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Author SHA1 Message Date
ClaudeandClaude Opus 5.5 f4ae028154 evidence: digest reads DFG Re20 result.json of schema 1 or 2
final_physical_digest.py indexed [0] on the bare-list (schema 1) native
receipt. v4_cases() accepts schema 1 and the versioned schema-2 object
and rejects others. Existing outputs and final-physical-digest.json are
unchanged; that digest records the previous postprocessor hash, so a
rerun with this version is a new digest.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
2026-10-20 18:36:44 +00:00
Frank14f 70f66176bc docs: record six-case physical validation evidence for 750e8a4
Preserve native gate outcomes and source/output hashes. No simulation or production source changes.
2026-10-20 22:46:29 +08:00
ClaudeandCodex 750e8a483e test: DFG Re20 steady rule as agreed (10 % range, 2 % slope, window-mean verdict)
Supersedes 71221837. Samples every t* 0.5 (interval-mean forces), trailing
t* 50..60 window (21 samples); range <= 10 % and |slope*window| <= 2 % of
each official band width. Verdict on the window mean with the distance to
the nearest band edge. Our engineering rule, frozen before any run.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
(cherry picked from commit 869d60d78e)
2026-10-20 21:59:15 +08:00
ClaudeandCodex 6a03f463bc test: DFG Re20 steady rule per review (1 % band, range and slope, 0.5 s samples)
Samples every 0.5 s at synchronized root steps; trailing 5 s window (11
samples); range and |slope*window| each at most 1 % of the official band
width. States the fluid-on-cylinder force sign, reports cd_positive,
defaults to the refined case and uses the review's label.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
(cherry picked from commit 71221837f9)
2026-10-20 21:59:15 +08:00
ClaudeandCodex 46dc6ba086 test: add DFG 2D-1 Re20 runner against official reference intervals
Reuses the pinned Re100 runner and helpers unchanged; sets only the
lattice viscosity for Re 20. Reports Cd, Cl and p_diff (dp * 0.04 for
U = 0.2 m/s), a steady rule frozen before any run (window ranges at most
a tenth of each official interval width) and no interval verdict when
not steady. Declares the pressure-NEQ outlet and Zou-He inlet deviations.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
(cherry picked from commit 9b8ff90609)
2026-10-20 21:59:15 +08:00
ClaudeandCodex e1efc18274 test: follow the recursive _advance in three-level feed checks
baba5e0 replaced _advance_child with _advance(index, parent_buffer) driven
from _hop; the two feed-order tests still patched the removed method.
Patch _advance and record only index 2 (L1 hop feeding L2); assertions,
expected order and the stale-feed negative control are unchanged.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
(cherry picked from commit 3f47436073)
2026-10-20 21:57:57 +08:00
7 changed files with 3527 additions and 13 deletions
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# DFG 2D-1 (Re 20) against the official reference intervals
`tests/validation/run_dfg_re20.py` runs the steady DFG 2D-1 case on the refined
channel root (D40 root, D80 wide fine patch) and on the uniform D80 grid. Geometry,
inflow, initial state, layout and observation are those of the pinned Re100 runner
(`run_refined_dfg.py`, `re100_helpers.py`, both unchanged); only the lattice
viscosity is set for Re 20 (root tau 0.56, fine 0.62, uniform 0.62, lattice speed 0.01).
Label: "compared against the official reference bands", not a full benchmark
certification: the outlet is pressure-NEQ (`neq_extrap`), not do-nothing, and the
inlet is local Zou-He.
## Quantities
- Cd = 2 Fx / (rho U^2 D), Cl = 2 Fy / (rho U^2 D), interval means over each sample.
- p_diff = p(0.15, 0.2) - p(0.25, 0.2), linear extrapolation to the exact surface
points (`re100_helpers.pressure_probes`). The helper returns dp / (rho U^2) in
scaled units; p_diff = dp * 0.04 for U = 0.2 m/s, rho = 1. Both are reported.
- Official intervals (Schaefer & Turek 1996): Cd [5.57, 5.59], Cl [0.0104, 0.0110],
p_diff [0.1172, 0.1176].
## Bounds and steady rule (frozen before any run)
- End time t* = 60 (30 s physical): 240,000 refined root steps, 480,000 uniform steps.
- One sample every t* = 0.5 (0.25 s) at the end of a synchronized root step; Cd and
Cl are interval means. Trailing window t* 50..60 inclusive (21 samples).
- Steady rule (our engineering choice, not official): in the window, for each of Cd,
Cl, p_diff, max - min <= 10 % and |least-squares slope x window| <= 2 % of its
official interval width (range 2e-3 / 6e-5 / 4e-5; slope 4e-4 / 1.2e-5 / 8e-6).
Absolute limits, so the small Cl is never a divisor. Never relaxed after a run.
- The verdict uses the window mean; the distance to the nearest interval edge is
reported for each quantity (negative outside).
- Force sign: fluid on cylinder, x along the inflow, y up from the bottom wall; Cd > 0
and the official Cl > 0 (`cd_positive` is reported).
- Not steady at t* = 60: status `NOT_STEADY`, no interval verdict. Health limits
(Mach <= 0.2, rho in [0.5, 1.5]) stop the run with `UNHEALTHY`.
- Steady: `WITHIN_INTERVALS` or `OUTSIDE_INTERVALS`, with the per-quantity verdict.
## Run
```
python tests/validation/run_dfg_re20.py --output <new-dir> --plan
CUDA_VISIBLE_DEVICES=<n> python tests/validation/run_dfg_re20.py --case both \
--collision SRT --output <new-dir> --max-wall-seconds <cap>
```
The uniform D80 control separates method error from refinement error. `--plan` writes `plan.json` only. A GPU run writes `plan.json` and `result.json`
(per case: lattice parameters, every sample, window ranges, status, verdict).
Host contract tests: `tests/unit/test_dfg_re20.py`.
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待 Grok 独立复核:750e8a4 本轮六例物理验证
==========================================
固定候选 `750e8a483ec47dcf472e528edc1cf2936f0e7e83`,工作树 `/home/frank14f/CelerisLab-release-prep-20261020` 干净。六例全部完成、退出码 0、无超时;调度器和六个子进程均已消失,最终 `nvidia-smi` 无计算进程。206 个源码/测试/文档哈希与启动 manifest 一致,各例运行前后 source map 相同,原生结果与外部摘要一致;V2 原生源码捕获及 runner 哈希也一致。V4 采用外部 manifest 绑定,没有冒称 runner 内部具备同样 provenance。没有新实验、阈值变更、源码变更、main 合并或公开发布。
六例状态及进程墙钟秒数:V2 zero refined `periodic` 511.409,zero uniform `periodic` 325.254;fixed refined `driven_diagnostics_complete` 530.173,fixed uniform 同状态 333.016;V4 refined `NOT_STEADY` 315.714,uniform `NOT_STEADY` 114.183。墙钟包含初始化和观测开销,仅用于执行记录,不能作正式性能比较。
**V2 zero:MRT、unshifted,均达到 t*=300。** 每例 3480 条 history;refined 1.2M steps,uniform 2.4M steps。各提取 14 个 t*>250 的周期,末五周期全部原生周期门槛通过,各自与冻结参考比较通过。
| 周期指标 | refined | uniform | 原门槛 |
|---|---:|---:|---:|
| 末五周期范围 | 281.663875–298.232508 | 281.590556–298.153468 | 起点>=250,5 个连续周期 |
| period min / max | 3.311073 / 3.316868 | 3.311314 / 3.314196 | 每周期严格在 (2,5) |
| period ptp/mean | 0.00174873 | 0.000869972 | <=0.005 |
| 末周期距最后力采样 | 1.757492 | 1.836532 | [0,5] |
| 连续周期最大间隙 | 0 | 0 | <1e-8 |
| 最小 Cl peak-to-peak | 2.003137 | 1.998667 | >=0.2 |
| Cd_min / Cd_max 跨周期 range | 8.14323e-5 / 1.39714e-4 | 2.60406e-4 / 8.66420e-5 | 每项<=0.005 |
| Cl_min / Cl_max 跨周期 range | 1.96279e-4 / 1.15290e-4 | 1.59490e-4 / 1.82477e-4 | 每项<=0.005 |
| dp_min / dp_max 跨周期 range | 5.50774e-4 / 5.87194e-4 | 8.12699e-4 / 7.99311e-4 | 每项<=0.005 |
| 周期质量均值 ptp/abs(mean) | 3.61945e-8 | 8.51505e-9 | <=1e-4 |
| 最大周期均值 flux_relative | 6.35676e-6 | 5.22752e-5 | <=0.005 |
末周期实际值:refined period=3.312817588、St=0.301857852、Cd=[3.160863689,3.234990541]、Cl=[-1.019161308,0.984224152]、dp=[2.404928344,2.499337133];uniform period=3.311313790、St=0.301994937、Cd=[3.161468623,3.231458726]、Cl=[-1.016677997,0.982020469]、dp=[2.420541455,2.513318511]。
| 末周期参考误差 | refined | uniform | 原门槛 |
|---|---:|---:|---:|
| Cd_min / Cd_max 相对误差 | 0.00107520 / 0.00235425 | 0.000884026 / 0.00125993 | 每项<=0.02 |
| Cl_min / Cl_max 绝对误差 | 0.00212432 / 0.00234646 | 0.00460763 / 0.00455014 | 每项<=0.03 |
| dp_min / dp_max 相对误差 | 0.00638037 / 0.00306172 | 0.0000703422 / 0.00251519 | 每项<=0.02 |
| St 相对误差 | 0.0000558054 | 0.000509970 | <=0.02 |
| Cd / Cl / dp waveform RMS | 0.00472589 / 0.00216188 / 0.0117979 | 0.00317231 / 0.00337428 / 0.00382206 | 描述指标,不是 gate |
`matched_case_pass=false` 原样保留:四次 V2 调用均选择单 case,runner 只有 `--case both` 的两结果原生比较分支才赋值这一字段。它不等于 zero 的各自周期或参考比较失败,也不能由执行者自行改为 true;本轮没有运行该 paired-case 原生比较。fixed 没有官方 DFG 参考 verdict,完成执行不等于物理验收。
**Fixed Jet 健康与 CV。** 两例达到 t*=300,五个 250–300 诊断窗均完整。原健康规则为 physical leaf 数据及 impulse 有限、rho_min>=0.5、rho_max<=1.5、Mach<=0.2。所有 3480 条 history 均有限,观测数值如下。
| 指标 | refined | uniform |
|---|---:|---:|
| 全序列 rho min / max | 0.994218661 / 1.004163150 | 0.993391573 / 1.004678726 |
| 全序列 max Mach | 0.0422925943 | 0.0421810197 |
| mass t*=0.5 / t*=300 | 0.8931541481 / 0.8931214909 | 0.8936680602 / 0.8936524063 |
| 上述端点质量相对变化 | -3.65640e-5 | -1.75164e-5 |
| t*=290–300 mass ptp/mean | 8.40337e-5 | 6.31000e-5 |
| 290–300 Cd / Cl 均值 | 3.184020005 / -0.580990812 | 3.182612828 / -0.582235721 |
CV 各 501 个端点,间距 t*=0.02,积分区间 290–300(root time 40000)。排除首端点之前的 impulse,只累加后 500 个区间;root reaction impulse refined=(254.721600438,-46.479264945),uniform=(254.609026243,-46.578857642)。两条矩形轮廓 refined 为 (48,44,160,120)/(44,36,180,128),uniform 的 x 坐标均加 0.25。以原式 `J_CV=-ΔP-∫outward_momentum_flux dt`,残差为 `J_CV-J_raw`,系数除以 `duration*0.5*U_root²*D_root=80`。这里是 wall+aperture 原始流体对物体反作用,不是已修正的 nozzle thrust。
| 动量残差系数 (x,y) | refined | uniform |
|---|---|---|
| 内轮廓、stride1 | (2.24958e-4,-1.00611e-4) | (1.78190e-4,-7.24811e-5) |
| 外轮廓、stride1 | (7.88038e-5,-4.35879e-5) | (-8.30841e-5,-1.99246e-5) |
| 外减内 | (-1.46155e-4,5.70231e-5) | (-2.61274e-4,5.25565e-5) |
| stride2 相对 stride1 最大分量差 | 1.18312e-5 | 2.19402e-5 |
| stride4 相对 stride1 最大分量差 | 4.44884e-5 | 6.26044e-5 |
CV 未定义验收门槛,以上仅为离线积分诊断。质量记录缺少 raw `mass_into_fluid` Jet 源账本,无法扣除质量源判断闭合。`ΔM+∫outward_mass_flux dt` 仅是表观质量源:refined 内/外=-0.0172316912/-0.646617293 root mass;uniform=3.519017515/3.575029022。相对初始 CV 库存分别 (-2.37505e-6,-5.74501e-5)/(4.84891e-4,3.17573e-4)。轮廓间质量差异保留供审查,不能据此宣称质量闭合通过。
**V4:SRT,无 Jet,t*=60。** uniform 480k/refined 240k steps,各 120 个样本。末窗 t*=50–60 共 21 点;drift 是原 runner 的 `abs(OLS slope per t*)*10`。
| case / 指标 | 末窗 range | 原 range 上限 | 末窗 drift | 原 drift 上限 |
|---|---:|---:|---:|---:|
| refined Cd | 9.86614e-4 | 0.002 | 4.68834e-6 | 0.0004 |
| refined Cl | 6.95374e-5 | 6e-5 | 3.28188e-6 | 1.2e-5 |
| refined p_diff | 1.45066e-4 | 4e-5 | 9.28999e-6 | 8e-6 |
| uniform Cd | 1.19061e-3 | 0.002 | 1.60374e-4 | 0.0004 |
| uniform Cl | 7.93289e-5 | 6e-5 | 5.92289e-6 | 1.2e-5 |
| uniform p_diff | 1.27157e-4 | 4e-5 | 2.80735e-5 | 8e-6 |
两例均有 Cl range、p_diff range/drift 超限,保持 `steady=false,status=NOT_STEADY,verdict=null`。末窗均值 refined=(Cd 5.588876919,Cl 0.010732806,p_diff 0.117811546),uniform=(5.586439289,0.010680915,0.117402607)。原区间 Cd=[5.57,5.59]、Cl=[0.0104,0.011]、p_diff=[0.1172,0.1176];refined 压差均值在区间外,uniform 均值在区间内,但均不能越过稳态 gate。
120 点全序列(t*=0.5–60)存在初始瞬态和反复起伏:refined Cd/Cl/p_diff 的增量符号变化次数为 82/80/82,uniform 为 79/78/81;末窗仍为 13/13/14 和 12/13/11。末窗有符号 OLS slope per t* refined=(-4.68834e-7,-3.28188e-7,-9.28999e-7),uniform=(-1.60374e-5,+5.92289e-7,-2.80735e-6)。这只是当前采样分辨率下的非单调时序描述,不能确定振荡频率、物理/数值根因,也不是发散或瓶颈结论。完整 JSON 保留全序列及逐 10 t* 窗统计。边界偏差仍为 pressure-NEQ/neq_extrap outlet 与 local Zou-He inlet,不能称为原始 do-nothing DFG 边界。
**复核边界与证据。** 本轮不是发布通过:短套件仍为 767 passed/24 failed/1 skipped;V1 历史 pin 阻塞,V3 四例原 TG dry-run 均被 frozen-source guard 拒绝、尚无 CUDA 计算或 TG 结果;未接纳待修订 `56004f44`,没有修改 dtype/NumPy/数值核心。下一步由 Claude 提交修订和解释、Grok 独立复核,再由集成任务接受明确通过审查的 SHA。
原始证据根 `/home/frank14f/CelerisLab-release-evidence-20261020/physical-750e8a4/followup-queue`。`final-physical-digest.json` 约 99 KB,含全部六例原生小摘要、门槛、CV 抽稀结果、源/输出哈希、进程检查和限制;后处理脚本 `final_physical_digest.py` 不导入或运行模拟器。原始 history/log 只保留在 Horsea,没有上传巨量日志。
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"""Read-only postprocessing of the six existing, authorized simulation outputs."""
import csv
import hashlib
import json
import math
from pathlib import Path
import subprocess
import datetime
import numpy as np
Q = Path('/home/frank14f/CelerisLab-release-evidence-20261020/physical-750e8a4/followup-queue')
R = Path('/home/frank14f/CelerisLab-release-prep-20261020')
SHA = '750e8a483ec47dcf472e528edc1cf2936f0e7e83'
def read(p):
return json.loads(p.read_text())
def v4_cases(data):
"""DFG Re20 result.json: schema 1 is a bare case list, schema 2 is {schema, provenance, cases}."""
if isinstance(data, list): return data
if isinstance(data, dict) and data.get('schema') == 2: return data['cases']
raise ValueError('unknown DFG Re20 result schema')
def sha(p):
return hashlib.sha256(p.read_bytes()).hexdigest()
def cmd(*a):
return subprocess.check_output(a, text=True).strip()
def span(a):
return float(np.ptp(a))
def finite(x):
if isinstance(x, dict): return all(finite(v) for v in x.values())
if isinstance(x, list): return all(finite(v) for v in x)
return not isinstance(x, (int,float)) or math.isfinite(x)
def stats(rows, key):
t=np.array([v['tstar'] for v in rows]); v=np.array([r[key] for r in rows])
d=np.diff(v); nz=np.sign(d[d!=0])
return dict(samples=len(v),first=float(v[0]),last=float(v[-1]),min=float(min(v)),max=float(max(v)),mean=float(np.mean(v)),range=span(v),ols_slope_per_tstar=float(np.polyfit(t-t[0],v,1)[0]),increment_sign_changes=int(np.count_nonzero(nz[1:]!=nz[:-1])),total_variation=float(np.abs(d).sum()))
state=read(Q/'state.json'); manifest=read(Q/'manifest.json'); execution=read(Q/'execution.json')
out=dict(schema=1,utc=datetime.datetime.now(datetime.timezone.utc).isoformat(),sha=SHA,evidence_root=str(Q),postprocessor_sha256=sha(Path(__file__)),scope='Offline read-only digest; no new simulation, gate edit, acceptance promotion, or performance claim',verification={},cases={})
v=out['verification']; v['all_six_completed']=len(state['jobs'])==6 and all(x['status']=='COMPLETED' for x in state['jobs'].values())
v['all_exit_zero_no_timeout']=all(x['exit_code']==0 and not x['timeout'] for x in state['jobs'].values())
v['head']=cmd('git','-C',str(R),'rev-parse','HEAD');v['git_status_porcelain']=cmd('git','-C',str(R),'status','--porcelain');v['clean_fixed_head']=v['head']==SHA and not v['git_status_porcelain']
v['tree']=cmd('git','-C',str(R),'rev-parse','HEAD^{tree}');v['src_tree']=cmd('git','-C',str(R),'rev-parse','HEAD:src')
v['tracked_source_map_matches_manifest']=all(sha(R/p)==h for p,h in manifest['files_sha256'].items());v['tracked_source_map_count']=len(manifest['files_sha256'])
v['execution_final_source_matches_manifest']=all(execution['source_after'][k]==manifest[k] for k in ['sha','tree','src_tree','git_status','git_diff_sha256','files_sha256'])
pids=[state['scheduler_pid']]+[x['pid'] for x in state['jobs'].values()]
v['tracked_processes']={}
for pid in pids:
p=subprocess.run(['ps','-p',str(pid),'-o','pid=,ppid=,stat=,comm='],capture_output=True,text=True)
v['tracked_processes'][str(pid)]=p.stdout.strip() or 'absent'
v['no_tracked_process_running']=all(s=='absent' or ' Z' in s for s in v['tracked_processes'].values())
v['gpu_compute_processes']=cmd('nvidia-smi','--query-compute-apps=gpu_uuid,pid,process_name,used_gpu_memory','--format=csv')
out['hashes']={p.name:sha(p) for p in [Q/'manifest.json',Q/'execution.json',Q/'state.json',Q/'queue-plan.json',Q/'receipt-preflight.json',Q/'authorized_followup_queue.py',Q/'v4_external_timing.py']}
for label,sj in state['jobs'].items():
p=Q/label; r=read(p/'result.json'); c=out['cases'][label]=dict(status=sj['native_status'],exit_code=sj['exit_code'],timeout=sj['timeout'],process_wall_seconds=sj['wall_seconds'],pid=sj['pid'],gpu_uuid=sj['gpu_uuid'],source_unchanged=r['source_unchanged'])
c['source_matches_manifest']=all(r['source'][k]==manifest[k] and r['source_after'][k]==manifest[k] for k in ['sha','tree','src_tree','git_status','git_diff_sha256','files_sha256'])
c['external_manifest_hash_matches']=r['external_manifest_sha256']==sha(Q/'manifest.json')
c['hashes']={str(z.relative_to(p)):sha(z) for z in [p/'command.json',p/'result.json',*sorted((p/'output').rglob('*.json')),*sorted((p/'output').rglob('*.csv')),*sorted((p/'output').rglob('*.jsonl'))]}
if label.startswith('v4'):
n=v4_cases(read(p/'output/result.json'))[0]; rows=n['rows']
captured=r['native_results'][0]
c['native_receipt_matches_external_result']=all(n[k]==z for k,z in captured.items() if k not in ['last_row','rows_count']) and captured['last_row']==rows[-1] and captured['rows_count']==len(rows)
c['external_receipt_history_handling']='V4 external receipt stores row count and last row; full native rows are separately hashed'
c['native_all_finite']=finite(n)
c['native']={k:z for k,z in n.items() if k not in ['rows','lattice']}
c['full_series']={k:stats(rows,k) for k in ['cd','cl','p_diff']}
c['ten_tstar_windows']={str(a):{k:stats([z for z in rows if a<=z['tstar']<=a+10],k) for k in ['cd','cl','p_diff']} for a in range(0,60,10)}
c['last_window']=dict(tstar=[50,60],metrics={k:stats(rows[-21:],k) for k in ['cd','cl','p_diff']})
c['health']=dict(rho_min=min(z['rho_min'] for z in rows),rho_max=max(z['rho_max'] for z in rows),max_mach=max(z['max_mach'] for z in rows))
continue
case=label.rsplit('-',1)[1]; base=p/'output'/case;n=read(base/'summary.json');plan=read(p/'output/plan.json')
c['native_receipt_matches_external_result']={k:z for k,z in n.items() if k!='history'}==r['native_summary']
c['external_receipt_history_handling']='V2 external receipt omits the history path; complete history.csv is separately hashed'
c['native_all_finite']=finite(n)
c['native_runner_hash_matches']=plan['runner_sha256']==sha(R/'tests/validation/run_refined_dfg.py')
sm=plan['source_manifest'];c['native_source_capture_matches']=sm['checkout_revision']==SHA and not sm['checkout_dirty'] and all(sha(R/f)==h==manifest['files_sha256'][f] for f,h in sm['sha256'].items())
c['native_source_capture_file_count']=len(sm['sha256'])
c['native']={k:z for k,z in n.items() if k not in ['history','cycles','jet_diagnostic_windows']}; c['comparison']=read(p/'output/comparison.json');c['gates']=plan['gates'];c['reference_gates']=plan['reference_gates'];c['diagnostic_windows']=n['jet_diagnostic_windows']
rows=[{k:float(z) for k,z in row.items()} for row in csv.DictReader((base/'history.csv').open())];late=[x for x in rows if x['tstar']>=290]
c['health']=dict(rows=len(rows),tstar=[rows[0]['tstar'],rows[-1]['tstar']],all_finite=finite(rows),rho_min=min(z['rho_min'] for z in rows),rho_max=max(z['rho_max'] for z in rows),max_mach=max(z['max_mach'] for z in rows),mass_first=rows[0]['mass'],mass_last=rows[-1]['mass'],mass_change_fraction=(rows[-1]['mass']-rows[0]['mass'])/rows[0]['mass'],mass_late_range_fraction=span([z['mass'] for z in late])/np.mean([z['mass'] for z in late]))
if n['cycles']:
tail=n['cycles'][-5:]; periods=[z['period'] for z in tail]; masses=[z['mass_time_mean'] for z in tail]
c['periodic_actual']=dict(cycles_total=len(n['cycles']),tail_cycles=len(tail),tail_start=tail[0]['start'],tail_end=tail[-1]['end'],period_min=min(periods),period_max=max(periods),period_mean=float(np.mean(periods)),period_relative_range=span(periods)/np.mean(periods),last_cycle_age=rows[-1]['tstar_force']-tail[-1]['end'],consecutive_max_gap=max(abs(a['end']-b['start']) for a,b in zip(tail,tail[1:])),minimum_lift_amplitude=min(z['cl_amplitude'] for z in tail),extrema_ranges={k+'_'+e:span([z[k+'_'+e] for z in tail]) for k in ['cd','cl','dp'] for e in ['min','max']},mass_relative_range=span(masses)/abs(np.mean(masses)),max_cycle_flux_relative=max(z['flux_relative'] for z in tail),last_cycle={k:z for k,z in tail[-1].items() if not k.endswith('_waveform')})
cv=[json.loads(x) for x in (base/'cv_history.jsonl').read_text().splitlines()];t=np.array([x['time_root'] for x in cv]);inv=np.array([x['inventory'] for x in cv]);flux=np.array([x['outward_flux'] for x in cv]);j=np.array([x['interval_impulse_root'] for x in cv[1:]]).sum(axis=0);duration=t[-1]-t[0];norm=duration*.5*.01**2*40
cvout=c['cv']=dict(samples=len(cv),all_finite=finite(cv),tstar=[cv[0]['tstar'],cv[-1]['tstar']],duration_root=duration,coefficient_normalization=norm,raw_body_reaction_impulse_root=j.tolist(),first_preceding_impulse_excluded=True,contours_root=plan['cv_observation'][case+'_contours_root'],mass_qualification='Apparent mass source only: raw Jet mass_into_fluid ledger was not recorded, so mass-source-subtracted closure cannot be assessed',acceptance='offline diagnostics only; no CV pass threshold was defined',strides={})
for stride in [1,2,4]:
idx=np.arange(0,len(t),stride);assert idx[-1]==len(t)-1
integral=np.trapz(flux[idx],t[idx],axis=0); delta=inv[-1]-inv[0];jcv=-delta[:,1:]-integral[:,1:];res=jcv-j
cvout['strides'][str(stride)]=dict(samples=len(idx),momentum_delta_root=delta[:,1:].tolist(),outward_momentum_integral_root=integral[:,1:].tolist(),cv_reaction_impulse_root=jcv.tolist(),residual_impulse_root=res.tolist(),residual_coefficient=(res/norm).tolist(),apparent_mass_source_root=(delta[:,0]+integral[:,0]).tolist(),apparent_mass_source_fraction_initial_inventory=((delta[:,0]+integral[:,0])/inv[0,:,0]).tolist())
a=np.array(cvout['strides']['1']['residual_coefficient']);cvout['contour_residual_coefficient_difference']=(a[1]-a[0]).tolist();cvout['coarsening_coefficient_difference']={s:(np.array(cvout['strides'][s]['residual_coefficient'])-a).tolist() for s in ['2','4']}
v['all_six_source_unchanged']=all(c['source_unchanged'] and c['source_matches_manifest'] and c['external_manifest_hash_matches'] for c in out['cases'].values())
v['all_six_native_receipts_match']=all(c['native_receipt_matches_external_result'] and c['native_all_finite'] for c in out['cases'].values())
v['all_v2_native_captures_match']=all(c['native_runner_hash_matches'] and c['native_source_capture_matches'] for k,c in out['cases'].items() if k.startswith('v2'))
out['limitations']=['V1 historical source pin remains blocked','V3 original TG source guard blocked all four dry-runs before CUDA; no TG result or acceptance','Short suite remains 767 passed, 24 failed, 1 skipped; not a release pass','Matched_case_pass remains false because each invocation selected one case; native paired-case comparison branch did not execute','Fixed Jet CV is diagnostic; mass source ledger absent; no physical acceptance','V4 both NOT_STEADY with original ranges/drifts/bands; boundary deviations retained','No formal performance claim: timings include observation/profiling and startup is separately recorded']
dest=Q/'final-physical-digest.json';dest.write_text(json.dumps(out,indent=2,allow_nan=False)+'\n')
print(json.dumps(dict(output=str(dest),bytes=dest.stat().st_size,sha256=sha(dest),verification=v),indent=2))
+79
View File
@@ -0,0 +1,79 @@
"""CPU-only contract tests for run_dfg_re20. Not CUDA or DFG acceptance evidence."""
import sys
from pathlib import Path
import unittest
sys.path.insert(0, str(Path(__file__).resolve().parents[1] / "validation"))
import run_dfg_re20 as v # noqa: E402
import run_refined_dfg as rr # noqa: E402
h, _ = rr.helpers(rr.DEFAULT_SOURCE)
def rows(values, tstar_end=v.TSTAR_MAX):
n = int(round(tstar_end / v.SAMPLE_TSTAR))
return [dict(tstar=(i + 1) * v.SAMPLE_TSTAR, **values(i)) for i in range(n)]
class Re20Contract(unittest.TestCase):
def test_lattice_parameters_and_bounds(self):
root, uniform = v.lattice_parameters(40), v.lattice_parameters(80)
self.assertAlmostEqual(root["tau"], 0.56, places=12)
self.assertAlmostEqual(uniform["tau"], 0.62, places=12)
self.assertEqual((root["steps"], root["interval"]), (240000, 2000))
self.assertEqual((uniform["steps"], uniform["interval"]), (480000, 4000))
self.assertAlmostEqual(v.plan()["refined_fine_tau"], 0.62, places=12)
def test_config_only_changes_viscosity(self):
base = v._re100_config(h, 40, "SRT", "none")
cfg, body, p = v.config(h, 40, "SRT")
self.assertAlmostEqual(cfg["physics"]["viscosity"], 0.01 * 40 / 20, places=15)
self.assertEqual((p["re"], p["viscosity"]), (20.0, cfg["physics"]["viscosity"]))
base[0]["physics"]["viscosity"] = cfg["physics"]["viscosity"]
self.assertEqual(base[0], cfg)
self.assertEqual(base[1], body)
with self.assertRaisesRegex(ValueError, "no Jets"):
v.config(h, 40, "MRT", "zero")
def test_units(self):
s = v.sample([2.0, -0.5], 4, 40, 3.0)
den = rr.SPEED**2 * 40 / 2
self.assertAlmostEqual(s["cd"], 2.0 / 4 / den)
self.assertAlmostEqual(s["cl"], -0.5 / 4 / den)
self.assertAlmostEqual(s["p_diff"], 3.0 * 0.04)
self.assertEqual(s["dp_scaled"], 3.0)
def test_steady_and_verdict(self):
inside = dict(cd=5.58, cl=0.0106, p_diff=0.1174)
out = v.summarize(rows(lambda i: inside))
self.assertEqual((out["status"], out["steady"], out["window_samples"]),
("WITHIN_INTERVALS", True, 21))
self.assertTrue(out["cd_positive"])
self.assertAlmostEqual(out["edge_distance"]["cl"], 0.0002)
self.assertTrue(all(out["verdict"].values()))
low = v.summarize(rows(lambda i: dict(inside, cl=0.0100)))
self.assertEqual(low["status"], "OUTSIDE_INTERVALS")
self.assertFalse(low["verdict"]["cl"])
def test_slow_drift_gives_no_verdict(self):
# Range 2e-5 passes (limit 6e-5); slope * window 2e-5 exceeds 1.2e-5.
out = v.summarize(rows(lambda i: dict(cd=5.58, cl=0.0106 + 1e-6 * i, p_diff=0.1174)))
self.assertEqual((out["status"], out["verdict"]), ("NOT_STEADY", None))
self.assertLessEqual(out["ranges"]["cl"], out["range_limits"]["cl"])
self.assertGreater(out["drifts"]["cl"], out["slope_limits"]["cl"])
def test_noise_range(self):
quiet = v.summarize(rows(lambda i: dict(cd=5.58, cl=0.0106 + 2e-5 * (i % 2), p_diff=0.1174)))
self.assertTrue(quiet["steady"]) # within the range limit, no trend
noisy = v.summarize(rows(lambda i: dict(cd=5.58, cl=0.0106 + 1e-4 * (i % 2), p_diff=0.1174)))
self.assertEqual(noisy["status"], "NOT_STEADY")
self.assertGreater(noisy["ranges"]["cl"], noisy["range_limits"]["cl"])
def test_incomplete_run_gives_no_verdict(self):
out = v.summarize(rows(lambda i: dict(cd=5.58, cl=0.0106, p_diff=0.1174), tstar_end=30))
self.assertEqual((out["status"], out["verdict"]), ("INCOMPLETE", None))
if __name__ == "__main__":
unittest.main()
@@ -80,11 +80,12 @@ class ThreeLevelCPU(unittest.TestCase):
f, g = run._levels[1:]
b = g.boundary
events, feeds = [], []
advance, gather = run._advance_child, run._gather_halo
def record_feed(buffer, **kw):
self.assertIs(buffer, (f.current, f.spare)[len(feeds)])
feeds.append(buffer)
advance(buffer, **kw)
advance, gather = run._advance, run._gather_halo
def record_feed(index, buffer, **kw): # index 2: L1 hop feeds L2
if index == 2:
self.assertIs(buffer, (f.current, f.spare)[len(feeds)])
feeds.append(buffer)
advance(index, buffer, **kw)
def record_halo(level, buffer, **kw):
if level is g:
events.append(("halo", buffer))
@@ -95,7 +96,7 @@ class ThreeLevelCPU(unittest.TestCase):
self.assertIs(kind, g.kind)
events.append(("step", src))
g.kernel.side_effect = record_step
with patch.object(run, "_advance_child", side_effect=record_feed), \
with patch.object(run, "_advance", side_effect=record_feed), \
patch.object(run, "_gather_halo", side_effect=record_halo):
run.step()
self.assertEqual(feeds, [f.current, f.spare])
@@ -105,8 +106,8 @@ class ThreeLevelCPU(unittest.TestCase):
self.assertGreater(len(np.unique(b.tables["block"])), 1)
# Negative control: reusing L1's old source at the midpoint must fail.
feeds.clear()
with patch.object(run, "_advance_child", side_effect=lambda buffer, **kw:
record_feed(f.current, **kw)):
with patch.object(run, "_advance", side_effect=lambda index, buffer, **kw:
record_feed(index, f.current if index == 2 else buffer, **kw)):
with self.assertRaises(AssertionError):
run.step()
run.close()
@@ -172,11 +173,12 @@ class ThreeLevelGPU(unittest.TestCase):
p1, p2 = run.patch, run.child_patch
run.initialize(state(16, 16, 1), state(*p1.fine_shape, 2), state(*p2.fine_shape, 3))
f = run._levels[1]
feeds, original = [], run._advance_child
def record(buffer, **kw):
feeds.append(int(buffer))
original(buffer, **kw)
with patch.object(run, "_advance_child", side_effect=record):
feeds, original = [], run._advance
def record(index, buffer, **kw): # index 2: L1 hop feeds L2
if index == 2:
feeds.append(int(buffer))
original(index, buffer, **kw)
with patch.object(run, "_advance", side_effect=record):
cur, spare = int(f.current), int(f.spare)
run.step(1)
self.assertEqual(feeds, [cur, spare]) # current G, then the new G of hop 1
+222
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@@ -0,0 +1,222 @@
"""Steady DFG 2D-1 (Re 20): refined and uniform runs against the official reference intervals.
Not a full benchmark certification. Declared deviations from the official setup:
pressure-NEQ outlet (``neq_extrap``) instead of do-nothing, local Zou-He inlet.
Geometry, inflow profile, initial state, refined layout and observation reuse the
pinned Re100 runner (``run_refined_dfg``) and ``re100_helpers`` unchanged; only the
lattice viscosity is set for Re 20 (nu = U_lattice * D / 20 at the root level).
Units. The helpers use scaled DFG units with mean inflow speed 1, so
Cd = 2 Fx / (rho U^2 D) and Cl = 2 Fy / (rho U^2 D) are scale-free, and
``pressure_probes`` returns dp / (rho U^2). The official p_diff = p(0.15, 0.2) -
p(0.25, 0.2) uses U = 0.2 m/s, rho = 1, so p_diff = dp * 0.04. Both are reported;
only p_diff is compared with the official interval. Forces use the existing sign
convention: F is the force of the fluid on the cylinder, i.e. the refined raw
exchange impulse (window ledger, ``total.impulse``) or the uniform ``read_force``,
with x along the inflow and y up from the bottom wall. Cd must be positive, and the
official Cl is positive (centre 0.20 below the centreline 0.205), so a flipped sign
shows up as Cl outside its interval.
Sampling. One sample every SAMPLE_TSTAR (t* = U t / D; 0.25 s), taken at the end of
a completed root step with all levels synchronized; the step index is recorded. Cd
and Cl are means over the sample interval (window exchange ledger refined, per-batch
forces uniform), which filters acoustic and step-parity oscillation; p_diff is the
end-of-interval value at the exact surface points.
Steady rule (our engineering choice, frozen before any run; not official). Over the
trailing WINDOW_TSTAR (t* 50..60 inclusive, 21 samples), for each of Cd, Cl and
p_diff: range (max - min) <= 10 % and |least-squares slope * window| <= 2 % of the
width of its official interval. Absolute limits, so the small Cl is never a divisor;
the slope term bounds slow monotone drift that the range alone would pass. If the
rule fails at TSTAR_MAX the run reports "not steady" and gives no interval verdict;
limits are never relaxed after a run. The verdict uses the window mean, and the
distance of each mean to its nearest interval edge is reported (negative outside).
"""
import argparse
import json
import math
import os
from pathlib import Path
import sys
import time
from tempfile import TemporaryDirectory
import numpy as np
HERE = Path(__file__).resolve().parent
sys.path.insert(0, str(HERE))
import run_refined_dfg as rr # noqa: E402
RE = 20.0
U_PHYS = 0.2 # m/s mean inflow; rho = 1
TSTAR_MAX = 60.0 # 30 s physical
SAMPLE_TSTAR = 0.5 # 0.25 s
WINDOW_TSTAR = 10.0 # trailing 5 s, 21 samples
# Schaefer & Turek (1996), 2D-1 lower/upper bounds.
BANDS = dict(cd=(5.57, 5.59), cl=(0.0104, 0.0110), p_diff=(0.1172, 0.1176))
STEADY_RANGE = {k: (hi - lo) / 10 for k, (lo, hi) in BANDS.items()}
STEADY_SLOPE = {k: (hi - lo) / 50 for k, (lo, hi) in BANDS.items()}
DEVIATIONS = ("pressure-NEQ outlet (neq_extrap), not do-nothing", "local Zou-He inlet")
_re100_config = rr.config
def config(h, diameter, collision="SRT", jet_scenario="none"):
"""The pinned Re100 configuration with the lattice viscosity set for Re 20."""
if jet_scenario != "none":
raise ValueError("DFG 2D-1 runs have no Jets")
cfg, body, p = _re100_config(h, diameter, collision, jet_scenario)
nu = p["mean_speed"] * p["diameter"] / RE
cfg["physics"]["viscosity"] = nu
return cfg, body, dict(p, viscosity=nu, re=RE)
def lattice_parameters(diameter, speed=rr.SPEED):
nu = speed * diameter / RE
return dict(viscosity=nu, tau=0.5 + 3 * nu, steps=math.ceil(TSTAR_MAX * diameter / speed),
interval=round(SAMPLE_TSTAR * diameter / speed))
def sample(impulse, n, diameter, dp):
den = rr.SPEED**2 * diameter / 2
return dict(cd=float(impulse[0] / n / den), cl=float(impulse[1] / n / den),
dp_scaled=float(dp), p_diff=float(dp) * U_PHYS**2)
def summarize(rows):
"""Steady rule over the trailing window, then the interval verdict (or none)."""
if not rows or rows[-1]["tstar"] < TSTAR_MAX - 1e-9:
return dict(status="INCOMPLETE", steady=False, verdict=None)
window = [r for r in rows if r["tstar"] >= TSTAR_MAX - WINDOW_TSTAR - 1e-9]
t = np.array([r["tstar"] for r in window])
ranges = {k: max(r[k] for r in window) - min(r[k] for r in window) for k in BANDS}
drifts = {k: abs(np.polyfit(t, [r[k] for r in window], 1)[0]) * WINDOW_TSTAR for k in BANDS}
steady = all(ranges[k] <= STEADY_RANGE[k] and drifts[k] <= STEADY_SLOPE[k] for k in BANDS)
final = {k: float(np.mean([r[k] for r in window])) for k in BANDS}
edge = {k: min(final[k] - BANDS[k][0], BANDS[k][1] - final[k]) for k in BANDS}
result = dict(window_samples=len(window), ranges=ranges, drifts=drifts,
range_limits=STEADY_RANGE, slope_limits=STEADY_SLOPE, steady=steady,
window_mean=final, edge_distance=edge, bands=BANDS,
deviations=DEVIATIONS, cd_positive=final["cd"] > 0)
if not steady:
return dict(result, status="NOT_STEADY", verdict=None)
inside = {k: BANDS[k][0] <= final[k] <= BANDS[k][1] for k in BANDS}
return dict(result, status="WITHIN_INTERVALS" if all(inside.values()) else "OUTSIDE_INTERVALS",
verdict=inside)
def healthy(row):
return row["max_mach"] <= 0.2 and row["rho_min"] >= 0.5 and row["rho_max"] <= 1.5
def run_case(a, h, case):
from contextlib import ExitStack
from CelerisLab.cuda.context import CudaContext
from CelerisLab.lbm.descriptors import FLUID
from CelerisLab.lbm.refinement_stepper import FixedPatchStepper
from CelerisLab.simulation import Simulation
refined = case == "refined"
cfgdict, bodydict, p = config(h, 40 if refined else 80, a.collision)
lp = lattice_parameters(p["diameter"])
rows = []
with ExitStack() as stack:
if refined:
cfg, pair, body, host = rr.host_geometry(a.source, h, a.collision)
context = stack.enter_context(CudaContext(0))
backend = stack.enter_context(FixedPatchStepper(
cfg, rr.PLACEMENTS["wide"], context=context, coarse_boundary="channel",
base_block=rr.BASE_BLOCK, fine_block=rr.FINE_BLOCK, fine_objects=(body,),
observe_raw_exchange=True, observe_window_exchange=True))
from CelerisLab.lbm.channel import channel_masks
from CelerisLab.lbm.refinement import ACTIVE
from CelerisLab.lbm.descriptors import SOLID
masks = [channel_masks(pair.coarse_shape)[0] & ~pair.covered,
(pair.fine_kind == ACTIVE)
& ((host.flags.reshape(pair.fine_shape) & SOLID) == 0)]
backend.initialize(rr.initial_state(pair.coarse_shape, (0.0, 0.0), 1.0, root=True),
rr.initial_state(pair.fine_shape, pair.fine_origin, 0.5))
probe_p = dict(p, center=[(80.5 - pair.fine_origin[0]) / 0.5 - 0.5,
(81.0 - pair.fine_origin[1]) / 0.5 - 0.5], radius=40.0)
else:
tmp = Path(stack.enter_context(TemporaryDirectory()))
(tmp / "lbm.json").write_text(json.dumps(cfgdict))
(tmp / "body.json").write_text(json.dumps(bodydict))
sim = stack.enter_context(Simulation(str(tmp / "lbm.json"), str(tmp / "body.json"),
device_id=0))
sim.initialize()
probe_p = p
fluid = (sim.field.flag.reshape(p["ny"], p["nx"]) & FLUID) != 0
begin = 0
while begin < lp["steps"]:
rr.check_deadline(a.deadline)
n = min(lp["interval"], lp["steps"] - begin)
if refined:
impulse = rr.advance_refined_interval(backend, n, a.deadline, "window")
fields = [rr.macros(g) for g in backend.download()]
rho, ux, uy = fields[1]
fluid = masks[1]
vals = [tuple(v[m] for v in f) for m, f in zip(masks, fields)]
else:
impulse, done = np.zeros(2), 0
while done < n:
batch = min(100, n - done)
sim.run(batch)
impulse += sim.read_force(0).astype(np.float64) * batch
done += batch
m = sim.get_macroscopic()
rho, ux, uy = [np.asarray(m[k], np.float64).reshape(p["ny"], p["nx"])
for k in ("rho", "ux", "uy")]
vals = [(rho[fluid], ux[fluid], uy[fluid])]
begin += n
row = dict(step=begin, tstar=begin * rr.SPEED / p["diameter"],
**sample(impulse, n, p["diameter"],
h.pressure_probes(rho, fluid, probe_p)["dp"]),
rho_min=float(min(v[0].min() for v in vals)),
rho_max=float(max(v[0].max() for v in vals)),
max_mach=float(max(np.sqrt(3 * (v[1]**2 + v[2]**2)).max() for v in vals)))
rr.ensure_finite(row)
rows.append(row)
if not healthy(row):
break
summary = summarize(rows) if healthy(rows[-1]) else dict(status="UNHEALTHY", steady=False,
verdict=None)
return dict(case=case, collision=a.collision, lattice=lp, rows=rows, **summary)
def plan(collision="SRT"):
return dict(re=RE, collision=collision, tstar_max=TSTAR_MAX, sample_tstar=SAMPLE_TSTAR,
window_tstar=WINDOW_TSTAR, bands=BANDS, range_limits=STEADY_RANGE, slope_limits=STEADY_SLOPE,
deviations=DEVIATIONS, pressure_scale=U_PHYS**2,
refined_root=lattice_parameters(40), refined_fine_tau=0.5 + 3 * 2 * rr.SPEED * 40 / RE,
uniform=lattice_parameters(80),
label="compared against the official reference bands (non-canonical neq_extrap outlet, zou_he_local inlet); not a full benchmark certification")
def main():
parser = argparse.ArgumentParser(description=__doc__.splitlines()[0])
parser.add_argument("--case", choices=["refined", "uniform", "both"], default="refined")
parser.add_argument("--collision", choices=["SRT", "MRT"], default="SRT")
parser.add_argument("--source", type=Path, default=rr.DEFAULT_SOURCE)
parser.add_argument("--output", type=Path, required=True)
parser.add_argument("--plan", action="store_true", help="Write the frozen plan; no CUDA")
parser.add_argument("--max-wall-seconds", type=float)
a = parser.parse_args()
a.source = a.source.resolve()
a.output.mkdir(parents=True, exist_ok=False)
(a.output / "plan.json").write_text(json.dumps(plan(a.collision), indent=2, allow_nan=False))
if a.plan:
return
if not a.max_wall_seconds or a.max_wall_seconds <= 0 or not os.environ.get("CUDA_VISIBLE_DEVICES"):
raise SystemExit("GPU run needs --max-wall-seconds > 0 and explicit CUDA_VISIBLE_DEVICES")
h, _ = rr.helpers(a.source)
rr.config = config # host_geometry builds its root configuration through this name
a.deadline = time.monotonic() + a.max_wall_seconds
cases = ["refined", "uniform"] if a.case == "both" else [a.case]
results = [run_case(a, h, case) for case in cases]
(a.output / "result.json").write_text(json.dumps(results, indent=2, allow_nan=False))
if __name__ == "__main__":
main()