Linear ODE Systems
Definition
A system of homogeneous linear first-order ODEs with constant coefficients:
written in matrix form as .
Intuition
The matrix stretches and rotates the state vector ; the natural directions of stretching are the eigenvectors. Along each eigendirection the system decouples into a scalar ODE , so the solution is a sum of exponentials weighted by eigenvalues — a direct vector-space generalisation of the scalar characteristic root cases.
Formal Description
The exponential ansatz converts the system into the eigenvalue problem
The characteristic equation for the matrix is
Each eigenvalue with eigenvector gives a solution .
Key Results
Three cases arise, analogous to the scalar characteristic root cases:
| Eigenvalues | General solution |
|---|---|
| Distinct real | |
| Complex conjugates | Separate real and imaginary parts using Euler’s formula |
| Repeated eigenvalue | Second solution involves (as in scalar case) |
The principle of superposition applies since the system is linear.
Applications
- Phase-plane analysis and stability of equilibria in two-dimensional dynamical systems.
- Coupled mechanical or electrical oscillators.
- Reducing any th-order scalar ODE to a first-order system (companion matrix form) for numerical or analytical treatment.
Trade-offs
- Finding eigenvectors requires solving ; repeated eigenvalues may yield defective matrices requiring generalised eigenvectors.
- For complex eigenvalues, Euler’s formula is needed to extract real-valued solution components.
- Scales well to systems in principle, but eigendecomposition becomes expensive for large .