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Dataset Description

Overview

This dataset contains solutions to the two-dimensional wave equation within a circular domain. The wave equation is a fundamental linear hyperbolic partial differential equation (PDE) given by:

2u2t=c2Δu,in D×[0,T], \frac{\partial^2 u}{\partial^2 t} = c^2 \Delta u, \quad \text{in } \mathcal{D} \times [0, T],

with initial conditions defined as:

u0(x,y)=πK2i,jaij(i2+j2)rsin(πix)sin(πjy). u_0(x, y) = \frac{\pi}{K^2} \sum_{i, j} a_{i j}\left(i^2+j^2\right)^{-r} \sin (\pi i x) \sin (\pi j y).

In our experiments, the parameters are set as follows:

  • $K = 10$
  • $c = 2.0$
  • $r = 0.5$
  • $a \in \mathbb{R}^{K \times K}$, with values uniformly sampled from the range $[-1, 1]$.

The solution domain is a circle centered at $[0.5, 0.5]$ with radius 1. We enforce zero Dirichlet boundary conditions across the domain.

Dataset Specifications

The dataset was generated using a finite element method (FEM) on a triangular mesh in a circular domain. The mesh is generated using the Delaunay algorithm with the following specifications:

  • Number of points (nodes): 16431
  • Mesh elements:
    • Triangles: 32441

Temporal discretization is performed with a time step $\Delta t = 0.001$, and each trajectory is simulated for 100 time steps.

Data Structure

Each dataset file contains the following arrays:

  • x: (Array of shape [16431]) The x-coordinates of the mesh points.
  • y: (Array of shape [16431]) The y-coordinates of the mesh points.
  • u0: (Array of shape [16431, batch_size]) The initial condition ( u_0 ) at each mesh point for each sampled configuration.
  • u: (Array of shape [16431, 100, batch_size]) The solution ( u ) at each mesh point for each time step and for each sampled configuration.

Applications

This dataset is suitable for applications in:

  • Machine learning for scientific computing
  • Time-dependent PDE solvers
  • Reduced-order modeling and surrogate modeling for hyperbolic equations

Additional Information

  • The dataset is generated using PyTorch-based FEM solvers (TensorMesh) and supports integration with machine learning frameworks.
  • The temporal and spatial discretization must adhere to the Courant-Friedrichs-Levy (CFL) condition for stability. For the finite element method (FEM) solution, the Crank-Nicolson time-stepping scheme is utilized to ensure energy conservation during the simulation.
  • The circular domain and multi-frequency initial conditions allow the dataset to cover a range of spatial scales and complexities in wave propagation.
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