| enabling a wavelet-Galerkin turbulent flow field representation with expansion coefficients in identical physical & wavelet space
“When Fourier meets Navier” in a physical H(1/2) energy Hilbert space there is a global unique H(1/2) solution of the corresponding weak variation equation of the non-linear, non-stationary Navier-Stokes equations ("solution"). The standard numerical approximation method for PDE is the Ritz-Galerkin method which is usually equipped with finite element approximation spaces (FEM). In case of negative scaled Hilbert spaces the Ritz-Galerkin method accompanied by finte element approximation spaces becomes a boundary element method (BEM) related to the underlying singular equation representation. The required finite (boundary) element approximation properties of the BEM face some challenges in case of non-linearity and/or non-periodic boundary conditions. The wavelet extension method is used to represent functions that have discontinuities and sharp peaks, and for accurately deconstructing and reconstructing finite, non-periodic and/or non-stationary signals, (MeM). Here we go with a collection of some useful supporting tool sets:
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