Remember to submit the answers to TR 4 and TR 5 to your teacher as part of your Module 7: Lesson 2 Assignment.
TR 4. Calculate the period of a 1.50-m pendulum. Verify your answer using the simulation.
TR 5. On the hypothetical planet Xeon, a pendulum with a length of 95.0 cm swings with a frequency of 1.50 Hz. What is the acceleration due to gravity on Xeon?
You saw in Module 7: Lesson 1 that simple harmonic motion (SHM) is sinusoidal in nature.
SHM is also related to uniform circular motion (UCM). Did you notice that the x-axis in the simulation showed radian units? Why would this way of measuring angles be chosen? Could it be because the circumference of a circle is π times the diameter and the writers were trying to make the relationship between SHM and UCM more obvious? Or is it because it makes the formula easier to work with?
Look closely at the similarities between the SHM and the UCM equations. Manipulating the equation for the period of a pendulum in terms of acceleration gives , which is extremely similar to from uniform circular motion.
This is not surprising if you recall that UCM is vibratory, with a constant period and frequency. Since both equations describe periodic vibratory motion, they should have the same form.
Remember to submit the answers to TR 6 and TR 7 to your teacher as part of your Module 7: Lesson 2 Assignment.
Reopen the Simple Harmonic Motion: Pendulum Motion simulation, if necessary, and complete the following questions.
Observe uniform circular motion and simple harmonic motion at the same time by doing the following:
TR 6. Describe one similarity and one difference between the velocity vector on the reference circle and the velocity vector on the pendulum.
Without changing any of the settings from TR 7, turn on the graphing function (), and select “Velocity” in the first box, as illustrated below. Drag the green bar on the top of the graphing popup to the left so you can see the graph and the pendulum clearly.
TR 7.