A modified monotonicity-preserving high-order scheme with application to computation of multi-phase flows
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[1] G. A. Gerolymos,et al. Very-high-order weno schemes , 2009, J. Comput. Phys..
[2] Zeyao Mo,et al. Hybrid monotonicity-preserving piecewise parabolic method for compressible Euler equations , 2017 .
[3] Meng-Sing Liou,et al. Integration of Navier-Stokes Equations Using Dual Time Stepping and a Multigrid Method , 1995 .
[4] Yufeng Yao,et al. Direct numerical simulation of supersonic turbulent flows around a tandem expansion-compression corner , 2015 .
[5] E. Puckett,et al. A High-Order Projection Method for Tracking Fluid Interfaces in Variable Density Incompressible Flows , 1997 .
[6] Sharath S. Girimaji,et al. WENO-enhanced gas-kinetic scheme for direct simulations of compressible transition and turbulence , 2013, J. Comput. Phys..
[7] Fei Liao,et al. Optimized low-dissipation and low-dispersion schemes for compressible flows , 2018, J. Comput. Phys..
[8] Bruno Després,et al. Contact Discontinuity Capturing Schemes for Linear Advection and Compressible Gas Dynamics , 2002, J. Sci. Comput..
[9] Christian Tenaud,et al. High order one-step monotonicity-preserving schemes for unsteady compressible flow calculations , 2004 .
[10] Olivier Roussel,et al. Unsteady compressible flow computations using an adaptive multiresolution technique coupled with a high-order one-step shock-capturing scheme , 2015 .
[11] Axel Voigt,et al. Benchmark computations of diffuse interface models for two‐dimensional bubble dynamics , 2012 .
[12] Åsmund Ervik,et al. Computation of three-dimensional three-phase flow of carbon dioxide using a high-order WENO scheme , 2017, J. Comput. Phys..
[13] Cong-Tu Ha,et al. Numerical simulations of compressible flows using multi-fluid models , 2015 .
[14] Tim Colonius,et al. Finite-volume WENO scheme for viscous compressible multicomponent flows , 2014, J. Comput. Phys..
[15] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[16] Huanan Yang,et al. An artificial compression method for ENO schemes - The slope modification method. [essentially nonoscillatory , 1990 .
[17] Bin Chen,et al. A multiphase MPS solver for modeling multi-fluid interaction with free surface and its application in oil spill , 2017 .
[18] J. H. M. ten Thije Boonkkamp,et al. Embedded WENO: A design strategy to improve existing WENO schemes , 2017, J. Comput. Phys..
[19] Mark H. Carpenter,et al. Computational Considerations for the Simulation of Shock-Induced Sound , 1998, SIAM J. Sci. Comput..
[20] Eckart Meiburg,et al. A numerical study of the convergence properties of ENO schemes , 1990 .
[21] D. Kuzmin,et al. Quantitative benchmark computations of two‐dimensional bubble dynamics , 2009 .
[22] Cong Huang,et al. A simple smoothness indicator for the WENO scheme with adaptive order , 2018, J. Comput. Phys..
[23] P. Sweby. High Resolution Schemes Using Flux Limiters for Hyperbolic Conservation Laws , 1984 .
[24] P. Woodward,et al. The Piecewise Parabolic Method (PPM) for Gas Dynamical Simulations , 1984 .
[25] Chi-Wang Shu,et al. Recovering High-Order Accuracy in WENO Computations of Steady-State Hyperbolic Systems , 2006, J. Sci. Comput..
[26] A. Chinnayya,et al. A computational study of the interaction of gaseous detonations with a compressible layer , 2017 .
[27] Phillip Colella,et al. A limiter for PPM that preserves accuracy at smooth extrema , 2008, J. Comput. Phys..
[28] P. Lax. Weak solutions of nonlinear hyperbolic equations and their numerical computation , 1954 .
[29] Yuxi Chen,et al. A fifth-order finite difference scheme for hyperbolic equations on block-adaptive curvilinear grids , 2016, J. Comput. Phys..
[30] O. Zanotti,et al. ECHO: a Eulerian conservative high-order scheme for general relativistic magnetohydrodynamics and magnetodynamics , 2007, 0704.3206.
[31] Rong Wang,et al. A New Mapped Weighted Essentially Non-oscillatory Scheme , 2012, J. Sci. Comput..
[32] P. Roe. CHARACTERISTIC-BASED SCHEMES FOR THE EULER EQUATIONS , 1986 .
[33] J. Brackbill,et al. A continuum method for modeling surface tension , 1992 .
[34] A. Chorin. A Numerical Method for Solving Incompressible Viscous Flow Problems , 1997 .
[35] Ian M. Mitchell,et al. A hybrid particle level set method for improved interface capturing , 2002 .
[36] Wayne A. Smith,et al. Preconditioning Applied to Variable and Constant Density Flows , 1995 .
[37] P. Roe. Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .
[38] Marcel Vinokur,et al. Spectral (finite) volume method for conservation laws on unstructured grids V: Extension to three-dimensional systems , 2006, J. Comput. Phys..
[39] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[40] Alain Lerat. An efficient high-order compact scheme for the unsteady compressible Euler and Navier-Stokes equations , 2016, J. Comput. Phys..
[41] Ming Yu,et al. A new weighting method for improving the WENO‐Z scheme , 2018 .
[42] Miguel R. Visbal,et al. On the use of higher-order finite-difference schemes on curvilinear and deforming meshes , 2002 .
[43] A. J. Kriel. Error analysis of flux limiter schemes at extrema , 2017, J. Comput. Phys..
[44] Chi-Wang Shu,et al. High Order Weighted Essentially Nonoscillatory Schemes for Convection Dominated Problems , 2009, SIAM Rev..
[45] Paul E. Dimotakis,et al. Mixing, scalar boundedness, and numerical dissipation in large-eddy simulations , 2018, J. Comput. Phys..
[46] H. Rouse,et al. Cavitation and pressure distribution: head forms at zero angle of yaw , 1948 .
[47] Chi-Wang Shu. Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws , 1998 .
[48] Ali H. Nayfeh,et al. Computations of the Compressible Multiphase Flow Over the Cavitating High-Speed Torpedo , 2003 .
[49] Ali H. Nayfeh,et al. Numerical simulation of 3-D incompressible, multi-phase flows over cavitating projectiles , 2004 .
[50] Dinshaw S. Balsara,et al. An efficient class of WENO schemes with adaptive order , 2016, J. Comput. Phys..
[51] Zhaorui Li,et al. A high‐order finite difference method for numerical simulations of supersonic turbulent flows , 2012 .
[52] A. Harten. ENO schemes with subcell resolution , 1989 .
[53] Shiyi Chen,et al. A hybrid scheme for compressible magnetohydrodynamic turbulence , 2016, J. Comput. Phys..
[54] Chi-Wang Shu. Numerical experiments on the accuracy of ENO and modified ENO schemes , 1990 .
[55] B. V. Leer,et al. Towards the ultimate conservative difference scheme. II. Monotonicity and conservation combined in a second-order scheme , 1974 .
[56] Zhiwei He,et al. An improved accurate monotonicity-preserving scheme for the Euler equations , 2016 .
[57] Charbel Farhat,et al. A higher-order generalized ghost fluid method for the poor for the three-dimensional two-phase flow computation of underwater implosions , 2008, J. Comput. Phys..
[58] Robert Saye. Implicit mesh discontinuous Galerkin methods and interfacial gauge methods for high-order accurate interface dynamics, with applications to surface tension dynamics, rigid body fluid-structure interaction, and free surface flow: Part I , 2017, J. Comput. Phys..
[59] C. Merkle,et al. Computational modeling of the dynamics of sheet cavitation , 1998 .
[60] S. Osher,et al. Some results on uniformly high-order accurate essentially nonoscillatory schemes , 1986 .
[61] H. Huynh,et al. Accurate Monotonicity-Preserving Schemes with Runge-Kutta Time Stepping , 1997 .
[62] Dong-Hyun Kim,et al. A compressive interface-capturing scheme for computation of compressible multi-fluid flows , 2017 .
[63] Nikolaus A. Adams,et al. A new class of adaptive high-order targeted ENO schemes for hyperbolic conservation laws , 2018, J. Comput. Phys..
[64] Bing Wang,et al. An incremental-stencil WENO reconstruction for simulation of compressible two-phase flows , 2017, International Journal of Multiphase Flow.
[65] Manuel Torrilhon,et al. Compact third-order limiter functions for finite volume methods , 2009, J. Comput. Phys..
[66] Chi-Wang Shu,et al. Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .
[67] R. Keppens,et al. MPI-AMRVAC FOR SOLAR AND ASTROPHYSICS , 2014, 1407.2052.
[68] Bruno Costa,et al. An improved WENO-Z scheme , 2016, J. Comput. Phys..
[69] Cong-Tu Ha,et al. Evaluation of a new scaling term in preconditioning schemes for computations of compressible cavitating and ventilated flows , 2016 .
[70] M. Dumbser,et al. High-Order Unstructured Lagrangian One-Step WENO Finite Volume Schemes for Non-Conservative Hyperbolic Systems: Applications to Compressible Multi-Phase Flows , 2013, 1304.4816.
[71] Jack R. Edwards,et al. An investigation of interface-sharpening schemes for multi-phase mixture flows , 2009, J. Comput. Phys..
[72] E. Tadmor,et al. Convenient total variation diminishing conditions for nonlinear difference schemes. Final report , 1988 .
[73] Gordon Erlebacher,et al. Interaction of a shock with a longitudinal vortex , 1996, Journal of Fluid Mechanics.
[74] Ratnesh K. Shukla,et al. Adaptive finite-volume WENO schemes on dynamically redistributed grids for compressible Euler equations , 2016, J. Comput. Phys..
[75] R. C. Swanson. On Some Numerical Dissipation Schemes , 1998 .
[76] Jacob A. McFarland,et al. A numerical method for shock driven multiphase flow with evaporating particles , 2017, J. Comput. Phys..
[77] Seung Hyun Kim,et al. An improved consistent, conservative, non-oscillatory and high order finite difference scheme for variable density low Mach number turbulent flow simulation , 2018, J. Comput. Phys..
[78] R. Clift,et al. Bubbles, Drops, and Particles , 1978 .
[79] S. Osher,et al. Weighted essentially non-oscillatory schemes , 1994 .
[80] Francesco Bassi,et al. Multicomponent gas flow computations by a discontinuous Galerkin scheme using L2-projection of perfect gas EOS , 2016, J. Comput. Phys..
[81] Olivier Desjardins,et al. A discontinuous Galerkin conservative level set scheme for interface capturing in multiphase flows , 2013, J. Comput. Phys..
[82] Martí Raga,et al. New computational techniques for finite-difference Weighted Essentially Non-Oscillatory schemes and related problems , 2014 .
[83] B. V. Leer,et al. Towards the ultimate conservative difference scheme V. A second-order sequel to Godunov's method , 1979 .
[84] I. Bohachevsky,et al. Finite difference method for numerical computation of discontinuous solutions of the equations of fluid dynamics , 1959 .
[85] Farshid Nazari,et al. High-order low-dissipation low-dispersion diagonally implicit Runge-Kutta schemes , 2015, J. Comput. Phys..