WENO interpolation for Lagrangian particles in highly compressible flow regimes
暂无分享,去创建一个
Luis Bravo | Peter E. Hamlington | Y. Kozak | S. S. Dammati | Alexei Poludnenko | Y. Kozak | P. Hamlington | L. Bravo | A. Poludnenko | Sai Sandeep Dammati
[1] P. Woodward,et al. The Piecewise Parabolic Method (PPM) for Gas Dynamical Simulations , 1984 .
[2] T. Miyauchi,et al. Combustion regime classification of HCCI/PCCI combustion using Lagrangian fluid particle tracking , 2015 .
[3] The Influence of Chemical Kinetics on the Structure of Hydrogen-Air Detonations , 2012 .
[4] C. Carter,et al. Simultaneous 10 kHz TPIV, OH PLIF, and CH2O PLIF measurements of turbulent flame structure and dynamics , 2016 .
[5] S. Pope,et al. An algorithm for tracking fluid particles in numerical simulations of homogeneous turbulence , 1988 .
[6] Jianchun Wang,et al. Intermittency caused by compressibility: a Lagrangian study , 2015, Journal of Fluid Mechanics.
[7] M. Ihme,et al. The cross-scale physical-space transfer of kinetic energy in turbulent premixed flames , 2017 .
[8] Ahmadreza Pishevar,et al. A New fourth order central WENO method for 3D hyperbolic conservation laws , 2012, Appl. Math. Comput..
[9] Pui-Kuen Yeung,et al. LAGRANGIAN INVESTIGATIONS OF TURBULENCE , 2003 .
[10] J. Monaghan. Smoothed particle hydrodynamics , 2005 .
[11] Paul G. Arias,et al. A flame particle tracking analysis of turbulence–chemistry interaction in hydrogen–air premixed flames , 2016 .
[12] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[13] Elaine S. Oran,et al. Flame acceleration and DDT in channels with obstacles: Effect of obstacle spacing , 2008 .
[14] Ronald K. Hanson,et al. Cavity Flame-Holders for Ignition and Flame Stabilization in Scramjets: An Overview , 2001 .
[15] J. Bell,et al. A combined computational and experimental characterization of lean premixed turbulent low swirl laboratory flames , 2012 .
[16] Wai-Sun Don,et al. A high-order WENO-Z finite difference based particle-source-in-cell method for computation of particle-laden flows with shocks , 2009, J. Comput. Phys..
[17] B. Taylor,et al. Lagrangian analysis of high-speed turbulent premixed reacting flows: Thermochemical trajectories in hydrogen–air flames , 2017 .
[18] P. Londrillo,et al. High-Order Upwind Schemes for Multidimensional Magnetohydrodynamics , 1999, astro-ph/9910086.
[19] E. Oran,et al. Spontaneous transition of turbulent flames to detonations in unconfined media. , 2011, Physical review letters.
[20] W. Sirignano,et al. Fluid Dynamics and Transport of Droplets and Sprays , 1999 .
[21] G. S. Patterson,et al. DIFFUSION EXPERIMENTS WITH NUMERICALLY INTEGRATED ISOTROPIC TURBULENCE. , 1974 .
[22] Michael Dumbser,et al. Central Weighted ENO Schemes for Hyperbolic Conservation Laws on Fixed and Moving Unstructured Meshes , 2017, SIAM J. Sci. Comput..
[23] James M. Stone,et al. An unsplit Godunov method for ideal MHD via constrained transport in three dimensions , 2007, J. Comput. Phys..
[24] Lars Hernquist,et al. Following the flow: tracer particles in astrophysical fluid simulations , 2013, 1305.2195.
[25] Chi-Wang Shu. Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws , 1998 .
[26] C. Gheller,et al. The mixing and transport properties of the intra cluster medium: a numerical study using tracers particles , 2009, 0910.1925.
[27] P. Hamlington,et al. Compressible Turbulence Effects on Premixed Autoignition , 2017 .
[28] S. Taki,et al. Numerical Analysis of Two-Dimensional Nonsteady Detonations , 1978 .
[29] Swetaprovo Chaudhuri,et al. Genesis and evolution of premixed flames in turbulence , 2018, Combustion and Flame.
[30] A. Harten. High Resolution Schemes for Hyperbolic Conservation Laws , 2017 .
[31] J. Monaghan,et al. Extrapolating B splines for interpolation , 1985 .
[32] Gabriella Puppo,et al. A third order central WENO scheme for 2D conservation laws , 2000 .
[33] J. Stone,et al. PARTICLE–GAS DYNAMICS WITH ATHENA: METHOD AND CONVERGENCE , 2010, 1005.4980.
[34] Chi-Wang Shu,et al. Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .
[35] Jun Zhu,et al. A new type of multi-resolution WENO schemes with increasingly higher order of accuracy on triangular meshes , 2019, J. Comput. Phys..
[36] Shigeru Tachibana,et al. A combined computational and experimental characterization of lean premixed turbulent low swirl laboratory flames , 2012 .
[37] Wai-Sun Don,et al. An improved weighted essentially non-oscillatory scheme for hyperbolic conservation laws , 2008, J. Comput. Phys..
[38] C. Carter,et al. Relationship between local reaction rate and flame structure in turbulent premixed flames from simultaneous 10 kHz TPIV, OH PLIF, and CH2O PLIF , 2017 .
[39] Mengping Zhang,et al. On the positivity of linear weights in WENO approximations , 2009 .
[40] A. Fedorov. Transition and Stability of High-Speed Boundary Layers , 2011 .
[41] Rainer Grauer,et al. Density-PDFs and Lagrangian statistics of highly compressible turbulence , 2008 .
[42] S. Osher,et al. Weighted essentially non-oscillatory schemes , 1994 .
[43] M. Semplice,et al. Adaptive Mesh Refinement for Hyperbolic Systems Based on Third-Order Compact WENO Reconstruction , 2014, Journal of Scientific Computing.
[44] R. Klessen,et al. Statistical properties of supersonic turbulence in the Lagrangian and Eulerian frameworks , 2011, Journal of Fluid Mechanics.
[45] F. Ham,et al. High Fidelity Simulations of Primary Breakup and Vaporization of Liquid Jet in Cross Flow (JICF) , 2018, 2018 Joint Propulsion Conference.
[46] MPIA Heidelberg,et al. Protoplanetary Disk Turbulence Driven by the Streaming Instability: Linear Evolution and Numerical Methods , 2007, astro-ph/0702625.
[47] John B. McLaughlin,et al. An algorithm for tracking fluid particles in a spectral simulation of turbulent channel flow , 1992 .
[48] P. Teuben,et al. Athena: A New Code for Astrophysical MHD , 2008, 0804.0402.
[49] Jianchun Wang,et al. Acceleration of passive tracers in compressible turbulent flow. , 2013, Physical review letters.
[50] G. Strang. On the Construction and Comparison of Difference Schemes , 1968 .
[51] B. Coriton,et al. Influence of combustion on principal strain-rate transport in turbulent premixed flames , 2015 .
[52] Chi-Wang Shu,et al. High Order Weighted Essentially Nonoscillatory Schemes for Convection Dominated Problems , 2009, SIAM Rev..
[53] R. Klessen,et al. Turbulent mixing in the interstellar medium: an application for Lagrangian tracer particles , 2008, 0805.0196.
[54] J. Anderson,et al. Modern Compressible Flow: With Historical Perspective , 1982 .
[55] R. Grauer,et al. Lyapunov exponents and information dimension of the mass distribution in turbulent compressible flows , 2010 .
[56] Giulio Borghesi,et al. Complex chemistry DNS of n-heptane spray autoignition at high pressure and intermediate temperature conditions , 2013 .
[57] Peter E. Hamlington,et al. Benchmark Direct Numerical Simulations with Lagrangian Tracers for Evaluating Combustion Diagnostics Algorithms , 2019, AIAA Scitech 2019 Forum.
[58] R W Hockney,et al. Computer Simulation Using Particles , 1966 .
[59] R. Pletcher,et al. Computational Fluid Mechanics and Heat Transfer. By D. A ANDERSON, J. C. TANNEHILL and R. H. PLETCHER. Hemisphere, 1984. 599 pp. $39.95. , 1986, Journal of Fluid Mechanics.
[60] Elaine S. Oran,et al. Numerical simulations of hydrogen detonations with detailed chemical kinetics , 2013 .
[61] Andrew T. Corrigan,et al. Progress in Efficient, High-Fidelity, Rotating Detonation Engine Simulations , 2019, AIAA Scitech 2019 Forum.
[62] T. Skjold. Dust explosion modeling: Status and prospects , 2018 .
[63] A. Koichi Hayashi,et al. Numerical study on three-dimensional C-J detonation waves: detailed propagating mechanism and existence of OH radical , 2005 .
[64] Elaine S. Oran,et al. The interaction of high-speed turbulence with flames: Global properties and internal flame structure , 2009, 1106.3699.
[65] S. S. Dammati,et al. Novel Lagrangian-Particle Tracking Method for Highly Compressible, Turbulent, Reacting Flows , 2019, AIAA Scitech 2019 Forum.
[66] J. Urzay,et al. Spatially localized multi-scale energy transfer in turbulent premixed combustion , 2018, Journal of Fluid Mechanics.
[67] Elaine S. Oran,et al. Numerical simulations of detonations in hydrogen-air and methane-air mixtures , 1981 .
[68] I. Boyd,et al. Modeling of Heat Transfer Attenuation by Ablative Gases During the Stardust Reentry , 2012 .
[69] M. Ihme,et al. Spectral kinetic energy transfer in turbulent premixed reacting flows. , 2016, Physical review. E.
[70] C. Birdsall,et al. Plasma Physics via Computer Simulation , 2018 .
[71] E. Oran,et al. Numerical simulation of dilute and dense layered coal-dust explosions , 2015 .
[72] M. Maxey,et al. Methods for evaluating fluid velocities in spectral simulations of turbulence , 1989 .
[73] Dimos Poulikakos,et al. High order interpolation and differentiation using B-splines , 2004 .
[74] Chaowei Hu,et al. No . 98-32 Weighted Essentially Non-Oscillatory Schemes on Triangular Meshes , 1998 .
[75] F. Toschi,et al. Lagrangian Properties of Particles in Turbulence , 2009 .
[76] A. K. Oppenheim,et al. Recent Progress in Detonation Research , 1963 .
[77] E. Toro. Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .
[78] Peter S. Bernard,et al. The effect of interpolation errors on the Lagrangian analysis of simulated turbulent channel flow , 1994 .
[79] Steve Bryson,et al. High-Order Central WENO Schemes for Multidimensional Hamilton-Jacobi Equations , 2013, SIAM J. Numer. Anal..