Motion of a Rigid Body: the Inertia Tensor
Michael Fowler
Definition of Rigid
We're thinking here of an idealized solid, in which the distance between any two internal points stays the same as the body moves around. That is, we ignore vibrations, or strains in the material resulting from inside or outside stresses. In fact, this is almost always an excellent approximation for ordinary solids subject to typical stresses  obvious exceptions being rubber, flesh, etc. Following Landau, we'll usually begin by representing the body as a collection of particles of different massesheld in their places by massless bonds. This approach has the merit that the dynamics can be expressed cleanly in terms of sums over the particles, but for an ordinary solid we'll finally take a continuum limit, replacing the finite sums over the constituent particles by integrals over a continuous mass distribution.
Rotation of a Body about a Fixed Axis
As a preliminary, let's look at a body firmly attached to a rod fixed in space, and rotating with angular veloci
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Anharmonic Oscillators
Michael Fowler
Introduction
Landau (para 28) considers a simple harmonic oscillator with added small potential energy terms . We'll simplify slightly by dropping theterm, to give an equation of motion
(We'll always takepositive, otherwise only small oscillations will be stable.)
We'll do perturbation theory (following Landau):
(Standard practice in most books would be to write with the superscript indicating the order of the perturbation  we're following Landau's notation, hopefully reducing confusion...)
We take as the leading term
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Motion in a Rapidly Oscillating Field: the Ponderomotive Force
Michael Fowler
Introduction
Imagine first a particle of massmoving along a line in a smoothly varying potential , so Now add in a rapidly oscillating force, not necessarily small, acting on the particle:
where are in general functions of position. This force is oscillating much more rapidly than any oscillation of the particle in the original potential, and we'll assume that the position of the particle as a function of time can be written as a sum of a "slow motion" and a rapid oscillation ,
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Parametric Resonance
Michael Fowler
Introduction
(Following Landau para 27)
A onedimensional simple harmonic oscillator, a mass on a spring,
has two parameters, and For some systems, the parameters can be changed externally (an example being the length of a pendulum if at the top end the string goes over a pulley).
We are interested here in the system's response to some externally imposed periodic variation of its parameters, and in particular we'll be looking at resonant response, meaning large response to a small imposed variation.
Note first that imposed variation in the mass term is easily dealt with, by simply redefining the time variable to , meaning
Then
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