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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, with U=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 azimuth beta = 0 (a symmetry, fixed).
  • Constant everywhere: |U_inf|=1, cube edge c=1, physical spin omega=0.25 rad/s (omega* = omega·c/U = 0.25), dt* = 5e-3, sampling every 8 steps (dt*_sample = 0.04), to t* = 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 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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