Matrix Exponentials and Repeated Modes
Solve a constant system even when the matrix lacks an eigenvector basis.
Builds on Phase Portraits and Stability
The bigger question: How do coupled variables move together?
On this page
The idea
The scalar exponential generalizes to . For a constant matrix, differentiation gives and . Thus solves any homogeneous constant system.
Visual guide
- x₁ = te⁻ᵗ
- x₂ = e⁻ᵗ
Method and assumptions
If , then . For a Jordan block with nilpotent , factor ; the nilpotent series terminates. In general, requires commuting matrices.
Worked example: a defective matrix
For , write with . Then . Initial state yields , which cannot be produced by a single eigenvector alone.
Try it yourself.
Choose an answer and explain your reasoning to yourself. Use a hint if you get stuck.
Hint 1 · Find a starting point
Expand the matrix exponential as a power series.
Hint 2 · Take the next step
Every power N² and higher is zero.
Show the reasoning
Answer: I+tN
Only I and tN survive. The identity is necessary to give eᴺ⁰=I.
Before moving on: what would make one of the other answers wrong? Saying why is part of understanding.
Worked example: rotation
For , . Splitting the series into even and odd powers gives , the rotation matrix. State norm is preserved.
Interpreting the result
A negative repeated eigenvalue can produce a transient polynomial factor before eventual decay. A plot over a short interval may show growth in one component even though all states eventually approach zero.
Practice
- What is ?
- Compute when .
- Does eventually decay?
Show worked solutions
- The identity matrix.
- , since every higher power vanishes.
- Yes. Its maximum for is at , after which it tends to zero.
Further study
MIT OpenCourseWare: Differential Equations provides a full university course with additional lectures and exercises.
Pause before the next idea.
Can you explain how the visualization connects to this lesson’s goal? If a step still feels uncertain, put this lesson on your review list and try the check again another day.