Rayleigh-Brillouin scattering spectra (RBS) in molecular Oxygen have been simulated by DSMC. Different scattering models have been implemented based either on the Larsen-Borgnakke relaxation model and on the Classical Trajectories technique. Results are compared with recent experimentally measured spectra showing good agreement. It is suggested that DSMC-based models be used in the interpretation of light scattering experiments in place of the simplified kinetic models, widely used for the interpretation of RBS experiments. Actually, the former have a firmer physical ground and are readily extended to treat gas mixtures of arbitrary complexity. (C) 2016 Elsevier Masson SAS. All rights reserved.

Rayleigh-Brillouin scattering in molecular Oxygen by CT-DSMC simulations

Bruno Domenico;
2017

Abstract

Rayleigh-Brillouin scattering spectra (RBS) in molecular Oxygen have been simulated by DSMC. Different scattering models have been implemented based either on the Larsen-Borgnakke relaxation model and on the Classical Trajectories technique. Results are compared with recent experimentally measured spectra showing good agreement. It is suggested that DSMC-based models be used in the interpretation of light scattering experiments in place of the simplified kinetic models, widely used for the interpretation of RBS experiments. Actually, the former have a firmer physical ground and are readily extended to treat gas mixtures of arbitrary complexity. (C) 2016 Elsevier Masson SAS. All rights reserved.
2017
Istituto di Nanotecnologia - NANOTEC
Inglese
64
8
16
https://www.sciencedirect.com/science/article/abs/pii/S0997754616301765?via%3Dihub
Sì, ma tipo non specificato
Direct simulation Monte Carlo
Classical trajectory calculations
CT-DSMC
Rarefied gas dynamics
3
info:eu-repo/semantics/article
262
Bruno, Domenico; Frezzotti, Aldo; Ghiroldi Gian, Pietro
01 Contributo su Rivista::01.01 Articolo in rivista
open
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/372065
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