Type a command or search the notes. Tab cycles completions. Up and down recall history when blank. Escape dismisses, then leaves the prompt.
MATH
[1251]

Theorems from Stability of systems

All theorems from Stability of systems.

Back to Stability of systems

Discrete stability from root moduli

Write a characteristic root in polar form as

rj=ρjeiθj.r_j=\rho_j e^{i\theta_j}.

Then

∣rjn∣=ρjn.|r_j^n|=\rho_j^n.

Thus ρj<1\rho_j<1 gives a decaying mode, ρj>1\rho_j>1 gives an unbounded mode and ρj=1\rho_j=1 gives a non-decaying mode.

For the whole system, every solution decays precisely when all characteristic roots satisfy ∣rj∣<1|r_j|<1. A root with ∣rj∣>1|r_j|>1 supplies an unbounded solution. If all roots satisfy ∣rj∣≤1|r_j|\le1 and a unit-modulus root is present, its multiplicity decides the remaining case: when each such root is simple, every solution is bounded but some do not decay; a repeated unit-modulus root instead produces an unbounded term nrjnnr_j^n.

Continuous stability from real parts

For a characteristic root r=α+iβr=\alpha+i\beta,

∣ert∣=eαt.|e^{rt}|=e^{\alpha t}.

Therefore α<0\alpha<0 gives decay, α>0\alpha>0 gives an unbounded mode and, for a simple root, α=0\alpha=0 gives a non-decaying oscillatory or constant mode. A repeated root on the imaginary axis introduces a term tertt e^{rt}, whose magnitude is unbounded.

For the whole system, every solution decays precisely when all characteristic roots have negative real part. A root with positive real part supplies an unbounded solution. If no root has positive real part but a root lies on the imaginary axis and each such root is simple, every solution is bounded but some do not decay. A repeated root there gives an unbounded solution.

On this page