Ermentrout and Rinzel (1984) developed a model for firefly flashing.
The basic model suggests that a firefly will flash regularly without stimulus (
With a flashing stimulus that flashes at its own rate (
That model is given by
where the difference in the phases (
It is typical to rescale nonlinear equations to seek natural units. In this case, we choose a dimensionless time,
and a dimensionless phase difference,
Which gives the dimensionless equation for the phase difference
Consider the dimensionless equation for the phase difference
Use the phase space of
The firefly model is a good example of a system that can be modeled with a phase diagram.
What happens when we have differential equations that are not first order?
We can convert this to a system of first order equations by defining a new variable
We can still use the phase space method to analyze the system in the
Assume a dimensionless harmonic oscillator:
We convert this to a system of first order equations:
We can graph the system in the
At each point
Represent this vector as an arrow in the
Continue this process until you have a good representation of the flow field.
Hint: Start with points that are easy to sketch. But we will eventually use a computer to do this.
Consider the pair of first order equations:
Note that there will only be horizontal arrows on this line. Why?
Sketch the arrows on the
Now, SEPERATELY, please do this separately lest we draw historical symbols that we should not. Fascism has no home here, y'all.
Note that there will only be vertical arrows on this line. Why?
Sketch the arrows on the
Now try another line, the
What shape are the arrows tracing out in the phase space for the harmonic oscillator?
These curves never touch, why is that? What does a closed curve in this phase space represent?