Investigation on the Solubility of SO2and CO2in Imidazolium-Based Ionic Liquids Using NPT Monte Carlo Simulation

2011 ◽  
Vol 115 (46) ◽  
pp. 13599-13607 ◽  
Author(s):  
Ahmadreza. F. Ghobadi ◽  
Vahid Taghikhani ◽  
J. Richard Elliott
Keyword(s):  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Ionic Liquids

Monte Carlo simulation for the antiscaling performance of Gemini ionic liquids

2019 ◽  
Vol 285 ◽  
pp. 408-415 ◽  
Author(s):  
Amr Elgendy ◽  
A.E. Elkholy ◽  
N.M. El Basiony ◽  
M.A. Migahed
Keyword(s):  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Ionic Liquids

Electron Scattering in Solids

1990 ◽  
Vol 48 (2) ◽  
pp. 4-5
Author(s):  
Ryuichi Shimizu ◽  
Ze-Jun Ding
Keyword(s):  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Angular Distribution ◽  
Elastic Scattering ◽  
Electron Scattering ◽  
Cross Sections ◽  
Expansion Method ◽  
Electron Excitation ◽  
Partial Wave Expansion ◽  
Backscattered Electrons

Monte Carlo simulation has been becoming most powerful tool to describe the electron scattering in solids, leading to more comprehensive understanding of the complicated mechanism of generation of various types of signals for microbeam analysis.The present paper proposes a practical model for the Monte Carlo simulation of scattering processes of a penetrating electron and the generation of the slow secondaries in solids. The model is based on the combined use of Gryzinski’s inner-shell electron excitation function and the dielectric function for taking into account the valence electron contribution in inelastic scattering processes, while the cross-sections derived by partial wave expansion method are used for describing elastic scattering processes. An improvement of the use of this elastic scattering cross-section can be seen in the success to describe the anisotropy of angular distribution of elastically backscattered electrons from Au in low energy region, shown in Fig.l. Fig.l(a) shows the elastic cross-sections of 600 eV electron for single Au-atom, clearly indicating that the angular distribution is no more smooth as expected from Rutherford scattering formula, but has the socalled lobes appearing at the large scattering angle.

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