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Kinematics of a particle in a straight line · Subtopic 2 of 3

Vertical Motion under Gravity

Without air resistance, every object near the Earth accelerates downwards at g=9.8g=9.8 m s⁻². Pick a positive direction (usually up), make a=−9.8a=-9.8, and use suvat. At the top of its flight an object is momentarily still: v=0v=0.

Edexcel YMA01 WME01≈ 35 minRevision 5 · updated 2026-10-27
Section 1 of 14

Learning objectives

  • Use a=±9.8a=\pm9.8 with a clear positive direction.
  • Find times and speeds for dropped objects.
  • Find greatest height and time to the top using v=0v=0.
  • Find when an object is at a given height, including starting above the ground.
Pause and think

A ball is thrown straight up and caught at the same height. Compare the time going up with the time coming down, and the speed thrown with the speed caught.

Section 2 of 14

Core idea

Start hereThrowing a ball straight up

Throw a ball up: it slows, stops for an instant, and falls back faster and faster. The whole flight has the same acceleration, 9.89.8 m s−2^{-2} downwards, so one set of suvat equations describes it from start to finish.

The big idea

Take up as positive: a=−9.8a=-9.8. At the top v=0v=0. Displacement below the start is negative.

1. Up and down

Ball projected up at 14.7 m/s
0.511.522.53246810120t (s)height (m)s = 14.7t − 4.9t²top: 11.0 m at 1.5 s
Symmetric: 1.51.5 s up, 1.51.5 s down. It returns to the start at 14.714.7 m s−1^{-1} downwards.
Worked exampleProjected up at 14.7 m s⁻¹

Time to the top, greatest height, time to return.

Goal
tt, ss, total tt.
Strategy
v=0v=0 at the top.
  1. 0=14.7−9.8t⇒t=1.50=14.7-9.8t\Rightarrow t=1.5
    v=u+atv=u+at.
  2. 0=14.72−19.6s⇒s=11.00=14.7^2-19.6s\Rightarrow s=11.0
    v2=u2+2asv^2=u^2+2as.
  3. 0=14.7t−4.9t2⇒t=30=14.7t-4.9t^2\Rightarrow t=3
    Back to s=0s=0.
Answer1.51.5 s; 11.011.0 m; 33 s.
✓ CheckSymmetric: up time = down time ✓.
Worked exampleFrom a 20 m tower

Same projection from the top of a 20 m tower. Time to reach the ground?

Goal
tt.
Strategy
Ground is s=−20s=-20.
  1. −20=14.7t−4.9t2-20=14.7t-4.9t^2
    s=ut+12at2s=ut+\frac12at^2.
  2. 4.9t2−14.7t−20=04.9t^2-14.7t-20=0
    Rearrange.
  3. t=14.7+216.09+3929.8=4.02t=\frac{14.7+\sqrt{216.09+392}}{9.8}=4.02
    Positive root.
Answer4.024.02 s.
✓ CheckMore than the 33 s round trip ✓.
Worked exampleTime above 9.8 m

For the 14.7 m s−1^{-1} projection, how long is the ball above 9.8 m?

Goal
Duration.
Strategy
Two times at that height.
  1. 9.8=14.7t−4.9t2⇒t2−3t+2=09.8=14.7t-4.9t^2\Rightarrow t^2-3t+2=0
    Divide by 4.9.
  2. t=1, 2t=1,\ 2
    Going up, coming down.
Answer11 s.
✓ CheckSymmetric about the top at 1.51.5 s ✓.
Common misconceptionMixed signs Choose a positive direction once and stick to it for uu, aa and ss.
Pause and think

A stone falls from rest for 2 s. Distance?

Summary

  • a=−9.8a=-9.8 (up positive).
  • Top: v=0v=0.
Key words
Projected
Given an initial velocity.
HistoryThe Leaning Tower story. A famous story says Galileo dropped two balls of different mass from the Leaning Tower of Pisa to show they land together. It may never have happened, but in 1971 astronaut David Scott dropped a hammer and a feather on the Moon, with no air, and they did hit the ground together.
Fun factFalling faster than you think. After just 33 seconds of free fall (ignoring air resistance) an object is moving at about 2929 m s⁻¹, over 100100 km/h. Skydivers stop accelerating at around 5555 m s⁻¹ because of air resistance.
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