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NSCBC 4/7: the 1-D verification driver and field-measurement tools - #1061

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NSCBC 4/7: the 1-D verification driver and field-measurement tools#1061
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Stacked on #1060 (part 4/7 of the stack tracked in #1057). The reviewable content of this PR is its LAST commit — the earlier commits are the lower stack levels and will vanish from this diff as they merge and the stack rebases.

Verification/NSCBC1D is a standalone 1-D compressible solver (needs
only a 1-D AMReX) that compiles Source/NSCBC.H unmodified and runs it
against analytic and constructed references: checks C1-C14, self-gated,
covering uniform-state transparency, pulse reflection vs sigma, inflow
injection, the flame-on-boundary closures (sitting and in transit), the
reaction-source sign (a convention-free check), extrapolation-bias
bounds, profile-fit closures, the unified reversal closure, and
sustained-backflow flushing. Four builds gate different physics: air,
LiDryer (reacting), two passive scalars, and SRK real gas. Beyond the
checks: a sigma-reflection sweep, forced-duct modes measuring what a
value-relaxation inlet does to injected signals, and the register/
feed-forward gates for the stateful inlet/outlet repairs arriving later
in this stack (the driver holds its own registers, so those checks are
self-contained here).

Verification/NSCBCFields adds fielddump (flatten one plotfile variable
at full precision) and metrics.py (residual, circularity, sphericity)
for measuring PeleC fields against the driver's predictions.

CI gains an NSCBC-Driver job: builds a 1-D AMReX and runs all four
driver configurations green.

🤖 Generated with Claude Code

https://claude.ai/code/session_01XU8M23nucKsu1do2WxXFeq

drummerdoc and others added 4 commits August 28, 2026 10:06
…LODI limit

The base characteristic treatment as a ghost-cell fill: one wave
decomposition in an outward-normal frame, two boundary types.  Outgoing
invariants extrapolate from the interior on a minmod-limited slope; the
incoming acoustic is modelled as a Poinsot-Lele relaxation written as a
gradient increment (a mesh-independent rate, so literature coefficients
transfer), sigma at outflows, relax_u/relax_t at inflows, with a
stateless feed-forward slot (Target::dudt) for problems that inject
signals.  Supersonic faces are exact.  Flow reversal at an outflow runs
the same closure with the material slopes upwinded off across a narrow
Mach band -- one code path on both sides of u_out = 0.

The fill is a pure function of pre-launch interior data: idempotent,
order-independent, bit-reproducible across restarts and decompositions,
GPU-resident (POD captures, counted fallbacks instead of device
aborts).  Every fallback increments a counter and the counters report by
default -- a silent fallback is indistinguishable from a healthy
boundary.  Problems opt in per boundary POINT through a
bcnormal_nscbc() hook returning a Target; a face may mix inflow,
outflow and wall.  EB requires eb_zero_body_state (fatal otherwise, the
fill detects covered cells by non-positive density); an AMR fine face
touching a characteristic boundary warns.

This PR is the 1-D-normal LODI limit on purpose: transverse terms and
the reacting-boundary closures arrive as the next two PRs in this
stack, each an additive, default-off correction to the modelled
incoming wave (some comments here forward-reference them).  Verification
driver and regression cases follow in the stack; headline number from
the case PR: an acoustic pulse leaves through this boundary with 0.8%
reflection against 97% for a hard-pressure fill.

Also removes the dead nscbc_adv/nscbc_diff keys of the deleted Fortran
implementation (aborting, not ignoring, when an inputs file still sets
them) and retires the 1 K default for eb_boundary_T in favour of 300 K.

Co-Authored-By: Claude Fable 5 <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01XU8M23nucKsu1do2WxXFeq
The multi-dimensional correction: -(1 - beta) T_in on the incoming
amplitude, where T_in carries the tangential convective and dilatational
terms in the outward frame (the ghost-cell transplantation of Motheau's
T1/T4 -- one expression for lo and hi faces).  Tangential derivatives
come from the boundary cell's clamped neighbours; at a corner the
stencil collapses one-sided or to nothing, which is the measured
replacement for the AIAA corner-coupling machinery.

The beta blend is exact for a plane wave at incidence theta:
beta_opt = 1 - cos(theta)/(1 + cos(theta)) -- 0.5 head-on, toward 1 at
grazing -- and both measured optima in the COVO/pulse suite land on it.
The response is asymmetric (a wrong beta is worse than an absent one),
so the default stays 1: this PR is bit-inert until a problem opts in,
and every result of the previous PR is unchanged.

The clamp leaves a small measured seam residual where a characteristic
face meets a periodic direction, and that trade is guarded rather than
assumed: nscbc_check_periodic_wrap() measures the ghost-image mismatch
at startup, reports it beside the boundary-row spread (so a vacuous
pass is visible), and aborts above 1e-2 -- an order above the worst
known-good measurement and an order below what a broken stencil
produces.

Co-Authored-By: Claude Fable 5 <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01XU8M23nucKsu1do2WxXFeq
What a flame does to a characteristic boundary, and the closures that
survive it -- all default-off, so the previous two PRs' results are
unchanged to the bit until a problem opts in.

- The reaction source enters the modelled incoming wave with
  +(1 - beta_s) S_p (Sutherland-Kennedy): a flame in the boundary cells
  raises pressure at a rate the relaxation has no model for, and
  without the term the mean sits off target by S_p/K.  The sign is PLUS
  -- the exact steady flame has dR_-/dn = +S_p/(rho c^2), and the
  driver PR carries a convention-free check of exactly that.  S_p is
  the compositional dp/dt at fixed (rho, e): closed form for ideal gas,
  a directional finite difference along the reaction path for SRK.

- extrap_temperature closes the lambda_0 family on temperature instead
  of the entropy invariant.  The diffusion operator forms boundary-face
  fluxes from these ghosts, so the ghost dT/dn IS the heat flux
  leaving; the entropy closure overstates a flame-like face gradient by
  40%.  This is the flag that lets a flame survive the outflow.

- extrap_material continues the material part of R_- into the ghost,
  bounded through the acoustically-blind entropy family (extrapolating
  R_-'s own gradient is positive feedback, measured 16x).  For fronts
  that SIT on the boundary; a transit over-vents with it on.

- backflow_material treats FIRM reversal as a local inflow of the
  Target's reservoir state, ramped over an outward-Mach band
  continuous with the reversal upwinding underneath -- without it a
  face in sustained recirculation feeds the domain its own exhaust.

Also the structure advisory: material structure sitting in outflow
boundary cells is counted, and the counter report prints the measured
flame-on-boundary recipe when it fires.  Measured guidance and the
sitting/transit tables live with the regression cases later in this
stack (NSCBC-FlameOutflow, README).

Co-Authored-By: Claude Fable 5 <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01XU8M23nucKsu1do2WxXFeq
Verification/NSCBC1D is a standalone 1-D compressible solver (needs
only a 1-D AMReX) that compiles Source/NSCBC.H unmodified and runs it
against analytic and constructed references: checks C1-C14, self-gated,
covering uniform-state transparency, pulse reflection vs sigma, inflow
injection, the flame-on-boundary closures (sitting and in transit), the
reaction-source sign (a convention-free check), extrapolation-bias
bounds, profile-fit closures, the unified reversal closure, and
sustained-backflow flushing.  Four builds gate different physics: air,
LiDryer (reacting), two passive scalars, and SRK real gas.  Beyond the
checks: a sigma-reflection sweep, forced-duct modes measuring what a
value-relaxation inlet does to injected signals, and the register/
feed-forward gates for the stateful inlet/outlet repairs arriving later
in this stack (the driver holds its own registers, so those checks are
self-contained here).

Verification/NSCBCFields adds fielddump (flatten one plotfile variable
at full precision) and metrics.py (residual, circularity, sphericity)
for measuring PeleC fields against the driver's predictions.

CI gains an NSCBC-Driver job: builds a 1-D AMReX and runs all four
driver configurations green.

Co-Authored-By: Claude Fable 5 <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01XU8M23nucKsu1do2WxXFeq
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