Introduction
Hello folks, I've recently started teaching myself physics and one of the ways I do this was through hands-on experiments.
I am looking for feedback on these, really any kind, for example
Notes on experiment setup
What would you have done differently?
Mistakes, things not considered or mentioned
How would you follow up on this experiment?
Note: if the math on this page does not render properly for you, it is also available as a notion site here https://flawless-door-cdd.notion.site/Pendulum-Experiment-144c27137da88054b4eff55713e23c4e?pvs=74
Goal
Measure the relationship between a pendulum length and its period
Compare predictions based on Newton’s laws with empirical results
Methods
3 separate trials for 3 different pendulum lengths (27.5, 37.5 and 50cm) were performed. The pendulum was constructed using of a piece of lightweight twine tied vertically to a ASUS Zenfone 10 (172.0g, 14.65cm height, 6.81cm width) on the lower end and a ruler on the top end. The ruler was weighed down using a textbook, allowing the twine and smartphone to hang off the edge of a desk. The smartphone was raised and released from a 30 degree angle and allowed to swing until rest. Data[math]^{[1]}[/math] was gathered using the phyphox app and the phone’s accelerometer.
Predictions
Length of Period
Simplifying assumptions:
Twine is massless
Friction between twine and ruler, smartphone negligible
Drag negligible
Neglecting drag, we can approximate the maximum speed at the bottom of the pendulum using conservation of mechanical energy:
[math]K_i+U_{Gi}=0+mg(L-Lcos\frac{\pi}{6})=\frac{1}{2}mv_{max}^2+0=K_f+U_{Gf}[/math]
[math]\begin{equation} \tag{1} v_{max}=\sqrt{2gL(1-cos\frac{\pi}{6})} \end{equation}[/math]
Similarly, we can use Newton’s 2nd law to get the same expression
[math]F_{net_t}=-mgsin\theta =ma_t \rightarrow a_t=-gsin\theta[/math]
[math]a_t=\alpha L=\frac{d \omega}{dt}L=\frac{\omega d \omega}{d\theta}L[/math]
[math]-\frac{g}{L}sin\theta d\theta=\omega d \omega[/math]
Integrating both sides, we get
[math]\frac{g}{L}cos\theta=\frac{\omega^2}{2} + C[/math]
For [math]\omega=0[/math], [math]\theta=\frac{\pi}{6}[/math], therefore [math]C=\frac{g}{L}cos\frac{\pi}{6}[/math]
[math]\begin{equation} \tag{2} \omega(\theta)=\sqrt{2\frac{g}{L}(cos\theta-cos\frac{\pi}{6})}\end{equation}[/math]
For [math]\omega_{max}[/math], [math]\theta=0[/math], therefore
[math]v_{max}=\omega_{max}L=\sqrt{2gL(1-cos\frac{\pi}{6})}[/math]
Using [math](2)[/math], we can find the period by integrating over the first quarter of the pendulum’s motion
[math]\omega(\theta)=\frac{d\theta}{dt} \rightarrow \int_{0}^{\frac{T}{4}}dt=\int_{-\frac{\pi}{6}}^{0}\frac{1}{w(\theta)}[/math]
[math]\begin{equation} \tag{3} T=4\int_{-\frac{\pi}{6}}^{0}\frac{1}{\sqrt{2\frac{g}{L}(cos\theta-cos\frac{\pi}{6})}}\end{equation}[/math]
The right hand side can be computed numerically[math]^{[2]}[/math] for the different values of [math]L[/math], yielding the following predictions
[math]T(L=0.5)=1.44\text{s}[/math]
[math]T(L=0.37)=1.24\text{s}[/math]
[math]T(L=0.27)=1.06\text{s}[/math]
We also predict the results to be proportional to the square root of the length, i.e. [math]T \propto \sqrt{L}[/math].
Results
Periods were calculated using the average difference between subsequent acceleration peaks during the first 10 seconds in each trial.
Length (cm, measured to middle of phone)
Avg. Trial 1 Period (s)
Avg. Trial 2 Period (s)
Avg. Trial 3 Period (s)
Avg. of Trials (s)
27.5
1.09
1.09
1.09
1.09
37.5
1.26
1.26
1.26
1.26
50
1.46
1.48
1.47
1.47
Discussion
The results of the experiment agree very closely with our predictions. There is a consistent discrepancy in the empirical data showing longer periods by 2.5-3.3 seconds, presumably owning to drag and friction.
Raw data and results can be accessed here https://drive.google.com/drive/u/0/folders/1nR-IkVcfyhPUA8RYpGqp_Z4cSbe8epto
https://www.integral-calculator.com/ was used for this task