Abstract:We propose a simple modification of standard WENO finite volume methods for Cartesian grids, which retains the full spatial order of accuracy of the one-dimensional discretization when applied to nonlinear multidimensional systems of conservation laws.We derive formulas, which allow us to compute high-order accurate point values of the conserved quantities at grid cell interfaces. Using those point values, we can compute a highorder flux at the center of a grid cell interface. Finally, we use those point value… Show more
a b s t r a c tWe present a WENO finite volume method for the approximation of hyperbolic conservation laws on adaptively refined Cartesian grids.On each single patch of the AMR grid, we use a modified dimension-by-dimension WENO method, which was recently developed by Buchmüller and Helzel (2014) [1]. This method retains the full spatial order of accuracy of the underlying one-dimensional WENO reconstruction for nonlinear multidimensional problems, and requires only one flux computation per interface.
a b s t r a c tWe present a WENO finite volume method for the approximation of hyperbolic conservation laws on adaptively refined Cartesian grids.On each single patch of the AMR grid, we use a modified dimension-by-dimension WENO method, which was recently developed by Buchmüller and Helzel (2014) [1]. This method retains the full spatial order of accuracy of the underlying one-dimensional WENO reconstruction for nonlinear multidimensional problems, and requires only one flux computation per interface.
“…To achieve an accuracy higher than second order one must use higher order accurate averaged fluxes because point value fluxes would only be second-order approximations and, thus, degrade the accuracy to the second order [4,35].…”
Section: Dimension By Dimension Cweno Reconstructionmentioning
confidence: 99%
“…(16) we just need to obtain point values at the face centers. This averaging procedure has previously been used to obtain higher order averaged flux in the multidimensional PPM (piecewise parabolic method) [35] and WENO schemes [4]. Whereas, we are applying it in the framework of a central scheme which naturally allows the computation of non-oscillatory point values (U + i+1/2,j,k , U − i−1/2,j,k ) at the face-center.…”
Section: B Fourth Order Accurate Averaged Fluxesmentioning
confidence: 99%
“…This method of computing higher-order point value at the face-center has previously been used in the framework of the third order CWENO scheme of Kurganov and Levy [21], fourth order PPM scheme [35] and fourth order WENO scheme [4]. We are applying this method to develop a fourth-order accurate CWENO scheme.…”
Section: B Fourth Order Accurate Averaged Fluxesmentioning
confidence: 99%
“…These initial conditions result in the advection of the initial density profile due to constant velocity components and constant pressure (see for example [4] Example 2. Initial conditions for the 2D Euler vortex evolution problem (see for example [13]) are,…”
Section: A the Euler Equations Of Gas Dynamicsmentioning
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