DiffusionReactionProblem#
Formulation of the diffusion-reaction problem.
- class DiffusionReactionProblem(alpha=0.0001)[source]#
Bases:
TimeDependentProblem,SpatialProblemImplementation of the one-dimensional diffusion-reaction problem on the space-time domain \(\Omega\times T = [-\pi, \pi] \times [0, 1]\).
The problem is governed by the forced diffusion-reaction equation
\[\frac{\partial u}{\partial t} - \alpha \frac{\partial^2 u}{\partial x^2} = f(x, t),\]where \(u = u(x, t)\) is the solution field, \(\alpha\) is the diffusion coefficient, and \(f(x, t)\) is a forcing term.
Homogeneous Dirichlet boundary conditions are imposed at the spatial boundaries:
\[u(-\pi, t) = u(\pi, t) = 0, \qquad t \in [0, 1].\]The initial condition is prescribed as
\[u(x, 0) = \sin(x) + \frac{1}{2}\sin(2x) + \frac{1}{3}\sin(3x) + \frac{1}{4}\sin(4x) + \frac{1}{8}\sin(8x).\]The analytical solution is given by
\[u(x, t) = e^{-t} \left( \sin(x) + \frac{1}{2}\sin(2x) + \frac{1}{3}\sin(3x) + \frac{1}{4}\sin(4x) + \frac{1}{8}\sin(8x) \right).\]See also
Original reference: Si, Chenhao, et al. Complex Physics-Informed Neural Network. arXiv preprint arXiv:2502.04917 (2025). DOI: arXiv:2502.04917.
- Example:
>>> problem = DiffusionReactionProblem()
Initialization of the
DiffusionReactionProblem.- solution(pts)[source]#
Implementation of the analytical solution of the diffusion-reaction problem.
- Parameters:
pts (LabelTensor) – Points where the solution is evaluated.
- Returns:
The analytical solution of the diffusion-reaction problem.
- Return type: