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patch_5Oct
...
patch_12Oc
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@ -1,4 +1,4 @@
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LAMMPS (15 Feb 2016)
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LAMMPS (6 Oct 2016)
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# FENE beadspring benchmark
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units lj
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@ -43,25 +43,25 @@ Neighbor list info ...
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master list distance cutoff = 1.52
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ghost atom cutoff = 1.52
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binsize = 0.76 -> bins = 45 45 45
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Memory usage per processor = 11.5189 Mbytes
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Memory usage per processor = 12.0423 Mbytes
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Step Temp E_pair E_mol TotEng Press
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0 0.97029772 0.44484087 20.494523 22.394765 4.6721833
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100 0.9729966 0.4361122 20.507698 22.40326 4.6548819
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Loop time of 0.978585 on 1 procs for 100 steps with 32000 atoms
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Loop time of 0.977647 on 1 procs for 100 steps with 32000 atoms
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Performance: 105948.895 tau/day, 102.188 timesteps/s
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100.0% CPU use with 1 MPI tasks x no OpenMP threads
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Performance: 106050.541 tau/day, 102.286 timesteps/s
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99.9% CPU use with 1 MPI tasks x no OpenMP threads
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MPI task timing breakdown:
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Section | min time | avg time | max time |%varavg| %total
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---------------------------------------------------------------
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Pair | 0.19562 | 0.19562 | 0.19562 | 0.0 | 19.99
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Bond | 0.087475 | 0.087475 | 0.087475 | 0.0 | 8.94
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Neigh | 0.44861 | 0.44861 | 0.44861 | 0.0 | 45.84
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Comm | 0.032932 | 0.032932 | 0.032932 | 0.0 | 3.37
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Output | 0.00010395 | 0.00010395 | 0.00010395 | 0.0 | 0.01
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Modify | 0.19413 | 0.19413 | 0.19413 | 0.0 | 19.84
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Other | | 0.01972 | | | 2.02
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Pair | 0.19421 | 0.19421 | 0.19421 | 0.0 | 19.86
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Bond | 0.08741 | 0.08741 | 0.08741 | 0.0 | 8.94
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Neigh | 0.45791 | 0.45791 | 0.45791 | 0.0 | 46.84
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Comm | 0.032649 | 0.032649 | 0.032649 | 0.0 | 3.34
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Output | 0.00012207 | 0.00012207 | 0.00012207 | 0.0 | 0.01
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Modify | 0.18071 | 0.18071 | 0.18071 | 0.0 | 18.48
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Other | | 0.02464 | | | 2.52
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Nlocal: 32000 ave 32000 max 32000 min
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Histogram: 1 0 0 0 0 0 0 0 0 0
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@ -1,4 +1,4 @@
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LAMMPS (15 Feb 2016)
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LAMMPS (6 Oct 2016)
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# FENE beadspring benchmark
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units lj
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@ -43,25 +43,25 @@ Neighbor list info ...
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master list distance cutoff = 1.52
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ghost atom cutoff = 1.52
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binsize = 0.76 -> bins = 45 45 45
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Memory usage per processor = 3.91518 Mbytes
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Memory usage per processor = 4.14663 Mbytes
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Step Temp E_pair E_mol TotEng Press
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0 0.97029772 0.44484087 20.494523 22.394765 4.6721833
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100 0.97145835 0.43803883 20.502691 22.397872 4.626988
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Loop time of 0.271187 on 4 procs for 100 steps with 32000 atoms
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Loop time of 0.269205 on 4 procs for 100 steps with 32000 atoms
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Performance: 382319.453 tau/day, 368.749 timesteps/s
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99.6% CPU use with 4 MPI tasks x no OpenMP threads
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Performance: 385133.446 tau/day, 371.464 timesteps/s
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99.8% CPU use with 4 MPI tasks x no OpenMP threads
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MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
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---------------------------------------------------------------
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Pair | 0.048621 | 0.050076 | 0.051229 | 0.4 | 18.47
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Bond | 0.022254 | 0.022942 | 0.023567 | 0.3 | 8.46
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Neigh | 0.11873 | 0.11881 | 0.11887 | 0.0 | 43.81
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Comm | 0.019066 | 0.021357 | 0.024297 | 1.3 | 7.88
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Output | 5.0068e-05 | 5.5015e-05 | 6.1035e-05 | 0.1 | 0.02
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Modify | 0.048737 | 0.050198 | 0.051231 | 0.4 | 18.51
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Other | | 0.007751 | | | 2.86
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Pair | 0.049383 | 0.049756 | 0.049988 | 0.1 | 18.48
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Bond | 0.022701 | 0.022813 | 0.022872 | 0.0 | 8.47
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Neigh | 0.11982 | 0.12002 | 0.12018 | 0.0 | 44.58
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Comm | 0.020274 | 0.021077 | 0.022348 | 0.5 | 7.83
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Output | 5.3167e-05 | 5.6148e-05 | 6.3181e-05 | 0.1 | 0.02
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Modify | 0.046276 | 0.046809 | 0.047016 | 0.1 | 17.39
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Other | | 0.008669 | | | 3.22
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Nlocal: 8000 ave 8030 max 7974 min
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Histogram: 1 0 0 1 0 1 0 0 0 1
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@ -1,4 +1,4 @@
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LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
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# FENE beadspring benchmark
|
||||
|
||||
variable x index 1
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||||
@ -59,25 +59,25 @@ Neighbor list info ...
|
||||
master list distance cutoff = 1.52
|
||||
ghost atom cutoff = 1.52
|
||||
binsize = 0.76 -> bins = 89 89 45
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Memory usage per processor = 12.8735 Mbytes
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Memory usage per processor = 13.2993 Mbytes
|
||||
Step Temp E_pair E_mol TotEng Press
|
||||
0 0.97027498 0.44484087 20.494523 22.394765 4.6721833
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100 0.97682955 0.44239968 20.500229 22.407862 4.6527025
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Loop time of 1.20889 on 4 procs for 100 steps with 128000 atoms
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Loop time of 1.14845 on 4 procs for 100 steps with 128000 atoms
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||||
Performance: 85764.410 tau/day, 82.720 timesteps/s
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99.8% CPU use with 4 MPI tasks x no OpenMP threads
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||||
Performance: 90277.919 tau/day, 87.074 timesteps/s
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99.9% CPU use with 4 MPI tasks x no OpenMP threads
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||||
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MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
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||||
Pair | 0.21738 | 0.23306 | 0.23926 | 1.9 | 19.28
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Bond | 0.094536 | 0.10196 | 0.10534 | 1.4 | 8.43
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Neigh | 0.52311 | 0.52392 | 0.52519 | 0.1 | 43.34
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Comm | 0.090161 | 0.10022 | 0.12557 | 4.7 | 8.29
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Output | 0.00012207 | 0.00017327 | 0.00019598 | 0.2 | 0.01
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Modify | 0.19662 | 0.20262 | 0.20672 | 0.8 | 16.76
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Other | | 0.04694 | | | 3.88
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Pair | 0.2203 | 0.22207 | 0.22386 | 0.3 | 19.34
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Bond | 0.094861 | 0.095302 | 0.095988 | 0.1 | 8.30
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Neigh | 0.52127 | 0.5216 | 0.52189 | 0.0 | 45.42
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Comm | 0.079585 | 0.082159 | 0.084366 | 0.7 | 7.15
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Output | 0.00013304 | 0.00015306 | 0.00018501 | 0.2 | 0.01
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Modify | 0.18351 | 0.18419 | 0.1856 | 0.2 | 16.04
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Other | | 0.04298 | | | 3.74
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Nlocal: 32000 ave 32015 max 31983 min
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Histogram: 1 0 1 0 0 0 0 0 1 1
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@ -1,4 +1,4 @@
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LAMMPS (15 Feb 2016)
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LAMMPS (6 Oct 2016)
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# LAMMPS benchmark of granular flow
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# chute flow of 32000 atoms with frozen base at 26 degrees
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||||
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||||
@ -47,24 +47,24 @@ Neighbor list info ...
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master list distance cutoff = 1.1
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||||
ghost atom cutoff = 1.1
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||||
binsize = 0.55 -> bins = 73 37 68
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Memory usage per processor = 15.567 Mbytes
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||||
Step Atoms KinEng 1 Volume
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Memory usage per processor = 16.0904 Mbytes
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||||
Step Atoms KinEng c_1 Volume
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0 32000 784139.13 1601.1263 29833.783
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100 32000 784292.08 1571.0968 29834.707
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Loop time of 0.550482 on 1 procs for 100 steps with 32000 atoms
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Loop time of 0.534174 on 1 procs for 100 steps with 32000 atoms
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Performance: 1569.534 tau/day, 181.659 timesteps/s
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100.1% CPU use with 1 MPI tasks x no OpenMP threads
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||||
Performance: 1617.451 tau/day, 187.205 timesteps/s
|
||||
99.8% CPU use with 1 MPI tasks x no OpenMP threads
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||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
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||||
Pair | 0.33849 | 0.33849 | 0.33849 | 0.0 | 61.49
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Neigh | 0.040353 | 0.040353 | 0.040353 | 0.0 | 7.33
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Comm | 0.018023 | 0.018023 | 0.018023 | 0.0 | 3.27
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Output | 0.00020385 | 0.00020385 | 0.00020385 | 0.0 | 0.04
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Modify | 0.13155 | 0.13155 | 0.13155 | 0.0 | 23.90
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Other | | 0.02186 | | | 3.97
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Pair | 0.33346 | 0.33346 | 0.33346 | 0.0 | 62.43
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Neigh | 0.043902 | 0.043902 | 0.043902 | 0.0 | 8.22
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Comm | 0.018391 | 0.018391 | 0.018391 | 0.0 | 3.44
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Output | 0.00022411 | 0.00022411 | 0.00022411 | 0.0 | 0.04
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Modify | 0.11666 | 0.11666 | 0.11666 | 0.0 | 21.84
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Other | | 0.02153 | | | 4.03
|
||||
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Nlocal: 32000 ave 32000 max 32000 min
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Histogram: 1 0 0 0 0 0 0 0 0 0
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@ -1,4 +1,4 @@
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LAMMPS (15 Feb 2016)
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LAMMPS (6 Oct 2016)
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# LAMMPS benchmark of granular flow
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# chute flow of 32000 atoms with frozen base at 26 degrees
|
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@ -47,24 +47,24 @@ Neighbor list info ...
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master list distance cutoff = 1.1
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ghost atom cutoff = 1.1
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binsize = 0.55 -> bins = 73 37 68
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Memory usage per processor = 6.81783 Mbytes
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Step Atoms KinEng 1 Volume
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Memory usage per processor = 7.04927 Mbytes
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Step Atoms KinEng c_1 Volume
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0 32000 784139.13 1601.1263 29833.783
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100 32000 784292.08 1571.0968 29834.707
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Loop time of 0.13141 on 4 procs for 100 steps with 32000 atoms
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Loop time of 0.171815 on 4 procs for 100 steps with 32000 atoms
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Performance: 6574.833 tau/day, 760.976 timesteps/s
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99.3% CPU use with 4 MPI tasks x no OpenMP threads
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Performance: 5028.653 tau/day, 582.020 timesteps/s
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99.7% CPU use with 4 MPI tasks x no OpenMP threads
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MPI task timing breakdown:
|
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Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
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Pair | 0.062505 | 0.067 | 0.07152 | 1.5 | 50.99
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Neigh | 0.010041 | 0.0101 | 0.010178 | 0.1 | 7.69
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Comm | 0.012347 | 0.012895 | 0.013444 | 0.5 | 9.81
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Output | 6.3896e-05 | 0.00010294 | 0.00014091 | 0.3 | 0.08
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Modify | 0.031802 | 0.032348 | 0.032897 | 0.3 | 24.62
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Other | | 0.008965 | | | 6.82
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Pair | 0.093691 | 0.096898 | 0.10005 | 0.8 | 56.40
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Neigh | 0.011976 | 0.012059 | 0.012146 | 0.1 | 7.02
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Comm | 0.016384 | 0.017418 | 0.018465 | 0.8 | 10.14
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Output | 7.7963e-05 | 0.00010747 | 0.00013304 | 0.2 | 0.06
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Modify | 0.031744 | 0.031943 | 0.032167 | 0.1 | 18.59
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Other | | 0.01339 | | | 7.79
|
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Nlocal: 8000 ave 8008 max 7992 min
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Histogram: 2 0 0 0 0 0 0 0 0 2
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@ -1,4 +1,4 @@
|
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LAMMPS (15 Feb 2016)
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LAMMPS (6 Oct 2016)
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# LAMMPS benchmark of granular flow
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# chute flow of 32000 atoms with frozen base at 26 degrees
|
||||
|
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@ -57,24 +57,24 @@ Neighbor list info ...
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master list distance cutoff = 1.1
|
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ghost atom cutoff = 1.1
|
||||
binsize = 0.55 -> bins = 146 73 68
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Memory usage per processor = 15.7007 Mbytes
|
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Step Atoms KinEng 1 Volume
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Memory usage per processor = 16.1265 Mbytes
|
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Step Atoms KinEng c_1 Volume
|
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0 128000 3136556.5 6404.5051 119335.13
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100 128000 3137168.3 6284.3873 119338.83
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Loop time of 0.906913 on 4 procs for 100 steps with 128000 atoms
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Loop time of 0.832365 on 4 procs for 100 steps with 128000 atoms
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Performance: 952.683 tau/day, 110.264 timesteps/s
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99.7% CPU use with 4 MPI tasks x no OpenMP threads
|
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Performance: 1038.006 tau/day, 120.140 timesteps/s
|
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99.8% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
|
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MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 0.51454 | 0.53094 | 0.55381 | 2.0 | 58.54
|
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Neigh | 0.042597 | 0.043726 | 0.045801 | 0.6 | 4.82
|
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Comm | 0.063027 | 0.064657 | 0.067367 | 0.7 | 7.13
|
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Output | 0.00024891 | 0.00059718 | 0.00086498 | 1.0 | 0.07
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Modify | 0.16508 | 0.17656 | 0.1925 | 2.6 | 19.47
|
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Other | | 0.09043 | | | 9.97
|
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Pair | 0.5178 | 0.52208 | 0.52793 | 0.5 | 62.72
|
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Neigh | 0.047003 | 0.047113 | 0.047224 | 0.0 | 5.66
|
||||
Comm | 0.05233 | 0.052988 | 0.053722 | 0.2 | 6.37
|
||||
Output | 0.00024986 | 0.00032717 | 0.00036693 | 0.3 | 0.04
|
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Modify | 0.15517 | 0.15627 | 0.15808 | 0.3 | 18.77
|
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Other | | 0.0536 | | | 6.44
|
||||
|
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Nlocal: 32000 ave 32000 max 32000 min
|
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Histogram: 4 0 0 0 0 0 0 0 0 0
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@ -87,4 +87,4 @@ Total # of neighbors = 460532
|
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Ave neighs/atom = 3.59791
|
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Neighbor list builds = 2
|
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Dangerous builds = 0
|
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Total wall time: 0:00:01
|
||||
Total wall time: 0:00:00
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# bulk Cu lattice
|
||||
|
||||
variable x index 1
|
||||
@ -49,25 +49,25 @@ Neighbor list info ...
|
||||
master list distance cutoff = 5.95
|
||||
ghost atom cutoff = 5.95
|
||||
binsize = 2.975 -> bins = 25 25 25
|
||||
Memory usage per processor = 10.2238 Mbytes
|
||||
Memory usage per processor = 11.2238 Mbytes
|
||||
Step Temp E_pair E_mol TotEng Press
|
||||
0 1600 -113280 0 -106662.09 18703.573
|
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50 781.69049 -109873.35 0 -106640.13 52273.088
|
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100 801.832 -109957.3 0 -106640.77 51322.821
|
||||
Loop time of 5.90097 on 1 procs for 100 steps with 32000 atoms
|
||||
Loop time of 5.96529 on 1 procs for 100 steps with 32000 atoms
|
||||
|
||||
Performance: 7.321 ns/day, 3.278 hours/ns, 16.946 timesteps/s
|
||||
Performance: 7.242 ns/day, 3.314 hours/ns, 16.764 timesteps/s
|
||||
99.9% CPU use with 1 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 5.2121 | 5.2121 | 5.2121 | 0.0 | 88.33
|
||||
Neigh | 0.58212 | 0.58212 | 0.58212 | 0.0 | 9.86
|
||||
Comm | 0.030392 | 0.030392 | 0.030392 | 0.0 | 0.52
|
||||
Output | 0.00023389 | 0.00023389 | 0.00023389 | 0.0 | 0.00
|
||||
Modify | 0.060871 | 0.060871 | 0.060871 | 0.0 | 1.03
|
||||
Other | | 0.01527 | | | 0.26
|
||||
Pair | 5.2743 | 5.2743 | 5.2743 | 0.0 | 88.42
|
||||
Neigh | 0.59212 | 0.59212 | 0.59212 | 0.0 | 9.93
|
||||
Comm | 0.030399 | 0.030399 | 0.030399 | 0.0 | 0.51
|
||||
Output | 0.00026202 | 0.00026202 | 0.00026202 | 0.0 | 0.00
|
||||
Modify | 0.050487 | 0.050487 | 0.050487 | 0.0 | 0.85
|
||||
Other | | 0.01776 | | | 0.30
|
||||
|
||||
Nlocal: 32000 ave 32000 max 32000 min
|
||||
Histogram: 1 0 0 0 0 0 0 0 0 0
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# bulk Cu lattice
|
||||
|
||||
variable x index 1
|
||||
@ -49,25 +49,25 @@ Neighbor list info ...
|
||||
master list distance cutoff = 5.95
|
||||
ghost atom cutoff = 5.95
|
||||
binsize = 2.975 -> bins = 25 25 25
|
||||
Memory usage per processor = 5.09629 Mbytes
|
||||
Memory usage per processor = 5.59629 Mbytes
|
||||
Step Temp E_pair E_mol TotEng Press
|
||||
0 1600 -113280 0 -106662.09 18703.573
|
||||
50 781.69049 -109873.35 0 -106640.13 52273.088
|
||||
100 801.832 -109957.3 0 -106640.77 51322.821
|
||||
Loop time of 1.58019 on 4 procs for 100 steps with 32000 atoms
|
||||
Loop time of 1.64562 on 4 procs for 100 steps with 32000 atoms
|
||||
|
||||
Performance: 27.338 ns/day, 0.878 hours/ns, 63.284 timesteps/s
|
||||
Performance: 26.252 ns/day, 0.914 hours/ns, 60.767 timesteps/s
|
||||
99.8% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 1.3617 | 1.366 | 1.3723 | 0.4 | 86.45
|
||||
Neigh | 0.15123 | 0.15232 | 0.15374 | 0.2 | 9.64
|
||||
Comm | 0.033429 | 0.041275 | 0.047066 | 2.7 | 2.61
|
||||
Output | 0.00011301 | 0.0001573 | 0.000211 | 0.3 | 0.01
|
||||
Modify | 0.014694 | 0.015085 | 0.015421 | 0.2 | 0.95
|
||||
Other | | 0.005342 | | | 0.34
|
||||
Pair | 1.408 | 1.4175 | 1.4341 | 0.9 | 86.14
|
||||
Neigh | 0.15512 | 0.15722 | 0.16112 | 0.6 | 9.55
|
||||
Comm | 0.029105 | 0.049986 | 0.061822 | 5.8 | 3.04
|
||||
Output | 0.00010991 | 0.00011539 | 0.00012302 | 0.0 | 0.01
|
||||
Modify | 0.013383 | 0.013573 | 0.013883 | 0.2 | 0.82
|
||||
Other | | 0.007264 | | | 0.44
|
||||
|
||||
Nlocal: 8000 ave 8008 max 7993 min
|
||||
Histogram: 2 0 0 0 0 0 0 0 1 1
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# bulk Cu lattice
|
||||
|
||||
variable x index 1
|
||||
@ -49,25 +49,25 @@ Neighbor list info ...
|
||||
master list distance cutoff = 5.95
|
||||
ghost atom cutoff = 5.95
|
||||
binsize = 2.975 -> bins = 49 49 25
|
||||
Memory usage per processor = 10.1402 Mbytes
|
||||
Memory usage per processor = 11.1402 Mbytes
|
||||
Step Temp E_pair E_mol TotEng Press
|
||||
0 1600 -453120 0 -426647.73 18704.012
|
||||
50 779.50001 -439457.02 0 -426560.06 52355.276
|
||||
100 797.97828 -439764.76 0 -426562.07 51474.74
|
||||
Loop time of 6.46849 on 4 procs for 100 steps with 128000 atoms
|
||||
Loop time of 6.60121 on 4 procs for 100 steps with 128000 atoms
|
||||
|
||||
Performance: 6.679 ns/day, 3.594 hours/ns, 15.460 timesteps/s
|
||||
Performance: 6.544 ns/day, 3.667 hours/ns, 15.149 timesteps/s
|
||||
99.9% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 5.581 | 5.5997 | 5.6265 | 0.8 | 86.57
|
||||
Neigh | 0.65287 | 0.658 | 0.66374 | 0.5 | 10.17
|
||||
Comm | 0.075706 | 0.11015 | 0.13655 | 7.2 | 1.70
|
||||
Output | 0.00026488 | 0.00028312 | 0.00029302 | 0.1 | 0.00
|
||||
Modify | 0.069607 | 0.072407 | 0.074555 | 0.7 | 1.12
|
||||
Other | | 0.02794 | | | 0.43
|
||||
Pair | 5.6676 | 5.7011 | 5.7469 | 1.3 | 86.36
|
||||
Neigh | 0.66423 | 0.67119 | 0.68082 | 0.7 | 10.17
|
||||
Comm | 0.079367 | 0.13668 | 0.1791 | 10.5 | 2.07
|
||||
Output | 0.00026989 | 0.00028622 | 0.00031209 | 0.1 | 0.00
|
||||
Modify | 0.060046 | 0.062203 | 0.065009 | 0.9 | 0.94
|
||||
Other | | 0.02974 | | | 0.45
|
||||
|
||||
Nlocal: 32000 ave 32092 max 31914 min
|
||||
Histogram: 1 0 0 1 0 1 0 0 0 1
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# 3d Lennard-Jones melt
|
||||
|
||||
variable x index 1
|
||||
@ -50,20 +50,20 @@ Memory usage per processor = 8.21387 Mbytes
|
||||
Step Temp E_pair E_mol TotEng Press
|
||||
0 1.44 -6.7733681 0 -4.6134356 -5.0197073
|
||||
100 0.7574531 -5.7585055 0 -4.6223613 0.20726105
|
||||
Loop time of 2.26309 on 1 procs for 100 steps with 32000 atoms
|
||||
Loop time of 2.26185 on 1 procs for 100 steps with 32000 atoms
|
||||
|
||||
Performance: 19088.920 tau/day, 44.187 timesteps/s
|
||||
Performance: 19099.377 tau/day, 44.212 timesteps/s
|
||||
99.9% CPU use with 1 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 1.9341 | 1.9341 | 1.9341 | 0.0 | 85.46
|
||||
Neigh | 0.2442 | 0.2442 | 0.2442 | 0.0 | 10.79
|
||||
Comm | 0.024158 | 0.024158 | 0.024158 | 0.0 | 1.07
|
||||
Output | 0.00011611 | 0.00011611 | 0.00011611 | 0.0 | 0.01
|
||||
Modify | 0.053222 | 0.053222 | 0.053222 | 0.0 | 2.35
|
||||
Other | | 0.007258 | | | 0.32
|
||||
Pair | 1.9328 | 1.9328 | 1.9328 | 0.0 | 85.45
|
||||
Neigh | 0.2558 | 0.2558 | 0.2558 | 0.0 | 11.31
|
||||
Comm | 0.024061 | 0.024061 | 0.024061 | 0.0 | 1.06
|
||||
Output | 0.00012612 | 0.00012612 | 0.00012612 | 0.0 | 0.01
|
||||
Modify | 0.040887 | 0.040887 | 0.040887 | 0.0 | 1.81
|
||||
Other | | 0.008214 | | | 0.36
|
||||
|
||||
Nlocal: 32000 ave 32000 max 32000 min
|
||||
Histogram: 1 0 0 0 0 0 0 0 0 0
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# 3d Lennard-Jones melt
|
||||
|
||||
variable x index 1
|
||||
@ -50,20 +50,20 @@ Memory usage per processor = 4.09506 Mbytes
|
||||
Step Temp E_pair E_mol TotEng Press
|
||||
0 1.44 -6.7733681 0 -4.6134356 -5.0197073
|
||||
100 0.7574531 -5.7585055 0 -4.6223613 0.20726105
|
||||
Loop time of 0.640733 on 4 procs for 100 steps with 32000 atoms
|
||||
Loop time of 0.635957 on 4 procs for 100 steps with 32000 atoms
|
||||
|
||||
Performance: 67422.779 tau/day, 156.071 timesteps/s
|
||||
99.7% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
Performance: 67929.172 tau/day, 157.243 timesteps/s
|
||||
99.9% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 0.49487 | 0.51733 | 0.5322 | 1.9 | 80.74
|
||||
Neigh | 0.061131 | 0.063685 | 0.065433 | 0.6 | 9.94
|
||||
Comm | 0.02457 | 0.042349 | 0.069598 | 8.1 | 6.61
|
||||
Output | 5.9843e-05 | 6.3181e-05 | 6.6996e-05 | 0.0 | 0.01
|
||||
Modify | 0.012961 | 0.013863 | 0.014491 | 0.5 | 2.16
|
||||
Other | | 0.003448 | | | 0.54
|
||||
Pair | 0.51335 | 0.51822 | 0.52569 | 0.7 | 81.49
|
||||
Neigh | 0.063695 | 0.064309 | 0.065397 | 0.3 | 10.11
|
||||
Comm | 0.027525 | 0.03629 | 0.041959 | 3.1 | 5.71
|
||||
Output | 6.3896e-05 | 6.6698e-05 | 7.081e-05 | 0.0 | 0.01
|
||||
Modify | 0.012472 | 0.01254 | 0.012618 | 0.1 | 1.97
|
||||
Other | | 0.004529 | | | 0.71
|
||||
|
||||
Nlocal: 8000 ave 8037 max 7964 min
|
||||
Histogram: 2 0 0 0 0 0 0 0 1 1
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# 3d Lennard-Jones melt
|
||||
|
||||
variable x index 1
|
||||
@ -50,20 +50,20 @@ Memory usage per processor = 8.13678 Mbytes
|
||||
Step Temp E_pair E_mol TotEng Press
|
||||
0 1.44 -6.7733681 0 -4.6133849 -5.0196788
|
||||
100 0.75841891 -5.759957 0 -4.6223375 0.20008866
|
||||
Loop time of 2.57914 on 4 procs for 100 steps with 128000 atoms
|
||||
Loop time of 2.55762 on 4 procs for 100 steps with 128000 atoms
|
||||
|
||||
Performance: 16749.768 tau/day, 38.773 timesteps/s
|
||||
Performance: 16890.677 tau/day, 39.099 timesteps/s
|
||||
99.8% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 2.042 | 2.1092 | 2.1668 | 3.1 | 81.78
|
||||
Neigh | 0.23982 | 0.24551 | 0.25233 | 1.0 | 9.52
|
||||
Comm | 0.067088 | 0.13887 | 0.22681 | 15.7 | 5.38
|
||||
Output | 0.00013185 | 0.00021666 | 0.00027108 | 0.4 | 0.01
|
||||
Modify | 0.060348 | 0.071269 | 0.077063 | 2.5 | 2.76
|
||||
Other | | 0.01403 | | | 0.54
|
||||
Pair | 2.0583 | 2.0988 | 2.1594 | 2.6 | 82.06
|
||||
Neigh | 0.24411 | 0.24838 | 0.25585 | 0.9 | 9.71
|
||||
Comm | 0.066397 | 0.13872 | 0.1863 | 11.9 | 5.42
|
||||
Output | 0.00012994 | 0.00021023 | 0.00025702 | 0.3 | 0.01
|
||||
Modify | 0.055533 | 0.058343 | 0.061791 | 1.2 | 2.28
|
||||
Other | | 0.0132 | | | 0.52
|
||||
|
||||
Nlocal: 32000 ave 32060 max 31939 min
|
||||
Histogram: 1 0 1 0 0 0 0 1 0 1
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# Rhodopsin model
|
||||
|
||||
units real
|
||||
@ -56,6 +56,7 @@ timestep 2.0
|
||||
|
||||
run 100
|
||||
PPPM initialization ...
|
||||
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:316)
|
||||
G vector (1/distance) = 0.248835
|
||||
grid = 25 32 32
|
||||
stencil order = 5
|
||||
@ -70,41 +71,41 @@ Neighbor list info ...
|
||||
master list distance cutoff = 12
|
||||
ghost atom cutoff = 12
|
||||
binsize = 6 -> bins = 10 13 13
|
||||
Memory usage per processor = 91.7487 Mbytes
|
||||
Memory usage per processor = 93.2721 Mbytes
|
||||
---------------- Step 0 ----- CPU = 0.0000 (sec) ----------------
|
||||
TotEng = -25356.2064 KinEng = 21444.8313 Temp = 299.0397
|
||||
PotEng = -46801.0377 E_bond = 2537.9940 E_angle = 10921.3742
|
||||
E_dihed = 5211.7865 E_impro = 213.5116 E_vdwl = -2307.8634
|
||||
E_coul = 207025.8927 E_long = -270403.7333 Press = -142.6035
|
||||
E_coul = 207025.8927 E_long = -270403.7333 Press = -149.3301
|
||||
Volume = 307995.0335
|
||||
---------------- Step 50 ----- CPU = 17.6362 (sec) ----------------
|
||||
TotEng = -25330.0828 KinEng = 21501.0029 Temp = 299.8230
|
||||
PotEng = -46831.0857 E_bond = 2471.7004 E_angle = 10836.4975
|
||||
E_dihed = 5239.6299 E_impro = 227.1218 E_vdwl = -1993.2754
|
||||
E_coul = 206797.6331 E_long = -270410.3930 Press = 237.6701
|
||||
Volume = 308031.5639
|
||||
---------------- Step 100 ----- CPU = 35.9089 (sec) ----------------
|
||||
TotEng = -25290.7593 KinEng = 21592.0117 Temp = 301.0920
|
||||
PotEng = -46882.7709 E_bond = 2567.9807 E_angle = 10781.9408
|
||||
E_dihed = 5198.7432 E_impro = 216.7834 E_vdwl = -1902.4783
|
||||
E_coul = 206659.2326 E_long = -270404.9733 Press = 6.9960
|
||||
Volume = 308133.9888
|
||||
Loop time of 35.9089 on 1 procs for 100 steps with 32000 atoms
|
||||
---------------- Step 50 ----- CPU = 17.2007 (sec) ----------------
|
||||
TotEng = -25330.0321 KinEng = 21501.0036 Temp = 299.8230
|
||||
PotEng = -46831.0357 E_bond = 2471.7033 E_angle = 10836.5108
|
||||
E_dihed = 5239.6316 E_impro = 227.1219 E_vdwl = -1993.2763
|
||||
E_coul = 206797.6655 E_long = -270410.3927 Press = 237.6866
|
||||
Volume = 308031.5640
|
||||
---------------- Step 100 ----- CPU = 35.0315 (sec) ----------------
|
||||
TotEng = -25290.7387 KinEng = 21591.9096 Temp = 301.0906
|
||||
PotEng = -46882.6484 E_bond = 2567.9789 E_angle = 10781.9556
|
||||
E_dihed = 5198.7493 E_impro = 216.7863 E_vdwl = -1902.6458
|
||||
E_coul = 206659.5006 E_long = -270404.9733 Press = 6.7898
|
||||
Volume = 308133.9933
|
||||
Loop time of 35.0316 on 1 procs for 100 steps with 32000 atoms
|
||||
|
||||
Performance: 0.481 ns/day, 49.874 hours/ns, 2.785 timesteps/s
|
||||
Performance: 0.493 ns/day, 48.655 hours/ns, 2.855 timesteps/s
|
||||
99.9% CPU use with 1 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 25.731 | 25.731 | 25.731 | 0.0 | 71.66
|
||||
Bond | 1.2771 | 1.2771 | 1.2771 | 0.0 | 3.56
|
||||
Kspace | 3.2094 | 3.2094 | 3.2094 | 0.0 | 8.94
|
||||
Neigh | 4.4538 | 4.4538 | 4.4538 | 0.0 | 12.40
|
||||
Comm | 0.068507 | 0.068507 | 0.068507 | 0.0 | 0.19
|
||||
Output | 0.00025916 | 0.00025916 | 0.00025916 | 0.0 | 0.00
|
||||
Modify | 1.1417 | 1.1417 | 1.1417 | 0.0 | 3.18
|
||||
Other | | 0.027 | | | 0.08
|
||||
Pair | 25.021 | 25.021 | 25.021 | 0.0 | 71.42
|
||||
Bond | 1.2834 | 1.2834 | 1.2834 | 0.0 | 3.66
|
||||
Kspace | 3.2116 | 3.2116 | 3.2116 | 0.0 | 9.17
|
||||
Neigh | 4.2767 | 4.2767 | 4.2767 | 0.0 | 12.21
|
||||
Comm | 0.069283 | 0.069283 | 0.069283 | 0.0 | 0.20
|
||||
Output | 0.00028205 | 0.00028205 | 0.00028205 | 0.0 | 0.00
|
||||
Modify | 1.14 | 1.14 | 1.14 | 0.0 | 3.25
|
||||
Other | | 0.02938 | | | 0.08
|
||||
|
||||
Nlocal: 32000 ave 32000 max 32000 min
|
||||
Histogram: 1 0 0 0 0 0 0 0 0 0
|
||||
@ -113,9 +114,9 @@ Histogram: 1 0 0 0 0 0 0 0 0 0
|
||||
Neighs: 1.20281e+07 ave 1.20281e+07 max 1.20281e+07 min
|
||||
Histogram: 1 0 0 0 0 0 0 0 0 0
|
||||
|
||||
Total # of neighbors = 12028107
|
||||
Total # of neighbors = 12028098
|
||||
Ave neighs/atom = 375.878
|
||||
Ave special neighs/atom = 7.43187
|
||||
Neighbor list builds = 11
|
||||
Dangerous builds = 0
|
||||
Total wall time: 0:00:37
|
||||
Total wall time: 0:00:36
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# Rhodopsin model
|
||||
|
||||
units real
|
||||
@ -56,6 +56,7 @@ timestep 2.0
|
||||
|
||||
run 100
|
||||
PPPM initialization ...
|
||||
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:316)
|
||||
G vector (1/distance) = 0.248835
|
||||
grid = 25 32 32
|
||||
stencil order = 5
|
||||
@ -70,52 +71,52 @@ Neighbor list info ...
|
||||
master list distance cutoff = 12
|
||||
ghost atom cutoff = 12
|
||||
binsize = 6 -> bins = 10 13 13
|
||||
Memory usage per processor = 36.629 Mbytes
|
||||
Memory usage per processor = 37.3604 Mbytes
|
||||
---------------- Step 0 ----- CPU = 0.0000 (sec) ----------------
|
||||
TotEng = -25356.2064 KinEng = 21444.8313 Temp = 299.0397
|
||||
PotEng = -46801.0377 E_bond = 2537.9940 E_angle = 10921.3742
|
||||
E_dihed = 5211.7865 E_impro = 213.5116 E_vdwl = -2307.8634
|
||||
E_coul = 207025.8927 E_long = -270403.7333 Press = -142.6035
|
||||
E_coul = 207025.8927 E_long = -270403.7333 Press = -149.3301
|
||||
Volume = 307995.0335
|
||||
---------------- Step 50 ----- CPU = 4.7461 (sec) ----------------
|
||||
TotEng = -25330.0828 KinEng = 21501.0029 Temp = 299.8230
|
||||
PotEng = -46831.0857 E_bond = 2471.7004 E_angle = 10836.4975
|
||||
E_dihed = 5239.6299 E_impro = 227.1218 E_vdwl = -1993.2754
|
||||
E_coul = 206797.6331 E_long = -270410.3930 Press = 237.6701
|
||||
Volume = 308031.5639
|
||||
---------------- Step 100 ----- CPU = 9.6332 (sec) ----------------
|
||||
TotEng = -25290.7591 KinEng = 21592.0117 Temp = 301.0920
|
||||
PotEng = -46882.7708 E_bond = 2567.9807 E_angle = 10781.9408
|
||||
E_dihed = 5198.7432 E_impro = 216.7834 E_vdwl = -1902.4783
|
||||
E_coul = 206659.2327 E_long = -270404.9733 Press = 6.9960
|
||||
Volume = 308133.9888
|
||||
Loop time of 9.63322 on 4 procs for 100 steps with 32000 atoms
|
||||
---------------- Step 50 ----- CPU = 4.6056 (sec) ----------------
|
||||
TotEng = -25330.0321 KinEng = 21501.0036 Temp = 299.8230
|
||||
PotEng = -46831.0357 E_bond = 2471.7033 E_angle = 10836.5108
|
||||
E_dihed = 5239.6316 E_impro = 227.1219 E_vdwl = -1993.2763
|
||||
E_coul = 206797.6655 E_long = -270410.3927 Press = 237.6866
|
||||
Volume = 308031.5640
|
||||
---------------- Step 100 ----- CPU = 9.3910 (sec) ----------------
|
||||
TotEng = -25290.7386 KinEng = 21591.9096 Temp = 301.0906
|
||||
PotEng = -46882.6482 E_bond = 2567.9789 E_angle = 10781.9556
|
||||
E_dihed = 5198.7493 E_impro = 216.7863 E_vdwl = -1902.6458
|
||||
E_coul = 206659.5007 E_long = -270404.9733 Press = 6.7898
|
||||
Volume = 308133.9933
|
||||
Loop time of 9.39107 on 4 procs for 100 steps with 32000 atoms
|
||||
|
||||
Performance: 1.794 ns/day, 13.379 hours/ns, 10.381 timesteps/s
|
||||
99.9% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
Performance: 1.840 ns/day, 13.043 hours/ns, 10.648 timesteps/s
|
||||
99.8% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 6.4364 | 6.5993 | 6.7208 | 4.7 | 68.51
|
||||
Bond | 0.30755 | 0.32435 | 0.35704 | 3.4 | 3.37
|
||||
Kspace | 0.92248 | 1.0782 | 1.2597 | 13.0 | 11.19
|
||||
Neigh | 1.1669 | 1.1672 | 1.1675 | 0.0 | 12.12
|
||||
Comm | 0.094674 | 0.098065 | 0.10543 | 1.4 | 1.02
|
||||
Output | 0.00015521 | 0.00016224 | 0.00018215 | 0.1 | 0.00
|
||||
Modify | 0.32982 | 0.34654 | 0.35365 | 1.6 | 3.60
|
||||
Other | | 0.01943 | | | 0.20
|
||||
Pair | 6.2189 | 6.3266 | 6.6072 | 6.5 | 67.37
|
||||
Bond | 0.30793 | 0.32122 | 0.3414 | 2.4 | 3.42
|
||||
Kspace | 0.87994 | 1.1644 | 1.2855 | 15.3 | 12.40
|
||||
Neigh | 1.1358 | 1.136 | 1.1362 | 0.0 | 12.10
|
||||
Comm | 0.08292 | 0.084935 | 0.087077 | 0.5 | 0.90
|
||||
Output | 0.00015712 | 0.00016558 | 0.00018501 | 0.1 | 0.00
|
||||
Modify | 0.33717 | 0.34246 | 0.34794 | 0.7 | 3.65
|
||||
Other | | 0.01526 | | | 0.16
|
||||
|
||||
Nlocal: 8000 ave 8143 max 7933 min
|
||||
Histogram: 1 2 0 0 0 0 0 0 0 1
|
||||
Nghost: 22733.5 ave 22769 max 22693 min
|
||||
Histogram: 1 0 0 0 0 2 0 0 0 1
|
||||
Neighs: 3.00703e+06 ave 3.0975e+06 max 2.96493e+06 min
|
||||
Neighs: 3.00702e+06 ave 3.0975e+06 max 2.96492e+06 min
|
||||
Histogram: 1 2 0 0 0 0 0 0 0 1
|
||||
|
||||
Total # of neighbors = 12028107
|
||||
Total # of neighbors = 12028098
|
||||
Ave neighs/atom = 375.878
|
||||
Ave special neighs/atom = 7.43187
|
||||
Neighbor list builds = 11
|
||||
Dangerous builds = 0
|
||||
Total wall time: 0:00:10
|
||||
Total wall time: 0:00:09
|
||||
@ -1,4 +1,4 @@
|
||||
LAMMPS (15 Feb 2016)
|
||||
LAMMPS (6 Oct 2016)
|
||||
# Rhodopsin model
|
||||
|
||||
variable x index 1
|
||||
@ -77,6 +77,7 @@ timestep 2.0
|
||||
|
||||
run 100
|
||||
PPPM initialization ...
|
||||
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:316)
|
||||
G vector (1/distance) = 0.248593
|
||||
grid = 48 60 36
|
||||
stencil order = 5
|
||||
@ -91,52 +92,52 @@ Neighbor list info ...
|
||||
master list distance cutoff = 12
|
||||
ghost atom cutoff = 12
|
||||
binsize = 6 -> bins = 19 26 13
|
||||
Memory usage per processor = 95.5339 Mbytes
|
||||
Memory usage per processor = 96.9597 Mbytes
|
||||
---------------- Step 0 ----- CPU = 0.0000 (sec) ----------------
|
||||
TotEng = -101425.4887 KinEng = 85779.3251 Temp = 299.0304
|
||||
PotEng = -187204.8138 E_bond = 10151.9760 E_angle = 43685.4968
|
||||
E_dihed = 20847.1460 E_impro = 854.0463 E_vdwl = -9231.4537
|
||||
E_coul = 827053.5824 E_long = -1080565.6077 Press = -142.3092
|
||||
E_coul = 827053.5824 E_long = -1080565.6077 Press = -149.0358
|
||||
Volume = 1231980.1340
|
||||
---------------- Step 50 ----- CPU = 18.7806 (sec) ----------------
|
||||
TotEng = -101320.2677 KinEng = 86003.4837 Temp = 299.8118
|
||||
PotEng = -187323.7514 E_bond = 9887.1072 E_angle = 43346.7922
|
||||
E_dihed = 20958.7032 E_impro = 908.4715 E_vdwl = -7973.4457
|
||||
E_coul = 826141.3831 E_long = -1080592.7629 Press = 238.0161
|
||||
Volume = 1232126.1855
|
||||
---------------- Step 100 ----- CPU = 38.3684 (sec) ----------------
|
||||
TotEng = -101158.1849 KinEng = 86355.6149 Temp = 301.0393
|
||||
PotEng = -187513.7998 E_bond = 10272.0693 E_angle = 43128.6454
|
||||
E_dihed = 20793.9759 E_impro = 867.0826 E_vdwl = -7586.7186
|
||||
E_coul = 825583.7122 E_long = -1080572.5667 Press = 15.2151
|
||||
Volume = 1232535.8423
|
||||
Loop time of 38.3684 on 4 procs for 100 steps with 128000 atoms
|
||||
---------------- Step 50 ----- CPU = 18.1689 (sec) ----------------
|
||||
TotEng = -101320.0211 KinEng = 86003.4933 Temp = 299.8118
|
||||
PotEng = -187323.5144 E_bond = 9887.1189 E_angle = 43346.8448
|
||||
E_dihed = 20958.7108 E_impro = 908.4721 E_vdwl = -7973.4486
|
||||
E_coul = 826141.5493 E_long = -1080592.7617 Press = 238.0404
|
||||
Volume = 1232126.1814
|
||||
---------------- Step 100 ----- CPU = 37.2027 (sec) ----------------
|
||||
TotEng = -101157.9546 KinEng = 86355.7413 Temp = 301.0398
|
||||
PotEng = -187513.6959 E_bond = 10272.0456 E_angle = 43128.7018
|
||||
E_dihed = 20794.0107 E_impro = 867.0928 E_vdwl = -7587.2409
|
||||
E_coul = 825584.2416 E_long = -1080572.5474 Press = 15.1729
|
||||
Volume = 1232535.8440
|
||||
Loop time of 37.2028 on 4 procs for 100 steps with 128000 atoms
|
||||
|
||||
Performance: 0.450 ns/day, 53.289 hours/ns, 2.606 timesteps/s
|
||||
Performance: 0.464 ns/day, 51.671 hours/ns, 2.688 timesteps/s
|
||||
99.9% CPU use with 4 MPI tasks x no OpenMP threads
|
||||
|
||||
MPI task timing breakdown:
|
||||
Section | min time | avg time | max time |%varavg| %total
|
||||
---------------------------------------------------------------
|
||||
Pair | 26.205 | 26.538 | 26.911 | 5.0 | 69.17
|
||||
Bond | 1.298 | 1.3125 | 1.3277 | 1.0 | 3.42
|
||||
Kspace | 3.7099 | 4.0992 | 4.4422 | 13.3 | 10.68
|
||||
Neigh | 4.6137 | 4.6144 | 4.615 | 0.0 | 12.03
|
||||
Comm | 0.21398 | 0.21992 | 0.22886 | 1.2 | 0.57
|
||||
Output | 0.00030518 | 0.00031543 | 0.00033307 | 0.1 | 0.00
|
||||
Modify | 1.5066 | 1.5232 | 1.5388 | 1.0 | 3.97
|
||||
Other | | 0.06051 | | | 0.16
|
||||
Pair | 25.431 | 25.738 | 25.984 | 4.0 | 69.18
|
||||
Bond | 1.2966 | 1.3131 | 1.3226 | 0.9 | 3.53
|
||||
Kspace | 3.7563 | 4.0123 | 4.3127 | 10.0 | 10.79
|
||||
Neigh | 4.3778 | 4.378 | 4.3782 | 0.0 | 11.77
|
||||
Comm | 0.1903 | 0.19549 | 0.20485 | 1.3 | 0.53
|
||||
Output | 0.00031805 | 0.00037521 | 0.00039601 | 0.2 | 0.00
|
||||
Modify | 1.4861 | 1.5051 | 1.5122 | 0.9 | 4.05
|
||||
Other | | 0.05992 | | | 0.16
|
||||
|
||||
Nlocal: 32000 ave 32000 max 32000 min
|
||||
Histogram: 4 0 0 0 0 0 0 0 0 0
|
||||
Nghost: 47957 ave 47957 max 47957 min
|
||||
Histogram: 4 0 0 0 0 0 0 0 0 0
|
||||
Neighs: 1.20281e+07 ave 1.20572e+07 max 1.1999e+07 min
|
||||
Neighs: 1.20281e+07 ave 1.20572e+07 max 1.19991e+07 min
|
||||
Histogram: 2 0 0 0 0 0 0 0 0 2
|
||||
|
||||
Total # of neighbors = 48112472
|
||||
Total # of neighbors = 48112540
|
||||
Ave neighs/atom = 375.879
|
||||
Ave special neighs/atom = 7.43187
|
||||
Neighbor list builds = 11
|
||||
Dangerous builds = 0
|
||||
Total wall time: 0:00:39
|
||||
Total wall time: 0:00:38
|
||||
|
Before Width: | Height: | Size: 1.6 KiB |
@ -1,9 +0,0 @@
|
||||
\documentclass[12pt]{article}
|
||||
\pagestyle{empty}
|
||||
\begin{document}
|
||||
|
||||
$$
|
||||
F^C = A \omega_{ij} \qquad \qquad r_{ij} < r_c
|
||||
$$
|
||||
|
||||
\end{document}
|
||||
BIN
doc/src/Eqs/pair_dpd_energy.jpg
Normal file
|
After Width: | Height: | Size: 25 KiB |
12
doc/src/Eqs/pair_dpd_energy.tex
Normal file
@ -0,0 +1,12 @@
|
||||
\documentclass[12pt]{article}
|
||||
\pagestyle{empty}
|
||||
\begin{document}
|
||||
|
||||
\begin{eqnarray*}
|
||||
du_{i}^{cond} & = & \kappa_{ij}(\frac{1}{\theta_{i}}-\frac{1}{\theta_{j}})\omega_{ij}^{2} + \alpha_{ij}\omega_{ij}\zeta_{ij}^{q}(\Delta{t})^{-1/2} \\
|
||||
du_{i}^{mech} & = & -\frac{1}{2}\gamma_{ij}\omega_{ij}^{2}(\frac{\vec{r_{ij}}}{r_{ij}}\bullet\vec{v_{ij}})^{2} -
|
||||
\frac{\sigma^{2}_{ij}}{4}(\frac{1}{m_{i}}+\frac{1}{m_{j}})\omega_{ij}^{2} -
|
||||
\frac{1}{2}\sigma_{ij}\omega_{ij}(\frac{\vec{r_{ij}}}{r_{ij}}\bullet\vec{v_{ij}})\zeta_{ij}(\Delta{t})^{-1/2} \\
|
||||
\end{eqnarray*}
|
||||
|
||||
\end{document}
|
||||
BIN
doc/src/Eqs/pair_dpd_energy_terms.jpg
Normal file
|
After Width: | Height: | Size: 8.7 KiB |
11
doc/src/Eqs/pair_dpd_energy_terms.tex
Normal file
@ -0,0 +1,11 @@
|
||||
\documentclass[12pt]{article}
|
||||
\pagestyle{empty}
|
||||
\begin{document}
|
||||
|
||||
\begin{eqnarray*}
|
||||
\alpha_{ij}^{2} & = & 2k_{B}\kappa_{ij} \\
|
||||
\sigma^{2}_{ij} & = & 2\gamma_{ij}k_{B}\Theta_{ij} \\
|
||||
\Theta_{ij}^{-1} & = & \frac{1}{2}(\frac{1}{\theta_{i}}+\frac{1}{\theta_{j}}) \\
|
||||
\end{eqnarray*}
|
||||
|
||||
\end{document}
|
||||
BIN
doc/src/JPG/gran_funnel.png
Normal file
|
After Width: | Height: | Size: 117 KiB |
BIN
doc/src/JPG/gran_funnel_small.jpg
Normal file
|
After Width: | Height: | Size: 2.2 KiB |
BIN
doc/src/JPG/gran_mixer.png
Normal file
|
After Width: | Height: | Size: 224 KiB |
BIN
doc/src/JPG/gran_mixer_small.jpg
Normal file
|
After Width: | Height: | Size: 3.0 KiB |
@ -1,7 +1,7 @@
|
||||
<!-- HTML_ONLY -->
|
||||
<HEAD>
|
||||
<TITLE>LAMMPS Users Manual</TITLE>
|
||||
<META NAME="docnumber" CONTENT="5 Oct 2016 version">
|
||||
<META NAME="docnumber" CONTENT="12 Oct 2016 version">
|
||||
<META NAME="author" CONTENT="http://lammps.sandia.gov - Sandia National Laboratories">
|
||||
<META NAME="copyright" CONTENT="Copyright (2003) Sandia Corporation. This software and manual is distributed under the GNU General Public License.">
|
||||
</HEAD>
|
||||
@ -21,7 +21,7 @@
|
||||
<H1></H1>
|
||||
|
||||
LAMMPS Documentation :c,h3
|
||||
5 Oct 2016 version :c,h4
|
||||
12 Oct 2016 version :c,h4
|
||||
|
||||
Version info: :h4
|
||||
|
||||
|
||||
@ -282,78 +282,135 @@ the "minimize"_minimize.html command. A parallel tempering
|
||||
3.4 Commands listed by category :link(cmd_4),h4
|
||||
|
||||
This section lists all LAMMPS commands, grouped by category. The
|
||||
"next section"_#cmd_5 lists the same commands alphabetically. Note
|
||||
that some style options for some commands are part of specific LAMMPS
|
||||
packages, which means they cannot be used unless the package was
|
||||
included when LAMMPS was built. Not all packages are included in a
|
||||
default LAMMPS build. These dependencies are listed as Restrictions
|
||||
in the command's documentation.
|
||||
"next section"_#cmd_5 lists the same commands alphabetically. The
|
||||
next section also includes (long) lists of style options for entries
|
||||
that appear in the following categories as a single command (fix,
|
||||
compute, pair, etc). Commands that are added by user packages are not
|
||||
included in these categories, but they are in the next section.
|
||||
|
||||
Initialization:
|
||||
|
||||
"atom_modify"_atom_modify.html, "atom_style"_atom_style.html,
|
||||
"boundary"_boundary.html, "dimension"_dimension.html,
|
||||
"newton"_newton.html, "processors"_processors.html, "units"_units.html
|
||||
"newton"_newton.html,
|
||||
"package"_package.html,
|
||||
"processors"_processors.html,
|
||||
"suffix"_suffix.html,
|
||||
"units"_units.html
|
||||
|
||||
Atom definition:
|
||||
Setup simulation box:
|
||||
|
||||
"create_atoms"_create_atoms.html, "create_box"_create_box.html,
|
||||
"lattice"_lattice.html, "read_data"_read_data.html,
|
||||
"read_dump"_read_dump.html, "read_restart"_read_restart.html,
|
||||
"region"_region.html, "replicate"_replicate.html
|
||||
"boundary"_boundary.html,
|
||||
"box"_box.html,
|
||||
"change_box"_change_box.html,
|
||||
"create_box"_create_box.html,
|
||||
"dimension"_dimension.html,
|
||||
"lattice"_lattice.html,
|
||||
"region"_region.html
|
||||
|
||||
Setup atoms:
|
||||
|
||||
"atom_modify"_atom_modify.html,
|
||||
"atom_style"_atom_style.html,
|
||||
"balance"_balance.html,
|
||||
"create_atoms"_create_atoms.html,
|
||||
"create_bonds"_create_bonds.html,
|
||||
"delete_atoms"_delete_atoms.html,
|
||||
"delete_bonds"_delete_bonds.html,
|
||||
"displace_atoms"_displace_atoms.html,
|
||||
"group"_group.html,
|
||||
"mass"_mass.html,
|
||||
"molecule"_molecule.html,
|
||||
"read_data"_read_data.html,
|
||||
"read_dump"_read_dump.html,
|
||||
"read_restart"_read_restart.html,
|
||||
"replicate"_replicate.html,
|
||||
"set"_set.html,
|
||||
"velocity"_velocity.html
|
||||
|
||||
Force fields:
|
||||
|
||||
"angle_coeff"_angle_coeff.html, "angle_style"_angle_style.html,
|
||||
"bond_coeff"_bond_coeff.html, "bond_style"_bond_style.html,
|
||||
"dielectric"_dielectric.html, "dihedral_coeff"_dihedral_coeff.html,
|
||||
"angle_coeff"_angle_coeff.html,
|
||||
"angle_style"_angle_style.html,
|
||||
"bond_coeff"_bond_coeff.html,
|
||||
"bond_style"_bond_style.html,
|
||||
"bond_write"_bond_write.html,
|
||||
"dielectric"_dielectric.html,
|
||||
"dihedral_coeff"_dihedral_coeff.html,
|
||||
"dihedral_style"_dihedral_style.html,
|
||||
"improper_coeff"_improper_coeff.html,
|
||||
"improper_style"_improper_style.html,
|
||||
"kspace_modify"_kspace_modify.html, "kspace_style"_kspace_style.html,
|
||||
"pair_coeff"_pair_coeff.html, "pair_modify"_pair_modify.html,
|
||||
"pair_style"_pair_style.html, "pair_write"_pair_write.html,
|
||||
"kspace_modify"_kspace_modify.html,
|
||||
"kspace_style"_kspace_style.html,
|
||||
"pair_coeff"_pair_coeff.html,
|
||||
"pair_modify"_pair_modify.html,
|
||||
"pair_style"_pair_style.html,
|
||||
"pair_write"_pair_write.html,
|
||||
"special_bonds"_special_bonds.html
|
||||
|
||||
Settings:
|
||||
|
||||
"comm_style"_comm_style.html, "group"_group.html, "mass"_mass.html,
|
||||
"min_modify"_min_modify.html, "min_style"_min_style.html,
|
||||
"neigh_modify"_neigh_modify.html, "neighbor"_neighbor.html,
|
||||
"reset_timestep"_reset_timestep.html, "run_style"_run_style.html,
|
||||
"set"_set.html, "timestep"_timestep.html, "velocity"_velocity.html
|
||||
"comm_modify"_comm_modify.html,
|
||||
"comm_style"_comm_style.html,
|
||||
"info"_info.html,
|
||||
"min_modify"_min_modify.html,
|
||||
"min_style"_min_style.html,
|
||||
"neigh_modify"_neigh_modify.html,
|
||||
"neighbor"_neighbor.html,
|
||||
"partition"_partition.html,
|
||||
"reset_timestep"_reset_timestep.html,
|
||||
"run_style"_run_style.html,
|
||||
"timer"_timer.html,
|
||||
"timestep"_timestep.html
|
||||
|
||||
Fixes:
|
||||
Operations within timestepping (fixes) and diagnositics (computes):
|
||||
|
||||
"fix"_fix.html, "fix_modify"_fix_modify.html, "unfix"_unfix.html
|
||||
|
||||
Computes:
|
||||
|
||||
"compute"_compute.html, "compute_modify"_compute_modify.html,
|
||||
"uncompute"_uncompute.html
|
||||
"compute"_compute.html,
|
||||
"compute_modify"_compute_modify.html,
|
||||
"fix"_fix.html,
|
||||
"fix_modify"_fix_modify.html,
|
||||
"uncompute"_uncompute.html,
|
||||
"unfix"_unfix.html
|
||||
|
||||
Output:
|
||||
|
||||
"dump"_dump.html, "dump image"_dump_image.html,
|
||||
"dump_modify"_dump_modify.html, "dump movie"_dump_image.html,
|
||||
"restart"_restart.html, "thermo"_thermo.html,
|
||||
"thermo_modify"_thermo_modify.html, "thermo_style"_thermo_style.html,
|
||||
"undump"_undump.html, "write_data"_write_data.html,
|
||||
"write_dump"_write_dump.html, "write_restart"_write_restart.html
|
||||
"dump image"_dump_image.html,
|
||||
"dump movie"_dump_image.html,
|
||||
"dump"_dump.html,
|
||||
"dump_modify"_dump_modify.html,
|
||||
"restart"_restart.html,
|
||||
"thermo"_thermo.html,
|
||||
"thermo_modify"_thermo_modify.html,
|
||||
"thermo_style"_thermo_style.html,
|
||||
"undump"_undump.html,
|
||||
"write_coeff"_write_coeff.html,
|
||||
"write_data"_write_data.html,
|
||||
"write_dump"_write_dump.html,
|
||||
"write_restart"_write_restart.html
|
||||
|
||||
Actions:
|
||||
|
||||
"delete_atoms"_delete_atoms.html, "delete_bonds"_delete_bonds.html,
|
||||
"displace_atoms"_displace_atoms.html, "change_box"_change_box.html,
|
||||
"minimize"_minimize.html, "neb"_neb.html "prd"_prd.html,
|
||||
"rerun"_rerun.html, "run"_run.html, "temper"_temper.html
|
||||
"minimize"_minimize.html,
|
||||
"neb"_neb.html,
|
||||
"prd"_prd.html,
|
||||
"rerun"_rerun.html,
|
||||
"run"_run.html,
|
||||
"tad"_tad.html,
|
||||
"temper"_temper.html
|
||||
|
||||
Miscellaneous:
|
||||
Input script control:
|
||||
|
||||
"clear"_clear.html, "echo"_echo.html, "if"_if.html,
|
||||
"include"_include.html, "jump"_jump.html, "label"_label.html,
|
||||
"log"_log.html, "next"_next.html, "print"_print.html,
|
||||
"shell"_shell.html, "variable"_variable.html
|
||||
"clear"_clear.html,
|
||||
"echo"_echo.html,
|
||||
"if"_if.html,
|
||||
"include"_include.html,
|
||||
"jump"_jump.html,
|
||||
"label"_label.html,
|
||||
"log"_log.html,
|
||||
"next"_next.html,
|
||||
"print"_print.html,
|
||||
"python"_python.html,
|
||||
"quit"_quit.html,
|
||||
"shell"_shell.html,
|
||||
"variable"_variable.html
|
||||
|
||||
:line
|
||||
|
||||
@ -599,6 +656,7 @@ USER-INTEL, k = KOKKOS, o = USER-OMP, t = OPT.
|
||||
"viscous"_fix_viscous.html,
|
||||
"wall/colloid"_fix_wall.html,
|
||||
"wall/gran"_fix_wall_gran.html,
|
||||
"wall/gran/region"_fix_wall_gran_region.html,
|
||||
"wall/harmonic"_fix_wall.html,
|
||||
"wall/lj1043"_fix_wall.html,
|
||||
"wall/lj126"_fix_wall.html,
|
||||
@ -617,6 +675,7 @@ package"_Section_start.html#start_3.
|
||||
"atc"_fix_atc.html,
|
||||
"ave/correlate/long"_fix_ave_correlate_long.html,
|
||||
"colvars"_fix_colvars.html,
|
||||
"dpd/energy"_fix_dpd_energy.html,
|
||||
"drude"_fix_drude.html,
|
||||
"drude/transform/direct"_fix_drude_transform.html,
|
||||
"drude/transform/reverse"_fix_drude_transform.html,
|
||||
@ -922,6 +981,7 @@ KOKKOS, o = USER-OMP, t = OPT.
|
||||
"tip4p/long (o)"_pair_coul.html,
|
||||
"tri/lj"_pair_tri_lj.html,
|
||||
"vashishta (o)"_pair_vashishta.html,
|
||||
"vashishta/table (o)"_pair_vashishta.html,
|
||||
"yukawa (go)"_pair_yukawa.html,
|
||||
"yukawa/colloid (go)"_pair_yukawa_colloid.html,
|
||||
"zbl (go)"_pair_zbl.html :tb(c=4,ea=c)
|
||||
|
||||
@ -54,30 +54,30 @@ accelerate: run with various acceleration options (OpenMP, GPU, Phi)
|
||||
balance: dynamic load balancing, 2d system
|
||||
body: body particles, 2d system
|
||||
colloid: big colloid particles in a small particle solvent, 2d system
|
||||
comb: models using the COMB potential
|
||||
comb: models using the COMB potential
|
||||
coreshell: core/shell model using CORESHELL package
|
||||
crack: crack propagation in a 2d solid
|
||||
crack: crack propagation in a 2d solid
|
||||
deposit: deposit atoms and molecules on a surface
|
||||
dipole: point dipolar particles, 2d system
|
||||
dreiding: methanol via Dreiding FF
|
||||
eim: NaCl using the EIM potential
|
||||
ellipse: ellipsoidal particles in spherical solvent, 2d system
|
||||
flow: Couette and Poiseuille flow in a 2d channel
|
||||
flow: Couette and Poiseuille flow in a 2d channel
|
||||
friction: frictional contact of spherical asperities between 2d surfaces
|
||||
hugoniostat: Hugoniostat shock dynamics
|
||||
indent: spherical indenter into a 2d solid
|
||||
indent: spherical indenter into a 2d solid
|
||||
kim: use of potentials in Knowledge Base for Interatomic Models (KIM)
|
||||
meam: MEAM test for SiC and shear (same as shear examples)
|
||||
melt: rapid melt of 3d LJ system
|
||||
meam: MEAM test for SiC and shear (same as shear examples)
|
||||
melt: rapid melt of 3d LJ system
|
||||
micelle: self-assembly of small lipid-like molecules into 2d bilayers
|
||||
min: energy minimization of 2d LJ melt
|
||||
msst: MSST shock dynamics
|
||||
min: energy minimization of 2d LJ melt
|
||||
msst: MSST shock dynamics
|
||||
nb3b: use of nonbonded 3-body harmonic pair style
|
||||
neb: nudged elastic band (NEB) calculation for barrier finding
|
||||
nemd: non-equilibrium MD of 2d sheared system
|
||||
neb: nudged elastic band (NEB) calculation for barrier finding
|
||||
nemd: non-equilibrium MD of 2d sheared system
|
||||
obstacle: flow around two voids in a 2d channel
|
||||
peptide: dynamics of a small solvated peptide chain (5-mer)
|
||||
peri: Peridynamic model of cylinder impacted by indenter
|
||||
peri: Peridynamic model of cylinder impacted by indenter
|
||||
pour: pouring of granular particles into a 3d box, then chute flow
|
||||
prd: parallel replica dynamics of vacancy diffusion in bulk Si
|
||||
python: using embedded Python in a LAMMPS input script
|
||||
|
||||
@ -37,7 +37,7 @@ pitfalls or alternatives.
|
||||
|
||||
Please see some of the closed issues for examples of how to
|
||||
suggest code enhancements, submit proposed changes, or report
|
||||
elated issues and how they are resoved.
|
||||
possible bugs and how they are resoved.
|
||||
|
||||
As an alternative to using GitHub, you may e-mail the
|
||||
"core developers"_http://lammps.sandia.gov/authors.html or send
|
||||
|
||||
@ -68,7 +68,7 @@ Look at the {in.chain} input script provided in the {bench} directory
|
||||
of the LAMMPS distribution to see the original script that these 2
|
||||
scripts are based on. If that script had the line
|
||||
|
||||
restart 50 tmp.restart :pre
|
||||
restart 50 tmp.restart :pre
|
||||
|
||||
added to it, it would produce 2 binary restart files (tmp.restart.50
|
||||
and tmp.restart.100) as it ran.
|
||||
@ -76,17 +76,17 @@ and tmp.restart.100) as it ran.
|
||||
This script could be used to read the 1st restart file and re-run the
|
||||
last 50 timesteps:
|
||||
|
||||
read_restart tmp.restart.50 :pre
|
||||
read_restart tmp.restart.50 :pre
|
||||
|
||||
neighbor 0.4 bin
|
||||
neigh_modify every 1 delay 1 :pre
|
||||
neighbor 0.4 bin
|
||||
neigh_modify every 1 delay 1 :pre
|
||||
|
||||
fix 1 all nve
|
||||
fix 2 all langevin 1.0 1.0 10.0 904297 :pre
|
||||
fix 1 all nve
|
||||
fix 2 all langevin 1.0 1.0 10.0 904297 :pre
|
||||
|
||||
timestep 0.012 :pre
|
||||
timestep 0.012 :pre
|
||||
|
||||
run 50 :pre
|
||||
run 50 :pre
|
||||
|
||||
Note that the following commands do not need to be repeated because
|
||||
their settings are included in the restart file: {units, atom_style,
|
||||
@ -107,25 +107,25 @@ lmp_g++ -r tmp.restart.50 tmp.restart.data :pre
|
||||
|
||||
Then, this script could be used to re-run the last 50 steps:
|
||||
|
||||
units lj
|
||||
atom_style bond
|
||||
pair_style lj/cut 1.12
|
||||
pair_modify shift yes
|
||||
bond_style fene
|
||||
units lj
|
||||
atom_style bond
|
||||
pair_style lj/cut 1.12
|
||||
pair_modify shift yes
|
||||
bond_style fene
|
||||
special_bonds 0.0 1.0 1.0 :pre
|
||||
|
||||
read_data tmp.restart.data :pre
|
||||
read_data tmp.restart.data :pre
|
||||
|
||||
neighbor 0.4 bin
|
||||
neigh_modify every 1 delay 1 :pre
|
||||
neighbor 0.4 bin
|
||||
neigh_modify every 1 delay 1 :pre
|
||||
|
||||
fix 1 all nve
|
||||
fix 2 all langevin 1.0 1.0 10.0 904297 :pre
|
||||
fix 1 all nve
|
||||
fix 2 all langevin 1.0 1.0 10.0 904297 :pre
|
||||
|
||||
timestep 0.012 :pre
|
||||
timestep 0.012 :pre
|
||||
|
||||
reset_timestep 50
|
||||
run 50 :pre
|
||||
reset_timestep 50
|
||||
run 50 :pre
|
||||
|
||||
Note that nearly all the settings specified in the original {in.chain}
|
||||
script must be repeated, except the {pair_coeff} and {bond_coeff}
|
||||
@ -2092,11 +2092,11 @@ lattice fcc 5.376 orient x 1 0 0 orient y 0 1 0 orient z 0 0 1
|
||||
region box block 0 4 0 4 0 4
|
||||
create_box 1 box
|
||||
create_atoms 1 box
|
||||
mass 1 39.948
|
||||
mass 1 39.948
|
||||
pair_style lj/cut 13.0
|
||||
pair_coeff * * 0.2381 3.405
|
||||
timestep $\{dt\}
|
||||
thermo $d :pre
|
||||
thermo $d :pre
|
||||
|
||||
# equilibration and thermalization :pre
|
||||
|
||||
|
||||
@ -552,32 +552,32 @@ lmp.command(cmd) # invoke a single LAMMPS command, cmd = "run 100" :pre
|
||||
|
||||
xlo = lmp.extract_global(name,type) # extract a global quantity
|
||||
# name = "boxxlo", "nlocal", etc
|
||||
# type = 0 = int
|
||||
# 1 = double :pre
|
||||
# type = 0 = int
|
||||
# 1 = double :pre
|
||||
|
||||
coords = lmp.extract_atom(name,type) # extract a per-atom quantity
|
||||
# name = "x", "type", etc
|
||||
# type = 0 = vector of ints
|
||||
# 1 = array of ints
|
||||
# 2 = vector of doubles
|
||||
# 3 = array of doubles :pre
|
||||
# type = 0 = vector of ints
|
||||
# 1 = array of ints
|
||||
# 2 = vector of doubles
|
||||
# 3 = array of doubles :pre
|
||||
|
||||
eng = lmp.extract_compute(id,style,type) # extract value(s) from a compute
|
||||
v3 = lmp.extract_fix(id,style,type,i,j) # extract value(s) from a fix
|
||||
# id = ID of compute or fix
|
||||
# style = 0 = global data
|
||||
# 1 = per-atom data
|
||||
# 2 = local data
|
||||
# type = 0 = scalar
|
||||
# 1 = vector
|
||||
# 2 = array
|
||||
# i,j = indices of value in global vector or array :pre
|
||||
# style = 0 = global data
|
||||
# 1 = per-atom data
|
||||
# 2 = local data
|
||||
# type = 0 = scalar
|
||||
# 1 = vector
|
||||
# 2 = array
|
||||
# i,j = indices of value in global vector or array :pre
|
||||
|
||||
var = lmp.extract_variable(name,group,flag) # extract value(s) from a variable
|
||||
# name = name of variable
|
||||
# group = group ID (ignored for equal-style variables)
|
||||
# flag = 0 = equal-style variable
|
||||
# 1 = atom-style variable :pre
|
||||
# name = name of variable
|
||||
# group = group ID (ignored for equal-style variables)
|
||||
# flag = 0 = equal-style variable
|
||||
# 1 = atom-style variable :pre
|
||||
|
||||
flag = lmp.set_variable(name,value) # set existing named string-style variable to value, flag = 0 if successful
|
||||
natoms = lmp.get_natoms() # total # of atoms as int
|
||||
|
||||
@ -14,7 +14,7 @@ atom_style style args :pre
|
||||
|
||||
style = {angle} or {atomic} or {body} or {bond} or {charge} or {dipole} or \
|
||||
{dpd} or {electron} or {ellipsoid} or {full} or {line} or {meso} or \
|
||||
{molecular} or {peri} or {smd} or {sphere} or {tri} or \
|
||||
{molecular} or {peri} or {smd} or {sphere} or {tri} or \
|
||||
{template} or {hybrid} :ulb,l
|
||||
args = none for any style except the following
|
||||
{body} args = bstyle bstyle-args
|
||||
|
||||
@ -135,7 +135,7 @@ and angular momentum of a particle. If the {vel} option is set to
|
||||
{yes}, then ghost atoms store these quantities; if {no} then they do
|
||||
not. The {yes} setting is needed by some pair styles which require
|
||||
the velocity state of both the I and J particles to compute a pairwise
|
||||
I,J interaction.
|
||||
I,J interaction, as well as by some compute and fix commands.
|
||||
|
||||
Note that if the "fix deform"_fix_deform.html command is being used
|
||||
with its "remap v" option enabled, then the velocities for ghost atoms
|
||||
|
||||
@ -152,11 +152,11 @@ lattice fcc 5.376 orient x 1 0 0 orient y 0 1 0 orient z 0 0 1
|
||||
region box block 0 4 0 4 0 4
|
||||
create_box 1 box
|
||||
create_atoms 1 box
|
||||
mass 1 39.948
|
||||
mass 1 39.948
|
||||
pair_style lj/cut 13.0
|
||||
pair_coeff * * 0.2381 3.405
|
||||
timestep $\{dt\}
|
||||
thermo $d :pre
|
||||
thermo $d :pre
|
||||
|
||||
# equilibration and thermalization :pre
|
||||
|
||||
|
||||
@ -52,7 +52,7 @@ The KSpace contribution is calculated using the method in
|
||||
"(Heyes)"_#Heyes for the Ewald method and a related method for PPPM,
|
||||
as specified by the "kspace_style pppm"_kspace_style.html command.
|
||||
For PPPM, the calcluation requires 1 extra FFT each timestep that
|
||||
per-atom energy is calculated. Thie "document"_PDF/kspace.pdf
|
||||
per-atom energy is calculated. This "document"_PDF/kspace.pdf
|
||||
describes how the long-range per-atom energy calculation is performed.
|
||||
|
||||
Various fixes can contribute to the per-atom potential energy of the
|
||||
@ -68,9 +68,9 @@ As an example of per-atom potential energy compared to total potential
|
||||
energy, these lines in an input script should yield the same result
|
||||
in the last 2 columns of thermo output:
|
||||
|
||||
compute peratom all pe/atom
|
||||
compute pe all reduce sum c_peratom
|
||||
thermo_style custom step temp etotal press pe c_pe :pre
|
||||
compute peratom all pe/atom
|
||||
compute pe all reduce sum c_peratom
|
||||
thermo_style custom step temp etotal press pe c_pe :pre
|
||||
|
||||
NOTE: The per-atom energy does not any Lennard-Jones tail corrections
|
||||
invoked by the "pair_modify tail yes"_pair_modify.html command, since
|
||||
|
||||
@ -16,20 +16,20 @@ ID, group-ID are documented in "compute"_compute.html command :ulb,l
|
||||
property/atom = style name of this compute command :l
|
||||
input = one or more atom attributes :l
|
||||
possible attributes = id, mol, proc, type, mass,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
q, mux, muy, muz, mu,
|
||||
radius, diameter, omegax, omegay, omegaz,
|
||||
angmomx, angmomy, angmomz,
|
||||
shapex,shapey, shapez,
|
||||
quatw, quati, quatj, quatk, tqx, tqy, tqz,
|
||||
end1x, end1y, end1z, end2x, end2y, end2z,
|
||||
corner1x, corner1y, corner1z,
|
||||
corner2x, corner2y, corner2z,
|
||||
corner3x, corner3y, corner3z,
|
||||
nbonds,
|
||||
angmomx, angmomy, angmomz,
|
||||
shapex,shapey, shapez,
|
||||
quatw, quati, quatj, quatk, tqx, tqy, tqz,
|
||||
end1x, end1y, end1z, end2x, end2y, end2z,
|
||||
corner1x, corner1y, corner1z,
|
||||
corner2x, corner2y, corner2z,
|
||||
corner3x, corner3y, corner3z,
|
||||
nbonds,
|
||||
vfrac, s0,
|
||||
spin, eradius, ervel, erforce,
|
||||
spin, eradius, ervel, erforce,
|
||||
rho, drho, e, de, cv,
|
||||
i_name, d_name :pre
|
||||
id = atom ID
|
||||
|
||||
@ -15,12 +15,12 @@ compute ID group-ID property/local attribute1 attribute2 ... keyword args ... :p
|
||||
ID, group-ID are documented in "compute"_compute.html command :ulb,l
|
||||
property/local = style name of this compute command :l
|
||||
one or more attributes may be appended :l
|
||||
possible attributes = natom1 natom2 ntype1 ntype2
|
||||
patom1 patom2 ptype1 ptype2
|
||||
batom1 batom2 btype
|
||||
aatom1 aatom2 aatom3 atype
|
||||
datom1 datom2 datom3 dtype
|
||||
iatom1 iatom2 iatom3 itype :pre
|
||||
possible attributes = natom1 natom2 ntype1 ntype2
|
||||
patom1 patom2 ptype1 ptype2
|
||||
batom1 batom2 btype
|
||||
aatom1 aatom2 aatom3 atype
|
||||
datom1 datom2 datom3 dtype
|
||||
iatom1 iatom2 iatom3 itype :pre
|
||||
|
||||
natom1, natom2 = IDs of 2 atoms in each pair (within neighbor cutoff)
|
||||
ntype1, ntype2 = type of 2 atoms in each pair (within neighbor cutoff)
|
||||
@ -129,8 +129,6 @@ The attributes that start with "a", "d", "i", refer to similar values
|
||||
for "angles"_angle_style.html, "dihedrals"_dihedral_style.html, and
|
||||
"impropers"_improper_style.html.
|
||||
|
||||
The optional {cutoff} keyword
|
||||
|
||||
[Output info:]
|
||||
|
||||
This compute calculates a local vector or local array depending on the
|
||||
|
||||
@ -155,8 +155,8 @@ Thus, for example, if you wish to use this compute to find the bond
|
||||
with maximum stretch, you can do it as follows:
|
||||
|
||||
compute 1 all property/local batom1 batom2
|
||||
compute 2 all bond/local dist
|
||||
compute 3 all reduce max c_1\[1\] c_1\[2\] c_2 replace 1 3 replace 2 3
|
||||
compute 2 all bond/local dist
|
||||
compute 3 all reduce max c_1\[1\] c_1\[2\] c_2 replace 1 3 replace 2 3
|
||||
thermo_style custom step temp c_3\[1\] c_3\[2\] c_3\[3\] :pre
|
||||
|
||||
The first two input values in the compute reduce command are vectors
|
||||
|
||||
@ -17,11 +17,11 @@ rigid/local = style name of this compute command :l
|
||||
rigidID = ID of fix rigid/small command or one of its variants :l
|
||||
input = one or more rigid body attributes :l
|
||||
possible attributes = id, mol, mass,
|
||||
x, y, z, xu, yu, zu, ix, iy, iz
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
x, y, z, xu, yu, zu, ix, iy, iz
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
omegax, omegay, omegaz,
|
||||
angmomx, angmomy, angmomz,
|
||||
quatw, quati, quatj, quatk,
|
||||
angmomx, angmomy, angmomz,
|
||||
quatw, quati, quatj, quatk,
|
||||
tqx, tqy, tqz,
|
||||
inertiax, inertiay, inertiaz
|
||||
id = atom ID of atom within body which owns body properties
|
||||
|
||||
@ -128,10 +128,10 @@ d = dimension and V is the volume of the system, the result should be
|
||||
These lines in an input script for a 3d system should yield that
|
||||
result. I.e. the last 2 columns of thermo output will be the same:
|
||||
|
||||
compute peratom all stress/atom NULL
|
||||
compute p all reduce sum c_peratom\[1\] c_peratom\[2\] c_peratom\[3\]
|
||||
variable press equal -(c_p\[1\]+c_p\[2\]+c_p\[3\])/(3*vol)
|
||||
thermo_style custom step temp etotal press v_press :pre
|
||||
compute peratom all stress/atom NULL
|
||||
compute p all reduce sum c_peratom\[1\] c_peratom\[2\] c_peratom\[3\]
|
||||
variable press equal -(c_p\[1\]+c_p\[2\]+c_p\[3\])/(3*vol)
|
||||
thermo_style custom step temp etotal press v_press :pre
|
||||
|
||||
[Output info:]
|
||||
|
||||
|
||||
0
doc/src/compute_temp_asphere.txt
Executable file → Normal file
0
doc/src/compute_temp_body.txt
Executable file → Normal file
0
doc/src/compute_temp_sphere.txt
Executable file → Normal file
@ -218,14 +218,14 @@ larger version.
|
||||
|
||||
variable x equal 100
|
||||
variable y equal 25
|
||||
lattice hex 0.8442
|
||||
region box block 0 $x 0 $y -0.5 0.5
|
||||
create_box 1 box :pre
|
||||
lattice hex 0.8442
|
||||
region box block 0 $x 0 $y -0.5 0.5
|
||||
create_box 1 box :pre
|
||||
|
||||
variable xx equal 0.0
|
||||
variable yy equal 0.0
|
||||
variable v equal "(0.2*v_y*ylat * cos(v_xx/xlat * 2.0*PI*4.0/v_x) + 0.5*v_y*ylat - v_yy) > 0.0"
|
||||
create_atoms 1 box var v set x xx set y yy :pre
|
||||
create_atoms 1 box var v set x xx set y yy :pre
|
||||
|
||||
:c,image(JPG/sinusoid_small.jpg,JPG/sinusoid.jpg)
|
||||
|
||||
|
||||
@ -55,13 +55,13 @@ args = list of arguments for a particular style :l
|
||||
|
||||
{custom} or {custom/gz} or {custom/mpiio} args = list of atom attributes
|
||||
possible attributes = id, mol, proc, procp1, type, element, mass,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu,
|
||||
xsu, ysu, zsu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu,
|
||||
xsu, ysu, zsu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
q, mux, muy, muz, mu,
|
||||
radius, diameter, omegax, omegay, omegaz,
|
||||
angmomx, angmomy, angmomz, tqx, tqy, tqz,
|
||||
c_ID, c_ID\[N\], f_ID, f_ID\[N\], v_name :pre
|
||||
angmomx, angmomy, angmomz, tqx, tqy, tqz,
|
||||
c_ID, c_ID\[N\], f_ID, f_ID\[N\], v_name :pre
|
||||
|
||||
id = atom ID
|
||||
mol = molecule ID
|
||||
|
||||
@ -20,14 +20,14 @@ file = name of file to write dump info to :l
|
||||
args = list of arguments for a particular style :l
|
||||
{custom/vtk} args = list of atom attributes
|
||||
possible attributes = id, mol, proc, procp1, type, element, mass,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu,
|
||||
xsu, ysu, zsu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu,
|
||||
xsu, ysu, zsu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
q, mux, muy, muz, mu,
|
||||
radius, diameter, omegax, omegay, omegaz,
|
||||
angmomx, angmomy, angmomz, tqx, tqy, tqz,
|
||||
spin, eradius, ervel, erforce,
|
||||
c_ID, c_ID\[N\], f_ID, f_ID\[N\], v_name :pre
|
||||
angmomx, angmomy, angmomz, tqx, tqy, tqz,
|
||||
spin, eradius, ervel, erforce,
|
||||
c_ID, c_ID\[N\], f_ID, f_ID\[N\], v_name :pre
|
||||
|
||||
id = atom ID
|
||||
mol = molecule ID
|
||||
|
||||
@ -215,17 +215,17 @@ to the dump file. The {every} keyword cannot be used with the dump
|
||||
For example, the following commands will
|
||||
write snapshots at timesteps 0,10,20,30,100,200,300,1000,2000,etc:
|
||||
|
||||
variable s equal logfreq(10,3,10)
|
||||
dump 1 all atom 100 tmp.dump
|
||||
dump_modify 1 every v_s first yes :pre
|
||||
variable s equal logfreq(10,3,10)
|
||||
dump 1 all atom 100 tmp.dump
|
||||
dump_modify 1 every v_s first yes :pre
|
||||
|
||||
The following commands would write snapshots at the timesteps listed
|
||||
in file tmp.times:
|
||||
|
||||
variable f file tmp.times
|
||||
variable s equal next(f)
|
||||
dump 1 all atom 100 tmp.dump
|
||||
dump_modify 1 every v_s :pre
|
||||
variable s equal next(f)
|
||||
dump 1 all atom 100 tmp.dump
|
||||
dump_modify 1 every v_s :pre
|
||||
|
||||
NOTE: When using a file-style variable with the {every} keyword, the
|
||||
file of timesteps must list a first timestep that is beyond the
|
||||
@ -475,9 +475,6 @@ be generated by variable formulas that use comparison or Boolean math
|
||||
operators or special functions like gmask() and rmask() and grmask().
|
||||
See the "variable"_variable.html command doc page for details.
|
||||
|
||||
NOTE: The LAST option, discussed below, is not yet implemented. It
|
||||
will be soon.
|
||||
|
||||
The specified value must be a simple numeric value or the word LAST.
|
||||
If LAST is used, it refers to the value of the attribute the last time
|
||||
the dump command was invoked to produce a snapshot. This is a way to
|
||||
@ -686,10 +683,10 @@ this is used.
|
||||
variable colors string &
|
||||
"red green blue yellow white &
|
||||
purple pink orange lime gray"
|
||||
variable mol atom mol%10
|
||||
dump 1 all image 250 image.*.jpg v_mol type &
|
||||
zoom 1.6 adiam 1.5
|
||||
dump_modify 1 pad 5 amap 0 10 sa 1 10 $\{colors\} :pre
|
||||
variable mol atom mol%10
|
||||
dump 1 all image 250 image.*.jpg v_mol type &
|
||||
zoom 1.6 adiam 1.5
|
||||
dump_modify 1 pad 5 amap 0 10 sa 1 10 $\{colors\} :pre
|
||||
|
||||
In this case, 10 colors are defined, and molecule IDs are
|
||||
mapped to one of the colors, even if there are 1000s of molecules.
|
||||
|
||||
@ -58,7 +58,7 @@ keyword = {type} or {ave} or {start} or {prefactor} or {file} or {overwrite} or
|
||||
fix 1 all ave/correlate 5 100 1000 c_myTemp file temp.correlate
|
||||
fix 1 all ave/correlate 1 50 10000 &
|
||||
c_thermo_press\[1\] c_thermo_press\[2\] c_thermo_press\[3\] &
|
||||
type upper ave running title1 "My correlation data" :pre
|
||||
type upper ave running title1 "My correlation data" :pre
|
||||
fix 1 all ave/correlate 1 50 10000 c_thermo_press\[*\]
|
||||
|
||||
[Description:]
|
||||
|
||||
@ -55,7 +55,7 @@ keyword = {type} or {start} or {file} or {overwrite} or {title1} or {title2} or
|
||||
fix 1 all ave/correlate/long 5 1000 c_myTemp file temp.correlate
|
||||
fix 1 all ave/correlate/long 1 10000 &
|
||||
c_thermo_press\[1\] c_thermo_press\[2\] c_thermo_press\[3\] &
|
||||
type upper title1 "My correlation data" nlen 15 ncount 3 :pre
|
||||
type upper title1 "My correlation data" nlen 15 ncount 3 :pre
|
||||
|
||||
[Description:]
|
||||
|
||||
|
||||
0
doc/src/fix_bond_break.txt
Executable file → Normal file
0
doc/src/fix_bond_create.txt
Executable file → Normal file
0
doc/src/fix_bond_swap.txt
Executable file → Normal file
@ -28,7 +28,7 @@ parameter = {x} or {y} or {z} or {xy} or {xz} or {yz}
|
||||
factor = multiplicative factor for change in box length at end of run
|
||||
{vel} value = V
|
||||
V = change box length at this velocity (distance/time units),
|
||||
effectively an engineering strain rate
|
||||
effectively an engineering strain rate
|
||||
{erate} value = R
|
||||
R = engineering strain rate (1/time units)
|
||||
{trate} value = R
|
||||
@ -36,10 +36,10 @@ parameter = {x} or {y} or {z} or {xy} or {xz} or {yz}
|
||||
{volume} value = none = adjust this dim to preserve volume of system
|
||||
{wiggle} values = A Tp
|
||||
A = amplitude of oscillation (distance units)
|
||||
Tp = period of oscillation (time units)
|
||||
Tp = period of oscillation (time units)
|
||||
{variable} values = v_name1 v_name2
|
||||
v_name1 = variable with name1 for box length change as function of time
|
||||
v_name2 = variable with name2 for change rate as function of time
|
||||
v_name2 = variable with name2 for change rate as function of time
|
||||
{xy}, {xz}, {yz} args = style value
|
||||
style = {final} or {delta} or {vel} or {erate} or {trate} or {wiggle}
|
||||
{final} value = tilt
|
||||
@ -48,17 +48,17 @@ parameter = {x} or {y} or {z} or {xy} or {xz} or {yz}
|
||||
dtilt = change in tilt factor at end of run (distance units)
|
||||
{vel} value = V
|
||||
V = change tilt factor at this velocity (distance/time units),
|
||||
effectively an engineering shear strain rate
|
||||
effectively an engineering shear strain rate
|
||||
{erate} value = R
|
||||
R = engineering shear strain rate (1/time units)
|
||||
{trate} value = R
|
||||
R = true shear strain rate (1/time units)
|
||||
{wiggle} values = A Tp
|
||||
A = amplitude of oscillation (distance units)
|
||||
Tp = period of oscillation (time units)
|
||||
Tp = period of oscillation (time units)
|
||||
{variable} values = v_name1 v_name2
|
||||
v_name1 = variable with name1 for tilt change as function of time
|
||||
v_name2 = variable with name2 for change rate as function of time :pre
|
||||
v_name2 = variable with name2 for change rate as function of time :pre
|
||||
|
||||
zero or more keyword/value pairs may be appended :l
|
||||
keyword = {remap} or {flip} or {units} :l
|
||||
|
||||
83
doc/src/fix_dpd_energy.txt
Normal file
@ -0,0 +1,83 @@
|
||||
"LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc :c
|
||||
|
||||
:link(lws,http://lammps.sandia.gov)
|
||||
:link(ld,Manual.html)
|
||||
:link(lc,Section_commands.html#comm)
|
||||
|
||||
:line
|
||||
|
||||
fix dpd/energy command :h3
|
||||
|
||||
[Syntax:]
|
||||
|
||||
fix ID group-ID dpd/energy :pre
|
||||
|
||||
ID, group-ID are documented in "fix"_fix.html command
|
||||
dpd/energy = style name of this fix command :ul
|
||||
|
||||
[Examples:]
|
||||
|
||||
fix 1 all dpd/energy :pre
|
||||
|
||||
[Description:]
|
||||
|
||||
Perform constant energy dissipative particle dynamics (DPD-E)
|
||||
integration. This fix updates the internal energies for particles in
|
||||
the group at each timestep. It must be used in conjunction with a
|
||||
deterministic integrator (e.g. "fix nve"_fix_nve.html) that updates
|
||||
the particle positions and velocities.
|
||||
|
||||
For fix {dpd/energy}, the particle internal temperature is related to
|
||||
the particle internal energy through a mesoparticle equation of state.
|
||||
An additional fix must be specified that defines the equation of state
|
||||
for each particle, e.g. "fix eos/cv"_fix_eos_cv.html.
|
||||
|
||||
This fix must be used with the "pair_style
|
||||
dpd/fdt/energy"_pair_style.html command.
|
||||
|
||||
Note that numerous variants of DPD can be specified by choosing an
|
||||
appropriate combination of the integrator and "pair_style
|
||||
dpd/fdt/energy"_pair_style.html command. DPD under isoenergetic conditions
|
||||
can be specified by using fix {dpd/energy}, fix {nve} and pair_style
|
||||
{dpd/fdt/energy}. DPD under isoenthalpic conditions can
|
||||
be specified by using fix {dpd/energy}, fix {nph} and pair_style
|
||||
{dpd/fdt/energy}. Examples of each DPD variant are provided in the
|
||||
examples/USER/dpd directory.
|
||||
|
||||
:line
|
||||
|
||||
[Restrictions:]
|
||||
|
||||
This command is part of the USER-DPD package. It is only enabled if
|
||||
LAMMPS was built with that package. See the "Making
|
||||
LAMMPS"_Section_start.html#start_3 section for more info.
|
||||
|
||||
This fix must be used with an additional fix that specifies time
|
||||
integration, e.g. "fix nve"_fix_nve.html.
|
||||
|
||||
The fix {dpd/energy} requires the {dpd} "atom_style"_atom_style.html
|
||||
to be used in order to properly account for the particle internal
|
||||
energies and temperature.
|
||||
|
||||
The fix {dpd/energy} must be used with an additional fix that specifies the
|
||||
mesoparticle equation of state for each particle.
|
||||
|
||||
[Related commands:]
|
||||
|
||||
"fix nve"_fix_nve.html "fix eos/cv"_fix_eos_cv.html
|
||||
|
||||
[Default:] none
|
||||
|
||||
:line
|
||||
|
||||
:link(Lisal)
|
||||
[(Lisal)] M. Lisal, J.K. Brennan, J. Bonet Avalos, "Dissipative
|
||||
particle dynamics at isothermal, isobaric, isoenergetic, and
|
||||
isoenthalpic conditions using Shardlow-like splitting algorithms.",
|
||||
J. Chem. Phys., 135, 204105 (2011).
|
||||
|
||||
:link(Larentzos)
|
||||
[(Larentzos)] J.P. Larentzos, J.K. Brennan, J.D. Moore, and
|
||||
W.D. Mattson, "LAMMPS Implementation of Constant Energy Dissipative
|
||||
Particle Dynamics (DPD-E)", ARL-TR-6863, U.S. Army Research
|
||||
Laboratory, Aberdeen Proving Ground, MD (2014).
|
||||
@ -63,7 +63,7 @@ applied by GD before computing a pressure drop or comparing it to
|
||||
other methods, such as the pump method "(Zhu)"_#Zhu. The pressure
|
||||
correction is discussed and described in "(Strong)"_#Strong.
|
||||
|
||||
NOTE: For a complete example including the considerations discussed
|
||||
For a complete example including the considerations discussed
|
||||
above, see the examples/USER/flow_gauss directory.
|
||||
|
||||
NOTE: Only the flux of the atoms in group-ID will be conserved. If the
|
||||
@ -93,6 +93,19 @@ work on the system must have {fix_modify energy yes} set as well. This
|
||||
includes thermostat fixes and any constraints that hold the positions
|
||||
of wall atoms fixed, such as "fix spring/self"_fix_spring_self.html.
|
||||
|
||||
If this fix is used in a simulation with the "rRESPA"_run_style.html
|
||||
integrator, the applied acceleration must be computed and applied at the same
|
||||
rRESPA level as the interactions between the flowing fluid and the obstacle.
|
||||
The rRESPA level at which the acceleration is applied can be changed using
|
||||
the "fix_modify"_fix_modify.html {respa} option discussed below. If the
|
||||
flowing fluid and the obstacle interact through multiple interactions that are
|
||||
computed at different rRESPA levels, then there must be a separate flow/gauss
|
||||
fix for each level. For example, if the flowing fluid and obstacle interact
|
||||
through pairwise and long-range Coulomb interactions, which are computed at
|
||||
rRESPA levels 3 and 4, respectively, then there must be two separate
|
||||
flow/gauss fixes, one that specifies {fix_modify respa 3} and one with
|
||||
{fix_modify respa 4}.
|
||||
|
||||
:line
|
||||
|
||||
[Restart, fix_modify, output, run start/stop, minimize info:]
|
||||
@ -109,6 +122,11 @@ fix to subtract the work done from the
|
||||
system's potential energy as part of "thermodynamic
|
||||
output"_thermo_style.html.
|
||||
|
||||
The "fix_modify"_fix_modify.html {respa} option is supported by this
|
||||
fix. This allows the user to set at which level of the "rRESPA"_run_style.html
|
||||
integrator the fix computes and adds the external acceleration. Default is the
|
||||
outermost level.
|
||||
|
||||
This fix computes a global scalar and a global 3-vector of forces,
|
||||
which can be accessed by various "output
|
||||
commands"_Section_howto.html#howto_15. The scalar is the negative of the
|
||||
|
||||
0
doc/src/fix_lb_fluid.txt
Executable file → Normal file
0
doc/src/fix_lb_momentum.txt
Executable file → Normal file
0
doc/src/fix_lb_pc.txt
Executable file → Normal file
0
doc/src/fix_lb_rigid_pc_sphere.txt
Executable file → Normal file
0
doc/src/fix_lb_viscous.txt
Executable file → Normal file
@ -120,7 +120,7 @@ The global vector contains four values in this order:
|
||||
To print these quantities to the log file with descriptive column
|
||||
headers, the following LAMMPS commands are suggested:
|
||||
|
||||
fix msst all msst z
|
||||
fix msst all msst z
|
||||
fix_modify msst energy yes
|
||||
variable dhug equal f_msst\[1\]
|
||||
variable dray equal f_msst\[2\]
|
||||
|
||||
0
doc/src/fix_nph_asphere.txt
Executable file → Normal file
0
doc/src/fix_nph_body.txt
Executable file → Normal file
0
doc/src/fix_nph_sphere.txt
Executable file → Normal file
0
doc/src/fix_npt_asphere.txt
Executable file → Normal file
0
doc/src/fix_npt_body.txt
Executable file → Normal file
0
doc/src/fix_npt_sphere.txt
Executable file → Normal file
0
doc/src/fix_nve_asphere.txt
Executable file → Normal file
0
doc/src/fix_nve_asphere_noforce.txt
Executable file → Normal file
0
doc/src/fix_nve_body.txt
Executable file → Normal file
0
doc/src/fix_nve_line.txt
Executable file → Normal file
0
doc/src/fix_nve_sphere.txt
Executable file → Normal file
0
doc/src/fix_nve_tri.txt
Executable file → Normal file
0
doc/src/fix_nvt_asphere.txt
Executable file → Normal file
0
doc/src/fix_nvt_body.txt
Executable file → Normal file
0
doc/src/fix_nvt_sphere.txt
Executable file → Normal file
@ -167,14 +167,14 @@ headers, the following LAMMPS commands are suggested. Here the
|
||||
the thermo keyword {etotal} to print the quantity <i>etot</i>. See
|
||||
also the "thermo_style"_thermo_style.html command.
|
||||
|
||||
fix fix_id all msst z
|
||||
fix_modify fix_id energy yes
|
||||
variable dhug equal f_fix_id\[1\]
|
||||
variable dray equal f_fix_id\[2\]
|
||||
variable lgr_vel equal f_fix_id\[3\]
|
||||
variable lgr_pos equal f_fix_id\[4\]
|
||||
variable T_qm equal f_fix_id\[5\]
|
||||
thermo_style custom step temp ke pe lz pzz etotal v_dhug v_dray v_lgr_vel v_lgr_pos v_T_qm f_fix_id :pre
|
||||
fix fix_id all msst z
|
||||
fix_modify fix_id energy yes
|
||||
variable dhug equal f_fix_id\[1\]
|
||||
variable dray equal f_fix_id\[2\]
|
||||
variable lgr_vel equal f_fix_id\[3\]
|
||||
variable lgr_pos equal f_fix_id\[4\]
|
||||
variable T_qm equal f_fix_id\[5\]
|
||||
thermo_style custom step temp ke pe lz pzz etotal v_dhug v_dray v_lgr_vel v_lgr_pos v_T_qm f_fix_id :pre
|
||||
|
||||
The global scalar under the entry f_fix_id is the quantity of thermo
|
||||
energy as an extra part of <i>etot</i>. This global scalar and the
|
||||
|
||||
@ -75,7 +75,7 @@ but no more than max_steps will be taken. If max_steps is reached, an error warn
|
||||
is printed and the simulation is stopped.
|
||||
|
||||
After each ODE step, the solution error {e} is tested and weighted using the absTol
|
||||
and relTol values. The error vector is weighted as {e} / (relTol * | {u} | + absTol)
|
||||
and relTol values. The error vector is weighted as {e} / (relTol * |{u}| + absTol)
|
||||
where {u} is the solution vector. If the norm of the error is <= 1, the solution is
|
||||
accepted, {h} is increased by a proportional amount, and the next ODE step is begun.
|
||||
Otherwise, {h} is shrunk and the ODE step is repeated.
|
||||
|
||||
@ -17,8 +17,8 @@ store/state = style name of this fix command :l
|
||||
N = store atom attributes every N steps, N = 0 for initial store only :l
|
||||
input = one or more atom attributes :l
|
||||
possible attributes = id, mol, type, mass,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu, xsu, ysu, zsu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
x, y, z, xs, ys, zs, xu, yu, zu, xsu, ysu, zsu, ix, iy, iz,
|
||||
vx, vy, vz, fx, fy, fz,
|
||||
q, mux, muy, muz, mu,
|
||||
radius, diameter, omegax, omegay, omegaz,
|
||||
angmomx, angmomy, angmomz, tqx, tqy, tqz,
|
||||
|
||||
@ -49,6 +49,10 @@ variable, it should be specified as v_name, where name is the variable
|
||||
name. In this case, the variable will be evaluated each timestep, and
|
||||
its value used to determine the target temperature.
|
||||
|
||||
NOTE: This thermostat will generate an error if the current
|
||||
temperature is zero at the end of a timestep. It cannot rescale a
|
||||
zero temperature.
|
||||
|
||||
Equal-style variables can specify formulas with various mathematical
|
||||
functions, and include "thermo_style"_thermo_style.html command
|
||||
keywords for the simulation box parameters and timestep and elapsed
|
||||
|
||||
@ -43,6 +43,10 @@ Rescaling is performed every N timesteps. The target temperature is a
|
||||
ramped value between the {Tstart} and {Tstop} temperatures at the
|
||||
beginning and end of the run.
|
||||
|
||||
NOTE: This thermostat will generate an error if the current
|
||||
temperature is zero at the end of a timestep it is inovoked on. It
|
||||
cannot rescale a zero temperature.
|
||||
|
||||
{Tstart} can be specified as an equal-style "variable"_variable.html.
|
||||
In this case, the {Tstop} setting is ignored. If the value is a
|
||||
variable, it should be specified as v_name, where name is the variable
|
||||
@ -50,7 +54,7 @@ name. In this case, the variable will be evaluated each timestep, and
|
||||
its value used to determine the target temperature.
|
||||
|
||||
Equal-style variables can specify formulas with various mathematical
|
||||
functions, and include "thermo_style"_thermo_style.html command
|
||||
functions, and include "thermo_style"_thermox_style.html command
|
||||
keywords for the simulation box parameters and timestep and elapsed
|
||||
time. Thus it is easy to specify a time-dependent temperature.
|
||||
|
||||
|
||||
0
doc/src/fix_ti_spring.txt
Executable file → Normal file
@ -163,6 +163,8 @@ Any dimension (xyz) that has a granular wall must be non-periodic.
|
||||
|
||||
[Related commands:]
|
||||
|
||||
"fix move"_fix_move.html, "pair_style granular"_pair_gran.html
|
||||
"fix move"_fix_move.html,
|
||||
"fix wall/gran/region"_fix_wall_gran_region.html,
|
||||
"pair_style granular"_pair_gran.html
|
||||
|
||||
[Default:] none
|
||||
|
||||
199
doc/src/fix_wall_gran_region.txt
Normal file
@ -0,0 +1,199 @@
|
||||
"LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc :c
|
||||
|
||||
:link(lws,http://lammps.sandia.gov)
|
||||
:link(ld,Manual.html)
|
||||
:link(lc,Section_commands.html#comm)
|
||||
|
||||
:line
|
||||
|
||||
fix wall/gran/region command :h3
|
||||
|
||||
[Syntax:]
|
||||
|
||||
fix ID group-ID wall/gran/region fstyle Kn Kt gamma_n gamma_t xmu dampflag wallstyle regionID :pre
|
||||
|
||||
ID, group-ID are documented in "fix"_fix.html command :ulb,l
|
||||
wall/region = style name of this fix command :l
|
||||
fstyle = style of force interactions between particles and wall :l
|
||||
possible choices: hooke, hooke/history, hertz/history :pre
|
||||
Kn = elastic constant for normal particle repulsion (force/distance units or pressure units - see discussion below) :l
|
||||
Kt = elastic constant for tangential contact (force/distance units or pressure units - see discussion below) :l
|
||||
gamma_n = damping coefficient for collisions in normal direction (1/time units or 1/time-distance units - see discussion below) :l
|
||||
gamma_t = damping coefficient for collisions in tangential direction (1/time units or 1/time-distance units - see discussion below) :l
|
||||
xmu = static yield criterion (unitless value between 0.0 and 1.0e4) :l
|
||||
dampflag = 0 or 1 if tangential damping force is excluded or included :l
|
||||
wallstyle = region (see "fix wall/gran"_fix_wall_gran.html for options for other kinds of walls) :l
|
||||
region-ID = region whose boundary will act as wall :l,ule
|
||||
|
||||
[Examples:]
|
||||
|
||||
fix wall all wall/gran/region hooke/history 1000.0 200.0 200.0 100.0 0.5 1 region myCone :pre
|
||||
|
||||
[Description:]
|
||||
|
||||
Treat the surface of the geometric region defined by the {region-ID}
|
||||
as a bounding frictional wall which interacts with nearby finite-size
|
||||
granular particles when they are close enough to touch the wall. See
|
||||
the "fix wall/region"_fix_wall_region.html and "fix
|
||||
wall/gran"_fix_wall_gran.html commands for related kinds of walls for
|
||||
non-granular particles and simpler wall geometries, respectively.
|
||||
|
||||
Here are snapshots of example models using this command.
|
||||
Corresponding input scripts can be found in examples/granregion.
|
||||
Click on the images to see a bigger picture. Movies of these
|
||||
simulations are "here on the Movies
|
||||
page"_http://lammps.sandia.gov/movies.html#granregion of the
|
||||
LAMMPS web site.
|
||||
|
||||
:image(JPG/gran_funnel_small.jpg,JPG/gran_funnel.png)
|
||||
:image(JPG/gran_mixer_small.jpg,JPG/gran_mixer.png)
|
||||
|
||||
:line
|
||||
|
||||
The distance between a particle and the region boundary is the
|
||||
distance to the nearest point on the region surface. The force the
|
||||
wall exerts on the particle is along the direction between that point
|
||||
and the particle center, which is the direction normal to the surface
|
||||
at that point. Note that if the region surface is comprised of
|
||||
multiple "faces", then each face can exert a force on the particle if
|
||||
it is close enough. E.g. for "region_style block"_region.html, a
|
||||
particle in the interior, near a corner of the block, could feel wall
|
||||
forces from 1, 2, or 3 faces of the block.
|
||||
|
||||
Regions are defined using the "region"_region.html command. Note that
|
||||
the region volume can be interior or exterior to the bounding surface,
|
||||
which will determine in which direction the surface interacts with
|
||||
particles, i.e. the direction of the surface normal. The exception to
|
||||
this is if one or more {open} options are specified for the region
|
||||
command, in which case particles interact with both the interior and
|
||||
exterior surfaces of regions.
|
||||
|
||||
Regions can either be primitive shapes (block, sphere, cylinder, etc)
|
||||
or combinations of primitive shapes specified via the {union} or
|
||||
{intersect} region styles. These latter styles can be used to
|
||||
construct particle containers with complex shapes. Regions can also
|
||||
move dynamically via the "region"_region.html command keywords (move)
|
||||
and {rotate}, or change their shape by use of variables as inputs to
|
||||
the "region"_region.html command. If such a region is used with this
|
||||
fix, then the region surface will move in time in the corresponding
|
||||
manner.
|
||||
|
||||
NOTE: As discussed on the "region"_region.html command doc page,
|
||||
regions in LAMMPS do not get wrapped across periodic boundaries. It
|
||||
is up to you to ensure that the region location with respect to
|
||||
periodic or non-periodic boundaries is specified appropriately via the
|
||||
"region"_region.html and "boundary"_boundary.html commands when using
|
||||
a region as a wall that bounds particle motion.
|
||||
|
||||
NOTE: For primitive regions with sharp corners and/or edges (e.g. a
|
||||
block or cylinder), wall/particle forces are computed accurately for
|
||||
both interior and exterior regions. For {union} and {intersect}
|
||||
regions, additional sharp corners and edges may be present due to the
|
||||
intersection of the surfaces of 2 or more primitive volumes. These
|
||||
corners and edges can be of two types: concave or convex. Concave
|
||||
points/edges are like the corners of a cube as seen by particles in
|
||||
the interior of a cube. Wall/particle forces around these features
|
||||
are computed correctly. Convex points/edges are like the corners of a
|
||||
cube as seen by particles exterior to the cube, i.e. the points jut
|
||||
into the volume where particles are present. LAMMPS does NOT compute
|
||||
the location of these convex points directly, and hence wall/particle
|
||||
forces in the cutoff volume around these points suffer from
|
||||
inaccuracies. The basic problem is that the outward normal of the
|
||||
surface is not continuous at these points. This can cause particles
|
||||
to feel no force (they don't "see" the wall) when in one location,
|
||||
then move a distance epsilon, and suddenly feel a large force because
|
||||
they now "see" the wall. In a worst-case scenario, this can blow
|
||||
particles out of the simulation box. Thus, as a general rule you
|
||||
should not use the fix wall/gran/region command with {union} or
|
||||
{interesect} regions that have convex points or edges resulting from
|
||||
the union/intersection (convex points/edges in the union/intersection
|
||||
due to a single sub-region are still OK).
|
||||
|
||||
NOTE: Similarly, you should not define {union} or {intersert} regions
|
||||
for use with this command that share an overlapping common face that
|
||||
is part of the overall outer boundary (interior boundary is OK), even
|
||||
if the face is smooth. E.g. two regions of style block in a {union}
|
||||
region, where the two blocks overlap on one or more of their faces.
|
||||
This is because LAMMPS discards points that are part of multiple
|
||||
sub-regions when calculating wall/particle interactions, to avoid
|
||||
double-counting the interaction. Having two coincident faces could
|
||||
cause the face to become invisible to the particles. The solution is
|
||||
to make the two faces differ by epsilon in their position.
|
||||
|
||||
The nature of the wall/particle interactions are determined by the
|
||||
{fstyle} setting. It can be any of the styles defined by the
|
||||
"pair_style granular"_pair_gran.html commands. Currently this is
|
||||
{hooke}, {hooke/history}, or {hertz/history}. The equation for the
|
||||
force between the wall and particles touching it is the same as the
|
||||
corresponding equation on the "pair_style granular"_pair_gran.html doc
|
||||
page, but the effective radius is calculated using the radius of the
|
||||
particle and the radius of curvature of the wall at the contact point.
|
||||
|
||||
Specifically, delta = radius - r = overlap of particle with wall,
|
||||
m_eff = mass of particle, and RiRj/Ri+Rj is the effective radius, with
|
||||
Rj replaced by the radius of curvature of the wall at the contact
|
||||
point. The radius of curvature can be negative for a concave wall
|
||||
section, e.g. the interior of cylinder. For a flat wall, delta =
|
||||
radius - r = overlap of particle with wall, m_eff = mass of particle,
|
||||
and the effective radius of contact is just the radius of the
|
||||
particle.
|
||||
|
||||
The parameters {Kn}, {Kt}, {gamma_n}, {gamma_t}, {xmu} and {dampflag}
|
||||
have the same meaning and units as those specified with the
|
||||
"pair_style granular"_pair_gran.html commands. This means a NULL can
|
||||
be used for either {Kt} or {gamma_t} as described on that page. If a
|
||||
NULL is used for {Kt}, then a default value is used where {Kt} = 2/7
|
||||
{Kn}. If a NULL is used for {gamma_t}, then a default value is used
|
||||
where {gamma_t} = 1/2 {gamma_n}.
|
||||
|
||||
Note that you can choose a different force styles and/or different
|
||||
values for the 6 wall/particle coefficients than for particle/particle
|
||||
interactions. E.g. if you wish to model the wall as a different
|
||||
material.
|
||||
|
||||
[Restart, fix_modify, output, run start/stop, minimize info:]
|
||||
|
||||
Similiar to "fix wall/gran"_fix_wall_gran.html command, this fix
|
||||
writes the shear friction state of atoms interacting with the wall to
|
||||
"binary restart files"_restart.html, so that a simulation can continue
|
||||
correctly if granular potentials with shear "history" effects are
|
||||
being used. This fix also includes info about a moving region in the
|
||||
restart file. See the "read_restart"_read_restart.html command for
|
||||
info on how to re-specify a fix in an input script that reads a
|
||||
restart file, so that the operation of the fix continues in an
|
||||
uninterrupted fashion.
|
||||
|
||||
Note that info about region definitions is NOT included in restart
|
||||
files. So you must re-define your region and if it is a moving
|
||||
region, define its motion attributes in a way that is consistent with
|
||||
the simulation that wrote the restart file. In particular, if you
|
||||
want to change its motion attributes (e.g. its velocity), then you
|
||||
should insure the postition/orientation of the region at the initial
|
||||
restart timestep is the same as it was on the timestep the restart
|
||||
file was written. If this is not possible, then you may need to
|
||||
ignore info in the restart file by defining a new fix wall/gran/region
|
||||
command in your restart script (e.g. with a different fix ID).
|
||||
|
||||
None of the "fix_modify"_fix_modify.html options are relevant to this
|
||||
fix. No global or per-atom quantities are stored by this fix for
|
||||
access by various "output commands"_Section_howto.html#howto_15. No
|
||||
parameter of this fix can be used with the {start/stop} keywords of
|
||||
the "run"_run.html command. This fix is not invoked during "energy
|
||||
minimization"_minimize.html.
|
||||
|
||||
[Restrictions:]
|
||||
|
||||
This fix is part of the GRANULAR package. It is only enabled if
|
||||
LAMMPS was built with that package. See the "Making
|
||||
LAMMPS"_Section_start.html#start_3 section for more info.
|
||||
|
||||
[Related commands:]
|
||||
|
||||
"fix_move"_fix_move.html,
|
||||
"fix wall/gran"_fix_wall_gran.html,
|
||||
"fix wall/region"_fix_wall_region.html,
|
||||
"pair_style granular"_pair_gran.html,
|
||||
"region"_region.html
|
||||
|
||||
[Default:] none
|
||||
|
||||
@ -32,6 +32,7 @@ Fixes :h1
|
||||
fix_drag
|
||||
fix_drude
|
||||
fix_drude_transform
|
||||
fix_dpd_energy
|
||||
fix_dt_reset
|
||||
fix_efield
|
||||
fix_ehex
|
||||
@ -148,6 +149,7 @@ Fixes :h1
|
||||
fix_viscous
|
||||
fix_wall
|
||||
fix_wall_gran
|
||||
fix_wall_gran_region
|
||||
fix_wall_piston
|
||||
fix_wall_reflect
|
||||
fix_wall_region
|
||||
|
||||
@ -253,7 +253,7 @@ group mobile dynamic all region ss
|
||||
fix 1 mobile nve
|
||||
run $\{nsteps\}
|
||||
group mobile static
|
||||
run $\{nsteps\} :pre
|
||||
run $\{nsteps\} :pre
|
||||
|
||||
NOTE: All fixes and computes take a group ID as an argument, but they
|
||||
do not all allow for use of a dynamic group. If you get an error
|
||||
|
||||
@ -109,19 +109,19 @@ Here is an example of a double loop which uses the if and
|
||||
"jump"_jump.html commands to break out of the inner loop when a
|
||||
condition is met, then continues iterating thru the outer loop.
|
||||
|
||||
label loopa
|
||||
label loopa
|
||||
variable a loop 5
|
||||
label loopb
|
||||
label loopb
|
||||
variable b loop 5
|
||||
print "A,B = $a,$b"
|
||||
print "A,B = $a,$b"
|
||||
run 10000
|
||||
if "$b > 2" then "jump SELF break"
|
||||
next b
|
||||
jump in.script loopb
|
||||
label break
|
||||
if "$b > 2" then "jump SELF break"
|
||||
next b
|
||||
jump in.script loopb
|
||||
label break
|
||||
variable b delete
|
||||
next a
|
||||
jump SELF loopa :pre
|
||||
next a
|
||||
jump SELF loopa :pre
|
||||
|
||||
:line
|
||||
|
||||
|
||||
@ -103,19 +103,19 @@ Here is an example of a double loop which uses the if and
|
||||
"jump"_jump.html commands to break out of the inner loop when a
|
||||
condition is met, then continues iterating thru the outer loop.
|
||||
|
||||
label loopa
|
||||
label loopa
|
||||
variable a loop 5
|
||||
label loopb
|
||||
label loopb
|
||||
variable b loop 5
|
||||
print "A,B = $a,$b"
|
||||
print "A,B = $a,$b"
|
||||
run 10000
|
||||
if "$b > 2" then "jump SELF break"
|
||||
next b
|
||||
jump in.script loopb
|
||||
label break
|
||||
if "$b > 2" then "jump SELF break"
|
||||
next b
|
||||
jump in.script loopb
|
||||
label break
|
||||
variable b delete
|
||||
next a
|
||||
jump SELF loopa :pre
|
||||
next a
|
||||
jump SELF loopa :pre
|
||||
|
||||
[Restrictions:]
|
||||
|
||||
|
||||
0
doc/src/min_style.txt
Executable file → Normal file
@ -116,19 +116,19 @@ Here is an example of a double loop which uses the "if"_if.html and
|
||||
"jump"_jump.html commands to break out of the inner loop when a
|
||||
condition is met, then continues iterating thru the outer loop.
|
||||
|
||||
label loopa
|
||||
label loopa
|
||||
variable a loop 5
|
||||
label loopb
|
||||
label loopb
|
||||
variable b loop 5
|
||||
print "A,B = $a,$b"
|
||||
print "A,B = $a,$b"
|
||||
run 10000
|
||||
if $b > 2 then "jump in.script break"
|
||||
next b
|
||||
jump in.script loopb
|
||||
label break
|
||||
if $b > 2 then "jump in.script break"
|
||||
next b
|
||||
jump in.script loopb
|
||||
label break
|
||||
variable b delete :pre
|
||||
next a
|
||||
jump in.script loopa :pre
|
||||
next a
|
||||
jump in.script loopa :pre
|
||||
|
||||
[Restrictions:]
|
||||
|
||||
|
||||
0
doc/src/pair_dipole.txt
Executable file → Normal file
@ -33,78 +33,95 @@ pair_coeff * * 3.0 1.0 0.1 2.5 :pre
|
||||
|
||||
[Description:]
|
||||
|
||||
Styles {dpd/fdt} and {dpd/fdt/energy} set the fluctuation-dissipation
|
||||
theorem parameters and compute the conservative force for dissipative
|
||||
particle dynamics (DPD). The conservative force on atom I due to atom
|
||||
J is given by
|
||||
Styles {dpd/fdt} and {dpd/fdt/energy} compute the force for dissipative
|
||||
particle dynamics (DPD) simulations. The {dpd/fdt} style is used to
|
||||
perform DPD simulations under isothermal and isobaric conditions,
|
||||
while the {dpd/fdt/energy} style is used to perform DPD simulations
|
||||
under isoenergetic and isoenthalpic conditions (see "(Lisal)"_#Lisal).
|
||||
For DPD simulations in general, the force on atom I due to atom J is
|
||||
given as a sum of 3 terms
|
||||
|
||||
:c,image(Eqs/pair_dpd_conservative.jpg)
|
||||
:c,image(Eqs/pair_dpd.jpg)
|
||||
|
||||
where the weighting factor, omega_ij, varies between 0 and 1, and is
|
||||
chosen to have the following functional form:
|
||||
where Fc is a conservative force, Fd is a dissipative force, and Fr is
|
||||
a random force. Rij is a unit vector in the direction Ri - Rj, Vij is
|
||||
the vector difference in velocities of the two atoms = Vi - Vj, alpha
|
||||
is a Gaussian random number with zero mean and unit variance, dt is
|
||||
the timestep size, and w(r) is a weighting factor that varies between
|
||||
0 and 1. Rc is the cutoff. The weighting factor, omega_ij, varies
|
||||
between 0 and 1, and is chosen to have the following functional form:
|
||||
|
||||
:c,image(Eqs/pair_dpd_omega.jpg)
|
||||
|
||||
where Rij is a unit vector in the direction Ri - Rj, and Rc is the
|
||||
cutoff. Note that alternative definitions of the weighting function
|
||||
exist, but would have to be implemented as a separate pair style
|
||||
command.
|
||||
Note that alternative definitions of the weighting function exist, but
|
||||
would have to be implemented as a separate pair style command.
|
||||
|
||||
These pair style differ from the other dpd styles in that the
|
||||
dissipative and random forces are not computed within the pair style.
|
||||
This style can be combined with the "fix shardlow"_fix_shardlow.html
|
||||
to perform the stochastic integration of the dissipative and random
|
||||
forces through the Shardlow splitting algorithm approach.
|
||||
For style {dpd/fdt}, the fluctuation-dissipation theorem defines gamma
|
||||
to be set equal to sigma*sigma/(2 T), where T is the set point
|
||||
temperature specified as a pair style parameter in the above examples.
|
||||
The following coefficients must be defined for each pair of atoms types
|
||||
via the "pair_coeff"_pair_coeff.html command as in the examples above,
|
||||
or in the data file or restart files read by the
|
||||
"read_data"_read_data.html or "read_restart"_read_restart.html commands:
|
||||
|
||||
A (force units)
|
||||
sigma (force*time^(1/2) units)
|
||||
cutoff (distance units) :ul
|
||||
|
||||
The last coefficient is optional. If not specified, the global DPD
|
||||
cutoff is used.
|
||||
|
||||
Style {dpd/fdt/energy} is used to perform DPD simulations
|
||||
under isoenergetic and isoenthalpic conditions. The fluctuation-dissipation
|
||||
theorem defines gamma to be set equal to sigma*sigma/(2 dpdTheta), where
|
||||
dpdTheta is the average internal temperature for the pair. The particle
|
||||
internal temperature is related to the particle internal energy through
|
||||
a mesoparticle equation of state (see "fix eos"_fix.html). The
|
||||
differential internal conductive and mechanical energies are computed
|
||||
within style {dpd/fdt/energy} as:
|
||||
|
||||
:c,image(Eqs/pair_dpd_energy.jpg)
|
||||
|
||||
where
|
||||
|
||||
:c,image(Eqs/pair_dpd_energy_terms.jpg)
|
||||
|
||||
Zeta_ij^q is a second Gaussian random number with zero mean and unit
|
||||
variance that is used to compute the internal conductive energy. The
|
||||
fluctuation-dissipation theorem defines alpha*alpha to be set
|
||||
equal to 2*kB*kappa, where kappa is the mesoparticle thermal
|
||||
conductivity parameter. The following coefficients must be defined for
|
||||
each pair of atoms types via the "pair_coeff"_pair_coeff.html
|
||||
command as in the examples above, or in the data file or restart files
|
||||
read by the "read_data"_read_data.html or "read_restart"_read_restart.html
|
||||
commands:
|
||||
|
||||
A (force units)
|
||||
sigma (force*time^(1/2) units)
|
||||
kappa (energy*temperature/time units)
|
||||
cutoff (distance units) :ul
|
||||
|
||||
The last coefficient is optional. If not specified, the global DPD
|
||||
cutoff is used.
|
||||
|
||||
The pairwise energy associated with styles {dpd/fdt} and
|
||||
{dpd/fdt/energy} is only due to the conservative force term Fc, and is
|
||||
shifted to be zero at the cutoff distance Rc. The pairwise virial is
|
||||
calculated using only the conservative term.
|
||||
|
||||
For style {dpd/fdt}, the fluctuation-dissipation theorem defines gamma
|
||||
to be set equal to sigma*sigma/(2 T), where T is the set point
|
||||
temperature specified as a pair style parameter in the above examples.
|
||||
This style can be combined with "fix shardlow"_fix_shardlow.html to
|
||||
perform DPD simulations under isothermal and isobaric conditions (see
|
||||
"(Lisal)"_#Lisal). The following coefficients must be defined for
|
||||
each pair of atoms types via the "pair_coeff"_pair_coeff.html command
|
||||
as in the examples above, or in the data file or restart files read by
|
||||
the "read_data"_read_data.html or "read_restart"_read_restart.html
|
||||
commands:
|
||||
|
||||
A (force units)
|
||||
sigma (force*time^(1/2) units)
|
||||
cutoff (distance units) :ul
|
||||
|
||||
The last coefficient is optional. If not specified, the global DPD
|
||||
cutoff is used.
|
||||
|
||||
For style {dpd/fdt/energy}, the fluctuation-dissipation theorem
|
||||
defines gamma to be set equal to sigma*sigma/(2 dpdTheta), where
|
||||
dpdTheta is the average internal temperature for the pair.
|
||||
Furthermore, the fluctuation-dissipation defines alpha*alpha to be set
|
||||
equal to 2*kB*kappa, where kappa is the mesoparticle thermal
|
||||
conductivity parameter. This style can be combined with "fix
|
||||
shardlow"_fix_shardlow.html to perform DPD simulations under
|
||||
isoenergetic and isoenthalpic conditions (see "(Lisal)"_#Lisal). The
|
||||
following coefficients must be defined for each pair of atoms types
|
||||
via the "pair_coeff"_pair_coeff.html command as in the examples above,
|
||||
or in the data file or restart files read by the
|
||||
"read_data"_read_data.html or "read_restart"_read_restart.html
|
||||
commands:
|
||||
|
||||
A (force units)
|
||||
sigma (force*time^(1/2) units)
|
||||
kappa (1/time units)
|
||||
cutoff (distance units) :ul
|
||||
|
||||
The last coefficient is optional. If not specified, the global DPD
|
||||
cutoff is used.
|
||||
|
||||
For style {dpd/fdt/energy}, the particle internal temperature is
|
||||
related to the particle internal energy through a mesoparticle
|
||||
equation of state. Thus, an an additional "fix eos"_fix.html must be
|
||||
specified.
|
||||
The forces computed through the {dpd/fdt} and {dpd/fdt/energy} styles
|
||||
can be integrated with the velocity-Verlet integration scheme or the
|
||||
Shardlow splitting integration scheme described by "(Lisal)"_#Lisal.
|
||||
In the cases when these pair styles are combined with the
|
||||
"fix shardlow"_fix_shardlow.html, these pair styles differ from the
|
||||
other dpd styles in that the dissipative and random forces are split
|
||||
from the force calculation and are not computed within the pair style.
|
||||
Thus, only the conservative force is computed by the pair style,
|
||||
while the stochastic integration of the dissipative and random forces
|
||||
are handled through the Shardlow splitting algorithm approach. The
|
||||
Shardlow splitting algorithm is advantageous, especially when
|
||||
performing DPD under isoenergetic conditions, as it allows
|
||||
significantly larger timesteps to be taken.
|
||||
|
||||
:line
|
||||
|
||||
@ -132,6 +149,6 @@ energies and temperatures.
|
||||
|
||||
:link(Lisal)
|
||||
[(Lisal)] M. Lisal, J.K. Brennan, J. Bonet Avalos, "Dissipative
|
||||
particle dynamics as isothermal, isobaric, isoenergetic, and
|
||||
particle dynamics at isothermal, isobaric, isoenergetic, and
|
||||
isoenthalpic conditions using Shardlow-like splitting algorithms.",
|
||||
J. Chem. Phys., 135, 204105 (2011).
|
||||
|
||||
0
doc/src/pair_gayberne.txt
Executable file → Normal file
@ -170,7 +170,7 @@ so that there is effectively no interaction (e.g. epsilon = 0.0 in a
|
||||
LJ potential). Or, for {hybrid} and {hybrid/overlay} simulations, you
|
||||
can use this form of the pair_coeff command in your input script:
|
||||
|
||||
pair_coeff 2 3 none :pre
|
||||
pair_coeff 2 3 none :pre
|
||||
|
||||
or this form in the "Pair Coeffs" section of the data file:
|
||||
|
||||
|
||||
@ -188,9 +188,9 @@ lattce(I,J) = lattice structure of I-J reference structure:
|
||||
bcc = body centered cubic
|
||||
dim = dimer
|
||||
b1 = rock salt (NaCl structure)
|
||||
hcp = hexagonal close-packed
|
||||
c11 = MoSi2 structure
|
||||
l12 = Cu3Au structure (lower case L, followed by 12)
|
||||
hcp = hexagonal close-packed
|
||||
c11 = MoSi2 structure
|
||||
l12 = Cu3Au structure (lower case L, followed by 12)
|
||||
b2 = CsCl structure (interpenetrating simple cubic)
|
||||
nn2(I,J) = turn on second-nearest neighbor MEAM formulation for
|
||||
I-J pair (see for example "(Lee)"_#Lee).
|
||||
|
||||
@ -41,7 +41,9 @@ supplemental information of the following paper: "(Chenoweth et al.,
|
||||
2008)"_#Chenoweth_2008. The version integrated into LAMMPS matches
|
||||
the most up-to-date version of ReaxFF as of summer 2010. For more
|
||||
technical details about the pair reax/c implementation of ReaxFF, see
|
||||
the "(Aktulga)"_#Aktulga paper.
|
||||
the "(Aktulga)"_#Aktulga paper. The {reax/c} style was initially
|
||||
implemented as a stand-alone C code and is now integrated into LAMMPS
|
||||
as a package.
|
||||
|
||||
The {reax/c/kk} style is a Kokkos version of the ReaxFF potential that is
|
||||
derived from the {reax/c} style. The Kokkos version can run on GPUs and
|
||||
@ -163,11 +165,11 @@ To print these quantities to the log file (with descriptive column
|
||||
headings) the following commands could be included in an input script:
|
||||
|
||||
compute reax all pair reax/c
|
||||
variable eb equal c_reax\[1\]
|
||||
variable ea equal c_reax\[2\]
|
||||
variable eb equal c_reax\[1\]
|
||||
variable ea equal c_reax\[2\]
|
||||
\[...\]
|
||||
variable eqeq equal c_reax\[14\]
|
||||
thermo_style custom step temp epair v_eb v_ea ... v_eqeq :pre
|
||||
variable eqeq equal c_reax\[14\]
|
||||
thermo_style custom step temp epair v_eb v_ea \[...\] v_eqeq :pre
|
||||
|
||||
Only a single pair_coeff command is used with the {reax/c} style which
|
||||
specifies a ReaxFF potential file with parameters for all needed
|
||||
@ -237,7 +239,7 @@ nbrhood_cutoff: Denotes the near neighbors cutoff (in Angstroms)
|
||||
regarding the bonded interactions. (default value = 5.0)
|
||||
|
||||
hbond_cutoff: Denotes the cutoff distance (in Angstroms) for hydrogen
|
||||
bond interactions.(default value = 7.5. Value of 0.0 turns off
|
||||
bond interactions.(default value = 7.5. A value of 0.0 turns off
|
||||
hydrogen bonds)
|
||||
|
||||
bond_graph_cutoff: is the threshold used in determining what is a
|
||||
|
||||
0
doc/src/pair_resquared.txt
Executable file → Normal file
4
doc/src/pair_smtbq.txt
Executable file → Normal file
@ -158,7 +158,7 @@ Divided line :ul
|
||||
3) Potential parameters:
|
||||
|
||||
Keyword for element1, element2 and interaction potential ('second_moment' or 'buck' or 'buckPlusAttr') between element 1 and 2. If the potential is 'second_moment', specify 'oxide' or 'metal' for metal-oxygen or metal-metal interactions respectively.
|
||||
Potential parameter: <pre><br/> If type of potential is 'second_moment' : {A (eV)}, {p}, {ξ<sup>0</sup>} (eV) and {q} <br/> {r<sub>c1</sub>} (Å), {r<sub>c2</sub>} (Å) and {r<sub>0</sub>} (Å) <br/> If type of potential is 'buck' : {C} (eV) and {ρ} (Å) <br/> If type of potential is 'buckPlusAttr' : {C} (eV) and {ρ} (Å) <br/> {D} (eV), {B} (Å<sup>-1</sup>), {r<sub>1</sub><sup>OO</sup>} (Å) and {r<sub>2</sub><sup>OO</sup>} (Å) </pre>
|
||||
Potential parameter: <pre><br/> If type of potential is 'second_moment' : {A (eV)}, {p}, {ξ<sup>0</sup>} (eV) and {q} <br/> {r<sub>c1</sub>} (Å), {r<sub>c2</sub>} (Å) and {r<sub>0</sub>} (Å) <br/> If type of potential is 'buck' : {C} (eV) and {ρ} (Å) <br/> If type of potential is 'buckPlusAttr' : {C} (eV) and {ρ} (Å) <br/> {D} (eV), {B} (Å<sup>-1</sup>), {r<sub>1</sub><sup>OO</sup>} (Å) and {r<sub>2</sub><sup>OO</sup>} (Å) </pre>
|
||||
Divided line :ul
|
||||
|
||||
4) Tables parameters:
|
||||
@ -185,7 +185,7 @@ Divided line :ul
|
||||
|
||||
8) Mode for the electronegativity equalization (Qeq) :
|
||||
|
||||
Keyword mode: <pre> <br/> QEqAll (one QEq group) | no parameters <br/> QEqAllParallel (several QEq groups) | no parameters <br/> Surface | zlim (QEq only for z>zlim) </pre>
|
||||
Keyword mode: <pre> <br/> QEqAll (one QEq group) | no parameters <br/> QEqAllParallel (several QEq groups) | no parameters <br/> Surface | zlim (QEq only for z>zlim) </pre>
|
||||
Parameter if necessary
|
||||
Divided line :ul
|
||||
|
||||
|
||||
@ -96,15 +96,15 @@ tantalum potential provided in the LAMMPS potentials directory
|
||||
combines the {snap} and {zbl} pair styles. It is invoked
|
||||
by the following commands:
|
||||
|
||||
variable zblcutinner equal 4
|
||||
variable zblcutouter equal 4.8
|
||||
variable zblz equal 73
|
||||
pair_style hybrid/overlay &
|
||||
zbl $\{zblcutinner\} $\{zblcutouter\} snap
|
||||
pair_coeff * * zbl 0.0
|
||||
pair_coeff 1 1 zbl $\{zblz\}
|
||||
pair_coeff * * snap ../potentials/Ta06A.snapcoeff Ta &
|
||||
../potentials/Ta06A.snapparam Ta :pre
|
||||
variable zblcutinner equal 4
|
||||
variable zblcutouter equal 4.8
|
||||
variable zblz equal 73
|
||||
pair_style hybrid/overlay &
|
||||
zbl $\{zblcutinner\} $\{zblcutouter\} snap
|
||||
pair_coeff * * zbl 0.0
|
||||
pair_coeff 1 1 zbl $\{zblz\}
|
||||
pair_coeff * * snap ../potentials/Ta06A.snapcoeff Ta &
|
||||
../potentials/Ta06A.snapparam Ta :pre
|
||||
|
||||
It is convenient to keep these commands in a separate file that can
|
||||
be inserted in any LAMMPS input script using the "include"_include.html
|
||||
|
||||
@ -191,13 +191,18 @@ input script should specify all fixes it will use. However, note that
|
||||
some fixes store an internal "state" which is written to the restart
|
||||
file. This allows the fix to continue on with its calculations in a
|
||||
restarted simulation. To re-enable such a fix, the fix command in the
|
||||
new input script must use the same fix-ID and group-ID as was used in
|
||||
the input script that wrote the restart file. If a match is found,
|
||||
LAMMPS prints a message indicating that the fix is being re-enabled.
|
||||
If no match is found before the first run or minimization is performed
|
||||
by the new script, the "state" information for the saved fix is
|
||||
discarded. See the doc pages for individual fixes for info on which
|
||||
ones can be restarted in this manner.
|
||||
new input script must be of the same style and use the same fix-ID as
|
||||
was used in the input script that wrote the restart file.
|
||||
|
||||
If a match is found, LAMMPS prints a message indicating that the fix
|
||||
is being re-enabled. If no match is found before the first run or
|
||||
minimization is performed by the new script, the "state" information
|
||||
for the saved fix is discarded. LAMMPS will also print a list of
|
||||
fixes for which the information is being discarded. See the doc pages
|
||||
for individual fixes for info on which ones can be restarted in this
|
||||
manner. Note that fixes which are created internally by other LAMMPS
|
||||
commands (computes, fixes, etc) will have style names which are
|
||||
all-capitalized, and IDs which are generated internally.
|
||||
|
||||
Likewise, the "computes"_fix.html used for a simulation are not stored
|
||||
in the restart file. This means the new input script should specify
|
||||
@ -213,6 +218,14 @@ re-created fix will be re-enabled with the stored state information as
|
||||
described in the previous paragraph, so that the compute can continue
|
||||
its calculations in a consistent manner.
|
||||
|
||||
NOTE: There are a handful of commands which can be used before or
|
||||
between runs which require a system initialization. Examples include
|
||||
the "balance", "displace_atoms", and "delete_atoms" commands. This is
|
||||
because they may migrate atoms to new processors. Thus they will also
|
||||
discard unused "state" information from fixes. This means that, if
|
||||
desired, you must re-specify the relevant fixes and computes (which
|
||||
create fixes) before those commands are used.
|
||||
|
||||
Some pair styles, like the "granular pair styles"_pair_gran.html, also
|
||||
use a fix to store "state" information that persists from timestep to
|
||||
timestep. In the case of granular potentials, it is contact
|
||||
|
||||