Files
CelerisLab/tests/validation/jet_cv_measurements.py
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388 lines
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Python

"""Measurement-only continuation diagnostics. Never changes populations or commands."""
import hashlib
import json
from pathlib import Path
import numpy as np
OFFSETS = np.array([1.5, 2.5, 3.5])
LINEAR = np.array([2.5, -1.5, 0.0])
QUADRATIC = np.array([4.375, -5.25, 1.875])
EVIDENCE_LIMIT = 32 * 1024**2
def install_evidence(replacements, limit=None):
"""Preflight retained bytes before replacing files; cap failure preserves old pair.
Staged compression bytes are temporary disk overhead, not retained evidence.
This guards budget failures, not a transactional crash-recovery filesystem.
"""
temporary = set(replacements.values())
try:
directory = next(iter(replacements)).parent
retained = sum(
p.stat().st_size
for p in directory.iterdir()
if p.is_file() and p not in temporary
)
projected = retained - sum(p.stat().st_size for p in replacements if p.exists())
projected += sum(p.stat().st_size for p in temporary)
if limit is not None and projected > limit:
raise RuntimeError(
"Dense-root 32 MiB retained-evidence budget would be exceeded; last verified files preserved"
)
for target, staged in replacements.items():
staged.replace(target)
finally:
for p in temporary:
if p.exists():
p.unlink()
def write_evidence_text(path, text, *, dense_root=False):
staged = path.with_name("." + path.name + ".pending")
staged.write_text(text)
install_evidence({path: staged}, EVIDENCE_LIMIT if dense_root else None)
def sample_steps(c):
"""Same reference times at both scales; dense startup retained."""
if c.get("dense_root", False):
return np.arange(c["steps"] + 1, dtype=int)
return old_sample_steps(c)
def old_sample_steps(c):
"""Exact previous physical cadence, clipped to this campaign's endpoint."""
s2 = c["scale"] ** 2
end = c.get("steps", 3200 * s2) // s2
reference = sorted(set(range(0, min(100, end) + 1)) | set(range(100, end + 1, 4)))
return np.array(reference, int) * s2
def absolute_aperture_interval_mass(rows, blowing, suction):
"""Sum absolute aperture NET masses for one root interval, not per-link flux."""
return float(abs(rows[blowing, 3].sum()) + abs(rows[suction, 3].sum()))
def factors(scale):
"""Lref=one s=1 root length, Tref=one s=1 root time, rho_ref=1."""
return dict(
length=1 / scale,
time=1 / scale**2,
velocity=scale,
mass=1 / scale**2,
momentum=1 / scale,
impulse=1 / scale,
force=scale,
volume_rate=1.0,
mass_rate=1.0,
pressure=scale**2,
)
def primitives(g, cx, cy):
f = np.asarray(g, np.float64)
rho = f.sum(axis=0)
mom = np.stack([np.einsum("q,qyx->yx", v, f) for v in (cx, cy)])
return rho, mom / rho
def contour_terms(rho, vel, origin, rectangle, nu, h=0.5):
"""Independent split of total outward momentum flux into advective,p,viscous."""
x0, y0, x1, y1 = np.rint((np.array(rectangle) - np.tile(origin, 2)) / h).astype(int)
duy, dux = np.gradient(vel[0], h)
dvy, dvx = np.gradient(vel[1], h)
adv = rho * vel[:, None] * vel[None, :]
pressure = np.zeros_like(adv)
pressure[0, 0] = pressure[1, 1] = (rho - 1) / 3
viscous = -rho * nu * np.array([[2 * dux, duy + dvx], [duy + dvx, 2 * dvy]])
out = []
for field in (adv, pressure, viscous):
flux = np.zeros(2)
for i, sign in ((x0, -1), (x1, 1)):
flux += (
sign
* 0.5
* (field[:, 0, y0:y1, i - 1] + field[:, 0, y0:y1, i]).sum(axis=1)
* h
)
for j, sign in ((y0, -1), (y1, 1)):
flux += (
sign
* 0.5
* (field[:, 1, j - 1, x0:x1] + field[:, 1, j, x0:x1]).sum(axis=1)
* h
)
out.append(flux)
return np.array(out)
def ray_geometry(fluid, origin, center, radius, h=0.5):
z, w = np.polynomial.legendre.leggauss(32)
theta = np.array([np.pi / 2, 3 * np.pi / 2])[:, None] + np.pi / 12 * z
normal = np.stack((np.cos(theta), np.sin(theta)), axis=-1)
positions = np.asarray(center) + normal[:, :, None, :] * (
radius + h * OFFSETS[None, None, :, None]
)
local = (positions - origin) / h - 0.5
ix = np.floor(local[..., 0]).astype(int)
iy = np.floor(local[..., 1]).astype(int)
a = local[..., 0] - ix
b = local[..., 1] - iy
if not (
np.all(ix >= 0)
and np.all(iy >= 0)
and np.all(ix + 1 < fluid.shape[1])
and np.all(iy + 1 < fluid.shape[0])
):
raise ValueError("Ray interpolation leaves allocated grid")
for dy, dx in ((0, 0), (0, 1), (1, 0), (1, 1)):
if not fluid[iy + dy, ix + dx].all():
raise ValueError("Ray stencil must be active fluid")
return dict(
ix=ix,
iy=iy,
a=a,
b=b,
normal=normal,
ds=w * radius * np.pi / 12,
positions=positions,
origin=np.asarray(origin),
h=h,
)
def reconstruct_aperture(rho, vel, geo, *, return_absolute=False):
field = np.concatenate((rho[None], vel), axis=0)
x, y, a, b = geo["ix"], geo["iy"], geo["a"], geo["b"]
ray = (
field[:, y, x] * (1 - a) * (1 - b)
+ field[:, y, x + 1] * a * (1 - b)
+ field[:, y + 1, x] * (1 - a) * b
+ field[:, y + 1, x + 1] * a * b
)
estimates = []
absolute = []
for coeff in (LINEAR, QUADRATIC):
wall = np.einsum("cajk,k->caj", ray, coeff)
un = np.einsum("caj,ajc->aj", wall[1:], geo["normal"])
q = np.sum(un * geo["ds"], axis=1)
mass = np.sum(wall[0] * un * geo["ds"], axis=1)
estimates.append(np.stack((q, mass), axis=-1))
absolute.append(
np.stack(
(
np.sum(abs(un) * geo["ds"], axis=1),
np.sum(abs(wall[0] * un) * geo["ds"], axis=1),
),
axis=-1,
)
)
if return_absolute:
return ray, np.array(estimates), np.array(absolute)
return ray, np.array(estimates)
class MeasurementRecorder:
"""Retain reconstructible per-sample terms and sparse full primitive snapshots."""
def __init__(self, c, output, fluid_u, leaves, origin_a, cx, cy):
self.c = c
self.output = Path(output)
self.fluid_u = fluid_u
self.leaves = leaves
self.origin_a = np.asarray(origin_a)
self.cx = cx
self.cy = cy
self.records = []
self.sparse_rays = []
self.ray_steps = set(old_sample_steps(c).tolist())
self.rays = [
ray_geometry(fluid_u, (0.0, 0.0), np.array(c["center"]), c["diameter"] / 2),
ray_geometry(leaves[1], origin_a, np.array(c["center"]), c["diameter"] / 2),
]
self.snapshots = []
def capture(self, step, ug, levels, cv_data, nearest_flux, velocity_error):
c = self.c
s = c["scale"]
record = dict(
step=step,
t_reference=step / s**2,
t_star=step * c["u"] / c["diameter"],
velocity_error=velocity_error,
)
arrays = [ug, *levels]
masks = [self.fluid_u, *self.leaves]
hs = [0.5, 1.0, 0.5]
primitive = [primitives(g, self.cx, self.cy) for g in arrays]
stats = []
for (rho, vel), mask, h in zip(primitive, masks, hs):
if (
not np.isfinite(rho[mask]).all()
or rho[mask].min() <= 0
or not np.isfinite(vel[:, mask]).all()
):
raise RuntimeError(
"Invalid density/velocity on an active composite leaf"
)
stats.append(
[
rho[mask].min(),
rho[mask].max(),
np.max(abs(rho[mask] - 1)),
np.linalg.norm(vel[:, mask], axis=0).max() * s,
rho[mask].sum() * h * h / s**2,
]
)
record["level_stats"] = stats # uniform, AMR root leaf, AMR fine leaf
record["global_mass_reference"] = [stats[0][-1], stats[1][-1] + stats[2][-1]]
record["cv_inventory"] = []
record["cv_flux"] = []
record["momentum_flux_terms"] = []
save_ray = not c.get("dense_root", False) or step in self.ray_steps
ray_record = dict(
sample_index=len(self.records),
arc_ray_values=[],
arc_estimates=[],
arc_absolute_estimates=[],
)
if not c.get("dense_root", False):
record["arc_ray_values"] = []
record["arc_estimates"] = []
record["nearest_mass_flux"] = [
nearest_flux[k] for k in ("uniform_adapter", "amr_api")
]
for idx, (name, p, origin) in enumerate(
[
("uniform_adapter", primitive[0], (0.0, 0.0)),
("amr_api", primitive[2], self.origin_a),
]
):
rho, vel = p
record["cv_inventory"].append([x[0] for x in cv_data[name]])
record["cv_flux"].append([x[1] for x in cv_data[name]])
terms = np.array(
[contour_terms(rho, vel, origin, r, c["nu"]) for r in c["contours"]]
)
np.testing.assert_allclose(
terms.sum(axis=1),
np.array(record["cv_flux"][-1])[:, 1:],
atol=2e-12,
rtol=2e-10,
)
record["momentum_flux_terms"].append(terms)
if save_ray:
ray, estimates, absolute = reconstruct_aperture(
rho, vel, self.rays[idx], return_absolute=True
)
ray_record["arc_ray_values"].append(ray)
ray_record["arc_estimates"].append(estimates)
ray_record["arc_absolute_estimates"].append(absolute)
if not c.get("dense_root", False):
record["arc_ray_values"].append(ray)
record["arc_estimates"].append(estimates)
if c.get("dense_root", False) and save_ray:
self.sparse_rays.append(ray_record)
self.records.append(record)
if step // s**2 in (0, 100, 800, 1600, 3200) and step % s**2 == 0:
fields = {}
for name, (rho, vel), mask, h, origin in zip(
("uniform", "amr_root", "amr_fine"),
primitive,
masks,
hs,
((0.0, 0.0), (0.0, 0.0), self.origin_a),
):
fields[name + "_rho"] = np.where(mask, rho, np.nan).astype(np.float32)
fields[name + "_velocity_reference"] = np.where(
mask[None], vel * s, np.nan
).astype(np.float32)
fields[name + "_origin_reference"] = np.asarray(origin) / s
fields[name + "_h_reference"] = np.array(h / s)
file = self.output / f"fields_s{s}_tref{step//s**2}.npz"
staged = file.with_name("." + file.name + ".pending.npz")
np.savez_compressed(staged, **fields)
install_evidence(
{file: staged}, EVIDENCE_LIMIT if c.get("dense_root", False) else None
)
self.snapshots.append(
dict(
file=file.name,
sha256=hashlib.sha256(file.read_bytes()).hexdigest(),
bytes=file.stat().st_size,
t_reference=step / s**2,
)
)
def flush(self):
path = self.output / f"samples_s{self.c['scale']}.npz"
arrays = {k: np.array([r[k] for r in self.records]) for k in self.records[0]}
if self.c.get("dense_root", False):
arrays["ray_sample_indices"] = np.array(
[r["sample_index"] for r in self.sparse_rays], dtype=int
)
for key in ("arc_ray_values", "arc_estimates", "arc_absolute_estimates"):
arrays[key] = np.array([r[key] for r in self.sparse_rays])
for i, g in enumerate(self.rays):
for k in ("normal", "ds", "positions"):
arrays[f"ray_{i}_{k}"] = g[k]
arrays["ray_offsets_fine_cells"] = OFFSETS
arrays["linear_coefficients"] = LINEAR
arrays["quadratic_coefficients"] = QUADRATIC
staged = path.with_name("." + path.name + ".pending.npz")
np.savez_compressed(staged, **arrays)
metadata = dict(
schema=2 if self.c.get("dense_root", False) else 1,
case=self.c,
dense_root=bool(self.c.get("dense_root", False)),
ray_sample_index_key=(
"ray_sample_indices" if self.c.get("dense_root", False) else None
),
raw_absolute_throughput_definition="Cumulative sum of abs(blowing NET dm)+abs(suction NET dm) per root interval; unresolved within-aperture/substep reversals; not abs(window net).",
absolute_throughput_definition="Quadrature integral of abs(reconstructed u.n), abs(reconstructed rho*u.n); not abs(signed integral), not prescribed nominal, not exact wall truth.",
reference_conversion=factors(self.c["scale"]),
sample_file=path.name,
sample_sha256=hashlib.sha256(staged.read_bytes()).hexdigest(),
sample_count=len(self.records),
snapshots=self.snapshots,
level_stats_columns=[
"rho_min",
"rho_max",
"max_abs_rho_minus_1",
"max_speed_reference",
"mass_reference",
],
raw_partition_order=["wall", "aperture", "total", "blowing", "suction"],
raw_columns=["Jx", "Jy", "angular_impulse", "mass_into_fluid"],
backend_order=["uniform_adapter", "amr_api"],
level_order=["uniform", "amr_root_leaf", "amr_fine_leaf"],
momentum_term_order=["advection", "pressure", "negative_viscous_traction"],
arc_estimate_axes=[
"sample",
"backend",
"linear_or_quadratic",
"blowing_or_suction",
"Q_or_M",
],
arc_ray_axes=[
"sample",
"backend",
"rho_ux_uy",
"aperture",
"gauss_point",
"normal_offset",
],
warning="Extrapolation and nearest-node values are estimator-dependent, not exact wall values. Fields/ray arrays use root-lattice units except explicitly named reference arrays.",
)
meta_path = self.output / f"samples_s{self.c['scale']}.json"
meta_staged = meta_path.with_name("." + meta_path.name + ".pending")
meta_staged.write_text(json.dumps(metadata, indent=2) + "\n")
install_evidence(
{path: staged, meta_path: meta_staged},
EVIDENCE_LIMIT if self.c.get("dense_root", False) else None,
)