Datasets:
Re float64 20 90 | regime stringclasses 2
values | strouhal float64 0 0.24 | t float32 161 200 | vorticity list | wake_amplitude float64 0 0.47 |
|---|---|---|---|---|---|
20 | steady | 0 | 160.5 | [[3.3364624977111816,7.565970420837402,5.745246887207031,3.5771536827087402,2.4402363300323486,1.776(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 161 | [[3.3364601135253906,7.5659637451171875,5.745244026184082,3.577150821685791,2.440220355987549,1.7763(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 161.5 | [[3.336465835571289,7.565976142883301,5.74524450302124,3.5771384239196777,2.4402284622192383,1.77634(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 162 | [[3.3364644050598145,7.565984725952148,5.745255470275879,3.577155113220215,2.440234899520874,1.77633(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 162.5 | [[3.336461067199707,7.565976142883301,5.745248794555664,3.5771477222442627,2.4402334690093994,1.7763(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 163 | [[3.336459159851074,7.565969944000244,5.745251178741455,3.577162981033325,2.4402406215667725,1.77634(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 163.5 | [[3.3364615440368652,7.565975189208984,5.745244979858398,3.5771431922912598,2.4402174949645996,1.776(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 164 | [[3.3364696502685547,7.565978050231934,5.74525260925293,3.577162742614746,2.4402403831481934,1.77633(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 164.5 | [[3.336459159851074,7.565987586975098,5.745251655578613,3.5771427154541016,2.4402194023132324,1.7763(...TRUNCATED) | 0.000001 |
20 | steady | 0 | 165 | [[3.3364627361297607,7.56597900390625,5.745248317718506,3.577138900756836,2.440225124359131,1.776340(...TRUNCATED) | 0.000001 |
Confined cylinder wake, lattice-Boltzmann, Re 20-100 (9 runs, 720 vorticity snapshots, 240 x 100)
2-D flow past a cylinder (diameter D = 20 lattice cells) 3 D downstream of a uniform inlet in a channel 5 D high and 12 D long (blockage 0.2), no-slip walls, pressure outlet; D2Q9 BGK lattice-Boltzmann, inlet velocity 0.1 (Mach 0.17), no turbulence model. Each run covers 200 convective units (t U / D); the last 40 are stored (saturated wake), a vorticity snapshot (normalised by U/D, 0 inside the cylinder) every 0.5 units, labelled by Reynolds number, wake regime (steady or shedding), Strouhal number and wake amplitude. For regime classification, interpolation in Re and wake forecasting. The channel is far shorter than the entrance length, so the cylinder sees a nearly uniform inflow with thin wall boundary layers. Grid: x = i, y = j lattice cells, cylinder centre and solid cells in meta.json.
cylinder_wake_lbm v1.0.0 (revision v1.0.0) · licence cc-by-4.0 · part of the PINNeAPPle zoo
Configs and splits
| Config | Split | Samples | Parquet rows | Parquet files | Content |
|---|---|---|---|---|---|
default |
train |
480 | 480 | 1 | 6 runs, Re 20, 30, 50, 60, 80, 90 (80 snapshots each) |
default |
test |
240 | 240 | 1 | 3 held-out Reynolds numbers, Re 40, 70, 100 (80 snapshots each) |
Split rule: by Reynolds number: every snapshot of a run is in the same split
Columns
| Column | Unit | Type | Description |
|---|---|---|---|
Re |
- | float64 | Reynolds number U D / nu |
regime |
- | string | wake regime of the run: steady or shedding |
strouhal |
- | float64 | Strouhal number f D / U of the run (0 for a steady wake) |
t |
D/U | float32 | convective time of the snapshot |
vorticity |
U/D | float32[240, 100] | vorticity on the 240 x 100 lattice (x along the channel), 0 in the cylinder |
wake_amplitude |
- | float64 | rms transverse velocity / U, 2 D behind the cylinder |
Load
With the library (the npz files, SHA-256 checked; arrays with their full shape):
pip install "pinneapple @ git+https://github.com/PINNeAPPle-Labs/PINNeAPPle"
import pinneapple as pp
d = pp.datasets.load("cylinder_wake_lbm", split="test")
print(d.n_rows, d.columns)
print(d["vorticity"].shape)
With datasets (the Parquet files of this repo):
from datasets import load_dataset
ds = load_dataset("PINNeAPPle-Labs/cylinder-wake-lbm", split="test", revision="v1.0.0")
print(ds)
ds = ds.with_format("numpy")
print(ds[0]["vorticity"].shape)
Provenance
python scripts/zoo/cylinder_data.py generate --out DIR; pinneapple_simulation.numerical_solvers.cylinder_wake (the lab experiment cylinder_lbm runs the same function)
Verification
Solver checks (python scripts/zoo/cylinder_data.py verify; pinneapple_simulation.numerical_solvers.cylinder_wake.verify): developed low-Re channel flow against plane Poiseuille, max profile error 7.6 % / 4.3 % on the 2x coarser / dataset grid (first order, full-way bounce-back walls), centreline over mean velocity 1.43 / 1.46 vs 1.5. Resolution study at Re 100 (D = 20, 30, 40 lattice cells, same physical time and sampling): Strouhal 0.2444 / 0.2458 / 0.2460, so the dataset grid (D = 20) is within 0.7 % of D = 40; vorticity rms 2 D behind the cylinder within 0.3 %; transverse-velocity rms within 6.7 % (0.9 % at D = 30). At Re 120, D = 20 gives a Strouhal number 4.4 % below D = 30 (relaxation time 0.55, near the stability limit), so the dataset stops at Re 100. Every shedding run is saturated: the probe rms changes by at most 5 % across the stored window; below the onset (Re <= 50, confinement delays it from the unconfined ~47) disturbances decay. Strouhal number from a Hann-windowed, peak-refined spectrum (raw FFT bins are 0.025 apart). All fields finite.
Files
The npz files are the library's format and the source of truth: pp.datasets.load downloads them from this repo at the tagged revision and refuses any file whose SHA-256 differs from the manifest of the package. The Parquet files under data/ are derived from them by pinneapple_hub.zoo.parquet.write_dataset and hold the same numbers (a test round-trips npz -> Parquet -> arrays bit for bit); they are what the dataset viewer and load_dataset read.
| File | Size | SHA-256 |
|---|---|---|
train-00.npz |
28.3 MB | 7932f317a12d52e77abb0cebbcf32f750562650999279b32f83dbdbf6008127f |
train-01.npz |
14.2 MB | 86f534293e63c57ec2fa9e0c0213a386b3b245b64e69a5dfb82d66938e38b672 |
test.npz |
21.3 MB | 6c50430490bfd1493067cf016b11fb1073034f2ab5b6ca97afb09a40ac46e130 |
Total 63.8 MB of npz.
Citation
Cylinder wake dataset generated with PINNeAPPle (pinneapple_simulation.numerical_solvers.cylinder_wake, D2Q9 lattice Boltzmann); PINNeAPPle, Zenodo DOI 10.5281/zenodo.23343062.
Cite
If you use this dataset, please cite PINNeAPPle (software, Zenodo DOI 10.5281/zenodo.23343062; see CITATION.cff):
@software{pinneapple,
author = {Barros, Yan and Schiassi, Enrico},
title = {PINNeAPPle},
doi = {10.5281/zenodo.23343062},
url = {https://github.com/PINNeAPPle-Labs/PINNeAPPle}
}
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