Light intensity effects on diffusion‐influenced fluorescence quenching in a hard‐sphere liquid: Molecular dynamics simulation and the many‐body Smoluchowski equation approach

1995 ◽  
Vol 102 (24) ◽  
pp. 9557-9564 ◽  
Author(s):  
T. Bandyopadhyay
Keyword(s):  
Molecular Dynamics ◽  
Molecular Dynamics Simulation ◽  
Light Intensity ◽  
Fluorescence Quenching ◽  
Hard Sphere ◽  
Dynamics Simulation ◽  
Equation Approach ◽  
Many Body ◽  
Hard Sphere Liquid ◽  
The Many

Molecular Dynamics Simulation of Sputtering with Mmany-Body Interactions

1988 ◽  
Vol 100 ◽  
Author(s):  
Davy Y. Lo ◽  
Tom A. Tombrello ◽  
Mark H. Shapiro ◽  
Don E. Harrison
Keyword(s):  
Molecular Dynamics ◽  
Molecular Dynamics Simulation ◽  
Single Crystal ◽  
Low Energy ◽  
Dynamics Simulation ◽  
Embedded Atom Method ◽  
Many Body ◽  
Embedded Atom ◽  
Dynamics Simulations ◽  
Small Single Crystal

ABSTRACTMany-body forces obtained by the Embedded-Atom Method (EAM) [41 are incorporated into the description of low energy collisions and surface ejection processes in molecular dynamics simulations of sputtering from metal targets. Bombardments of small, single crystal Cu targets (400–500 atoms) in three different orientations ({100}, {110}, {111}) by 5 keV Ar+ ions have been simulated. The results are compared to simulations using purely pair-wise additive interactions. Significant differences in the spectra of ejected atoms are found.

Molecular Dynamics Simulation of Thermal Conductivity of Aluminum

2013 ◽  
Vol 336 ◽  
pp. 47-55
Author(s):  
Jamal Davoodi ◽  
Samaneh Khoshkhatti
Keyword(s):  
Thermal Conductivity ◽  
Molecular Dynamics ◽  
Molecular Dynamics Simulation ◽  
Equations Of Motion ◽  
Fixed Number ◽  
Dynamics Simulation ◽  
Many Body ◽  
Macro Scale ◽  
Body Potential ◽  
Increasing Temperature

In this research, the thermal conductivity of aluminum (Al) in macro scale was investigated by the molecular dynamics simulation technique. We used FORTRAN programming in the simulations and used a fixed number of atoms, N, confined to a fixed pressure, P, and maintained at a constant preset temperature, T, i.e. the NPT ensemble. The Sutton-Chen many-body potential was used to calculate energy and force. The temperature and pressure of the system were controlled by Nosé-Hoover thermostat and Berendsen barostat respectively. We could solve the equations of motion using the Velocity Verlet algorithm. We calculated the thermal conductivity of Al in the macro scale using the Green-Kubo method. Moreover, we have studied the effect of increasing temperature on the value of the thermal conductivity of Al. The obtained results showed that the computed thermal conductivities are in good agreement with experimental data.

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