Predeclare zero-damping pinball development cases

docs/steady_pinball_fiv.md

@@ -5,7 +5,8 @@ rho=1, mean U=.01, nu=.004, D=20, Re_D=50. Centres are (600,255.5),
 (626,270.5), (626,240.5), radius10. No upstream cylinder. Passive probes stay
 at (800,295.5), (800,255.5), (800,215.5), radius5. Every omega is zero.
 Parabolic inlet, regularized NEQ damping1; y bounce-back planes .5/510.5;
-NEQ-extrapolated outlet with existing backflow clamp/blending. Initial fluid is
+NEQ-extrapolated outlet with backflow clamp (the configured blend is inactive in
+this MRT route). Initial fluid is
 parabolic equilibrium. Fixed warmup is 4 NX/U=512000 steps.
 
 Geometry and fluid parameters follow DynamisLab 609116ec26f19766f5e9ce2b0df427d4e24faae8,
@@ -71,3 +72,33 @@ This stage makes no claim of physical grid convergence or vibration suppression.
 Run from checkout with PYTHONPATH=src and the existing Python environment:
 `python research/steady_pinball/run.py --smoke --out <new-external-directory>`
 then separately `--out <new-free-directory>` and `--fixed --out <new-fixed-directory>`.
+
+## Zero-damping development follow-up (predeclared 2026-10-31)
+
+The original d0bcefa run and its zeta=.01 results remain historical evidence.
+The current runner exposes three fixed `--case` choices, all with C=0 as requested:
+
+| Case | M / (rho 3 pi D^2/4) | fn | M | K | Purpose |
+|---|---:|---:|---:|---:|---|
+| Z0 | 10 | .0001 | 9424.77796 | .00372075320 | Remove damping only |
+| M2 | 2 | .0001 | 1884.95559 | .000744150640 | Reduce mass and stiffness together at fixed fn |
+| R2 | 2 | .00006 | 1884.95559 | .000267894231 | Change stiffness only relative to M2 |
+
+R2 deliberately places fn at the retained fixed-body lift peak, f=.00006
+(St=.12 on mean U). This is an informed development choice, not independent
+physical validation or a promise of lock-in. All geometries, fluid settings,
+512000-step fixed warmup, y0=v0=0, force time level and unfiltered RHS are unchanged.
+No run result may select a replacement parameter or an automatic extension.
+
+Each case has a 600000-step cap, the same 300 D/U physical duration. This equals
+60 natural periods for Z0/M2 and 36 for R2. Compare the common final200000 native
+steps, and six100000-step blocks, retaining actual natural/response frequencies
+and ongoing drift. Do not call those blocks ten R2 periods. No settled-VIV claim
+follows from a larger displacement. Report all three outcomes, including quiet
+responses or stopped cases, alongside the existing fixed and damped-free records.
+
+Unchanged stops: |y|>D, invalid move/speed, nonfinite values or no_donor. A 1800s
+per-case wall cap and GPU headroom check bound resource use. Preserve partial rows;
+do not add damping, clip trajectories, filter forces, or relax any stop. Each
+case adds72MB of scalar history, no full fields. The separate Legacy/modern
+baseline diagnosis does not change this FSI protocol.

research/steady_pinball/run.py

@@ -1,6 +1,6 @@
 """Uncontrolled paper-geometry steady Re_D=50, one transverse assembly DOF.
 
-One fixed protocol; --smoke performs 32 warmup + 32 observation steps only.
+Three predeclared zero-damping structures; --smoke uses only 32 + 32 steps.
 See docs/steady_pinball_fiv.md for historical solver differences and new structure.
 """
 from __future__ import annotations
@@ -18,6 +18,7 @@ D, U, NU = 20., .01, .004
 CENTRES = ((600., 255.5), (626., 270.5), (626., 240.5))
 PROBES = ((800., 295.5), (800., 255.5), (800., 215.5))
 WARMUP, STEPS, PERIOD = 512000, 600000, 10000
+STRUCTURES = {'Z0': (10., 1.e-4), 'M2': (2., 1.e-4), 'R2': (2., 6.e-5)}
 COLUMNS = ('step', 'y', 'v', 'cme_F', 'cme_U', 'cme_L', 'wen_F', 'wen_U', 'wen_L',
            'node_F', 'node_U', 'node_L', 'eq_only', 'no_donor', 'crossings')
 ROOT = Path(__file__).resolve().parents[2]
@@ -29,10 +30,15 @@ def config():
 
 class Structure:
     """Exact damped oscillator update for a force held over dt=1; no force filter."""
-    def __init__(self):
+    def __init__(self, mass_ratio=10., frequency=1.e-4, zeta=0.):
-        self.mass = 10. * 3. * math.pi * D * D / 4.
+        if not (math.isfinite(mass_ratio) and mass_ratio > 0. and
-        self.omega = 2. * math.pi / PERIOD
+                math.isfinite(frequency) and frequency > 0. and
-        self.zeta = .01
+                math.isfinite(zeta) and 0. <= zeta < 1.):
+            raise ValueError('positive finite mass ratio/frequency and 0 <= zeta < 1 required')
+        self.mass_ratio, self.frequency = mass_ratio, frequency
+        self.mass = mass_ratio * 3. * math.pi * D * D / 4.
+        self.omega = 2. * math.pi * frequency
+        self.zeta = zeta
         self.stiffness = self.mass * self.omega**2
         self.damping = 2. * self.zeta * self.mass * self.omega
         self.y = self.v = 0.
@@ -68,6 +74,8 @@ def main():
     ap.add_argument('--out', required=True, type=Path)
     ap.add_argument('--fixed', action='store_true', help='same modern moving-path geometry held fixed')
     ap.add_argument('--smoke', action='store_true', help='32+32 steps, no physical result')
+    ap.add_argument('--case', choices=STRUCTURES, default='Z0',
+                    help='predeclared structure; all cases have zero structural damping')
     args = ap.parse_args()
     out = args.out.resolve()
     if out == ROOT or ROOT in out.parents:
@@ -76,7 +84,7 @@ def main():
     cfg = config()
     (out/'config.json').write_text(json.dumps(cfg, indent=2)+'\n')
     source = subprocess.check_output(['git', '-C', str(ROOT), 'rev-parse', 'HEAD'], text=True).strip()
-    s = Structure()
+    s = Structure(*STRUCTURES[args.case], zeta=0.)
     warmup, count = (32, 32) if args.smoke else (WARMUP, STEPS)
     rows = np.lib.format.open_memmap(out/'steps.npy', mode='w+', dtype=np.float64,
                                      shape=(count, len(COLUMNS)))
@@ -87,11 +95,13 @@ def main():
     col = {k: names.index(k) for k in names}
     status, completed, f_last = 'running', 0, 0.
     started = time.monotonic()
-    report = dict(source=source, fixed=args.fixed, smoke=args.smoke, columns=COLUMNS,
+    report = dict(source=source, case=args.case, fixed=args.fixed, smoke=args.smoke, columns=COLUMNS,
                   structure=dict(mass=s.mass, stiffness=s.stiffness, damping=s.damping,
-                                 zeta=s.zeta, fn=1./PERIOD, y0=0., v0=0.),
+                                 mass_ratio_three_disks=s.mass_ratio,
+                                 zeta=s.zeta, fn=s.frequency, Tn=1./s.frequency, y0=0., v0=0.),
                   warmup_steps=warmup, requested_steps=count, dt=1., D=D, U=U, nu=NU,
-                  duration_Tn=count/PERIOD, duration_tU_D=count*U/D,
+                  duration_Tn=count*s.frequency, duration_tU_D=count*U/D,
+                  summary_block_steps=10*PERIOD,
                   rhs='sum of three instantaneous CME_y + Wen_y, one-step lag, no filtering')
     try:
         with Simulation(str(out/'config.json')) as sim:
@@ -135,7 +145,7 @@ def main():
                 f_last = float(cme.sum(dtype=np.float64)+wen.sum(dtype=np.float64))
                 if completed % PERIOD == 0:
                     rows.flush()
-                    print(json.dumps(dict(event='period', step=completed, t_Tn=completed/PERIOD,
+                    print(json.dumps(dict(event='progress', step=completed, t_Tn=completed*s.frequency,
                                           y_D=s.y/D, elapsed_s=time.monotonic()-started)), flush=True)
             else:
                 status = 'smoke_completed' if args.smoke else 'duration_completed_not_qualified'

tests/unit/test_steady_pinball.py

@@ -26,7 +26,7 @@ def test_actual_loader_and_paper_geometry(tmp_path):
 
 
 def test_structure_rest_equilibrium_and_energy_decay():
-    s = runner.Structure()
+    s = runner.Structure(zeta=.01)
     assert s.candidate(0.) == (0., 0.)
     assert s.mass == pytest.approx(10*3*math.pi*100)
     s.y, s.v = .2, 0.
@@ -52,3 +52,33 @@ def test_report_uses_completed_rows_and_net_force():
     assert got[0]['end_step'] == 4
     assert got[0]['y_rms_D'] == .1
     assert got[0]['fy_rms'] == 6.
+
+
+@pytest.mark.parametrize('case', ['Z0', 'M2', 'R2'])
+def test_zero_damping_cases_conserve_unforced_energy_and_match_forced_solution(case):
+    s = runner.Structure(*runner.STRUCTURES[case])
+    assert s.zeta == s.damping == 0.
+    s.y, s.v = .2, 1.e-5
+    y0, v0 = s.y, s.v
+    energy = .5*s.mass*v0**2 + .5*s.stiffness*y0**2
+    for _ in range(12345):
+        s.y, s.v = s.candidate(0.)
+    assert .5*s.mass*s.v**2 + .5*s.stiffness*s.y**2 == pytest.approx(energy, rel=2e-11)
+    force, elapsed = 1.e-4, 3210
+    s.y, s.v = y0, v0
+    for _ in range(elapsed):
+        s.y, s.v = s.candidate(force)
+    phase = s.omega*elapsed
+    equilibrium = force/s.stiffness
+    expected_y = equilibrium+(y0-equilibrium)*math.cos(phase)+v0*math.sin(phase)/s.omega
+    expected_v = -(y0-equilibrium)*s.omega*math.sin(phase)+v0*math.cos(phase)
+    assert (s.y, s.v) == pytest.approx((expected_y, expected_v), abs=2e-11)
+
+
+def test_predeclared_comparisons_change_structure_only():
+    z, m, r = [runner.Structure(*runner.STRUCTURES[k]) for k in ['Z0', 'M2', 'R2']]
+    assert m.mass/z.mass == pytest.approx(.2)
+    assert m.stiffness/z.stiffness == pytest.approx(.2)
+    assert r.mass == m.mass
+    assert r.stiffness/m.stiffness == pytest.approx(.36)
+    assert [runner.STEPS*s.frequency for s in [z, m, r]] == pytest.approx([60., 60., 36.])