LGCLNAJun 26, 2021

PhyCRNet: Physics-informed Convolutional-Recurrent Network for Solving Spatiotemporal PDEs

arXiv:2106.14103v1281 citations
Originality Highly original
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This work addresses the problem of efficiently solving high-dimensional spatiotemporal PDEs for researchers in computational science and engineering, offering a novel method that improves upon existing PINN approaches.

The authors tackled the limitations of physics-informed neural networks (PINNs) in solving spatiotemporal PDEs by proposing PhyCRNet, a physics-informed convolutional-recurrent network that hard-encodes initial/boundary conditions and uses an encoder-decoder architecture for feature extraction, achieving superior accuracy, extrapolability, and generalizability compared to state-of-the-art baselines on nonlinear PDEs like 2D Burgers' equations.

Partial differential equations (PDEs) play a fundamental role in modeling and simulating problems across a wide range of disciplines. Recent advances in deep learning have shown the great potential of physics-informed neural networks (PINNs) to solve PDEs as a basis for data-driven modeling and inverse analysis. However, the majority of existing PINN methods, based on fully-connected NNs, pose intrinsic limitations to low-dimensional spatiotemporal parameterizations. Moreover, since the initial/boundary conditions (I/BCs) are softly imposed via penalty, the solution quality heavily relies on hyperparameter tuning. To this end, we propose the novel physics-informed convolutional-recurrent learning architectures (PhyCRNet and PhyCRNet-s) for solving PDEs without any labeled data. Specifically, an encoder-decoder convolutional long short-term memory network is proposed for low-dimensional spatial feature extraction and temporal evolution learning. The loss function is defined as the aggregated discretized PDE residuals, while the I/BCs are hard-encoded in the network to ensure forcible satisfaction (e.g., periodic boundary padding). The networks are further enhanced by autoregressive and residual connections that explicitly simulate time marching. The performance of our proposed methods has been assessed by solving three nonlinear PDEs (e.g., 2D Burgers' equations, the $λ$-$ω$ and FitzHugh Nagumo reaction-diffusion equations), and compared against the start-of-the-art baseline algorithms. The numerical results demonstrate the superiority of our proposed methodology in the context of solution accuracy, extrapolability and generalizability.

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