to the air or water. Air resistance acts upwards on a ball falling through still air.
Thrust / driving force
Contact
A force that propels an object.An aircraft’s propeller pushes air backwards; the air pushes the aircraft forwards. On a car, the road provides the forward driving force on the tyres.
Upthrust
Contact
An upward force from a fluid on an object in it.Water pushes up on a boat. Floating at rest means upthrust balances weight; sinking objects still experience upthrust.

Pulling and stretching

Hanging load with upward rope tension and downward weight; stretched spring exerting a restoring force towards the fixed end.
A rope pulls along its length. A spring’s force acts to restore its original shape.
ForceWhat it doesDirection or example
Tension
Contact
A pulling force transmitted through a taut rope, string or cable.Acts along the rope, away from the attached object. An ordinary rope cannot push.
Elastic force / spring force
Contact
A stretched or compressed elastic object pushes or pulls back.Towards its original shape: a stretched spring pulls its ends together; a compressed spring pushes them apart.

Across a gap: magnets and charges

Two bar magnets with unlike poles facing attract; a charged balloon attracts small paper pieces across a gap.
Non-contact forces still involve two interacting objects.
ForceWhat it doesDirection or example
Magnetic force
Non-contact
Attraction or repulsion involving magnets; attraction between a magnet and magnetic material.Unlike poles attract; like poles repel. A magnet attracts iron even if the iron was not already a permanent magnet.
Electrostatic force
Non-contact
Attraction or repulsion involving electric charges.Unlike charges attract; like charges repel. A charged object can also attract neutral objects, such as small paper pieces.
Before a force question, ask: Which object am I studying? What is touching it? Are gravity, magnets or electric charges acting across a gap? Then name each force and add its direction. “Movement” and “energy” are not names of forces.

2. Describe the push or pull

A force is a push or pull caused by an interaction between objects. Force is measured in newtons, N.

Scalar: size onlyVector: size and direction
Mass, time, distance, speed, energyForce, displacement, velocity, acceleration, momentum
Two rightward force arrows with lengths in the ratio one to two.
When drawing vectors, use one scale and include arrowheads.

Magnitude means size. “20 N” gives the magnitude; “20 N east” also gives the direction.

3. What is touching what?

Contact forcesNon-contact forces
Friction, air resistance, tension in a rope, normal contact force from a surfaceGravity, electrostatic force, magnetic force

Normal contact force acts at right angles to a surface. Tension is a pulling force transmitted through a stretched rope or cable. Identify both objects in an interaction, not just one.

Two opposite interaction arrows for a tyre and road, and for Earth and a ball.
Forces can act even when the objects are separated.

4. Mass and weight are different

Mass is measured in kilograms. Weight is the gravitational force on an object, measured in newtons. A gravitational field is a region where a mass experiences a force.

Weight = mass × gravitational field strength
W = mg. Use kg, N/kg and N. The value of g will be given in calculations.
The same two kilogram case on Earth and the Moon, with calculated weights.
Moving the case changes its weight, not its mass.
  • Use a calibrated spring balance or newtonmeter to measure weight.
  • Weight acts towards Earth’s centre. In a diagram, draw it acting at the object’s centre of mass.
  • At a fixed g, W ∝ m: doubling the mass doubles the weight.

Rearrange: m = W ÷ g. For W = 49 N and g = 9.8 N/kg, m = 5.0 kg.

5. Combine forces on one object

The resultant force is one force with the same effect as all the forces on an object together.

  1. Same line and same direction: add the forces.
  2. Same line and opposite directions: subtract the smaller from the larger.
  3. Give the direction of the larger force.
A car with 700 newtons drive right and 500 newtons resistance left.
The diagram shows horizontal forces only.
A zero resultant means no change in velocity. It does not necessarily mean the object is stationary.

6. Higher only: forces in two dimensions

A free-body diagram shows only the forces acting on the chosen object. Replace the object with a dot or simple outline; label each force and its direction.

A scale grid showing four newtons east followed by three newtons north and the resultant diagonal.
Use a ruler and protractor to find the resultant’s size and direction. Scale drawings are the required method here.
  1. Choose a scale, such as 1 cm represents 1 N.
  2. Draw the first force, then draw the second from its arrowhead.
  3. The resultant runs from the first tail to the final head.

Resolving does the reverse: replace one force with two perpendicular components. Draw a rectangle with the original arrow as its diagonal. The two sides show forces with the same combined effect.

For equilibrium, the resultant is zero. A force polygon drawn head to tail closes.

7. A force can transfer energy

Work done is energy transferred by a force moving an object. The distance must be measured along the force’s line of action.

Work done = force × distance
W = Fs. Work W in J, force F in N, distance s in m. Here W means work; in W = mg it means weight.
Trolley pulled by a thirty newton force through four metres.
One joule is one newton-metre: 1 J = 1 N m.

Rearrange: F = W ÷ s and s = W ÷ F. Convert centimetres to metres first. Friction transfers energy to thermal stores, increasing the temperature of objects and surroundings.

8. Stretch, compress or bend

Spring regains original shape after release; bent wire stays bent.
Compare shape before loading and after release.

Changing an object’s shape is deformation. A stationary object needs forces at more than one point: pulling both ends of a spring, pressing both ends of a foam block, or supporting a ruler while pushing its middle.

Elastic deformationInelastic deformation
The object returns to its original shape when forces are removed.A permanent change of shape remains when forces are removed.
Extension is the increase in length, not the final length. A spring going from 8.0 cm to 11.0 cm extends 3.0 cm = 0.030 m.

9. A spring as a force meter

Up to its limit of proportionality, extension is directly proportional to force. A graph of force against extension is a straight line through the origin.

Force = spring constant × extension
F = ke. F in N, k in N/m, e in m. The same equation applies to compression in the proportional region.
Force versus extension graph linear to four newtons then curved.
Beyond the proportional region, do not assume a constant F ÷ e.

Worked example: F = 6.0 N and e = 0.030 m. Then k = F ÷ e = 200 N/m. A larger spring constant means more force is needed for the same extension.

10. Store energy by stretching

A stretching force does work and stores elastic potential energy. If the object is not permanently deformed, the work done equals the energy stored.

Eₑ = ½ke², up to the limit of proportionality.
With k = 200 N/m and e = 0.030 m:
Eₑ = 0.5 × 200 × 0.030² = 0.090 J.
  • Convert extension to metres before squaring it.
  • Doubling extension stores four times as much energy if k stays constant.
  • Do not use the final force × extension: the force increased during stretching.

11. Required practical 18: force and extension

Secured clamp stand with spring, slotted masses, pointer and vertical ruler.
The pointer and ruler must be close together to reduce reading error.
  1. Measure the unloaded spring length.
  2. Add a known weight and wait for the spring to stop moving.
  3. Read the new length at eye level. Calculate extension.
  4. Repeat for a range of weights. Repeat readings to identify anomalies and calculate means.
  5. Plot force against extension. Use the straight region to calculate k.
  6. Remove weights to check whether the spring returns to its starting length.

Keep the spring and ruler position the same. Secure the stand, place a tray below the masses and avoid stretching the spring so far that it breaks.

12. Distance or displacement?

A journey three hundred metres east followed by one hundred metres west.
Displacement links the starting and finishing positions directly.

Distance is the total path travelled. Displacement is the straight-line change of position, with a direction. A completed lap has a distance greater than zero but zero displacement.

13. How quickly does it move?

Typical movementApproximate speed
Walking1.5 m/s
Running3 m/s
Cycling6 m/s
Car in urban trafficAbout 13 m/s (roughly 30 mph)
TrainAbout 50 m/s; services vary
Sound in airAbout 330 m/s

Age, fitness, terrain and distance affect a person’s speed. Vehicle, wind and sound speeds also vary with conditions.

Distance = speed × time: s = vt.
Average speed = total distance ÷ total time, including stops.

Worked example: 600 m in 5.0 min means 600 ÷ 300 = 2.0 m/s. To convert km/h to m/s, multiply by 1000 then divide by 3600.

14. Velocity includes direction

Velocity is speed in a stated direction: for example, 8 m/s north. Two cyclists can have the same speed but different velocities if they travel in opposite directions.

Higher only: an object moving round a circle at steady speed still changes velocity because its direction changes. It is accelerating even though the speedometer reading is constant.
Circular track with equal length tangential velocity arrows at the top and right.
Higher only: constant speed does not mean constant velocity.

15. Distance–time graphs

Robot distance increases to twenty metres at four seconds, is constant until eight seconds, then reaches thirty metres at twelve seconds.
Read both axes and units before describing the motion.
Graph featureMeaning
Straight rising lineConstant speed
Horizontal lineStationary
Steeper rising lineGreater speed
Curve getting steeperSpeed increasing

Speed = gradient = change in distance ÷ change in time. For the first section: 20 ÷ 4 = 5.0 m/s. Use two well-separated points on a straight line.

16. Higher only: an instant on a curved graph

Curved distance-time graph and tangent at five seconds.
The tangent is a straight line with the same slope as the curve at the chosen time.
  1. Draw a tangent at the time required.
  2. Choose two widely spaced points on the tangent.
  3. Calculate its gradient in m/s. This is the speed at that instant.

For the illustrated tangent, (75 − 0) ÷ (10 − 2.5) = 10 m/s. Using the start and finish of the curved journey gives an average instead.

17. Changing velocity

Acceleration is change in velocity per second. Deceleration means slowing down. A positive/negative sign depends on the direction you chose as positive.

a = (v − u) ÷ t
a in m/s², velocities v and u in m/s, time t in s.
From 4 to 16 m/s in 6 s: a = (16 − 4) ÷ 6 = 2 m/s².

A car reaching 20 m/s in 10 s accelerates at about 2 m/s². Free fall close to Earth, without air resistance, is about 9.8 m/s².

Trolley velocity rises to eight metres per second, stays steady, then returns to zero.
The gradient gives acceleration: a horizontal velocity graph means constant velocity, not rest unless v = 0.

Higher only: the area under a velocity–time graph gives displacement. If motion stays in one direction, this is also distance. Split the area into rectangles and triangles or count grid squares. If velocity becomes negative, calculate signed areas for displacement and add the magnitudes for distance.

18. Constant acceleration and distance

For uniform (constant) acceleration, use:

v² − u² = 2as
v and u in m/s, a in m/s², s in m.
From rest, a = 2.0 m/s² over 25 m:
v² = 0² + 2 × 2.0 × 25 = 100, so v = 10 m/s.
  • Square the velocities, not their difference.
  • For slowing down, keep signs consistent.
  • Take the square root at the end if finding velocity.

19. Why falling objects stop accelerating

Three snapshots of a falling object with constant weight and increasing air resistance.
Arrow lengths compare force sizes; they do not show the distance travelled.
  1. At release, weight is greater than air resistance: the object accelerates downwards.
  2. As it speeds up, air resistance increases. The resultant force and acceleration decrease.
  3. Eventually air resistance equals weight. The resultant is zero.
  4. The object keeps falling at constant terminal velocity.

The same idea applies to falling through a liquid: the resisting force increases with speed.

20. Newton’s first and second laws

First lawSecond law
Zero resultant force: stay at rest or continue at constant velocity.A resultant force causes acceleration: F = ma.
F = ma: resultant force in N = mass in kg × acceleration in m/s².
A 500 kg trolley-system accelerating at 0.40 m/s² needs a resultant force of 200 N.
  • For constant mass, doubling the resultant force doubles acceleration.
  • For constant force, doubling mass halves acceleration.
  • Calculate the resultant, not just the driving force, before using F = ma.

Higher only: inertia is the tendency to remain at rest or at constant velocity. Inertial mass measures how difficult velocity is to change: m = F ÷ a.

21. Required practical 19: force, mass and acceleration

Trolley on a track pulled over a pulley, passing two light gates with a card.
Measure the moving mass of the whole trolley–hanger system, not just the trolley.
Investigate forceInvestigate mass
Move slotted masses from trolley to hanger. Pulling weight increases while total moving mass stays constant.Keep the hanger load constant and add masses to the trolley. Pulling force stays approximately constant.
  1. Measure the card length. Gate speed = card length ÷ time blocking the beam.
  2. Use speeds at two gates and travel time between them to find acceleration, or use a motion sensor/data logger.
  3. Release from the same position without a push. Repeat each setting and calculate a mean.
  4. Use a low-friction track. Account for friction rather than assuming hanger weight is exactly the resultant.
  5. Plot a against F at constant mass. For the mass investigation, plot a against 1/m to test inverse proportionality.

Use a catch tray and a trolley stop. Keep the hanging mass from striking the floor during measurement.

22. Newton’s third law

Two trolley interaction forces, equal and opposite, acting on different trolleys.
The arrows represent the forces each trolley exerts on the other.

Whenever two objects interact, the forces they exert on each other are equal in magnitude and opposite in direction. They are the same type of force and act on different objects.

Book on table: the table’s upward push on the book pairs with the book’s downward push on the table. The book’s weight pairs with its gravitational pull on Earth. Weight and support on the book are balanced forces, but not a third-law pair.

23. Stopping takes distance

Thinking stage then braking stage along the road.
Stopping distance = thinking distance + braking distance.
Thinking distanceBraking distance
Distance moved during the driver’s reaction time. At steady speed: speed × reaction time.Distance moved after brakes begin acting until the vehicle stops.
Increases with speed, tiredness, alcohol, some drugs and distraction.Increases with speed, poor tyres/brakes, and wet or icy roads.

Example: at 20 m/s with a 0.70 s reaction time, thinking distance = 14 m. Add a 25 m braking distance to get a 39 m stopping distance.

24. Measure reaction time fairly

Vertical ruler with a marked starting zero level and method reminders.
The ruler is caught between the tester’s fingers; use the supplied distance-to-time conversion table.

A partner holds a ruler with zero level with the top of your thumb. They release it without warning; you catch it. Read the fall distance and use a conversion table to find reaction time. Repeat and calculate a mean.

  • Keep the hand position, ruler, person and release method the same when testing one factor.
  • Practise first; learning can change results.
  • Typical reaction times are about 0.2–0.9 s.
  • A small laboratory test is not a complete model of driving in traffic.
Example ruler conversion table (ideal free fall)
Fall distance / cmReaction time / s
100.14
200.20
300.25
400.29
500.32

25. Braking transfers energy

Friction in the brakes does work, reducing the vehicle’s kinetic energy and warming the brakes. Road–tyre grip also limits the braking force.

  • Greater speed means greater kinetic energy to transfer.
  • At the same braking force, more kinetic energy means a longer braking distance.
  • At the same mass, doubling speed makes kinetic energy four times larger. With constant braking force, braking distance is then four times larger.
  • A larger braking force gives a larger deceleration, but very large decelerations can overheat brakes or cause loss of control.
Higher only: estimating road forces.
A 1000 kg car slows from 20 m/s to rest in 4 s.
a = (0 − 20) ÷ 4 = −5 m/s².
F = 1000 × (−5) = −5000 N: a 5000 N resultant opposite the motion.
Energy transferred from a slowing vehicle to warming brakes and surroundings.
Braking does work against friction.

26. Higher only: momentum and collisions

Two kilogram trolley moving right at three metres per second collides with stationary one kilogram trolley, then they join.
Treat both trolleys as one system when applying conservation of momentum.

Momentum = mass × velocity: p = mv, in kg m/s. Momentum has a direction.

In a closed system, with no resultant external force, total momentum before = total momentum after.
For the diagram: (2.0 × 3.0) + (1.0 × 0) = (2.0 + 1.0)v.
6.0 = 3.0v, so v = 2.0 m/s right.
  1. Choose a positive direction and give opposite motion a negative sign.
  2. Add the momenta of all objects before the event.
  3. Set this equal to total momentum afterwards.
  4. Do not assume kinetic energy is conserved in a collision. Momentum and energy are different quantities.