

Study with the several resources on Docsity
Earn points by helping other students or get them with a premium plan
Prepare for your exams
Study with the several resources on Docsity
Earn points to download
Earn points by helping other students or get them with a premium plan
Homework exercises from physics 505, autumn 2005, focusing on nonlinear behavior in oscillators, specifically a pendulum. Students are asked to find the frequency of oscillation to second order in the dimensionless parameter α and determine the maximum amplitude for which the frequency differs by less than 20% from the linear result. Additionally, students are asked to compare the results with the small angle approximation and investigate the phase space trajectories for different initial conditions and with damping.
Typology: Assignments
1 / 3
This page cannot be seen from the preview
Don't miss anything!


Due 11/30/
Overview: Recall that solving physics problems is not (just) about solving differential equations. Use physical reasoning to help solve the following exercises and be certain to show your work. It is also important that you practice completely solving these exercises, checking for errors as you go along.
2 2
where, as noted in Lecture 12, 1 6 for the pendulum ( i.e ., from expanding
sin ). In the lecture we focused on a first order analysis, i.e., keeping only terms up to first order in (note that here is dimensionless). Here we want to see how much the result changes if we keep terms up to second order. Assume the following form for the solution
2
and find the form of the frequency (in terms of 0 , and A 1 ) to second order in
. For the value appropriate to the pendulum, how large can the amplitude A 1
be before the frequency differs by more than 20% from the linear result 0.
2 2
a) Define a dimensionless time unit by 0 t (really an phase) and rewrite the
equation of motion in terms of this new “time”. What single parameter describes the behavior of the pendulum?
b) Write a fourth-order Runge-Kutta script to solve this equation of motion for
HINT: We can always rewrite a 2nd^ order differential equation as two 1st^ order equations,
The R-K solution is then given by
5 0 0 1 2 3 4
1 0 0
1 2 0 0
2 3 0 0
4 0 0 3
c) Ignore the friction term for the moment. Start the pendulum at 0 0.
plot the corresponding result for the small angle approximation, sin , that