暂无分享,去创建一个
[1] P. Degond,et al. All speed scheme for the low Mach number limit of the isentropic Euler equations , 2009, 0908.1929.
[2] Stéphane Dellacherie,et al. Analysis of Godunov type schemes applied to the compressible Euler system at low Mach number , 2010, J. Comput. Phys..
[3] Raphaël Loubère,et al. A second order all Mach number IMEX finite volume solver for the three dimensional Euler equations , 2020, J. Comput. Phys..
[4] Ilya Peshkov,et al. On a pure hyperbolic alternative to the Navier-Stokes equations , 2014 .
[5] Vincenzo Casulli,et al. Semi-implicit finite difference methods for the two-dimensional shallow water equation , 1990 .
[6] Lorenzo Pareschi,et al. A Unified IMEX Runge-Kutta Approach for Hyperbolic Systems with Multiscale Relaxation , 2017, SIAM J. Numer. Anal..
[7] P. Lax,et al. On Upstream Differencing and Godunov-Type Schemes for Hyperbolic Conservation Laws , 1983 .
[8] G. Russo,et al. High Order Asymptotically Strong-Stability-Preserving Methods for Hyperbolic Systems with Stiff Relaxation , 2003 .
[9] Shi Jin,et al. Efficient Asymptotic-Preserving (AP) Schemes For Some Multiscale Kinetic Equations , 1999, SIAM J. Sci. Comput..
[10] Michael Dumbser,et al. ADER-WENO finite volume schemes with space-time adaptive mesh refinement , 2012, J. Comput. Phys..
[11] Michael Dumbser,et al. Semi-implicit discontinuous Galerkin methods for the incompressible Navier–Stokes equations on adaptive staggered Cartesian grids , 2016, 1612.09558.
[12] Claus-Dieter Munz,et al. On Godunov-type schemes for Lagrangian gas dynamics , 1994 .
[13] Vincenzo Casulli,et al. A SEMI-IMPLICIT FINITE DIFFERENCE METHOD FOR NON-HYDROSTATIC, FREE-SURFACE FLOWS , 1999 .
[14] Dinshaw S. Balsara,et al. High order direct Arbitrary-Lagrangian-Eulerian (ALE) PNPM schemes with WENO Adaptive-Order reconstruction on unstructured meshes , 2019, J. Comput. Phys..
[15] Gabriella Puppo,et al. CWENO: Uniformly accurate reconstructions for balance laws , 2016, Math. Comput..
[16] Claus-Dieter Munz,et al. Coupling of compressible and incompressible flow regions using the multiple pressure variables approach , 2015 .
[17] Fabrice Deluzet,et al. An Asymptotic Preserving scheme for the Euler equations in a strong magnetic field , 2008, J. Comput. Phys..
[18] A. Stroud. Approximate calculation of multiple integrals , 1973 .
[19] Michael Dumbser,et al. Finite volume schemes of very high order of accuracy for stiff hyperbolic balance laws , 2008, J. Comput. Phys..
[20] Steven J. Ruuth,et al. Implicit-explicit Runge-Kutta methods for time-dependent partial differential equations , 1997 .
[21] Lorenzo Pareschi,et al. Implicit-explicit runge-kutta schemes and applications to hyperbolic systems with relaxation , 2010, 1009.2757.
[22] Tao Xiong,et al. A high order semi-implicit IMEX WENO scheme for the all-Mach isentropic Euler system , 2019, J. Comput. Phys..
[23] Raphaël Loubère,et al. Second-order implicit-explicit total variation diminishing schemes for the Euler system in the low Mach regime , 2017, J. Comput. Phys..
[24] E. Hofer,et al. A Partially Implicit Method for Large Stiff Systems of ODEs with Only Few Equations Introducing Small Time-Constants , 1976 .
[25] Michael Dumbser,et al. Arbitrary high order PNPM schemes on unstructured meshes for the compressible Navier–Stokes equations , 2010 .
[26] Michael Dumbser,et al. Space-time adaptive ADER-DG schemes for dissipative flows: Compressible Navier-Stokes and resistive MHD equations , 2016, Comput. Phys. Commun..
[27] Eleuterio F. Toro,et al. Flux splitting schemes for the Euler equations , 2012 .
[28] Dinshaw S. Balsara,et al. Self-adjusting, positivity preserving high order schemes for hydrodynamics and magnetohydrodynamics , 2012, J. Comput. Phys..
[29] Rémi Abgrall,et al. An adaptive shock-capturing algorithm for solving unsteady reactive flows , 2003 .
[30] W. Boscheri. A space-time semi-Lagrangian advection scheme on staggered Voronoi meshes applied to free surface flows , 2020 .
[31] Michael Dumbser,et al. A conservative, weakly nonlinear semi-implicit finite volume scheme for the compressible Navier-Stokes equations with general equation of state , 2016, Appl. Math. Comput..
[32] Philip M. Gresho,et al. On the theory of semi‐implicit projection methods for viscous incompressible flow and its implementation via a finite element method that also introduces a nearly consistent mass matrix. Part 1: Theory , 1990 .
[33] R. LeVeque. Finite Volume Methods for Hyperbolic Problems: Characteristics and Riemann Problems for Linear Hyperbolic Equations , 2002 .
[34] E. Toro. Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .
[35] Claus-Dieter Munz,et al. A contribution to the construction of diffusion fluxes for finite volume and discontinuous Galerkin schemes , 2007, J. Comput. Phys..
[36] R. Klein. Semi-implicit extension of a Godunov-type scheme based on low Mach number asymptotics , 1995 .
[37] E. Turkel,et al. Preconditioned methods for solving the incompressible low speed compressible equations , 1987 .
[38] Chi-Wang Shu,et al. Strong Stability-Preserving High-Order Time Discretization Methods , 2001, SIAM Rev..
[39] G. Russo,et al. Central WENO schemes for hyperbolic systems of conservation laws , 1999 .
[40] P. Roe,et al. On Godunov-type methods near low densities , 1991 .
[41] Samuel Kokh,et al. Large Time Step and Asymptotic Preserving Numerical Schemes for the Gas Dynamics Equations with Source Terms , 2013, SIAM J. Sci. Comput..
[42] S. Orszag,et al. Small-scale structure of the Taylor–Green vortex , 1983, Journal of Fluid Mechanics.
[43] Francis Filbet,et al. High Order Semi-implicit Schemes for Time Dependent Partial Differential Equations , 2016, Journal of Scientific Computing.
[44] Chaowei Hu,et al. No . 98-32 Weighted Essentially Non-Oscillatory Schemes on Triangular Meshes , 1998 .
[45] Pierre Degond,et al. An Asymptotic-Preserving all-speed scheme for the Euler and Navier-Stokes equations , 2011, J. Comput. Phys..
[46] Florian Bernard,et al. Linearly implicit all Mach number shock capturing schemes for the Euler equations , 2019, J. Comput. Phys..
[47] H. Guillard,et al. On the behavior of upwind schemes in the low Mach number limit: II. Godunov type schemes , 2004 .
[48] M. Dumbser,et al. An efficient semi-implicit finite volume method for axially symmetric compressible flows in compliant tubes , 2015 .
[49] Santiago Badia,et al. Assessment of variational multiscale models for the large eddy simulation of turbulent incompressible flows , 2015 .
[50] Michael Dumbser,et al. A staggered space-time discontinuous Galerkin method for the three-dimensional incompressible Navier-Stokes equations on unstructured tetrahedral meshes , 2016, J. Comput. Phys..
[51] M. Dumbser,et al. Semi-implicit staggered discontinuous Galerkin schemes for axially symmetric viscous compressible flows in elastic tubes , 2018 .
[52] Luigi Brugnano,et al. Iterative Solution of Piecewise Linear Systems , 2007, SIAM J. Sci. Comput..
[53] Michael Dumbser,et al. Central Weighted ENO Schemes for Hyperbolic Conservation Laws on Fixed and Moving Unstructured Meshes , 2017, SIAM J. Sci. Comput..
[54] Axel Klar. An Asymptotic Preserving Numerical Scheme for Kinetic Equations in the Low Mach Number Limit , 1999 .
[55] T. Alazard,et al. Low Mach Number Limit of the Full Navier-Stokes Equations , 2005, math/0501386.
[56] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[57] Michael Dumbser,et al. Arbitrary high order non-oscillatory finite volume schemes on unstructured meshes for linear hyperbolic systems , 2007, J. Comput. Phys..
[58] With Invariant Submanifolds,et al. Systems of Conservation Laws , 2009 .
[59] Song Jiang,et al. Low Mach number limit of full Navier–Stokes equations in a 3D bounded domain , 2015 .
[60] Giovanni Russo,et al. On a Class of Uniformly Accurate IMEX Runge--Kutta Schemes and Applications to Hyperbolic Systems with Relaxation , 2009, SIAM J. Sci. Comput..
[61] Katja Bachmeier,et al. Numerical Heat Transfer And Fluid Flow , 2016 .