Required practicals › Measuring g by free fall
REQUIRED PRACTICAL 3Measuring g by free fall
Determining the acceleration due to gravity by timing a freely falling object.
Theory: Motion graphs and the SUVAT equations · Mass and weight
What you are trying to do
Determine the acceleration due to gravity by timing an object in free fall over a range of measured heights.
Apparatus
- Electromagnet holding a steel ball, on a tall clamp stand
- Trapdoor switch at the bottom, wired so the falling ball stops the clock
- Electronic timer started by the release circuit
- Metre rule; set squares help measure to the right points
Variables
- Independent: the drop height h
- Dependent: the fall time t
- Control: the same ball throughout, released from rest each time
Method
- Switching off the electromagnet releases the ball and starts the timer in the same instant; the ball breaking the trapdoor contact stops it.
- Measure the height from the bottom of the ball to the trapdoor. Measuring to the wrong point on the ball is the classic systematic error.
- Time three drops at each height and take the mean, then repeat over a range of heights from around 0.4 m to over a metre.
Analysis
- From rest, h = ½gt², so a graph of h against t² is a straight line through the origin with gradient g/2.
- Doubling the gradient gives g. The graph is the whole point: it averages every reading at once, and an intercept exposes a systematic error that a single calculation would silently absorb.
A worked set of readings
Mean of three electronically timed drops at each height:
| h / m | t / s | t² / s² |
|---|---|---|
| 0.400 | 0.286 | 0.0815 |
| 0.600 | 0.350 | 0.1223 |
| 0.800 | 0.404 | 0.1631 |
| 1.000 | 0.452 | 0.2039 |
| 1.200 | 0.495 | 0.2446 |
The gradient of h against t² is 4.905 m s⁻², and doubling it gives g = 9.81 m s⁻². The line passes through the origin, so no release delay crept in here; in a real run a small positive intercept on the t² axis is the delay's signature.
Where the uncertainty comes from
- Release delay: The electromagnet's field takes a moment to collapse, so the ball leaves slightly after the timer starts. That inflates every t equally, curving the small-h end and pulling g down: a systematic error, invisible to repeats.
- Timing resolution: Electronic timing is good to a millisecond; the shortest drops are under 0.3 s, so prefer larger heights where the percentage error is smaller.
- Height measurement: Bottom of ball to trapdoor, with the rule vertical; a set square against the stand helps.
- Random scatter: Small: release is electrical, not human. The mean of three still guards against the occasional glancing trapdoor hit.
What earns the marks
- Plot h against t² and double the gradient; never average single-reading values of g.
- Name the electromagnet delay as a systematic error and give its direction: measured times too long, so g comes out too small.
- Say the height was measured to the bottom of the ball.
- An intercept on the h against t² graph is evidence of the systematic error, not a reason to force the line through the origin.
- Explain why timing by hand with a stopwatch would not do: reaction time is a large fraction of a sub-second fall.
Safety
A steel ball dropped from over a metre stings: keep feet and fingers clear of the landing zone and clamp the stand so it cannot topple.
Method and analysis here follow the standard approach; your school may vary the apparatus. Always follow your teacher’s risk assessment in the lab.