video video 8 8 | label class label 25
classes |
|---|---|
0Re100_psi0 | |
0Re100_psi0 | |
0Re100_psi0 | |
1Re100_psi15 | |
1Re100_psi15 | |
1Re100_psi15 | |
2Re100_psi30 | |
2Re100_psi30 | |
2Re100_psi30 | |
3Re100_psi45 | |
3Re100_psi45 | |
3Re100_psi45 | |
4Re100_psi60 | |
4Re100_psi60 | |
4Re100_psi60 | |
5Re150_psi0 | |
5Re150_psi0 | |
5Re150_psi0 | |
6Re150_psi15 | |
6Re150_psi15 | |
6Re150_psi15 | |
7Re150_psi30 | |
7Re150_psi30 | |
7Re150_psi30 | |
8Re150_psi45 | |
8Re150_psi45 | |
8Re150_psi45 | |
9Re150_psi60 | |
9Re150_psi60 | |
9Re150_psi60 | |
10Re200_psi0 | |
10Re200_psi0 | |
10Re200_psi0 | |
11Re200_psi15 | |
11Re200_psi15 | |
11Re200_psi15 | |
12Re200_psi30 | |
12Re200_psi30 | |
12Re200_psi30 | |
13Re200_psi45 | |
13Re200_psi45 | |
13Re200_psi45 | |
14Re200_psi60 | |
14Re200_psi60 | |
14Re200_psi60 | |
15Re300_psi0 | |
15Re300_psi0 | |
15Re300_psi0 | |
16Re300_psi15 | |
16Re300_psi15 | |
16Re300_psi15 | |
17Re300_psi30 | |
17Re300_psi30 | |
17Re300_psi30 | |
18Re300_psi45 | |
18Re300_psi45 | |
18Re300_psi45 | |
19Re300_psi60 | |
19Re300_psi60 | |
19Re300_psi60 | |
20Re50_psi0 | |
20Re50_psi0 | |
20Re50_psi0 | |
21Re50_psi15 | |
21Re50_psi15 | |
21Re50_psi15 | |
22Re50_psi30 | |
22Re50_psi30 | |
22Re50_psi30 | |
23Re50_psi45 | |
23Re50_psi45 | |
23Re50_psi45 | |
24Re50_psi60 | |
24Re50_psi60 | |
24Re50_psi60 |
Parametric rotating-cube CFD dataset
Unsteady laminar flow around a finite, rotating cube, simulated with OpenFOAM ESI
v2512 (pimpleFoam, AMI sliding-mesh) over a 2-D parameter grid. Built to train/evaluate
neural operators on oscillating/rotating-structure flows, extending the 3-D rotating-cube
case of Gao, Cheng & Jaiman (φ-GNN) from a single simulation to a 25-case sweep.
Parameter grid (25 cases)
- Re ∈ {50, 100, 150, 200, 300} — varied by viscosity only (
nu = U·c/Re, withU=c=1). - psi ∈ {0, 15, 30, 45, 60}° — inflow elevation out of the x–y plane,
U_inf = (cos psi, 0, sin psi); in-plane azimuthbeta = 0(a symmetry, fixed). - Constant everywhere:
|U_inf|=1, cube edgec=1, physical spinomega=0.25rad/s (omega* = omega·c/U = 0.25),dt* = 5e-3, sampling every 8 steps (dt*_sample = 0.04), tot* = 200. The cube rotates about +z; rotation sense fixed.
psi is the physically meaningful axis: tilting the inflow toward the spin axis adds an
axial through-flow that is not reducible to a frame rotation (oblique/yawed rotating
flow, helical wakes). beta is degenerate (frame rotation about z) and held at 0.
Repository layout
data/<case>/<case>.tar.zst.partNNN # ~4 GB split parts of the per-case archive
data/<case>/<case>.tar.zst.sha256 # checksum of the reassembled archive
data/<case>/PARTS_COMPLETE # marker: all parts for this case are uploaded
visualization/<case>/ # 3 mp4s per case: vorticity, Umag (|U|), p (z=0 slice)
code/ # generator + solver + visualization scripts
README.md # this card
Archives are split into ~4 GB parts (the run server's uplink can't reliably commit a single 55 GB file). Reassemble a case, verify, and extract:
cat data/Re100_psi30/Re100_psi30.tar.zst.part* > Re100_psi30.tar.zst
sha256sum -c data/Re100_psi30/Re100_psi30.tar.zst.sha256 # (path in the .sha256 is the bare name)
zstd -d Re100_psi30.tar.zst -c | tar -x # -> Re100_psi30/
Each <case>.tar.zst extracts to an OpenFOAM case directory decomposed across 12 MPI
ranks (processor0..11/). Storage is lean by design: the rigid-rotation mesh is
stored once (processor*/constant/polyMesh, with the rotating cellZone), and only
U and p are written per snapshot (binary), 4991 snapshots per case over t* = 0..200.
Reconstructing a sample
The mesh is the t=0 configuration; the inner cylinder (r < c) co-rotates rigidly. To get
physical node positions at snapshot time t, rotate the rotating cellZone points by
theta = omega·t about +z (omega = 0.25). U is stored in the absolute frame. A
worked z=0-slice example (with this rotation applied) is in code/visualize_sample.py.
Force coefficients (stationary average, t* ∈ [150, 200])
Aref = c² = 1, magUInf = 1; Cd drag (x), Cl lift (y, Magnus), Cs axial (z).
| Re \ psi | 0° | 15° | 30° | 45° | 60° |
|---|---|---|---|---|---|
| Cd 50 | 2.334 | 2.270 | 2.094 | 1.790 | 1.321 |
| 100 | 1.718 | 1.690 | 1.620 | 1.428 | 1.038 |
| 150 | 1.513 | 1.497 | 1.407 | 1.289 | 0.916 |
| 200 | 1.423 | 1.413 | 1.307 | 1.075 | 0.843 |
| 300 | 1.358 | 1.354 | 1.297 | 1.096 | 0.641 |
| Cs 50 | 0.000 | -0.653 | -1.163 | -1.535 | -1.811 |
| 100 | 0.000 | -0.503 | -0.844 | -1.109 | -1.308 |
| 150 | 0.000 | -0.463 | -0.824 | -0.991 | -1.155 |
| 200 | 0.000 | -0.450 | -0.827 | -1.087 | -1.095 |
| 300 | 0.000 | -0.430 | -0.816 | -1.032 | -1.149 |
Trends (both axes carry distinct physics): Cd falls with Re and with psi; Cs (axial force) grows 0 → ~-1.8 with psi; in-plane shedding amplitude shrinks with psi and grows with Re; Cl < 0 throughout (Magnus lift from the fixed +z spin).
Validation & caveats
- Static-cube validation (low-blockage, separate mesh): Cd = 0.978 vs paper 0.935, empirical bracket [0.854, 1.122] — pass.
- Laminar-validity ceiling: highest at the high-Re / low-psi corner (Re=300, psi ≤ 15), where shedding fluctuation peaks; treat that corner as the resolution/validity edge of the current mesh. Higher psi monotonically stabilises the wake.
- Mesh: ~294k hex cells, semi-structured (O-grid in x–y, banded in z); cube finite in z (|z| < c/2). Numerics: 2nd-order implicit time, Gauss linear, PIMPLE, 1 non-orthogonal corrector, residual tol 1e-8.
Citation
Reproduces/extends: R. Gao, Z. Cheng, R. K. Jaiman, A Mesh-Adaptive Hypergraph Neural Network for Unsteady Flow Around Oscillating and Rotating Structures.
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