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Motion in a Straight Line
When acceleration is constant — a car braking steadily, a stone falling freely — five equations connect displacement , initial velocity , final velocity , acceleration and time . Each equation leaves out one of the five quantities, so if you know three, one equation will always give you a fourth. These are the equations.
The big picture
The suvat equations are what calculus gives when acceleration is constant: integrate once to get , again to get , and eliminate or to get the rest. So they are not five facts to memorise but one idea written five ways. The real skill is modelling: choosing a positive direction, listing the known and wanted quantities, spotting which quantity is irrelevant, and recognising where one stage of motion ends and another begins. Vertical motion under gravity is the classic application, with throughout the flight, and the same thinking extends directly to projectiles in two dimensions.
What you'll be able to do
- Derive and use the five constant-acceleration equations
- Select the appropriate equation by identifying known and unknown quantities
- Solve problems involving vertical motion under gravity
- Handle multi-stage motion and two objects moving in the same line
The suvat equations
For motion in a straight line with : is displacement, initial velocity, final velocity, acceleration, time.
Integrating with at gives ; integrating again with at gives . The others follow by elimination.
List , fill in what is known, mark what is wanted, and choose the equation that does not contain the fifth quantity.
Example 1A train decelerates uniformly from 30 m s⁻¹ to 12 m s⁻¹ over a distance of 420 m. Find the deceleration and the time taken.
Tip — A deceleration is a negative acceleration. Write in the equations, but you may quote "deceleration 0.9 m s⁻²" in the answer.
Vertical motion under gravity
Objects moving freely under gravity have constant acceleration m s⁻² downwards, if air resistance is ignored. OCR uses unless told otherwise.
Taking upwards as positive gives for the whole flight — on the way up, at the top, and on the way down.
At the highest point the velocity is momentarily zero, but the acceleration is still .
Example 1A ball is thrown vertically upwards at 14.7 m s⁻¹ from a point 2 m above the ground. Find the greatest height above the ground and the time until it hits the ground.
Solving for the whole flight in one equation works because acceleration is the same throughout. There is no need to split into "up" and "down" stages — just use the correct signed displacement for the end point.
Multi-stage motion
If acceleration changes part-way through, split the motion into stages with constant acceleration in each. The final velocity of one stage is the initial velocity of the next.
A velocity–time sketch is often the fastest way to organise a multi-stage problem, since distances are areas.
Example 1A cyclist accelerates from rest at 0.5 m s⁻² for 12 s, then continues at constant speed. How far has she travelled after 40 s?
Two objects in the same line
When two objects move along the same line, write each one’s displacement from a common origin as a function of time, then set them equal to find when they meet.
Take care if they start at different times — the later one has been moving for seconds.
Example 1Car A passes a point at a constant 20 m s⁻¹. At that instant car B starts from rest at and accelerates at 2.5 m s⁻² in the same direction. When and where does B catch A?
Tip — The solution is the moment they are together at the start. Always interpret each root rather than discarding one silently.
Think like an examiner
- Write out with known values before choosing an equation.
- State the positive direction and sign accordingly.
- Use m s⁻² and give answers to 3 significant figures unless told otherwise.
- Comment on modelling assumptions such as air resistance where relevant.
Common misconceptions
Constant acceleration
Stretch yourself
A stone is dropped from rest at the top of a cliff. One second later a second stone is thrown vertically downwards from the same point at 12 m s⁻¹. Both reach the sea at the same instant. Find the height of the cliff. Take m s⁻².
Hint — Let the first stone fall for seconds; the second falls for seconds. Equate their displacements.
Reveal solution
Questions students ask
How do I choose which suvat equation to use?
Why is sometimes 9.8 and sometimes 9.81?
Can suvat give negative time?
What assumptions are made in free-fall problems?
Key takeaways
- Five suvat equations apply only to constant acceleration.
- List known and wanted quantities; use the equation without the fifth.
- Under gravity, (up positive) throughout the motion.
- Split multi-stage motion; velocity carries over between stages.
- For two objects, equate displacements from a common origin.
How this fits the course
Related
Leads to
Test yourself
Answer a few questions, then review anything you missed.
Keep practising
Start with the quiz above to check the key ideas. You can also choose another topic from the practice library.
Related lessons
All 8 lessons- Same chapterDisplacement, Velocity and AccelerationUnderstanding the fundamental concepts of motion.
- Same chapterMotion GraphsInterpret displacement–time and velocity–time graphs
- Same chapterVariable AccelerationDifferentiate to obtain velocity and acceleration from displacement
Put the methods into practice: see how A-Level maths duels work. An account is required to play; the overview and sample are public.