Phy 340 class notes for Fall, 1999

Aug 25 Sep 8 Oct 4 Nov 1 Phy 340 page
Aug 30 Sep 13 Oct 11 Nov 8
Sep 20 Oct 18 Nov 15
Sep 27 Oct 25 Nov 22
Nov 29

Phy 340, Week 6

27 Sep Exam

29 Sep Talk about a homework problem, the one of finding how the roots of a quadratic equation move around as you vary one of the parameters.

Briefly recapitulate the solution of the damped simple harmonic oscillator. What happens when there's an additional forcing term in the equation? Use the property of linearity for this "inhomegeneous, linear, ordinary" differential equation. You break the problem into three steps: 1. solve the homogeneous part, thowing away the inhomogeous term. This has arbitrary constants in the solution.
2. Find and onesolution to the whole equation. This need not have any arbitrary constants in it.
3. Add parts 1 and 2 to get the whole solution.

The pendulum. Quickly set it up (a repeat of previous work). Show how to get one integral of the equation by integrating dq. This is exactly the same as just writing down the conservation of energy and using mgh for the gravitational potential energy.

1 Oct Harmonic oscillator hung from the ceiling. Show how the inhomogeous solution just shifts the origin. The basis of the spring scale.

If I hold a mass suspended from a spring and move my hand up and down, what is the response? Write the equation and again show how to guess the solution. The distinctive difference in this case is that there is a denominator that may vanish. What happens as the forcing frequency becomes close to the natural frequency? Discuss this and assign a homework problem to take the limit (having fixed some initial conditions).

Go back to the forced, damped harmonic oscillator and show how to solve it using complex exponentials.


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