A force is a push or pull. Forces have units of Newtons (N). We measure force using a Newton meter.
Scalar quantities have size ("magnitude") only and no direction. Example: mass.
Scalar quantities can be added normally. Example: 36 kg + 14 kg = 50 kg.
Examples of scalars: mass, distance, speed, energy, time, power.
Vector quantities have both size (magnitude) and direction. Examples: force, velocity, acceleration, displacement, weight, momentum.
In a scale diagram each force is drawn as an arrow of the appropriate length and direction (e.g. 1 cm = 1 N). Place the arrows head-to-tail. The resultant is the arrow from the start of the first to the end of the last.
Measure the resultant arrow length then multiply by the scale to find the magnitude of the resultant force.
If one vector is at right angles to another, we can use Pythagoras' theorem to find the resultant vector.
We can also use scale diagrams to find a resultant vector.
In a scale diagram, draw each vector as an arrow to scale. Join them head-to-tail. The resultant is the arrow from start to finish.
The resultant vector is found by placing vectors head-to-tail and drawing an arrow from the tail of the first to the head of the last.
The direction of the resultant can be measured with a protractor from the scale diagram.
All objects attract each other due to the force of gravity. The strength of gravity at the surface of a planet is determined by its mass.
Gravitational field strength (g) is a measure of the gravitational force per kilogram at a location. On Earth, g = 9.8 N/kg.
Weight is the force on an object due to gravity. Weight is a vector, measured in Newtons (N).
Mass is the amount of matter an object contains. Mass is a scalar with SI unit kilogram (kg). Mass stays the same wherever the object is; weight changes with g.
The Moon has less mass than Earth, so its gravitational field strength is less (≈1.625 N/kg).
W = weight (N), m = mass (kg), g = gravitational field strength (N/kg). On Earth: g = 9.8 N/kg unless told otherwise.
When quantities are given with prefixes, convert to SI units first.
The forces acting on any object can be shown using a force diagram (free body diagram) — labelled arrows showing all forces acting on the object.
When forces are perpendicular we can also look at them separately.
Sometimes there is no horizontal force. For example, if you throw an object (and air resistance is negligible) there is only gravity acting on it. Therefore it doesn't accelerate sideways at all — its horizontal velocity is constant.
If you shoot a bullet horizontally and drop a bullet at the same time, they will hit the ground at the same time — the sideways motion of the bullet doesn't matter as it is perpendicular to gravity.
When a force moves an object, work is done. Work done equals the energy transferred. The units of work done are Joules (J).
W = work done (J), F = force applied (N), s = distance moved in the direction of the force (m). The force and distance must be in the same direction.
When quantities have prefixes, convert to SI units first before substituting into W = F × s.
| Prefix | Symbol | Multiply by | Example (force) | Example (distance) | Example (energy) |
|---|---|---|---|---|---|
| Giga | G | ×10⁹ (×1 000 000 000) | 1 GN = 1×10⁹ N | 1 Gm = 1×10⁹ m | 1 GJ = 1×10⁹ J |
| Mega | M | ×10⁶ (×1 000 000) | 1 MN = 1×10⁶ N | 1 Mm = 1×10⁶ m | 1 MJ = 1×10⁶ J |
| kilo | k | ×10³ (×1 000) | 1 kN = 1 000 N | 1 km = 1 000 m | 1 kJ = 1 000 J |
| milli | m | ×10⁻³ (÷ 1 000) | 1 mN = 0.001 N | 1 mm = 0.001 m | 1 mJ = 0.001 J |
For there to be acceleration, there must be an unbalanced (resultant) force. In other words, if the resultant force acting on an object is zero, its motion does not change.
There are two cases:
When there is a resultant force, the object accelerates. The acceleration is directly proportional to the resultant force and inversely proportional to the mass.
F = resultant force (N), m = mass (kg), a = acceleration (m/s²). A bigger resultant force gives a bigger acceleration; a bigger mass gives a smaller acceleration.
Sometimes the resultant force is known and we need to find the mass or the acceleration instead. Always start from F = m × a, then rearrange to make the unknown the subject.
Remember to convert grams to kilograms first (1 g = 0.001 kg, so divide grams by 1 000).
Whenever one object exerts a force on a second object, the second object exerts an equal and opposite force back on the first.
Real situations involve several forces at once. To solve them, work in two steps.
When an object falls through the air, two forces act on it: its weight (downwards, caused by gravity) and air resistance (upwards, opposing its motion).
A velocity-time graph shows how the speed of a falling skydiver changes over time. Its shape tells the whole story of the jump.
| Time (s) | 0 | 5 | 10 | 15 | 20 | 25 | 30 | 35 | 40 | 45 | 50 | 55 | 60 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Velocity (m/s) | 0 | 28 | 43 | 48 | 50 | 50 | 50 | 49 | 12 | 10 | 10 | 10 | 0 |
Any mass that is moving carries momentum.
p = momentum (in kg m/s), m = mass (in kg), v = velocity (in m/s). Because the equation contains velocity (a vector), momentum is also a vector: it acts in the direction the object is moving.
If the momentum is known, you can still find a missing mass or velocity — always starting from p = m × v.
Always convert quantities to SI units before using p = m × v.
Conservation of momentum means that the total momentum before a collision or explosion equals the total momentum afterwards (when no external forces act).
For a collision where one object is initially at rest, work in two steps.
Conservation of momentum also applies to explosions (objects flying apart).
Thinking distance is the distance the vehicle travels while the driver reacts to a hazard — from seeing the hazard to pressing the brake — before the brakes are applied.
| Driver | Condition | Reaction time (s) |
|---|---|---|
| A | wide awake | 0.7 |
| B | using a hands-free phone | 0.9 |
| C | very tired and listening to music | 1.2 |
Braking distance is the distance the vehicle travels from the moment the brakes are applied to the moment it stops.