用主拉伸构建物理约束的神经材料模型,提升软材料力学预测精度。
Polyconvex Physics-Augmented Neural Network Constitutive Models in Principal Stretches
- 基于主拉伸构造满足多凸性的能量函数,融合深度网络与物理规律。
- 在合成与实验数据上实现对多种软材料行为的准确拟合。
- 适合需要高精度力学建模的材料设计与仿真研究者。
精确的软材料本构模型对理解其力学行为及保障设计预测可靠性至关重要。近年来科学机器学习提出灵活通用的材料模型架构,可捕捉多种材料行为,减少对专家构建解析模型的依赖。研究重点逐渐转向在神经网络架构中嵌入物理约束,以规范过参数化模型。现有主流方法如输入凸神经网络(ICNN)和神经常微分方程(NODE)均基于柯西-格林张量的不变量,未使用主拉伸。本文构建基于主拉伸的通用多凸函数,在物理感知的深度学习框架中提供与不变量方法的对比分析。该框架基于最新理论:多凸函数可表征为右拉伸张量 $\mathbf{U}$、其余子张量 $\text{cof}\mathbf{U}$ 及其行列式 $J$ 的凸函数。任意对称二阶张量的凸函数可由其特征值的凸对称函数描述。因此,先通过深度霍尔德集结合 ICNN 描述 $\mathbf{U}$ 与 $\text{cof}\mathbf{U}$ 的特征值上的凸函数;再由第三个 ICNN 输入 $J$ 及前述两个凸函数,输出总应变能。模型在合成与实验数据上验证了对任意材料行为的拟合能力。
原文摘要 · Abstract (English)
Accurate constitutive models of soft materials are crucial for understanding their mechanical behavior and ensuring reliable predictions in the design process. To this end, scientific machine learning research has produced flexible and general material model architectures that can capture the behavior of a wide range of materials, reducing the need for expert-constructed closed-form models. The focus has gradually shifted towards embedding physical constraints in the network architecture to regularize these over-parameterized models. Two popular approaches are input convex neural networks (ICNN) and neural ordinary differential equations (NODE). A related alternative has been the generalization of closed-form models, such as sparse regression from a large library. Remarkably, all prior work using ICNN or NODE uses the invariants of the Cauchy-Green tensor and none uses the principal stretches. In this work, we construct general polyconvex functions of the principal stretches in a physics-aware deep-learning framework and offer insights and comparisons to invariant-based formulations. The framework is based on recent developments to characterize polyconvex functions in terms of convex functions of the right stretch tensor $\mathbf{U}$, its cofactor $\text{cof}\mathbf{U}$, and its determinant $J$. Any convex function of a symmetric second-order tensor can be described with a convex and symmetric function of its eigenvalues. Thus, we first describe convex functions of $\mathbf{U}$ and $\text{cof}\mathbf{U}$ in terms of their respective eigenvalues using deep Holder sets composed with ICNN functions. A third ICNN takes as input $J$ and the two convex functions of $\mathbf{U}$ and $\text{cof}\mathbf{U}$, and returns the strain energy as output. The ability of the model to capture arbitrary materials is demonstrated using synthetic and experimental data.
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