We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservation laws. Our new method is based on a central weighted nonoscillatory approach. The heart of our method is the reconstruction step, in which a genuinely two-dimensional interpolant is reconstructed from cell averages by taking a convex combination of building blocks in the form of biquadratic polynomials. Similarly to other central schemes, our new method enjoys the simplicity of the black-box approach. All that is required in order to solve a problem is to supply the flux function and an estimate on the speed of propagation. The high-resolution properties of the scheme as well as its resistance to mesh orientation, and the effectiveness of...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a new third-order essentially non-oscillatory central scheme for approximating solutions ...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a new third-order essentially non-oscillatory central scheme for approximating solutions ...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a new third-order essentially non-oscillatory central scheme for approximating solutions ...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservat...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approx- imating ...
We present a new third-order essentially non-oscillatory central scheme for approximating solutions ...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a family of high-order, essentially non-oscillatory, central schemes for approximating ...
We present a new third-order essentially non-oscillatory central scheme for approximating solutions ...