Consider the non-linear equation
\begin{equation}
N_{t+1} = N_t\exp{[r(1-N_t/K)]},
\end{equation}
where $r$ and $K$ are the growth rate and carrying capacity, respectively. This
is a simple model for the population growth of a single species.
We can plot this equation for different values of $r$.
In [1]:
In the above examples, we observe stable equilibrium ($r=1.8$), and stable
cycles with 2 points ($r=2.3$) or 4 points ($r=2.6$). Although not explicitly
shown, this stable behavior can be seen for any initial value of $N_0$ and $K$.
On the other hand, setting $r=3.3$, we will observe that the behavior of the
population depends on the initial value $N_0/K$. The code to produce the plots
is as follows:
In [2]:
The behavior seen above heavily depends on the initial seed value of $N_0$, and
we can see that although the 3 graphs have the same $r$ value, no two graphs
exhibit the same bahavior. This strong dependence on the inital values indicates
that the value of the growth rate $r$ is in the chaotic regime.
It is interesting to see that the equation we are modelling appears as a very
simple and deterministic population growth model, and yes it exhibits
deterministic, as well a arbitrarily dynamic behavior for large enough values of
the growth rate ($r>2.692$).
Two competing species
We can also model the competition of two species using two coupled deterministic
equations similar to the single species case,
\(N_1(t+1) = N_1(t)\exp{\{r_1[K_1 - \alpha_{11}N_1(t) -
\alpha_{12}N_2(t)]/K_1\}}\)
\(N_2(t+1) = N_2(t)\exp{\{r_2[K_2 - \alpha_{21}N_1(t) -
\alpha_{22}N_2(t)]/K_2\}}\)