1.4.1 The harmonic oscillator
A mass attached to the end of a spring and oscillating about the rest position is called a harmonic oscillator. It has many practical uses including suspensions on motorbikes and cars and pendulum clocks. Its motion can be represented by a second order differential equation of the form
where p and q are constants and and
.
For a derivation of this equation click here.
Representation as a pair of linear equations.
Substituting
the equation becomes
To find the equilibrium point
The equilibria occur when
There is only one equilibrium point at (0,0) provided that
and q is a positive constant so
Thus there is only one equilibrium point at (0,0).
To classify the equilibrium point
Consider p=0
Looking at the tr-det diagram it can be seen that the equilibrium point is a neutrally stable centre. Practically this represents undamped motion as p is the damping constant. The solutions are periodic and oscillate forever with constant amplitude.
As an example consider p=0, q=4
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Consider
Using the tr-det diagram the equilibrium point is a stable spiral (focus).
Practically this represents damped motion with the solutions oscillating with decreasing amplitude as they tend to the rest position.
As an example consider p=2, q=4
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Consider
Using the tr-det diagram the equilibrium point is a stable degenerate node. It is not a star node since the matrix A is not diagonal. It is therefore an improper stable node.
Practically this represents a critically damped system. The trajectories no longer oscillate as they tend to the rest position. There is one directrix.
As an example consider p=4, q=4
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Consider
Using the tr-det diagram the equilibrium point is a stable node. The system is now over damped and again no oscillations take place. There are two directrices.
As an example consider p=5, q=4
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