Back to top

Experiment: Determining gravitational acceleration g by free fall

To determine the value of gravitational acceleration g by timing a steel ball falling freely through measured heights.

  • Specialist SPM Physics tutoring
  • 5,000+ students helped
  • Experienced Physics teachers
  • Fully online 1-to-1, nationwide
  • Real 1-hour paid trial, from RM50/hr
  • Built on the official SPM syllabus

Aim

To determine the value of gravitational acceleration g by timing a steel ball falling freely through measured heights.

Variables

  • Manipulated: Height of fall, h
  • Responding: Time of fall, t
  • Constant: The same steel ball and release mechanism

Apparatus & materials

  • Steel ball
  • Electromagnet
  • Electronic timer
  • Trapdoor (release-to-timer switch)
  • Metre rule
  • Retort stand
  • Low-voltage power supply
  • Connecting wires

Procedure

  1. Mount the electromagnet at the top of the stand so it holds the steel ball, with a trapdoor switch directly below.
  2. Adjust the height of fall to h = 0.400 m, measured with the metre rule from the bottom of the ball to the trapdoor.
  3. Switch off the electromagnet to release the ball; this starts the timer, and the ball stops it on hitting the trapdoor.
  4. Record the time of fall t; repeat three times and take the average.
  5. Repeat for h = 0.500, 0.600, 0.700 and 0.800 m.
  6. Record h, t and calculate t² for each height.

Tabulating results

Record the height h in m, the three timings and their average t in s, and the derived value t² in s². Head each column with the quantity and unit.

The graph

Plot h (y-axis) against t² (x-axis). A straight line through the origin shows h is directly proportional to t².

Analysis

For free fall from rest, h = ½gt², so the gradient of the h–t² graph equals ½g. Therefore g = 2 × gradient.

Precautions

  • Measure h precisely from the bottom of the ball to the trapdoor.
  • Make sure the ball is released cleanly and falls straight onto the trapdoor.
  • Repeat each timing and average to reduce random error.

Force and Motion I · Graph skills

Sample results and what they show

These are example readings, not a mark scheme. For heights h = 0.400, 0.500, 0.600, 0.700, 0.800 m the time of fall t rose from about 0.286 s to 0.404 s, giving t² of about 0.082, 0.102, 0.122, 0.143 and 0.163 s².

The times are short, so the electronic timer matters: a hand-held stopwatch could not resolve 0.286 s reliably. Notice that t does not rise in proportion to h, increasing h from 0.400 m to 0.800 m only raises t from about 0.29 s to 0.40 s, not double, because h depends on t².

It is t² that is proportional to h: t² almost exactly doubles from 0.082 s² to 0.163 s² as h doubles. Repeat each drop three times and average, because a stray reading from a late release or the ball clipping the trapdoor will otherwise shift a point off the line.

Reading the graph and finding the answer

Plot h / m on the y-axis against t² / s² on the x-axis. The points should lie on a straight line through the origin, showing h is proportional to t².

Take the gradient from a large triangle on the best-fit line. Using (0.082 s², 0.400 m) and (0.163 s², 0.800 m): gradient = (0.800 − 0.400) m ÷ (0.163 − 0.082) s² = 0.400 m ÷ 0.081 s² = 4.94 m s⁻².

For free fall from rest h = ½gt², so the gradient equals ½g and therefore g = 2 × gradient = 2 × 4.94 m s⁻² = 9.88 m s⁻², close to 9.81 m s⁻². If the line has a small positive intercept on the h-axis, suspect that the ball began to move slightly before the timer started.

Marks examiners look for

State the variables: manipulated h / m, responding t / s, with the same steel ball and release mechanism kept constant. Measuring h from the bottom of the ball to the trapdoor is the point most often lost, measuring to the centre or the top introduces a systematic error.

Tabulate h / m, the three timings t₁, t₂, t₃ / s, the average t / s and t² / s², with units in the headings and consistent decimals. Repeating each timing and averaging is the fair-test move that earns credit, because it reduces the random error in a very short time.

On the graph, plot t² on the x-axis and draw a single best-fit line; a line forced through the origin when the points suggest otherwise loses the plotting mark. Finish with g quoted to a unit and sensible significant figures, and a conclusion linking the straight line to h ∝ t².

Do not treat air resistance as significant for a dense steel ball over these small heights.

Source: DSKP KSSM Physics Form 4 and 5 (Versi English) (Bahagian Pembangunan Kurikulum (BPK), KPM)

Written by the spmphysics.com.my editorial team.· Updated 5 Sept 2026

Frequently asked questions

Do I need a lab to practise?
No, the Paper 3 graph and analysis skills can be practised from home with example data.
Why is an electronic timer used instead of a stopwatch?
The times are only a few tenths of a second, and a hand-operated stopwatch carries about 0.2 s of reaction-time error, comparable to the reading itself. The electromagnet-and-trapdoor timer starts and stops automatically, so it resolves times like 0.286 s to the millisecond and keeps the random error small.
Why plot h against t² rather than h against t?
Because h = ½gt², a graph of h against t is a curve. Plotting h against t² straightens it into a line through the origin with gradient ½g, which is easy to use to find g.
Why measure the height to the bottom of the ball?
The ball starts to fall from its lowest point and the timer stops when that point reaches the trapdoor. Measuring to the bottom matches the actual distance fallen; measuring to the centre or top adds a fixed extra length that shows up as an intercept and makes g inaccurate.

Book a Trial Class

One-hour paid trial · Same-day reply · from RM50/hr

Book a Trial Class

One-hour paid trial · Same-day reply