Fixed points of f are points x such that f(x) = x^2+c = x. This is equivalent to the equation x^2-x+c=0, which has the above roots using the quadratic formula.
As c increases, the parabola f_c moves upwards. From the following picture, we can see that for c < 1/4, there are two fixed points, and for c > 1/4, there are no fixed points. This agrees with the fact that the roots we found above are not real for c > 1/4.
For c=-1, there are four points of intersection of the second iterate of f_c (in green) and the identity function. Two of these are fixed points, so there are two points of period two. See the picture below.
The behavior is qualitatively the same as for c=0. Thus the same qualitative picture holds. See picture below.
For c=-1.1, there is an attracting period two orbit. Although there are still two fixed points, they are now repelling.
For c=-1.3, a period four orbit is now the attracting set. There are still two fixed points, as well as a period two orbit, but they are all repelling.
Points -1 and 2 are fixed points. Points less than -2 or greater than 2 go off to infinity. All other points have orbits with no periodicity and are unpredictable in the long term (although stay bounded). This is an example of the behavior commonly known as chaos.
Dynamics of the quadratic family do not change with every distinct c value; there are regions of c values for which the family has the same dynamics. The dynamics remains the same in the region 0 > c > -0.75 and in the region -0.75 > c > -1.1. The behavior seen for values c=-0.4, -1.1, and -1.3 represents all distinct dynamical behavior occuring for 0 > c > -1.3.
From the pictures below, it appears that the fixed point changes from attracting to repelling at the value c=-0.75. In the next section, you verify this analytically.
The derivative of f_c(x) is f_c'(x)=2x. This evaluated at the fixed points gives the slope of the tangent line at each of the fixed points.
At the larger fixed point (1+SquareRoot[1-4c])/2, the slope is
1+SquareRoot[1-4c]
At the smaller fixed point (1-SquareRoot[1-4c])/2, the slope is
1-SquareRoot[1-4c].
The larger fixed point is always repelling.
The smaller fixed point is attracting for c > -0.75, repelling
for c < -0.75, and neutral for c=-0.75.
This relies on the answer to the previous problem combined with the following facts about a fixed point. A fixed point for a function is:
Explanation:
The linear function g(x)=a x has fixed point 0. g^n(x)=
a ^n x, and if |a| < 1, then a^n becomes arbitrarily
small as n becomes large. If |a| > 1, a^n becomes
arbitrarily large. Thus the fixed point 0 is attracting for |a| < 1
and repelling for |a| > 1.
Since the iteration of a nonlinear function near a fixed point is similar to iteration of a linear function with same slope, we get the above fact.
See the answer to the above question.
The slope of the graph of the second iterate at the period two points
determines whether the period two points are attracting, repelling, or
neutral. If the absolute value of the slope is:
The slope of the graph of the nth iterate at the period n points determines whether they are attracting, repelling, or neutral. The condition is the same as before.
The curve splits at the bifurcation point, which you verified previously as -0.75.
For c>-0.75, the stable set is a fixed point. Thus there is only one visible curve for these c values. For c<-0.75, a period two orbit becomes the attracting set. The two branches you see correspond to this attracting period two orbit.
As c decreases, the period two orbit ceases to be attracting, and an attracting period four orbit appears. In turn, this stops being attracting, and an attracting period eight orbit appears. In general, each bifurcation indicates a doubling in the period of the attracting set. For this reason, such a sequence of bifurcations is sometimes referred to as the period doubling sequence.
As in the iteration diagram, the orbit diagram near c=-2 is a big mess. It displays behavior sometimes referred to as chaos.
Using Chaos Lab #2 for c=-2, this is a matter of observing whether iterates are in the left or right half of the picture.
Using Chaos Lab #2 for c=-2, experiment with a variety of starting points, writing down the first four iterates, until you find a point which has the appropriate itinerary. x=1.6 will do. As the length of the itinerary becomes longer, the size of the region of points with the same itinerary decreases. The size decreases by a constant scale factor for each extra + or - in the itinerary.
Your ability to predict the future will depend on two things:
If there is any error in the initial conditions, in future predictions
it will be exponentially compounded. The further into the future you
wish to predict, the more iterations involved. Since a model for the
physical world has inherent inaccuracies, predicting only a short time
into the future may be good, but at some time, predictions will lose
all accuracy.
You should be able to see a region with an attracting period three orbit. A slightly less obvious region is of period six. There are regions of other periods. From the article above, you know that in the region in which there is an attracting period n, there are points of every period ">" n. (They are repelling so you do not see them.)
Authors: Michael Huberty and Evelyn Sander
Comments to:
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Created: Jun 24 1996 ---
Last modified: Jul 9 1996