Experiment: Determination of g by Time of Flight

1. Aim

To determine acceleration due to gravity by measuring time taken by a freely falling steel ball over a known distance.


2. Apparatus / Components Required


3. Theory & Principle

For free fall from rest:

\[S=\frac{1}{2}gt^2 \quad \Rightarrow \quad g=\frac{2S}{t^2}\]

Measure drop height $S$ and time of flight $t$ to compute $g$.

Example from setup: $S=27\text{ cm}$ with $t\approx0.2354\text{ s}$ gives $g\approx974.5\text{ cm/s}^2$.


4. Circuit Diagram / Setup

  1. Fix electromagnet at known height.
  2. Place contact sensor directly below drop path.
  3. Hold steel ball with electromagnet and release under software control.
  4. Measure vertical distance from ball’s lowest point to sensor.

5. Procedure

  1. Measure $S$ accurately.
  2. Perform one release and verify trigger timings.
  3. Run repeated trials (50-100 readings recommended).
  4. Save time data (tof.csv).
  5. Compute $g$ for each reading.
  6. Plot histogram and fit Gaussian for random error estimate.


6. Observation Table

Trial $S$ (m) $t$ (s) $g=2S/t^2$ (m/s$^2$)
1      
2      
3      
     
Mean      

7. Results and Discussion


8. Precautions

  1. Keep ball release point fixed for all trials.
  2. Ensure sensor contact is reliable and noise-free.
  3. Minimize lateral motion during release.
  4. Use enough trials to separate random and systematic error.

9. Troubleshooting

Symptom Possible Cause Corrective Action
Very high/low $g$ Wrong distance reference Re-measure $S$ from correct point
Large scatter in $t$ Irregular release mechanics Improve magnet-ball alignment
Missed impacts Sensor contact issue Recheck contact plate wiring

10. Viva-Voce Questions

Q1. Why does delayed release affect measured g?

Ans: Timing starts before actual free fall if magnetic hold decays slowly, increasing measured $t$ and lowering calculated $g$.

Q2. Why take many trials?

Ans: To estimate uncertainty and separate random fluctuations from systematic bias.