Scheme III (piecewise linear) and V (piecewise parabolic) of Van Leer are shown to yield identical solutions provided the initial conditions are chosen in an appropriate manner. This result is counter intuitive since it is generally believed that piecewise linear and piecewise parabolic methods cannot produce the same solutions due to their different degrees of approximation. The result also shows a key connection between the approaches of discontinuous and continuous representations
First and second order explicit difference schemes are derived for a three dimensional hyperbolic sy...
A general strategy exists for constructing Energy Stable Weighted Essentially Non Oscillatory (ESWEN...
While enjoying demonstrated improvement in accuracy, efficiency, and robustness over existing scheme...
In the fourth installment of the celebrated series of five papers entitled "Towards the ultimate con...
The relative computational effort among the spatially five point numerical flux functions of Harten,...
The effect of reducing the formal order of accuracy of a finite-difference scheme in order to optimi...
The upwind leapfrog method for the advection equation, which is non-dissipative and very accurate, i...
For advection schemes based on fluctuation splitting, a design criterion of optimizing the time step...
breed of upwind schemes have been produced since the beginning of the 90s. To be practically useful,...
A new, nonoscillatory upwind scheme is developed for the multidimensional convection equation. The s...
A time-dependent extension of the first-order hyperbolic system method for advection-diffusion probl...
Popular high-order schemes with compact stencils for Computational Fluid Dynamics (CFD) include Disc...
A time-accurate, upwind, finite volume method for computing compressible flows on unstructured grids...
The diffusive characteristics of two upwind schemes, multi-dimensional fluctuation splitting and loc...
This paper focuses on the evolution of advection upstream splitting method (AUSM) schemes. The main ...
First and second order explicit difference schemes are derived for a three dimensional hyperbolic sy...
A general strategy exists for constructing Energy Stable Weighted Essentially Non Oscillatory (ESWEN...
While enjoying demonstrated improvement in accuracy, efficiency, and robustness over existing scheme...
In the fourth installment of the celebrated series of five papers entitled "Towards the ultimate con...
The relative computational effort among the spatially five point numerical flux functions of Harten,...
The effect of reducing the formal order of accuracy of a finite-difference scheme in order to optimi...
The upwind leapfrog method for the advection equation, which is non-dissipative and very accurate, i...
For advection schemes based on fluctuation splitting, a design criterion of optimizing the time step...
breed of upwind schemes have been produced since the beginning of the 90s. To be practically useful,...
A new, nonoscillatory upwind scheme is developed for the multidimensional convection equation. The s...
A time-dependent extension of the first-order hyperbolic system method for advection-diffusion probl...
Popular high-order schemes with compact stencils for Computational Fluid Dynamics (CFD) include Disc...
A time-accurate, upwind, finite volume method for computing compressible flows on unstructured grids...
The diffusive characteristics of two upwind schemes, multi-dimensional fluctuation splitting and loc...
This paper focuses on the evolution of advection upstream splitting method (AUSM) schemes. The main ...
First and second order explicit difference schemes are derived for a three dimensional hyperbolic sy...
A general strategy exists for constructing Energy Stable Weighted Essentially Non Oscillatory (ESWEN...
While enjoying demonstrated improvement in accuracy, efficiency, and robustness over existing scheme...