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Checks CFL and Fourier stability criteria for PDE simulations, performs von Neumann analysis, detects stiffness, and recommends explicit vs implicit time-stepping.
How this skill is triggered — by the user, by Claude, or both
Slash command
/full:numerical-stabilityThis skill is limited to the following tools:
The summary Claude sees in its skill listing — used to decide when to auto-load this skill
Provide a repeatable checklist and script-driven checks to keep time-dependent simulations stable and defensible.
Provide a repeatable checklist and script-driven checks to keep time-dependent simulations stable and defensible.
scripts/requirements.txt for dependencies| Input | Description | Example |
|---|---|---|
Grid spacing dx | Spatial discretization | 0.01 m |
Time step dt | Temporal discretization | 1e-4 s |
Velocity v | Advection speed | 1.0 m/s |
Diffusivity D | Thermal/mass diffusivity | 1e-5 m²/s |
Reaction rate k | First-order rate constant | 100 s⁻¹ |
| Dimensions | 1D, 2D, or 3D | 2 |
| Scheme type | Explicit or implicit | explicit |
Is the problem stiff (fast + slow dynamics)?
├── YES → Use implicit or IMEX scheme
│ └── Check conditioning with matrix_condition.py
└── NO → Is CFL/Fourier satisfied with reasonable dt?
├── YES → Use explicit scheme (cheaper per step)
└── NO → Consider implicit or reduce dx
| Physics | Number | Explicit Limit (1D) | Formula |
|---|---|---|---|
| Advection | CFL | C ≤ 1 | C = v·dt/dx |
| Diffusion | Fourier | Fo ≤ 0.5 | Fo = D·dt/dx² |
| Reaction | Reaction | R ≤ 1 | R = k·dt |
Multi-dimensional correction: For d dimensions, diffusion limit is Fo ≤ 1/(2d).
| Script | Key Outputs |
|---|---|
scripts/cfl_checker.py | metrics.cfl, metrics.fourier, recommended_dt, stable |
scripts/von_neumann_analyzer.py | results.max_amplification, results.stable |
scripts/matrix_condition.py | results.condition_number, results.is_symmetric |
scripts/stiffness_detector.py | results.stiffness_ratio, results.real_part_stiffness_ratio, results.imag_dominated, results.stiff, results.recommendation, results.warning |
scripts/cfl_checker.pydt if neededscripts/stiffness_detector.py if multiple scalesscripts/von_neumann_analyzer.pyscripts/matrix_condition.py for implicit solvesUser: My phase-field simulation is blowing up after 100 steps. I'm using explicit Euler with dx=0.01, dt=1e-4, and diffusivity D=1.0.
Agent workflow:
python3 scripts/cfl_checker.py --dx 0.01 --dt 1e-4 --diffusivity 1.0 --dimensions 2 --json
Fo = 1.0 × 1e-4 / (0.01)² = 1.0Fo ≤ 0.252.5e-5 (the tool's recommended_dt, giving Fo = 0.25)cfl_checker.pydt or change scheme# Check CFL/Fourier for 2D diffusion-advection
python3 scripts/cfl_checker.py --dx 0.1 --dt 0.01 --velocity 1.0 --diffusivity 0.1 --dimensions 2 --json
# Von Neumann analysis for custom 3-point stencil
python3 scripts/von_neumann_analyzer.py --coeffs 0.2,0.6,0.2 --dx 1.0 --nk 128 --json
# Detect stiffness from eigenvalue estimates
python3 scripts/stiffness_detector.py --eigs=-1,-1000 --json
# Check matrix conditioning for implicit system
python3 scripts/matrix_condition.py --matrix A.npy --norm 2 --json
| Error | Cause | Resolution |
|---|---|---|
dx and dt must be positive | Zero or negative values | Provide valid positive numbers |
No stability criteria applied | Missing velocity/diffusivity | Provide at least one physics parameter |
Matrix not found: <path> | Invalid path | Check matrix file exists |
Could not compute eigenvalues | Singular or ill-formed matrix | Check matrix validity |
| Scenario | Meaning | Action |
|---|---|---|
stable: true | All checked criteria satisfied | Proceed with simulation |
stable: false | At least one limit violated | Reduce dt or change scheme |
stable: null | No criteria could be applied | Provide more physics inputs |
| Stiffness ratio > 1000 | Problem is stiff | Use implicit integrator |
| Condition number > 10⁸ | Poorly-conditioned (status: poorly-conditioned) | Preconditioning likely needed |
| Condition number > 10¹⁰ | Ill-conditioned (status: ill-conditioned) | Use scaling/preconditioning |
Conditioning thresholds assume IEEE double precision: solving loses roughly
log10(κ)significant digits, and a matrix becomes numerically singular nearκ ≈ 1/eps ≈ 4.5e15. The> 10⁸/> 10¹⁰cutoffs (matchingmatrix_condition.pystatus) leave ample margin; well-conditioned-for-double FEM matrices (κ up to ~10⁶–10⁷) reportstatus: ok.
Do not declare a scheme/time step "stable" until each applicable item below is satisfied with a recorded value from the scripts, not a mental estimate.
cfl_checker.py --json and recorded metrics.cfl, metrics.fourier, and/or metrics.reaction against the reported limits.* (explicit defaults: CFL ≤ 1, Fo ≤ 1/(2d), R ≤ 1), with stable: true and the intended criteria present in criteria_applied.criteria_applied is non-empty and stable is not null — i.e. at least one physics parameter (--velocity/--diffusivity/--reaction-rate) was actually supplied so a real check ran, not a silent no-op.--dx (anisotropic grids: smallest dx/dy/dz) and re-ran cfl_checker.py after any mesh refinement, since Fo ∝ dt/dx² makes the limit highly sensitive to dx.dt is below the limit, recorded the tool's recommended_dt (and the --safety factor used) so the margin to the stability boundary is explicit and reproducible.von_neumann_analyzer.py --json and confirmed results.max_amplification ≤ 1 (stable: true); noted k_at_max and resolved any even-length-stencil warning.stiffness_detector.py --json and recorded real_part_stiffness_ratio, imag_dominated, and stiff; only chose BDF/Radau when stiff: true on the real-part ratio (not on magnitude alone) and there is no warning.matrix_condition.py --json and recorded condition_number and status; treated poorly-conditioned (>1e8) / ill-conditioned (>1e10) as a flag to scale/precondition before trusting the solve.| Tempting shortcut | Why it's wrong / what to do |
|---|---|
"Implicit scheme, so any dt is fine." | Unconditional stability is not accuracy. cfl_checker.py reports stable: true with relaxed (infinite) limits for --scheme implicit and even adds a note to "check accuracy" — a large dt still ruins temporal error. Size dt for accuracy, not just stability. |
| "It ran 100 steps without crashing, so the setup is stable." | Late-time blow-up from round-off, conservation loss, or marginal Fo is common. Completion ≠ correctness — record metrics.fourier/metrics.cfl vs limits.* and confirm stable: true before trusting the run. |
"The 1D Fourier limit is 0.5, so Fo ≤ 0.5 is safe." | The explicit diffusion limit is Fo ≤ 1/(2d) — 0.25 in 2D, 0.167 in 3D. Pass the real --dimensions; cfl_checker.py tightens diffusion_limit automatically, and using 0.5 in 2D/3D is an instability. |
| "Stiffness ratio is huge, so use BDF/Radau." | The magnitude stiffness_ratio is misleading for oscillatory/advective/Hamiltonian spectra. Check imag_dominated and real_part_stiffness_ratio: if imag_dominated: true the detector returns stiff: false with a warning — prefer symplectic/leapfrog or a CFL-sized A-stable scheme, not implicit stiff solvers. |
"I tightened dt, so the old mesh's dt still works after refining dx." | Fo ∝ dt/dx²: halving dx quadruples Fo. Reusing a pre-refinement dt reintroduces a violation. Recompute with cfl_checker.py after every mesh change. |
| "The matrix solved, so its conditioning is fine." | A solve can return numbers while silently losing ~log10(κ) digits. Record condition_number/status from matrix_condition.py; poorly-conditioned/ill-conditioned means scale or precondition before trusting the result. |
dx, dt, and safety are validated as finite positive numbers before any computation; velocity, diffusivity, and reaction_rate, when supplied, are validated as finite--dimensions is restricted to {1, 2, 3} (cfl_checker.py raises and exits 2 otherwise)--eigs) are capped at 10,000 entries and validated as finite numbers--coeffs) are capped at 10,000 entries and validated as finite floatsmatrix_condition.py reads a single matrix file (.npy or text) specified by --matrix; no directory traversal beyond the given pathnp.load() is called with allow_pickle=False to prevent arbitrary code execution via crafted .npy files (matrix_condition.py, stiffness_detector.py)cfl_checker.py, von_neumann_analyzer.py, matrix_condition.py, stiffness_detector.py) with explicit argument listseval(), exec(), or dynamic code generationshell=True)--json) produces structured, parseable results without shell-interpretable contentstiff verdict is based on scale separation among genuinely decaying modes (Re(λ) < 0); the magnitude ratio is still reported as stiffness_ratio. Imaginary-axis-dominated spectra (oscillatory/advection/Hamiltonian) are flagged via imag_dominated and a warning, and are NOT classified as stiff — for those, prefer symplectic/leapfrog or an A-stable scheme sized by the CFL limit, not BDF/Radau.references/stability_criteria.md - Decision thresholds and formulasreferences/common_pitfalls.md - Frequent failure modes and fixesreferences/scheme_catalog.md - Stability properties of common schemesnpx claudepluginhub heshamfs/materials-simulation-skills --plugin core-numericalSelects and configures time integration methods for ODE/PDE simulations: Runge-Kutta, BDF, Rosenbrock, Adams, with adaptive step control and IMEX splitting for stiff/non-stiff problems.
Classifies ODE/PDE type, selects analytical or numerical solution methods, validates solutions, and interprets physical meaning.
Analyzes diffusion processes via SDEs, Fokker-Planck equations, first-passage times, and Monte Carlo validation. Use for probability density evolution, mean first-passage times, or parameter sensitivity analysis.