A measure of the rate at which nearby trajectories in a dynamical system diverge, indicating chaos.The Lyapunov exponent is a number that tells you how quickly two nearly identical starting points in a dynamical system move apart over time. If the exponent is positive, the system is chaotic: tiny differences grow exponentially, making long-term predictions impossible. If it is negative or zero, nearby trajectories converge or stay close, indicating stable or regular behavior.
The concept was introduced by the Russian mathematician Aleksandr Lyapunov in the 1890s in his work on stability of motion, though its connection to chaos was recognized much later in the 20th century.
Think of two points in a system's state space, separated by a tiny distance. As time evolves, that distance changes roughly as the initial distance times e^(λt), where λ is the Lyapunov exponent. A positive λ means the separation grows without bound (until it saturates), a negative λ means it shrinks, and a zero λ means it stays constant. In practice, you compute λ by tracking the average logarithmic growth rate over many steps, often using a linearization of the system's equations.
Lyapunov exponents are used to diagnose chaos in weather models, financial time series, and mechanical systems, helping engineers decide when a system is predictable or needs control.
The largest Lyapunov exponent for the Earth's atmosphere is positive, which is why weather forecasts become unreliable beyond about two weeks.
| δ(t) | variable | separation between trajectories at time t — separation |
| δ₀ | variable | initial separation between trajectories — separation |
| λ | variable | Lyapunov exponent — lyapunov exponent per second |
| t | variable | time — time second |


