Molecular dynamics computer simulations of sputtering of benzene sample by large mixed Lennard-Jones clusters

2014 ◽  
Vol 326 ◽  
pp. 185-189 ◽  
Author(s):  
L. Rzeznik ◽  
Z. Postawa
Keyword(s):  
Molecular Dynamics ◽  
Computer Simulations ◽  
Lennard Jones

Dynamics of a Supercooled Lennard-Jones System: Qualitative and Quantitative Tests of Mode-Coupling Theory

1997 ◽  
Vol 126 ◽  
pp. 35-42 ◽  
Author(s):  
Walter Kob ◽  
Markus Nauroth ◽  
Hans C. Andersen
Keyword(s):  
Molecular Dynamics ◽  
Computer Simulations ◽  
Low Temperatures ◽  
Mode Coupling ◽  
Coupling Theory ◽  
Mode Coupling Theory ◽  
Qualitative And Quantitative ◽  
Lennard Jones ◽  
Coupling Equations ◽  
Universal Properties

Using molecular dynamics computer simulations, we investigate the dynamics of a binary Lennard-Jones system at low temperatures. We show that this dynamics can be described well by mode-coupling theory. By solving numerically the mode-coupling equations for this system, we demonstrate that the theory is not only able to correctly predict the universal properties of this dynamics but also the nonuniversal properties.

Multicanonical Molecular Dynamics Simulation Study of the Liquid-Solid and Solid-Solid Transitions in Lennard-Jones Clusters

2011 ◽  
Author(s):  
Toshihiro Kaneko ◽  
Kenji Yasuoka ◽  
Ayori Mitsutake ◽  
Xiao Cheng Zeng
Keyword(s):  
Molecular Dynamics ◽  
Heat Capacity ◽  
Transition Temperature ◽  
Peak Position ◽  
Temperature Curve ◽  
Dynamics Simulation ◽  
Lennard Jones ◽  
Dynamics Simulations ◽  
First Time ◽  
Good Agreement

Multicanonical molecular dynamics simulations are applied, for the first time, to study the liquid-solid and solid-solid transitions in Lennard-Jones (LJ) clusters. The transition temperatures are estimated based on the peak position in the heat capacity versus temperature curve. For LJ31, LJ58 and LJ98, our results on the solid-solid transition temperature are in good agreement with previous ones. For LJ309, the predicted liquid-solid transition temperature is also in agreement with previous result.

scholarly journals Simulation of Mechanical Deformation and Tribology of Nano-Thin Amorphous Hydrogenated Carbon (a:Ch) Films Using Molecular Dynamics

1996 ◽  
Vol 436 ◽  
Author(s):  
J. N. Glosli ◽  
M. R. Philpott ◽  
J. Belak
Keyword(s):  
Molecular Dynamics ◽  
Substrate Temperature ◽  
Computer Simulations ◽  
Mechanical Deformation ◽  
Porous Graphite ◽  
Pure Carbon ◽  
Substrate Temperatures ◽  
Amorphous Hydrogenated Carbon ◽  
Deposition Energy

AbstractMolecular dynamics computer simulations are used to study the effect of substrate temperature on the microstructure of deposited amorphous hydrogenated carbon (a:CH) films. A transition from dense diamond-like films to porous graphite-like films is observed between substrate temperatures of 400K and 600K for a deposition energy of 20 eV. The dense a:CH film grown at 300K and 20 eV has a hardness (˜50 GPa) about half that of a pure carbon (a:C) film grown under the same conditions.

Molecular Dynamics Study of Ion Impact Phenomena and Compressive Stress in Thin Films

1993 ◽  
Vol 317 ◽  
Author(s):  
N.A. Marks ◽  
P. Guan ◽  
D.R. Mckenzie ◽  
B.A. PailThorpe
Keyword(s):  
Molecular Dynamics ◽  
Three Dimensional ◽  
Carbon Films ◽  
Loss Mechanism ◽  
Ion Energy ◽  
Lennard Jones ◽  
Impact Phenomena ◽  
Ion Impact ◽  
Dynamics Simulations ◽  
The Impact

ABSTRACTMolecular dynamics simulations of nickel and carbon have been used to study the phenomena due to ion impact. The nickel and carbon interactions were described using the Lennard-Jones and Stillinger-Weber potentials respectively. The phenomena occurring after the impact of 100 e V to 1 keV ions were studied in the nickel simulations, which were both two and three-dimensional. Supersonic focussed collision sequences (or focusons) were observed, and associated with these focusons were unexpected sonic bow waves, which were a major energy loss mechanism for the focuson. A number of 2D carbon films were grown and the stress in the films as a function of incident ion energy was Measured. With increasing energy the stress changed from tensile to compressive and reached a maximum around 50 eV, in agreement with experiment.

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