This document, originally detailed in arXiv hal-00084616, explores the development and application of a new numerical technique for simulating intricate physical phenomena. The primary goal of this research is to overcome the limitations of traditional fixed-grid approaches by introducing dynamic mesh refinement strategies.
The proposed methodology integrates an adaptive discretization scheme that intelligently adjusts the computational grid based on local solution characteristics, such as gradients and curvatures. This ensures higher resolution in critical regions while maintaining computational efficiency elsewhere.
Key aspects of the method include:
The core partial differential equation (PDE) often encountered in such systems can be broadly represented as:
∂u / ∂t = ∇ · (K ∇u) + f(u, t)
Where:
u
represents the unknown field variable (e.g., temperature, concentration).t
is time.K
is a diffusion or conductivity tensor.f(u, t)
is a source/sink term, which can be non-linear or time-dependent.For spatial discretization, a finite element approach is employed. For instance, a basis function φi(x)
for approximating u(x)
might involve a summation:
u(x) ≈ Σi=1N Ui φi(x)
Here, Ui
are the nodal values and N
is the total number of nodes. The adaptive strategy ensures that the mesh density (and thus N
) is optimal across the domain.
The results presented in arXiv hal-00084616 demonstrate that this adaptive method significantly improves accuracy and reduces computational cost compared to uniform-grid methods, particularly for problems with sharp fronts or localized phenomena. Future research will focus on extending this framework to multi-physics problems and incorporating machine learning techniques for even more efficient adaptation.