Viscous face spectral radius (model 2)
Purpose
Model 2 estimates (lambda_{mathrm{vis}}) using an explicit length scale \(d\) (cell size or wall distance). Family overview: Viscous face spectral radius (overview).
Formula
Derivation (sketch)
Diffusion rate \(\nu/d^{2}\) with \(\nu\sim\mu/(\rho\,\mathrm{Re})\) yields an inverse-time scale. Mapping onto a face contribution linear in \(A\) produces the form above (engineering factors \(2\) and \(1/2\)).
Unlike model 1, there is no separate energy Prandtl channel; a single total viscosity is used.
Source map
ViscousFaceSpectralRadiusModel2inTimeStepPolicyTests:
tests/solver/timestep_policy_test.cpp(when intermediate curve tests are present)Contract Workbench id:
viscous_spectral_radius_model2(when wired)
What this proves / does not prove
Proves (when tests present): algebra and \(1/d\) scaling versus the pure API.
Does not prove: optimal geometric definition of \(d\) on a mesh.
References
Diffusion time-scale argument (standard CFD notes; Blazek discusses viscous spectral limits in boundary layers in the same chapters as model 1).
Length-based viscous CFL estimates appear in many unstructured codes; SU2-style (mu S^{2}/rho) is a related but not identical form (area-squared without explicit (d)).
Family overview: Viscous face spectral radius (overview).