PLAID Benchmarks¶
We provide interactive benchmarks hosted on Hugging Face, in which anyone can test their own SciML method. These benchmarks involve regression problems posed on datasets provided in PLAID format. Some of these datasets have been introduced in the MMGP (Mesh Morphing Gaussian Process) paper [1], and the PLAID paper [2]. A ranking is automatically updated based on a score computed on the testing set of each dataset. For the benchmarks to be meaningful, the outputs on the testing sets are not made public.
The relative RMSE is the considered metric for comparing methods. Let \(\{ \mathbf{U}^i_{\rm ref} \}_{i=1}^{n_\star}\) and \(\{ \mathbf{U}^i_{\rm pred} \}_{i=1}^{n_\star}\) be the test observations and predictions, respectively, of a given field of interest. The relative RMSE is defined as
where \(N^i\) is the number of nodes in the mesh \(i\), and \(\max(\mathbf{U}^i_{\rm ref})\) is the maximum entry in the vector \(\mathbf{U}^i_{\rm ref}\). Similarly for scalar outputs:
Resources¶
AirfRANS, introduced in [3] is an additional dataset provided in PLAID format and various variants. Since the outputs on the testing sets are public, no benchmark application is provided for this dataset.
Benchmark results¶
As of August 5, 2025
Dataset |
MGN |
MMGP |
Vi-Transf. |
Augur |
FNO |
MARIO |
|---|---|---|---|---|---|---|
Tensile2d |
0.0673 |
0.0026 |
0.0116 |
0.0154 |
0.0123 |
0.0038 |
2D_MultiScHypEl |
0.0437 |
❌ |
0.0325 |
0.0232 |
0.0302 |
0.0573 |
2D_ElPlDynamics |
0.1202 |
❌ |
0.0227 |
0.0346 |
0.0215 |
0.0319 |
Rotor37 |
0.0074 |
0.0014 |
0.0029 |
0.0033 |
0.0313 |
0.0017 |
2D_profile |
0.0593 |
0.0365 |
0.0312 |
0.0425 |
0.0972 |
0.0307 |
VKI-LS59 |
0.0684 |
0.0312 |
0.0193 |
0.0267 |
0.0215 |
0.0124 |
❌: Not compatible with topology variation
Note
MMGP does not support variable mesh topologies, which limits its applicability to certain datasets and often necessitates custom preprocessing for new cases. However, when morphing is either unnecessary or inexpensive, it offers a highly efficient solution, combining fast training with good accuracy (e.g.,
Tensile2dandRotor37).MARIO is computationally expensive to train but achieves consistently a very strong performance across most datasets. Its result on
2D_MultiScHypElis slightly worse than other tested methods, which may reflect the challenge of capturing complex shape variability in these cases.Vi-Transformer and Augur perform well across all datasets, showing strong versatility and generalization capabilities.
FNO suffers on datasets featuring unstructured meshes with pronounced anisotropies, due to the loss of accuracy introduced by projections to and from regular grids (e.g.,
Rotor37and2D_profile). Additionally, the use of a 3D regular grid onRotor37results in substantial computational overhead.
References¶
F. Casenave, B. Staber, and X. Roynard. MMGP: a Mesh Morphing Gaussian Process-based machine learning method for regression of physical problems under non-parameterized geometrical variability. Thirty-seventh Conference on Neural Information Processing Systems, 2023. URL: https://arxiv.org/abs/2305.12871.
F. Casenave, X. Roynard, B. Staber, W. Piat, M. A. Bucci, N. Akkari, A. Kabalan, X. M. V. Nguyen, L. Saverio, R. Carpintero Perez, A. Kalaydjian, S. Fouché, T. Gonon, G. Najjar, E. Menier, M. Nastorg, G. Catalani, and C. Rey. Physics-Learning AI Datamodel (PLAID) datasets: a collection of physics simulations for machine learning. 2025. URL: https://arxiv.org/abs/2505.02974.
F. Bonnet, J. Mazari, P. Cinnella, and P. Gallinari. AirfRANS: High Fidelity Computational Fluid Dynamics Dataset for Approximating Reynolds-Averaged Navier–Stokes Solutions. In S. Koyejo, S. Mohamed, A. Agarwal, D. Belgrave, K. Cho, and A. Oh, editors, Advances in Neural Information Processing Systems, volume 35, 23463–23478. Curran Associates, Inc., 2022. URL: https://arxiv.org/abs/2212.07564.