CRITICAL POINTS & BIFURCATION

x ← r·x·(1−x), a single line, and inside it live both order and chaos. For r below 3 the population settles on one equilibrium wherever it starts; past 3 it alternates between two levels, then four, then eight, each doubling costing an interval of r about 4.669 times shorter than the last — the Feigenbaum constant, which recurs in countless other systems. Beyond 3.57 lies chaos, yet in the middle of the chaotic band a period-3 window opens near r = 3.83, and magnifying any small branch reveals the whole diagram again.

▸ Logistic map x' = r·x·(1−x)…
▸ Raise r: 1 point → 2 → 4 → 8 → chaos
▸ Feigenbaum constant δ ≈ 4.669
▸ Period-3 window amid the chaos…
▸ Online. ✅
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⌂ Complex systems

Simulation room Critical points & bifurcation

Bifurcation (Logistic Map)
Online
🔱 the road to chaos
Now showing
🔱 Regime
Parameter r—
Behavior—
Scenario—
Order ↔ chaos
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Drag r to move the cursor on the bifurcation diagram — see 1 point → 2 → 4 → chaos · the xₙ sequence below
Population trajectory xₙ over time (period-doubling → chaos)xₙ
About Bifurcation (Logistic Map)

x ← r·x·(1−x), a single line, and inside it live both order and chaos. For r below 3 the population settles on one equilibrium wherever it starts; past 3 it alternates between two levels, then four, then eight, each doubling costing an interval of r about 4.669 times shorter than the last — the Feigenbaum constant, which recurs in countless other systems. Beyond 3.57 lies chaos, yet in the middle of the chaotic band a period-3 window opens near r = 3.83, and magnifying any small branch reveals the whole diagram again.

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