Parametric equations
The logistic map models a population with limited resources. As grows, the orbit goes from a fixed point through period 2, 4, 8, … and then into chaos. The bifurcation diagram puts on the horizontal axis and the long-run orbit values on the vertical axis, and it shows Feigenbaum universality.
Bifurcation diagram: for each , drop the transient and plot the attractor set of .
Interaction
- Parameter r: change and watch the orbit go from a fixed point through period doubling into chaos
- Initial value x₀: change the starting point, and compare the sensitivity to initial values in the chaotic region with the insensitivity in the periodic region
- Bifurcation / Orbit / Cobweb: switch among three readings and compare the long-run distribution, the time series, and step-by-step iteration
- Feigenbaum: mark the ratio of the gaps between period doublings and compare it with the universal constant
What to notice
- The bifurcation diagram projects the long-run attractors onto one parameter plane, so fixed points, period doubling, and chaotic bands are visible at once.
- The orbit and cobweb views stay at the current . They explain one vertical slice of the bifurcation diagram through local dynamics.
- The Feigenbaum marks show how quickly the period-doubling gaps shrink, a scaling law at the edge of chaos.
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