MPE StudioMath of Planet Earth
Dynamical Toolkit · 11

Instability in Stiff Systems

When fast decay forces tiny explicit time steps

A stiff system contains fast-decaying modes that severely restrict explicit time stepping even after the physical transient has disappeared.

watchone idea
→
manipulateone example
→
leave withone intuition

The essential idea: for u′=λu with λ<0, Forward Euler is stable only when |1+λΔt|<1.

Watch the concept

One Concept · One Example

VIDEO COMPANION

Instability in Stiff Systems

Presented by Charlotte Moser · Coming soon

What to notice

The idea in 30 seconds

The mathematical structure

Explicit amplification

Forward Euler repeatedly multiplies by one factor.

uₙ=(1+λΔt)ⁿu₀

Implicit amplification

Backward Euler damps every negative real λ for any positive step.

uₙ₊₁=uₙ/(1−λΔt)
Explore

Cross the stability boundary

Reproduce the slides' λ=−1000 experiment and compare exact, Forward Euler, and Backward Euler solutions.

00.01
KEY TAKEAWAY

In stiff problems, numerical stability rather than physical time scale can dominate computational cost.