解决固体力学中PINN的无限域与几何缺陷问题。
Finite-PINN: A Physics-Informed Neural Network with Finite Geometric Encoding for Solid Mechanics
- 引入有限几何编码,将解空间从欧氏转为混合欧氏-拓扑空间。
- 支持强弱形式联合训练,可处理正向与反向固体力学问题。
- 适合需要高精度场重建的工程结构分析场景。
PINN模型在流体偏微分方程问题上已展现能力,其在固体力学中的潜力也初现端倪。本研究识别出将PINN应用于一般固体力学问题时的两大挑战:一是PINN生成解于无限域,与多数固体结构的有限边界冲突;二是其解空间为欧氏空间,难以应对常见复杂几何形状。为此,本文提出适用于一般固体力学问题的有限几何编码物理信息神经网络(Finite-PINN)。该模型通过在神经网络输入中引入有限几何编码,将解空间由传统欧氏空间转变为混合欧氏-拓扑空间。模型采用强形式与弱形式损失联合训练,可广泛应用于固体力学的正向与反向问题。对于正向问题,当结构几何信息预处理后,能高效逼近解;对于反向问题,可在极稀疏观测下,通过嵌入物理规律与几何信息,有效重构全场解。
原文摘要 · Abstract (English)
PINN models have demonstrated capabilities in addressing fluid PDE problems, and their potential in solid mechanics is beginning to emerge. This study identifies two key challenges when using PINN to solve general solid mechanics problems. These challenges become evident when comparing the limitations of PINN with the well-established numerical methods commonly used in solid mechanics, such as the finite element method (FEM). Specifically: a) PINN models generate solutions over an infinite domain, which conflicts with the finite boundaries typical of most solid structures; and b) the solution space utilised by PINN is Euclidean, which is inadequate for addressing the complex geometries often present in solid structures. This work presents a PINN architecture for general solid mechanics problems, referred to as the Finite-PINN model. The model is designed to effectively tackle two key challenges, while retaining as much of the original PINN framework as possible. To this end, the Finite-PINN incorporates finite geometric encoding into the neural network inputs, thereby transforming the solution space from a conventional Euclidean space into a hybrid Euclidean-topological space. The model is comprehensively trained using both strong-form and weak-form loss formulations, enabling its application to a wide range of forward and inverse problems in solid mechanics. For forward problems, the Finite-PINN model efficiently approximates solutions to solid mechanics problems when the geometric information of a given structure has been preprocessed. For inverse problems, it effectively reconstructs full-field solutions from very sparse observations by embedding both physical laws and geometric information within its architecture.
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