docs: S0 draft — fail-closed motion commit, derived centres, candidate tolerances, S1 scope
Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
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Claude Opus 5.5
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@@ -82,12 +82,21 @@ fluid pull from a solid slot of a moving body is BFL-written.
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## 4. State, masks and authority
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- Host `ObjectState` is the single authority for `offset = (dx, dy)`,
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`velocity = (vx, vy)` and `omega`. Velocity is supplied, never differenced
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from offsets.
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- Per body a small device **motion record** `{c^{n-1}, c^n, u^n}` is uploaded
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with the action buffer; action-slot meaning is not overloaded. (CANDIDATE
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layout; OPEN.)
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- Host `ObjectState` is the single authority for one displacement
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`offset = (dx, dy)` relative to the immutable base centre, plus
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`velocity = (vx, vy)` and `omega`. Centres are always derived
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(`c = base + offset`), never stored as independent state. Velocity is
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supplied, never differenced from offsets.
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- `c^{n-1}` is derived from the last *committed* offset, `c^n` from the
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offset being applied. Per body a small device **motion record**
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`{c^{n-1}, c^n, u^n}` is uploaded with the action buffer; action-slot meaning
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is not overloaded. (CANDIDATE layout; OPEN.)
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- Fail-closed commit: an enqueued upload is not a completed one. The new
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offset becomes the committed offset only after the stream synchronization
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that follows the upload and the step group succeeds. Any upload or later
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synchronization failure leaves host and device motion state unknown: the
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simulation is marked unusable (existing `_require_usable` lifecycle), and
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no API may report a host/device match afterwards.
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- Membership is never read from a flag that M1 is overwriting. The host
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verifies at `add_body` that every swept-band cell has base flag FLUID, so the
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band's base state is known without reading `flag_gpu`.
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@@ -97,7 +106,9 @@ fluid pull from a solid slot of a moving body is BFL-written.
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## 5. Refill of fresh cells (CANDIDATE)
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- Stored time level: everything in `ddf` at M1 is post-collision `G^{n-1}`; the
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refill writes all 9 slots at that same level.
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refill writes all 9 slots at that same level, so every slot of a fresh cell
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that the following pull or a q < 1/2 link may read is defined. Donor values
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are read at the same level `G^{n-1}` (old-fluid cells, untouched by M1).
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- `G = f_eq(rho_bar, u_w(x)) + G_neq(x_d)` where `rho_bar` = mean density of
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valid neighbours and `x_d` = the valid neighbour best aligned with the outward
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normal `(x - c^n)/|x - c^n|`; `G_neq(x_d) = G(x_d) - f_eq(rho(x_d), u(x_d))`.
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@@ -146,6 +157,12 @@ switch cancels with the switching momentum. Whether `sum u_w dm` approximates
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impulse, per crossing cycle). Momentum conservation is also distinct from
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Galilean invariance, which G4 tests.
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External reference note: waLBerla's covered/refill momentum switches
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(`conserveMomentumWhenMapping`, `conserveMomentumWhenRestoring`) default to
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false (Astra), so their existence does not establish which combination its
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validation cases use. A bookkeeping identity alone does not select the
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physical force either.
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Accumulators (separate, per body, per step window; all reported raw):
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`link_cme`, `link_wen_correction` (= `sum u_w dm`), `node_cover`,
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`node_uncover`, plus counters of crossings and refill fallbacks, so force
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@@ -182,8 +199,11 @@ mass), `zeta = c/c_crit = 0.01`, `U* = U/(f_N D)` with `f_N` the natural
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frequency in fluid assuming an inviscid added-mass term; the paper also
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reports frequencies normalised by the in-vacuo value. Our runner derives `k`
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from that in-fluid `f_N` (added-mass coefficient as stated in the paper) and
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never from the vacuum formula; `c_crit` definition to be confirmed (OPEN). Stability/convergence is gated by a halved-time-step run, not
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assumed from the mass ratio.
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never from the vacuum formula; `c_crit` convention and the original
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comparison data are still OPEN. Stability/convergence is gated by fluid
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time/space refinement of the coupled run, not assumed from the mass ratio;
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structural sub-stepping does not substitute for fluid-coupling time
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refinement.
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## 9. Gates (map; tolerances OPEN, declared before runs)
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@@ -196,7 +216,32 @@ KC 5 in-line (needs 2-component offset) · G6 Leontini free transverse VIV
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(m* = 10, ζ = 0.01, Re = 200, definitions pending) · G7 time-level contract
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frozen before the oscillator.
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## 10. Remaining decisions
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Candidate pre-run engineering tolerances (Astra; for discussion, not
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literature limits or measured outcomes; norms, averaging window, convergence
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protocol and physical reference uncertainty must be fixed before adoption, and
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none may be weakened after seeing runs):
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normalised momentum-ledger residual FP32 ≤ 5e-6 (FP64 oracle ≤ 2e-13);
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10-cycle relative mass drift ≤ 1e-4; prescribed-motion grid study D = 40/80/160
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with final-step amplitude change ≤ 2 % and phase ≤ 2°; enlarged domain
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amplitude change ≤ 1 %; matched-frame force RMS ≤ 2 % and improving with
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refinement; VIV refinement amplitude ≤ 2 %, frequency ≤ 1 %, five consecutive
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cycle amplitudes within 1 %.
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## 10. Proposed minimal S1 scope (host only; held until cross-review)
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- `add_body` moving-circle declaration: base centre, declared offset box
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(x/y), speed bound; swept-band computation and band-placement validation.
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- `set_body(offset=..., velocity=..., omega=...)` validation before mutation
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(section 7) and the fail-closed commit of section 4.
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- Motion-record host layout and upload path; exclusion of moving bodies from
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the packed `CurvedBoundaryKernel` links (stationary packing unchanged).
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- Explicit rejections for unsupported modes.
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- Host tests (Astra runs them): rejection-before-mutation, band geometry,
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derived centres, fail-closed behaviour under an injected upload/sync
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failure, stationary packing byte-identical. No kernels, no GPU runs, no
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y-only VIV oscillator (S4), no force RHS.
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## 11. Remaining decisions
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Structural RHS (section 6); motion-record layout; refill details; coupling
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scheme; benchmark definitions and digitized reference data; tolerances;
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