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Estimating Acceleration Using Motion Experiments with a Cart and Free-Falling Ball Report

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Introduction

The experiment was conducted to estimate the acceleration due to gravity based on the kinematics equation of motion in three scenarios: a fan-powered cart, cart motion along an inclined plane, and a free-falling ball. The relationships between velocity and time and position and time were used to assess whether the experiment results agreed with the theory of motion and gravity. When the equations generated from the graphs matched the theoretical equations, the researcher proceeded to calculate acceleration due to gravity. The researcher realized an error of 51%. From the graphs, it was deduced that the report results were consistent with the laws of motion.

Data Analysis

A Cart on a Track

The observed measurements and final results did not have a clear pattern. Furthermore, there was no clear trend in the graph. The plots were random values – they could not be predicted. The tables below indicate the data results from the various experiments.

  • Initial Position, x0 = 2.0 m
  • Final Position, x = 0.3 m
  • Distance, Δx = 2.0 – 0.3 = 1.7 m

Table 1a. Time Taken by a Fan-Powered Cart to Travel the Specified Distance

Stopwatch 1Stopwatch 2
Trial 14.12 s4.25 s
Trial 24.59 s4.57 s
Trial 34.75 s4.75 s

Average of Trials = (4.12+4.25+4.59+4.57+4.75+4.75)/6 = 4.505 s
Cart Acceleration, a = 2 Δx/t2 = 2(1.7)/4.5052 = 0.168 m/s2

Table 1b. Velocity vs. Time Graph.

Acceleration, a (m/s2)
Coefficient ‘A’0.04482A = a, or A = (½)a = 0.0448 x2 = 0.0896
Coefficient ‘m’0.08840.0884

A Cart Down the Incline

Average of Accelerations from Distance and Velocity Graphs = (0.0896+0.0884)/2 = 0.089 m/s2

  • Initial Position, x0 = 2.0 m
  • Final Position, x = 0.3 m
  • Distance Traveled, Δx = 1.7 m

Table 2a. Time Taken by a Cart to Travel the Specified Distance Along an Inclined Plane

Stopwatch 1Stopwatch 2
Trial 12.56 s2.50 s
Trial 22.43 s2.53 s
Trial 32.56 s2.50s

Average of Trials = (2.56+2.5+2.43+2.53+2.56+2.5)/6 = 2.51 s
Cart Acceleration, a = 2 Δx/t2 = 2(1.7)/2.512 = 0.54 m/s2

Table 2b. Velocity vs. Time Graph

Acceleration, a (m/s2)
Coefficient ‘A’0.2070.414
Coefficient ‘m’0.4430.443

Average of Accelerations from Distance and Velocity Graphs = (0.414+0.443)/2 = 0.429 m/s2
Incline Angle, θ = sin-1(h/H) = sin-1(0.13m/2.11m) = 3.53°
Acceleration due to Gravity, g = a/sinθ = 6.97 m/s2

A Free Fall Ball

Table 3a. Time Taken by a Ball to Fall the Specified Distance

Stopwatch 1Stopwatch 2
Trial 10.35 s0.69 s
Trial 20.34 s0.37 s
Trial 30.47s0.62 s

Average of Trials = (0.35+0.65+0.34+0.37+0.47+0.62)/6 = 0.47 s
Acceleration, a = 11.6 m/s2

Table 3b. Velocity vs. Time Graph

Acceleration, a (m/s2)
Coefficient ‘A’-14.7-29.4
Coefficient ‘m’-0.117-0.117

Average of accelerations from position vs. velocity graphs = -14.8 m/s2
Acceleration due to gravity, g = -9.81 m/s2

The calculations showed that acceleration (a) and coefficient (A) relate such that 2A=a. Additionally, the quadratic equation of the curve obtained, x = x0+vit+½at2, was similar to y=ax2=bx+c. From the graphs of velocity against time, the results estimated that the velocity of an object in motion decreased with increased time.

A graph of velocity against time
Figure 1: A graph of velocity against time

However, the graph of position against time showed that as time increased, the position increased to a given level, and then it started to fall. It was concluded that the experiment satisfied the kinematic equations of motion since the equations generated from the graphs matched the theoretical equations.

A graph of position against time
Figure 2: A graph of position against time

The deviations in data results were due to the uncertainty inherent in the experimental method. From the initial measurements, there existed elements of randomness in recording the stopwatch timer and position reading by the motion sensor. The experimental uncertainty is solved by conducting as many trials as possible using an accurate device and working within a regulated environment due to its nature (Kumar, 2020). For example, the table below shows that the errors calculated from stopwatch readings for the inclined plane experiment are random – they have no pattern.

Time (s)Error (%)
Stopwatch 12.56-1.82
2.433.43
2.56-1.82
Stopwatch 22.50.53
2.53-1.19
2.50.53

Conclusion

The researcher realized that the experimental results matched closely with the theoretical expectations. The report showed that the errors could have resulted from the limitation of experiment data, inaccuracy of the tools, and increasing data sample size by conducting as many trials as possible. Similarly, the researcher found that using more accurate sensors could improve the reliability of collected data.

Reference

Kumar, S. (2020). Newton’s Laws of Motion and Friction Mechanics (Vol. 3). Sanjay Kumar.

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"Estimating Acceleration Using Motion Experiments with a Cart and Free-Falling Ball." IvyPanda, 18 Aug. 2025, ivypanda.com/essays/estimating-acceleration-using-motion-experiments-with-a-cart-and-free-falling-ball/.

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IvyPanda. (2025) 'Estimating Acceleration Using Motion Experiments with a Cart and Free-Falling Ball'. 18 August.

References

IvyPanda. 2025. "Estimating Acceleration Using Motion Experiments with a Cart and Free-Falling Ball." August 18, 2025. https://ivypanda.com/essays/estimating-acceleration-using-motion-experiments-with-a-cart-and-free-falling-ball/.

1. IvyPanda. "Estimating Acceleration Using Motion Experiments with a Cart and Free-Falling Ball." August 18, 2025. https://ivypanda.com/essays/estimating-acceleration-using-motion-experiments-with-a-cart-and-free-falling-ball/.


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IvyPanda. "Estimating Acceleration Using Motion Experiments with a Cart and Free-Falling Ball." August 18, 2025. https://ivypanda.com/essays/estimating-acceleration-using-motion-experiments-with-a-cart-and-free-falling-ball/.

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