Strange Attractors
Monochromatic silver Lorenz on a charcoal slate background.
Price
$29.00
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|---|---|---|
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The mathematics
The Lorenz system is the canonical example of deterministic chaos. Three coupled ordinary differential equations — dx/dt = σ(y−x), dy/dt = x(ρ−z)−y, dz/dt = xy−βz — derived by Edward Lorenz in 1963 while modeling atmospheric convection. The trajectory through 3D phase space traces the now-iconic butterfly manifold, wrapping forever around two unstable equilibria without repeating. This print renders the literal path of a point obeying these equations, integrated over millions of fourth-order Runge-Kutta steps.
In the Strange Attractors collection
A strange attractor is a region of phase space toward which a dynamical system evolves over time — but unlike a fixed point or a periodic orbit, the trajectory never repeats. It folds and stretches forever inside a bounded volume. The Lorenz attractor, discovered by Edward Lorenz in 1963 while modeling atmospheric convection, is the canonical example: three coupled differential equations whose solutions trace a butterfly-shaped manifold that has become a symbol of deterministic chaos. The Clifford and Aizawa systems extend this idea with different nonlinear couplings, producing scrolls, shells, and toroidal sheets. What you see in these images is not a sketch or a stylization — each line is the literal trajectory of a point obeying the equations, rendered at full numerical precision over millions of integration steps.
dx/dt = σ(y−x), dy/dt = x(ρ−z)−y, dz/dt = xy−βz