# A Tour of Second-Order Ordinary Differential Equations

Requires a Wolfram Notebook System

Interact on desktop, mobile and cloud with the free Wolfram CDF Player or other Wolfram Language products.

Requires a Wolfram Notebook System

Edit on desktop, mobile and cloud with any Wolfram Language product.

This Demonstration is a tour of autonomous second-order ordinary differential equations (ODEs). The systems chosen represent most of the possible important qualitative behaviors. The general form of a second-order ODE is:

[more]
Contributed by: Brian Vick (March 2011)

Open content licensed under CC BY-NC-SA

## Snapshots

## Details

Some of the characteristics of the systems of ODEs selected for this tour are described. These insights suggest interesting explorations.

For the linear system, produces an unstable spiral, is a center, and produces a stable spiral.

For the van der Pol equation, reduces to a linear center. As increases, a limit cycle forms.

The critical value of the parameter for all the bifurcation cases occurs at , where the number and stability of the fixed points change, causing a qualitatively different dynamical picture.

The saddle node has no fixed points for and fixed points at for .

The transcritical fixed points at and switch stability at .

The supercritical pitchfork has one stable fixed point at for . When , becomes unstable and a pair of symmetric stable points forms at .

The subcritical pitchfork has a stable fixed point at and a symmetric pair of unstable points at for . When , becomes unstable and all trajectories diverge.

For both the supercritical and subcritical Hopf cases, the origin is a stable spiral when and bifurcates to an unstable spiral when . When , the trajectories approach limit cycles.

Reference:

S. H. Strogatz, *Nonlinear Dynamics and Chaos*, Jackson, TN: Perseus Books Publishing, 1994.

## Permanent Citation