Logistic Map — Definition, Formula & Examples
The logistic map is a recurrence relation that takes a number between 0 and 1, applies a simple quadratic rule, and feeds the output back in as the next input. Despite its simplicity, it can produce stable fixed points, periodic cycles, or fully chaotic sequences depending on a single parameter.
The logistic map is the discrete dynamical system defined by , where represents the state at iteration and is a bifurcation parameter. For the orbit converges to 0; for it converges to a nonzero fixed point; for a cascade of period-doubling bifurcations occurs, leading to deterministic chaos for most values near and beyond.
Key Formula
Where:
- = State at iteration n, a value in [0, 1]
- = Bifurcation parameter, typically in [0, 4]
- = State at the next iteration
How It Works
Pick a parameter and an initial value between 0 and 1. Repeatedly apply the rule to generate a sequence. For small , the sequence settles to a single value (a fixed point). As you increase past 3, the long-term behavior alternates between 2 values, then 4, then 8, and so on — this is period doubling. Beyond approximately , the orbit becomes chaotic for most values of , meaning tiny changes in lead to wildly different sequences. This sensitivity to initial conditions is a hallmark of chaos.
Worked Example
Problem: Let r = 2.5 and x₀ = 0.4. Compute the first three iterates of the logistic map.
Iteration 1: Apply the formula with x₀ = 0.4.
Iteration 2: Now use x₁ = 0.6.
Iteration 3: Since x₂ = 0.6, the same calculation repeats.
Answer: The sequence reaches the fixed point x* = 0.6 after just one iteration. This is expected because for r = 2.5 (which lies between 1 and 3), the logistic map converges to the fixed point x* = 1 − 1/r = 1 − 0.4 = 0.6.
Why It Matters
The logistic map is a canonical example in nonlinear dynamics courses, demonstrating how deterministic rules produce unpredictable behavior. It appears in population biology (modeling boom-bust cycles), cryptography (pseudo-random number generation), and serves as the simplest gateway to understanding the Feigenbaum constants and universality in chaotic systems.
Common Mistakes
Mistake: Using an initial value outside [0, 1] or a parameter r > 4 and expecting bounded behavior.
Correction: For r > 4, most orbits escape to negative infinity. The logistic map's rich dynamics occur specifically for r ∈ [0, 4] with x₀ ∈ (0, 1).
