Lorenz Model
This simple model was developed by Edward Lorenz in 1963 to study fluid mechanics (based on Navier-Stokes equations). It is the first ever model of a chaotic dynamical system. Chaos arises when a deterministic, nonlinear dynamical system exhibits long-term unpredictability in behavior due to sensitivity to initial conditions.
The model is a three-dimentional system of differential equations. Specifically, the model describes the convection motion of a fluid in a small idealized \"Rayleigh-Benard\" container. The basic presumption is that there is fluid in a container with surfaces at different temperatures. The model shows that the fluid motion eventually leads to a chaotic behavior. When plotted in the three spatial dimensions, the dynamics of the model describe a shape called \"strange attractor.\"
Default Dynamics
(Please describe default dynamics for this model.)
No state variables defined.
| Name | Default Value | Description |
|---|---|---|
| $\sigma$ | - | Convection parameter |
| \(r\) | - | - |
| \(b\) | - | - |
| \(c\) | - | - |
| \(del\) | - | - |
Download Source File (lorenz_model.ode)
The source code file can be used with XPP/XPPAUT or other simulation tools.
- Miran Bozicevic, Arizona State University
- Jae Hoon David Yu, Arizona State University
- (1963). Deterministic nonperiodic flow. Journal of the Atmospheric Sciences. 20 : 130-141
Loading model data...