用物理约束神经算子精准模拟高频气泡动态,兼具可解释性与高效性。
BubbleOKAN: A Physics-Informed Interpretable Neural Operator for High-Frequency Bubble Dynamics
- 基于KAN架构的两步DeepOKAN模型,融合样条与径向基函数提升高频特征表达。
- 在三种典型气泡动力学场景下,对低频与高频行为均实现高精度建模。
- 相比传统数值求解器和主流神经算子,更优的泛化能力与物理一致性适合工程仿真应用。
本文采用物理信息神经算子,将压力输入映射为对应的气泡半径响应。提出两步DeepONet架构,引入Rowdy自适应激活函数以缓解深度学习模型的固有谱偏见,增强高频特征表征能力。进一步构建基于柯尔莫哥洛夫-阿诺德网络(KAN)的两步DeepOKAN模型,在无需显式激活函数的前提下,显著提升可解释性并高效捕捉高频气泡动力学。研究对比了样条基函数与径向基函数(RBF)在构建通用近似基方面的性能,发现样条基在处理高频动态时更具优势,并揭示了RBF在学习高频信号时的性能瓶颈。模型在三类代表性场景中系统评估:(1) 单初始半径下的雷利-普莱斯特定律;(2) 单初始半径下的凯勒-米克西斯方程;(3) 多初始半径下的凯勒-米克西斯动力学。与傅里叶神经算子、小波神经算子、OFormer及卷积神经算子等先进方法对比,结果表明DeepOKAN能准确捕捉低频与高频行为,为传统数值求解器提供了有前景的替代方案。
原文摘要 · Abstract (English)
In this work, we employ physics-informed neural operators to map pressure profiles from an input function space to the corresponding bubble radius responses. Our approach employs a two-step DeepONet architecture. To address the intrinsic spectral bias of deep learning models, our model incorporates the Rowdy adaptive activation function, enhancing the representation of high-frequency features. Moreover, we introduce the Kolmogorov-Arnold network (KAN) based two-step DeepOKAN model, which enhances interpretability (often lacking in conventional multilayer perceptron architectures) while efficiently capturing high-frequency bubble dynamics without explicit utilization of activation functions in any form. We particularly investigate the use of spline basis functions in combination with radial basis functions (RBF) within our architecture, as they demonstrate superior performance in constructing a universal basis for approximating high-frequency bubble dynamics compared to alternative formulations. Furthermore, we emphasize on the performance bottleneck of RBF while learning the high frequency bubble dynamics and showcase the advantage of using spline basis function for the trunk network in overcoming this inherent spectral bias. The model is systematically evaluated across three representative scenarios: (1) bubble dynamics governed by the Rayleigh-Plesset equation with a single initial radius, (2) bubble dynamics governed by the Keller-Miksis equation with a single initial radius, and (3) Keller-Miksis dynamics with multiple initial radii. We also compare our results with state-of-the-art neural operators, including Fourier Neural Operators, Wavelet Neural Operators, OFormer, and Convolutional Neural Operators. Our findings demonstrate that the two-step DeepOKAN accurately captures both low- and high-frequency behaviors, and offers a promising alternative to conventional numerical solvers.
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