research: reuse quadrature and clarify snapshot and VIV coordinates

README.md

@@ -394,6 +394,12 @@ before `run()`, the force will be reset to zero. For the common usage pattern
 | `sim.load_checkpoint(path)` | Restore from HDF5 (config must match) |
 | `sim.snapshot()` / `sim.restore()` | In-memory field snapshot |
 
+In-memory snapshots save populations only. Restore keeps the current clock,
+controls, observations, geometry and flags; use it only while geometry is
+unchanged. This is not a restart or an FSI rollback. In particular, do not
+restore a snapshot taken before a translating circle changed position.
+This geometry restriction is a caller precondition, not a runtime check.
+
 #### Low-level access
 
 | Attribute | Description |

docs/moving_bodies.md

@@ -30,6 +30,10 @@ cells (M1 `MovingCircleCells`), moving-wall Bouzidi with wall velocity
   mass, eq_only, no_donor, crossings) accumulated since obs were zeroed;
   `obs`/`read_force` keep their contract (CME on the body).
 - `get_flags()` reads device flags back when moving circles exist.
+- `snapshot()` / `restore()` save and restore populations only, keeping the
+  current clock, controls, observations, geometry and flags. Use them only
+  with unchanged geometry; restoring across a translation is unsupported
+  and is not rejected at runtime. They do not provide FSI rollback.
 
 *Supported:* dense double buffer, D2Q9, FP32 unshifted, SRT/MRT, circles,
 spin. *Rejected before mutation:* EsoPull, ddf shifting, D3Q19, refinement /

docs/validation/viv_re150_predeclare.md

@@ -29,10 +29,17 @@ Claude, Grok and Astra at 1abfe954; implemented in research/viv_re150/.
 
 - D = 40, MRT, dense double buffer; U_lat = .04, nu = U D / 150 = .010667,
   tau = .532.
-- Box [0, 75 D] × [0, 60 D] (3000 × 2400) with the cylinder centre at
-  (30 D, 30 D): 30 D from the inlet, 45 D from the outlet, centred in y
-  (Kolahdouz §4.1.1). Qin's own box ([0, 40 D] × [0, 20 D], centre (10 D, 10 D))
-  is the target paper's, not ours.
+- Nominal 75 D × 60 D lattice allocation (3000 × 2400), based on the
+  Kolahdouz §4.1.1 layout. Coordinate clarification of the existing run:
+  the driver uses `(30 D, (ny - 1)/2)` = `(1200, 1199.5)` in lattice
+  coordinates, or `(30 D, 29.9875 D)`. The earlier `(30 D, 30 D)` wording
+  described the nominal box, not the exact executed centre.
+  Free-slip reflection planes are at `y = .5` and `y = ny - 1.5 = 2398.5`;
+  their separation is 2398 cells = 59.95 D, with the centre exactly midway,
+  29.975 D from each wall. Node counts are not physical wall-to-wall lengths.
+  This corrects the description, without changing the historical geometry
+  or results. Qin's own box ([0, 40 D] × [0, 20 D], centre (10 D, 10 D)) is
+  the target paper's, not ours.
 - Boundaries: uniform Zou–He inlet, NEQ outlet (rho = 1, backflow clamp),
   free-slip y walls. Kolahdouz uses a traction outlet: declared mismatch.
 - Qin's own VIV box (40 D × 20 D) is not used; a smaller box would be a

research/duetsch_re100_kc5/protocol.py

@@ -8,6 +8,7 @@ s/T in [0.25 + (k-1), 0.25 + k); cycle 0 is the startup quarter.
 from __future__ import annotations
 
 import math
+from functools import lru_cache
 
 import numpy as np
 
@@ -53,10 +54,16 @@ def bin_phase(s, T):
     return None
 
 
+@lru_cache(maxsize=8)
+def _quadrature_rule(points):
+    """Reuse the nodes and weights, which depend only on quadrature order."""
+    return np.polynomial.legendre.leggauss(points)
+
+
 def interval_bases(n, T, points=16):
     """Single-step interval averages over [n, n + 1] of cos phi |cos phi| and sin phi
     (phi in radians = 2 pi s / T - pi / 2), Gauss-Legendre quadrature."""
-    x, w = np.polynomial.legendre.leggauss(points)
+    x, w = _quadrature_rule(points)
     s = int(n) % T + 0.5 * (x + 1.0)  # periodic: identical bases in every cycle
     phi = 2.0 * np.pi * s / T - 0.5 * np.pi
     c = np.cos(phi)

research/viv_re150/run.py

@@ -1,8 +1,9 @@
 """One-shot predeclared VIV run (docs/validation/viv_re150_predeclare.md).
 
-Re 150, U* = 5, m/(rho D^2) = 2, zeta = 0, D = 40 on a 75 D x 60 D native
-channel (uniform inlet, NEQ outlet, free-slip y walls), cylinder at
-(30 D, 30 D). Structural RHS = CME + Wen (diagnostics: raw CME, node terms).
+Re 150, U* = 5, m/(rho D^2) = 2, zeta = 0, D = 40 on a nominal 75 D x 60 D
+lattice (uniform inlet, NEQ outlet, free-slip y walls). The cylinder is at
+(30 D, (ny - 1)/2); y-wall planes are .5 and ny - 1.5 in lattice coordinates.
+Structural RHS = CME + Wen (diagnostics: raw CME, node terms).
 Research driver only: Simulation API, no production change.
 
     PYTHONPATH=src python research/viv_re150/run.py --out /path/outside/checkout

tests/unit/test_duetsch_protocol.py

@@ -82,6 +82,35 @@ def test_interval_bases_and_morison_fit_recover_known_coefficients():
     assert p.morison_fit(f, b[:, 0], b[:, 1]) == pytest.approx((2.09, 1.45), abs=1e-9)
 
 
+def test_quadrature_rule_reused_across_steps_and_periods(monkeypatch):
+    original = np.polynomial.legendre.leggauss
+    orders = []
+
+    def counted(points):
+        orders.append(points)
+        return original(points)
+
+    p._quadrature_rule.cache_clear()
+    monkeypatch.setattr(np.polynomial.legendre, "leggauss", counted)
+    try:
+        for points in (16, 8, 16):
+            for period in (T, 2 * T):
+                for n in (0, 123, period + 123):
+                    p.interval_bases(n, period, points)
+        assert orders == [16, 8]
+    finally:
+        p._quadrature_rule.cache_clear()
+
+
+def test_interval_sine_basis_matches_exact_integral():
+    for period in (T, 2 * T):
+        half_width = math.pi / period
+        for n in (0, period // 4, period // 2, period - 1, 7 * period + 123):
+            midpoint = 2 * math.pi * ((n % period) + .5) / period - math.pi / 2
+            expected = math.sin(midpoint) * math.sin(half_width) / half_width
+            assert p.interval_bases(n, period)[1] == pytest.approx(expected, rel=0, abs=2e-15)
+
+
 def test_geometry_repeats_exactly_across_cycles():
     A = p.amplitude(20)
     for m in (0, 1, T // 4, T // 2 - 1, 7 * T // 12):