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70 Commits

Author SHA1 Message Date
63e71cd45b patch to add DPD-VV 2016-10-12 07:35:47 -06:00
4a5d9eaae2 Merge pull request #217 from akohlmey/small-fixes
Collected small changes and bugfixes
2016-10-12 07:32:08 -06:00
4e3a55047f Merge pull request #215 from timattox/USER-DPD_bugfix_for_dtsqrt
USER-DPD Bugfix: reset_dt() is not called when I thought it should be called.
2016-10-12 07:30:10 -06:00
f8a26dd158 update Timer::force_timeout() to trigger at next loop iteration 2016-10-12 07:26:03 -04:00
c24bf512f3 update #include statements for system includes 2016-10-12 00:00:53 -04:00
6b4ab0a390 update .gitignore 2016-10-12 00:00:21 -04:00
adc98e07df whitespace cleanup in USER-DPD 2016-10-11 23:58:36 -04:00
39a22039e9 correct broken link 2016-10-11 23:57:40 -04:00
b75860048b updates for recent changes to the manual 2016-10-11 23:50:45 -04:00
0eb7fbf34d tweaks to new USER-DPD docs 2016-10-11 15:43:59 -06:00
2f07a627a2 Forgot to remove my call to reset_dt() 2016-10-11 16:30:41 -04:00
559637f4bc USER-DPD Bugfix: reset_dt() is not called when I thought it should be called.
Move the calculation of dtsqrt inside FixShardlow::initial_integrate()
2016-10-11 16:11:29 -04:00
fbf7df14b5 Merge pull request #212 from timattox/USER-DPD_fix_eos_atom_style_checks
USER-DPD: Add atom_style compatibility checks in fix_eos_*.cpp files.
2016-10-11 13:40:00 -06:00
6f1162927a Merge pull request #207 from timattox/USER-DPD_new_VV_for_DPD
USER-DPD: add support for using VV with DPD
2016-10-11 13:39:25 -06:00
803dc57bfa Merge pull request #214 from akohlmey/make-no-lib-no-mpiio
make no-lib should also remove MPIIO and USER-LB packages
2016-10-11 12:42:53 -06:00
3e8e2911cc Merge pull request #213 from akohlmey/improper-virial-bugfixes
Improper virial bugfixes
2016-10-11 12:42:08 -06:00
04f5eadcf1 added LAST option to dump_modify thresh, more restart info printed out to screen 2016-10-11 12:39:52 -06:00
b00b40bccd make no-lib should also remove MPIIO and USER-LB packages 2016-10-11 08:03:59 -04:00
ef079ae4eb bugfix for AngleAngle term in CLASS2 impropers by Ivan A. Strelnikov, ICP RAS
this closes #56
2016-10-10 23:56:36 -04:00
bb0bfd508b Merge branch 'master' into improper-virial-bugfixes 2016-10-10 23:55:36 -04:00
e70d530c46 Merge pull request #203 from rbberger/txt2rst-external-link-fix
txt2rst external link fix
2016-10-10 13:59:27 -06:00
ed8cc82713 Merge pull request #211 from akohlmey/add-respa-to-fix-flow-gauss
Add respa support to fix flow/gauss
2016-10-10 13:59:01 -06:00
27dac02466 Merge pull request #209 from akohlmey/static-double-deallocation-workaround
workaround for double free issue when using USER-COLVARS with with lammps python wrapper and python package
2016-10-10 13:58:16 -06:00
467bcad0a0 Merge pull request #204 from rbberger/fix-user-omp
Migrate changes from GRANULAR to USER-OMP
2016-10-10 13:57:37 -06:00
a2b0840064 USER-DPD: Add atom_style compatibility checks in fix_eos_*.cpp files. 2016-10-10 13:40:33 -04:00
144e6a8091 whitespace cleanup 2016-10-10 09:40:09 -04:00
72ac073412 edited documentation
(cherry picked from commit eff14c74b0)
2016-10-10 09:38:54 -04:00
49c45ab03b edited documentation
(cherry picked from commit fd560889c3)
2016-10-10 09:38:53 -04:00
c2cd439944 first draft of documentation for respa
(cherry picked from commit d7dcbcfbd9)
2016-10-10 09:38:53 -04:00
e96ebb29bc adjusted default respa level to be outermost
(cherry picked from commit 7fc4d46a41)
2016-10-10 09:38:53 -04:00
3ce178d43f now understand how respa works in lammps
(cherry picked from commit c829027e83)
2016-10-10 09:38:52 -04:00
23781d6ec9 added respa to fix_flow_gauss, not fully understood yet
(cherry picked from commit 8d9737b04d)
2016-10-10 09:38:52 -04:00
fca6d721c0 completed synchronization with non-threaded version 2016-10-10 09:16:21 -04:00
dd192ca7ea whitespace cleanup 2016-10-10 09:15:42 -04:00
683689c808 revert to previous style conventions for size_t constants 2016-10-08 11:00:23 -04:00
e01e90eb96 workaround for double free issue when using USER-COLVARS with lammps code loaded as shared library into a standalone executable 2016-10-08 10:45:22 -04:00
9507a786f0 USER-DPD: whitespace and indentation fixes 2016-10-07 15:59:47 -04:00
9789f047d7 USER-DPD: update the USER/dpd examples and their reference outputs 2016-10-07 15:55:35 -04:00
e27ed6c94a USER-DPD: Added support to use VV integrator with USER-DPD if desired.
Includes documentation and examples.
NOTE: VV requires very small timesteps under isoenergetic conditions.
Consider using fix_shardlow instead, since this VV support is
primarily for comparison purposes.
2016-10-07 15:03:30 -04:00
615a2da044 Migrate changes from GRANULAR to USER-OMP 2016-10-06 21:48:06 -04:00
7f3a7c5cbe Fix broken link 2016-10-06 20:33:24 -04:00
e78b4267b7 Fix issue with external links containing anchors 2016-10-06 20:29:07 -04:00
e9fed80928 Merge pull request #202 from akohlmey/doc-formatting-fixes
collected documentation updates and corrections from LAMMPS-ICMS
2016-10-06 15:49:44 -06:00
54fc194e5b Merge pull request #199 from akohlmey/small-changes
Collected small changes and bugfixes
2016-10-06 15:49:24 -06:00
b3d2fb91bb new fix wall/gran/region command, REBO bug fix, new example log files 2016-10-06 15:47:41 -06:00
19984c9bd1 Revert "bugfix for AngleAngle term in CLASS2 impropers by Ivan A. Strelnikov, ICP RAS"
This reverts commit 83bcdb6a50.
2016-10-06 17:23:10 -04:00
f92618a33b Revert "bugfix for virial tally for improper style umbrella from Steven Vandenbrande (U Gent)"
This reverts commit 4921dc18a0.
2016-10-06 17:21:38 -04:00
887981cfaa bugfix for virial tally for improper style umbrella from Steven Vandenbrande (U Gent)
this closes #182

(cherry picked from commit 4921dc18a0)
2016-10-06 17:20:22 -04:00
0b5d71537a collected documentation updates and corrections from LAMMPS-ICMS
fixes formatting issues due to tabs, permission issues and
a few typos and badly worded text.
2016-10-06 15:48:18 -04:00
c213457550 Merge pull request #197 from giacomofiorin/colvars_2016-10-05
Colvars 2016-10-05
2016-10-06 13:02:52 -06:00
0f45cd61a5 Merge pull request #196 from akohlmey/charmm-cmap-updates
Some more cmap-related updates for ch2lmp
2016-10-06 13:02:27 -06:00
493873fb93 clean up doc src 2016-10-06 13:00:46 -06:00
60a031ebac Merge branch 'USER-DPD_pair_exp6_rx_mathfix' of https://github.com/timattox/lammps_USER-DPD into small-changes
This closes #201
2016-10-06 14:28:08 -04:00
27e76a70b9 Merge branch 'USER-DPD_hybrid_atom_bugfix' of https://github.com/timattox/lammps_USER-DPD into small-changes
This closes #200
2016-10-06 14:27:27 -04:00
e1e9a5c126 USER-DPD: math corrections in pair_exp6_rx.cpp (by Jim Larentzos) 2016-10-06 13:49:47 -04:00
d31121b18c USER-DPD: bugfix in unpack_comm_hybrid(); now works with hybrid atom style 2016-10-06 13:21:27 -04:00
0853cdbe6f update reference data files for updated/corrected clayff parameters 2016-10-06 11:47:08 -04:00
83bcdb6a50 bugfix for AngleAngle term in CLASS2 impropers by Ivan A. Strelnikov, ICP RAS
this closes #56
2016-10-06 11:27:18 -04:00
22ce671804 improved whitespace handling in msi2lmp for force fields and topologies 2016-10-06 11:16:59 -04:00
4921dc18a0 bugfix for virial tally for improper style umbrella from Steven Vandenbrande (U Gent)
this closes #182
2016-10-06 10:47:08 -04:00
d133167bf6 Merge branch 'master' of https://github.com/albapa/lammps into small-changes
USER-QUIP related improvements from github user albapa. This closes #198
2016-10-06 09:32:50 -04:00
8ea063378e add NETCDF libs (as defined in QUIP) to the linking line if QUIP was built with NETCDF support 2016-10-06 12:16:25 +01:00
fd16118cbb removed dump_modify command 2016-10-06 12:02:41 +01:00
f9f955d5b5 update include statement format 2016-10-05 22:34:44 -04:00
d7d321a512 some more updates to the README file to reflect the inclusion of the CMAP example and renamed file names 2016-10-05 18:41:45 -04:00
8809a603fb Colvars update: issue a warning that cannot be ignored regarding total forces 2016-10-05 18:26:21 -04:00
969d3cf4b0 Colvars update: make ABF check that the colvar isn't using already subtractAppliedForce 2016-10-05 18:25:40 -04:00
326fdf2cf1 added 1GB1 example from Robert Latour and update 1AC7 example files 2016-10-05 18:20:09 -04:00
f32819dd10 added tweak to write out the command line used for the conversion to the beginning of the LAMMPS input 2016-10-05 18:13:46 -04:00
c07a01c661 import updated README file for charmm2lammps.pl with CMAP support 2016-10-05 18:11:52 -04:00
720 changed files with 101555 additions and 25054 deletions

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@ -1,4 +1,4 @@
LAMMPS (15 Feb 2016)
LAMMPS (6 Oct 2016)
# FENE beadspring benchmark
units lj
@ -43,25 +43,25 @@ Neighbor list info ...
master list distance cutoff = 1.52
ghost atom cutoff = 1.52
binsize = 0.76 -> bins = 45 45 45
Memory usage per processor = 11.5189 Mbytes
Memory usage per processor = 12.0423 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0.97029772 0.44484087 20.494523 22.394765 4.6721833
100 0.9729966 0.4361122 20.507698 22.40326 4.6548819
Loop time of 0.978585 on 1 procs for 100 steps with 32000 atoms
Loop time of 0.977647 on 1 procs for 100 steps with 32000 atoms
Performance: 105948.895 tau/day, 102.188 timesteps/s
100.0% CPU use with 1 MPI tasks x no OpenMP threads
Performance: 106050.541 tau/day, 102.286 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 | 0.19562 | 0.19562 | 0.19562 | 0.0 | 19.99
Bond | 0.087475 | 0.087475 | 0.087475 | 0.0 | 8.94
Neigh | 0.44861 | 0.44861 | 0.44861 | 0.0 | 45.84
Comm | 0.032932 | 0.032932 | 0.032932 | 0.0 | 3.37
Output | 0.00010395 | 0.00010395 | 0.00010395 | 0.0 | 0.01
Modify | 0.19413 | 0.19413 | 0.19413 | 0.0 | 19.84
Other | | 0.01972 | | | 2.02
Pair | 0.19421 | 0.19421 | 0.19421 | 0.0 | 19.86
Bond | 0.08741 | 0.08741 | 0.08741 | 0.0 | 8.94
Neigh | 0.45791 | 0.45791 | 0.45791 | 0.0 | 46.84
Comm | 0.032649 | 0.032649 | 0.032649 | 0.0 | 3.34
Output | 0.00012207 | 0.00012207 | 0.00012207 | 0.0 | 0.01
Modify | 0.18071 | 0.18071 | 0.18071 | 0.0 | 18.48
Other | | 0.02464 | | | 2.52
Nlocal: 32000 ave 32000 max 32000 min
Histogram: 1 0 0 0 0 0 0 0 0 0

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@ -1,4 +1,4 @@
LAMMPS (15 Feb 2016)
LAMMPS (6 Oct 2016)
# FENE beadspring benchmark
units lj
@ -43,25 +43,25 @@ Neighbor list info ...
master list distance cutoff = 1.52
ghost atom cutoff = 1.52
binsize = 0.76 -> bins = 45 45 45
Memory usage per processor = 3.91518 Mbytes
Memory usage per processor = 4.14663 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0.97029772 0.44484087 20.494523 22.394765 4.6721833
100 0.97145835 0.43803883 20.502691 22.397872 4.626988
Loop time of 0.271187 on 4 procs for 100 steps with 32000 atoms
Loop time of 0.269205 on 4 procs for 100 steps with 32000 atoms
Performance: 382319.453 tau/day, 368.749 timesteps/s
99.6% CPU use with 4 MPI tasks x no OpenMP threads
Performance: 385133.446 tau/day, 371.464 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 | 0.048621 | 0.050076 | 0.051229 | 0.4 | 18.47
Bond | 0.022254 | 0.022942 | 0.023567 | 0.3 | 8.46
Neigh | 0.11873 | 0.11881 | 0.11887 | 0.0 | 43.81
Comm | 0.019066 | 0.021357 | 0.024297 | 1.3 | 7.88
Output | 5.0068e-05 | 5.5015e-05 | 6.1035e-05 | 0.1 | 0.02
Modify | 0.048737 | 0.050198 | 0.051231 | 0.4 | 18.51
Other | | 0.007751 | | | 2.86
Pair | 0.049383 | 0.049756 | 0.049988 | 0.1 | 18.48
Bond | 0.022701 | 0.022813 | 0.022872 | 0.0 | 8.47
Neigh | 0.11982 | 0.12002 | 0.12018 | 0.0 | 44.58
Comm | 0.020274 | 0.021077 | 0.022348 | 0.5 | 7.83
Output | 5.3167e-05 | 5.6148e-05 | 6.3181e-05 | 0.1 | 0.02
Modify | 0.046276 | 0.046809 | 0.047016 | 0.1 | 17.39
Other | | 0.008669 | | | 3.22
Nlocal: 8000 ave 8030 max 7974 min
Histogram: 1 0 0 1 0 1 0 0 0 1

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@ -1,4 +1,4 @@
LAMMPS (15 Feb 2016)
LAMMPS (6 Oct 2016)
# FENE beadspring benchmark
variable x index 1
@ -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
Memory usage per processor = 12.8735 Mbytes
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
100 0.97682955 0.44239968 20.500229 22.407862 4.6527025
Loop time of 1.20889 on 4 procs for 100 steps with 128000 atoms
Loop time of 1.14845 on 4 procs for 100 steps with 128000 atoms
Performance: 85764.410 tau/day, 82.720 timesteps/s
99.8% CPU use with 4 MPI tasks x no OpenMP threads
Performance: 90277.919 tau/day, 87.074 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 | 0.21738 | 0.23306 | 0.23926 | 1.9 | 19.28
Bond | 0.094536 | 0.10196 | 0.10534 | 1.4 | 8.43
Neigh | 0.52311 | 0.52392 | 0.52519 | 0.1 | 43.34
Comm | 0.090161 | 0.10022 | 0.12557 | 4.7 | 8.29
Output | 0.00012207 | 0.00017327 | 0.00019598 | 0.2 | 0.01
Modify | 0.19662 | 0.20262 | 0.20672 | 0.8 | 16.76
Other | | 0.04694 | | | 3.88
Pair | 0.2203 | 0.22207 | 0.22386 | 0.3 | 19.34
Bond | 0.094861 | 0.095302 | 0.095988 | 0.1 | 8.30
Neigh | 0.52127 | 0.5216 | 0.52189 | 0.0 | 45.42
Comm | 0.079585 | 0.082159 | 0.084366 | 0.7 | 7.15
Output | 0.00013304 | 0.00015306 | 0.00018501 | 0.2 | 0.01
Modify | 0.18351 | 0.18419 | 0.1856 | 0.2 | 16.04
Other | | 0.04298 | | | 3.74
Nlocal: 32000 ave 32015 max 31983 min
Histogram: 1 0 1 0 0 0 0 0 1 1

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@ -1,4 +1,4 @@
LAMMPS (15 Feb 2016)
LAMMPS (6 Oct 2016)
# LAMMPS benchmark of granular flow
# chute flow of 32000 atoms with frozen base at 26 degrees
@ -47,24 +47,24 @@ Neighbor list info ...
master list distance cutoff = 1.1
ghost atom cutoff = 1.1
binsize = 0.55 -> bins = 73 37 68
Memory usage per processor = 15.567 Mbytes
Step Atoms KinEng 1 Volume
Memory usage per processor = 16.0904 Mbytes
Step Atoms KinEng c_1 Volume
0 32000 784139.13 1601.1263 29833.783
100 32000 784292.08 1571.0968 29834.707
Loop time of 0.550482 on 1 procs for 100 steps with 32000 atoms
Loop time of 0.534174 on 1 procs for 100 steps with 32000 atoms
Performance: 1569.534 tau/day, 181.659 timesteps/s
100.1% CPU use with 1 MPI tasks x no OpenMP threads
Performance: 1617.451 tau/day, 187.205 timesteps/s
99.8% CPU use with 1 MPI tasks x no OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 0.33849 | 0.33849 | 0.33849 | 0.0 | 61.49
Neigh | 0.040353 | 0.040353 | 0.040353 | 0.0 | 7.33
Comm | 0.018023 | 0.018023 | 0.018023 | 0.0 | 3.27
Output | 0.00020385 | 0.00020385 | 0.00020385 | 0.0 | 0.04
Modify | 0.13155 | 0.13155 | 0.13155 | 0.0 | 23.90
Other | | 0.02186 | | | 3.97
Pair | 0.33346 | 0.33346 | 0.33346 | 0.0 | 62.43
Neigh | 0.043902 | 0.043902 | 0.043902 | 0.0 | 8.22
Comm | 0.018391 | 0.018391 | 0.018391 | 0.0 | 3.44
Output | 0.00022411 | 0.00022411 | 0.00022411 | 0.0 | 0.04
Modify | 0.11666 | 0.11666 | 0.11666 | 0.0 | 21.84
Other | | 0.02153 | | | 4.03
Nlocal: 32000 ave 32000 max 32000 min
Histogram: 1 0 0 0 0 0 0 0 0 0

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@ -1,4 +1,4 @@
LAMMPS (15 Feb 2016)
LAMMPS (6 Oct 2016)
# LAMMPS benchmark of granular flow
# chute flow of 32000 atoms with frozen base at 26 degrees
@ -47,24 +47,24 @@ Neighbor list info ...
master list distance cutoff = 1.1
ghost atom cutoff = 1.1
binsize = 0.55 -> bins = 73 37 68
Memory usage per processor = 6.81783 Mbytes
Step Atoms KinEng 1 Volume
Memory usage per processor = 7.04927 Mbytes
Step Atoms KinEng c_1 Volume
0 32000 784139.13 1601.1263 29833.783
100 32000 784292.08 1571.0968 29834.707
Loop time of 0.13141 on 4 procs for 100 steps with 32000 atoms
Loop time of 0.171815 on 4 procs for 100 steps with 32000 atoms
Performance: 6574.833 tau/day, 760.976 timesteps/s
99.3% CPU use with 4 MPI tasks x no OpenMP threads
Performance: 5028.653 tau/day, 582.020 timesteps/s
99.7% CPU use with 4 MPI tasks x no OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 0.062505 | 0.067 | 0.07152 | 1.5 | 50.99
Neigh | 0.010041 | 0.0101 | 0.010178 | 0.1 | 7.69
Comm | 0.012347 | 0.012895 | 0.013444 | 0.5 | 9.81
Output | 6.3896e-05 | 0.00010294 | 0.00014091 | 0.3 | 0.08
Modify | 0.031802 | 0.032348 | 0.032897 | 0.3 | 24.62
Other | | 0.008965 | | | 6.82
Pair | 0.093691 | 0.096898 | 0.10005 | 0.8 | 56.40
Neigh | 0.011976 | 0.012059 | 0.012146 | 0.1 | 7.02
Comm | 0.016384 | 0.017418 | 0.018465 | 0.8 | 10.14
Output | 7.7963e-05 | 0.00010747 | 0.00013304 | 0.2 | 0.06
Modify | 0.031744 | 0.031943 | 0.032167 | 0.1 | 18.59
Other | | 0.01339 | | | 7.79
Nlocal: 8000 ave 8008 max 7992 min
Histogram: 2 0 0 0 0 0 0 0 0 2

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@ -1,4 +1,4 @@
LAMMPS (15 Feb 2016)
LAMMPS (6 Oct 2016)
# LAMMPS benchmark of granular flow
# chute flow of 32000 atoms with frozen base at 26 degrees
@ -57,24 +57,24 @@ Neighbor list info ...
master list distance cutoff = 1.1
ghost atom cutoff = 1.1
binsize = 0.55 -> bins = 146 73 68
Memory usage per processor = 15.7007 Mbytes
Step Atoms KinEng 1 Volume
Memory usage per processor = 16.1265 Mbytes
Step Atoms KinEng c_1 Volume
0 128000 3136556.5 6404.5051 119335.13
100 128000 3137168.3 6284.3873 119338.83
Loop time of 0.906913 on 4 procs for 100 steps with 128000 atoms
Loop time of 0.832365 on 4 procs for 100 steps with 128000 atoms
Performance: 952.683 tau/day, 110.264 timesteps/s
99.7% CPU use with 4 MPI tasks x no OpenMP threads
Performance: 1038.006 tau/day, 120.140 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 | 0.51454 | 0.53094 | 0.55381 | 2.0 | 58.54
Neigh | 0.042597 | 0.043726 | 0.045801 | 0.6 | 4.82
Comm | 0.063027 | 0.064657 | 0.067367 | 0.7 | 7.13
Output | 0.00024891 | 0.00059718 | 0.00086498 | 1.0 | 0.07
Modify | 0.16508 | 0.17656 | 0.1925 | 2.6 | 19.47
Other | | 0.09043 | | | 9.97
Pair | 0.5178 | 0.52208 | 0.52793 | 0.5 | 62.72
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
Modify | 0.15517 | 0.15627 | 0.15808 | 0.3 | 18.77
Other | | 0.0536 | | | 6.44
Nlocal: 32000 ave 32000 max 32000 min
Histogram: 4 0 0 0 0 0 0 0 0 0
@ -87,4 +87,4 @@ Total # of neighbors = 460532
Ave neighs/atom = 3.59791
Neighbor list builds = 2
Dangerous builds = 0
Total wall time: 0:00:01
Total wall time: 0:00:00

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@ -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
50 781.69049 -109873.35 0 -106640.13 52273.088
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

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@ -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

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@ -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

View File

@ -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

View File

@ -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

View File

@ -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

View File

@ -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

View File

@ -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

View File

@ -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

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@ -1,9 +0,0 @@
\documentclass[12pt]{article}
\pagestyle{empty}
\begin{document}
$$
F^C = A \omega_{ij} \qquad \qquad r_{ij} < r_c
$$
\end{document}

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@ -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}

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\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}

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@ -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

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@ -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)

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@ -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

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@ -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

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@ -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

View File

@ -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

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@ -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

View File

@ -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

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@ -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

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@ -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

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@ -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

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@ -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

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@ -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

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@ -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

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@ -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:]

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0
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0
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@ -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)

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@ -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

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@ -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

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@ -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.

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@ -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:]

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@ -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:]

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0
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0
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@ -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

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@ -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).

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@ -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
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0
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0
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0
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0
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@ -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
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0
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0
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0
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0
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0
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0
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0
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0
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0
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0
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0
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0
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0
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0
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@ -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

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@ -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.

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@ -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,

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@ -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

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@ -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.

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@ -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

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@ -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

View File

@ -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

View File

@ -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

View File

@ -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

View File

@ -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
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View 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
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@ -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
View File

View 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:

View 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).

View File

@ -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
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4
doc/src/pair_smtbq.txt Executable file → Normal file
View 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}, {&#958<sup>0</sup>} (eV) and {q} <br/> {r<sub>c1</sub>} (&#197), {r<sub>c2</sub>} (&#197) and {r<sub>0</sub>} (&#197) <br/> If type of potential is 'buck' : {C} (eV) and {&#961} (&#197) <br/> If type of potential is 'buckPlusAttr' : {C} (eV) and {&#961} (&#197) <br/> {D} (eV), {B} (&#197<sup>-1</sup>), {r<sub>1</sub><sup>OO</sup>} (&#197) and {r<sub>2</sub><sup>OO</sup>} (&#197) </pre>
Potential parameter: <pre><br/> If type of potential is 'second_moment' : {A (eV)}, {p}, {&#958<sup>0</sup>} (eV) and {q} <br/> {r<sub>c1</sub>} (&#197), {r<sub>c2</sub>} (&#197) and {r<sub>0</sub>} (&#197) <br/> If type of potential is 'buck' : {C} (eV) and {&#961} (&#197) <br/> If type of potential is 'buckPlusAttr' : {C} (eV) and {&#961} (&#197) <br/> {D} (eV), {B} (&#197<sup>-1</sup>), {r<sub>1</sub><sup>OO</sup>} (&#197) and {r<sub>2</sub><sup>OO</sup>} (&#197) </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

View File

@ -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

View File

@ -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

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