Datasets:
PoreML V1 — pore-scale multiphase flow trajectories
![]() drainage — capillary-dominated invasion of a rock; here a generated sphere pack at 256³, the front still compact |
![]() trapping — a flood strands disconnected ganglia; predicting which blobs survive is the hard part |
![]() GDL — water transport through a fuel-cell gas-diffusion layer, a thin high-porosity fibrous slab |
![]() underfill — capillary underfill of a flip-chip package, a coherent front sweeping past solder bumps |
Blue is the invading phase, grey the solid. One stored frame per campaign, at roughly 70 % of the trajectory.
560 lattice-Boltzmann simulations of two-phase flow through porous media — 158,546 stored 3-D frames, 3.32 TB. Four campaigns, seven geometry families, real micro-CT rock alongside procedurally generated media, at two spatial resolutions. Every run carries the solver's own metadata, so a trajectory can be traced back to the geometry, the capillary number and the contact angle that produced it.
The dataset is the benchmark behind poreml, and it is published whole rather than as a
curated subset, so that training, held-out evaluation and transfer tests can all be drawn from
the same 560 runs.
At a glance
| campaign | families | runs | frames | size | domain (D × H × W) | what it is |
|---|---|---|---|---|---|---|
| drainage | bentheimer, buffberea, castlegate (µCT) · blob, poly, sphere (generated) | 176 | 69,473 | 1,046 GB | 128×128×161 · 256×256×289 | capillary-dominated invasion of a rock, inlet reservoir → rock → porous plate → outlet |
| GDL | gdl_ct, gdl_ct_20, gdl_ct_40 (µCT) · fiber (generated) | 176 | 53,654 | 1,080 GB | 128×128×77 · 256×256×141 | water transport in fuel-cell gas-diffusion layers, a thin high-porosity fibrous slab |
| trapping | bentheimer, buffberea, castlegate (µCT) · blob, poly, sphere (generated) | 176 | 23,040 | 390 GB | 128×128×144 · 256×256×272 | two-stage: equilibration, then a flood that strands disconnected ganglia |
| underfill | flipchip (generated) | 32 | 12,379 | 808 GB | 22–48 × 482 × 432–476 | capillary underfill of a flip-chip package, a wide thin domain around solder bumps |
| total | 560 | 158,546 | 3,324 GB |
Each campaign exists at a 128-class resolution and, except underfill, a 256-class resolution — 16 runs per campaign, the same geometry families at twice the linear size.
Download
The repository is the dataset directory. Clone it straight into data/case and the paths
line up with the benchmark's default data.root with nothing to move:
pip install huggingface_hub hdf5plugin h5py
hf download PoreML/PoreML_V1 --repo-type dataset --local-dir data/case
One campaign, or one family, is a glob away — useful, since the full set is 3.3 TB:
# just the 128-class GDL runs (~476 GB)
hf download PoreML/PoreML_V1 --repo-type dataset --local-dir data/case \
--include "GDL/runs/*/128x128x64/*"
# a single run (~3.2 GB)
hf download PoreML/PoreML_V1 --repo-type dataset --local-dir data/case \
--include "drainage/runs/blob/128/drain_blob128_0000_128_M1_th140_b99/*"
from huggingface_hub import snapshot_download
snapshot_download("PoreML/PoreML_V1", repo_type="dataset", local_dir="data/case",
allow_patterns=["trapping/runs/sphere/128/*"])
hdf5pluginis not optional. Every trajectory is Zstandard-compressed (HDF5 filter id 32015).import hdf5pluginbeforeh5py.File(...)or HDF5 reports the filter as unavailable and the read fails. Forh5ls/h5dump, pointHDF5_PLUGIN_PATHathdf5plugin's plugin directory.
Layout
Every run is one directory, at <campaign>/runs/<family>/<size>/<run_id>/. <size> is the
geometry's shape (128, 128x128x64, 256, 256x256x128, 26x482x476); the simulated
domain is longer along the flow axis, see below.
drainage and GDL — one stage, one trajectory:
<run_id>.h5 the trajectory — zstd-3 HDF5
<run_id>.xdmf ParaView index over the .h5 (relative paths)
run_meta.json solver, geometry, environment, progress, protocol (`extra`)
metrics.csv the solver's own per-block scalars (saturation, front position, pressures)
report.md the solver's one-page run summary
<run_id>.conversion.json how this copy was produced: encoding, sizes and checksums
trapping — two stages, and note there is no plain run_meta.json. The stored trajectory
is the second (flood) stage; the equilibration that preceded it is described but not stored:
flood_<run_id>.h5 the flood trajectory — the only .h5 in the directory
flood_<run_id>.xdmf
run_meta_flood.json the flood stage: its `status` / `finish_type` describe the .h5
run_meta_stab.json the preceding equilibration stage (no trajectory kept)
metrics_flood.csv per-block scalars, one file per stage
metrics_stab.csv
flood_report.md
stab_report.md
<run_id>.conversion.json
underfill — the HDF5 carries a uf_ prefix, and the geometry is generated, so its
parameters travel with it:
uf_<run_id>.h5
uf_<run_id>.xdmf
run_meta.json
metrics.csv
report.md
<run_id>_geometry.json the generated flip-chip geometry's parameters
<run_id>.npy the solid mask as bool — identical to `/rock` in the .h5, kept for convenience
<run_id>.conversion.json
A reader should glob for the single *.h5 in a run directory rather than assume the file is
named after the run, and should fall back to run_meta_flood.json where run_meta.json is
absent.
Reading one frame
import glob, json
import h5py, hdf5plugin # noqa: F401 — registers the Zstandard filter
import numpy as np
run = "data/case/drainage/runs/blob/128/drain_blob128_0000_128_M1_th140_b99"
meta = json.load(open(f"{run}/run_meta.json"))
lo, hi = meta["extra"]["regions"]["rock"] # score the rock, not the buffers
M, theta = meta["extra"]["M"], meta["solver"]["theta"]
with h5py.File(glob.glob(f"{run}/*.h5")[0], "r") as f:
solid = f["rock"][..., lo:hi].astype(bool) # 1 = solid
steps = sorted(f["steps"])
phi = f[f"steps/{steps[len(steps) // 2]}/phi"][..., lo:hi]
pore = ~solid
phi = np.where(pore, phi, -1.0) # phi is NaN inside solid
saturation = (phi[pore] > 0).mean() # non-wetting fraction of the pore space
print(f"{len(steps)} frames | M={M} theta={theta} | rock {solid.shape} "
f"porosity={pore.mean():.3f} | S_nw={saturation:.3f}")
# 380 frames | M=1.0 theta=140.0 | rock (128, 128, 128) porosity=0.283 | S_nw=0.305
Inside a trajectory
/rock (D, H, W) uint8 1 = solid
/steps/<step:09d>/phi (D, H, W) float32 phase field; > 0 non-wetting, < 0 wetting, NaN in solid
/steps/<step:09d>/p (D, H, W) float32 pressure
/steps/<step:09d>/u (D, H, W, 3) float32 velocity
Root attributes carry fields (phi,p,u), dtype, shape, the run conditions — M (viscosity
ratio), ca (capillary number), theta (contact angle, degrees), sigma, nu0, chi,
cs2 = 1/3, u_in — and run_meta, a JSON snapshot of the metadata taken while the run was
writing. Frames are stored every 5,000 lattice steps in drainage, GDL and the trapping flood,
and every 1,000 in underfill and the trapping equilibration stage (extra.block).
Three things bite readers who treat the arrays naively:
phiisNaNinside the solid, not zero. Fill it before it reaches a model or a loss (poremluses −1.0) and mask it out of any metric.- The domain is longer than the rock along the last axis.
extra.regionsin the metadata gives the half-open spans: drainage hasinbuf,rock,plate,outbuf(e.g.{"inbuf": [0,7], "rock": [7,135], "plate": [135,155], "outbuf": [155,161]}), GDL and trapping haveinbuf,rock,outbuf, and underfill records no regions because it has no buffers. Saturation computed over the whole domain will not agree with the solver's ownmetrics.csv: the inlet buffer is always fully invaded and the plate is a boundary device, so score therockspan. - The last spatial axis is the flow axis, inlet at index 0, outlet at −1.
rho and umag are not stored. Both were exact functions of what is here — rho = p / cs2
and umag = ‖u‖ — and together cost 32 % of the bytes, so they were dropped in a 2026-09-13
repack. Recompute them if you need them.
Physics and sampling
Colour-gradient lattice Boltzmann, D3Q19, immiscible two-phase, β = 0.99. Each campaign sweeps
a grid of viscosity ratio M against contact angle theta:
| campaign | M |
theta |
ca |
|---|---|---|---|
| drainage | 0.05, 0.1, 0.2, 1 | 120°, 130°, 140°, 150° | 1 × 10⁻⁵ |
| GDL | 1, 5, 10, 20 | 120°, 130°, 140°, 150° | 1 × 10⁻⁵ |
| trapping | 0.05, 0.1, 0.2, 1 | 120°, 130°, 140°, 150° | not recorded |
| underfill | 5, 10, 20, 30 | 30°, 40°, 50° | not recorded |
Contact angles above 90° make the invading phase non-wetting (drainage); the underfill
campaign is the wetting-invasion case. The capillary number is held fixed and low in the two
campaigns that record it, so those runs are capillary-dominated. M and theta are the only
two conditions the benchmark conditions its models on — trapping and underfill record no ca,
so it is the one parameter that cannot span every campaign.
Runs stop on their own terms and record why in status / finish_type — breakthrough,
pore-volume cap, immobilisation of the invading phase, or a filled package. Trajectory length
therefore varies a great deal (17 to 1,266 stored frames), which is why any aggregate over
this dataset should average per run first, then over runs; otherwise the long runs
dominate.
Citation
@misc{poreml_v1,
title = {PoreML V1: pore-scale multiphase flow trajectories for machine-learning benchmarks},
author = {PoreML},
year = {2026},
howpublished = {\url{https://huggingface.co/datasets/PoreML/PoreML_V1}}
}
Released under the MIT licence.
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