Dataset Viewer

The dataset viewer is not available for this subset.

Cannot get the split names for the config 'default' of the dataset.

Exception:    SplitsNotFoundError
Message:      The split names could not be parsed from the dataset config.
Traceback:    Traceback (most recent call last):
                File "/usr/local/lib/python3.12/site-packages/datasets/inspect.py", line 289, in get_dataset_config_info
                  for split_generator in builder._split_generators(
                                         ^^^^^^^^^^^^^^^^^^^^^^^^^^
                File "/usr/local/lib/python3.12/site-packages/datasets/packaged_modules/hdf5/hdf5.py", line 64, in _split_generators
                  with h5py.File(first_file, "r") as h5:
                       ^^^^^^^^^^^^^^^^^^^^^^^^^^
                File "/usr/local/lib/python3.12/site-packages/h5py/_hl/files.py", line 564, in __init__
                  fid = make_fid(name, mode, userblock_size, fapl, fcpl, swmr=swmr)
                        ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
                File "/usr/local/lib/python3.12/site-packages/h5py/_hl/files.py", line 238, in make_fid
                  fid = h5f.open(name, flags, fapl=fapl)
                        ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
                File "h5py/_objects.pyx", line 56, in h5py._objects.with_phil.wrapper
                File "h5py/_objects.pyx", line 57, in h5py._objects.with_phil.wrapper
                File "h5py/h5f.pyx", line 102, in h5py.h5f.open
              FileNotFoundError: [Errno 2] Unable to synchronously open file (unable to open file: name = 'hf://datasets/polymathic-ai/euler_multi_quadrants_openBC@9fc7040e6915d58fc61a23aa91441f9b2bc7c575/data/train/euler_multi_quadrants_openBC_gamma_1.13_C3H8_16.hdf5', errno = 2, error message = 'No such file or directory', flags = 0, o_flags = 0)
              
              The above exception was the direct cause of the following exception:
              
              Traceback (most recent call last):
                File "/src/services/worker/src/worker/job_runners/config/split_names.py", line 65, in compute_split_names_from_streaming_response
                  for split in get_dataset_split_names(
                               ^^^^^^^^^^^^^^^^^^^^^^^^
                File "/usr/local/lib/python3.12/site-packages/datasets/inspect.py", line 343, in get_dataset_split_names
                  info = get_dataset_config_info(
                         ^^^^^^^^^^^^^^^^^^^^^^^^
                File "/usr/local/lib/python3.12/site-packages/datasets/inspect.py", line 294, in get_dataset_config_info
                  raise SplitsNotFoundError("The split names could not be parsed from the dataset config.") from err
              datasets.inspect.SplitsNotFoundError: The split names could not be parsed from the dataset config.

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YAML Metadata Warning: empty or missing yaml metadata in repo card (https://huggingface.co/docs/hub/datasets-cards)

Euler Multi-quadrants - Riemann problems (compressible, inviscid fluid)

NOTE: this dataset is distributed in two separate datasets: euler_multi_quadrants_openBC with open boundary conditions and euler_multi_quadrants_periodicBC with periodic boundary conditions.

One line description of the data: Evolution of different gases starting with piecewise constant initial data in quadrants.

Longer description of the data: The evolution can give rise to shocks, rarefaction waves, contact discontinuities, interaction with each other and domain walls.

Associated paper: Paper.

Domain experts: Marsha Berger(Flatiron Institute & NYU), Ruben Ohana (CCM, Flatiron Institute & Polymathic AI), Michael McCabe (Polymathic AI).

Code or software used to generate the data: Clawpack (AMRClaw).

Equation: Euler equations for a compressible gas:

$\begin{align*} U_t + F(U)_x + G(U)_y &= 0 \\ \textrm{where} \quad U = \begin{bmatrix} \rho \\ \rho u \\ \rho v \\ e \end{bmatrix}, \quad F(U) = \begin{bmatrix} \rho u \\ \rho u^2 + p \\ \rho u v \\ u(e + p) \end{bmatrix},& \quad G(U) = \begin{bmatrix} \rho v \\ \rho u v \\ \rho v^2 + p \\ v(e + p) \end{bmatrix}, \quad \\ e = \frac{p}{(\gamma - 1)} + \frac{\rho (u^2 + v^2)}{2}&, \quad p = A\rho^{\gamma}. \end{align*}$

with $\rho$ the density, $u$ and $v$ the $x$ and $y$ velocity components, $e$ the energy, $p$ the pressure, $\gamma$ the gas constant, and $A>0$ is a function of entropy.

Dataset	FNO	TFNO	Unet	CNextU-net
`euler_multi-quadrants_periodicBC`	0.4081	0.4163	0.1834	$\mathbf{0.1531}$

Table: VRMSE metrics on test sets (lower is better). Best results are shown in bold. VRMSE is scaled such that predicting the mean value of the target field results in a score of 1.

About the data

Dimension of discretized data: 100 timesteps of 512x512 images.

Fields available in the data: density (scalar field), energy (scalar field), pressure (scalar field), momentum (vector field).

Number of trajectories: 500 per set of parameters, 10 000 in total.

Estimated size of the ensemble of all simulations: 5.17 TB.

Grid type: uniform, cartesian coordinates.

Initial conditions: Randomly generated initial quadrants.

Boundary conditions: Periodic or open.

Simulation time-step: variable.

Data are stored separated by ($\Delta t$): 0.015s (1.5s for 100 timesteps).

Total time range ($t_{min}$ to $t_{max}$): $t_{min} = 0$, $t_{max}=1.5s$.

Spatial domain size ($L_x$, $L_y$): $L_x = 1$ and $L_y = 1$.

Set of coefficients or non-dimensional parameters evaluated: all combinations of $\gamma$ constant of the gas at a certain temperature: $\gamma=${1.13,1.22,1.3,1.33,1.365,1.4,1.404,1.453,1.597,1.76} and boundary conditions: {extrap, periodic}.

Approximate time to generate the data: 80 hours on 160 CPU cores for all data (periodic and open BC).

Hardware used to generate the data and precision used for generating the data: Icelake nodes, double precision.

What is interesting and challenging about the data:

What phenomena of physical interest are catpured in the data: capture the shock formations and interactions. Multiscale shocks.

How to evaluate a new simulator operating in this space: the new simulator should predict the shock at the right location and time, and the right shock strength, as compared to a pressure gauge monitoring the exact solution.

Please cite the associated paper if you use this data in your research:

@article{mandli2016clawpack,
  title={Clawpack: building an open source ecosystem for solving hyperbolic PDEs},
  author={Mandli, Kyle T and Ahmadia, Aron J and Berger, Marsha and Calhoun, Donna and George, David L and Hadjimichael, Yiannis and Ketcheson, David I and Lemoine, Grady I and LeVeque, Randall J},
  journal={PeerJ Computer Science},
  volume={2},
  pages={e68},
  year={2016},
  publisher={PeerJ Inc.}
}

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