This work presents a physics-informed, data-free neural solver for partial differential equations, built on a graph neural network architecture that utilises message passing, and uses gradients of finite-element shape functions rather than automatic differentiation operators to compute the residuals of the equation from the displacements predicted by the network itself.
Abstract
We present a physics-informed, data-free neural solver for partial differential equations, built on a graph neural network architecture that utilises message passing. By relying on the weak form of the problem, we use gradients of finite-element shape functions (which are therefore polynomials) rather than automatic differentiation operators to compute the residuals of the equation from the displacements predicted by the network itself. Our approach generalises to previously unseen load cases and geometries, achieving easily convergence errors in the residuals of less than 1% and being capable of scaling up to models of considerable size and arbitrary geometries. To ensure compliance with the laws of physics and provide guarantees regarding the inference, it is possible to use the residual itself as an error indicator for the inference, and thus perform a refinement at the testing stage if the residual tolerance set in advance by the user is not met. Examples are provided to demonstrate the performance of the proposed method. This results in a method that avoids the costly process of obtaining, curating and storing high-fidelity synthetic data for training the neural network. Whilst this is not unique to our method, it is the first time it has been combined with a geometric machine learning technique capable of providing the necessary geometric bias to overcome the well-known difficulties of physics-informed neural networks.
A mesh-free numerical framework based on \textit{Kolmogorov--Arnold Physics-Informed Neural Networks} (KAN-PINNs) is developed for the approximation of fourth-order elliptic boundary value problems, with specific application to the biharmonic equation governing thin plate deflection. Unlike conventional Multi-Layer Per...
Neural operators are typically trained in a supervised fashion, which requires a dataset to be generated with a classical solver. Training them physics-informed, i.e., purely from the governing equations, removes this large offline cost and allows fresh samples to be drawn at every optimization step, but has so far bee...
Shi-Zheng Wen, Siddhartha Mishra, Marius Zeinhofer· 0 citations
Neural operators have become a popular approach to approximate the solution operators of parametric partial differential equations (PDEs). However, existing neural operators either require a large amount of simulation data or a long physics-informed training on GPUs, and they cannot tell how accurate an individual pred...
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This work presents a hybrid numerical approach for solving linear systems arising from the discretization of the two‐dimensional parametric Helmholtz equation. A convolutional neural network based on the U‐Net architecture is trained in a self‐supervised manner (i.e., without explicitly generating reference solutions...
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This paper presents a comparative study of classical numerical and machine learning techniques for solving the nonlinear Monge–Ampère Equation (MAE). A finite difference method (FDM) implemented in MATLAB is first validated using a quadratic exact solution on a square domain. Two neural network approaches are then inve...
C. Ogbonna, Maliki Olaniyi S, Nkem Ogbonna· International journal of re...· 0 citations
This work systematically revisit the Deep Energy Method, placing it in the broader context of physics-informed learning and variational modeling, and identifies the class of problems for which energy minimization provides intrinsic advantages in terms of stability, robustness and interpretability.
T. Rabczuk, Yi-Zheng Wang· 0 citations
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