Appendix C. Perturbation analysis of the necessary and sufficient conditions for cycles.
In the model, aggressiveness and density are related by the general function
.
|
(C.1)
|
As the stability conditions are
given in terms of the parameter c, which is the partial derivative
calculated at the system’s equilibrium (
), we are interested in using the slope of
the function A at equilibrium. We fix the value of aggressiveness at
and examine the function
.
|
(C.2)
|
Let
be the proportional change in aggressiveness
resulting from a (small) proportional perturbation
of the variable
from the equilibrium value
. These unitless quantities are defined as
|
(C.3)
|
|
|
|
.
|
(C.4)
|
We now recast the necessary and
sufficient conditions for unstable dynamics in terms of these two quantities.
For small values of
we consider the line that is tangent to the
graph of
at the point (
). This is given by the expression
.
|
(C.5)
|
Using Eq. C.5 we can approximate
the quantity
as follows
.
|
(C.6)
|
From Eq. C.3 we have
so
.
|
(C.7)
|
Placing this result into the conditions in Eqs. 22 and 23
|
(C.8)
|
.
|
(C.9)
|
These can be simplified further by noticing that
.
|
(C.10)
|
This gives
|
(C.11)
|
.
|
(C.12)
|