Vibrational Modeling with an Anharmonic Oscillator Model in Direct Simulation Monte Carlo
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[1] Luc Mieussens,et al. IXV post-flight reconstruction and analysis of the aerothermodynamic measurements along the rarefied portion of the reentry trajectory , 2021 .
[2] T. Schwartzentruber,et al. Non-Boltzmann vibrational energy distributions and coupling to dissociation rate. , 2019, The Journal of chemical physics.
[3] C. Munz,et al. Combining particle-in-cell and direct simulation Monte Carlo for the simulation of reactive plasma flows , 2019, Physics of Fluids.
[4] Liwu Liu,et al. High-temperature partition functions, specific heats and spectral radiative properties of diatomic molecules with an improved calculation of energy levels , 2018 .
[5] Stephen M. Longshaw,et al. dsmcFoam+: An OpenFOAM based direct simulation Monte Carlo solver , 2017, Comput. Phys. Commun..
[6] Manuel Torrilhon,et al. The 35-Moment System with the Maximum-Entropy Closure for Rarefied Gas Flows , 2017 .
[7] Thomas E. Schwartzentruber,et al. Nonequilibrium Gas Dynamics and Molecular Simulation , 2017 .
[8] D. Griffiths. Introduction to Quantum Mechanics , 2016 .
[9] Alina A. Alexeenko,et al. Ab initio-informed maximum entropy modeling of rovibrational relaxation and state-specific dissociation with application to the O2 + O system. , 2016, The Journal of chemical physics.
[10] D. Levin,et al. A study of internal energy relaxation in shocks using molecular dynamics based models. , 2015, The Journal of chemical physics.
[11] Alina A. Alexeenko,et al. Effect of O2 + O ab initio and Morse additive pairwise potentials on dissociation and relaxation rates for nonequilibrium flow calculations , 2015 .
[12] G. Candler,et al. An improved potential energy surface and multi-temperature quasiclassical trajectory calculations of N2 + N2 dissociation reactions. , 2015, The Journal of chemical physics.
[13] Marco Panesi,et al. General multi-group macroscopic modeling for thermo-chemical non-equilibrium gas mixtures. , 2015, The Journal of chemical physics.
[14] F. Esposito,et al. N2, O2, NO state-to-state vibrational kinetics in hypersonic boundary layers: The problem of rescaling rate coefficients to uniform vibrational ladders , 2015 .
[15] T. Schwartzentruber,et al. Rovibrational coupling in molecular nitrogen at high temperature: An atomic-level study , 2014 .
[16] Thomas E. Schwartzentruber,et al. Progress and Future Prospects for Particle-Based Simulation of Hypersonic Flow , 2013 .
[17] A. Soufiani,et al. High-Temperature and Nonequilibrium Partition Function and Thermodynamic Data of Diatomic Molecules , 2009 .
[18] M. Capitelli,et al. Recombination-Assisted Nitrogen Dissociation Rates Under Nonequilibrium Conditions , 2008 .
[19] J. Loureiro,et al. Vibrational distributions in N2 with an improved calculation of energy levels using the RKR method , 2008 .
[20] J. L. Stollery,et al. Hypersonic and High-Temperature Gas Dynamics – Second edition J.D. Anderson American Institute of Aeronautics and Astronautics, 1801 Alexander Bell Drive, Suite 500, Reston, VA, USA. 20191-4344. 2006. 811pp. Illustrated. $64.95 (AIAA members), $90.95 (non-members). ISBN 1-56347-780-7. , 2007, The Aeronautical Journal (1968).
[21] L. Marraffa,et al. High-Temperature Thermodynamic Properties of Mars-Atmosphere Components , 2004 .
[22] Katsuhisa Koura,et al. Direct simulation Monte Carlo study of rotational nonequilibrium in shock wave and spherical expansion of nitrogen using classical trajectory calculations , 2002 .
[23] I. Adamovich,et al. Semiclassical modeling of state-specific dissociation rates in diatomic gases , 2000 .
[24] Hrvoje Jasak,et al. A tensorial approach to computational continuum mechanics using object-oriented techniques , 1998 .
[25] Katsuhisa Koura,et al. Monte Carlo direct simulation of rotational relaxation of nitrogen through high total temperature shock waves using classical trajectory calculations , 1998 .
[26] Katsuhisa Koura,et al. 4 Carlo direct simulation of rotational relaxation of diatomic molecules using classical trajectory calculations: Nitrogen shock wave , 1997 .
[27] Stefan Dietrich,et al. Scalar and Parallel Optimized Implementation of the Direct Simulation Monte Carlo Method , 1996 .
[28] Stephen M. Ruffin,et al. Prediction of Vibrational Relaxation in Hypersonic Expanding Flows Part 2: Results , 1995 .
[29] S. Ruffin,et al. Prediction of vibrational relaxation in hypersonic expanding flows. I: Model development , 1995 .
[30] I. Adamovich,et al. Vibrational relaxation and dissociation behind shock waves. Part 1 - Kinetic rate models. , 1995 .
[31] K. Koura. A set of model cross sections for the Monte Carlo simulation of rarefied real gases: Atom–diatom collisions , 1994 .
[32] James B. Anderson,et al. Direct Monte Carlo simulation of chemical reaction systems: Internal energy transfer and an energy‐dependent unimolecular reaction , 1993 .
[33] Iain D. Boyd,et al. Models for direct Monte Carlo simulation of coupled vibration-dissociation , 1993 .
[34] Graeme A. Bird,et al. Definition of mean free path for real gases , 1983 .
[35] Claus Borgnakke,et al. Statistical collision model for Monte Carlo simulation of polyatomic gas mixture , 1975 .
[36] P. V. Marrone,et al. Chemical Relaxation with Preferential Dissociation from Excited Vibrational Levels , 1963 .
[37] P. V. Marrone,et al. Effect of Dissociation on the Rate of Vibrational Relaxation , 1962 .
[38] J. D. Teare,et al. Theory of Radiation from Luminous Shock Waves in Nitrogen , 1959 .
[39] R. L. Roy,et al. LEVEL: A computer program for solving the radial Schrödinger equation for bound and quasibound levels , 2017 .
[40] Hugh M. Hulburt,et al. Potential Energy Functions for Diatomic Molecules , 1941 .