This iterative function composition is equivalent to writing a recurrence relation with an initial condition:
\[ x_0 = 16 \]
\[ x_{n+1} = \sqrt{x_{n}} \]
Exercise
Determine the fate of the orbit of \(x_0=2\) in: \[F(x) = \sin(x)\]
In other words, what can we say about: \[\lim_{n \to \infty} F^{n}(2) \]
Determine the fate of the orbit of \(x_0=2\) in \[F(x) = \sin(x)\]
Exercise
Determine the fate of the orbit of \(x_0=2\) in: \[C(x) = \cos(x)\]
In other words, what can we say about: \[\lim_{n \to \infty} C^{n}(2) \]
Determine the fate of the orbit of \(x_0=2\) in \[C(x) = \cos(x)\]
Remember our algorithm for square root?
Algorithm — Square Root
Given a number \(x\), calculate \(\sqrt{x}\) to desired precision.
Make a guess, \(g\).
Calculate new guess: \(\frac{1}{2}( g + \frac{x}{g} )\)
Repeate step (2) as many times as you like, plugging in the new guess each time.
Algorithm — Square Root
Given a number \(x\), calculate \(\sqrt{x}\) to desired precision.
Make a guess, \(g\).
Calculate new guess: \(\frac{1}{2}( g + \frac{x}{g} )\)
Repeate step (2) as many times as you like, plugging in the new guess each time.
\(r\) is a parameter that encapsulates growth and carrying capacity. \(P\) is a population density.
Slightly Less Trivial Population Dynamics
\[P_{n+1} = r P_{n} (1 - P_{n}) \]
Analyze this system for:
\( r = 2.5 \)
\( r = 3 \)
\( r = 3.5 \)
\( r = 4 \)
\(P_{n+1} = r P_{n} (1 - P_{n}) \)
\(\quad \)
Determinism
Given a dynamical system and inital conditions, if I ask you to find the \(83^{\text{rd}}\) term, you should all get exactly the same answer.
That is deterministic. That is not random.
Chaos
A system is chaotic if it exhibits sensitive dependence on initial conditions.
But, even if it were the case that the natural laws had
no longer any secret for us, we could still only know the initial situation approximately.
If that enabled us to predict the succeeding situation with the same
approximation, that is all we require, and we should say that the phenomenon
had been predicted, that it is governed by laws. But it is not always so;
it may happen that small differences in the initial conditions produce very great ones
in the final phenomena. A small error in the former will produce an enormous
error in the latter. Prediction becomes impossible, and we have the fortuitous
phenomenon.