3.02MechanicsCore

Motion in a Straight Line

When acceleration is constant — a car braking steadily, a stone falling freely — five equations connect displacement ss, initial velocity uu, final velocity vv, acceleration aa and time tt. 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 suvat\textbf{suvat} equations.

45 min Kinematics

The big picture

The suvat equations are what calculus gives when acceleration is constant: integrate aa once to get v=u+atv = u + at, again to get s=ut+12at2s = ut + \tfrac12at^{2}, and eliminate tt or uu 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 a=−ga = -g 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
1

The suvat equations

For motion in a straight line with constant acceleration\textbf{constant acceleration}: ss is displacement, uu initial velocity, vv final velocity, aa acceleration, tt time.

Integrating aa with v=uv = u at t=0t = 0 gives v=u+atv = u + at; integrating again with s=0s = 0 at t=0t = 0 gives s=ut+12at2s = ut + \tfrac12at^{2}. The others follow by elimination.

List s,u,v,a,ts, u, v, a, t, fill in what is known, mark what is wanted, and choose the equation that does not contain the fifth quantity.

v=u+atv = u + at
No ss.
s=12(u+v)ts = \tfrac12(u + v)t
No aa.
s=ut+12at2s = ut + \tfrac12at^{2}
No vv.
s=vt−12at2s = vt - \tfrac12at^{2}
No uu.
v2=u2+2asv^{2} = u^{2} + 2as
No tt.
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.
1u=30u = 30, v=12v = 12, s=420s = 420; want aa and tt.
2v2=u2+2asv^{2} = u^{2} + 2as: 144=900+840a144 = 900 + 840a, so a=−0.9a = -0.9.
3s=12(u+v)ts = \tfrac12(u + v)t: 420=21t420 = 21t, so t=20t = 20.
AnswerDeceleration 0.90.9 m s⁻²; time 2020 s.

Tip — A deceleration is a negative acceleration. Write a=−0.9a = -0.9 in the equations, but you may quote "deceleration 0.9 m s⁻²" in the answer.

2

Vertical motion under gravity

Objects moving freely under gravity have constant acceleration g=9.8g = 9.8 m s⁻² downwards, if air resistance is ignored. OCR uses g=9.8g = 9.8 unless told otherwise.

Taking upwards as positive gives a=−9.8a = -9.8 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 −9.8-9.8.

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.
1Up positive, a=−9.8a = -9.8. At the top v=0v = 0: 0=14.72−19.6s0 = 14.7^{2} - 19.6s, so s=11.025s = 11.025 m above the launch point.
2Greatest height above the ground: 13.02513.025 m.
3Ground is s=−2s = -2: −2=14.7t−4.9t2-2 = 14.7t - 4.9t^{2}, so 4.9t2−14.7t−2=04.9t^{2} - 14.7t - 2 = 0.
4t=14.7+216.09+39.29.8=14.7+15.9789.8=3.13t = \dfrac{14.7 + \sqrt{216.09 + 39.2}}{9.8} = \dfrac{14.7 + 15.978}{9.8} = 3.13 s (reject the negative root).
AnswerGreatest height 13.013.0 m; hits the ground after 3.133.13 s.
Why this works

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.

3

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?
1Stage 1: v=0+0.5×12=6v = 0 + 0.5 \times 12 = 6 m s⁻¹ and s=12×0.5×144=36s = \tfrac12 \times 0.5 \times 144 = 36 m.
2Stage 2: 28 s at 6 m s⁻¹ gives 168168 m.
Answer204204 m
4

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 t−t0t - t_{0} seconds.

Example 1Car A passes a point PP at a constant 20 m s⁻¹. At that instant car B starts from rest at PP and accelerates at 2.5 m s⁻² in the same direction. When and where does B catch A?
1A: s=20ts = 20t. B: s=1.25t2s = 1.25t^{2}.
21.25t2=20t1.25t^{2} = 20t gives t=0t = 0 or t=16t = 16.
3At t=16t = 16: s=320s = 320.
AnswerAfter 16 s, 320 m from PP.

Tip — The solution t=0t = 0 is the moment they are together at the start. Always interpret each root rather than discarding one silently.

Think like an examiner

  • Write out s,u,v,a,ts, u, v, a, t with known values before choosing an equation.
  • State the positive direction and sign gg accordingly.
  • Use g=9.8g = 9.8 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

Using suvat when acceleration varies with time.
Suvat only applies to constant acceleration; otherwise use calculus.
Taking a=+9.8a = +9.8 for a ball thrown upwards with up as positive.
Gravity acts downwards, so a=−9.8a = -9.8.
Saying acceleration is zero at the top of the flight.
Velocity is zero there; acceleration is still −g-g.
Using s=0s = 0 for the ground when launching from a height.
Measure displacement from the launch point: the ground is at s=−hs = -h.

Constant acceleration

v=u+atv = u + at
No ss.
s=ut+12at2s = ut + \tfrac12at^{2}
No vv.
v2=u2+2asv^{2} = u^{2} + 2as
No tt.
s=12(u+v)ts = \tfrac12(u + v)t
No aa.

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 g=9.8g = 9.8 m s⁻².

Hint — Let the first stone fall for tt seconds; the second falls for t−1t - 1 seconds. Equate their displacements.

Reveal solution
SolutionTaking down as positive: first stone s=4.9t2s = 4.9t^{2}; second stone s=12(t−1)+4.9(t−1)2s = 12(t - 1) + 4.9(t - 1)^{2}. Equating: 4.9t2=12t−12+4.9t2−9.8t+4.94.9t^{2} = 12t - 12 + 4.9t^{2} - 9.8t + 4.9, so 0=2.2t−7.10 = 2.2t - 7.1 and t=7.12.2=3.227t = \dfrac{7.1}{2.2} = 3.227 s. Height =4.9×3.2272=51.0= 4.9 \times 3.227^{2} = 51.0 m. Check with the second stone: it falls for 2.2272.227 s, covering 12×2.227+4.9×2.2272=26.73+24.31=51.012 \times 2.227 + 4.9 \times 2.227^{2} = 26.73 + 24.31 = 51.0 m ✓. ■\blacksquare

Questions students ask

How do I choose which suvat equation to use?
Identify which of s,u,v,a,ts, u, v, a, t is neither given nor wanted, and use the equation without it.
Why is gg sometimes 9.8 and sometimes 9.81?
OCR uses 9.8 m s⁻² unless a question states otherwise. Always use the value given.
Can suvat give negative time?
A quadratic in tt can have a negative root. It usually corresponds to a time before the motion started and is rejected — but say so.
What assumptions are made in free-fall problems?
The object is a particle, air resistance is negligible, and gg is constant over the height involved.

Key takeaways

  • Five suvat equations apply only to constant acceleration.
  • List known and wanted quantities; use the equation without the fifth.
  • Under gravity, a=−9.8a = -9.8 (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

Test yourself

Answer a few questions, then review anything you missed.

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