A meshfree exterior calculus for generalizable and data-efficient learning of physics from point clouds
Learn how to apply meshfree exterior calculus to point clouds for data-efficient physics learning, enabling generalizable and transferable models across different resolutions and geometries
- Build a meshfree exterior calculus framework using sparse Schur complement solves to equip ε-ball graphs with virtual node and edge measures
- Apply the MEEC framework to point clouds to learn structure-preserving descriptions of physics
- Configure MEEC-Net, a data-efficient surrogate model, to transfer across resolutions, geometries, and physical parameters
- Test the generalizability of MEEC-Net on various physics problems and datasets
- Compare the performance of MEEC-Net with other state-of-the-art methods for learning physics from point clouds
Researchers and engineers working on physics-informed neural networks, computational physics, and geometric deep learning can benefit from this approach to improve model generalizability and data efficiency
💡 Meshfree exterior calculus enables the creation of data-efficient and generalizable models for learning physics from point clouds, allowing for transferability across different resolutions, geometries, and physical parameters
🌐 Introducing meshfree exterior calculus for data-efficient learning of physics from point clouds! 🚀 Generalizable and transferable models across resolutions and geometries 📈
Key Takeaways
Learn how to apply meshfree exterior calculus to point clouds for data-efficient physics learning, enabling generalizable and transferable models across different resolutions and geometries
Full Article
Abstract:
arXiv:2605.08436v1 Announce Type: cross Abstract: We introduce a meshfree exterior calculus (MEEC) for learning structure-preserving descriptions of physics on point clouds, and use it to build MEEC-Net, a data-efficient surrogate that transfers across resolutions, geometries, and physical parameters. MEEC equips an $\varepsilon$-ball graph with virtual node and edge measures via a single sparse Schur complement solve; the resulting complex satisfies discrete conservation exactly, is end-to-end
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