Kolmogorov flow in two dimensional strongly coupled Yukawa liquid: A molecular dynamics study

2015 ◽  
Vol 22 (10) ◽  
pp. 103706 ◽  
Author(s):  
Akanksha Gupta ◽  
Rajaraman Ganesh ◽  
Ashwin Joy
Keyword(s):  
Molecular Dynamics ◽  
Two Dimensional ◽  
Strongly Coupled ◽  
Kolmogorov Flow

Kolmogorov flow in two dimensional strongly coupled dusty plasma

2014 ◽  
Vol 21 (7) ◽  
pp. 073707 ◽  
Author(s):  
Akanksha Gupta ◽  
R. Ganesh ◽  
Ashwin Joy
Keyword(s):  
Dusty Plasma ◽  
Two Dimensional ◽  
Strongly Coupled ◽  
Kolmogorov Flow ◽  
Strongly Coupled Dusty Plasma

Shear Flows in Two Dimensional Strongly Coupled Yukawa Liquids: A Large Scale Molecular Dynamics Study

2011 ◽  
Author(s):  
R. Ganesh ◽  
J. Ashwin ◽  
Vladimir Yu. Nosenko ◽  
Padma K. Shukla ◽  
Markus H. Thoma ◽  
...  
Keyword(s):  
Molecular Dynamics ◽  
Large Scale ◽  
Shear Flows ◽  
Two Dimensional ◽  
Strongly Coupled

scholarly journals Polarized Thermal Conductivity of Two-Dimensional Dusty Plasmas

2021 ◽  
Author(s):  
Aamir Shahzad ◽  
Madiha Naheed ◽  
Aadil Mahboob ◽  
Muhammad Kashif ◽  
Alina Manzoor ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Molecular Dynamics ◽  
Simulation Method ◽  
Dusty Plasmas ◽  
Two Dimensional ◽  
Strongly Coupled ◽  
External Force Field ◽  
Theoretical Predictions ◽  
System Temperature ◽  
Non Equilibrium Molecular Dynamics

The computation of thermalt properties of dusty plasmas is substantial task in the area of science and technology. The thermal conductivity (λ) has been computed by applying polarization effect through molecular dynamics (MD) simulations of two dimensional (2D) strongly coupled complex dusty plasmas (SCCDPs). The effects of polarization on thermal conductivity have been measured for a wide range of Coulomb coupling (Γ) and Debye screening (κ) parameters using homogeneous non-equilibrium molecular dynamics (HNEMD) method for suitable system sizes. The HNEMD simulation method is employed at constant external force field strength (F*) and varying polarization effects. The algorithm provides precise results with rapid convergence and minute dimension effects. The outcomes have been compared with earlier available simulation results of molecular dynamics, theoretical predictions and experimental results of complex dusty plasma liquids. The calculations show that the kinetic energy of SCCDPS depends upon the system temperature (≡ 1/Г) and it is independent of higher screening parameter. Furthermore, it has shown that the presented HNEMD method has more reliable results than those obtained through earlier known numerical methods.

Molecular dynamics study of two dimensional and adsorbed microclusters

1980 ◽  
Vol 72 (8) ◽  
pp. 4562-4568 ◽  
Author(s):  
Mariana Weissmann ◽  
Norah V. Cohan
Keyword(s):  
Molecular Dynamics ◽  
Two Dimensional

Molecular Dynamics Simulations of Shock-Defect Interactions in Two-Dimensional Nonreactive Crystals

1992 ◽  
Vol 296 ◽  
Author(s):  
Robert S. Sinkovits ◽  
Lee Phillips ◽  
Elaine S. Oran ◽  
Jay P. Boris
Keyword(s):  
Molecular Dynamics ◽  
Hexagonal Lattice ◽  
Square Lattice ◽  
Two Dimensional ◽  
Connection Machine ◽  
Defect Sites ◽  
Principal Axes ◽  
Shock Motion ◽  
Defect Interactions ◽  
Dynamics Simulations

AbstractThe interactions of shocks with defects in two-dimensional square and hexagonal lattices of particles interacting through Lennard-Jones potentials are studied using molecular dynamics. In perfect lattices at zero temperature, shocks directed along one of the principal axes propagate through the crystal causing no permanent disruption. Vacancies, interstitials, and to a lesser degree, massive defects are all effective at converting directed shock motion into thermalized two-dimensional motion. Measures of lattice disruption quantitatively describe the effects of the different defects. The square lattice is unstable at nonzero temperatures, as shown by its tendency upon impact to reorganize into the lower-energy hexagonal state. This transition also occurs in the disordered region associated with the shock-defect interaction. The hexagonal lattice can be made arbitrarily stable even for shock-vacancy interactions through appropriate choice of potential parameters. In reactive crystals, these defect sites may be responsible for the onset of detonation. All calculations are performed using a program optimized for the massively parallel Connection Machine.

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