Example Of Lab Report Physics

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Sep 11, 2025 · 7 min read

Table of Contents
The Pendulum: A Comprehensive Example of a Physics Lab Report
This article provides a detailed example of a physics lab report, focusing on the simple pendulum experiment. It covers all the essential sections, from abstract to conclusion, illustrating how to effectively present scientific findings in a clear, concise, and professional manner. Understanding how to write a strong lab report is crucial for success in physics and other scientific disciplines. This example will guide you through the process, highlighting key elements and best practices for writing a high-quality report.
Abstract
This experiment investigated the relationship between the period of a simple pendulum and its length, mass, and initial angle of displacement. Using a simple pendulum apparatus, we measured the period for varying lengths, masses, and angles. Our results strongly supported the theoretical prediction that the period is primarily dependent on the length of the pendulum, independent of mass, and approximately independent of the initial angle for small angles. We calculated a value for g, the acceleration due to gravity, from our data and compared it to the accepted value, assessing the accuracy and limitations of our experimental method.
Introduction
The simple pendulum, a mass suspended from a fixed point by a light string, is a classic system used to illustrate fundamental principles of physics, specifically simple harmonic motion (SHM). The period (T) of a simple pendulum, the time taken for one complete oscillation, is theoretically given by the equation:
T = 2π√(L/g)
where:
- T is the period of oscillation (seconds)
- L is the length of the pendulum (meters)
- g is the acceleration due to gravity (m/s²)
This equation assumes that the amplitude (θ, the initial angle of displacement) is small (less than approximately 15°) and that air resistance is negligible. This experiment aims to verify this theoretical relationship by measuring the period of a simple pendulum for different lengths, masses, and initial angles, and subsequently calculating a value for g. By comparing our experimental value of g to the accepted value, we can assess the accuracy and precision of our experimental setup and methodology.
Materials and Methods
The experimental setup consisted of:
- A simple pendulum apparatus with a bob of adjustable mass.
- A stopwatch capable of measuring time to at least 0.1 seconds.
- A meter stick for measuring the length of the pendulum.
- A protractor for measuring the initial angle of displacement.
- A set of weights to change the mass of the pendulum bob.
The experiment was conducted in three phases:
Phase 1: Investigating the effect of length: We varied the length (L) of the pendulum while keeping the mass (m) and initial angle (θ) constant. We measured the time for 20 oscillations for each length and calculated the average period (T) for each trial. This was repeated for five different lengths.
Phase 2: Investigating the effect of mass: We kept the length (L) and initial angle (θ) constant and varied the mass (m) of the pendulum bob. Again, we measured the time for 20 oscillations for each mass and calculated the average period (T). This was repeated for five different masses.
Phase 3: Investigating the effect of initial angle: We kept the length (L) and mass (m) constant and varied the initial angle (θ). We measured the time for 20 oscillations for each angle and calculated the average period (T). This was repeated for five different angles, ranging from 5° to 30°.
Results
The data collected from each phase of the experiment are presented below in tabular format. Uncertainty measurements were incorporated into the data collection process, specifically in timing measurements using the stopwatch.
Table 1: Effect of Length on Period (m=100g, θ=10°)
Length (L) (m) ± 0.005m | Time for 20 Oscillations (s) ± 0.2s | Average Period (T) (s) |
---|---|---|
0.20 | 12.6 | 0.63 |
0.40 | 17.9 | 0.895 |
0.60 | 22.0 | 1.10 |
0.80 | 25.1 | 1.255 |
1.00 | 28.3 | 1.415 |
Table 2: Effect of Mass on Period (L=0.5m, θ=10°)
Mass (m) (g) ± 0.1g | Time for 20 Oscillations (s) ± 0.2s | Average Period (T) (s) |
---|---|---|
50 | 21.8 | 1.09 |
100 | 21.9 | 1.095 |
150 | 22.0 | 1.10 |
200 | 22.1 | 1.105 |
250 | 21.9 | 1.095 |
Table 3: Effect of Initial Angle on Period (L=0.5m, m=100g)
Initial Angle (θ) (°) ± 1° | Time for 20 Oscillations (s) ± 0.2s | Average Period (T) (s) |
---|---|---|
5 | 21.8 | 1.09 |
10 | 21.9 | 1.095 |
15 | 22.1 | 1.105 |
20 | 22.4 | 1.12 |
30 | 23.0 | 1.15 |
Graphical representations of the data (e.g., plots of T² vs. L for Phase 1) were also included in the full lab report to visually demonstrate the relationships between variables. A linear regression analysis was performed on the appropriate graphs to determine the slope and calculate the value of g. The uncertainties in the slope and subsequently in the calculated g were also determined using standard error propagation techniques.
Discussion
The results from Phase 1 clearly demonstrate a strong positive correlation between the length (L) and the period (T) of the pendulum. The graph of T² vs. L showed a linear relationship, consistent with the theoretical equation. The slope of the best-fit line was used to calculate a value for g.
The results from Phase 2 show that the mass (m) of the pendulum bob has a negligible effect on the period (T), as predicted by the theoretical equation. The slight variations observed in the periods are likely due to experimental uncertainties.
The results from Phase 3 indicate that the initial angle (θ) has a small effect on the period (T) for larger angles. For angles less than approximately 15°, the effect is minimal, again confirming the theoretical assumptions. At larger angles, the pendulum's motion deviates from simple harmonic motion, causing the period to increase.
The calculated value of g from our experiment (including uncertainty) was compared to the accepted value for g in our location. A percent difference was calculated to quantify the accuracy of our experimental method. Sources of error were identified and analyzed, including uncertainties in measurements, air resistance, and deviations from the ideal simple pendulum model.
Conclusion
This experiment successfully demonstrated the relationship between the period of a simple pendulum and its length, mass, and initial angle of displacement. Our results strongly support the theoretical predictions based on the equation T = 2π√(L/g), particularly for small angles of displacement. The calculated value of g, although slightly different from the accepted value, was within the acceptable range of experimental uncertainty. The sources of error identified highlight the importance of careful measurement and consideration of the limitations of the simple pendulum model in real-world conditions. Further investigations could explore the impact of air resistance in more detail or analyze the motion of the pendulum at larger angles using more complex mathematical models.
Frequently Asked Questions (FAQ)
-
Q: Why did we measure 20 oscillations instead of just one?
- A: Measuring multiple oscillations reduces the relative uncertainty in the measurement of the period. The uncertainty in the total time for 20 oscillations is the same as the uncertainty for one oscillation, but the average period is 20 times more precise.
-
Q: What are the main sources of error in this experiment?
- A: Sources of error include uncertainties in length and time measurements, air resistance, the finite mass of the string, and the assumption of small angles not always being perfectly met.
-
Q: How can we improve the accuracy of this experiment?
- A: Accuracy can be improved by using more precise measuring instruments (e.g., a digital timer with higher resolution), reducing air resistance (e.g., performing the experiment in a vacuum), using a lighter and more flexible string, and carefully controlling the initial angle of displacement.
-
Q: Why is the simple pendulum model an idealization?
- A: The simple pendulum model assumes a point mass, massless string, and no air resistance – conditions that are not perfectly met in a real-world experiment. These idealizations simplify the calculations but introduce errors.
-
Q: What are the applications of understanding simple pendulum motion?
- A: Understanding simple harmonic motion, as illustrated by the simple pendulum, is crucial in many areas of physics, including oscillations in mechanical systems, electrical circuits (LC circuits), and even quantum mechanics.
This comprehensive example demonstrates the structure and content expected in a high-quality physics lab report. Remember to adapt this example to your specific experiment and always meticulously document your procedures and findings. Clear and accurate communication of your experimental process and results is essential for scientific rigor.
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