Skip to article frontmatterSkip to article content
Site not loading correctly?

This may be due to an incorrect BASE_URL configuration. See the MyST Documentation for reference.

10.7 Asymptotic stability: Adams, BDF

10.7.1Stability domains of Adams methods

See here for the schemes

Linear multistep method

For stability we require the roots ww of

ρ(w)−zσ(w)\rho(w) - z \sigma(w)

to be less than one

∣wi(z)∣<1|w_i(z)| < 1

We find the values of zz for which ∣w∣=1|w|=1

w=eiθ,z=ρ(eiθ)σ(eiθ)w = e^{i \theta}, \qquad z = \frac{\rho(e^{i\theta})}{\sigma(e^{i\theta})}
<Figure size 640x480 with 1 Axes>
<Figure size 640x480 with 1 Axes>

These discs are bigger than those for the AB methods, but they are also not A-stable methods. The imaginary axis is not contained in their stability domains, so these methods cannot be used for hyperbolic problems.

10.7.2Stability domains for BDF methods

See here for the schemes

Backward differentiation formula

<Figure size 640x480 with 1 Axes>

The region of asymptotic stability is the exterior of these discs. Only the BDF1 and BDF2 discs are entirely to the right of the imaginary axis and these are A-stable.