Molecular Dynamics (MD) simulations were performed to compute the mean-squared displacement (\(MSD\)), self-diffusivity constant (\(D\)), dynamic viscosity (\(\eta\)), isochoric heat capacity (\(Cv\)), and the thermal conductivity (\(k\)) of liquid Argon. To do this, we performed a sensitivity analysis by varying the number of Ar atoms (N) in the system (N = 128, 256, 512, 1024, and 2048), force field parameters obtained from three sources (Barker-Fisher-Watts, Rahman, and White), integration steps (dt = 0.5, 1, and 2 femtoseconds), and the method used to evaluate the atomic forces (a simple method that scales with \(~N^2\) and a Verlet lists method that scales with \(~N\). The sensitivity study consists of 90 simulations in total. The following page presents the results obtained in two large tables (Table 1 containing the results using the simple force evaluation method, and Table 2 containing the results obtained from using the Verlet lists method). The trajectories' files produced by Scymol are available for download in the Comments column of the tables.
Parameters | N | Time-step (\(ps\)) |
Temperature (\(K\)) |
MSD (\(Å^2\)) |
Diffusivity (\(Å^2/ps\)) |
Viscosity | Heat capacity (\(E/K/{atom}\)) |
Thermal conductivity |
Comments |
Barker-Fischer-Watts | 128 | 0.5 | xx | xx | xx | xx | xx | xx | cc |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
256 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
512 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
1024 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
2048 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
Rahman | 128 | 0.5 | xx | xx | xx | xx | xx | xx | cc |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
256 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
512 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
1024 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
2048 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
White | 128 | 0.5 | xx | xx | xx | xx | xx | xx | cc |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
256 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
512 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
1024 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc | ||
2048 | 0.5 | xx | xx | xx | xx | xx | xx | cc | |
1 | xx | xx | xx | xx | xx | xx | cc | ||
2 | xx | xx | xx | xx | xx | xx | cc |