Pith. sign in

REVIEW 4 major objections 5 minor 7 cited by

X-MeshGraphNet: Scalable Multi-Scale Graph Neural Networks for Physics Simulation

T0 review · 4 major / 5 minor · reviewed 2026-08-12 · deepseek-v4-flash

Pith's one-line read Partitioning a GNN into halo-padded subgraphs matches full-graph training.

desk verdict Solid scalability engineering with a sound halo-equivalence argument, but the headline accuracy claim is untested against any full-graph or mesh-based baseline. read the letter →

arxiv 2411.17164 v2 pith:7Z3YWQPE submitted 2024-11-26 cs.LG physics.comp-ph

classification cs.LGphysics.comp-ph
keywords graphneuralnetworksphysicssimulationpartitioninghaloregionsmulti-scalemesh-freecomputationalfluiddynamicsautomotiveaerodynamics
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

X-MeshGraphNet claims that a graph neural network for physics simulation can be trained on many small partitions of a large graph without losing accuracy, provided each partition carries a halo of nodes wide enough to cover the number of message-passing layers. When gradients from all partitions are aggregated before each update, the paper argues, partitioned training is mathematically equivalent to training on the full graph, so memory can be cut almost linearly by increasing the number of partitions. It also removes the need for simulation meshes by building graphs directly from uniform point clouds sampled on an object's surface and connecting each point to its k nearest neighbors, and it layers coarse and fine point clouds into a multi-scale graph for long-range interactions. On a 500-car aerodynamic dataset, the model predicts surface pressure and wall shear stress with an R² of 0.942 for drag force, and the same halo scheme is extended to a 3D UNet for volumetric flow prediction.

What carries the argument

The load-bearing mechanism is halo partitioning: the graph is split into balanced subgraphs by a partitioning scheme, each subgraph is padded with a halo containing all nodes within a distance of L hops, where L is the number of message-passing layers, and the subgraphs are treated as independent batches whose gradients are summed before the optimizer step. Because message passing is local, every non-halo node's update depends on exactly the same nodes it would depend on in the full graph, which is what makes the equivalence claim hold. The second mechanism is the custom multi-scale graph: nested point clouds (500k, 1M, and 2M points in the case study) where each level is a superset of the previous, connected by k-nearest-neighbor edges, with 5-nearest-neighbor inverse-distance interpolation used to map CFD ground truth onto the point cloud.

What would settle it

Run the same training setup on a geometry with thin or highly curved surface features and compare predictions when the number of nearest neighbors is increased from 6 to, say, 12; if accuracy on those regions changes materially, the k-NN point-cloud graph is not preserving the surface connectivity the model needs.

Watch

Extended reading notes

Core claim

The paper's central discovery is that halo-region partitioning with gradient aggregation makes distributed GNN training equivalent to full-graph training as long as the halo size equals the number of message-passing layers and no operation depends on global statistics. Because each partition then contains the complete L-hop computational neighborhood of every non-halo node, forward and backward passes produce exactly the gradients the full graph would produce. This equivalence lets X-MeshGraphNet scale to graphs with millions of nodes on limited GPU memory, and it extends the same partitioning idea to convolutional UNet architectures by setting the halo size to the network's receptive field. Alongside this, the paper shows that a k-nearest-neighbor graph on a uniform surface point cloud from an STL file can replace a simulation mesh as the model input, eliminating meshing at inference while matching full-graph accuracy.

Load-bearing premise

The argument depends on the assumption that a uniform point cloud on an object's surface, connected by six nearest-neighbor edges, faithfully represents the physical surface, and that interpolating simulation data onto that cloud with five nearest neighbors loses negligible accuracy.

Editorial extensions

If this is right

  • Memory usage scales down almost proportionally with the number of partitions: peak GPU memory dropped from 50.4 GB on one partition to 3 GB on 32 partitions for a 1-level graph.
  • Training across partitions is equivalent to full-graph training, so models can be trained on graphs too large for any single GPU without sacrificing accuracy.
  • Inference needs only the CAD geometry, not a generated mesh, so real-time aerodynamic predictions become practical.
  • The halo-partitioning idea carries over to UNet-style volume models, with halo size matched to the receptive field, producing a scalable 3D flow predictor.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The equivalence argument only survives if the network avoids global statistics like batch normalization; a useful follow-up would be to test whether a group-normalized or layer-normalized variant retains the same partition equivalence in practice.
  • Because the graph is built from point clouds independently of any mesh, the approach should extend to dynamic or deformable geometries by re-sampling and re-partitioning per time step, a direction the authors name as future work.
  • If k-NN surface graphs prove sufficient for a range of geometries, mesh generation could disappear from the surrogate-modeling pipeline entirely, shifting the bottleneck to point-cloud sampling and graph partitioning.
  • A direct test of the interpolation assumption would be to compare predictions trained on interpolated point-cloud targets against predictions trained on native mesh-node targets for the same geometries.
Share X Bluesky LinkedIn Reddit HN

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

4 major / 5 minor

Summary. The paper proposes X-MeshGraphNet, an extension of MeshGraphNet that trains on large graphs by partitioning them into subgraphs with halo regions of width equal to the number of message-passing layers, combined with gradient aggregation, and claims this is equivalent to full-graph training. The model also removes the need for simulation meshes by constructing graphs from STL geometry via uniform point-cloud sampling and k-nearest-neighbor connectivity, and builds multi-scale graphs by nesting fine point clouds around coarse ones. The method is evaluated on the DrivAerML automotive aerodynamics dataset for surface pressure and wall shear stress prediction, reporting R2=0.942 for force and average relative errors in Table I. The paper further reports memory-scaling and strong-scaling experiments on H100 clusters comparing X-MeshGraphNet with a distributed message-passing MeshGraphNet baseline, and extends the halo-partitioning scheme to a 3D UNet model for volumetric flow-field prediction.

Significance. If the central claims hold, the paper offers a practical contribution: it provides a theoretically grounded way to partition GNN training across GPUs without changing the model's computations, and it eliminates the mesh-generation bottleneck at inference by working directly from tessellated geometry. The halo-equivalence argument in Section III-A is mathematically sound under the stated conditions (halo size at least the number of layers, no global batch statistics, and correct gradient aggregation), and the memory-scaling measurements in Section V-F are credible and useful. The release of code through NVIDIA Modulus is a concrete strength. However, the empirical support for the headline accuracy claim is incomplete, and the custom k-NN graph construction introduces a physical-fidelity risk that is not directly validated. The multi-scale architecture is also under-specified, which makes the extension claims harder to evaluate.

major comments (4)
  1. [Section V-E / Abstract] The central claim that X-MeshGraphNet "maintains the predictive accuracy of full-graph GNNs" is not directly tested, because no full-graph training baseline is reported. Section V-E reports R2=0.942 and Table I relative errors for X-MeshGraphNet alone; these numbers measure the model's absolute accuracy on the DrivAerML test set but not its equivalence to full-graph training. To support the headline claim, the paper should include a full-graph baseline trained on the same point-cloud graph, and a mesh-based MeshGraphNet baseline trained on the original .vtp surface, and show that the partitioned model matches both. This is load-bearing because the abstract and the conclusion in Section VII both assert accuracy maintenance as a key result.
  2. [Section V-C / Section VII] The custom graph construction connects each surface point to its six nearest Euclidean neighbors (Section V-C), which can create edges across thin panels, gaps, or concave regions, thereby mixing physically unconnected surface areas. The paper itself acknowledges in Section VII that fixed k-NN graphs may introduce "topological biases" and leaves their mitigation to future work, yet the central claim of replacing mesh-based training depends on the k-NN graph being a physically faithful discretization. A concrete test would be to compare accuracy against a mesh-based MeshGraphNet trained on the original CFD surface mesh, or to use surface-respecting connectivity derived from the STL triangulation. Without such a comparison, the accuracy results are conditional on an unvalidated graph-construction assumption.
  3. [Section III-C / Section V-C / Figure 8] The multi-scale extension is under-specified, and the scaling results contain an inconsistency. Section III-C describes building hierarchical point clouds but does not state how the message-passing layers operate on inter-scale edges, nor how halo partitioning and gradient aggregation are applied across scales. The equivalence argument in Section III-A is formulated for a single graph, and the paper does not show that it extends to the multi-scale setting. Additionally, Section V-C states that the 3-level graph contains 500k, 1M, and 2M points at successive levels, while the Figure 8 caption refers to a "3-level graph of 700,000 nodes"; these numbers need to be reconciled. The multi-scale claim requires a precise architectural description and, ideally, a partitioning-aware explanation of how nodes at different scales exchange messages.
  4. [Section V-F] The strong-scaling comparison against distributed MeshGraphNet is not fully controlled. The baseline is taken from the NVIDIA Modulus repository (reference [17]), but the paper does not report the version, the same-model check, hyperparameter settings, or communication-volume measurements. Since the baseline is from the same institution and no independent implementation is described, the comparison should state whether both methods use identical model architecture, number of message-passing layers, hidden dimension, and batching, and should report per-GPU runtime breakdowns. The memory-scaling results for X-MeshGraphNet alone in Section V-F2 are still informative, but the claimed superiority over distributed message passing is weakened without these details.
minor comments (5)
  1. [Section V-A] The sentence "One can choose to exclude the 3D positions from the input data, and that will likely promote of the model" is grammatically incomplete; presumably "promote generalization" or "improve the model" was intended.
  2. [Section VI] The sentence "The final MSE loss on the test set is 0.00125.The model effectively captures..." has a missing space after the period, and no repeated-seed statistics or confidence intervals are reported for the volume model.
  3. [Section VI] For X-UNet3D, the paper states a halo size of 40 but does not report the receptive-field verification it recommends in the same section; please provide the measured minimum halo size or an equivalence check on a representative volume to support the claim of mathematical equivalence.
  4. [Section V-B / Figure 5] The test-set definition ("10% of the samples, with 20% of the test set out-of-distribution based on drag coefficients") should specify whether the split is fixed and how the OOD samples are selected; otherwise the reported R2=0.942 is not reproducible.
  5. [Figures 3 and 4] Pressure and wall shear stress fields are compared only visually for a single sample; adding quantitative error maps or per-quantity metrics (e.g., normalized L2 error over the surface) would strengthen the accuracy assessment.

Circularity Check

0 steps flagged · score 0.0 of 10

No circularity found: the halo-partitioning equivalence is a construction-level guarantee, and accuracy and scaling are evaluated on external benchmark data; the untested full-graph accuracy claim is an evidence gap, not a circular step.

full rationale

No circular step is present. The central claim — that partitioned training with halo regions is equivalent to full-graph training — is not inferred from any fitted data; it is guaranteed by construction in Section III-A: the halo size (15, equal to the 15 message-passing layers) preserves every interior node's complete L-hop computational graph, computations are required to stay local (batch normalization is explicitly excluded), halo nodes are filtered out before the loss, and per-partition gradients are summed before the update. Halo exchange and gradient aggregation are standard sufficient conditions under which the message-passing equations (1)–(4) hold identically on partitioned and full graphs, so the equivalence is a design theorem rather than a self-definitional derivation. The accuracy figures (R2 = 0.942; Table I) are evaluated on held-out cars from the external DrivAerML benchmark, including out-of-distribution drag extremes, against independently computed HRLES data, and no parameter fitted on the test set is renamed as a prediction. The scaling comparison (Figure 8) does cite the authors' own NVIDIA Modulus framework [17] for the Distributed MeshGraphNet baseline, but the evidence is measured per-sample runtimes plus a mechanistic argument (all-to-all communication vs DDP with halos) that does not reduce to the citation; per the review rules, a code-reproduced baseline is real evidence and does not raise the circularity score. The genuine weakness — the abstract's claim that X-MeshGraphNet 'maintains the predictive accuracy of full-graph GNNs' is never tested against an actual full-graph or mesh-based MeshGraphNet accuracy run, and the 6-NN Euclidean graph may bridge physically unconnected surface regions across thin or curved features — is an empirical-validity gap, not a circular reduction; the paper itself discloses the k-NN topological-bias concern as future work in Section VII.

Assumptions & free parameters 6 free parameters · 4 assumptions · 0 invented entities

The central claims rest on hand-set graph construction hyperparameters (k, point cloud sizes, halo size, layer count, hidden size, partition count) and on the domain assumption that a k-NN point cloud graph on the object surface preserves the physical connectivity needed for accurate aerodynamic prediction. No new physical entities are introduced.

free parameters (6)
  • k (number of nearest neighbors) = 6
    Hand-chosen connectivity for graph construction; ablation (Section V-G) shows k=6 vs k=12 changes validation loss, so the value materially affects results.
  • Point cloud sizes per scale level = 500k, 1M, 2M points for levels 1, 2, 3
    Chosen resolutions for the 3-level multi-scale graph (Section V-C); directly sets the problem size and multi-scale behavior.
  • Halo size = 15
    Set equal to the number of message-passing layers (15) to guarantee equivalence with full-graph training (Section III-A).
  • Number of message-passing layers = 15
    Architecture hyperparameter that defines the receptive field and required halo size; choice affects accuracy and compute.
  • Hidden dimension = 512
    Chosen after ablation between 256 and 512 (Section V-G); affects model capacity and memory.
  • Number of partitions = 21
    Selected for training distribution on available GPUs (Section V-C); affects load balancing and halo overhead.
assumptions (4)
  • domain assumption A k-NN graph on a uniform surface point cloud is a sufficient discretization for learning surface pressure and wall shear stress.
    The model's accuracy depends on the graph connectivity reflecting physical interactions; this is asserted in Sections III-B and V-C without validation against mesh-based graphs.
  • domain assumption Interpolating CFD ground truth from VTK meshes to point clouds via 5-NN inverse distance weighting introduces no significant error.
    Section V-C specifies the interpolation procedure but provides no error analysis or sensitivity study.
  • ad hoc to paper Local message passing with no global batch statistics is sufficient for the target task; batch normalization is excluded.
    Section III-A states this condition for equivalence; it restricts the architecture to avoid operations that depend on global statistics, which may limit performance or complicate training.
  • domain assumption The DrivAerML dataset provides accurate ground truth for training and evaluation.
    The model is trained and evaluated against this dataset without independent validation of the CFD data; standard for surrogate modeling but still an assumption.

how reviews work

0 comments
Cite this review

Pith. "Pith review of X-MeshGraphNet: Scalable Multi-Scale Graph Neural Networks for Physics Simulation." pith.science (2026). https://pith.science/paper/7Z3YWQPE

@misc{pith2026241117164,
  author       = {Pith},
  title        = {Pith review of: X-MeshGraphNet: Scalable Multi-Scale Graph Neural Networks for Physics Simulation},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/7Z3YWQPE}},
  note         = {Machine review of arXiv:2411.17164}
}
read the original abstract

Graph Neural Networks (GNNs) have gained significant traction for simulating complex physical systems, with models like MeshGraphNet demonstrating strong performance on unstructured simulation meshes. However, these models face several limitations, including scalability issues, requirement for meshing at inference, and challenges in handling long-range interactions. In this work, we introduce X-MeshGraphNet, a scalable, multi-scale extension of MeshGraphNet designed to address these challenges. X-MeshGraphNet overcomes the scalability bottleneck by partitioning large graphs and incorporating halo regions that enable seamless message passing across partitions. This, combined with gradient aggregation, ensures that training across partitions is equivalent to processing the entire graph at once. To remove the dependency on simulation meshes, X-MeshGraphNet constructs custom graphs directly from tessellated geometry files (e.g., STLs) by generating point clouds on the surface or volume of the object and connecting k-nearest neighbors. Additionally, our model builds multi-scale graphs by iteratively combining coarse and fine-resolution point clouds, where each level refines the previous, allowing for efficient long-range interactions. Our experiments demonstrate that X-MeshGraphNet maintains the predictive accuracy of full-graph GNNs while significantly improving scalability and flexibility. This approach eliminates the need for time-consuming mesh generation at inference, offering a practical solution for real-time simulation across a wide range of applications. The code for reproducing the results presented in this paper is available through NVIDIA Modulus.

Figures

Figures reproduced from arXiv: 2411.17164 by the authors.

Figure 1
Figure 1. Illustration of the partitioning scheme with Halo on [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. An illustration of the geometry variation in samples [PITH_FULL_IMAGE:figures/full_fig_p006_2.png] view at source ↗
Figure 3
Figure 3. Comparison between the predictions and the ground truth for pressure for Sample 320. [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figures from the paper (7 more)
Figure 4
Figure 4. Figure 4: Comparison between the predictions and the ground truth for wall shear stress for Sample 320. [PITH_FULL_IMAGE:figures/full_fig_p007_4.png]
Figure 5
Figure 5. Figure 5: Comparison between the predicted and ground truth [PITH_FULL_IMAGE:figures/full_fig_p008_5.png]
Figure 6
Figure 6. Figure 6: Memory and performance trade-offs between activation [PITH_FULL_IMAGE:figures/full_fig_p008_6.png]
Figure 7
Figure 7. Figure 7: Memory scaling of X-MeshGraphNet on a single [PITH_FULL_IMAGE:figures/full_fig_p008_7.png]
Figure 9
Figure 9. Figure 9: Validation loss for different configurations considered in the limited ablation study. Configurations resulting in lower [PITH_FULL_IMAGE:figures/full_fig_p009_9.png]
Figure 10
Figure 10. Figure 10: Comparison between the predicted and ground truth pressure for Sample 200. [PITH_FULL_IMAGE:figures/full_fig_p010_10.png]
Figure 11
Figure 11. Figure 11: Comparison between the predicted and ground truth velocity magnitude for Sample 200. [PITH_FULL_IMAGE:figures/full_fig_p010_11.png]

Discussion (0). Continue with ORCID to comment.

Forward citations

Cited by 7 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. CoFINN: Conservation Flux Informed Neural Networks for Physics Problems Governed by Conservation Laws

    cs.CV 2026-07 conditional novelty 6.0 of 10

    Embedding finite-volume HLLC flux conservation into CNN training cuts airfoil drag prediction error substantially versus pure pixel MAE, especially in low-data regimes.

  2. Point-wise Diffusion Models for Physical Systems with Shape Variations: Application to Spatio-temporal and Large-scale system

    physics.comp-ph 2025-08 unverdicted novelty 6.0 of 10

    A point-wise diffusion transformer predicts spatio-temporal physical fields on arbitrary meshes and point clouds, claiming up to 200x faster inference and better accuracy than image-based diffusion surrogates.

  3. A Benchmarking Framework for AI models in Automotive Aerodynamics

    cs.LG 2025-07 conditional novelty 6.0 of 10

    A new benchmarking framework standardizes evaluation of AI automotive aerodynamics models, demonstrated on three models with the DrivAerML dataset.

  4. A Mixture of Experts Gating Network for Enhanced Surrogate Modeling in External Aerodynamics

    cs.LG 2025-08 conditional novelty 5.0 of 10

    A mixture-of-experts gating network that fuses predictions from DoMINO, X-MeshGraphNet, and FigConvNet reduces L-2 prediction error for automotive surface pressure and wall shear stress below each individual expert on...

  5. Inferring processes within dynamic forest models using hybrid modeling

    q-bio.QM 2025-08 unverdicted novelty 5.0 of 10

    The abstract claims a hybrid gap-model plus neural-network approach, FINN, improves forest growth inference and forecasting, but the manuscript body is an unrelated diffusion-model paper, so the abstract's claims are ...

  6. DoMINO: A Decomposable Multi-scale Iterative Neural Operator for Modeling Large Scale Engineering Simulations

    cs.LG 2025-01 conditional novelty 5.0 of 10

    DoMINO is a point-cloud-based neural operator that predicts aerodynamic surface and volume fields on large automotive meshes with moderate accuracy and holds up on out-of-distribution car designs.

  7. GeoTransolver: Learning Physics on Irregular Domains Using Multi-scale Geometry Aware Physics Attention Transformer

    cs.LG 2025-12 conditional novelty 4.0 of 10

    GeoTransolver, a geometry-aware attention transformer, improves surrogate CFD accuracy over existing baselines on three automotive/aerospace datasets, but the paper has major reporting gaps.

Reference graph

Works this paper leans on

18 extracted references · 7 canonical work pages · cited by 7 Pith papers

  1. [17]

    NVIDIA Modulus: An open-source framework for physics-based deep learning in science and engineering,

    Modulus Contributors, “NVIDIA Modulus: An open-source framework for physics-based deep learning in science and engineering,” 2023. [Online]. Available: https://github.com/NVIDIA/modulus

  2. [1]

    Relational inductive biases, deep learning, and graph networks,

    P. W. Battaglia, J. B. Hamrick, V . Bapst, A. Sanchez-Gonzalez, V . Zam- baldi, M. Malinowski, A. Tacchetti, D. Raposo, A. Santoro, R. Faulkner, et al., “Relational inductive biases, deep learning, and graph networks,” arXiv preprint arXiv:1806.01261 , 2018

  3. [2]

    Gated graph sequence neural networks,

    Y . Li, D. Tarlow, M. Brockschmidt, and R. Zemel, “Gated graph sequence neural networks,” arXiv preprint arXiv:1511.05493 , 2015

  4. [3]

    Learning mesh-based simulation with graph networks,

    T. Pfaff, M. Fortunato, A. Sanchez-Gonzalez, and P. W. Battaglia, “Learning mesh-based simulation with graph networks,” arXiv preprint arXiv:2010.03409, 2020

  5. [4]

    Learning to simulate complex physics with graph networks,

    A. Sanchez-Gonzalez, J. Godwin, T. Pfaff, R. Ying, J. Leskovec, and P. Battaglia, “Learning to simulate complex physics with graph networks,” in International conference on machine learning , pp. 8459– 8468, PMLR, 2020

  6. [5]

    Graphcast: Learning skillful medium-range global weather forecasting,

    R. Lam, A. Sanchez-Gonzalez, M. Willson, P. Wirnsberger, M. For- tunato, F. Alet, S. Ravuri, T. Ewalds, Z. Eaton-Rosen, W. Hu, et al. , “Graphcast: Learning skillful medium-range global weather forecasting,” arXiv preprint arXiv:2212.12794 , 2022

  7. [6]

    Learning reduced-order models for cardiovascular simulations with graph neural networks,

    L. Pegolotti, M. R. Pfaller, N. L. Rubio, K. Ding, R. B. Brufau, E. Darve, and A. L. Marsden, “Learning reduced-order models for cardiovascular simulations with graph neural networks,” Computers in Biology and Medicine, vol. 168, p. 107676, 2024

  8. [7]

    Multiscale meshgraphnets,

    M. Fortunato, T. Pfaff, P. Wirnsberger, A. Pritzel, and P. Battaglia, “Multiscale meshgraphnets,” arXiv preprint arXiv:2210.00612 , 2022

Show all 18 references
  1. [8]

    Deep learning for real-time aerodynamic evaluations of arbitrary vehicle shapes,

    S. J. Jacob, M. Mrosek, C. Othmer, and H. K ¨ostler, “Deep learning for real-time aerodynamic evaluations of arbitrary vehicle shapes,” arXiv preprint arXiv:2108.05798, 2021

  2. [9]

    U-net: Convolutional networks for biomedical image segmentation,

    O. Ronneberger, P. Fischer, and T. Brox, “U-net: Convolutional networks for biomedical image segmentation,” in Medical image computing and computer-assisted intervention–MICCAI 2015: 18th international con- ference, Munich, Germany, October 5-9, 2015, proceedings, part III 18 ...

  3. [10]

    3d flow field estimation around a vehicle using convolutional neural networks.,

    F. Chen and K. Akasaka, “3d flow field estimation around a vehicle using convolutional neural networks.,” in BMVC, p. 396, 2021

  4. [11]

    Drivaernet: A parametric car dataset for data-driven aerodynamic design and graph-based drag pre- diction,

    M. Elrefaie, F. Ahmed, and A. Dai, “Drivaernet: A parametric car dataset for data-driven aerodynamic design and graph-based drag pre- diction,” in International Design Engineering Technical Conferences and Computers and Information in Engineering Conference , vol. 88360, p. V0...

  5. [12]

    Pointnet: Deep learning on point sets for 3d classification and segmentation,

    C. R. Qi, H. Su, K. Mo, and L. J. Guibas, “Pointnet: Deep learning on point sets for 3d classification and segmentation,” in Proceedings of the IEEE conference on computer vision and pattern recognition , pp. 652– 660, 2017

  6. [13]

    Sur- rogate modeling of car drag coefficient with depth and normal ren- derings,

    B. Song, C. Yuan, F. Permenter, N. Arechiga, and F. Ahmed, “Sur- rogate modeling of car drag coefficient with depth and normal ren- derings,” in International Design Engineering Technical Conferences and Computers and Information in Engineering Conference , vol. 87301, p. V03A...

  7. [14]

    3d super-resolution model for vehicle flow field enrichment,

    T. L. Trinh, F. Chen, T. Nanri, and K. Akasaka, “3d super-resolution model for vehicle flow field enrichment,” in Proceedings of the IEEE/CVF Winter Conference on Applications of Computer Vision , pp. 5826–5835, 2024

  8. [15]

    Drivaerml: High-fidelity computational fluid dynamics dataset for road- car external aerodynamics,

    N. Ashton, C. Mockett, M. Fuchs, L. Fliessbach, H. Hetmann, T. Knacke, N. Schonwald, V . Skaperdas, G. Fotiadis, A. Walle, et al. , “Drivaerml: High-fidelity computational fluid dynamics dataset for road- car external aerodynamics,” arXiv preprint arXiv:2408.11969 , 2024

  9. [16]

    A fast and high quality multilevel scheme for partitioning irregular graphs,

    G. Karypis and V . Kumar, “A fast and high quality multilevel scheme for partitioning irregular graphs,” SIAM Journal on scientific Computing, vol. 20, no. 1, pp. 359–392, 1998

  10. [18]

    Fourier features let networks learn high frequency functions in low dimensional domains,

    M. Tancik, P. Srinivasan, B. Mildenhall, S. Fridovich-Keil, N. Raghavan, U. Singhal, R. Ramamoorthi, J. Barron, and R. Ng, “Fourier features let networks learn high frequency functions in low dimensional domains,” Advances in neural information processing systems , vol. 33, pp...

Pith tools

Reviewed August 12, 2026 · model on record in the stance chip above.