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Moving sample method for solving time-dependent partial differential equations

Beining Xu, Haijun Yu, Jiayu Zhai, Kejun Tang, Xiaoliang Wan

TL;DR

This work tackles the challenge of solving time-dependent PDEs with sharp local features using physics-informed neural networks by introducing Moving Sample Method (MSM), an adaptive sampling framework where collocation points migrate toward high-residual regions. The method combines a residual-driven sampling density with a velocity field learned from residual dynamics, linking sampling updates to transport equations and equidistribution principles. A pair of neural networks—one for the PDE solution $u_{\boldsymbol{\theta}}$ and one for the sampling potential $\boldsymbol{\phi}_{\boldsymbol{\eta}}$— jointly drive the solution and the adaptive mesh via $\boldsymbol{v}_{\boldsymbol{\eta}}=\nabla \boldsymbol{\phi}_{\boldsymbol{\eta}}$, with losses $\text{Loss}_u$ and $\text{Loss}_{\boldsymbol{v}}$ incorporating the residual $r_t$ and its time derivative $R_t$. Across Allen–Cahn, rotation, Burgers’, Fokker–Planck, and high-dimensional advection benchmarks, MSM-PINNs achieve higher accuracy with fewer sampling points than vanilla PINNs, particularly in regions exhibiting singular behavior or moving sharp features; the approach improves stability and efficiency but introduces extra training cost for the velocity field and requires careful handling of domain-boundary dynamics.

Abstract

Solving time-dependent partial differential equations (PDEs) that exhibit sharp gradients or local singularities is computationally demanding, as traditional physics-informed neural networks (PINNs) often suffer from inefficient point allocation that wastes resources on regions already well-resolved. This paper presents an adaptive sampling framework for PINNs aimed at efficiently solving time-dependent partial differential equations with pronounced local singularities. The method employs a residual-driven strategy, where the spatial-temporal distribution of training points is iteratively updated according to the error field from the previous iteration. This targeted allocation enables the network to concentrate computational effort on regions with significant residuals, achieving higher accuracy with fewer sampling points compared to uniform sampling. Numerical experiments on representative PDE benchmarks demonstrate that the proposed approach improves solution quality.

Moving sample method for solving time-dependent partial differential equations

TL;DR

This work tackles the challenge of solving time-dependent PDEs with sharp local features using physics-informed neural networks by introducing Moving Sample Method (MSM), an adaptive sampling framework where collocation points migrate toward high-residual regions. The method combines a residual-driven sampling density with a velocity field learned from residual dynamics, linking sampling updates to transport equations and equidistribution principles. A pair of neural networks—one for the PDE solution and one for the sampling potential — jointly drive the solution and the adaptive mesh via , with losses and incorporating the residual and its time derivative . Across Allen–Cahn, rotation, Burgers’, Fokker–Planck, and high-dimensional advection benchmarks, MSM-PINNs achieve higher accuracy with fewer sampling points than vanilla PINNs, particularly in regions exhibiting singular behavior or moving sharp features; the approach improves stability and efficiency but introduces extra training cost for the velocity field and requires careful handling of domain-boundary dynamics.

Abstract

Solving time-dependent partial differential equations (PDEs) that exhibit sharp gradients or local singularities is computationally demanding, as traditional physics-informed neural networks (PINNs) often suffer from inefficient point allocation that wastes resources on regions already well-resolved. This paper presents an adaptive sampling framework for PINNs aimed at efficiently solving time-dependent partial differential equations with pronounced local singularities. The method employs a residual-driven strategy, where the spatial-temporal distribution of training points is iteratively updated according to the error field from the previous iteration. This targeted allocation enables the network to concentrate computational effort on regions with significant residuals, achieving higher accuracy with fewer sampling points compared to uniform sampling. Numerical experiments on representative PDE benchmarks demonstrate that the proposed approach improves solution quality.
Paper Structure (19 sections, 2 theorems, 42 equations, 20 figures, 1 table, 1 algorithm)

This paper contains 19 sections, 2 theorems, 42 equations, 20 figures, 1 table, 1 algorithm.

Key Result

Theorem 2

\newlabeldynamics_thm2 Let $\boldsymbol{v}_t:\mathbb{R}^n\rightarrow\mathbb{R}^n$ be a bounded and twice differentiable velocity field of the flow mapping $\boldsymbol{X}_t$, that is, $\boldsymbol{X}_t(\boldsymbol{x})$ follows the ODE system Suppose the density functions $p_t$ satisfies the transport equation Then $p_t$ is the probability density of the probability flow mapping $\boldsymbol{X}_t

Figures (20)

  • Figure 5.1: MSM-PINNs result (left) and the corresponding absolute error (right) for the Allen-Cahn equation in Experiment \ref{['Allen-Cahn']}.
  • Figure 5.2: PINNs result (left) and the corresponding absolute error (right) for the Allen-Cahn equation in Experiment \ref{['Allen-Cahn']}.
  • Figure 5.3: The approximate distribution of adaptive sampling points for the Allen-Cahn equation in Experiment \ref{['Allen-Cahn']}.
  • Figure 5.4: MSM-PINNs result for the rotation equation in Experiment \ref{['rotation']}.
  • Figure 5.5: The trajectories of the adaptive sampling points for the rotation equation in Experiment \ref{['rotation']}.
  • ...and 15 more figures

Theorems & Definitions (6)

  • Remark 1
  • Theorem 2
  • Remark 3
  • Lemma 4
  • proof
  • proof