The eigenvalues of the system matrix determine whether exponential factors decrease or increase with time. Negative real parts move solutions toward the origin, while positive real parts move them away.
The Mechanism
For a linear coupled system
an eigenvalue produces a solution component proportional to . Therefore:
- if , then , so that component approaches the origin;
- if , then grows, so that component moves away;
| Eigenvalues | Behaviour near the origin | Classification |
|---|---|---|
| Two negative real eigenvalues | All trajectories move toward the origin | Stable node |
| Two positive real eigenvalues | All non-zero trajectories move away | Unstable node |
| Real eigenvalues with opposite signs | Toward the origin along one eigendirection and away along the other | Saddle point |
| , where | Trajectories spiral inward | Stable spiral |
| , where |
For example, eigenvalues and give factors and . Both tend to zero, so every solution approaches the origin, although one component decays faster.
The corresponding eigenvectors give the directions in which these components act. For two real eigenvalues, trajectories align with eigendirections; near a stable node, the slower-decaying component usually determines the final direction of approach because its exponential factor remains dominant for longer.
For instance, with eigenvalues and , both components decay, but decays more slowly than . The trajectory therefore tends to approach the origin tangent to the eigendirection associated with .
A common misconception is that any negative eigenvalue makes the origin stable. This is false: eigenvalues and produce a saddle because the positive eigenvalue creates an outward direction.
Exam Technique
This is HL-only content, AHL 5.17 Phase portraits, and may be tested across HL paper styles. Calculate the eigenvalues, inspect their signs or real parts, classify the equilibrium, and show the correct arrow direction; a GDC result without interpretation is incomplete.
