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190 Commits

Author SHA1 Message Date
87c028ed02 patch 20Jun17 2017-06-20 12:06:02 -06:00
84b530cca1 Merge pull request #537 from lammps/neb
minor changes to NEB doc pages and examples
2017-06-20 09:38:32 -06:00
50c9167913 small formatting correction in fix neb docs 2017-06-20 10:36:30 -04:00
d2610d9e7c minor changes to NEB doc pages and examples 2017-06-20 08:19:23 -06:00
326a8a1289 Merge pull request #536 from akohlmey/fix-nvcc-openmp-conflicts
Implement workaround for NVCC incompatibilities with OpenMP directives
2017-06-20 07:44:40 -06:00
b5300724bb Merge pull request #533 from lammps/user-intel
Updates for USER-INTEL package and NEB command flags/docs updates and issues
2017-06-20 07:44:17 -06:00
e129f18e6f Merge pull request #530 from akohlmey/no_static_sort_in_dump
Refactor Dump and Irregular classes to remove static class members
2017-06-20 07:43:49 -06:00
8c54fcd1b6 cleanup from aidan for fix reax/c/species and its KOKKOS version
this version eliminates the need for the PBCconnected list and avoids having to access the spec_atom array for ghost atoms
2017-06-19 17:31:54 -04:00
f5047ac3c7 augment fix shardlow check for ordering fixes to be KOKKOS compatible 2017-06-19 17:23:23 -04:00
164cedf353 protect all OpenMP pragmas with ifdefs and add special conditions for nvcc to ignore unsupported directives 2017-06-19 15:31:20 -04:00
3c329d1707 massive whitespace cleanup in USER-INTEL
removed are:
- DOS/Windows text format carriage return characters (^M)
- tabs replaced with spaces (tabs are evil!!)
- trailing whitespace
2017-06-19 13:23:01 -04:00
b687d16177 insert C++ file format indicator comments 2017-06-19 13:03:23 -04:00
9d3e34e492 add missing reference for lj/smooth/linear 2017-06-19 11:23:30 -04:00
8988b692a3 modified the documentation, first and last freeend can have different spring constants 2017-06-19 16:30:42 +02:00
c97415aefa corrected the initial free end 2017-06-19 14:57:39 +02:00
9b8de3ba29 remove ifdefs for selecting between plain and hybrid merge sort. use hybrid only. 2017-06-17 09:30:41 -04:00
cd88b31450 same PR, also has cosmetic changes to new fix neb options 2017-06-16 17:02:05 -06:00
9b9f6d6fe2 USER-INTEL upgrade from M Brown 2017-06-16 16:56:28 -06:00
c1b0b1b3f9 restore old qsort() based code and add preprocessor directives to switch
-DLMP_USE_LIBC_QSORT will use qsort() from libc to sort (requires static/global variables).
-DLMP_USE_MERGE_SORT will use a plain merge sort. slightly slower for expensive comparisons.
-DLMP_USE_HYBRID_SORT will use hybrid merge sort. faster than merge sort (no static/global variables)
2017-06-16 18:17:48 -04:00
bc0241576f Merge pull request #532 from akohlmey/restore-heuristics-in-fix-shardlow
recover running USER-DPD with USER-OMP and suffixes
2017-06-16 09:46:58 -06:00
2a6f026853 mergesort performance improvements
- use insertion sort to pre-sort data in 32-element chunks
- swap pointers between merge runs instead of copying the data
2017-06-16 08:05:55 -04:00
8728a8ddae restore heuristics for checking against integrators that broke after PR #499 was merged 2017-06-15 15:16:50 -04:00
9aa450b832 Merge pull request #528 from akohlmey/no_static_in_ring_comm
Refactor ring communication to no longer require static class variables
2017-06-15 11:13:07 -06:00
0588c382f0 Merge pull request #513 from v0i0/bugfix-airebo-nconj-kronecker
Bugfix in AIREBO as reported in #59 by @KammIma
2017-06-15 11:12:29 -06:00
d3c90f3c14 Merge pull request #510 from akohlmey/collected-small-changes
Collected small changes
2017-06-15 11:12:14 -06:00
b62d526cc9 Revert "avoid undesired negative forces for high particle velocities in granular models"
This reverts commit 066123007c.
2017-06-15 11:01:36 -04:00
1a29048940 Merge pull request #531 from ohenrich/user-cgdna
Affiliation Update for USER-CGDNA
2017-06-15 08:54:52 -06:00
0a6b3f8790 Merge pull request #527 from dstelter92/master
Added compute_scalar to fix_grem
2017-06-15 08:54:22 -06:00
7227bc415d Merge pull request #526 from andeplane/vashishta_gpu
Implemented pair style vashishta in GPU package
2017-06-15 08:52:13 -06:00
a4bc233d86 Merge pull request #525 from akohlmey/user-tally-refactor
Refactoring of USER-TALLY computes to handle sparse/hybrid system for many processors plus bugfixes
2017-06-15 08:51:24 -06:00
5c5b4ffadb Merge pull request #522 from akohlmey/tip4p-cleanup-refactor
Refactor and bugfix for some TIP4P pair styles
2017-06-15 08:48:52 -06:00
30177c4eae Merge pull request #521 from pastewka/17_dump_nc
Updated NetCDF dump style (dump netcdf)
2017-06-15 08:47:29 -06:00
178eff237b Merge pull request #520 from stanmoore1/kokkos_update
Kokkos library update to v2.03.05
2017-06-15 08:47:09 -06:00
576b7f1d97 Merge pull request #519 from Pakketeretet2/USER-MANIFOLD-gaussian-bump
Some extensions/cleanup in USER-MANIFOLD
2017-06-15 08:46:55 -06:00
86369fec6b Merge pull request #517 from akohlmey/select-rigid-reinit-option
Add `reinit` keyword to rigid body fixes
2017-06-15 08:46:29 -06:00
79341ac5d1 Merge pull request #516 from akohlmey/check-rigid-overlap
Implement check whether commands or styles try to change cached properties in rigid body integrators
2017-06-15 08:44:05 -06:00
66945294a9 Merge pull request #515 from stanmoore1/remove_fences
Remove unnecessary thread fences in Kokkos package
2017-06-15 08:40:43 -06:00
9a7207e34c Merge pull request #511 from akohlmey/add-compute-cnp
Integrate compute cnp/atom contributed by Paulo Branicio (USC)
2017-06-15 08:38:05 -06:00
d41c617d1d Merge pull request #509 from akohlmey/add-atomonly-npair-for-omp
add "atomonly" optimized neighbor list build styles to USER-OMP
2017-06-15 08:24:44 -06:00
1ec9e588ff Merge pull request #504 from andeplane/hexorder_fix
Using correct ndegree instead of nnn
2017-06-15 08:24:25 -06:00
3c7417fb59 Merge pull request #497 from lammps/add-user-reaxc-omp
Add USER-OMP compatible OpenMP support to USER-REAXC
2017-06-15 08:24:03 -06:00
34cfc7bd51 Merge pull request #490 from EmileMaras/NEB-Change
added several features to the NEB
2017-06-15 08:23:04 -06:00
c98bb7fa5f Corrected minor bug in utility script 2017-06-15 12:57:44 +01:00
77ca68a2b4 Changed affiliation 2017-06-15 12:52:19 +01:00
06fe703eed add missing mergesort header 2017-06-14 23:22:49 -04:00
8500a197ae whitespace cleanup 2017-06-14 23:13:10 -04:00
1f17e8ebbb remove need for static class member variables in Dump and Irregular
The dump and irregular classes were using qsort() from the C-library
for sorting lists through custom comparison functions, which required
access to additional data, which was passed via static class variables,
i.e. globals. This collides with having multiple LAMMPS instances in
the same address space.

the calls to qsort() are replaced with a custom merge sort, which passes
a void pointer to the comparison functions, which can contain any kind
of desired information, e.g. a class handle or a list
2017-06-14 23:10:53 -04:00
fcc387f232 change ring communication API to no longer require a static variable pointing to 'this' of the caller 2017-06-14 17:01:06 -04:00
e7634a44f4 updated thermo_modify in example 2017-06-14 13:11:54 -04:00
3214d639aa removed unneeded .gitignore 2017-06-14 12:26:52 -04:00
0ad66ecb89 Added compute_scalar to fix_grem for easier output managment, updated example to show use 2017-06-14 12:18:22 -04:00
e139a7fd45 Updated docs for vashishta/gpu 2017-06-14 13:52:03 +02:00
d7646aeeed Fixed opencl error 2017-06-14 12:03:47 +02:00
5f9341813d Removed debug output 2017-06-14 10:57:54 +02:00
8441307185 Removed non-general CUDA-dir in makefile 2017-06-14 10:28:46 +02:00
720af5c360 Added vashishta to OpenCL makefile 2017-06-14 10:27:52 +02:00
eeff0b8633 Added vashishta GPU package for NVidia 2017-06-14 10:24:16 +02:00
32b967ed9c add rigid body overlap warnings to change_box and delete_atoms 2017-06-13 16:26:49 -04:00
11751521e7 remove dead code 2017-06-12 22:49:31 -04:00
7a05d87f7c update USER-TALLY examples 2017-06-12 22:20:36 -04:00
b01143102d refactoring of USER-TALLY computes to handle sparse and hybrid systems
with sparse and hybrid systems, Pair::ev_tally() may not be called on
every processor and thus the computes in USER-TALLY may hang during
reverse communication because of the error->all() call after checking
whether callback from Pair::ev_tally() has been called at least once.
To address this cleanly, a second callback function needs to be added,
which is run during Pair::ev_setup() and will now handle all memory
re-allocation and clearing of accumulators, just like it is done for
regular tallied data.
2017-06-12 22:12:12 -04:00
e530ba46f4 cleanup and bugfix for compute heat/flux/tally
- make heatj a pointer instead of a static array
- fix memory leaks for eatom, stress
- simplify and streamline computation
2017-06-12 21:46:00 -04:00
420db44596 print incompatible pair style warnings in USER-TALLY only on MPI rank 0 2017-06-12 20:05:15 -04:00
cfeb9b5ba5 Merge branch 'collected-small-changes' of github.com:akohlmey/lammps into collected-small-changes 2017-06-12 14:20:50 -04:00
0c805d0b70 correctly skip over point particles and point dipoles when counting extendend particles in fix rigid/small 2017-06-12 14:20:38 -04:00
6b289b0794 change incorrect EINERTIA constant in rigid body integrators from 4.0 to 2.0 (same as in other integrators) 2017-06-12 14:07:40 -04:00
daa77176ad add restart support to fix deform. only "initial" data is restored and some consistency check performed 2017-06-10 17:28:17 -04:00
8f18c284d3 add crude check to print warning when using compute cnp/atom on multi-type system 2017-06-10 17:08:07 -04:00
06915162b0 whitespace cleanup 2017-06-10 16:56:54 -04:00
a849f35dcd adjust compute cnp/atom to match the documentation. need to skip atoms not in compute group. 2017-06-10 16:55:42 -04:00
4c69bbcf5c apply rigid body check to displace_atoms command 2017-06-10 11:37:54 -04:00
dd44189d1f fix bug in compute orientorder/atom argument parsing 2017-06-10 04:35:11 -04:00
2f6bbcfbbc output detailed multi-thread performance data only with "timer full" 2017-06-09 15:11:40 -04:00
2686b7f830 simplify compatibility check for fix reax/c/bonds with pair styles 2017-06-09 14:39:52 -04:00
d3a863e7af when identifying molecules/clusters fall back to unfiltered coordinates for ghost atoms 2017-06-09 14:35:12 -04:00
64e8000720 expand error message requiring a reax/c derived pair style 2017-06-09 11:42:35 -04:00
c160d0cd5e fix reax/c/species/omp doesn't is not needed anymore 2017-06-09 11:04:11 -04:00
9222278fb5 match reax/c pair style variants against prefix and not full name 2017-06-09 11:00:16 -04:00
bdf03757e6 MAINT: Simplified GPL headers. 2017-06-08 23:20:21 +02:00
c81bc108f9 DOC: Updated dump_modify and dump netcdf documentation. 2017-06-08 23:19:38 +02:00
10d2e7c380 MAINT: DumpNetCDF and DumpNetCDFMPIIO need access to thermo output. 2017-06-08 23:18:54 +02:00
bd83c7c7f9 MAINT: Updated contact data and fixed typos. 2017-06-08 23:02:22 +02:00
d51cee1b82 MAINT: Turned 'global' options into a 'thermo yes'/'thermo no' option that enables dumping of thermo data to the netcdf file (for parallel NetCDF/MPIIO variant). 2017-06-08 22:58:27 +02:00
be476c9e1d MAINT: Turned 'global' options into a 'thermo yes'/'thermo no' option that enables dumping of thermo data to the netcdf file. 2017-06-08 22:43:10 +02:00
0ecdb99885 fix uninitialized data access as reported by @martok in #174 2017-06-08 13:50:17 -04:00
00ce15d043 Remove tpls dir 2017-06-08 10:43:19 -06:00
5c1d17d1c0 Updating Kokkos lib to v2.03.05 2017-06-08 10:42:08 -06:00
afd4f5b0a6 Merge branch 'collected-small-changes' of github.com:akohlmey/lammps into collected-small-changes 2017-06-07 17:37:13 -04:00
31a734b03d sbmask function should be flagged as const indicating no side effects 2017-06-07 17:10:33 -04:00
2e728972e2 make pair styles lj/cut/tip4p/long/omp, lj/long/tip4p/long and lj/long/tip4p/long/omp consistent with the reset of tip4p styles 2017-06-07 17:09:45 -04:00
36c8b26fef BUG: DumpNCMPIIO is now called DumpNetCDFMPIIO 2017-06-07 14:01:36 +02:00
99ef36f440 MAINT: Switched NetCDF from 64BIT_OFFSET to 64BIT_DATA which can handle frames (of unlimited dimension) > 2 GB. This becomes important for system sizes 100 Mio atoms and upwards. 2017-06-07 13:52:33 +02:00
a2edef7c9c local variable fp in pair style eam/cd was shadowing class member. renamed local variable to fptr 2017-06-07 00:23:53 -04:00
1f9504c546 some more bookkeeping updates triggered by the lj/sf style removal 2017-06-06 17:31:45 -04:00
04ebd81ac5 minor whitespace cleanup 2017-06-06 17:26:18 -04:00
5cb56796a2 alias pair style lj/sf to lj/smooth/linear and remove/update related files 2017-06-06 17:26:06 -04:00
0c1b87c8cf Merge branch 'collected-small-changes' of github.com:akohlmey/lammps into collected-small-changes 2017-06-06 16:27:07 -04:00
cd67eaa5f4 update e-mail and affiliation for stefan paquay in USER-MANIFOLD related files 2017-06-06 16:26:57 -04:00
18dee3f78e Added Gaussian bump. Updated e-mail address. 2017-06-06 16:03:09 -04:00
06c8e95774 corrected the fix_neb documentation 2017-06-06 14:20:54 +02:00
d437650c77 make certain Domain::box_change is initialized before use 2017-06-06 08:08:10 -04:00
46c5cbae8f update rigid fix documentation for added reinit keyword 2017-06-05 18:04:09 -04:00
deff6c666e add flag "reinit" with args "yes" / "no" to fixes rigid & rigid/small 2017-06-05 17:31:43 -04:00
3a01836325 simplify code for rigid body overlap checks 2017-06-05 16:39:17 -04:00
0034d2db35 apply the rigid body checks to some more example codes 2017-06-05 16:30:30 -04:00
ed50bd2254 Removing unnecessary fences 2017-06-05 13:54:13 -06:00
90ca0852c7 use "body" list via Fix::extract() to correctly identify atoms in bodies 2017-06-05 15:48:23 -04:00
968de8548c apply test for overlap with rigid bodies to set and velocity command 2017-06-05 13:06:53 -04:00
95d6f05a76 add 3 APIs to Modify for checking if atoms overlap with any rigid fixes 2017-06-05 12:41:37 -04:00
ff58ccac28 add clarification to impact of special bonds to manybody potentials 2017-06-04 21:21:32 -04:00
e03cc99467 made the command options more lammps standard style 2017-06-02 23:42:16 +02:00
f59ee5bd62 enable support for dynamic groups in fix planeforce and fix lineforce 2017-06-02 08:45:15 -04:00
af5f19604c remove no longer correct sentence from set command docs 2017-05-31 23:36:39 -04:00
3025996407 Merge branch 'master' into add-user-reaxc-omp
This updates the code base with several required updates from master
2017-05-31 12:53:38 -04:00
d2b6559039 Fixing issue in fix_qeq_reax 2017-05-31 10:52:03 -06:00
3c0cef9927 Merge branch 'fix_domain_pointer' of https://github.com/andeplane/lammps into collected-small-changes 2017-05-31 07:10:16 -04:00
937cf0b996 Bugfix: Kronecker term ignored in spline forces.
The code ignored the kronecker(ktype, 0) or kronecker(ltype, 0)
terms in the contributing terms to NconjtmpI and NconjtmpJ.
The issue was present both in ::bondorder and ::bondorderLJ and
led to energy conservation issues.
It has been fixed by checking for the atom type before entering
the offending calculations and adding clarifying comments.
2017-05-31 12:20:12 +02:00
f57f1efdff Setting lattice to NULL before creating 2017-05-31 00:34:26 -07:00
2b3c124e61 add example input for compute cnp/atom 2017-05-31 00:43:53 -04:00
85e917ae52 integrate compute cnp/atom contributed by Paulo Branicio (USC) 2017-05-31 00:38:44 -04:00
0be2cd3d43 fix bug reported on lammps-users, when not using the first molecule template 2017-05-30 23:58:56 -04:00
066123007c avoid undesired negative forces for high particle velocities in granular models 2017-05-30 21:54:16 -04:00
167a51538e support atom style variables for assigning image flags with the set command 2017-05-30 21:52:32 -04:00
5c6f63d8b4 Merge branch 'fix_adapt_doc_fix' of https://github.com/Pakketeretet2/lammps into collected-small-changes 2017-05-30 17:06:25 -04:00
03ab8d0f48 major neighbor list style whitespace cleanup 2017-05-30 17:04:48 -04:00
75b567a457 add "atomonly" optimized neighbor list build styles to USER-OMP 2017-05-30 16:50:38 -04:00
cace3e3530 Added missing :pre to doc/src/fix_adapt.txt 2017-05-30 16:08:32 -04:00
286d4f2743 Merge pull request #506 from lammps/snap
SNAP changes by Aidan
2017-05-30 13:32:00 -06:00
952b18fc02 Merge pull request #494 from rbberger/small_updates
Collection of minor updates
2017-05-30 10:51:24 -06:00
816fa93429 Merge pull request #499 from akohlmey/add-fix-compute-style-bugfix
Fix bug where fix/compute style names were not correctly set with suffixes
2017-05-30 10:49:27 -06:00
f4f975edd6 Merge pull request #495 from akohlmey/doc-fixes
Collected small updates and bugfixes
2017-05-30 10:48:57 -06:00
cff4e4a837 Merge pull request #468 from andeplane/gcmc_fix_nlocal
Using correct value for atom->nlocal in translate/rotate in fix_gcmc.cpp
2017-05-30 10:45:39 -06:00
32db4660bd Merge pull request #460 from andeplane/gcmc_fix
Setting molecule COM to 0 after moving atoms
2017-05-30 10:45:23 -06:00
22fdb1fc14 SNAP changes by Aidan 2017-05-30 10:21:07 -06:00
412cb8f089 avoid hang in fix reax/c/species when multiple atoms have the exact same x-coordinate 2017-05-30 08:15:55 -04:00
092806ad4f no need for special whitespace handling in library interface 2017-05-30 07:55:48 -04:00
4ae314731d must not use strtok() in library function as it is not re-entrant and may be used inside LAMMPS commands 2017-05-30 07:42:10 -04:00
4b8d2e829c triclinic member variable is referenced in destructor and thus must be initialized in constructor 2017-05-30 07:41:01 -04:00
d93938f7e1 displace_atom rotate needs to operate on unwrapped coordinates with image flags set to zero 2017-05-29 16:57:35 -04:00
c904cfb8bc removed a bug in fix_neb.cpp which prevented the freeend to work properly, plus added an example for the neb freeend 2017-05-29 15:49:04 +02:00
32c87f3131 removed a bug in fix_neb.cpp which prevented the freeend to work properly, plus added an example for the neb freeend 2017-05-29 14:00:13 +02:00
ba0ddea5e1 Using correct ndegree instead of nnn 2017-05-28 15:44:12 -07:00
c0339120d2 add missing neighbor list class definitions to USER-OMP 2017-05-26 21:28:41 -04:00
5a23d2d1da fix bug in computing mixed EAM potentials introduced by TI modifications 2017-05-26 20:28:45 -04:00
de446ace2f Merge branch 'user-manifold-doc-fix' of https://github.com/Pakketeretet2/lammps into doc-fixes 2017-05-26 18:44:29 -04:00
2055110e05 Fixed typo in dox. 2017-05-26 17:38:21 -04:00
5b1e582f03 prevent segfault when defining pair_style comb3 without arguments 2017-05-26 10:52:20 -04:00
f1ec6dc41a dead code removal and reformatting 2017-05-25 18:55:07 -04:00
c3f6e27bfe augment documentation for newly added multi-threaded reax/c styles 2017-05-25 17:00:19 -04:00
0a2fe70511 remove redundant code from fix qeq/reax and qeq/reax/omp 2017-05-25 16:31:31 -04:00
53e7fee5b7 Merge branch 'doc-fixes' of github.com:akohlmey/lammps into doc-fixes 2017-05-25 10:11:31 -04:00
5291f2ed6e fix bug in fix shear/history reported by kevin hanley. see #500 2017-05-25 10:11:24 -04:00
99a68e487f fix suffix style handling bug for adding fixes and computes 2017-05-25 02:01:04 -04:00
271431ab18 clean up code so it can be compiled with and without OpenMP enabled regardless of whether the USER-OMP package is installed 2017-05-24 17:25:57 -04:00
88d4150d2b remove trailing whitespace 2017-05-24 16:29:56 -04:00
0e3cfbc007 remove trailing whitespace 2017-05-24 16:29:26 -04:00
5345ad2da7 merge in the remainder of the USER-REAXC-OMP code. still a lot of work to do. compiles only with -fopenmp active 2017-05-24 16:24:43 -04:00
ead05f81c0 Merge branch 'pair_morse_soft-doc-fix' of https://github.com/Pakketeretet2/lammps into doc-fixes 2017-05-24 13:56:54 -04:00
4f9e7cbd16 Cleaned up docs for pair_mores, a missing :pre ruined formatting. 2017-05-24 13:36:14 -04:00
bb890941ca first chunk of code from USER-REAXC-OMP imported and adapted into USER-REAXC 2017-05-24 00:19:36 -04:00
4002dce639 restore explicit NAN constants in output 2017-05-22 22:39:52 -04:00
c801cdd81f some more formatting cleanup in fix neb 2017-05-22 22:33:14 -04:00
9008a31190 more formatting cleanup
This cleans up and simplifies the neb command code some more
2017-05-22 21:55:55 -04:00
bdfb7c69ea Remove unused code detected by coverity CID 177700 2017-05-22 17:51:40 -04:00
084626e60b Fixes coverity issue CID 179426 2017-05-22 17:36:16 -04:00
a7d790a827 Fixes coverity issue CID 179439 2017-05-22 17:33:47 -04:00
8a630ff4ec Fixes coverity issue CID 179440 2017-05-22 17:32:07 -04:00
617ca4e0c8 Fixes coverity issue CID 179436 2017-05-22 17:30:46 -04:00
62601678cd when growing arrays with reallocate, always check against atom->nmax and not atom->nlocal or else these arrays may be of inconsistent size and communication can lead to data corruption 2017-05-22 17:16:19 -04:00
081910adbc do not try to free null communicators 2017-05-22 17:15:14 -04:00
f73fd0625d rename nall class member to numall to avoid confusion with the common convention nall = atom->nlocal+atom->nghost 2017-05-22 17:14:38 -04:00
06a4f47a4c Merge remote-tracking branch 'upstream/master' into small_updates 2017-05-22 17:14:29 -04:00
7185db98b4 NEBLongRange was incorrectly set to false by default. revert to true. 2017-05-22 17:13:38 -04:00
4780d72809 use '&&' and '||' instead of 'and' and 'or' operators for consistency 2017-05-22 14:42:42 -04:00
3fd91a239f avoid use '&&' and '||' instead of 'and' and 'or' for consistency 2017-05-22 14:41:01 -04:00
8bc829c7f1 change example inputs to be backward compatible 2017-05-22 14:40:01 -04:00
97d3c843c4 small documentation fixes to fix typos and formatting issues 2017-05-21 11:13:47 -04:00
546aed7ccd plug some memory leaks 2017-05-19 16:14:59 -04:00
6ef79d3715 silence several compiler warnings 2017-05-19 15:13:19 -04:00
c2bf3269ac formatting cleanup. combine 8 MPI_Allreduce() calls into 1 2017-05-19 15:02:29 -04:00
aca16745e4 restore spelling fix and semantic fix from upstream 2017-05-19 12:17:19 -04:00
a5110d81ea correct a bunch of documentation formatting issues for updated neb and fix neb commands 2017-05-19 12:13:23 -04:00
9593e05c9e Force PDF documentation build to fail on first error 2017-05-18 19:37:08 -04:00
d4ee03c778 changed doc links 2017-05-18 21:31:39 +02:00
069f3e746b small formating changes 2017-05-18 21:23:29 +02:00
8daba01151 some small formating change but does not work anymore 2017-05-18 16:48:20 +02:00
640edbc1d4 added several features to the NEB 2017-05-18 11:08:08 +02:00
7adc7f02e0 Stopped working on gaussian bump. 2017-05-03 11:21:18 -04:00
914848433a Using correct value for atom->nlocal 2017-05-01 00:02:57 +02:00
67fced37c8 Setting molecule COM to 0 after moving atoms 2017-04-26 20:10:18 +02:00
895 changed files with 81300 additions and 23026 deletions

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@ -100,6 +100,7 @@ epub: $(OBJECTS)
pdf: utils/txt2html/txt2html.exe
@(\
set -e; \
cd src; \
../utils/txt2html/txt2html.exe -b *.txt; \
htmldoc --batch lammps.book; \

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@ -0,0 +1,14 @@
\documentclass[12pt,article]{article}
\usepackage{indentfirst}
\usepackage{amsmath}
\begin{document}
\begin{eqnarray*}
r_{c}^{fcc} & = & \frac{1}{2} \left(\frac{\sqrt{2}}{2} + 1\right) \mathrm{a} \simeq 0.8536 \:\mathrm{a} \\
r_{c}^{bcc} & = & \frac{1}{2}(\sqrt{2} + 1) \mathrm{a} \simeq 1.207 \:\mathrm{a} \\
r_{c}^{hcp} & = & \frac{1}{2}\left(1+\sqrt{\frac{4+2x^{2}}{3}}\right) \mathrm{a}
\end{eqnarray*}
\end{document}

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@ -0,0 +1,12 @@
\documentclass[12pt,article]{article}
\usepackage{indentfirst}
\usepackage{amsmath}
\begin{document}
$$
Rc + Rs > 2*{\rm cutoff}
$$
\end{document}

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9
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@ -0,0 +1,9 @@
\documentclass[12pt]{article}
\begin{document}
$$
Q_{i} = \frac{1}{n_i}\sum_{j = 1}^{n_i} | \sum_{k = 1}^{n_{ij}} \vec{R}_{ik} + \vec{R}_{jk} |^2
$$
\end{document}

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@ -1,11 +0,0 @@
\documentclass[12pt]{article}
\begin{document}
\begin{eqnarray*}
F & = & F_{\mathrm{LJ}}(r) - F_{\mathrm{LJ}}(r_{\mathrm{c}}) \qquad r < r_{\mathrm{c}} \\
E & = & E_{\mathrm{LJ}}(r) - E_{\mathrm{LJ}}(r_{\mathrm{c}}) + (r - r_{\mathrm{c}}) F_{\mathrm{LJ}}(r_{\mathrm{c}}) \qquad r < r_{\mathrm{c}} \\
\mathrm{with} \qquad E_{\mathrm{LJ}}(r) & = & 4 \epsilon \left[ \left(\frac{\sigma}{r}\right)^{12} - \left(\frac{\sigma}{r}\right)^6 \right] \qquad \mathrm{and} \qquad F_{\mathrm{LJ}}(r) = - E^\prime_{\mathrm{LJ}}(r)
\end{eqnarray*}
\end{document}

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@ -1,7 +1,7 @@
<!-- HTML_ONLY -->
<HEAD>
<TITLE>LAMMPS Users Manual</TITLE>
<META NAME="docnumber" CONTENT="19 May 2017 version">
<META NAME="docnumber" CONTENT="20 Jun 2017 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
19 May 2017 version :c,h4
20 Jun 2017 version :c,h4
Version info: :h4

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@ -717,7 +717,7 @@ package"_Section_start.html#start_3.
"phonon"_fix_phonon.html,
"pimd"_fix_pimd.html,
"qbmsst"_fix_qbmsst.html,
"qeq/reax"_fix_qeq_reax.html,
"qeq/reax (ko)"_fix_qeq_reax.html,
"qmmm"_fix_qmmm.html,
"qtb"_fix_qtb.html,
"reax/c/bonds"_fix_reax_bonds.html,
@ -831,6 +831,7 @@ package"_Section_start.html#start_3.
"ackland/atom"_compute_ackland_atom.html,
"basal/atom"_compute_basal_atom.html,
"cnp/atom"_compute_cnp_atom.html,
"dpd"_compute_dpd.html,
"dpd/atom"_compute_dpd_atom.html,
"fep"_compute_fep.html,
@ -963,7 +964,7 @@ KOKKOS, o = USER-OMP, t = OPT.
"lj/expand (gko)"_pair_lj_expand.html,
"lj/gromacs (gko)"_pair_gromacs.html,
"lj/gromacs/coul/gromacs (ko)"_pair_gromacs.html,
"lj/long/coul/long (o)"_pair_lj_long.html,
"lj/long/coul/long (io)"_pair_lj_long.html,
"lj/long/dipole/long"_pair_dipole.html,
"lj/long/tip4p/long"_pair_lj_long.html,
"lj/smooth (o)"_pair_lj_smooth.html,
@ -1038,7 +1039,6 @@ package"_Section_start.html#start_3.
"lj/sdk (gko)"_pair_sdk.html,
"lj/sdk/coul/long (go)"_pair_sdk.html,
"lj/sdk/coul/msm (o)"_pair_sdk.html,
"lj/sf (o)"_pair_lj_sf.html,
"meam/spline (o)"_pair_meam_spline.html,
"meam/sw/spline"_pair_meam_sw_spline.html,
"mgpt"_pair_mgpt.html,
@ -1057,7 +1057,7 @@ package"_Section_start.html#start_3.
"oxdna2/excv"_pair_oxdna2.html,
"oxdna2/stk"_pair_oxdna2.html,
"quip"_pair_quip.html,
"reax/c (k)"_pair_reaxc.html,
"reax/c (ko)"_pair_reaxc.html,
"smd/hertz"_pair_smd_hertz.html,
"smd/tlsph"_pair_smd_tlsph.html,
"smd/triangulated/surface"_pair_smd_triangulated_surface.html,
@ -1225,7 +1225,7 @@ USER-OMP, t = OPT.
"msm/cg (o)"_kspace_style.html,
"pppm (go)"_kspace_style.html,
"pppm/cg (o)"_kspace_style.html,
"pppm/disp"_kspace_style.html,
"pppm/disp (i)"_kspace_style.html,
"pppm/disp/tip4p"_kspace_style.html,
"pppm/stagger"_kspace_style.html,
"pppm/tip4p (o)"_kspace_style.html :tb(c=4,ea=c)

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@ -8890,6 +8890,14 @@ This is a requirement to use this potential. :dd
See the newton command. This is a restriction to use this potential. :dd
{Pair style vashishta/gpu requires atom IDs} :dt
This is a requirement to use this potential. :dd
{Pair style vashishta/gpu requires newton pair off} :dt
See the newton command. This is a restriction to use this potential. :dd
{Pair style tersoff/gpu requires atom IDs} :dt
This is a requirement to use the tersoff/gpu potential. :dd

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@ -1502,7 +1502,7 @@ oxDNA model of Doye, Louis and Ouldridge at the University of Oxford.
This includes Langevin-type rigid-body integrators with improved
stability.
[Author:] Oliver Henrich (University of Edinburgh).
[Author:] Oliver Henrich (University of Strathclyde, Glasgow).
[Install or un-install:]
@ -2027,8 +2027,8 @@ algorithm to formulate single-particle constraint functions
g(xi,yi,zi) = 0 and their derivative (i.e. the normal of the manifold)
n = grad(g).
[Author:] Stefan Paquay (Eindhoven University of Technology (TU/e), The
Netherlands)
[Author:] Stefan Paquay (until 2017: Eindhoven University of Technology (TU/e), The
Netherlands; since 2017: Brandeis University, Waltham, MA, USA)
[Install or un-install:]

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@ -30,8 +30,8 @@ Dihedral Styles: charmm, harmonic, opls :l
Fixes: nve, npt, nvt, nvt/sllod :l
Improper Styles: cvff, harmonic :l
Pair Styles: buck/coul/cut, buck/coul/long, buck, eam, gayberne,
charmm/coul/long, lj/cut, lj/cut/coul/long, sw, tersoff :l
K-Space Styles: pppm :l
charmm/coul/long, lj/cut, lj/cut/coul/long, lj/long/coul/long, sw, tersoff :l
K-Space Styles: pppm, pppm/disp :l
:ule
[Speed-ups to expect:]
@ -42,62 +42,88 @@ precision mode. Performance improvements are shown compared to
LAMMPS {without using other acceleration packages} as these are
under active development (and subject to performance changes). The
measurements were performed using the input files available in
the src/USER-INTEL/TEST directory. These are scalable in size; the
results given are with 512K particles (524K for Liquid Crystal).
Most of the simulations are standard LAMMPS benchmarks (indicated
by the filename extension in parenthesis) with modifications to the
run length and to add a warmup run (for use with offload
benchmarks).
the src/USER-INTEL/TEST directory with the provided run script.
These are scalable in size; the results given are with 512K
particles (524K for Liquid Crystal). Most of the simulations are
standard LAMMPS benchmarks (indicated by the filename extension in
parenthesis) with modifications to the run length and to add a
warmup run (for use with offload benchmarks).
:c,image(JPG/user_intel.png)
Results are speedups obtained on Intel Xeon E5-2697v4 processors
(code-named Broadwell) and Intel Xeon Phi 7250 processors
(code-named Knights Landing) with "18 Jun 2016" LAMMPS built with
Intel Parallel Studio 2016 update 3. Results are with 1 MPI task
(code-named Knights Landing) with "June 2017" LAMMPS built with
Intel Parallel Studio 2017 update 2. Results are with 1 MPI task
per physical core. See {src/USER-INTEL/TEST/README} for the raw
simulation rates and instructions to reproduce.
:line
[Accuracy and order of operations:]
In most molecular dynamics software, parallelization parameters
(# of MPI, OpenMP, and vectorization) can change the results due
to changing the order of operations with finite-precision
calculations. The USER-INTEL package is deterministic. This means
that the results should be reproducible from run to run with the
{same} parallel configurations and when using determinstic
libraries or library settings (MPI, OpenMP, FFT). However, there
are differences in the USER-INTEL package that can change the
order of operations compared to LAMMPS without acceleration:
Neighbor lists can be created in a different order :ulb,l
Bins used for sorting atoms can be oriented differently :l
The default stencil order for PPPM is 7. By default, LAMMPS will
calculate other PPPM parameters to fit the desired acuracy with
this order :l
The {newton} setting applies to all atoms, not just atoms shared
between MPI tasks :l
Vectorization can change the order for adding pairwise forces :l
:ule
The precision mode (described below) used with the USER-INTEL
package can change the {accuracy} of the calculations. For the
default {mixed} precision option, calculations between pairs or
triplets of atoms are performed in single precision, intended to
be within the inherent error of MD simulations. All accumulation
is performed in double precision to prevent the error from growing
with the number of atoms in the simulation. {Single} precision
mode should not be used without appropriate validation.
:line
[Quick Start for Experienced Users:]
LAMMPS should be built with the USER-INTEL package installed.
Simulations should be run with 1 MPI task per physical {core},
not {hardware thread}.
For Intel Xeon CPUs:
Edit src/MAKE/OPTIONS/Makefile.intel_cpu_intelmpi as necessary. :ulb,l
If using {kspace_style pppm} in the input script, add "neigh_modify binsize cutoff" and "kspace_modify diff ad" to the input script for better
performance. Cutoff should be roughly the neighbor list cutoff. By
default the binsize is half the neighbor list cutoff. :l
"-pk intel 0 omp 2 -sf intel" added to LAMMPS command-line :l
Set the environment variable KMP_BLOCKTIME=0 :l
"-pk intel 0 omp $t -sf intel" added to LAMMPS command-line :l
$t should be 2 for Intel Xeon CPUs and 2 or 4 for Intel Xeon Phi :l
For some of the simple 2-body potentials without long-range
electrostatics, performance and scalability can be better with
the "newton off" setting added to the input script :l
If using {kspace_style pppm} in the input script, add
"kspace_modify diff ad" for better performance :l
:ule
For Intel Xeon Phi CPUs for simulations without {kspace_style
pppm} in the input script :
For Intel Xeon Phi CPUs:
Edit src/MAKE/OPTIONS/Makefile.knl as necessary. :ulb,l
Runs should be performed using MCDRAM. :l
"-pk intel 0 omp 2 -sf intel" {or} "-pk intel 0 omp 4 -sf intel"
should be added to the LAMMPS command-line. Choice for best
performance will depend on the simulation. :l
Runs should be performed using MCDRAM. :ulb,l
:ule
For Intel Xeon Phi CPUs for simulations with {kspace_style
pppm} in the input script:
For simulations using {kspace_style pppm} on Intel CPUs
supporting AVX-512:
Edit src/MAKE/OPTIONS/Makefile.knl as necessary. :ulb,l
Runs should be performed using MCDRAM. :l
Add "neigh_modify binsize 3" to the input script for better
performance. :l
Add "kspace_modify diff ad" to the input script for better
performance. :l
export KMP_AFFINITY=none :l
"-pk intel 0 omp 3 lrt yes -sf intel" or "-pk intel 0 omp 1 lrt yes
-sf intel" added to LAMMPS command-line. Choice for best performance
will depend on the simulation. :l
Add "kspace_modify diff ad" to the input script :ulb,l
The command-line option should be changed to
"-pk intel 0 omp $r lrt yes -sf intel" where $r is the number of
threads minus 1. :l
Do not use thread affinity (set KMP_AFFINITY=none) :l
The "newton off" setting may provide better scalability :l
:ule
For Intel Xeon Phi coprocessors (Offload):
@ -169,6 +195,10 @@ cat /proc/cpuinfo :pre
[Building LAMMPS with the USER-INTEL package:]
NOTE: See the src/USER-INTEL/README file for additional flags that
might be needed for best performance on Intel server processors
code-named "Skylake".
The USER-INTEL package must be installed into the source directory:
make yes-user-intel :pre
@ -322,8 +352,8 @@ follow in the input script.
NOTE: The USER-INTEL package will perform better with modifications
to the input script when "PPPM"_kspace_style.html is used:
"kspace_modify diff ad"_kspace_modify.html and "neigh_modify binsize
3"_neigh_modify.html should be added to the input script.
"kspace_modify diff ad"_kspace_modify.html should be added to the
input script.
Long-Range Thread (LRT) mode is an option to the "package
intel"_package.html command that can improve performance when using
@ -342,6 +372,10 @@ would normally perform best with "-pk intel 0 omp 4", instead use
environment variable "KMP_AFFINITY=none". LRT mode is not supported
when using offload.
NOTE: Changing the "newton"_newton.html setting to off can improve
performance and/or scalability for simple 2-body potentials such as
lj/cut or when using LRT mode on processors supporting AVX-512.
Not all styles are supported in the USER-INTEL package. You can mix
the USER-INTEL package with styles from the "OPT"_accelerate_opt.html
package or the "USER-OMP package"_accelerate_omp.html. Of course,
@ -467,7 +501,7 @@ supported.
Brown, W.M., Carrillo, J.-M.Y., Mishra, B., Gavhane, N., Thakker, F.M., De Kraker, A.R., Yamada, M., Ang, J.A., Plimpton, S.J., "Optimizing Classical Molecular Dynamics in LAMMPS," in Intel Xeon Phi Processor High Performance Programming: Knights Landing Edition, J. Jeffers, J. Reinders, A. Sodani, Eds. Morgan Kaufmann. :ulb,l
Brown, W. M., Semin, A., Hebenstreit, M., Khvostov, S., Raman, K., Plimpton, S.J. Increasing Molecular Dynamics Simulation Rates with an 8-Fold Increase in Electrical Power Efficiency. 2016 International Conference for High Performance Computing. In press. :l
Brown, W. M., Semin, A., Hebenstreit, M., Khvostov, S., Raman, K., Plimpton, S.J. "Increasing Molecular Dynamics Simulation Rates with an 8-Fold Increase in Electrical Power Efficiency."_http://dl.acm.org/citation.cfm?id=3014915 2016 High Performance Computing, Networking, Storage and Analysis, SC16: International Conference (pp. 82-95). :l
Brown, W.M., Carrillo, J.-M.Y., Gavhane, N., Thakkar, F.M., Plimpton, S.J. Optimizing Legacy Molecular Dynamics Software with Directive-Based Offload. Computer Physics Communications. 2015. 195: p. 95-101. :l
:ule

View File

@ -26,7 +26,7 @@ Define a computation that calculates the CNA (Common Neighbor
Analysis) pattern for each atom in the group. In solid-state systems
the CNA pattern is a useful measure of the local crystal structure
around an atom. The CNA methodology is described in "(Faken)"_#Faken
and "(Tsuzuki)"_#Tsuzuki.
and "(Tsuzuki)"_#Tsuzuki1.
Currently, there are five kinds of CNA patterns LAMMPS recognizes:
@ -93,5 +93,5 @@ above.
:link(Faken)
[(Faken)] Faken, Jonsson, Comput Mater Sci, 2, 279 (1994).
:link(Tsuzuki)
:link(Tsuzuki1)
[(Tsuzuki)] Tsuzuki, Branicio, Rino, Comput Phys Comm, 177, 518 (2007).

View File

@ -0,0 +1,111 @@
"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
compute cnp/atom command :h3
[Syntax:]
compute ID group-ID cnp/atom cutoff :pre
ID, group-ID are documented in "compute"_compute.html command
cnp/atom = style name of this compute command
cutoff = cutoff distance for nearest neighbors (distance units) :ul
[Examples:]
compute 1 all cnp/atom 3.08 :pre
[Description:]
Define a computation that calculates the Common Neighborhood
Parameter (CNP) for each atom in the group. In solid-state systems
the CNP is a useful measure of the local crystal structure
around an atom and can be used to characterize whether the
atom is part of a perfect lattice, a local defect (e.g. a dislocation
or stacking fault), or at a surface.
The value of the CNP parameter will be 0.0 for atoms not in the
specified compute group. Note that normally a CNP calculation should
only be performed on single component systems.
This parameter is computed using the following formula from
"(Tsuzuki)"_#Tsuzuki2
:c,image(Eqs/cnp_eq.jpg)
where the index {j} goes over the {n}i nearest neighbors of atom
{i}, and the index {k} goes over the {n}ij common nearest neighbors
between atom {i} and atom {j}. Rik and Rjk are the vectors connecting atom
{k} to atoms {i} and {j}. The quantity in the double sum is computed
for each atom.
The CNP calculation is sensitive to the specified cutoff value.
You should ensure that the appropriate nearest neighbors of an atom are
found within the cutoff distance for the presumed crystal structure.
E.g. 12 nearest neighbor for perfect FCC and HCP crystals, 14 nearest
neighbors for perfect BCC crystals. These formulas can be used to
obtain a good cutoff distance:
:c,image(Eqs/cnp_cutoff.jpg)
where a is the lattice constant for the crystal structure concerned
and in the HCP case, x = (c/a) / 1.633, where 1.633 is the ideal c/a
for HCP crystals.
Also note that since the CNP calculation in LAMMPS uses the neighbors
of an owned atom to find the nearest neighbors of a ghost atom, the
following relation should also be satisfied:
:c,image(Eqs/cnp_cutoff2.jpg)
where Rc is the cutoff distance of the potential, Rs is the skin
distance as specified by the "neighbor"_neighbor.html command, and
cutoff is the argument used with the compute cnp/atom command. LAMMPS
will issue a warning if this is not the case.
The neighbor list needed to compute this quantity is constructed each
time the calculation is performed (e.g. each time a snapshot of atoms
is dumped). Thus it can be inefficient to compute/dump this quantity
too frequently or to have multiple compute/dump commands, each with a
{cnp/atom} style.
[Output info:]
This compute calculates a per-atom vector, which can be accessed by
any command that uses per-atom values from a compute as input. See
"Section 6.15"_Section_howto.html#howto_15 for an overview of
LAMMPS output options.
The per-atom vector values will be real positive numbers. Some typical CNP
values:
FCC lattice = 0.0
BCC lattice = 0.0
HCP lattice = 4.4 :pre
FCC (111) surface ~ 13.0
FCC (100) surface ~ 26.5
FCC dislocation core ~ 11 :pre
[Restrictions:]
This compute is part of the USER-MISC 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:]
"compute cna/atom"_compute_cna_atom.html
"compute centro/atom"_compute_centro_atom.html
[Default:] none
:line
:link(Tsuzuki2)
[(Tsuzuki)] Tsuzuki, Branicio, Rino, Comput Phys Comm, 177, 518 (2007).

View File

@ -111,26 +111,26 @@ Coefficients parameterized by "(Fox)"_#Fox are assigned for each
atom type designating the chemical symbol and charge of each atom
type. Valid chemical symbols for compute saed are:
H: He: Li: Be: B:
C: N: O: F: Ne:
Na: Mg: Al: Si: P:
S: Cl: Ar: K: Ca:
Sc: Ti: V: Cr: Mn:
Fe: Co: Ni: Cu: Zn:
Ga: Ge: As: Se: Br:
Kr: Rb: Sr: Y: Zr:
Nb: Mo: Tc: Ru: Rh:
Pd: Ag: Cd: In: Sn:
Sb: Te: I: Xe: Cs:
Ba: La: Ce: Pr: Nd:
Pm: Sm: Eu: Gd: Tb:
Dy: Ho: Er: Tm: Yb:
Lu: Hf: Ta: W: Re:
Os: Ir: Pt: Au: Hg:
Tl: Pb: Bi: Po: At:
Rn: Fr: Ra: Ac: Th:
Pa: U: Np: Pu: Am:
Cm: Bk: Cf:tb(c=5,s=:)
H: He: Li: Be: B:
C: N: O: F: Ne:
Na: Mg: Al: Si: P:
S: Cl: Ar: K: Ca:
Sc: Ti: V: Cr: Mn:
Fe: Co: Ni: Cu: Zn:
Ga: Ge: As: Se: Br:
Kr: Rb: Sr: Y: Zr:
Nb: Mo: Tc: Ru: Rh:
Pd: Ag: Cd: In: Sn:
Sb: Te: I: Xe: Cs:
Ba: La: Ce: Pr: Nd:
Pm: Sm: Eu: Gd: Tb:
Dy: Ho: Er: Tm: Yb:
Lu: Hf: Ta: W: Re:
Os: Ir: Pt: Au: Hg:
Tl: Pb: Bi: Po: At:
Rn: Fr: Ra: Ac: Th:
Pa: U: Np: Pu: Am:
Cm: Bk: Cf:tb(c=5,s=:)
If the {echo} keyword is specified, compute saed will provide extra

View File

@ -231,11 +231,12 @@ the numbers of columns are 930, 2790, and 5580, respectively.
If the {quadratic} keyword value is set to 1, then additional
columns are appended to each per-atom array, corresponding to
a matrix of quantities that are products of two bispectrum components. If the
number of bispectrum components is {K}, then the number of matrix elements
is {K}^2. These are output in subblocks of {K}^2 columns, using the same
ordering of columns and sub-blocks as was used for the bispectrum
components.
the products of all distinct pairs of bispectrum components. If the
number of bispectrum components is {K}, then the number of distinct pairs
is {K}({K}+1)/2. These are output in subblocks of {K}({K}+1)/2 columns, using the same
ordering of sub-blocks as was used for the bispectrum
components. Within each sub-block, the ordering is upper-triangular,
(1,1),(1,2)...(1,{K}),(2,1)...({K}-1,{K}-1),({K}-1,{K}),({K},{K})
These values can be accessed by any command that uses per-atom values
from a compute as input. See "Section

View File

@ -17,6 +17,7 @@ Computes :h1
compute_chunk_atom
compute_cluster_atom
compute_cna_atom
compute_cnp_atom
compute_com
compute_com_chunk
compute_contact_atom

View File

@ -18,6 +18,7 @@ dihedral_coeff 1 1 286.1 1 124 1 1 90.0 0 1 90.0 0
dihedral_coeff 1 3 69.3 1 93.9 1 1 90 0 1 90 0 &
49.1 0 0.00 0 1 74.4 1 0 0.00 0 &
25.2 0 0.00 0 0 0.00 0 1 48.1 1
:pre
[Description:]

View File

@ -16,7 +16,8 @@ dump-ID = ID of dump to modify :ulb,l
one or more keyword/value pairs may be appended :l
these keywords apply to various dump styles :l
keyword = {append} or {buffer} or {element} or {every} or {fileper} or {first} or {flush} or {format} or {image} or {label} or {nfile} or {pad} or {precision} or {region} or {scale} or {sort} or {thresh} or {unwrap} :l
{append} arg = {yes} or {no}
{append} arg = {yes} or {no} or {at} N
N = index of frame written upon first dump
{buffer} arg = {yes} or {no}
{element} args = E1 E2 ... EN, where N = # of atom types
E1,...,EN = element name, e.g. C or Fe or Ga
@ -41,6 +42,7 @@ keyword = {append} or {buffer} or {element} or {every} or {fileper} or {first} o
{region} arg = region-ID or "none"
{scale} arg = {yes} or {no}
{sfactor} arg = coordinate scaling factor (> 0.0)
{thermo} arg = {yes} or {no}
{tfactor} arg = time scaling factor (> 0.0)
{sort} arg = {off} or {id} or N or -N
off = no sorting of per-atom lines within a snapshot
@ -139,12 +141,13 @@ and {dcd}. It also applies only to text output files, not to binary
or gzipped or image/movie files. If specified as {yes}, then dump
snapshots are appended to the end of an existing dump file. If
specified as {no}, then a new dump file will be created which will
overwrite an existing file with the same name. This keyword can only
take effect if the dump_modify command is used after the
"dump"_dump.html command, but before the first command that causes
dump snapshots to be output, e.g. a "run"_run.html or
"minimize"_minimize.html command. Once the dump file has been opened,
this keyword has no further effect.
overwrite an existing file with the same name. If the {at} option is present
({netcdf} only), then the frame to append to can be specified. Negative values
are counted from the end of the file. This keyword can only take effect if the
dump_modify command is used after the "dump"_dump.html command, but before the
first command that causes dump snapshots to be output, e.g. a "run"_run.html or
"minimize"_minimize.html command. Once the dump file has been opened, this
keyword has no further effect.
:line
@ -413,6 +416,13 @@ most effective when the typical magnitude of position data is between
:line
The {thermo} keyword ({netcdf} only) triggers writing of "thermo"_thermo.html
information to the dump file alongside per-atom data. The data included in the
dump file is identical to the data specified by
"thermo_style"_thermo_style.html.
:line
The {region} keyword only applies to the dump {custom}, {cfg},
{image}, and {movie} styles. If specified, only atoms in the region
will be written to the dump file or included in the image/movie. Only

View File

@ -24,7 +24,7 @@ args = list of atom attributes, same as for "dump_style custom"_dump.html :l,ule
[Examples:]
dump 1 all netcdf 100 traj.nc type x y z vx vy vz
dump_modify 1 append yes at -1 global c_thermo_pe c_thermo_temp c_thermo_press
dump_modify 1 append yes at -1 thermo yes
dump 1 all netcdf/mpiio 1000 traj.nc id type x y z :pre
[Description:]
@ -44,7 +44,7 @@ rank.
NetCDF files can be directly visualized via the following tools:
Ovito (http://www.ovito.org/). Ovito supports the AMBER convention and
all of the above extensions. :ule,b
all extensions of this dump style. :ule,b
VMD (http://www.ks.uiuc.edu/Research/vmd/). :l
@ -52,15 +52,9 @@ AtomEye (http://www.libatoms.org/). The libAtoms version of AtomEye
contains a NetCDF reader that is not present in the standard
distribution of AtomEye. :l,ule
In addition to per-atom data, global data can be included in the dump
file, which are the kinds of values output by the
"thermo_style"_thermo_style.html command . See "Section howto
6.15"_Section_howto.html#howto_15 for an explanation of per-atom
versus global data. The global output written into the dump file can
be from computes, fixes, or variables, by prefixing the compute/fix ID
or variable name with "c_" or "f_" or "v_" respectively, as in the
example above. These global values are specified via the "dump_modify
global"_dump_modify.html command.
In addition to per-atom data, "thermo"_thermo.html data can be included in the
dump file. The data included in the dump file is identical to the data specified
by "thermo_style"_thermo_style.html.
:link(netcdf-home,http://www.unidata.ucar.edu/software/netcdf/)
:link(pnetcdf-home,http://trac.mcs.anl.gov/projects/parallel-netcdf/)

View File

@ -47,7 +47,7 @@ keyword = {scale} or {reset} :l
fix 1 all adapt 1 pair soft a 1 1 v_prefactor
fix 1 all adapt 1 pair soft a 2* 3 v_prefactor
fix 1 all adapt 1 pair lj/cut epsilon * * v_scale1 coul/cut scale 3 3 v_scale2 scale yes reset yes
fix 1 all adapt 10 atom diameter v_size
fix 1 all adapt 10 atom diameter v_size :pre
variable ramp_up equal "ramp(0.01,0.5)"
fix stretch all adapt 1 bond harmonic r0 1 v_ramp_up :pre

View File

@ -565,8 +565,10 @@ more instructions on how to use the accelerated styles effectively.
[Restart, fix_modify, output, run start/stop, minimize info:]
No information about this fix is written to "binary restart
files"_restart.html. None of the "fix_modify"_fix_modify.html options
This fix will restore the initial box settings from "binary restart
files"_restart.html, which allows the fix to be properly continue
deformation, when using the start/stop options of the "run"_run.html
command. 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.

View File

@ -68,7 +68,7 @@ matrix that gives canonical sampling for a given A is computed automatically.
However, the GLE framework also allow for non-equilibrium sampling, that
can be used for instance to model inexpensively zero-point energy
effects "(Ceriotti2)"_#Ceriotti2. This is achieved specifying the {noneq}
keyword followed by the name of the file that contains the static covariance
keyword followed by the name of the file that contains the static covariance
matrix for the non-equilibrium dynamics. Please note, that the covariance
matrix is expected to be given in [temperature units].

View File

@ -67,11 +67,11 @@ The Langevin forces are computed as
\(F_r'\) is a random force proportional to
\(\sqrt \{ \frac \{2\, k_B \mathtt\{Tcom\}\, m'\}
\{\mathrm dt\, \mathtt\{damp\_com\} \}
\} \). :b
\} \).
\(f_r'\) is a random force proportional to
\(\sqrt \{ \frac \{2\, k_B \mathtt\{Tdrude\}\, m'\}
\{\mathrm dt\, \mathtt\{damp\_drude\} \}
\} \). :b
\} \).
Then the real forces acting on the particles are computed from the inverse
transform:
\begin\{equation\} F = \frac M \{M'\}\, F' - f' \end\{equation\}

View File

@ -10,68 +10,183 @@ fix neb command :h3
[Syntax:]
fix ID group-ID neb Kspring :pre
fix ID group-ID neb Kspring keyword value :pre
ID, group-ID are documented in "fix"_fix.html command
neb = style name of this fix command
Kspring = inter-replica spring constant (force/distance units) :ul
ID, group-ID are documented in "fix"_fix.html command :ulb,l
neb = style name of this fix command :l
Kspring = spring constant for parallel nudging force (force/distance units or force units, see parallel keyword) :l
zero or more keyword/value pairs may be appended :l
keyword = {parallel} or {perp} or {end} :l
{parallel} value = {neigh} or {ideal}
{neigh} = parallel nudging force based on distance to neighbor replicas (Kspring = force/distance units)
{ideal} = parallel nudging force based on interpolated ideal position (Kspring = force units)
{perp} value = {Kspring2}
{Kspring2} = spring constant for perpendicular nudging force (force/distance units)
{end} values = estyle Kspring3
{estyle} = {first} or {last} or {last/efirst} or {last/efirst/middle}
{first} = apply force to first replica
{last} = apply force to last replica
{last/efirst} = apply force to last replica and set its target energy to that of first replica
{last/efirst/middle} = same as {last/efirst} plus prevent middle replicas having lower energy than first replica
{Kspring3} = spring constant for target energy term (1/distance units) :pre,ule
[Examples:]
fix 1 active neb 10.0 :pre
fix 1 active neb 10.0
fix 2 all neb 1.0 perp 1.0 end last
fix 2 all neb 1.0 perp 1.0 end first 1.0 end last 1.0
fix 1 all neb 1.0 nudge ideal end last/efirst 1 :pre
[Description:]
Add inter-replica forces to atoms in the group for a multi-replica
Add nudging forces to atoms in the group for a multi-replica
simulation run via the "neb"_neb.html command to perform a nudged
elastic band (NEB) calculation for transition state finding. Hi-level
explanations of NEB are given with the "neb"_neb.html command and in
"Section 6.5"_Section_howto.html#howto_5 of the manual. The fix
neb command must be used with the "neb" command to define how
inter-replica forces are computed.
elastic band (NEB) calculation for finding the transition state.
Hi-level explanations of NEB are given with the "neb"_neb.html command
and in "Section_howto 5"_Section_howto.html#howto_5 of the manual.
The fix neb command must be used with the "neb" command and defines
how inter-replica nudging forces are computed. A NEB calculation is
divided in two stages. In the first stage n replicas are relaxed
toward a MEP until convergence. In the second stage, the climbing
image scheme (see "(Henkelman2)"_#Henkelman2) is enabled, so that the
replica having the highest energy relaxes toward the saddle point
(i.e. the point of highest energy along the MEP), and a second
relaxation is performed.
Only the N atoms in the fix group experience inter-replica forces.
Atoms in the two end-point replicas do not experience these forces,
but those in intermediate replicas do. During the initial stage of
NEB, the 3N-length vector of interatomic forces Fi = -Grad(V) acting
on the atoms of each intermediate replica I is altered, as described
in the "(Henkelman1)"_#Henkelman1 paper, to become:
A key purpose of the nudging forces is to keep the replicas equally
spaced. During the NEB calculation, the 3N-length vector of
interatomic force Fi = -Grad(V) for each replica I is altered. For
all intermediate replicas (i.e. for 1 < I < N, except the climbing
replica) the force vector becomes:
Fi = -Grad(V) + (Grad(V) dot That) That + Kspring (| Ri+i - Ri | - | Ri - Ri-1 |) That :pre
Fi = -Grad(V) + (Grad(V) dot T') T' + Fnudge_parallel + Fnudge_perp :pre
Ri are the atomic coordinates of replica I; Ri-1 and Ri+1 are the
coordinates of its neighbor replicas. That (t with a hat over it) is
the unit "tangent" vector for replica I which is a function of Ri,
T' is the unit "tangent" vector for replica I and is a function of Ri,
Ri-1, Ri+1, and the potential energy of the 3 replicas; it points
roughly in the direction of (Ri+i - Ri-1); see the
"(Henkelman1)"_#Henkelman1 paper for details.
"(Henkelman1)"_#Henkelman1 paper for details. Ri are the atomic
coordinates of replica I; Ri-1 and Ri+1 are the coordinates of its
neighbor replicas. The term (Grad(V) dot T') is used to remove the
component of the gradient parallel to the path which would tend to
distribute the replica unevenly along the path. Fnudge_parallel is an
artificial nudging force which is applied only in the tangent
direction and which maintains the equal spacing between replicas (see
below for more information). Fnudge_perp is an optional artificial
spring which is applied in a direction perpendicular to the tangent
direction and which prevent the paths from forming acute kinks (see
below for more information).
The first two terms in the above equation are the component of the
interatomic forces perpendicular to the tangent vector. The last term
is a spring force between replica I and its neighbors, parallel to the
tangent vector direction with the specified spring constant {Kspring}.
In the second stage of the NEB calculation, the interatomic force Fi
for the climbing replica (the replica of highest energy after the
first stage) is changed to:
The effect of the first two terms is to push the atoms of each replica
toward the minimum energy path (MEP) of conformational states that
transition over the energy barrier. The MEP for an energy barrier is
defined as a sequence of 3N-dimensional states which cross the barrier
at its saddle point, each of which has a potential energy gradient
parallel to the MEP itself.
Fi = -Grad(V) + 2 (Grad(V) dot T') T' :pre
The effect of the last term is to push each replica away from its two
neighbors in a direction along the MEP, so that the final set of
states are equidistant from each other.
and the relaxation procedure is continued to a new converged MEP.
During the second stage of NEB, the forces on the N atoms in the
replica nearest the top of the energy barrier are altered so that it
climbs to the top of the barrier and finds the saddle point. The
forces on atoms in this replica are described in the
"(Henkelman2)"_#Henkelman2 paper, and become:
:line
Fi = -Grad(V) + 2 (Grad(V) dot That) That :pre
The keyword {parallel} specifies how the parallel nudging force is
computed. With a value of {neigh}, the parallel nudging force is
computed as in "(Henkelman1)"_#Henkelman1 by connecting each
intermediate replica with the previous and the next image:
The inter-replica forces for the other replicas are unchanged from the
first equation.
Fnudge_parallel = {Kspring} * (|Ri+1 - Ri| - |Ri - Ri-1|) :pre
Note that in this case the specified {Kspring) is in force/distance
units.
With a value of {ideal}, the spring force is computed as suggested in
"(WeinenE)"_#WeinenE :
Fnudge_parallel = -{Kspring} * (RD-RDideal) / (2 * meanDist) :pre
where RD is the "reaction coordinate" see "neb"_neb.html section, and
RDideal is the ideal RD for which all the images are equally spaced.
I.e. RDideal = (I-1)*meanDist when the climbing replica is off, where
I is the replica number). The meanDist is the average distance
between replicas. Note that in this case the specified {Kspring) is
in force units.
Note that the {ideal} form of nudging can often be more effective at
keeping the replicas equally spaced.
:line
The keyword {perp} specifies if and how a perpendicual nudging force
is computed. It adds a spring force perpendicular to the path in
order to prevent the path from becoming too kinky. It can
significantly improve the convergence of the NEB calculation when the
resolution is poor. I.e. when few replicas are used; see
"(Maras)"_#Maras1 for details.
The perpendicular spring force is given by
Fnudge_perp = {Kspring2} * F(Ri-1,Ri,Ri+1) (Ri+1 + Ri-1 - 2 Ri) :pre
where {Kspring2} is the specified value. F(Ri-1 Ri R+1) is a smooth
scalar function of the angle Ri-1 Ri Ri+1. It is equal to 0.0 when
the path is straight and is equal to 1 when the angle Ri-1 Ri Ri+1 is
acute. F(Ri-1 Ri R+1) is defined in "(Jonsson)"_#Jonsson.
If {Kspring2} is set to 0.0 (the default) then no perpendicular spring
force is added.
:line
By default, no additional forces act on the first and last replicas
during the NEB relaxation, so these replicas simply relax toward their
respective local minima. By using the key word {end}, additional
forces can be applied to the first and/or last replicas, to enable
them to relax toward a MEP while constraining their energy.
The interatomic force Fi for the specified replica becomes:
Fi = -Grad(V) + (Grad(V) dot T' + (E-ETarget)*Kspring3) T', {when} Grad(V) dot T' < 0
Fi = -Grad(V) + (Grad(V) dot T' + (ETarget- E)*Kspring3) T', {when} Grad(V) dot T' > 0
:pre
where E is the current energy of the replica and ETarget is the target
energy. The "spring" constant on the difference in energies is the
specified {Kspring3} value.
When {estyle} is specified as {first}, the force is applied to the
first replica. When {estyle} is specified as {last}, the force is
applied to the last replica. Note that the {end} keyword can be used
twice to add forces to both the first and last replicas.
For both these {estyle} settings, the target energy {ETarget} is set
to the initial energy of the replica (at the start of the NEB
calculation).
If the {estyle} is specified as {last/efirst} or {last/efirst/middle},
force is applied to the last replica, but the target energy {ETarget}
is continuously set to the energy of the first replica, as it evolves
during the NEB relaxation.
The difference between these two {estyle} options is as follows. When
{estyle} is specified as {last/efirst}, no change is made to the
inter-replica force applied to the intermediate replicas (neither
first or last). If the initial path is too far from the MEP, an
intermediate repilica may relax "faster" and reach a lower energy than
the last replica. In this case the intermediate replica will be
relaxing toward its own local minima. This behavior can be prevented
by specifying {estyle} as {last/efirst/middle} which will alter the
inter-replica force applied to intermediate replicas by removing the
contribution of the gradient to the inter-replica force. This will
only be done if a particular intermediate replica has a lower energy
than the first replica. This should effectively prevent the
intermediate replicas from over-relaxing.
After converging a NEB calculation using an {estyle} of
{last/efirst/middle}, you should check that all intermediate replicas
have a larger energy than the first replica. If this is not the case,
the path is probably not a MEP.
Finally, note that if the last replica converges toward a local
minimum which has a larger energy than the energy of the first
replica, a NEB calculation using an {estyle} of {last/efirst} or
{last/efirst/middle} cannot reach final convergence.
[Restart, fix_modify, output, run start/stop, minimize info:]
@ -96,7 +211,12 @@ for more info on packages.
"neb"_neb.html
[Default:] none
[Default:]
The option defaults are nudge = neigh, perp = 0.0, ends is not
specified (no inter-replica force on the end replicas).
:line
:link(Henkelman1)
[(Henkelman1)] Henkelman and Jonsson, J Chem Phys, 113, 9978-9985 (2000).
@ -104,3 +224,15 @@ for more info on packages.
:link(Henkelman2)
[(Henkelman2)] Henkelman, Uberuaga, Jonsson, J Chem Phys, 113,
9901-9904 (2000).
:link(WeinenE)
[(WeinenE)] E, Ren, Vanden-Eijnden, Phys Rev B, 66, 052301 (2002).
:link(Jonsson)
[(Jonsson)] Jonsson, Mills and Jacobsen, in Classical and Quantum
Dynamics in Condensed Phase Simulations, edited by Berne, Ciccotti,
and Coker World Scientific, Singapore, 1998, p 385.
:link(Maras1)
[(Maras)] Maras, Trushin, Stukowski, Ala-Nissila, Jonsson,
Comp Phys Comm, 205, 13-21 (2016).

View File

@ -8,17 +8,19 @@
fix qeq/reax command :h3
fix qeq/reax/kk command :h3
fix qeq/reax/omp command :h3
[Syntax:]
fix ID group-ID qeq/reax Nevery cutlo cuthi tolerance params :pre
fix ID group-ID qeq/reax Nevery cutlo cuthi tolerance params args :pre
ID, group-ID are documented in "fix"_fix.html command
qeq/reax = style name of this fix command
Nevery = perform QEq every this many steps
cutlo,cuthi = lo and hi cutoff for Taper radius
tolerance = precision to which charges will be equilibrated
params = reax/c or a filename :ul
params = reax/c or a filename
args = {dual} (optional) :ul
[Examples:]
@ -59,6 +61,10 @@ potential file, except that eta is defined here as twice the eta value
in the ReaxFF file. Note that unlike the rest of LAMMPS, the units
of this fix are hard-coded to be A, eV, and electronic charge.
The optional {dual} keyword allows to perform the optimization
of the S and T matrices in parallel. This is only supported for
the {qeq/reax/omp} style. Otherwise they are processed separately.
[Restart, fix_modify, output, run start/stop, minimize info:]
No information about this fix is written to "binary restart

View File

@ -31,11 +31,12 @@ bodystyle = {single} or {molecule} or {group} :l
groupID1, groupID2, ... = list of N group IDs :pre
zero or more keyword/value pairs may be appended :l
keyword = {langevin} or {temp} or {iso} or {aniso} or {x} or {y} or {z} or {couple} or {tparam} or {pchain} or {dilate} or {force} or {torque} or {infile} :l
keyword = {langevin} or {reinit} or {temp} or {iso} or {aniso} or {x} or {y} or {z} or {couple} or {tparam} or {pchain} or {dilate} or {force} or {torque} or {infile} :l
{langevin} values = Tstart Tstop Tperiod seed
Tstart,Tstop = desired temperature at start/stop of run (temperature units)
Tdamp = temperature damping parameter (time units)
seed = random number seed to use for white noise (positive integer)
{reinit} = {yes} or {no}
{temp} values = Tstart Tstop Tdamp
Tstart,Tstop = desired temperature at start/stop of run (temperature units)
Tdamp = temperature damping parameter (time units)
@ -68,10 +69,10 @@ keyword = {langevin} or {temp} or {iso} or {aniso} or {x} or {y} or {z} or {coup
[Examples:]
fix 1 clump rigid single
fix 1 clump rigid single reinit yes
fix 1 clump rigid/small molecule
fix 1 clump rigid single force 1 off off on langevin 1.0 1.0 1.0 428984
fix 1 polychains rigid/nvt molecule temp 1.0 1.0 5.0
fix 1 polychains rigid/nvt molecule temp 1.0 1.0 5.0 reinit no
fix 1 polychains rigid molecule force 1*5 off off off force 6*10 off off on
fix 1 polychains rigid/small molecule langevin 1.0 1.0 1.0 428984
fix 2 fluid rigid group 3 clump1 clump2 clump3 torque * off off off
@ -87,7 +88,12 @@ means that each timestep the total force and torque on each rigid body
is computed as the sum of the forces and torques on its constituent
particles. The coordinates, velocities, and orientations of the atoms
in each body are then updated so that the body moves and rotates as a
single entity.
single entity. This is implemented by creating internal data structures
for each rigid body and performing time integration on these data
structures. Positions, velocities, and orientations of the constituent
particles are regenerated from the rigid body data structures in every
time step. This restricts which operations and fixes can be applied to
rigid bodies. See below for a detailed discussion.
Examples of large rigid bodies are a colloidal particle, or portions
of a biomolecule such as a protein.
@ -148,8 +154,9 @@ differences may accumulate to produce divergent trajectories.
NOTE: You should not update the atoms in rigid bodies via other
time-integration fixes (e.g. "fix nve"_fix_nve.html, "fix
nvt"_fix_nh.html, "fix npt"_fix_nh.html), or you will be integrating
their motion more than once each timestep. When performing a hybrid
nvt"_fix_nh.html, "fix npt"_fix_nh.html, "fix move"_fix_move.html),
or you will have conflicting updates to positions and velocities
resulting in unphysical behavior in most cases. When performing a hybrid
simulation with some atoms in rigid bodies, and some not, a separate
time integration fix like "fix nve"_fix_nve.html or "fix
nvt"_fix_nh.html should be used for the non-rigid particles.
@ -165,23 +172,29 @@ setting the force on them to 0.0 (via the "fix
setforce"_fix_setforce.html command), and integrating them as usual
(e.g. via the "fix nve"_fix_nve.html command).
NOTE: The aggregate properties of each rigid body are calculated one
time at the start of the first simulation run after these fixes are
specified. The properties include the position and velocity of the
center-of-mass of the body, its moments of inertia, and its angular
momentum. This is done using the properties of the constituent atoms
of the body at that point in time (or see the {infile} keyword
option). Thereafter, changing properties of individual atoms in the
body will have no effect on a rigid body's dynamics, unless they
affect the "pair_style"_pair_style.html interactions that individual
particles are part of. For example, you might think you could
displace the atoms in a body or add a large velocity to each atom in a
body to make it move in a desired direction before a 2nd run is
IMPORTANT NOTE: The aggregate properties of each rigid body are
calculated at the start of a simulation run and are maintained in
internal data structures. The properties include the position and
velocity of the center-of-mass of the body, its moments of inertia, and
its angular momentum. This is done using the properties of the
constituent atoms of the body at that point in time (or see the {infile}
keyword option). Thereafter, changing these properties of individual
atoms in the body will have no effect on a rigid body's dynamics, unless
they effect any computation of per-atom forces or torques. If the
keyword {reinit} is set to {yes} (the default), the rigid body data
structures will be recreated at the beginning of each {run} command;
if the keyword {reinit} is set to {no}, the rigid body data structures
will be built only at the very first {run} command and maintained for
as long as the rigid fix is defined. For example, you might think you
could displace the atoms in a body or add a large velocity to each atom
in a body to make it move in a desired direction before a 2nd run is
performed, using the "set"_set.html or
"displace_atoms"_displace_atoms.html or "velocity"_velocity.html
command. But these commands will not affect the internal attributes
of the body, and the position and velocity of individual atoms in the
body will be reset when time integration starts.
commands. But these commands will not affect the internal attributes
of the body unless {reinit} is set to {yes}. With {reinit} set to {no}
(or using the {infile} option, which implies {reinit} {no}) the position
and velocity of individual atoms in the body will be reset when time
integration starts again.
:line
@ -401,6 +414,14 @@ couple none :pre
The keyword/value option pairs are used in the following ways.
The {reinit} keyword determines, whether the rigid body properties
are reinitialized between run commands. With the option {yes} (the
default) this is done, with the option {no} this is not done. Turning
off the reinitialization can be helpful to protect rigid bodies against
unphysical manipulations between runs or when properties cannot be
easily recomputed (e.g. when read from a file). When using the {infile}
keyword, the {reinit} option is automatically set to {no}.
The {langevin} and {temp} and {tparam} keywords perform thermostatting
of the rigid bodies, altering both their translational and rotational
degrees of freedom. What is meant by "temperature" of a collection of
@ -778,7 +799,7 @@ exclude, "fix shake"_fix_shake.html
The option defaults are force * on on on and torque * on on on,
meaning all rigid bodies are acted on by center-of-mass force and
torque. Also Tchain = Pchain = 10, Titer = 1, Torder = 3.
torque. Also Tchain = Pchain = 10, Titer = 1, Torder = 3, reinit = yes.
:line

View File

@ -308,7 +308,8 @@ The option defaults are mesh = mesh/disp = 0 0 0, order = order/disp =
gewald = gewald/disp = 0.0, slab = 1.0, compute = yes, cutoff/adjust =
yes (MSM), pressure/scalar = yes (MSM), fftbench = yes (PPPM), diff = ik
(PPPM), mix/disp = pair, force/disp/real = -1.0, force/disp/kspace = -1.0,
split = 0, tol = 1.0e-6, and disp/auto = no.
split = 0, tol = 1.0e-6, and disp/auto = no. For pppm/intel, order =
order/disp = 7.
:line

View File

@ -33,12 +33,16 @@ style = {none} or {ewald} or {ewald/disp} or {ewald/omp} or {pppm} or {pppm/cg}
accuracy = desired relative error in forces
{pppm/gpu} value = accuracy
accuracy = desired relative error in forces
{pppm/intel} value = accuracy
accuracy = desired relative error in forces
{pppm/kk} value = accuracy
accuracy = desired relative error in forces
{pppm/omp} value = accuracy
accuracy = desired relative error in forces
{pppm/cg/omp} value = accuracy
accuracy = desired relative error in forces
{pppm/disp/intel} value = accuracy
accuracy = desired relative error in forces
{pppm/tip4p/omp} value = accuracy
accuracy = desired relative error in forces
{pppm/stagger} value = accuracy

View File

@ -301,6 +301,7 @@ compute_centro_atom.html
compute_chunk_atom.html
compute_cluster_atom.html
compute_cna_atom.html
compute_cnp_atom.html
compute_com.html
compute_com_chunk.html
compute_contact_atom.html
@ -446,7 +447,6 @@ pair_lj96.html
pair_lj_cubic.html
pair_lj_expand.html
pair_lj_long.html
pair_lj_sf.html
pair_lj_smooth.html
pair_lj_smooth_linear.html
pair_lj_soft.html

View File

@ -24,14 +24,15 @@ to the relevant fixes.
{manifold} @ {parameters} @ {equation} @ {description}
cylinder @ R @ x^2 + y^2 - R^2 = 0 @ Cylinder along z-axis, axis going through (0,0,0)
cylinder_dent @ R l a @ x^2 + y^2 - r(z)^2 = 0, r(x) = R if | z | > l, r(z) = R - a*(1 + cos(z/l))/2 otherwise @ A cylinder with a dent around z = 0
dumbbell @ a A B c @ -( x^2 + y^2 ) * (a^2 - z^2/c^2) * ( 1 + (A*sin(B*z^2))^4) = 0 @ A dumbbell @
dumbbell @ a A B c @ -( x^2 + y^2 ) + (a^2 - z^2/c^2) * ( 1 + (A*sin(B*z^2))^4) = 0 @ A dumbbell
ellipsoid @ a b c @ (x/a)^2 + (y/b)^2 + (z/c)^2 = 0 @ An ellipsoid
gaussian_bump @ A l rc1 rc2 @ if( x < rc1) -z + A * exp( -x^2 / (2 l^2) ); else if( x < rc2 ) -z + a + b*x + c*x^2 + d*x^3; else z @ A Gaussian bump at x = y = 0, smoothly tapered to a flat plane z = 0.
plane @ a b c x0 y0 z0 @ a*(x-x0) + b*(y-y0) + c*(z-z0) = 0 @ A plane with normal (a,b,c) going through point (x0,y0,z0)
plane_wiggle @ a w @ z - a*sin(w*x) = 0 @ A plane with a sinusoidal modulation on z along x.
sphere @ R @ x^2 + y^2 + z^2 - R^2 = 0 @ A sphere of radius R
supersphere @ R q @ | x |^q + | y |^q + | z |^q - R^q = 0 @ A supersphere of hyperradius R
spine @ a, A, B, B2, c @ -(x^2 + y^2)*(a^2 - z^2/f(z)^2)*(1 + (A*sin(g(z)*z^2))^4), f(z) = c if z > 0, 1 otherwise; g(z) = B if z > 0, B2 otherwise @ An approximation to a dendtritic spine
spine_two @ a, A, B, B2, c @ -(x^2 + y^2)*(a^2 - z^2/f(z)^2)*(1 + (A*sin(g(z)*z^2))^2), f(z) = c if z > 0, 1 otherwise; g(z) = B if z > 0, B2 otherwise @ Another approximation to a dendtritic spine
spine @ a, A, B, B2, c @ -(x^2 + y^2) + (a^2 - z^2/f(z)^2)*(1 + (A*sin(g(z)*z^2))^4), f(z) = c if z > 0, 1 otherwise; g(z) = B if z > 0, B2 otherwise @ An approximation to a dendtritic spine
spine_two @ a, A, B, B2, c @ -(x^2 + y^2) + (a^2 - z^2/f(z)^2)*(1 + (A*sin(g(z)*z^2))^2), f(z) = c if z > 0, 1 otherwise; g(z) = B if z > 0, B2 otherwise @ Another approximation to a dendtritic spine
thylakoid @ wB LB lB @ Various, see "(Paquay)"_#Paquay1 @ A model grana thylakoid consisting of two block-like compartments connected by a bridge of width wB, length LB and taper length lB
torus @ R r @ (R - sqrt( x^2 + y^2 ) )^2 + z^2 - r^2 @ A torus with large radius R and small radius r, centered on (0,0,0) :tb(s=@)

View File

@ -10,28 +10,31 @@ neb command :h3
[Syntax:]
neb etol ftol N1 N2 Nevery file-style arg :pre
neb etol ftol N1 N2 Nevery file-style arg keyword :pre
etol = stopping tolerance for energy (energy units) :ulb,l
ftol = stopping tolerance for force (force units) :l
N1 = max # of iterations (timesteps) to run initial NEB :l
N2 = max # of iterations (timesteps) to run barrier-climbing NEB :l
Nevery = print replica energies and reaction coordinates every this many timesteps :l
file-style= {final} or {each} or {none} :l
file-style = {final} or {each} or {none} :l
{final} arg = filename
filename = file with initial coords for final replica
coords for intermediate replicas are linearly interpolated between first and last replica
coords for intermediate replicas are linearly interpolated
between first and last replica
{each} arg = filename
filename = unique filename for each replica (except first) with its initial coords
{none} arg = no argument
all replicas assumed to already have their initial coords :pre
filename = unique filename for each replica (except first)
with its initial coords
{none} arg = no argument all replicas assumed to already have
their initial coords :pre
keyword = {verbose}
:ule
[Examples:]
neb 0.1 0.0 1000 500 50 final coords.final
neb 0.0 0.001 1000 500 50 each coords.initial.$i
neb 0.0 0.001 1000 500 50 none :pre
neb 0.0 0.001 1000 500 50 none verbose :pre
[Description:]
@ -43,8 +46,8 @@ NEB is a method for finding both the atomic configurations and height
of the energy barrier associated with a transition state, e.g. for an
atom to perform a diffusive hop from one energy basin to another in a
coordinated fashion with its neighbors. The implementation in LAMMPS
follows the discussion in these 3 papers: "(HenkelmanA)"_#HenkelmanA,
"(HenkelmanB)"_#HenkelmanB, and "(Nakano)"_#Nakano3.
follows the discussion in these 4 papers: "(HenkelmanA)"_#HenkelmanA,
"(HenkelmanB)"_#HenkelmanB, "(Nakano)"_#Nakano3 and "(Maras)"_#Maras2.
Each replica runs on a partition of one or more processors. Processor
partitions are defined at run-time using the -partition command-line
@ -70,18 +73,17 @@ I.e. the simulation domain, the number of atoms, the interaction
potentials, and the starting configuration when the neb command is
issued should be the same for every replica.
In a NEB calculation each atom in a replica is connected to the same
atom in adjacent replicas by springs, which induce inter-replica
forces. These forces are imposed by the "fix neb"_fix_neb.html
command, which must be used in conjunction with the neb command. The
group used to define the fix neb command defines the NEB atoms which
are the only ones that inter-replica springs are applied to. If the
group does not include all atoms, then non-NEB atoms have no
inter-replica springs and the forces they feel and their motion is
computed in the usual way due only to other atoms within their
replica. Conceptually, the non-NEB atoms provide a background force
field for the NEB atoms. They can be allowed to move during the NEB
minimization procedure (which will typically induce different
In a NEB calculation each replica is connected to other replicas by
inter-replica nudging forces. These forces are imposed by the "fix
neb"_fix_neb.html command, which must be used in conjunction with the
neb command. The group used to define the fix neb command defines the
NEB atoms which are the only ones that inter-replica springs are
applied to. If the group does not include all atoms, then non-NEB
atoms have no inter-replica springs and the forces they feel and their
motion is computed in the usual way due only to other atoms within
their replica. Conceptually, the non-NEB atoms provide a background
force field for the NEB atoms. They can be allowed to move during the
NEB minimization procedure (which will typically induce different
coordinates for non-NEB atoms in different replicas), or held fixed
using other LAMMPS commands such as "fix setforce"_fix_setforce.html.
Note that the "partition"_partition.html command can be used to invoke
@ -93,33 +95,18 @@ specified in different manners via the {file-style} setting, as
discussed below. Only atoms whose initial coordinates should differ
from the current configuration need be specified.
Conceptually, the initial configuration for the first replica should
be a state with all the atoms (NEB and non-NEB) having coordinates on
one side of the energy barrier. A perfect energy minimum is not
required, since atoms in the first replica experience no spring forces
from the 2nd replica. Thus the damped dynamics minimization will
drive the first replica to an energy minimum if it is not already
there. However, you will typically get better convergence if the
initial state is already at a minimum. For example, for a system with
a free surface, the surface should be fully relaxed before attempting
a NEB calculation.
Likewise, the initial configuration of the final replica should be a
state with all the atoms (NEB and non-NEB) on the other side of the
energy barrier. Again, a perfect energy minimum is not required,
since the atoms in the last replica also experience no spring forces
from the next-to-last replica, and thus the damped dynamics
minimization will drive it to an energy minimum.
Conceptually, the initial and final configurations for the first
replica should be states on either side of an energy barrier.
As explained below, the initial configurations of intermediate
replicas can be atomic coordinates interpolated in a linear fashion
between the first and last replicas. This is often adequate state for
between the first and last replicas. This is often adequate for
simple transitions. For more complex transitions, it may lead to slow
convergence or even bad results if the minimum energy path (MEP, see
below) of states over the barrier cannot be correctly converged to
from such an initial configuration. In this case, you will want to
generate initial states for the intermediate replicas that are
geometrically closer to the MEP and read them in.
from such an initial path. In this case, you will want to generate
initial states for the intermediate replicas that are geometrically
closer to the MEP and read them in.
:line
@ -135,10 +122,11 @@ is assigned to be a fraction of the distance. E.g. if there are 10
replicas, the 2nd replica will assign a position that is 10% of the
distance along a line between the starting and final point, and the
9th replica will assign a position that is 90% of the distance along
the line. Note that this procedure to produce consistent coordinates
across all the replicas, the current coordinates need to be the same
in all replicas. LAMMPS does not check for this, but invalid initial
configurations will likely result if it is not the case.
the line. Note that for this procedure to produce consistent
coordinates across all the replicas, the current coordinates need to
be the same in all replicas. LAMMPS does not check for this, but
invalid initial configurations will likely result if it is not the
case.
NOTE: The "distance" between the starting and final point is
calculated in a minimum-image sense for a periodic simulation box.
@ -150,8 +138,8 @@ interpolation is outside the periodic box, the atom will be wrapped
back into the box when the NEB calculation begins.
For a {file-style} setting of {each}, a filename is specified which is
assumed to be unique to each replica. This can be done by
using a variable in the filename, e.g.
assumed to be unique to each replica. This can be done by using a
variable in the filename, e.g.
variable i equal part
neb 0.0 0.001 1000 500 50 each coords.initial.$i :pre
@ -198,11 +186,10 @@ The minimizer tolerances for energy and force are set by {etol} and
A non-zero {etol} means that the NEB calculation will terminate if the
energy criterion is met by every replica. The energies being compared
to {etol} do not include any contribution from the inter-replica
forces, since these are non-conservative. A non-zero {ftol} means
that the NEB calculation will terminate if the force criterion is met
by every replica. The forces being compared to {ftol} include the
inter-replica forces between an atom and its images in adjacent
replicas.
nudging forces, since these are non-conservative. A non-zero {ftol}
means that the NEB calculation will terminate if the force criterion
is met by every replica. The forces being compared to {ftol} include
the inter-replica nudging forces.
The maximum number of iterations in each stage is set by {N1} and
{N2}. These are effectively timestep counts since each iteration of
@ -220,27 +207,27 @@ finding a good energy barrier. {N1} and {N2} must both be multiples
of {Nevery}.
In the first stage of NEB, the set of replicas should converge toward
the minimum energy path (MEP) of conformational states that transition
over the barrier. The MEP for a barrier is defined as a sequence of
3N-dimensional states that cross the barrier at its saddle point, each
of which has a potential energy gradient parallel to the MEP itself.
The replica states will also be roughly equally spaced along the MEP
due to the inter-replica spring force added by the "fix
neb"_fix_neb.html command.
a minimum energy path (MEP) of conformational states that transition
over a barrier. The MEP for a transition is defined as a sequence of
3N-dimensional states, each of which has a potential energy gradient
parallel to the MEP itself. The configuration of highest energy along
a MEP corresponds to a saddle point. The replica states will also be
roughly equally spaced along the MEP due to the inter-replica nugding
force added by the "fix neb"_fix_neb.html command.
In the second stage of NEB, the replica with the highest energy
is selected and the inter-replica forces on it are converted to a
force that drives its atom coordinates to the top or saddle point of
the barrier, via the barrier-climbing calculation described in
In the second stage of NEB, the replica with the highest energy is
selected and the inter-replica forces on it are converted to a force
that drives its atom coordinates to the top or saddle point of the
barrier, via the barrier-climbing calculation described in
"(HenkelmanB)"_#HenkelmanB. As before, the other replicas rearrange
themselves along the MEP so as to be roughly equally spaced.
When both stages are complete, if the NEB calculation was successful,
one of the replicas should be an atomic configuration at the top or
saddle point of the barrier, the potential energies for the set of
replicas should represent the energy profile of the barrier along the
MEP, and the configurations of the replicas should be a sequence of
configurations along the MEP.
the configurations of the replicas should be along (close to) the MEP
and the replica with the highest energy should be an atomic
configuration at (close to) the saddle point of the transition. The
potential energies for the set of replicas represents the energy
profile of the transition along the MEP.
:line
@ -284,9 +271,9 @@ ID2 x2 y2 z2
...
IDN xN yN zN :pre
The fields are the atom ID, followed by the x,y,z coordinates.
The lines can be listed in any order. Additional trailing information
on the line is OK, such as a comment.
The fields are the atom ID, followed by the x,y,z coordinates. The
lines can be listed in any order. Additional trailing information on
the line is OK, such as a comment.
Note that for a typical NEB calculation you do not need to specify
initial coordinates for very many atoms to produce differing starting
@ -310,38 +297,54 @@ this case), the print-out to the screen and master log.lammps file
contains a line of output, printed once every {Nevery} timesteps. It
contains the timestep, the maximum force per replica, the maximum
force per atom (in any replica), potential gradients in the initial,
final, and climbing replicas, the forward and backward energy barriers,
the total reaction coordinate (RDT), and the normalized reaction
coordinate and potential energy of each replica.
final, and climbing replicas, the forward and backward energy
barriers, the total reaction coordinate (RDT), and the normalized
reaction coordinate and potential energy of each replica.
The "maximum force per replica" is
the two-norm of the 3N-length force vector for the atoms in each
replica, maximized across replicas, which is what the {ftol} setting
is checking against. In this case, N is all the atoms in each
replica. The "maximum force per atom" is the maximum force component
of any atom in any replica. The potential gradients are the two-norm
of the 3N-length force vector solely due to the interaction potential i.e.
without adding in inter-replica forces. Note that inter-replica forces
are zero in the initial and final replicas, and only affect
the direction in the climbing replica. For this reason, the "maximum
force per replica" is often equal to the potential gradient in the
climbing replica. In the first stage of NEB, there is no climbing
replica, and so the potential gradient in the highest energy replica
is reported, since this replica will become the climbing replica
in the second stage of NEB.
The "maximum force per replica" is the two-norm of the 3N-length force
vector for the atoms in each replica, maximized across replicas, which
is what the {ftol} setting is checking against. In this case, N is
all the atoms in each replica. The "maximum force per atom" is the
maximum force component of any atom in any replica. The potential
gradients are the two-norm of the 3N-length force vector solely due to
the interaction potential i.e. without adding in inter-replica
forces.
The "reaction coordinate" (RD) for each
replica is the two-norm of the 3N-length vector of distances between
its atoms and the preceding replica's atoms, added to the RD of the
preceding replica. The RD of the first replica RD1 = 0.0;
the RD of the final replica RDN = RDT, the total reaction coordinate.
The normalized RDs are divided by RDT,
so that they form a monotonically increasing sequence
from zero to one. When computing RD, N only includes the atoms
being operated on by the fix neb command.
The "reaction coordinate" (RD) for each replica is the two-norm of the
3N-length vector of distances between its atoms and the preceding
replica's atoms, added to the RD of the preceding replica. The RD of
the first replica RD1 = 0.0; the RD of the final replica RDN = RDT,
the total reaction coordinate. The normalized RDs are divided by RDT,
so that they form a monotonically increasing sequence from zero to
one. When computing RD, N only includes the atoms being operated on by
the fix neb command.
The forward (reverse) energy barrier is the potential energy of the highest
replica minus the energy of the first (last) replica.
The forward (reverse) energy barrier is the potential energy of the
highest replica minus the energy of the first (last) replica.
Supplementary informations for all replicas can be printed out to the
screen and master log.lammps file by adding the verbose keyword. These
informations include the following. The "path angle" (pathangle) for
the replica i which is the angle between the 3N-length vectors (Ri-1 -
Ri) and (Ri+1 - Ri) (where Ri is the atomic coordinates of replica
i). A "path angle" of 180 indicates that replicas i-1, i and i+1 are
aligned. "angletangrad" is the angle between the 3N-length tangent
vector and the 3N-length force vector at image i. The tangent vector
is calculated as in "(HenkelmanA)"_#HenkelmanA for all intermediate
replicas and at R2 - R1 and RM - RM-1 for the first and last replica,
respectively. "anglegrad" is the angle between the 3N-length energy
gradient vector of replica i and that of replica i+1. It is not
defined for the final replica and reads nan. gradV is the norm of the
energy gradient of image i. ReplicaForce is the two-norm of the
3N-length force vector (including nudging forces) for replica i.
MaxAtomForce is the maximum force component of any atom in replica i.
When a NEB calculation does not converge properly, these suplementary
informations can help understanding what is going wrong. For instance
when the path angle becomes accute the definition of tangent used in
the NEB calculation is questionable and the NEB cannot may diverge
"(Maras)"_#Maras2.
When running on multiple partitions, LAMMPS produces additional log
files for each partition, e.g. log.lammps.0, log.lammps.1, etc. For a
@ -396,12 +399,16 @@ This command can only be used if LAMMPS was built with the REPLICA
package. See the "Making LAMMPS"_Section_start.html#start_3 section
for more info on packages.
:line
[Related commands:]
"prd"_prd.html, "temper"_temper.html, "fix
langevin"_fix_langevin.html, "fix viscous"_fix_viscous.html
"prd"_prd.html, "temper"_temper.html, "fix langevin"_fix_langevin.html,
"fix viscous"_fix_viscous.html
[Default:] none
[Default:]
none
:line
@ -414,3 +421,7 @@ langevin"_fix_langevin.html, "fix viscous"_fix_viscous.html
:link(Nakano3)
[(Nakano)] Nakano, Comp Phys Comm, 178, 280-289 (2008).
:link(Maras2)
[(Maras)] Maras, Trushin, Stukowski, Ala-Nissila, Jonsson,
Comp Phys Comm, 205, 13-21 (2016)

View File

@ -574,9 +574,9 @@ is used. If it is not used, you must invoke the package intel
command in your input script or or via the "-pk intel" "command-line
switch"_Section_start.html#start_7.
For the KOKKOS package, the option defaults neigh = full, neigh/qeq
= full, newton = off, binsize = 0.0, and comm = device. These settings
are made automatically by the required "-k on" "command-line
For the KOKKOS package, the option defaults neigh = full,
neigh/qeq = full, newton = off, binsize = 0.0, and comm = device.
These settings are made automatically by the required "-k on" "command-line
switch"_Section_start.html#start_7. You can change them bu using the
package kokkos command in your input script or via the "-pk kokkos"
"command-line switch"_Section_start.html#start_7.

View File

@ -7,6 +7,7 @@
:line
pair_style lj/long/coul/long command :h3
pair_style lj/long/coul/long/intel command :h3
pair_style lj/long/coul/long/omp command :h3
pair_style lj/long/coul/long/opt command :h3
pair_style lj/long/tip4p/long command :h3

View File

@ -1,114 +0,0 @@
"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
pair_style lj/sf command :h3
pair_style lj/sf/omp command :h3
[Syntax:]
pair_style lj/sf cutoff :pre
cutoff = global cutoff for Lennard-Jones interactions (distance units) :ul
[Examples:]
pair_style lj/sf 2.5
pair_coeff * * 1.0 1.0
pair_coeff 1 1 1.0 1.0 3.0 :pre
[Description:]
Style {lj/sf} computes a truncated and force-shifted LJ interaction
(Shifted Force Lennard-Jones), so that both the potential and the
force go continuously to zero at the cutoff "(Toxvaerd)"_#Toxvaerd:
:c,image(Eqs/pair_lj_sf.jpg)
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, or by mixing as described below:
epsilon (energy units)
sigma (distance units)
cutoff (distance units) :ul
The last coefficient is optional. If not specified, the global
LJ cutoff specified in the pair_style command is used.
:line
Styles with a {gpu}, {intel}, {kk}, {omp}, or {opt} suffix are
functionally the same as the corresponding style without the suffix.
They have been optimized to run faster, depending on your available
hardware, as discussed in "Section 5"_Section_accelerate.html
of the manual. The accelerated styles take the same arguments and
should produce the same results, except for round-off and precision
issues.
These accelerated styles are part of the GPU, USER-INTEL, KOKKOS,
USER-OMP and OPT packages, respectively. They are only enabled if
LAMMPS was built with those packages. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info.
You can specify the accelerated styles explicitly in your input script
by including their suffix, or you can use the "-suffix command-line
switch"_Section_start.html#start_7 when you invoke LAMMPS, or you can
use the "suffix"_suffix.html command in your input script.
See "Section 5"_Section_accelerate.html of the manual for
more instructions on how to use the accelerated styles effectively.
:line
[Mixing, shift, table, tail correction, restart, rRESPA info]:
For atom type pairs I,J and I != J, the epsilon and sigma
coefficients and cutoff distance for this pair style can be mixed.
Rin is a cutoff value and is mixed like the cutoff. The
default mix value is {geometric}. See the "pair_modify" command for
details.
The "pair_modify"_pair_modify.html shift option is not relevant for
this pair style, since the pair interaction goes to 0.0 at the cutoff.
The "pair_modify"_pair_modify.html table option is not relevant
for this pair style.
This pair style does not support the "pair_modify"_pair_modify.html
tail option for adding long-range tail corrections to energy and
pressure, since the energy of the pair interaction is smoothed to 0.0
at the cutoff.
This pair style writes its information to "binary restart
files"_restart.html, so pair_style and pair_coeff commands do not need
to be specified in an input script that reads a restart file.
This pair style can only be used via the {pair} keyword of the
"run_style respa"_run_style.html command. It does not support the
{inner}, {middle}, {outer} keywords.
:line
[Restrictions:]
This pair style is part of the USER-MISC 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:]
"pair_coeff"_pair_coeff.html
[Default:] none
:line
:link(Toxvaerd)
[(Toxvaerd)] Toxvaerd, Dyre, J Chem Phys, 134, 081102 (2011).

View File

@ -11,26 +11,26 @@ pair_style lj/smooth/linear/omp command :h3
[Syntax:]
pair_style lj/smooth/linear Rc :pre
pair_style lj/smooth/linear cutoff :pre
Rc = cutoff for lj/smooth/linear interactions (distance units) :ul
cutoff = global cutoff for Lennard-Jones interactions (distance units) :ul
[Examples:]
pair_style lj/smooth/linear 5.456108274435118
pair_coeff * * 0.7242785984051078 2.598146797350056
pair_coeff 1 1 20.0 1.3 9.0 :pre
pair_style lj/smooth/linear 2.5
pair_coeff * * 1.0 1.0
pair_coeff 1 1 0.3 3.0 9.0 :pre
[Description:]
Style {lj/smooth/linear} computes a LJ interaction that combines the
standard 12/6 Lennard-Jones function and subtracts a linear term that
includes the cutoff distance Rc, as in this formula:
Style {lj/smooth/linear} computes a truncated and force-shifted LJ
interaction (aka Shifted Force Lennard-Jones) that combines the
standard 12/6 Lennard-Jones function and subtracts a linear term based
on the cutoff distance, so that both, the potential and the force, go
continuously to zero at the cutoff Rc "(Toxvaerd)"_#Toxvaerd:
:c,image(Eqs/pair_lj_smooth_linear.jpg)
At the cutoff Rc, the energy and force (its 1st derivative) will be 0.0.
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
@ -41,8 +41,8 @@ epsilon (energy units)
sigma (distance units)
cutoff (distance units) :ul
The last coefficient is optional. If not specified, the global value
for Rc is used.
The last coefficient is optional. If not specified, the global
LJ cutoff specified in the pair_style command is used.
:line
@ -76,10 +76,11 @@ and cutoff distance can be mixed. The default mix value is geometric.
See the "pair_modify" command for details.
This pair style does not support the "pair_modify"_pair_modify.html
shift option for the energy of the pair interaction.
shift option for the energy of the pair interaction, since it goes
to 0.0 at the cutoff by construction.
The "pair_modify"_pair_modify.html table option is not relevant for
this pair style.
The "pair_modify"_pair_modify.html table option is not relevant
for this pair style.
This pair style does not support the "pair_modify"_pair_modify.html
tail option for adding long-range tail corrections to energy and
@ -103,3 +104,8 @@ This pair style can only be used via the {pair} keyword of the
"pair_coeff"_pair_coeff.html, "pair lj/smooth"_pair_lj_smooth.html
[Default:] none
:line
:link(Toxvaerd)
[(Toxvaerd)] Toxvaerd, Dyre, J Chem Phys, 134, 081102 (2011).

View File

@ -26,7 +26,7 @@ args = list of arguments for a particular style :ul
{morse/smooth/linear} args = cutoff
cutoff = global cutoff for Morse interactions (distance units)
{morse/soft} args = n lf cutoff
n = soft-core parameter
n = soft-core parameter
lf = transformation range is lf < lambda < 1
cutoff = global cutoff for Morse interactions (distance units)
:pre
@ -36,7 +36,7 @@ args = list of arguments for a particular style :ul
pair_style morse 2.5
pair_style morse/smooth/linear 2.5
pair_coeff * * 100.0 2.0 1.5
pair_coeff 1 1 100.0 2.0 1.5 3.0
pair_coeff 1 1 100.0 2.0 1.5 3.0 :pre
pair_style morse/soft 4 0.9 10.0
pair_coeff * * 100.0 2.0 1.5 1.0

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@ -74,7 +74,7 @@ placeholders for atom types that will be used with other potentials.
The python potential file has to start with the following code:
from __future__ import print_function
#
class LAMMPSPairPotential(object):
def __init__(self):
self.pmap=dict()
@ -163,9 +163,10 @@ pair_write 1 1 2000 rsq 0.01 2.5 lj1_lj2.table lj :pre
Note that it is strongly recommended to try to [delete] the potential
table file before generating it. Since the {pair_write} command will
always append to a table file, which pair style table will use the
first match. Thus when changing the potential function in the python
class, the table pair style will still read the old variant.
always [append] to a table file, while pair style table will use the
[first match]. Thus when changing the potential function in the python
class, the table pair style will still read the old variant unless the
table file is first deleted.
After switching the pair style to {table}, the potential tables need
to be assigned to the LAMMPS atom types like this:

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@ -8,6 +8,7 @@
pair_style reax/c command :h3
pair_style reax/c/kk command :h3
pair_style reax/c/omp command :h3
[Syntax:]

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@ -10,7 +10,8 @@ pair_style snap command :h3
[Syntax:]
pair_style snap :pre
pair_style snap
:pre
[Examples:]
@ -19,11 +20,11 @@ pair_coeff * * InP.snapcoeff In P InP.snapparam In In P P :pre
[Description:]
Style {snap} computes interactions
Pair style {snap} computes interactions
using the spectral neighbor analysis potential (SNAP)
"(Thompson)"_#Thompson20142. Like the GAP framework of Bartok et al.
"(Bartok2010)"_#Bartok20102, "(Bartok2013)"_#Bartok2013
it uses bispectrum components
which uses bispectrum components
to characterize the local neighborhood of each atom
in a very general way. The mathematical definition of the
bispectrum calculation used by SNAP is identical
@ -139,10 +140,15 @@ The default values for these keywords are
{rmin0} = 0.0
{diagonalstyle} = 3
{switchflag} = 0
{bzeroflag} = 1 :ul
{bzeroflag} = 1
{quadraticflag} = 1 :ul
Detailed definitions of these keywords are given on the "compute
Detailed definitions for all the keywords are given on the "compute
sna/atom"_compute_sna_atom.html doc page.
If {quadraticflag} is set to 1, then the SNAP energy expression includes the quadratic term,
0.5*B^t.alpha.B, where alpha is a symmetric {K} by {K} matrix.
The SNAP element file should contain {K}({K}+1)/2 additional coefficients
for each element, the upper-triangular elements of alpha.
:line

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@ -7,6 +7,7 @@
:line
pair_style vashishta command :h3
pair_style vashishta/gpu command :h3
pair_style vashishta/omp command :h3
pair_style vashishta/kk command :h3
pair_style vashishta/table command :h3

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@ -14,7 +14,7 @@ pair_style zero cutoff {nocoeff} :pre
zero = style name of this pair style
cutoff = global cutoff (distance units)
nocoeff = ignore all pair_coeff parameters (optional) :l
nocoeff = ignore all pair_coeff parameters (optional) :ul
[Examples:]

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@ -49,7 +49,6 @@ Pair Styles :h1
pair_lj_cubic
pair_lj_expand
pair_lj_long
pair_lj_sf
pair_lj_smooth
pair_lj_smooth_linear
pair_lj_soft

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@ -80,6 +80,7 @@ keyword = {type} or {type/fraction} or {mol} or {x} or {y} or {z} or \
value can be an atom-style variable (see below)
{image} nx ny nz
nx,ny,nz = which periodic image of the simulation box the atom is in
any of nx,ny,nz can be an atom-style variable (see below)
{bond} value = bond type for all bonds between selected atoms
{angle} value = angle type for all angles between selected atoms
{dihedral} value = dihedral type for all dihedrals between selected atoms
@ -363,9 +364,8 @@ A value of -1 means subtract 1 box length to get the true value.
LAMMPS updates these flags as atoms cross periodic boundaries during
the simulation. The flags can be output with atom snapshots via the
"dump"_dump.html command. If a value of NULL is specified for any of
nx,ny,nz, then the current image value for that dimension is
unchanged. For non-periodic dimensions only a value of 0 can be
specified. This keyword does not allow use of atom-style variables.
nx,ny,nz, then the current image value for that dimension is unchanged.
For non-periodic dimensions only a value of 0 can be specified.
This command can be useful after a system has been equilibrated and
atoms have diffused one or more box lengths in various directions.
This command can then reset the image values for atoms so that they

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@ -65,7 +65,13 @@ sense to define permanent bonds between atoms that interact via these
potentials, though such bonds may exist elsewhere in your system,
e.g. when using the "pair_style hybrid"_pair_hybrid.html command.
Thus LAMMPS ignores special_bonds settings when manybody potentials
are calculated.
are calculated. Please note, that the existence of explicit bonds
for atoms that are described by a manybody potential will alter the
neigborlist and thus can render the computation of those interactions
invalid, since those pairs are not only used to determine direct
pairwise interactions but also neighbors of neighbors and more.
The recommended course of action is to remove such bonds, or - if
that is not possible - use a special bonds setting of 1.0 1.0 1.0.
NOTE: Unlike some commands in LAMMPS, you cannot use this command
multiple times in an incremental fashion: e.g. to first set the LJ

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@ -10,6 +10,7 @@ PyLammps Tutorial :h1
<!-- RST
.. contents::
END_RST -->
Overview :h2

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@ -153,7 +153,7 @@ int main(int narg, char **arg)
for (int i = 0; i < natoms; i++) type[i] = 1;
lmp->input->one("delete_atoms group all");
lammps_create_atoms(lmp,natoms,NULL,type,x,v);
lammps_create_atoms(lmp,natoms,NULL,type,x,v,NULL,0);
lmp->input->one("run 10");
}

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@ -14,7 +14,7 @@
------------------------------------------------------------------------- */
/* ----------------------------------------------------------------------
Contributing author: Oliver Henrich (EPCC, University of Edinburgh)
Contributing author: Oliver Henrich (University of Strathclyde, Glasgow)
------------------------------------------------------------------------- */
"""

File diff suppressed because it is too large Load Diff

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@ -0,0 +1,51 @@
# Generation and relaxation of a partial dislocation in Cu perfect FCC crystal
# Initialization
units metal
boundary p p p
atom_style atomic
# create simulation box and system
lattice fcc 3.615 origin 0.01 0.01 0.01 orient x -1 -1 2 orient y 1 1 1 orient z -1 1 0
region mdbox block 0 3 0.0 14.0 0 84 units lattice
region system block 0 3 1.1 13.1 0 84 units lattice
create_box 2 mdbox
create_atoms 1 region system
# Define atoms mass and force field
mass * 63.54
pair_style eam/alloy
pair_coeff * * Cu_Mishin1.eam Cu Cu
# Delete a plane of atoms along the z direction to generate a partial dislocation
region dislocation_atoms block 0 3 7 14 41.9 42.1 units lattice
delete_atoms region dislocation_atoms
region quarter_up block 0 3 7 11 0 84 units lattice
group middle region quarter_up
# specify simulation parameters
timestep 0.004
# Relax configuration using conjugate gradient
#min_style cg
#minimize 1.0e-4 1.0e-6 100 1000
# Setup calculations
compute 1 all cnp/atom 3.086
compute 2 all cna/atom 3.086
compute 3 all centro/atom fcc
compute 4 all coord/atom cutoff 3.086
dump 1 all custom 100 dump.lammpstrj id type xu yu zu c_1 c_2 c_3 c_4
### Set up thermo display
thermo 10
thermo_style custom step atoms temp press pe ke etotal
# Relax the system performing a langevin dynamics (freeze motion along y 111 direction)
fix 1 all nve
fix 2 all langevin 50 1 0.1 699483
fix 3 all setforce NULL 0.0 NULL
fix 4 middle setforce 0.0 0.0 0.0
run 100
unfix 4
run 200

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@ -0,0 +1,185 @@
LAMMPS (19 May 2017)
OMP_NUM_THREADS environment is not set. Defaulting to 1 thread. (../comm.cpp:90)
using 1 OpenMP thread(s) per MPI task
# Generation and relaxation of a partial dislocation in Cu perfect FCC crystal
# Initialization
units metal
boundary p p p
atom_style atomic
# create simulation box and system
lattice fcc 3.615 origin 0.01 0.01 0.01 orient x -1 -1 2 orient y 1 1 1 orient z -1 1 0
Lattice spacing in x,y,z = 5.90327 6.26136 5.11238
region mdbox block 0 3 0.0 14.0 0 84 units lattice
region system block 0 3 1.1 13.1 0 84 units lattice
create_box 2 mdbox
Created orthogonal box = (0 0 0) to (17.7098 87.6591 429.44)
1 by 1 by 4 MPI processor grid
create_atoms 1 region system
Created 48384 atoms
# Define atoms mass and force field
mass * 63.54
pair_style eam/alloy
pair_coeff * * Cu_Mishin1.eam Cu Cu
# Delete a plane of atoms along the z direction to generate a partial dislocation
region dislocation_atoms block 0 3 7 14 41.9 42.1 units lattice
delete_atoms region dislocation_atoms
Deleted 76 atoms, new total = 48308
region quarter_up block 0 3 7 11 0 84 units lattice
group middle region quarter_up
16080 atoms in group middle
# specify simulation parameters
timestep 0.004
# Relax configuration using conjugate gradient
#min_style cg
#minimize 1.0e-4 1.0e-6 100 1000
# Setup calculations
compute 1 all cnp/atom 3.086
compute 2 all cna/atom 3.086
compute 3 all centro/atom fcc
compute 4 all coord/atom cutoff 3.086
dump 1 all custom 100 dump.lammpstrj id type xu yu zu c_1 c_2 c_3 c_4
### Set up thermo display
thermo 10
thermo_style custom step atoms temp press pe ke etotal
# Relax the system performing a langevin dynamics (freeze motion along y 111 direction)
fix 1 all nve
fix 2 all langevin 50 1 0.1 699483
fix 3 all setforce NULL 0.0 NULL
fix 4 middle setforce 0.0 0.0 0.0
run 100
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 7.50679
ghost atom cutoff = 7.50679
binsize = 3.75339, bins = 5 24 115
5 neighbor lists, perpetual/occasional/extra = 1 4 0
(1) pair eam/alloy, perpetual
attributes: half, newton on
pair build: half/bin/atomonly/newton
stencil: half/bin/3d/newton
bin: standard
(2) compute cnp/atom, occasional
attributes: full, newton on
pair build: full/bin/atomonly
stencil: full/bin/3d
bin: standard
(3) compute cna/atom, occasional
attributes: full, newton on
pair build: full/bin/atomonly
stencil: full/bin/3d
bin: standard
(4) compute centro/atom, occasional
attributes: full, newton on
pair build: full/bin/atomonly
stencil: full/bin/3d
bin: standard
(5) compute coord/atom, occasional
attributes: full, newton on
pair build: full/bin/atomonly
stencil: full/bin/3d
bin: standard
Per MPI rank memory allocation (min/avg/max) = 45.41 | 45.41 | 45.41 Mbytes
Step Atoms Temp Press PotEng KinEng TotEng
0 48308 0 -3388.0911 -169746.07 0 -169746.07
10 48308 7.35092 -3091.0864 -169715.96 45.900393 -169670.05
20 48308 9.9162268 -2822.7045 -169678.51 61.918604 -169616.59
30 48308 12.351316 -2726.7195 -169666.35 77.123716 -169589.23
40 48308 13.302856 -2703.586 -169662.9 83.06529 -169579.83
50 48308 12.782228 -2706.8662 -169662.36 79.814401 -169582.55
60 48308 12.198179 -2772.4206 -169670.02 76.167503 -169593.86
70 48308 10.663322 -2841.3384 -169677.48 66.583595 -169610.9
80 48308 9.1169804 -2932.3896 -169687.85 56.927974 -169630.92
90 48308 7.2905076 -3029.9433 -169699.09 45.523167 -169653.56
100 48308 5.4063635 -3139.4496 -169711.65 33.758252 -169677.89
Loop time of 10.9003 on 4 procs for 100 steps with 48308 atoms
Performance: 3.171 ns/day, 7.570 hours/ns, 9.174 timesteps/s
31.8% CPU use with 4 MPI tasks x 1 OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 9.8764 | 9.9587 | 10.021 | 1.6 | 91.36
Neigh | 0 | 0 | 0 | 0.0 | 0.00
Comm | 0.1232 | 0.18385 | 0.26683 | 12.1 | 1.69
Output | 0.45385 | 0.45451 | 0.45634 | 0.2 | 4.17
Modify | 0.25026 | 0.2537 | 0.25744 | 0.5 | 2.33
Other | | 0.04949 | | | 0.45
Nlocal: 12077 ave 12096 max 12020 min
Histogram: 1 0 0 0 0 0 0 0 0 3
Nghost: 14204 ave 14261 max 14109 min
Histogram: 1 0 0 0 0 1 0 0 0 2
Neighs: 814050 ave 818584 max 809212 min
Histogram: 1 0 0 0 0 2 0 0 0 1
FullNghs: 1.6281e+06 ave 1.63296e+06 max 1.61808e+06 min
Histogram: 1 0 0 0 0 0 1 0 0 2
Total # of neighbors = 6512400
Ave neighs/atom = 134.81
Neighbor list builds = 0
Dangerous builds = 0
unfix 4
run 200
Per MPI rank memory allocation (min/avg/max) = 45.41 | 45.41 | 45.41 Mbytes
Step Atoms Temp Press PotEng KinEng TotEng
100 48308 5.4063635 -3139.4496 -169711.65 33.758252 -169677.89
110 48308 15.260795 -2793.119 -169677.24 95.290993 -169581.95
120 48308 18.548656 -2433.1584 -169624.79 115.82096 -169508.97
130 48308 22.15831 -2276.626 -169604.28 138.36025 -169465.92
140 48308 24.393841 -2208.1771 -169596.16 152.31929 -169443.84
150 48308 24.797558 -2173.3145 -169591.43 154.84016 -169436.59
160 48308 24.73371 -2188.909 -169593.08 154.44148 -169438.64
170 48308 24.128467 -2220.3404 -169596.96 150.66225 -169446.29
180 48308 22.975708 -2275.1244 -169602.72 143.46422 -169459.26
190 48308 21.936324 -2348.3762 -169610.59 136.97413 -169473.61
200 48308 20.516249 -2432.8447 -169619.98 128.10694 -169491.87
210 48308 19.000566 -2510.2915 -169628.58 118.64276 -169509.93
220 48308 17.490407 -2597.299 -169638.24 109.21307 -169529.03
230 48308 16.062482 -2684.1203 -169648.31 100.29687 -169548.01
240 48308 14.360342 -2768.2313 -169657.7 89.668411 -169568.03
250 48308 12.802315 -2852.6965 -169666.99 79.939831 -169587.05
260 48308 11.258205 -2944.4533 -169677.52 70.298142 -169607.23
270 48308 9.6159129 -3038.6304 -169688.06 60.043393 -169628.02
280 48308 7.972425 -3129.0826 -169698.03 49.781176 -169648.25
290 48308 6.3752377 -3219.2054 -169708.23 39.808067 -169668.42
300 48308 4.7374688 -3306.1468 -169718.27 29.58156 -169688.69
Loop time of 23.0164 on 4 procs for 200 steps with 48308 atoms
Performance: 3.003 ns/day, 7.992 hours/ns, 8.689 timesteps/s
31.8% CPU use with 4 MPI tasks x 1 OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 20.221 | 20.423 | 20.57 | 3.1 | 88.73
Neigh | 0 | 0 | 0 | 0.0 | 0.00
Comm | 0.27748 | 0.42603 | 0.62832 | 21.4 | 1.85
Output | 1.5454 | 1.5473 | 1.5529 | 0.3 | 6.72
Modify | 0.48886 | 0.49773 | 0.50842 | 1.1 | 2.16
Other | | 0.1221 | | | 0.53
Nlocal: 12077 ave 12096 max 12020 min
Histogram: 1 0 0 0 0 0 0 0 0 3
Nghost: 14204 ave 14261 max 14109 min
Histogram: 1 0 0 0 0 1 0 0 0 2
Neighs: 814094 ave 818584 max 809212 min
Histogram: 1 0 0 0 0 2 0 0 0 1
FullNghs: 1.62852e+06 ave 1.63296e+06 max 1.61892e+06 min
Histogram: 1 0 0 0 0 0 0 1 0 2
Total # of neighbors = 6514094
Ave neighs/atom = 134.845
Neighbor list builds = 0
Dangerous builds = 0
Total wall time: 0:00:35

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@ -18,14 +18,14 @@ read_data ${rep}/lj.data
#dump dump all xyz 1000 ${rep}/dump.xyz
thermo 10
thermo_style custom step temp pe etotal press vol
timestep 1.0
fix fxnpt all npt temp ${T0} ${T0} 1000.0 iso ${press} ${press} 10000.0
fix fxgREM all grem ${lambda} -.03 -30000 fxnpt
thermo_modify press fxgREM_press
temper/grem 10000 100 ${lambda} fxgREM fxnpt 10294 98392 #${walker}
thermo 10
thermo_style custom step temp f_fxgREM pe etotal press vol
thermo_modify press fxgREM_press
timestep 1.0
temper/grem 10000 100 ${lambda} fxgREM fxnpt 10294 98392 #${walker}
#write_data ${rep}/lj-out.data

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@ -0,0 +1,177 @@
LAMMPS (19 May 2017)
units real
atom_style full
read_data data.spce
orthogonal box = (0.02645 0.02645 0.02641) to (35.5328 35.5328 35.4736)
1 by 1 by 1 MPI processor grid
reading atoms ...
4500 atoms
scanning bonds ...
2 = max bonds/atom
scanning angles ...
1 = max angles/atom
reading bonds ...
3000 bonds
reading angles ...
1500 angles
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
1 = max # of 1-4 neighbors
2 = max # of special neighbors
pair_style lj/cut/coul/long 12.0 12.0
kspace_style pppm 1.0e-4
pair_coeff 1 1 0.15535 3.166
pair_coeff * 2 0.0000 0.0000
bond_style harmonic
angle_style harmonic
dihedral_style none
improper_style none
bond_coeff 1 1000.00 1.000
angle_coeff 1 100.0 109.47
special_bonds lj/coul 0.0 0.0 1.0
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
2 = max # of special neighbors
neighbor 2.0 bin
fix 1 all shake 0.0001 20 0 b 1 a 1
0 = # of size 2 clusters
0 = # of size 3 clusters
0 = # of size 4 clusters
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
# make certain that shake constraints are satisfied
run 0 post no
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 8000 3375
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
1 neighbor lists, perpetual/occasional/extra = 1 0 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
Per MPI rank memory allocation (min/avg/max) = 26.54 | 26.54 | 26.54 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0 -16692.358 0 -16692.358 -1289.8319
Loop time of 3e-06 on 1 procs for 0 steps with 4500 atoms
group one molecule 1 2
6 atoms in group one
# the following section shows equivalences between using the force/tally compute and other computes and thermo keywords
# compute pairwise force between two molecules and everybody
compute fpa one group/group all pair yes kspace no boundary no
# tally pairwise force between two molecules and the all molecules
compute c1 one force/tally all
# tally the force of all with all (should be zero)
compute c2 all force/tally all
# collect per atom data. only reduce over the first group.
compute one one reduce sum c_c1[1] c_c1[2] c_c1[3]
compute red all reduce sum c_c2[1] c_c2[2] c_c2[3]
# determine magnitude of force
variable fpa equal sqrt(c_fpa[1]*c_fpa[1]+c_fpa[2]*c_fpa[2]+c_fpa[3]*c_fpa[3])
variable for equal sqrt(c_one[1]*c_one[1]+c_one[2]*c_one[2]+c_one[3]*c_one[3])
# round to 10**-10 absolute precision.
variable ref equal round(1e10*sqrt(c_red[1]*c_red[1]+c_red[2]*c_red[2]+c_red[3]*c_red[3]))*1e-10
variable all equal round(1e10*c_c2)*1e-10
velocity all create 300 432567 dist uniform
timestep 2.0
# v_fpa and v_for and c_c1, c_fpa[] and c_one[] should all each have the same value. v_ref and c_c2 should be zero
thermo_style custom step v_fpa v_for c_c1 c_fpa[1] c_one[1] c_fpa[2] c_one[2] c_fpa[3] c_one[3] v_ref v_all
thermo 10
run 50
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 8000 3375
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:77)
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:77)
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
2 neighbor lists, perpetual/occasional/extra = 1 1 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
(2) compute group/group, occasional, copy from (1)
attributes: half, newton on
pair build: copy
stencil: none
bin: none
Per MPI rank memory allocation (min/avg/max) = 28.47 | 28.47 | 28.47 Mbytes
Step v_fpa v_for c_c1 c_fpa[1] c_one[1] c_fpa[2] c_one[2] c_fpa[3] c_one[3] v_ref v_all
0 22.7331 22.7331 22.7331 -17.068295 -17.068295 -8.8348335 -8.8348334 -12.141369 -12.141369 0 0
10 11.736901 11.736901 11.736901 -3.3897029 -3.3897029 9.1193856 9.1193856 -6.5651786 -6.5651786 0 0
20 5.6120339 5.6120339 5.6120339 -0.60046861 -0.60046861 -4.4481306 -4.4481306 3.3687528 3.3687528 0 0
30 17.29261 17.29261 17.29261 6.179302 6.179302 -10.593979 -10.593979 12.190906 12.190906 0 0
40 18.664433 18.664433 18.664433 5.4727782 5.4727782 -6.9329319 -6.9329319 16.442148 16.442148 0 0
50 12.130407 12.130407 12.130407 -1.0321196 -1.0321196 8.0035558 8.0035558 -9.0567428 -9.0567428 0 0
Loop time of 13.9507 on 1 procs for 50 steps with 4500 atoms
Performance: 0.619 ns/day, 38.752 hours/ns, 3.584 timesteps/s
32.0% CPU use with 1 MPI tasks x no OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 12.594 | 12.594 | 12.594 | 0.0 | 90.27
Bond | 7.3e-05 | 7.3e-05 | 7.3e-05 | 0.0 | 0.00
Kspace | 0.56296 | 0.56296 | 0.56296 | 0.0 | 4.04
Neigh | 0.65858 | 0.65858 | 0.65858 | 0.0 | 4.72
Comm | 0.019093 | 0.019093 | 0.019093 | 0.0 | 0.14
Output | 0.055025 | 0.055025 | 0.055025 | 0.0 | 0.39
Modify | 0.057276 | 0.057276 | 0.057276 | 0.0 | 0.41
Other | | 0.004003 | | | 0.03
Nlocal: 4500 ave 4500 max 4500 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Nghost: 21131 ave 21131 max 21131 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Neighs: 2.60198e+06 ave 2.60198e+06 max 2.60198e+06 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Total # of neighbors = 2601983
Ave neighs/atom = 578.218
Ave special neighs/atom = 2
Neighbor list builds = 4
Dangerous builds = 1
Total wall time: 0:00:15

View File

@ -0,0 +1,177 @@
LAMMPS (19 May 2017)
units real
atom_style full
read_data data.spce
orthogonal box = (0.02645 0.02645 0.02641) to (35.5328 35.5328 35.4736)
2 by 2 by 1 MPI processor grid
reading atoms ...
4500 atoms
scanning bonds ...
2 = max bonds/atom
scanning angles ...
1 = max angles/atom
reading bonds ...
3000 bonds
reading angles ...
1500 angles
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
1 = max # of 1-4 neighbors
2 = max # of special neighbors
pair_style lj/cut/coul/long 12.0 12.0
kspace_style pppm 1.0e-4
pair_coeff 1 1 0.15535 3.166
pair_coeff * 2 0.0000 0.0000
bond_style harmonic
angle_style harmonic
dihedral_style none
improper_style none
bond_coeff 1 1000.00 1.000
angle_coeff 1 100.0 109.47
special_bonds lj/coul 0.0 0.0 1.0
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
2 = max # of special neighbors
neighbor 2.0 bin
fix 1 all shake 0.0001 20 0 b 1 a 1
0 = # of size 2 clusters
0 = # of size 3 clusters
0 = # of size 4 clusters
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
# make certain that shake constraints are satisfied
run 0 post no
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 3380 960
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
1 neighbor lists, perpetual/occasional/extra = 1 0 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
Per MPI rank memory allocation (min/avg/max) = 10.6 | 10.61 | 10.61 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0 -16692.358 0 -16692.358 -1289.8319
Loop time of 4.5e-06 on 4 procs for 0 steps with 4500 atoms
group one molecule 1 2
6 atoms in group one
# the following section shows equivalences between using the force/tally compute and other computes and thermo keywords
# compute pairwise force between two molecules and everybody
compute fpa one group/group all pair yes kspace no boundary no
# tally pairwise force between two molecules and the all molecules
compute c1 one force/tally all
# tally the force of all with all (should be zero)
compute c2 all force/tally all
# collect per atom data. only reduce over the first group.
compute one one reduce sum c_c1[1] c_c1[2] c_c1[3]
compute red all reduce sum c_c2[1] c_c2[2] c_c2[3]
# determine magnitude of force
variable fpa equal sqrt(c_fpa[1]*c_fpa[1]+c_fpa[2]*c_fpa[2]+c_fpa[3]*c_fpa[3])
variable for equal sqrt(c_one[1]*c_one[1]+c_one[2]*c_one[2]+c_one[3]*c_one[3])
# round to 10**-10 absolute precision.
variable ref equal round(1e10*sqrt(c_red[1]*c_red[1]+c_red[2]*c_red[2]+c_red[3]*c_red[3]))*1e-10
variable all equal round(1e10*c_c2)*1e-10
velocity all create 300 432567 dist uniform
timestep 2.0
# v_fpa and v_for and c_c1, c_fpa[] and c_one[] should all each have the same value. v_ref and c_c2 should be zero
thermo_style custom step v_fpa v_for c_c1 c_fpa[1] c_one[1] c_fpa[2] c_one[2] c_fpa[3] c_one[3] v_ref v_all
thermo 10
run 50
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 3380 960
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:77)
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:77)
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
2 neighbor lists, perpetual/occasional/extra = 1 1 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
(2) compute group/group, occasional, copy from (1)
attributes: half, newton on
pair build: copy
stencil: none
bin: none
Per MPI rank memory allocation (min/avg/max) = 11.58 | 11.59 | 11.6 Mbytes
Step v_fpa v_for c_c1 c_fpa[1] c_one[1] c_fpa[2] c_one[2] c_fpa[3] c_one[3] v_ref v_all
0 22.7331 22.7331 22.7331 -17.068295 -17.068295 -8.8348335 -8.8348334 -12.141369 -12.141369 0 0
10 11.736901 11.736901 11.736901 -3.3897029 -3.3897029 9.1193856 9.1193856 -6.5651786 -6.5651786 0 0
20 5.6120339 5.6120339 5.6120339 -0.60046861 -0.60046861 -4.4481306 -4.4481306 3.3687528 3.3687528 0 0
30 17.29261 17.29261 17.29261 6.179302 6.179302 -10.593979 -10.593979 12.190906 12.190906 0 0
40 18.664433 18.664433 18.664433 5.4727782 5.4727782 -6.9329319 -6.9329319 16.442148 16.442148 0 0
50 12.130407 12.130407 12.130407 -1.0321196 -1.0321196 8.0035558 8.0035558 -9.0567428 -9.0567428 0 0
Loop time of 4.31614 on 4 procs for 50 steps with 4500 atoms
Performance: 2.002 ns/day, 11.989 hours/ns, 11.584 timesteps/s
31.6% CPU use with 4 MPI tasks x no OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 3.5075 | 3.6114 | 3.7489 | 4.7 | 83.67
Bond | 8.6e-05 | 0.00010525 | 0.000141 | 0.0 | 0.00
Kspace | 0.2581 | 0.39489 | 0.49723 | 14.2 | 9.15
Neigh | 0.19826 | 0.19888 | 0.19918 | 0.1 | 4.61
Comm | 0.034639 | 0.037137 | 0.038938 | 0.9 | 0.86
Output | 0.025465 | 0.025997 | 0.027558 | 0.6 | 0.60
Modify | 0.044022 | 0.044175 | 0.044407 | 0.1 | 1.02
Other | | 0.003593 | | | 0.08
Nlocal: 1125 ave 1148 max 1097 min
Histogram: 1 0 0 1 0 0 0 0 1 1
Nghost: 12212.5 ave 12269 max 12162 min
Histogram: 1 0 0 1 0 1 0 0 0 1
Neighs: 650496 ave 675112 max 631353 min
Histogram: 1 0 0 1 1 0 0 0 0 1
Total # of neighbors = 2601983
Ave neighs/atom = 578.218
Ave special neighs/atom = 2
Neighbor list builds = 4
Dangerous builds = 1
Total wall time: 0:00:04

View File

@ -1,5 +1,4 @@
LAMMPS (21 Aug 2015-ICMS)
using 1 OpenMP thread(s) per MPI task
LAMMPS (19 May 2017)
units real
atom_style full
@ -50,6 +49,35 @@ fix 1 all shake 0.0001 20 0 b 1 a 1
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
# make certain that shake constraints are satisfied
run 0 post no
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 8000 3375
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
1 neighbor lists, perpetual/occasional/extra = 1 0 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
Per MPI rank memory allocation (min/avg/max) = 26.54 | 26.54 | 26.54 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0 -16692.358 0 -16692.358 -1289.8319
Loop time of 1e-06 on 1 procs for 0 steps with 4500 atoms
group oxy type 1
1500 atoms in group oxy
group hyd type 2
@ -88,6 +116,7 @@ thermo 10
run 50
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
@ -95,38 +124,49 @@ PPPM initialization ...
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 8000 3375
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:75)
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:75)
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:77)
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:77)
Neighbor list info ...
2 neighbor list requests
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7 -> bins = 6 6 6
Memory usage per processor = 17.381 Mbytes
Step epa epa E_vdwl vdwl E_coul coul eref pe c2 pair
0 -516632.19 -516632.19 3169.9382 3169.9382 46213.889 46213.889 49383.827 49383.827 49383.827 49383.827
10 -517027.36 -517027.36 3099.1322 3099.1322 45891.84 45891.84 48990.972 48990.972 48990.972 48990.972
20 -516828.06 -516828.06 3101.4321 3101.4321 45884.14 45884.14 48985.572 48985.572 48985.572 48985.572
30 -517032.1 -517032.1 3198.5939 3198.5939 45793.571 45793.571 48992.165 48992.165 48992.165 48992.165
40 -517095.56 -517095.56 3244.0797 3244.0797 45715.265 45715.265 48959.345 48959.345 48959.345 48959.345
50 -517273.54 -517273.54 3274.9142 3274.9142 45665.997 45665.997 48940.911 48940.911 48940.911 48940.911
binsize = 7, bins = 6 6 6
2 neighbor lists, perpetual/occasional/extra = 1 1 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
(2) compute group/group, occasional, copy from (1)
attributes: half, newton on
pair build: copy
stencil: none
bin: none
Per MPI rank memory allocation (min/avg/max) = 29.08 | 29.08 | 29.08 Mbytes
Step c_epa v_epa E_vdwl v_vdwl E_coul v_coul v_eref v_pe c_c2 v_pair
0 -516634.27 -516634.27 3169.9427 3169.9427 46212.482 46212.482 49382.425 49382.425 49382.425 49382.425
10 -517027.35 -517027.35 3099.1374 3099.1374 45891.866 45891.866 48991.003 48991.003 48991.003 48991.003
20 -516828.05 -516828.05 3101.4373 3101.4373 45884.156 45884.156 48985.594 48985.594 48985.594 48985.594
30 -517032.07 -517032.07 3198.5951 3198.5951 45793.595 45793.595 48992.191 48992.191 48992.191 48992.191
40 -517095.54 -517095.54 3244.0771 3244.0771 45715.292 45715.292 48959.369 48959.369 48959.369 48959.369
50 -517273.5 -517273.5 3274.9097 3274.9097 45666.025 45666.025 48940.935 48940.935 48940.935 48940.935
Loop time of 15.3339 on 1 procs for 50 steps with 4500 atoms
Loop time of 4.31105 on 1 procs for 50 steps with 4500 atoms
100.1% CPU use with 1 MPI tasks x 1 OpenMP threads
Performance: 2.004 ns/day 11.975 hours/ns 11.598 timesteps/s
Performance: 0.563 ns/day, 42.594 hours/ns, 3.261 timesteps/s
32.0% CPU use with 1 MPI tasks x no OpenMP threads
MPI task timings breakdown:
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 3.5071 | 3.5071 | 3.5071 | 0.0 | 81.35
Bond | 0.00025034 | 0.00025034 | 0.00025034 | 0.0 | 0.01
Kspace | 0.19991 | 0.19991 | 0.19991 | 0.0 | 4.64
Neigh | 0.31459 | 0.31459 | 0.31459 | 0.0 | 7.30
Comm | 0.010338 | 0.010338 | 0.010338 | 0.0 | 0.24
Output | 0.24722 | 0.24722 | 0.24722 | 0.0 | 5.73
Modify | 0.029466 | 0.029466 | 0.029466 | 0.0 | 0.68
Other | | 0.002182 | | | 0.05
Pair | 13.432 | 13.432 | 13.432 | 0.0 | 87.60
Bond | 0.000365 | 0.000365 | 0.000365 | 0.0 | 0.00
Kspace | 0.581 | 0.581 | 0.581 | 0.0 | 3.79
Neigh | 0.66081 | 0.66081 | 0.66081 | 0.0 | 4.31
Comm | 0.019908 | 0.019908 | 0.019908 | 0.0 | 0.13
Output | 0.57731 | 0.57731 | 0.57731 | 0.0 | 3.76
Modify | 0.058515 | 0.058515 | 0.058515 | 0.0 | 0.38
Other | | 0.003889 | | | 0.03
Nlocal: 4500 ave 4500 max 4500 min
Histogram: 1 0 0 0 0 0 0 0 0 0
@ -135,10 +175,10 @@ Histogram: 1 0 0 0 0 0 0 0 0 0
Neighs: 2.60198e+06 ave 2.60198e+06 max 2.60198e+06 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Total # of neighbors = 2601984
Ave neighs/atom = 578.219
Total # of neighbors = 2601983
Ave neighs/atom = 578.218
Ave special neighs/atom = 2
Neighbor list builds = 4
Dangerous builds = 1
Total wall time: 0:00:04
Total wall time: 0:00:16

View File

@ -1,5 +1,4 @@
LAMMPS (21 Aug 2015-ICMS)
using 1 OpenMP thread(s) per MPI task
LAMMPS (19 May 2017)
units real
atom_style full
@ -50,6 +49,35 @@ fix 1 all shake 0.0001 20 0 b 1 a 1
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
# make certain that shake constraints are satisfied
run 0 post no
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 3380 960
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
1 neighbor lists, perpetual/occasional/extra = 1 0 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
Per MPI rank memory allocation (min/avg/max) = 10.6 | 10.61 | 10.61 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0 -16692.358 0 -16692.358 -1289.8319
Loop time of 1.75e-06 on 4 procs for 0 steps with 4500 atoms
group oxy type 1
1500 atoms in group oxy
group hyd type 2
@ -88,6 +116,7 @@ thermo 10
run 50
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
@ -95,38 +124,49 @@ PPPM initialization ...
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 3380 960
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:75)
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:75)
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:77)
WARNING: Compute pe/tally only called from pair style (../compute_pe_tally.cpp:77)
Neighbor list info ...
2 neighbor list requests
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7 -> bins = 6 6 6
Memory usage per processor = 8.44413 Mbytes
Step epa epa E_vdwl vdwl E_coul coul eref pe c2 pair
0 -516632.19 -516632.19 3169.9382 3169.9382 46213.889 46213.889 49383.827 49383.827 49383.827 49383.827
10 -517027.36 -517027.36 3099.1322 3099.1322 45891.84 45891.84 48990.972 48990.972 48990.972 48990.972
20 -516828.06 -516828.06 3101.4321 3101.4321 45884.14 45884.14 48985.572 48985.572 48985.572 48985.572
30 -517032.1 -517032.1 3198.5939 3198.5939 45793.571 45793.571 48992.165 48992.165 48992.165 48992.165
40 -517095.56 -517095.56 3244.0797 3244.0797 45715.265 45715.265 48959.345 48959.345 48959.345 48959.345
50 -517273.54 -517273.54 3274.9142 3274.9142 45665.997 45665.997 48940.911 48940.911 48940.911 48940.911
binsize = 7, bins = 6 6 6
2 neighbor lists, perpetual/occasional/extra = 1 1 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
(2) compute group/group, occasional, copy from (1)
attributes: half, newton on
pair build: copy
stencil: none
bin: none
Per MPI rank memory allocation (min/avg/max) = 11.86 | 11.87 | 11.88 Mbytes
Step c_epa v_epa E_vdwl v_vdwl E_coul v_coul v_eref v_pe c_c2 v_pair
0 -516634.27 -516634.27 3169.9427 3169.9427 46212.482 46212.482 49382.425 49382.425 49382.425 49382.425
10 -517027.35 -517027.35 3099.1374 3099.1374 45891.866 45891.866 48991.003 48991.003 48991.003 48991.003
20 -516828.05 -516828.05 3101.4373 3101.4373 45884.156 45884.156 48985.594 48985.594 48985.594 48985.594
30 -517032.07 -517032.07 3198.5951 3198.5951 45793.595 45793.595 48992.191 48992.191 48992.191 48992.191
40 -517095.54 -517095.54 3244.0771 3244.0771 45715.292 45715.292 48959.369 48959.369 48959.369 48959.369
50 -517273.5 -517273.5 3274.9097 3274.9097 45666.025 45666.025 48940.935 48940.935 48940.935 48940.935
Loop time of 2.32344 on 4 procs for 50 steps with 4500 atoms
Loop time of 1.20533 on 4 procs for 50 steps with 4500 atoms
100.0% CPU use with 4 MPI tasks x 1 OpenMP threads
Performance: 7.168 ns/day 3.348 hours/ns 41.482 timesteps/s
Performance: 3.719 ns/day, 6.454 hours/ns, 21.520 timesteps/s
64.0% CPU use with 4 MPI tasks x no OpenMP threads
MPI task timings breakdown:
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 0.87053 | 0.90325 | 0.94364 | 2.8 | 74.94
Bond | 0.00015402 | 0.00018191 | 0.00020909 | 0.2 | 0.02
Kspace | 0.061657 | 0.10164 | 0.13394 | 8.4 | 8.43
Neigh | 0.088292 | 0.088332 | 0.088373 | 0.0 | 7.33
Comm | 0.017319 | 0.017806 | 0.018291 | 0.4 | 1.48
Output | 0.07067 | 0.070706 | 0.070813 | 0.0 | 5.87
Modify | 0.021655 | 0.021694 | 0.02173 | 0.0 | 1.80
Other | | 0.001719 | | | 0.14
Pair | 1.5561 | 1.8883 | 2.0327 | 14.1 | 81.27
Bond | 8.8e-05 | 0.000116 | 0.000135 | 0.0 | 0.00
Kspace | 0.094718 | 0.1933 | 0.26055 | 14.1 | 8.32
Neigh | 0.085117 | 0.1073 | 0.1147 | 3.9 | 4.62
Comm | 0.014156 | 0.017907 | 0.020005 | 1.8 | 0.77
Output | 0.071634 | 0.090599 | 0.097665 | 3.6 | 3.90
Modify | 0.019447 | 0.024101 | 0.026277 | 1.8 | 1.04
Other | | 0.001804 | | | 0.08
Nlocal: 1125 ave 1148 max 1097 min
Histogram: 1 0 0 1 0 0 0 0 1 1
@ -135,10 +175,10 @@ Histogram: 1 0 0 1 0 1 0 0 0 1
Neighs: 650496 ave 675112 max 631353 min
Histogram: 1 0 0 1 1 0 0 0 0 1
Total # of neighbors = 2601984
Ave neighs/atom = 578.219
Total # of neighbors = 2601983
Ave neighs/atom = 578.218
Ave special neighs/atom = 2
Neighbor list builds = 4
Dangerous builds = 1
Total wall time: 0:00:01
Total wall time: 0:00:02

View File

@ -1,5 +1,4 @@
LAMMPS (21 Aug 2015-ICMS)
using 1 OpenMP thread(s) per MPI task
LAMMPS (19 May 2017)
units real
atom_style full
@ -50,6 +49,35 @@ fix 1 all shake 0.0001 20 0 b 1 a 1
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
# make certain that shake constraints are satisfied
run 0 post no
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 8000 3375
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
1 neighbor lists, perpetual/occasional/extra = 1 0 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
Per MPI rank memory allocation (min/avg/max) = 26.54 | 26.54 | 26.54 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0 -16692.358 0 -16692.358 -1289.8319
Loop time of 2e-06 on 1 procs for 0 steps with 4500 atoms
group one molecule 1 2
6 atoms in group one
@ -79,6 +107,7 @@ thermo 10
run 50
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
@ -86,38 +115,32 @@ PPPM initialization ...
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 8000 3375
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:75)
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:75)
Neighbor list info ...
1 neighbor list requests
update every 1 steps, delay 10 steps, check yes
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7 -> bins = 6 6 6
Memory usage per processor = 24.631 Mbytes
Step press spa press one ref
0 26497.547 26497.547 26497.547 -2357033.6 -2357033.6
10 23665.073 23665.073 23665.073 -2096057.3 -2096057.3
20 23338.149 23338.149 23338.149 -2034283 -2034283
30 25946.4 25946.4 25946.4 -2002817 -2002817
40 27238.349 27238.349 27238.349 -2155411.5 -2155411.5
50 27783.092 27783.092 27783.092 -1862190.3 -1862190.3
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:79)
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:79)
Per MPI rank memory allocation (min/avg/max) = 35.9 | 35.9 | 35.9 Mbytes
Step c_press v_spa v_press v_one v_ref
0 26496.811 26496.811 26496.811 -2356992.7 -2356992.7
10 23665.129 23665.129 23665.129 -2096059 -2096059
20 23338.197 23338.197 23338.197 -2034284.1 -2034284.1
30 25946.434 25946.434 25946.434 -2002815.3 -2002815.3
40 27238.374 27238.374 27238.374 -2155408.7 -2155408.7
50 27783.107 27783.107 27783.107 -1862191.5 -1862191.5
Loop time of 14.2089 on 1 procs for 50 steps with 4500 atoms
Loop time of 4.15609 on 1 procs for 50 steps with 4500 atoms
100.1% CPU use with 1 MPI tasks x 1 OpenMP threads
Performance: 2.079 ns/day 11.545 hours/ns 12.031 timesteps/s
Performance: 0.608 ns/day, 39.469 hours/ns, 3.519 timesteps/s
32.0% CPU use with 1 MPI tasks x no OpenMP threads
MPI task timings breakdown:
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 3.6444 | 3.6444 | 3.6444 | 0.0 | 87.69
Bond | 0.0016105 | 0.0016105 | 0.0016105 | 0.0 | 0.04
Kspace | 0.22345 | 0.22345 | 0.22345 | 0.0 | 5.38
Neigh | 0.23588 | 0.23588 | 0.23588 | 0.0 | 5.68
Comm | 0.010035 | 0.010035 | 0.010035 | 0.0 | 0.24
Output | 0.0084085 | 0.0084085 | 0.0084085 | 0.0 | 0.20
Modify | 0.029978 | 0.029978 | 0.029978 | 0.0 | 0.72
Other | | 0.002368 | | | 0.06
Pair | 12.983 | 12.983 | 12.983 | 0.0 | 91.37
Bond | 0.002788 | 0.002788 | 0.002788 | 0.0 | 0.02
Kspace | 0.62745 | 0.62745 | 0.62745 | 0.0 | 4.42
Neigh | 0.49839 | 0.49839 | 0.49839 | 0.0 | 3.51
Comm | 0.018597 | 0.018597 | 0.018597 | 0.0 | 0.13
Output | 0.015852 | 0.015852 | 0.015852 | 0.0 | 0.11
Modify | 0.058415 | 0.058415 | 0.058415 | 0.0 | 0.41
Other | | 0.004126 | | | 0.03
Nlocal: 4500 ave 4500 max 4500 min
Histogram: 1 0 0 0 0 0 0 0 0 0
@ -132,4 +155,4 @@ Ave special neighs/atom = 2
Neighbor list builds = 3
Dangerous builds = 0
Total wall time: 0:00:04
Total wall time: 0:00:15

View File

@ -1,5 +1,4 @@
LAMMPS (21 Aug 2015-ICMS)
using 1 OpenMP thread(s) per MPI task
LAMMPS (19 May 2017)
units real
atom_style full
@ -50,6 +49,35 @@ fix 1 all shake 0.0001 20 0 b 1 a 1
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
# make certain that shake constraints are satisfied
run 0 post no
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 3380 960
Neighbor list info ...
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7, bins = 6 6 6
1 neighbor lists, perpetual/occasional/extra = 1 0 0
(1) pair lj/cut/coul/long, perpetual
attributes: half, newton on
pair build: half/bin/newton
stencil: half/bin/3d/newton
bin: standard
Per MPI rank memory allocation (min/avg/max) = 10.6 | 10.61 | 10.61 Mbytes
Step Temp E_pair E_mol TotEng Press
0 0 -16692.358 0 -16692.358 -1289.8319
Loop time of 4e-06 on 4 procs for 0 steps with 4500 atoms
group one molecule 1 2
6 atoms in group one
@ -79,6 +107,7 @@ thermo 10
run 50
PPPM initialization ...
WARNING: Using 12-bit tables for long-range coulomb (../kspace.cpp:321)
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
@ -86,44 +115,38 @@ PPPM initialization ...
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 3380 960
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:75)
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:75)
Neighbor list info ...
1 neighbor list requests
update every 1 steps, delay 10 steps, check yes
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7 -> bins = 6 6 6
Memory usage per processor = 12.0691 Mbytes
Step press spa press one ref
0 26497.547 26497.547 26497.547 -2357033.6 -2357033.6
10 23665.073 23665.073 23665.073 -2096057.3 -2096057.3
20 23338.149 23338.149 23338.149 -2034283 -2034283
30 25946.4 25946.4 25946.4 -2002817 -2002817
40 27238.349 27238.349 27238.349 -2155411.5 -2155411.5
50 27783.092 27783.092 27783.092 -1862190.3 -1862190.3
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:79)
WARNING: Compute stress/tally only called from pair style (../compute_stress_tally.cpp:79)
Per MPI rank memory allocation (min/avg/max) = 15.25 | 15.26 | 15.27 Mbytes
Step c_press v_spa v_press v_one v_ref
0 26496.811 26496.811 26496.811 -2356992.7 -2356992.7
10 23665.129 23665.129 23665.129 -2096059 -2096059
20 23338.197 23338.197 23338.197 -2034284.1 -2034284.1
30 25946.434 25946.434 25946.434 -2002815.3 -2002815.3
40 27238.374 27238.374 27238.374 -2155408.7 -2155408.7
50 27783.107 27783.107 27783.107 -1862191.5 -1862191.5
Loop time of 4.32017 on 4 procs for 50 steps with 4500 atoms
Loop time of 1.17266 on 4 procs for 50 steps with 4500 atoms
100.0% CPU use with 4 MPI tasks x 1 OpenMP threads
Performance: 7.368 ns/day 3.257 hours/ns 42.638 timesteps/s
Performance: 2.000 ns/day, 12.000 hours/ns, 11.574 timesteps/s
31.8% CPU use with 4 MPI tasks x no OpenMP threads
MPI task timings breakdown:
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 0.89832 | 0.93222 | 0.98611 | 3.4 | 79.50
Bond | 0.00081754 | 0.00096095 | 0.0011327 | 0.4 | 0.08
Kspace | 0.068058 | 0.12154 | 0.15522 | 9.4 | 10.36
Neigh | 0.065756 | 0.065785 | 0.065824 | 0.0 | 5.61
Comm | 0.017489 | 0.017982 | 0.018623 | 0.4 | 1.53
Output | 0.010985 | 0.011017 | 0.011111 | 0.1 | 0.94
Modify | 0.021429 | 0.021491 | 0.021551 | 0.0 | 1.83
Other | | 0.001671 | | | 0.14
Pair | 3.5816 | 3.6917 | 3.839 | 4.9 | 85.45
Bond | 0.001579 | 0.0016563 | 0.001709 | 0.1 | 0.04
Kspace | 0.22505 | 0.3716 | 0.48023 | 15.3 | 8.60
Neigh | 0.14558 | 0.14568 | 0.14575 | 0.0 | 3.37
Comm | 0.032009 | 0.03441 | 0.036274 | 0.8 | 0.80
Output | 0.02253 | 0.023115 | 0.024844 | 0.7 | 0.54
Modify | 0.046954 | 0.047086 | 0.047132 | 0.0 | 1.09
Other | | 0.004935 | | | 0.11
Nlocal: 1125 ave 1154 max 1092 min
Histogram: 1 0 0 0 1 0 1 0 0 1
Nghost: 12263.5 ave 12300 max 12219 min
Histogram: 1 0 1 0 0 0 0 0 0 2
Neighs: 650438 ave 678786 max 626279 min
Neighs: 650438 ave 678787 max 626279 min
Histogram: 1 0 0 1 1 0 0 0 0 1
Total # of neighbors = 2601750
@ -132,4 +155,4 @@ Ave special neighs/atom = 2
Neighbor list builds = 3
Dangerous builds = 0
Total wall time: 0:00:01
Total wall time: 0:00:04

View File

@ -1,136 +0,0 @@
LAMMPS (21 Aug 2015-ICMS)
using 1 OpenMP thread(s) per MPI task
units real
atom_style full
read_data data.spce
orthogonal box = (0.02645 0.02645 0.02641) to (35.5328 35.5328 35.4736)
1 by 1 by 1 MPI processor grid
reading atoms ...
4500 atoms
scanning bonds ...
2 = max bonds/atom
scanning angles ...
1 = max angles/atom
reading bonds ...
3000 bonds
reading angles ...
1500 angles
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
1 = max # of 1-4 neighbors
2 = max # of special neighbors
pair_style lj/cut/coul/long 12.0 12.0
kspace_style pppm 1.0e-4
pair_coeff 1 1 0.15535 3.166
pair_coeff * 2 0.0000 0.0000
bond_style harmonic
angle_style harmonic
dihedral_style none
improper_style none
bond_coeff 1 1000.00 1.000
angle_coeff 1 100.0 109.47
special_bonds lj/coul 0.0 0.0 1.0
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
2 = max # of special neighbors
neighbor 2.0 bin
fix 1 all shake 0.0001 20 0 b 1 a 1
0 = # of size 2 clusters
0 = # of size 3 clusters
0 = # of size 4 clusters
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
group one molecule 1 2
6 atoms in group one
# the following section shows equivalences between using the pe/tally compute and other computes and thermo keywords
# compute pairwise force between two molecules and everybody
compute fpa one group/group all pair yes kspace no boundary no
# tally pairwise force between two molecules and the all molecules
compute c1 one force/tally all
# tally the force of all with all (should be zero)
compute c2 all force/tally all
# collect per atom data. only reduce over the first group.
compute one one reduce sum c_c1[1] c_c1[2] c_c1[3]
compute red all reduce sum c_c2[1] c_c2[2] c_c2[3]
# determine magnitude of force
variable fpa equal sqrt(c_fpa[1]*c_fpa[1]+c_fpa[2]*c_fpa[2]+c_fpa[3]*c_fpa[3])
variable for equal sqrt(c_one[1]*c_one[1]+c_one[2]*c_one[2]+c_one[3]*c_one[3])
# round to 10**-10 absolute precision.
variable ref equal round(1e10*sqrt(c_red[1]*c_red[1]+c_red[2]*c_red[2]+c_red[3]*c_red[3]))*1e-10
velocity all create 300 432567 dist uniform
timestep 2.0
# v_fpa and v_for and c_c1, c_fpa[] and c_one[] should all each have the same value. v_ref and c_c2 should be zero
thermo_style custom step v_fpa v_for c_c1 c_fpa[1] c_one[1] c_fpa[2] c_one[2] c_fpa[3] c_one[3] v_ref c_c2
thermo 10
run 50
PPPM initialization ...
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 8000 3375
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:75)
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:75)
Neighbor list info ...
2 neighbor list requests
update every 1 steps, delay 10 steps, check yes
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7 -> bins = 6 6 6
Memory usage per processor = 16.7648 Mbytes
Step fpa for c1 fpa[1] one[1] fpa[2] one[2] fpa[3] one[3] ref c2
0 22.732789 22.732789 22.732789 -17.068392 -17.068392 -8.8345214 -8.8345214 -12.140878 -12.140878 0 0
10 11.736915 11.736915 11.736915 -3.3898298 -3.3898298 9.119272 9.119272 -6.5652948 -6.5652948 0 0
20 5.6119761 5.6119761 5.6119761 -0.60028931 -0.60028931 -4.4479886 -4.4479886 3.368876 3.368876 0 0
30 17.292617 17.292617 17.292617 6.1793856 6.1793856 -10.593927 -10.593927 12.190919 12.190919 0 0
40 18.664226 18.664226 18.664226 5.4725079 5.4725079 -6.933046 -6.933046 16.441955 16.441955 0 0
50 12.130282 12.130282 12.130282 -1.0321244 -1.0321244 8.0032646 8.0032646 -9.0568326 -9.0568326 0 0
Loop time of 4.11825 on 1 procs for 50 steps with 4500 atoms
100.0% CPU use with 1 MPI tasks x 1 OpenMP threads
Performance: 2.098 ns/day 11.440 hours/ns 12.141 timesteps/s
MPI task timings breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 3.5286 | 3.5286 | 3.5286 | 0.0 | 85.68
Bond | 6.1274e-05 | 6.1274e-05 | 6.1274e-05 | 0.0 | 0.00
Kspace | 0.1937 | 0.1937 | 0.1937 | 0.0 | 4.70
Neigh | 0.31454 | 0.31454 | 0.31454 | 0.0 | 7.64
Comm | 0.01037 | 0.01037 | 0.01037 | 0.0 | 0.25
Output | 0.039355 | 0.039355 | 0.039355 | 0.0 | 0.96
Modify | 0.029273 | 0.029273 | 0.029273 | 0.0 | 0.71
Other | | 0.002351 | | | 0.06
Nlocal: 4500 ave 4500 max 4500 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Nghost: 21131 ave 21131 max 21131 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Neighs: 2.60198e+06 ave 2.60198e+06 max 2.60198e+06 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Total # of neighbors = 2601984
Ave neighs/atom = 578.219
Ave special neighs/atom = 2
Neighbor list builds = 4
Dangerous builds = 1
Total wall time: 0:00:04

View File

@ -1,136 +0,0 @@
LAMMPS (21 Aug 2015-ICMS)
using 1 OpenMP thread(s) per MPI task
units real
atom_style full
read_data data.spce
orthogonal box = (0.02645 0.02645 0.02641) to (35.5328 35.5328 35.4736)
2 by 2 by 1 MPI processor grid
reading atoms ...
4500 atoms
scanning bonds ...
2 = max bonds/atom
scanning angles ...
1 = max angles/atom
reading bonds ...
3000 bonds
reading angles ...
1500 angles
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
1 = max # of 1-4 neighbors
2 = max # of special neighbors
pair_style lj/cut/coul/long 12.0 12.0
kspace_style pppm 1.0e-4
pair_coeff 1 1 0.15535 3.166
pair_coeff * 2 0.0000 0.0000
bond_style harmonic
angle_style harmonic
dihedral_style none
improper_style none
bond_coeff 1 1000.00 1.000
angle_coeff 1 100.0 109.47
special_bonds lj/coul 0.0 0.0 1.0
2 = max # of 1-2 neighbors
1 = max # of 1-3 neighbors
2 = max # of special neighbors
neighbor 2.0 bin
fix 1 all shake 0.0001 20 0 b 1 a 1
0 = # of size 2 clusters
0 = # of size 3 clusters
0 = # of size 4 clusters
1500 = # of frozen angles
fix 2 all nvt temp 300.0 300.0 100.0
group one molecule 1 2
6 atoms in group one
# the following section shows equivalences between using the pe/tally compute and other computes and thermo keywords
# compute pairwise force between two molecules and everybody
compute fpa one group/group all pair yes kspace no boundary no
# tally pairwise force between two molecules and the all molecules
compute c1 one force/tally all
# tally the force of all with all (should be zero)
compute c2 all force/tally all
# collect per atom data. only reduce over the first group.
compute one one reduce sum c_c1[1] c_c1[2] c_c1[3]
compute red all reduce sum c_c2[1] c_c2[2] c_c2[3]
# determine magnitude of force
variable fpa equal sqrt(c_fpa[1]*c_fpa[1]+c_fpa[2]*c_fpa[2]+c_fpa[3]*c_fpa[3])
variable for equal sqrt(c_one[1]*c_one[1]+c_one[2]*c_one[2]+c_one[3]*c_one[3])
# round to 10**-10 absolute precision.
variable ref equal round(1e10*sqrt(c_red[1]*c_red[1]+c_red[2]*c_red[2]+c_red[3]*c_red[3]))*1e-10
velocity all create 300 432567 dist uniform
timestep 2.0
# v_fpa and v_for and c_c1, c_fpa[] and c_one[] should all each have the same value. v_ref and c_c2 should be zero
thermo_style custom step v_fpa v_for c_c1 c_fpa[1] c_one[1] c_fpa[2] c_one[2] c_fpa[3] c_one[3] v_ref c_c2
thermo 10
run 50
PPPM initialization ...
G vector (1/distance) = 0.218482
grid = 15 15 15
stencil order = 5
estimated absolute RMS force accuracy = 0.0319435
estimated relative force accuracy = 9.61968e-05
using double precision FFTs
3d grid and FFT values/proc = 3380 960
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:75)
WARNING: Compute force/tally only called from pair style (../compute_force_tally.cpp:75)
Neighbor list info ...
2 neighbor list requests
update every 1 steps, delay 10 steps, check yes
master list distance cutoff = 14
ghost atom cutoff = 14
binsize = 7 -> bins = 6 6 6
Memory usage per processor = 8.16441 Mbytes
Step fpa for c1 fpa[1] one[1] fpa[2] one[2] fpa[3] one[3] ref c2
0 22.732789 22.732789 22.732789 -17.068392 -17.068392 -8.8345214 -8.8345214 -12.140878 -12.140878 0 0
10 11.736915 11.736915 11.736915 -3.3898298 -3.3898298 9.119272 9.119272 -6.5652948 -6.5652948 0 0
20 5.6119761 5.6119761 5.6119761 -0.60028931 -0.60028931 -4.4479886 -4.4479886 3.368876 3.368876 0 0
30 17.292617 17.292617 17.292617 6.1793856 6.1793856 -10.593927 -10.593927 12.190919 12.190919 0 0
40 18.664226 18.664226 18.664226 5.4725079 5.4725079 -6.933046 -6.933046 16.441955 16.441955 0 0
50 12.130282 12.130282 12.130282 -1.0321244 -1.0321244 8.0032646 8.0032646 -9.0568326 -9.0568326 0 0
Loop time of 1.13658 on 4 procs for 50 steps with 4500 atoms
100.0% CPU use with 4 MPI tasks x 1 OpenMP threads
Performance: 7.602 ns/day 3.157 hours/ns 43.991 timesteps/s
MPI task timings breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 0.85795 | 0.89088 | 0.93636 | 3.0 | 78.38
Bond | 3.4571e-05 | 4.4644e-05 | 5.4598e-05 | 0.1 | 0.00
Kspace | 0.059847 | 0.1051 | 0.1384 | 8.9 | 9.25
Neigh | 0.085891 | 0.085954 | 0.086 | 0.0 | 7.56
Comm | 0.01758 | 0.018091 | 0.019178 | 0.5 | 1.59
Output | 0.013697 | 0.013725 | 0.013805 | 0.0 | 1.21
Modify | 0.021068 | 0.021137 | 0.021205 | 0.0 | 1.86
Other | | 0.001656 | | | 0.15
Nlocal: 1125 ave 1148 max 1097 min
Histogram: 1 0 0 1 0 0 0 0 1 1
Nghost: 12212.5 ave 12269 max 12162 min
Histogram: 1 0 0 1 0 1 0 0 0 1
Neighs: 650496 ave 675112 max 631353 min
Histogram: 1 0 0 1 1 0 0 0 0 1
Total # of neighbors = 2601984
Ave neighs/atom = 578.219
Ave special neighs/atom = 2
Neighbor list builds = 4
Dangerous builds = 1
Total wall time: 0:00:01

View File

@ -2,12 +2,16 @@ Run these examples as:
mpirun -np 4 lmp_g++ -partition 4x1 -in in.neb.hop1
mpirun -np 4 lmp_g++ -partition 4x1 -in in.neb.hop2
mpirun -np 4 lmp_g++ -partition 4x1 -in in.neb.hop1.end
mpirun -np 3 lmp_g++ -partition 3x1 -in in.neb.sivac
mpirun -np 8 lmp_g++ -partition 4x2 -in in.neb.hop1
mpirun -np 8 lmp_g++ -partition 4x2 -in in.neb.hop2
mpirun -np 6 lmp_g++ -partition 3x2 -in in.neb.sivac
mpirun -np 9 lmp_g++ -partition 3x3 -in in.neb.sivac
mpirun -np 8 lmp_g++ -partition 4x2 -in in.neb.hop1.end
mpirun -np 8 lmp_g++ -partition 4x2 -in in.neb.sivac
Note that more than 4 replicas should be used for a precise estimate
of the activation energy corresponding to a transition.
If you uncomment the dump command lines in the input scripts, you can
create dump files to do visualization from via Python tools: (see

View File

@ -51,7 +51,7 @@ set group nebatoms type 3
group nonneb subtract all nebatoms
fix 1 lower setforce 0.0 0.0 0.0
fix 2 nebatoms neb 1.0
fix 2 nebatoms neb 1.0 parallel ideal
fix 3 all enforce2d
thermo 100

View File

@ -0,0 +1,56 @@
# 2d NEB surface simulation, hop from surface to become adatom
dimension 2
boundary p s p
atom_style atomic
neighbor 0.3 bin
neigh_modify delay 5
atom_modify map array sort 0 0.0
variable u uloop 20
# create geometry with flat surface
lattice hex 0.9
region box block 0 20 0 10 -0.25 0.25
read_data initial.hop1.end
# LJ potentials
pair_style lj/cut 2.5
pair_coeff * * 1.0 1.0 2.5
pair_modify shift yes
# define groups
region 1 block INF INF INF 1.25 INF INF
group lower region 1
group mobile subtract all lower
set group lower type 2
timestep 0.05
# group of NEB atoms - either block or single atom ID 412
region surround block 10 18 17 20 0 0 units box
group nebatoms region surround
#group nebatoms id 412
set group nebatoms type 3
group nonneb subtract all nebatoms
fix 1 lower setforce 0.0 0.0 0.0
fix 2 nebatoms neb 1.0 parallel ideal end first 1.0
fix 3 all enforce2d
thermo 100
#dump 1 nebatoms atom 10 dump.neb.$u
#dump 2 nonneb atom 10 dump.nonneb.$u
# run NEB for 2000 steps or to force tolerance
min_style quickmin
neb 0.0 0.1 1000 1000 100 final final.hop1

View File

@ -53,7 +53,7 @@ set group nebatoms type 3
group nonneb subtract all nebatoms
fix 1 lower setforce 0.0 0.0 0.0
fix 2 nebatoms neb 1.0
fix 2 nebatoms neb 1.0
fix 3 all enforce2d
thermo 100
@ -65,4 +65,4 @@ thermo 100
min_style fire
neb 0.0 0.01 1000 1000 100 final final.hop2
neb 0.0 0.05 1000 1000 100 final final.hop2

View File

@ -66,7 +66,7 @@ minimize 1.0e-6 1.0e-4 1000 10000
reset_timestep 0
fix 1 all neb 1.0
fix 1 all neb 1.0
thermo 100

View File

@ -0,0 +1,860 @@
LAMMPS data file via write_data, version 4 May 2017, timestep = 155
420 atoms
3 atom types
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2.1918578738841410e-01 1.9932852254455714e+01 ylo yhi
-2.8317404080785380e-01 2.8317404080785380e-01 zlo zhi
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LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 229.26196 146.68251 2.9774577 4.4127369 233.11559 0.023301843 0.0224626 1.4763579 0 -3.048332 0.33333333 -3.0250302 0.66666667 -3.0291888 1 -3.0474928
100 0.11027532 0.085410308 3.0967938 0.024201563 0.38551033 0.0017583261 0.0021866943 1.7710358 0 -3.0483469 0.31192818 -3.0465886 0.61093022 -3.0466143 1 -3.0487752
130 0.09954083 0.075481108 3.0927626 0.015664388 0.37491833 0.0017573704 0.0021913201 1.7713726 0 -3.048342 0.31428487 -3.0465846 0.61762817 -3.0466296 1 -3.048776
Climbing replica = 2
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
130 0.37838747 0.3502435 3.0927626 0.015664388 0.37491833 0.0017573704 0.0021913201 1.7713726 0 -3.048342 0.31428487 -3.0465846 0.61762817 -3.0466296 1 -3.048776
230 0.22757286 0.12027481 3.1250243 0.0081260569 0.14019507 0.0018364585 0.002278918 1.76926 0 -3.0483347 0.39730698 -3.0464983 0.64450769 -3.0466973 1 -3.0487772
278 0.096184498 0.085088496 3.1405655 0.0068164307 0.093861113 0.0018426056 0.002286256 1.7684765 0 -3.0483338 0.41277997 -3.0464912 0.65562984 -3.0467294 1 -3.0487775

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LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 229.26196 146.68251 2.9774577 4.4127369 233.11559 0.023301843 0.0224626 1.4763579 0 -3.048332 0.33333333 -3.0250302 0.66666667 -3.0291888 1 -3.0474928
100 0.11375359 0.085350745 3.0966418 0.0236765 0.38531777 0.0017582606 0.0021868783 1.7710738 0 -3.0483467 0.31201141 -3.0465884 0.61117406 -3.0466149 1 -3.0487753
119 0.09996986 0.078639268 3.0937691 0.017444108 0.3780308 0.0017574935 0.0021899317 1.7713574 0 -3.0483433 0.31354192 -3.0465858 0.61555533 -3.0466249 1 -3.0487758
Climbing replica = 2
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
119 0.3793192 0.35281863 3.0937691 0.017444108 0.3780308 0.0017574935 0.0021899317 1.7713574 0 -3.0483433 0.31354192 -3.0465858 0.61555533 -3.0466249 1 -3.0487758
219 0.20159133 0.12247026 3.1244061 0.0085896057 0.13938632 0.0018362816 0.0022783681 1.7693295 0 -3.048335 0.39646633 -3.0464988 0.64277703 -3.0466925 1 -3.0487771
266 0.099868725 0.086180598 3.1401661 0.0070922949 0.095128081 0.001842608 0.002286044 1.7685191 0 -3.048334 0.41231024 -3.0464914 0.65425179 -3.0467252 1 -3.0487774

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LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 4327.2753 2746.3378 0.082169072 4.9967651 4514.5424 0.42933428 0.42323635 1.8941131 0 -3.0535948 0.33333333 -2.6242605 0.66666667 -2.7623811 1 -3.0474969
87 0.095951502 0.052720903 0.005588927 0.065110105 0.12467831 0.0071014928 0.0022798007 2.3003372 0 -3.0535967 0.32435271 -3.0473127 0.62805027 -3.0464952 1 -3.048775
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
87 0.14137277 0.11108954 0.005588927 0.065110105 0.12467831 0.0071014928 0.0022798007 2.3003372 0 -3.0535967 0.32435271 -3.0473127 0.62805027 -3.0464952 1 -3.048775
124 0.099583263 0.085936899 0.0044220372 0.023873795 0.091308308 0.0071061754 0.0022863931 2.308121 0 -3.0535968 0.32223905 -3.0473329 0.61673898 -3.0464906 1 -3.048777

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LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 4327.2753 2746.3378 0.082169072 4.9967651 4514.5424 0.42933428 0.42323635 1.8941131 0 -3.0535948 0.33333333 -2.6242605 0.66666667 -2.7623811 1 -3.0474969
87 0.095951792 0.052720902 0.0055889267 0.065110091 0.12467831 0.0071014928 0.0022798007 2.3003372 0 -3.0535967 0.32435271 -3.0473127 0.62805027 -3.0464952 1 -3.048775
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
87 0.14137297 0.11108954 0.0055889267 0.065110091 0.12467831 0.0071014928 0.0022798007 2.3003372 0 -3.0535967 0.32435271 -3.0473127 0.62805027 -3.0464952 1 -3.048775
124 0.099582186 0.08593683 0.0044220345 0.023873731 0.091308197 0.0071061754 0.0022863931 2.3081211 0 -3.0535968 0.32223904 -3.0473329 0.61673896 -3.0464906 1 -3.048777

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LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 14.104748 10.419633 0.1227071 4.999238 8.2087606 0.0018276223 0.00064050211 0.98401186 0 -3.0514921 0.33333333 -3.0496673 0.66666667 -3.0496645 1 -3.050305
100 0.24646695 0.10792196 0.0077146918 0.058733261 0.63504706 0.001516756 0.0015151635 1.165391 0 -3.0514939 0.2890334 -3.0503533 0.59718494 -3.0499771 1 -3.0514923
200 0.061777741 0.050288749 0.0047486883 0.0095236035 0.88698597 0.0014465772 0.0014462528 1.1692938 0 -3.0514941 0.29975094 -3.0503052 0.62768286 -3.0500476 1 -3.0514938
261 0.048699591 0.038138604 0.0040083594 0.0074854409 0.95722712 0.0014243579 0.0014241377 1.1696848 0 -3.0514942 0.30525481 -3.0502812 0.6357998 -3.0500698 1 -3.051494
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
261 0.95753855 0.94297239 0.0040083594 0.0074854409 0.95722712 0.0014243579 0.0014241377 1.1696848 0 -3.0514942 0.30525481 -3.0502812 0.6357998 -3.0500698 1 -3.051494
361 0.072509627 0.06580631 0.0027545765 0.0044749366 0.016746483 0.0016018879 0.0016017805 1.1704611 0 -3.0514943 0.28176307 -3.0503855 0.50355454 -3.0498924 1 -3.0514942
381 0.04884836 0.040787876 0.0023445904 0.0035162935 0.017959209 0.0016017716 0.0016016898 1.1713862 0 -3.0514943 0.27120138 -3.0504399 0.50428218 -3.0498925 1 -3.0514942

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LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 14.104748 10.419633 0.1227071 4.999238 8.2087606 0.0018276223 0.00064050211 0.98401186 0 -3.0514921 0.33333333 -3.0496673 0.66666667 -3.0496645 1 -3.050305
100 0.24646695 0.10792196 0.0077146918 0.058733261 0.63504706 0.001516756 0.0015151635 1.165391 0 -3.0514939 0.2890334 -3.0503533 0.59718494 -3.0499771 1 -3.0514923
200 0.061777741 0.050288749 0.0047486883 0.0095236035 0.88698597 0.0014465772 0.0014462528 1.1692938 0 -3.0514941 0.29975094 -3.0503052 0.62768286 -3.0500476 1 -3.0514938
261 0.048699591 0.038138604 0.0040083594 0.0074854409 0.95722712 0.0014243579 0.0014241377 1.1696848 0 -3.0514942 0.30525481 -3.0502812 0.6357998 -3.0500698 1 -3.051494
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
261 0.95753855 0.94297239 0.0040083594 0.0074854409 0.95722712 0.0014243579 0.0014241377 1.1696848 0 -3.0514942 0.30525481 -3.0502812 0.6357998 -3.0500698 1 -3.051494
361 0.072509627 0.06580631 0.0027545765 0.0044749366 0.016746483 0.0016018879 0.0016017805 1.1704611 0 -3.0514943 0.28176307 -3.0503855 0.50355454 -3.0498924 1 -3.0514942
381 0.04884836 0.040787876 0.0023445904 0.0035162935 0.017959209 0.0016017716 0.0016016898 1.1713862 0 -3.0514943 0.27120138 -3.0504399 0.50428218 -3.0498925 1 -3.0514942

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LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 7.5525391 1.6345605 0.16683659 7.5525391 7.5525391 1.5383951 0 1.6207355 0 -2213.3343 0.33333333 -2212.7428 0.66666667 -2212.2247 1 -2211.7959
10 0.24005275 0.036502104 0.036483049 0.24005275 0.68351722 0.42916118 0.41794425 1.6989349 0 -2213.3365 0.32909183 -2212.9587 0.65386736 -2212.9073 1 -2213.3253
20 0.07940898 0.016398055 0.024706844 0.07940898 0.71637784 0.41387872 0.41157886 1.7343662 0 -2213.3369 0.32478734 -2212.9621 0.65348766 -2212.923 1 -2213.3346
30 0.094973707 0.0083631681 0.015145947 0.035267404 0.7535772 0.40072717 0.40024605 1.7504612 0 -2213.3372 0.32705584 -2212.9584 0.65894506 -2212.9365 1 -2213.3367
40 0.027727472 0.0044528145 0.011618173 0.022562656 0.76133752 0.39614635 0.39591731 1.7547519 0 -2213.3373 0.32873163 -2212.9562 0.66124255 -2212.9411 1 -2213.337
50 0.019429348 0.0030110281 0.0087135563 0.015391975 0.76952681 0.39274846 0.3926388 1.7578616 0 -2213.3373 0.33022595 -2212.9543 0.66307279 -2212.9446 1 -2213.3372
60 0.019009471 0.0016234562 0.0053426307 0.0086166186 0.77759617 0.38936861 0.38933364 1.7610433 0 -2213.3374 0.33187548 -2212.9523 0.66497617 -2212.948 1 -2213.3373
63 0.0097365134 0.0012734598 0.004777604 0.0076121987 0.77865149 0.38888778 0.38886047 1.7615294 0 -2213.3374 0.33212107 -2212.952 0.66525385 -2212.9485 1 -2213.3373
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
63 0.77865149 0.31085821 0.004777604 0.0076121987 0.77865149 0.38888778 0.38886047 1.7615294 0 -2213.3374 0.33212107 -2212.952 0.66525385 -2212.9485 1 -2213.3373
73 0.098175496 0.033609035 0.0027886955 0.0042742148 0.036594003 0.51024838 0.51023983 1.7607181 0 -2213.3374 0.27574151 -2213.0416 0.50432348 -2212.8271 1 -2213.3374
83 0.03341862 0.012760857 0.0020868177 0.0031625649 0.010189924 0.51014634 0.51014168 1.7602562 0 -2213.3374 0.26045338 -2213.0672 0.50355193 -2212.8272 1 -2213.3374
93 0.0097374358 0.0028416114 0.0014003718 0.0020986584 0.0053485291 0.51011052 0.51010848 1.7601202 0 -2213.3374 0.25397887 -2213.0783 0.50388111 -2212.8273 1 -2213.3374

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@ -0,0 +1,18 @@
LAMMPS (19 May 2017)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 7.5525391 1.6345605 0.16683659 7.5525391 7.5525391 1.5383951 0 1.6207355 0 -2213.3343 0.33333333 -2212.7428 0.66666667 -2212.2247 1 -2211.7959
10 0.24005275 0.036502104 0.036483049 0.24005275 0.68351722 0.42916118 0.41794425 1.6989349 0 -2213.3365 0.32909183 -2212.9587 0.65386736 -2212.9073 1 -2213.3253
20 0.07940898 0.016398055 0.024706844 0.07940898 0.71637784 0.41387872 0.41157886 1.7343662 0 -2213.3369 0.32478734 -2212.9621 0.65348766 -2212.923 1 -2213.3346
30 0.094973708 0.0083631681 0.015145947 0.035267404 0.7535772 0.40072717 0.40024605 1.7504612 0 -2213.3372 0.32705584 -2212.9584 0.65894506 -2212.9365 1 -2213.3367
40 0.027727472 0.0044528144 0.011618173 0.022562656 0.76133752 0.39614635 0.39591731 1.7547519 0 -2213.3373 0.32873163 -2212.9562 0.66124255 -2212.9411 1 -2213.337
50 0.019429341 0.0030110281 0.0087135565 0.015391975 0.7695268 0.39274846 0.3926388 1.7578616 0 -2213.3373 0.33022595 -2212.9543 0.66307279 -2212.9446 1 -2213.3372
60 0.019048963 0.0016262345 0.0053426844 0.0086167196 0.77759655 0.38936867 0.3893337 1.7610433 0 -2213.3374 0.33187545 -2212.9523 0.66497615 -2212.948 1 -2213.3373
63 0.0097037048 0.0012761841 0.0047749367 0.0076075138 0.77865545 0.38888554 0.38885827 1.7615318 0 -2213.3374 0.33212221 -2212.952 0.66525512 -2212.9485 1 -2213.3373
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
63 0.77865545 0.3108551 0.0047749367 0.0076075138 0.77865545 0.38888554 0.38885827 1.7615318 0 -2213.3374 0.33212221 -2212.952 0.66525512 -2212.9485 1 -2213.3373
73 0.098595989 0.033659485 0.0027927196 0.0042813387 0.038224344 0.51024759 0.51023901 1.7607156 0 -2213.3374 0.27595612 -2213.0413 0.50453988 -2212.8271 1 -2213.3374
83 0.033344977 0.012868685 0.0020880608 0.0031645847 0.010250413 0.51014677 0.5101421 1.7602601 0 -2213.3374 0.26053624 -2213.067 0.50358775 -2212.8272 1 -2213.3374
93 0.013254873 0.0038176141 0.0014928226 0.0022407967 0.0058577818 0.51011371 0.51011138 1.7601272 0 -2213.3374 0.25452741 -2213.0774 0.50382161 -2212.8273 1 -2213.3374
95 0.0099964951 0.0031053214 0.0014131665 0.0021184362 0.0053683638 0.51011105 0.51010897 1.7601232 0 -2213.3374 0.2540975 -2213.0781 0.50387313 -2212.8273 1 -2213.3374

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@ -1,10 +0,0 @@
LAMMPS (5 Oct 2016)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 4327.2753 2746.3378 0.3387091 5.0075576 4514.5424 0.42933428 0.42323635 1.8941131 0 -3.0535948 0.33333333 -2.6242605 0.66666667 -2.7623811 1 -3.0474969
100 0.10482184 0.085218486 0.014588241 0.066178594 0.19602237 0.0070900402 0.0022691875 2.3031875 0 -3.0535967 0.31839181 -3.0473647 0.63987598 -3.0465067 1 -3.0487759
111 0.096708467 0.07803707 0.013922973 0.05417562 0.2023467 0.0070871172 0.0022668002 2.3052945 0 -3.0535968 0.31853431 -3.0473633 0.64178871 -3.0465096 1 -3.0487764
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
111 0.2023467 0.1777038 0.013922973 0.05417562 0.2023467 0.0070871172 0.0022668002 2.3052945 0 -3.0535968 0.31853431 -3.0473633 0.64178871 -3.0465096 1 -3.0487764
179 0.096874474 0.090676856 0.01040177 0.023364005 0.096874474 0.0071047642 0.0022856172 2.3122768 0 -3.0535969 0.31577311 -3.0473955 0.61798541 -3.0464922 1 -3.0487778

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@ -1,10 +0,0 @@
LAMMPS (5 Oct 2016)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 4327.2753 2746.3378 0.3387091 5.0075576 4514.5424 0.42933428 0.42323635 1.8941131 0 -3.0535948 0.33333333 -2.6242605 0.66666667 -2.7623811 1 -3.0474969
100 0.10482171 0.085218406 0.014588234 0.066178435 0.19602242 0.0070900401 0.0022691875 2.3031875 0 -3.0535967 0.31839181 -3.0473647 0.639876 -3.0465067 1 -3.0487759
111 0.096708718 0.078036984 0.013922966 0.054175505 0.20234693 0.0070871172 0.0022668002 2.3052946 0 -3.0535968 0.31853431 -3.0473633 0.64178873 -3.0465096 1 -3.0487764
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
111 0.20234693 0.17770387 0.013922966 0.054175505 0.20234693 0.0070871172 0.0022668002 2.3052946 0 -3.0535968 0.31853431 -3.0473633 0.64178873 -3.0465096 1 -3.0487764
178 0.09975409 0.093814031 0.010577358 0.024247224 0.09975409 0.0071042931 0.0022851195 2.312004 0 -3.0535969 0.31607934 -3.0473923 0.618931 -3.0464926 1 -3.0487777

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@ -1,18 +0,0 @@
LAMMPS (5 Oct 2016)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 14.104748 10.419633 0.24852044 5.0039071 8.2116049 0.0018276223 0.00064050211 0.98401186 0 -3.0514921 0.33333333 -3.0496673 0.66666667 -3.0496645 1 -3.050305
100 0.24646695 0.10792196 0.01781018 0.098854684 0.63725646 0.001516756 0.0015151635 1.165391 0 -3.0514939 0.2890334 -3.0503533 0.59718494 -3.0499771 1 -3.0514923
200 0.061777741 0.050288749 0.012466513 0.020420207 0.88741041 0.0014465772 0.0014462528 1.1692938 0 -3.0514941 0.29975094 -3.0503052 0.62768286 -3.0500476 1 -3.0514938
300 0.056346766 0.030000618 0.0093152917 0.013765031 1.0101529 0.0014069751 0.0014068154 1.1699608 0 -3.0514942 0.30992449 -3.0502613 0.64174291 -3.0500873 1 -3.0514941
400 0.025589489 0.015671005 0.0061287063 0.008588518 1.1136424 0.001370987 0.0013709154 1.1704204 0 -3.0514943 0.32016645 -3.0502198 0.65324019 -3.0501233 1 -3.0514943
500 0.014778626 0.0092108366 0.0042668521 0.0059963914 1.1636579 0.0013527466 0.0013527072 1.1706283 0 -3.0514944 0.32550275 -3.0501993 0.65875414 -3.0501416 1 -3.0514943
600 0.08786211 0.020876327 0.0031421548 0.0051657363 1.1898894 0.0013430848 0.0013430599 1.1707681 0 -3.0514944 0.32831927 -3.0501889 0.66160681 -3.0501513 1 -3.0514944
633 0.0098132678 0.0055392541 0.0030063464 0.0043091323 1.1924486 0.0013420127 0.0013419893 1.1707818 0 -3.0514944 0.32862625 -3.0501878 0.66191769 -3.0501524 1 -3.0514944
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
633 1.1924486 1.1648685 0.0030063464 0.0043091323 1.1924486 0.0013420127 0.0013419893 1.1707818 0 -3.0514944 0.32862625 -3.0501878 0.66191769 -3.0501524 1 -3.0514944
733 0.095331134 0.089136608 0.0021551441 0.0031844438 0.043042998 0.0016022317 0.0016022168 1.170789 0 -3.0514944 0.29157063 -3.0503375 0.50358402 -3.0498922 1 -3.0514944
833 0.10539135 0.030724373 0.0013749699 0.002221013 0.10539135 0.0016019798 0.001601971 1.1732118 0 -3.0514944 0.26249002 -3.0504848 0.50415223 -3.0498924 1 -3.0514944
933 0.01883894 0.011496399 0.0011058925 0.0018178041 0.014621806 0.0016018934 0.0016018865 1.173866 0 -3.0514944 0.25788763 -3.0505113 0.50466375 -3.0498925 1 -3.0514944
996 0.0082457876 0.0036336551 0.00077325986 0.0013910671 0.0068823708 0.0016018293 0.0016018244 1.174511 0 -3.0514944 0.2544553 -3.0505324 0.50520462 -3.0498926 1 -3.0514944

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@ -1,18 +0,0 @@
LAMMPS (5 Oct 2016)
Running on 4 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 14.104748 10.419633 0.24852044 5.0039071 8.2116049 0.0018276223 0.00064050211 0.98401186 0 -3.0514921 0.33333333 -3.0496673 0.66666667 -3.0496645 1 -3.050305
100 0.24646695 0.10792196 0.01781018 0.098854684 0.63725646 0.001516756 0.0015151635 1.165391 0 -3.0514939 0.2890334 -3.0503533 0.59718494 -3.0499771 1 -3.0514923
200 0.061777741 0.050288749 0.012466513 0.020420207 0.88741041 0.0014465772 0.0014462528 1.1692938 0 -3.0514941 0.29975094 -3.0503052 0.62768286 -3.0500476 1 -3.0514938
300 0.056346766 0.030000618 0.0093152917 0.013765031 1.0101529 0.0014069751 0.0014068154 1.1699608 0 -3.0514942 0.30992449 -3.0502613 0.64174291 -3.0500873 1 -3.0514941
400 0.025589489 0.015671005 0.0061287063 0.008588518 1.1136424 0.001370987 0.0013709154 1.1704204 0 -3.0514943 0.32016645 -3.0502198 0.65324019 -3.0501233 1 -3.0514943
500 0.014778626 0.0092108366 0.0042668521 0.0059963914 1.1636579 0.0013527466 0.0013527072 1.1706283 0 -3.0514944 0.32550275 -3.0501993 0.65875414 -3.0501416 1 -3.0514943
600 0.08786211 0.020876327 0.0031421548 0.0051657363 1.1898894 0.0013430848 0.0013430599 1.1707681 0 -3.0514944 0.32831927 -3.0501889 0.66160681 -3.0501513 1 -3.0514944
633 0.0098132678 0.0055392541 0.0030063464 0.0043091323 1.1924486 0.0013420127 0.0013419893 1.1707818 0 -3.0514944 0.32862625 -3.0501878 0.66191769 -3.0501524 1 -3.0514944
Climbing replica = 3
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
633 1.1924486 1.1648685 0.0030063464 0.0043091323 1.1924486 0.0013420127 0.0013419893 1.1707818 0 -3.0514944 0.32862625 -3.0501878 0.66191769 -3.0501524 1 -3.0514944
733 0.095331134 0.089136608 0.0021551441 0.0031844438 0.043042998 0.0016022317 0.0016022168 1.170789 0 -3.0514944 0.29157063 -3.0503375 0.50358402 -3.0498922 1 -3.0514944
833 0.10539135 0.030724373 0.0013749699 0.002221013 0.10539135 0.0016019798 0.001601971 1.1732118 0 -3.0514944 0.26249002 -3.0504848 0.50415223 -3.0498924 1 -3.0514944
933 0.01883894 0.011496399 0.0011058925 0.0018178041 0.014621806 0.0016018934 0.0016018865 1.173866 0 -3.0514944 0.25788763 -3.0505113 0.50466375 -3.0498925 1 -3.0514944
996 0.0082457876 0.0036336551 0.00077325986 0.0013910671 0.0068823708 0.0016018293 0.0016018244 1.174511 0 -3.0514944 0.2544553 -3.0505324 0.50520462 -3.0498926 1 -3.0514944

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@ -1,14 +0,0 @@
LAMMPS (5 Oct 2016)
Running on 3 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 7.5525391 1.6345605 0.16683659 7.5525391 7.5525391 1.5383951 0 1.6207355 0 -2213.3343 0.5 -2212.4096 1 -2211.7959
10 0.27332818 0.040944923 0.039164338 0.27332818 0.17804882 0.51235911 0.497084 1.6790474 0 -2213.3364 0.49024121 -2212.824 1 -2213.3211
20 0.1820396 0.018049916 0.024428411 0.1820396 0.08601739 0.51038174 0.5080746 1.7224961 0 -2213.337 0.49199582 -2212.8266 1 -2213.3347
30 0.043288796 0.0068108825 0.017372479 0.043288796 0.049466709 0.51032316 0.5095943 1.7304745 0 -2213.3371 0.49553568 -2212.8268 1 -2213.3364
40 0.0421393 0.0037035761 0.01173707 0.0421393 0.026104735 0.51022733 0.5100163 1.7366752 0 -2213.3373 0.49838067 -2212.8271 1 -2213.3371
50 0.025897844 0.0022804241 0.0081056535 0.025897844 0.016908913 0.5101712 0.51008591 1.739143 0 -2213.3373 0.49923344 -2212.8272 1 -2213.3373
59 0.00962839 0.0012946076 0.005657505 0.009365729 0.012040803 0.51014185 0.51010207 1.7404554 0 -2213.3374 0.49955698 -2212.8272 1 -2213.3373
Climbing replica = 2
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
59 0.012040803 0.0031505502 0.005657505 0.009365729 0.012040803 0.51014185 0.51010207 1.7404554 0 -2213.3374 0.49955698 -2212.8272 1 -2213.3373
63 0.009152118 0.0016692472 0.0049645771 0.0081967836 0.009152118 0.51013743 0.51010776 1.7409028 0 -2213.3374 0.50022239 -2212.8272 1 -2213.3373

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@ -1,14 +0,0 @@
LAMMPS (5 Oct 2016)
Running on 3 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 7.5525391 1.6345605 0.16683659 7.5525391 7.5525391 1.5383951 0 1.6207355 0 -2213.3343 0.5 -2212.4096 1 -2211.7959
10 0.27332818 0.040944923 0.039164338 0.27332818 0.17804882 0.51235911 0.497084 1.6790474 0 -2213.3364 0.49024121 -2212.824 1 -2213.3211
20 0.1820396 0.018049916 0.024428411 0.1820396 0.08601739 0.51038174 0.5080746 1.7224961 0 -2213.337 0.49199582 -2212.8266 1 -2213.3347
30 0.043288796 0.0068108825 0.017372479 0.043288796 0.049466709 0.51032316 0.5095943 1.7304745 0 -2213.3371 0.49553568 -2212.8268 1 -2213.3364
40 0.042139305 0.0037035764 0.01173707 0.042139305 0.026104735 0.51022733 0.5100163 1.7366752 0 -2213.3373 0.49838067 -2212.8271 1 -2213.3371
50 0.025899631 0.0022805513 0.0081057075 0.025899631 0.016908929 0.5101712 0.51008591 1.739143 0 -2213.3373 0.49923345 -2212.8272 1 -2213.3373
59 0.0096285044 0.0012946258 0.0056576061 0.0093678253 0.012040919 0.51014185 0.51010207 1.7404554 0 -2213.3374 0.49955698 -2212.8272 1 -2213.3373
Climbing replica = 2
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
59 0.012040919 0.0031505771 0.0056576061 0.0093678253 0.012040919 0.51014185 0.51010207 1.7404554 0 -2213.3374 0.49955698 -2212.8272 1 -2213.3373
63 0.0091523813 0.0016692845 0.0049647607 0.0081998372 0.0091523813 0.51013743 0.51010775 1.7409028 0 -2213.3374 0.50022236 -2212.8272 1 -2213.3373

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@ -1,14 +0,0 @@
LAMMPS (5 Oct 2016)
Running on 3 partitions of processors
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
0 7.5525391 1.6345605 0.16683659 7.5525391 7.5525391 1.5383951 0 1.6207355 0 -2213.3343 0.5 -2212.4096 1 -2211.7959
10 0.27332818 0.040944923 0.039164338 0.27332818 0.17804882 0.51235911 0.497084 1.6790474 0 -2213.3364 0.49024121 -2212.824 1 -2213.3211
20 0.1820396 0.018049916 0.024428411 0.1820396 0.08601739 0.51038174 0.5080746 1.7224961 0 -2213.337 0.49199582 -2212.8266 1 -2213.3347
30 0.043288796 0.0068108825 0.017372479 0.043288796 0.049466709 0.51032316 0.5095943 1.7304745 0 -2213.3371 0.49553568 -2212.8268 1 -2213.3364
40 0.042139318 0.0037035773 0.011737071 0.042139318 0.026104737 0.51022733 0.5100163 1.7366752 0 -2213.3373 0.49838067 -2212.8271 1 -2213.3371
50 0.025904121 0.0022808707 0.0081058431 0.025904121 0.016908969 0.5101712 0.51008591 1.7391431 0 -2213.3373 0.49923346 -2212.8272 1 -2213.3373
59 0.0096287928 0.0012946716 0.005657861 0.0093731008 0.01204121 0.51014185 0.51010207 1.7404554 0 -2213.3374 0.49955696 -2212.8272 1 -2213.3373
Climbing replica = 2
Step MaxReplicaForce MaxAtomForce GradV0 GradV1 GradVc EBF EBR RDT RD1 PE1 RD2 PE2 ... RDN PEN
59 0.01204121 0.0031506449 0.005657861 0.0093731008 0.01204121 0.51014185 0.51010207 1.7404554 0 -2213.3374 0.49955696 -2212.8272 1 -2213.3373
63 0.0091530442 0.0016693787 0.0049652227 0.0082075097 0.0091530442 0.51013743 0.51010775 1.7409027 0 -2213.3374 0.50022228 -2212.8272 1 -2213.3373

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@ -8,8 +8,8 @@ twojmax 6
# optional
gamma 1
rfac0 0.99363
rmin0 0
diagonalstyle 3
bzeroflag 0
quadraticflag 0

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@ -5,7 +5,7 @@ variable zblcutinner equal 4
variable zblcutouter equal 4.8
variable zblz equal 74
# Specify hybrid with SNAP, ZBL, and long-range Coulomb
# Specify hybrid with SNAP and ZBL
pair_style hybrid/overlay &
zbl ${zblcutinner} ${zblcutouter} &

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@ -6,8 +6,8 @@ twojmax 8
# optional
gamma 1
rfac0 0.99363
rmin0 0
diagonalstyle 3
bzeroflag 0
quadraticflag 0

View File

@ -5,7 +5,7 @@ variable zblcutinner equal 4
variable zblcutouter equal 4.8
variable zblz equal 74
# Specify hybrid with SNAP, ZBL, and long-range Coulomb
# Specify hybrid with SNAP and ZBL
pair_style hybrid/overlay zbl ${zblcutinner} ${zblcutouter} snap table spline 10000 table spline 10000
pair_coeff 1 1 zbl ${zblz} ${zblz}

View File

@ -8,7 +8,6 @@
EXTRAMAKE = Makefile.lammps.standard
CUDA_HOME = /usr/local/cuda
CUDA_HOME = /home/projects/openmpi/1.8.1/intel/13.1.SP1.106/cuda/6.0.37
NVCC = nvcc
# Kepler CUDA

View File

@ -63,6 +63,7 @@ OBJS = $(OBJ_DIR)/lal_atom.o $(OBJ_DIR)/lal_ans.o \
$(OBJ_DIR)/lal_lj_coul_debye.o $(OBJ_DIR)/lal_lj_coul_debye_ext.o \
$(OBJ_DIR)/lal_coul_dsf.o $(OBJ_DIR)/lal_coul_dsf_ext.o \
$(OBJ_DIR)/lal_sw.o $(OBJ_DIR)/lal_sw_ext.o \
$(OBJ_DIR)/lal_vashishta.o $(OBJ_DIR)/lal_vashishta_ext.o \
$(OBJ_DIR)/lal_beck.o $(OBJ_DIR)/lal_beck_ext.o \
$(OBJ_DIR)/lal_mie.o $(OBJ_DIR)/lal_mie_ext.o \
$(OBJ_DIR)/lal_soft.o $(OBJ_DIR)/lal_soft_ext.o \
@ -117,6 +118,7 @@ CBNS = $(OBJ_DIR)/device.cubin $(OBJ_DIR)/device_cubin.h \
$(OBJ_DIR)/lj_coul_debye.cubin $(OBJ_DIR)/lj_coul_debye_cubin.h \
$(OBJ_DIR)/coul_dsf.cubin $(OBJ_DIR)/coul_dsf_cubin.h \
$(OBJ_DIR)/sw.cubin $(OBJ_DIR)/sw_cubin.h \
$(OBJ_DIR)/vashishta.cubin $(OBJ_DIR)/vashishta_cubin.h \
$(OBJ_DIR)/beck.cubin $(OBJ_DIR)/beck_cubin.h \
$(OBJ_DIR)/mie.cubin $(OBJ_DIR)/mie_cubin.h \
$(OBJ_DIR)/soft.cubin $(OBJ_DIR)/soft_cubin.h \
@ -613,6 +615,18 @@ $(OBJ_DIR)/lal_coul_dsf.o: $(ALL_H) lal_coul_dsf.h lal_coul_dsf.cpp $(OBJ_DIR)/c
$(OBJ_DIR)/lal_coul_dsf_ext.o: $(ALL_H) lal_coul_dsf.h lal_coul_dsf_ext.cpp lal_base_charge.h
$(CUDR) -o $@ -c lal_coul_dsf_ext.cpp -I$(OBJ_DIR)
$(OBJ_DIR)/vashishta.cubin: lal_vashishta.cu lal_precision.h lal_preprocessor.h
$(CUDA) --cubin -DNV_KERNEL -o $@ lal_vashishta.cu
$(OBJ_DIR)/vashishta_cubin.h: $(OBJ_DIR)/vashishta.cubin $(OBJ_DIR)/vashishta.cubin
$(BIN2C) -c -n vashishta $(OBJ_DIR)/vashishta.cubin > $(OBJ_DIR)/vashishta_cubin.h
$(OBJ_DIR)/lal_vashishta.o: $(ALL_H) lal_vashishta.h lal_vashishta.cpp $(OBJ_DIR)/vashishta_cubin.h $(OBJ_DIR)/lal_base_three.o
$(CUDR) -o $@ -c lal_vashishta.cpp -I$(OBJ_DIR)
$(OBJ_DIR)/lal_vashishta_ext.o: $(ALL_H) lal_vashishta.h lal_vashishta_ext.cpp lal_base_three.h
$(CUDR) -o $@ -c lal_vashishta_ext.cpp -I$(OBJ_DIR)
$(OBJ_DIR)/sw.cubin: lal_sw.cu lal_precision.h lal_preprocessor.h
$(CUDA) --cubin -DNV_KERNEL -o $@ lal_sw.cu

View File

@ -52,6 +52,7 @@ OBJS = $(OBJ_DIR)/lal_atom.o $(OBJ_DIR)/lal_answer.o \
$(OBJ_DIR)/lal_lj_coul_debye.o $(OBJ_DIR)/lal_lj_coul_debye_ext.o \
$(OBJ_DIR)/lal_coul_dsf.o $(OBJ_DIR)/lal_coul_dsf_ext.o \
$(OBJ_DIR)/lal_sw.o $(OBJ_DIR)/lal_sw_ext.o \
$(OBJ_DIR)/lal_vashishta.o $(OBJ_DIR)/lal_vashishta_ext.o \
$(OBJ_DIR)/lal_beck.o $(OBJ_DIR)/lal_beck_ext.o \
$(OBJ_DIR)/lal_mie.o $(OBJ_DIR)/lal_mie_ext.o \
$(OBJ_DIR)/lal_soft.o $(OBJ_DIR)/lal_soft_ext.o \
@ -92,7 +93,7 @@ KERS = $(OBJ_DIR)/device_cl.h $(OBJ_DIR)/atom_cl.h \
$(OBJ_DIR)/tersoff_cl.h $(OBJ_DIR)/tersoff_zbl_cl.h \
$(OBJ_DIR)/tersoff_mod_cl.h $(OBJ_DIR)/coul_cl.h \
$(OBJ_DIR)/coul_debye_cl.h $(OBJ_DIR)/zbl_cl.h \
$(OBJ_DIR)/lj_cubic_cl.h
$(OBJ_DIR)/lj_cubic_cl.h $(OBJ_DIR)/vashishta_cl.h
OCL_EXECS = $(BIN_DIR)/ocl_get_devices
@ -450,6 +451,15 @@ $(OBJ_DIR)/lal_sw.o: $(ALL_H) lal_sw.h lal_sw.cpp $(OBJ_DIR)/sw_cl.h $(OBJ_DIR)
$(OBJ_DIR)/lal_sw_ext.o: $(ALL_H) lal_sw.h lal_sw_ext.cpp lal_base_three.h
$(OCL) -o $@ -c lal_sw_ext.cpp -I$(OBJ_DIR)
$(OBJ_DIR)/vashishta_cl.h: lal_vashishta.cu $(PRE1_H)
$(BSH) ./geryon/file_to_cstr.sh vashishta $(PRE1_H) lal_vashishta.cu $(OBJ_DIR)/vashishta_cl.h;
$(OBJ_DIR)/lal_vashishta.o: $(ALL_H) lal_vashishta.h lal_vashishta.cpp $(OBJ_DIR)/vashishta_cl.h $(OBJ_DIR)/vashishta_cl.h $(OBJ_DIR)/lal_base_three.o
$(OCL) -o $@ -c lal_vashishta.cpp -I$(OBJ_DIR)
$(OBJ_DIR)/lal_vashishta_ext.o: $(ALL_H) lal_vashishta.h lal_vashishta_ext.cpp lal_base_three.h
$(OCL) -o $@ -c lal_vashishta_ext.cpp -I$(OBJ_DIR)
$(OBJ_DIR)/beck_cl.h: lal_beck.cu $(PRE1_H)
$(BSH) ./geryon/file_to_cstr.sh beck $(PRE1_H) lal_beck.cu $(OBJ_DIR)/beck_cl.h;

283
lib/gpu/lal_vashishta.cpp Normal file
View File

@ -0,0 +1,283 @@
/***************************************************************************
vashishta.cpp
-------------------
Anders Hafreager (UiO)
Class for acceleration of the vashishta pair style.
__________________________________________________________________________
This file is part of the LAMMPS Accelerator Library (LAMMPS_AL)
__________________________________________________________________________
begin : Mon June 12, 2017
email : andershaf@gmail.com
***************************************************************************/
#if defined(USE_OPENCL)
#include "vashishta_cl.h"
#elif defined(USE_CUDART)
const char *vashishta=0;
#else
#include "vashishta_cubin.h"
#endif
#include "lal_vashishta.h"
#include <cassert>
using namespace LAMMPS_AL;
#define VashishtaT Vashishta<numtyp, acctyp>
extern Device<PRECISION,ACC_PRECISION> device;
template <class numtyp, class acctyp>
VashishtaT::Vashishta() : BaseThree<numtyp,acctyp>(), _allocated(false) {
}
template <class numtyp, class acctyp>
VashishtaT::~Vashishta() {
clear();
}
template <class numtyp, class acctyp>
int VashishtaT::bytes_per_atom(const int max_nbors) const {
return this->bytes_per_atom_atomic(max_nbors);
}
template <class numtyp, class acctyp>
int VashishtaT::init(const int ntypes, const int nlocal, const int nall, const int max_nbors,
const double cell_size, const double gpu_split, FILE *_screen,
int* host_map, const int nelements, int*** host_elem2param, const int nparams,
const double* cutsq, const double* r0,
const double* gamma, const double* eta,
const double* lam1inv, const double* lam4inv,
const double* zizj, const double* mbigd,
const double* dvrc, const double* big6w,
const double* heta, const double* bigh,
const double* bigw, const double* c0,
const double* costheta, const double* bigb,
const double* big2b, const double* bigc)
{
int success;
success=this->init_three(nlocal,nall,max_nbors,0,cell_size,gpu_split,
_screen,vashishta,"k_vashishta","k_vashishta_three_center",
"k_vashishta_three_end");
if (success!=0)
return success;
// If atom type constants fit in shared memory use fast kernel
int lj_types=ntypes;
shared_types=false;
int max_shared_types=this->device->max_shared_types();
if (lj_types<=max_shared_types && this->_block_size>=max_shared_types) {
lj_types=max_shared_types;
shared_types=true;
}
_lj_types=lj_types;
_nparams = nparams;
_nelements = nelements;
UCL_H_Vec<numtyp4> dview(nparams,*(this->ucl_device),
UCL_WRITE_ONLY);
for (int i=0; i<nparams; i++) {
dview[i].x=(numtyp)0;
dview[i].y=(numtyp)0;
dview[i].z=(numtyp)0;
dview[i].w=(numtyp)0;
}
// pack coefficients into arrays
param1.alloc(nparams,*(this->ucl_device),UCL_READ_ONLY);
for (int i=0; i<nparams; i++) {
dview[i].x=static_cast<numtyp>(eta[i]);
dview[i].y=static_cast<numtyp>(lam1inv[i]);
dview[i].z=static_cast<numtyp>(lam4inv[i]);
dview[i].w=static_cast<numtyp>(zizj[i]);
}
ucl_copy(param1,dview,false);
param1_tex.get_texture(*(this->pair_program),"param1_tex");
param1_tex.bind_float(param1,4);
param2.alloc(nparams,*(this->ucl_device),UCL_READ_ONLY);
for (int i=0; i<nparams; i++) {
dview[i].x=static_cast<numtyp>(mbigd[i]);
dview[i].y=static_cast<numtyp>(dvrc[i]);
dview[i].z=static_cast<numtyp>(big6w[i]);
dview[i].w=static_cast<numtyp>(heta[i]);
}
ucl_copy(param2,dview,false);
param2_tex.get_texture(*(this->pair_program),"param2_tex");
param2_tex.bind_float(param2,4);
param3.alloc(nparams,*(this->ucl_device),UCL_READ_ONLY);
for (int i=0; i<nparams; i++) {
dview[i].x=static_cast<numtyp>(bigh[i]);
dview[i].y=static_cast<numtyp>(bigw[i]);
dview[i].z=static_cast<numtyp>(dvrc[i]);
dview[i].w=static_cast<numtyp>(c0[i]);
}
ucl_copy(param3,dview,false);
param3_tex.get_texture(*(this->pair_program),"param3_tex");
param3_tex.bind_float(param3,4);
param4.alloc(nparams,*(this->ucl_device),UCL_READ_ONLY);
for (int i=0; i<nparams; i++) {
double r0sq = r0[i]*r0[i]-1e-4; // TODO: should we have the 1e-4?
dview[i].x=static_cast<numtyp>(r0sq);
dview[i].y=static_cast<numtyp>(gamma[i]);
dview[i].z=static_cast<numtyp>(cutsq[i]);
dview[i].w=static_cast<numtyp>(r0[i]);
}
ucl_copy(param4,dview,false);
param4_tex.get_texture(*(this->pair_program),"param4_tex");
param4_tex.bind_float(param4,4);
param5.alloc(nparams,*(this->ucl_device),UCL_READ_ONLY);
for (int i=0; i<nparams; i++) {
dview[i].x=static_cast<numtyp>(bigc[i]);
dview[i].y=static_cast<numtyp>(costheta[i]);
dview[i].z=static_cast<numtyp>(bigb[i]);
dview[i].w=static_cast<numtyp>(big2b[i]);
}
ucl_copy(param5,dview,false);
param5_tex.get_texture(*(this->pair_program),"param5_tex");
param5_tex.bind_float(param5,4);
UCL_H_Vec<int> dview_elem2param(nelements*nelements*nelements,
*(this->ucl_device), UCL_WRITE_ONLY);
elem2param.alloc(nelements*nelements*nelements,*(this->ucl_device),
UCL_READ_ONLY);
for (int i = 0; i < nelements; i++)
for (int j = 0; j < nelements; j++)
for (int k = 0; k < nelements; k++) {
int idx = i*nelements*nelements+j*nelements+k;
dview_elem2param[idx] = host_elem2param[i][j][k];
}
ucl_copy(elem2param,dview_elem2param,false);
UCL_H_Vec<int> dview_map(lj_types, *(this->ucl_device), UCL_WRITE_ONLY);
for (int i = 0; i < ntypes; i++)
dview_map[i] = host_map[i];
map.alloc(lj_types,*(this->ucl_device), UCL_READ_ONLY);
ucl_copy(map,dview_map,false);
_allocated=true;
this->_max_bytes=param1.row_bytes()+param2.row_bytes()+param3.row_bytes()+param4.row_bytes()+param5.row_bytes()+
map.row_bytes()+elem2param.row_bytes();
return 0;
}
template <class numtyp, class acctyp>
void VashishtaT::clear() {
if (!_allocated)
return;
_allocated=false;
param1.clear();
param2.clear();
param3.clear();
param4.clear();
param5.clear();
map.clear();
elem2param.clear();
this->clear_atomic();
}
template <class numtyp, class acctyp>
double VashishtaT::host_memory_usage() const {
return this->host_memory_usage_atomic()+sizeof(Vashishta<numtyp,acctyp>);
}
#define KTHREADS this->_threads_per_atom
#define JTHREADS this->_threads_per_atom
// ---------------------------------------------------------------------------
// Calculate energies, forces, and torques
// ---------------------------------------------------------------------------
template <class numtyp, class acctyp>
void VashishtaT::loop(const bool _eflag, const bool _vflag, const int evatom) {
// Compute the block size and grid size to keep all cores busy
int BX=this->block_pair();
int eflag, vflag;
if (_eflag)
eflag=1;
else
eflag=0;
if (_vflag)
vflag=1;
else
vflag=0;
int GX=static_cast<int>(ceil(static_cast<double>(this->ans->inum())/
(BX/this->_threads_per_atom)));
// this->_nbor_data == nbor->dev_packed for gpu_nbor == 0 and tpa > 1
// this->_nbor_data == nbor->dev_nbor for gpu_nbor == 1 or tpa == 1
int ainum=this->ans->inum();
int nbor_pitch=this->nbor->nbor_pitch();
this->time_pair.start();
this->k_pair.set_size(GX,BX);
this->k_pair.run(&this->atom->x, &param1, &param2, &param3, &param4, &param5,
&map, &elem2param, &_nelements,
&this->nbor->dev_nbor, &this->_nbor_data->begin(),
&this->ans->force, &this->ans->engv,
&eflag, &vflag, &ainum, &nbor_pitch,
&this->_threads_per_atom);
BX=this->block_size();
GX=static_cast<int>(ceil(static_cast<double>(this->ans->inum())/
(BX/(KTHREADS*JTHREADS))));
this->k_three_center.set_size(GX,BX);
this->k_three_center.run(&this->atom->x, &param1, &param2, &param3, &param4, &param5,
&map, &elem2param, &_nelements,
&this->nbor->dev_nbor, &this->_nbor_data->begin(),
&this->ans->force, &this->ans->engv, &eflag, &vflag, &ainum,
&nbor_pitch, &this->_threads_per_atom, &evatom);
Answer<numtyp,acctyp> *end_ans;
#ifdef THREE_CONCURRENT
end_ans=this->ans2;
#else
end_ans=this->ans;
#endif
if (evatom!=0) {
this->k_three_end_vatom.set_size(GX,BX);
this->k_three_end_vatom.run(&this->atom->x, &param1, &param2, &param3, &param4, &param5,
&map, &elem2param, &_nelements,
&this->nbor->dev_nbor, &this->_nbor_data->begin(),
&this->nbor->dev_acc,
&end_ans->force, &end_ans->engv, &eflag, &vflag, &ainum,
&nbor_pitch, &this->_threads_per_atom, &this->_gpu_nbor);
} else {
this->k_three_end.set_size(GX,BX);
this->k_three_end.run(&this->atom->x, &param1, &param2, &param3, &param4, &param5,
&map, &elem2param, &_nelements,
&this->nbor->dev_nbor, &this->_nbor_data->begin(),
&this->nbor->dev_acc,
&end_ans->force, &end_ans->engv, &eflag, &vflag, &ainum,
&nbor_pitch, &this->_threads_per_atom, &this->_gpu_nbor);
}
this->time_pair.stop();
}
template class Vashishta<PRECISION,ACC_PRECISION>;

744
lib/gpu/lal_vashishta.cu Normal file
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@ -0,0 +1,744 @@
// **************************************************************************
// vashishta.cu
// -------------------
// Anders Hafreager (UiO)
//
// Device code for acceleration of the vashishta pair style
//
// __________________________________________________________________________
// This file is part of the LAMMPS Accelerator Library (LAMMPS_AL)
// __________________________________________________________________________
//
// begin : Mon June 12, 2017
// email : andershaf@gmail.com
// ***************************************************************************/
#ifdef NV_KERNEL
#include "lal_aux_fun1.h"
#ifndef _DOUBLE_DOUBLE
texture<float4> pos_tex;
texture<float4> param1_tex;
texture<float4> param2_tex;
texture<float4> param3_tex;
texture<float4> param4_tex;
texture<float4> param5_tex;
#else
texture<int4,1> pos_tex;
texture<int4> param1_tex;
texture<int4> param2_tex;
texture<int4> param3_tex;
texture<int4> param4_tex;
texture<int4> param5_tex;
#endif
#else
#define pos_tex x_
#define param1_tex param1
#define param2_tex param2
#define param3_tex param3
#define param4_tex param4
#define param5_tex param5
#endif
#define THIRD (numtyp)0.66666666666666666667
//#define THREE_CONCURRENT
#if (ARCH < 300)
#define store_answers_p(f, energy, virial, ii, inum, tid, t_per_atom, offset, \
eflag, vflag, ans, engv) \
if (t_per_atom>1) { \
__local acctyp red_acc[6][BLOCK_ELLIPSE]; \
red_acc[0][tid]=f.x; \
red_acc[1][tid]=f.y; \
red_acc[2][tid]=f.z; \
red_acc[3][tid]=energy; \
for (unsigned int s=t_per_atom/2; s>0; s>>=1) { \
if (offset < s) { \
for (int r=0; r<4; r++) \
red_acc[r][tid] += red_acc[r][tid+s]; \
} \
} \
f.x=red_acc[0][tid]; \
f.y=red_acc[1][tid]; \
f.z=red_acc[2][tid]; \
energy=red_acc[3][tid]; \
if (vflag>0) { \
for (int r=0; r<6; r++) \
red_acc[r][tid]=virial[r]; \
for (unsigned int s=t_per_atom/2; s>0; s>>=1) { \
if (offset < s) { \
for (int r=0; r<6; r++) \
red_acc[r][tid] += red_acc[r][tid+s]; \
} \
} \
for (int r=0; r<6; r++) \
virial[r]=red_acc[r][tid]; \
} \
} \
if (offset==0) { \
int ei=ii; \
if (eflag>0) { \
engv[ei]+=energy*(acctyp)0.5; \
ei+=inum; \
} \
if (vflag>0) { \
for (int i=0; i<6; i++) { \
engv[ei]+=virial[i]*(acctyp)0.5; \
ei+=inum; \
} \
} \
acctyp4 old=ans[ii]; \
old.x+=f.x; \
old.y+=f.y; \
old.z+=f.z; \
ans[ii]=old; \
}
#else
#define store_answers_p(f, energy, virial, ii, inum, tid, t_per_atom, offset, \
eflag, vflag, ans, engv) \
if (t_per_atom>1) { \
for (unsigned int s=t_per_atom/2; s>0; s>>=1) { \
f.x += shfl_xor(f.x, s, t_per_atom); \
f.y += shfl_xor(f.y, s, t_per_atom); \
f.z += shfl_xor(f.z, s, t_per_atom); \
energy += shfl_xor(energy, s, t_per_atom); \
} \
if (vflag>0) { \
for (unsigned int s=t_per_atom/2; s>0; s>>=1) { \
for (int r=0; r<6; r++) \
virial[r] += shfl_xor(virial[r], s, t_per_atom); \
} \
} \
} \
if (offset==0) { \
int ei=ii; \
if (eflag>0) { \
engv[ei]+=energy*(acctyp)0.5; \
ei+=inum; \
} \
if (vflag>0) { \
for (int i=0; i<6; i++) { \
engv[ei]+=virial[i]*(acctyp)0.5; \
ei+=inum; \
} \
} \
acctyp4 old=ans[ii]; \
old.x+=f.x; \
old.y+=f.y; \
old.z+=f.z; \
ans[ii]=old; \
}
#endif
__kernel void k_vashishta(const __global numtyp4 *restrict x_,
const __global numtyp4 *restrict param1,
const __global numtyp4 *restrict param2,
const __global numtyp4 *restrict param3,
const __global numtyp4 *restrict param4,
const __global numtyp4 *restrict param5,
const __global int *restrict map,
const __global int *restrict elem2param,
const int nelements,
const __global int * dev_nbor,
const __global int * dev_packed,
__global acctyp4 *restrict ans,
__global acctyp *restrict engv,
const int eflag, const int vflag, const int inum,
const int nbor_pitch, const int t_per_atom) {
__local int n_stride;
int tid, ii, offset;
atom_info(t_per_atom,ii,tid,offset);
acctyp energy=(acctyp)0;
acctyp4 f;
f.x=(acctyp)0; f.y=(acctyp)0; f.z=(acctyp)0;
acctyp virial[6];
for (int i=0; i<6; i++)
virial[i]=(acctyp)0;
__syncthreads();
if (ii<inum) {
int nbor, nbor_end;
int i, numj;
nbor_info(dev_nbor,dev_packed,nbor_pitch,t_per_atom,ii,offset,i,numj,
n_stride,nbor_end,nbor);
numtyp4 ix; fetch4(ix,i,pos_tex); //x_[i];
int itype=ix.w;
itype=map[itype];
for ( ; nbor<nbor_end; nbor+=n_stride) {
int j=dev_packed[nbor];
j &= NEIGHMASK;
numtyp4 jx; fetch4(jx,j,pos_tex); //x_[j];
int jtype=jx.w;
jtype=map[jtype];
int ijparam=elem2param[itype*nelements*nelements+jtype*nelements+jtype];
// Compute r12
numtyp delx = ix.x-jx.x;
numtyp dely = ix.y-jx.y;
numtyp delz = ix.z-jx.z;
numtyp rsq = delx*delx+dely*dely+delz*delz;
if (rsq<param4[ijparam].z) { // cutsq = param4[ijparam].z
numtyp4 param1_ijparam; fetch4(param1_ijparam,ijparam,param1_tex);
numtyp param1_eta=param1_ijparam.x;
numtyp param1_lam1inv=param1_ijparam.y;
numtyp param1_lam4inv=param1_ijparam.z;
numtyp param1_zizj=param1_ijparam.w;
numtyp4 param2_ijparam; fetch4(param2_ijparam,ijparam,param2_tex);
numtyp param2_mbigd=param2_ijparam.x;
numtyp param2_dvrc =param2_ijparam.y;
numtyp param2_big6w=param2_ijparam.z;
numtyp param2_heta =param2_ijparam.w;
numtyp4 param3_ijparam; fetch4(param3_ijparam,ijparam,param3_tex);
numtyp param3_bigh=param3_ijparam.x;
numtyp param3_bigw=param3_ijparam.y;
numtyp param3_dvrc=param3_ijparam.z;
numtyp param3_c0 =param3_ijparam.w;
numtyp r=sqrt(rsq);
numtyp rinvsq=1.0/rsq;
numtyp r4inv = rinvsq*rinvsq;
numtyp r6inv = rinvsq*r4inv;
numtyp reta = pow(r,-param1_eta);
numtyp lam1r = r*param1_lam1inv;
numtyp lam4r = r*param1_lam4inv;
numtyp vc2 = param1_zizj * exp(-lam1r)/r;
numtyp vc3 = param2_mbigd * r4inv*exp(-lam4r);
numtyp force = (param2_dvrc*r
- (4.0*vc3 + lam4r*vc3+param2_big6w*r6inv
- param2_heta*reta - vc2 - lam1r*vc2)
) * rinvsq;
f.x+=delx*force;
f.y+=dely*force;
f.z+=delz*force;
if (eflag>0)
energy += (param3_bigh*reta+vc2-vc3-param3_bigw*r6inv-r*param3_dvrc+param3_c0);
if (vflag>0) {
virial[0] += delx*delx*force;
virial[1] += dely*dely*force;
virial[2] += delz*delz*force;
virial[3] += delx*dely*force;
virial[4] += delx*delz*force;
virial[5] += dely*delz*force;
}
}
} // for nbor
store_answers(f,energy,virial,ii,inum,tid,t_per_atom,offset,eflag,vflag,
ans,engv);
} // if ii
}
#define threebody(delr1x, delr1y, delr1z, eflag, energy) \
{ \
numtyp r1 = ucl_sqrt(rsq1); \
numtyp rinvsq1 = ucl_recip(rsq1); \
numtyp rainv1 = ucl_recip(r1 - param_r0_ij); \
numtyp gsrainv1 = param_gamma_ij * rainv1; \
numtyp gsrainvsq1 = gsrainv1*rainv1/r1; \
numtyp expgsrainv1 = ucl_exp(gsrainv1); \
\
numtyp r2 = ucl_sqrt(rsq2); \
numtyp rinvsq2 = ucl_recip(rsq2); \
numtyp rainv2 = ucl_recip(r2 - param_r0_ik); \
numtyp gsrainv2 = param_gamma_ik * rainv2; \
numtyp gsrainvsq2 = gsrainv2*rainv2/r2; \
numtyp expgsrainv2 = ucl_exp(gsrainv2); \
\
numtyp rinv12 = ucl_recip(r1*r2); \
numtyp cs = (delr1x*delr2x + delr1y*delr2y + delr1z*delr2z) * rinv12; \
numtyp delcs = cs - param_costheta_ijk; \
numtyp delcssq = delcs*delcs; \
numtyp pcsinv = param_bigc_ijk*delcssq+1.0; \
numtyp pcsinvsq = pcsinv*pcsinv; \
numtyp pcs = delcssq/pcsinv; \
\
numtyp facexp = expgsrainv1*expgsrainv2; \
\
numtyp facrad = param_bigb_ijk * facexp*pcs; \
numtyp frad1 = facrad*gsrainvsq1; \
numtyp frad2 = facrad*gsrainvsq2; \
numtyp facang = param_big2b_ijk * facexp*delcs/pcsinvsq; \
numtyp facang12 = rinv12*facang; \
numtyp csfacang = cs*facang; \
numtyp csfac1 = rinvsq1*csfacang; \
\
fjx = delr1x*(frad1+csfac1)-delr2x*facang12; \
fjy = delr1y*(frad1+csfac1)-delr2y*facang12; \
fjz = delr1z*(frad1+csfac1)-delr2z*facang12; \
\
numtyp csfac2 = rinvsq2*csfacang; \
\
fkx = delr2x*(frad2+csfac2)-delr1x*facang12; \
fky = delr2y*(frad2+csfac2)-delr1y*facang12; \
fkz = delr2z*(frad2+csfac2)-delr1z*facang12; \
\
if (eflag>0) \
energy+=facrad; \
if (vflag>0) { \
virial[0] += delr1x*fjx + delr2x*fkx; \
virial[1] += delr1y*fjy + delr2y*fky; \
virial[2] += delr1z*fjz + delr2z*fkz; \
virial[3] += delr1x*fjy + delr2x*fky; \
virial[4] += delr1x*fjz + delr2x*fkz; \
virial[5] += delr1y*fjz + delr2y*fkz; \
} \
}
#define threebody_half(delr1x, delr1y, delr1z) \
{ \
numtyp r1 = ucl_sqrt(rsq1); \
numtyp rinvsq1 = ucl_recip(rsq1); \
numtyp rainv1 = ucl_recip(r1 - param_r0_ij); \
numtyp gsrainv1 = param_gamma_ij * rainv1; \
numtyp gsrainvsq1 = gsrainv1*rainv1/r1; \
numtyp expgsrainv1 = ucl_exp(gsrainv1); \
\
numtyp r2 = ucl_sqrt(rsq2); \
numtyp rainv2 = ucl_recip(r2 - param_r0_ik); \
numtyp gsrainv2 = param_gamma_ik * rainv2; \
numtyp expgsrainv2 = ucl_exp(gsrainv2); \
\
numtyp rinv12 = ucl_recip(r1*r2); \
numtyp cs = (delr1x*delr2x + delr1y*delr2y + delr1z*delr2z) * rinv12; \
numtyp delcs = cs - param_costheta_ijk; \
numtyp delcssq = delcs*delcs; \
numtyp pcsinv = param_bigc_ijk*delcssq+1.0; \
numtyp pcsinvsq = pcsinv*pcsinv; \
numtyp pcs = delcssq/pcsinv; \
\
numtyp facexp = expgsrainv1*expgsrainv2; \
\
numtyp facrad = param_bigb_ijk * facexp*pcs; \
numtyp frad1 = facrad*gsrainvsq1; \
numtyp facang = param_big2b_ijk * facexp*delcs/pcsinvsq; \
numtyp facang12 = rinv12*facang; \
numtyp csfacang = cs*facang; \
numtyp csfac1 = rinvsq1*csfacang; \
\
fjx = delr1x*(frad1+csfac1)-delr2x*facang12; \
fjy = delr1y*(frad1+csfac1)-delr2y*facang12; \
fjz = delr1z*(frad1+csfac1)-delr2z*facang12; \
}
__kernel void k_vashishta_three_center(const __global numtyp4 *restrict x_,
const __global numtyp4 *restrict param1,
const __global numtyp4 *restrict param2,
const __global numtyp4 *restrict param3,
const __global numtyp4 *restrict param4,
const __global numtyp4 *restrict param5,
const __global int *restrict map,
const __global int *restrict elem2param,
const int nelements,
const __global int * dev_nbor,
const __global int * dev_packed,
__global acctyp4 *restrict ans,
__global acctyp *restrict engv,
const int eflag, const int vflag,
const int inum, const int nbor_pitch,
const int t_per_atom, const int evatom) {
__local int tpa_sq, n_stride;
tpa_sq=fast_mul(t_per_atom,t_per_atom);
numtyp param_gamma_ij, param_r0sq_ij, param_r0_ij, param_gamma_ik, param_r0sq_ik, param_r0_ik;
numtyp param_costheta_ijk, param_bigc_ijk, param_bigb_ijk, param_big2b_ijk;
int tid, ii, offset;
atom_info(tpa_sq,ii,tid,offset);
acctyp energy=(acctyp)0;
acctyp4 f;
f.x=(acctyp)0; f.y=(acctyp)0; f.z=(acctyp)0;
acctyp virial[6];
for (int i=0; i<6; i++)
virial[i]=(acctyp)0;
__syncthreads();
if (ii<inum) {
int i, numj, nbor_j, nbor_end;
int offset_j=offset/t_per_atom;
nbor_info(dev_nbor,dev_packed,nbor_pitch,t_per_atom,ii,offset_j,i,numj,
n_stride,nbor_end,nbor_j);
int offset_k=tid & (t_per_atom-1);
numtyp4 ix; fetch4(ix,i,pos_tex); //x_[i];
int itype=ix.w;
itype=map[itype];
for ( ; nbor_j<nbor_end; nbor_j+=n_stride) {
int j=dev_packed[nbor_j];
j &= NEIGHMASK;
numtyp4 jx; fetch4(jx,j,pos_tex); //x_[j];
int jtype=jx.w;
jtype=map[jtype];
// Compute r12
numtyp delr1x = jx.x-ix.x;
numtyp delr1y = jx.y-ix.y;
numtyp delr1z = jx.z-ix.z;
numtyp rsq1 = delr1x*delr1x+delr1y*delr1y+delr1z*delr1z;
int ijparam=elem2param[itype*nelements*nelements+jtype*nelements+jtype];
numtyp4 param4_ijparam; fetch4(param4_ijparam,ijparam,param4_tex);
param_r0sq_ij=param4_ijparam.x;
if (rsq1 > param_r0sq_ij) continue;
param_gamma_ij=param4_ijparam.y;
param_r0_ij=param4_ijparam.w;
int nbor_k=nbor_j-offset_j+offset_k;
if (nbor_k<=nbor_j)
nbor_k+=n_stride;
for ( ; nbor_k<nbor_end; nbor_k+=n_stride) {
int k=dev_packed[nbor_k];
k &= NEIGHMASK;
numtyp4 kx; fetch4(kx,k,pos_tex);
int ktype=kx.w;
ktype=map[ktype];
int ikparam=elem2param[itype*nelements*nelements+ktype*nelements+ktype];
numtyp4 param4_ikparam; fetch4(param4_ikparam,ikparam,param4_tex);
numtyp delr2x = kx.x-ix.x;
numtyp delr2y = kx.y-ix.y;
numtyp delr2z = kx.z-ix.z;
numtyp rsq2 = delr2x*delr2x + delr2y*delr2y + delr2z*delr2z;
param_r0sq_ik=param4_ikparam.x;
if (rsq2 < param_r0sq_ik) {
param_gamma_ik=param4_ikparam.y;
param_r0_ik=param4_ikparam.w;
int ijkparam=elem2param[itype*nelements*nelements+jtype*nelements+ktype];
numtyp4 param5_ijkparam; fetch4(param5_ijkparam,ijkparam,param5_tex);
param_bigc_ijk=param5_ijkparam.x;
param_bigb_ijk=param5_ijkparam.z;
param_big2b_ijk=param5_ijkparam.w;
param_costheta_ijk=param5_ijkparam.y;
numtyp fjx, fjy, fjz, fkx, fky, fkz;
threebody(delr1x,delr1y,delr1z,eflag,energy);
f.x -= fjx + fkx;
f.y -= fjy + fky;
f.z -= fjz + fkz;
}
}
} // for nbor
numtyp pre;
if (evatom==1)
pre=THIRD;
else
pre=(numtyp)2.0;
energy*=pre;
for (int i=0; i<6; i++)
virial[i]*=pre;
store_answers_p(f,energy,virial,ii,inum,tid,tpa_sq,offset,
eflag,vflag,ans,engv);
} // if ii
}
__kernel void k_vashishta_three_end(const __global numtyp4 *restrict x_,
const __global numtyp4 *restrict param1,
const __global numtyp4 *restrict param2,
const __global numtyp4 *restrict param3,
const __global numtyp4 *restrict param4,
const __global numtyp4 *restrict param5,
const __global int *restrict map,
const __global int *restrict elem2param,
const int nelements,
const __global int * dev_nbor,
const __global int * dev_packed,
const __global int * dev_acc,
__global acctyp4 *restrict ans,
__global acctyp *restrict engv,
const int eflag, const int vflag,
const int inum, const int nbor_pitch,
const int t_per_atom, const int gpu_nbor) {
__local int tpa_sq, n_stride;
tpa_sq=fast_mul(t_per_atom,t_per_atom);
numtyp param_gamma_ij, param_r0sq_ij, param_r0_ij, param_gamma_ik, param_r0sq_ik, param_r0_ik;
numtyp param_costheta_ijk, param_bigc_ijk, param_bigb_ijk, param_big2b_ijk;
int tid, ii, offset;
atom_info(tpa_sq,ii,tid,offset);
acctyp energy=(acctyp)0;
acctyp4 f;
f.x=(acctyp)0; f.y=(acctyp)0; f.z=(acctyp)0;
acctyp virial[6];
for (int i=0; i<6; i++)
virial[i]=(acctyp)0;
__syncthreads();
if (ii<inum) {
int i, numj, nbor_j, nbor_end, k_end;
int offset_j=offset/t_per_atom;
nbor_info(dev_nbor,dev_packed,nbor_pitch,t_per_atom,ii,offset_j,i,numj,
n_stride,nbor_end,nbor_j);
int offset_k=tid & (t_per_atom-1);
numtyp4 ix; fetch4(ix,i,pos_tex); //x_[i];
int itype=ix.w;
itype=map[itype];
for ( ; nbor_j<nbor_end; nbor_j+=n_stride) {
int j=dev_packed[nbor_j];
j &= NEIGHMASK;
numtyp4 jx; fetch4(jx,j,pos_tex); //x_[j];
int jtype=jx.w;
jtype=map[jtype];
// Compute r12
numtyp delr1x = ix.x-jx.x;
numtyp delr1y = ix.y-jx.y;
numtyp delr1z = ix.z-jx.z;
numtyp rsq1 = delr1x*delr1x+delr1y*delr1y+delr1z*delr1z;
int ijparam=elem2param[itype*nelements*nelements+jtype*nelements+jtype];
numtyp4 param4_ijparam; fetch4(param4_ijparam,ijparam,param4_tex);
param_r0sq_ij = param4_ijparam.x;
if (rsq1 > param_r0sq_ij) continue;
param_gamma_ij=param4_ijparam.y;
param_r0_ij = param4_ijparam.w;
int nbor_k,numk;
if (dev_nbor==dev_packed) {
if (gpu_nbor) nbor_k=j+nbor_pitch;
else nbor_k=dev_acc[j]+nbor_pitch;
numk=dev_nbor[nbor_k];
nbor_k+=nbor_pitch+fast_mul(j,t_per_atom-1);
k_end=nbor_k+fast_mul(numk/t_per_atom,n_stride)+(numk & (t_per_atom-1));
nbor_k+=offset_k;
} else {
nbor_k=dev_acc[j]+nbor_pitch;
numk=dev_nbor[nbor_k];
nbor_k+=nbor_pitch;
nbor_k=dev_nbor[nbor_k];
k_end=nbor_k+numk;
nbor_k+=offset_k;
}
for ( ; nbor_k<k_end; nbor_k+=n_stride) {
int k=dev_packed[nbor_k];
k &= NEIGHMASK;
if (k == i) continue;
numtyp4 kx; fetch4(kx,k,pos_tex);
int ktype=kx.w;
ktype=map[ktype];
int ikparam=elem2param[jtype*nelements*nelements+ktype*nelements+ktype]; //jk
numtyp delr2x = kx.x - jx.x;
numtyp delr2y = kx.y - jx.y;
numtyp delr2z = kx.z - jx.z;
numtyp rsq2 = delr2x*delr2x + delr2y*delr2y + delr2z*delr2z;
numtyp4 param4_ikparam; fetch4(param4_ikparam,ikparam,param4_tex);
param_r0sq_ik=param4_ikparam.x;
if (rsq2 < param_r0sq_ik) {
param_gamma_ik=param4_ikparam.y;
param_r0_ik=param4_ikparam.w;
int ijkparam=elem2param[jtype*nelements*nelements+itype*nelements+ktype]; //jik
numtyp4 param5_ijkparam; fetch4(param5_ijkparam,ijkparam,param5_tex);
param_bigc_ijk=param5_ijkparam.x;
param_costheta_ijk=param5_ijkparam.y;
param_bigb_ijk=param5_ijkparam.z;
param_big2b_ijk=param5_ijkparam.w;
numtyp fjx, fjy, fjz;
//if (evatom==0) {
threebody_half(delr1x,delr1y,delr1z);
//} else {
// numtyp fkx, fky, fkz;
// threebody(delr1x,delr1y,delr1z,eflag,energy);
//}
f.x += fjx;
f.y += fjy;
f.z += fjz;
}
}
} // for nbor
#ifdef THREE_CONCURRENT
store_answers(f,energy,virial,ii,inum,tid,tpa_sq,offset,
eflag,vflag,ans,engv);
#else
store_answers_p(f,energy,virial,ii,inum,tid,tpa_sq,offset,
eflag,vflag,ans,engv);
#endif
} // if ii
}
__kernel void k_vashishta_three_end_vatom(const __global numtyp4 *restrict x_,
const __global numtyp4 *restrict param1,
const __global numtyp4 *restrict param2,
const __global numtyp4 *restrict param3,
const __global numtyp4 *restrict param4,
const __global numtyp4 *restrict param5,
const __global int *restrict map,
const __global int *restrict elem2param,
const int nelements,
const __global int * dev_nbor,
const __global int * dev_packed,
const __global int * dev_acc,
__global acctyp4 *restrict ans,
__global acctyp *restrict engv,
const int eflag, const int vflag,
const int inum, const int nbor_pitch,
const int t_per_atom, const int gpu_nbor) {
__local int tpa_sq, n_stride;
tpa_sq=fast_mul(t_per_atom,t_per_atom);
numtyp param_gamma_ij, param_r0sq_ij, param_r0_ij, param_gamma_ik, param_r0sq_ik, param_r0_ik;
numtyp param_costheta_ijk, param_bigc_ijk, param_bigb_ijk, param_big2b_ijk;
int tid, ii, offset;
atom_info(tpa_sq,ii,tid,offset);
acctyp energy=(acctyp)0;
acctyp4 f;
f.x=(acctyp)0; f.y=(acctyp)0; f.z=(acctyp)0;
acctyp virial[6];
for (int i=0; i<6; i++)
virial[i]=(acctyp)0;
__syncthreads();
if (ii<inum) {
int i, numj, nbor_j, nbor_end, k_end;
int offset_j=offset/t_per_atom;
nbor_info(dev_nbor,dev_packed,nbor_pitch,t_per_atom,ii,offset_j,i,numj,
n_stride,nbor_end,nbor_j);
int offset_k=tid & (t_per_atom-1);
numtyp4 ix; fetch4(ix,i,pos_tex); //x_[i];
int itype=ix.w;
itype=map[itype];
for ( ; nbor_j<nbor_end; nbor_j+=n_stride) {
int j=dev_packed[nbor_j];
j &= NEIGHMASK;
numtyp4 jx; fetch4(jx,j,pos_tex); //x_[j];
int jtype=jx.w;
jtype=map[jtype];
// Compute r12
numtyp delr1x = ix.x-jx.x;
numtyp delr1y = ix.y-jx.y;
numtyp delr1z = ix.z-jx.z;
numtyp rsq1 = delr1x*delr1x+delr1y*delr1y+delr1z*delr1z;
int ijparam=elem2param[itype*nelements*nelements+jtype*nelements+jtype];
numtyp4 param4_ijparam; fetch4(param4_ijparam,ijparam,param4_tex);
param_r0sq_ij=param4_ijparam.x;
if (rsq1 > param_r0sq_ij) continue;
param_gamma_ij=param4_ijparam.y;
param_r0_ij=param4_ijparam.w;
int nbor_k,numk;
if (dev_nbor==dev_packed) {
if (gpu_nbor) nbor_k=j+nbor_pitch;
else nbor_k=dev_acc[j]+nbor_pitch;
numk=dev_nbor[nbor_k];
nbor_k+=nbor_pitch+fast_mul(j,t_per_atom-1);
k_end=nbor_k+fast_mul(numk/t_per_atom,n_stride)+(numk & (t_per_atom-1));
nbor_k+=offset_k;
} else {
nbor_k=dev_acc[j]+nbor_pitch;
numk=dev_nbor[nbor_k];
nbor_k+=nbor_pitch;
nbor_k=dev_nbor[nbor_k];
k_end=nbor_k+numk;
nbor_k+=offset_k;
}
for ( ; nbor_k<k_end; nbor_k+=n_stride) {
int k=dev_packed[nbor_k];
k &= NEIGHMASK;
if (k == i) continue;
numtyp4 kx; fetch4(kx,k,pos_tex);
int ktype=kx.w;
ktype=map[ktype];
int ikparam=elem2param[jtype*nelements*nelements+ktype*nelements+ktype]; // jk
numtyp4 param4_ikparam; fetch4(param4_ikparam,ikparam,param4_tex);
numtyp delr2x = kx.x - jx.x;
numtyp delr2y = kx.y - jx.y;
numtyp delr2z = kx.z - jx.z;
numtyp rsq2 = delr2x*delr2x + delr2y*delr2y + delr2z*delr2z;
param_r0sq_ik=param4_ikparam.x;
if (rsq2 < param_r0sq_ik) {
param_gamma_ik=param4_ikparam.y;
param_r0_ik=param4_ikparam.w;
int ijkparam=elem2param[jtype*nelements*nelements+itype*nelements+ktype]; // jik
numtyp4 param5_ijkparam; fetch4(param5_ijkparam,ijkparam,param5_tex);
param_bigc_ijk=param5_ijkparam.x;
param_costheta_ijk=param5_ijkparam.y;
param_bigb_ijk=param5_ijkparam.z;
param_big2b_ijk=param5_ijkparam.w;
numtyp fjx, fjy, fjz, fkx, fky, fkz;
threebody(delr1x,delr1y,delr1z,eflag,energy);
f.x += fjx;
f.y += fjy;
f.z += fjz;
}
}
} // for nbor
energy*=THIRD;
for (int i=0; i<6; i++)
virial[i]*=THIRD;
#ifdef THREE_CONCURRENT
store_answers(f,energy,virial,ii,inum,tid,tpa_sq,offset,
eflag,vflag,ans,engv);
#else
store_answers_p(f,energy,virial,ii,inum,tid,tpa_sq,offset,
eflag,vflag,ans,engv);
#endif
} // if ii
}

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/***************************************************************************
vashishta.h
-------------------
Anders Hafreager (UiO9)
Class for acceleration of the vashishta pair style.
__________________________________________________________________________
This file is part of the LAMMPS Accelerator Library (LAMMPS_AL)
__________________________________________________________________________
begin : Mon June 12, 2017
email : andershaf@gmail.com
***************************************************************************/
#ifndef LAL_VASHISHTA_H
#define LAL_VASHISHTA_H
#include "lal_base_three.h"
namespace LAMMPS_AL {
template <class numtyp, class acctyp>
class Vashishta : public BaseThree<numtyp, acctyp> {
public:
Vashishta();
~Vashishta();
/// Clear any previous data and set up for a new LAMMPS run
/** \param max_nbors initial number of rows in the neighbor matrix
* \param cell_size cutoff + skin
* \param gpu_split fraction of particles handled by device
*
* Returns:
* - 0 if successfull
* - -1 if fix gpu not found
* - -3 if there is an out of memory error
* - -4 if the GPU library was not compiled for GPU
* - -5 Double precision is not supported on card **/
int init(const int ntypes, const int nlocal, const int nall, const int max_nbors,
const double cell_size, const double gpu_split, FILE *screen,
int* host_map, const int nelements, int*** host_elem2param, const int nparams,
const double* cutsq, const double* r0,
const double* gamma, const double* eta,
const double* lam1inv, const double* lam4inv,
const double* zizj, const double* mbigd,
const double* dvrc, const double* big6w,
const double* heta, const double* bigh,
const double* bigw, const double* c0,
const double* costheta, const double* bigb,
const double* big2b, const double* bigc);
/// Clear all host and device data
/** \note This is called at the beginning of the init() routine **/
void clear();
/// Returns memory usage on device per atom
int bytes_per_atom(const int max_nbors) const;
/// Total host memory used by library for pair style
double host_memory_usage() const;
// --------------------------- TYPE DATA --------------------------
/// If atom type constants fit in shared memory, use fast kernels
bool shared_types;
/// Number of atom types
int _lj_types;
/// param1.x = eta, param1.y = lam1inv, param1.z = lam4inv, param1.w = zizj
UCL_D_Vec<numtyp4> param1;
/// param2.x = mbigd, param2.y = dvrc, param2.z = big6w, param2.w = heta
UCL_D_Vec<numtyp4> param2;
/// param3.x = bigh, param3.y = bigw, param3.z = dvrc, param3.w = c0
UCL_D_Vec<numtyp4> param3;
/// param4.x = r0sq, param4.y = gamma, param4.z = cutsq, param4.w = r0
UCL_D_Vec<numtyp4> param4;
/// param5.x = bigc, param5.y = costheta, param5.z = bigb, param5.w = big2b
UCL_D_Vec<numtyp4> param5;
UCL_D_Vec<int> elem2param;
UCL_D_Vec<int> map;
int _nparams,_nelements;
UCL_Texture param1_tex, param2_tex, param3_tex, param4_tex, param5_tex;
private:
bool _allocated;
void loop(const bool _eflag, const bool _vflag, const int evatom);
};
}
#endif

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@ -0,0 +1,134 @@
/***************************************************************************
vashishta_ext.cpp
-------------------
Anders Hafreager (UiO)
Class for acceleration of the vashishta pair style.
__________________________________________________________________________
This file is part of the LAMMPS Accelerator Library (LAMMPS_AL)
__________________________________________________________________________
begin : Mon June 12, 2017
email : andershaf@gmail.com
***************************************************************************/
#include <iostream>
#include <cassert>
#include <math.h>
#include "lal_vashishta.h"
using namespace LAMMPS_AL;
static Vashishta<PRECISION,ACC_PRECISION> VashishtaMF;
// ---------------------------------------------------------------------------
// Allocate memory on host and device and copy constants to device
// ---------------------------------------------------------------------------
int vashishta_gpu_init(const int ntypes, const int inum, const int nall, const int max_nbors,
const double cell_size, int &gpu_mode, FILE *screen,
int* host_map, const int nelements, int*** host_elem2param, const int nparams,
const double* cutsq, const double* r0,
const double* gamma, const double* eta,
const double* lam1inv, const double* lam4inv,
const double* zizj, const double* mbigd,
const double* dvrc, const double* big6w,
const double* heta, const double* bigh,
const double* bigw, const double* c0,
const double* costheta, const double* bigb,
const double* big2b, const double* bigc) {
VashishtaMF.clear();
gpu_mode=VashishtaMF.device->gpu_mode();
double gpu_split=VashishtaMF.device->particle_split();
int first_gpu=VashishtaMF.device->first_device();
int last_gpu=VashishtaMF.device->last_device();
int world_me=VashishtaMF.device->world_me();
int gpu_rank=VashishtaMF.device->gpu_rank();
int procs_per_gpu=VashishtaMF.device->procs_per_gpu();
// disable host/device split for now
if (gpu_split != 1.0)
return -8;
VashishtaMF.device->init_message(screen,"vashishta/gpu",first_gpu,last_gpu);
bool message=false;
if (VashishtaMF.device->replica_me()==0 && screen)
message=true;
if (message) {
fprintf(screen,"Initializing Device and compiling on process 0...");
fflush(screen);
}
int init_ok=0;
if (world_me==0)
init_ok=VashishtaMF.init(ntypes, inum, nall, 500, cell_size, gpu_split, screen,
host_map, nelements, host_elem2param, nparams,
cutsq, r0, gamma, eta, lam1inv,
lam4inv, zizj, mbigd, dvrc, big6w, heta, bigh, bigw,
c0, costheta, bigb, big2b, bigc);
VashishtaMF.device->world_barrier();
if (message)
fprintf(screen,"Done.\n");
for (int i=0; i<procs_per_gpu; i++) {
if (message) {
if (last_gpu-first_gpu==0)
fprintf(screen,"Initializing Device %d on core %d...",first_gpu,i);
else
fprintf(screen,"Initializing Devices %d-%d on core %d...",first_gpu,
last_gpu,i);
fflush(screen);
}
if (gpu_rank==i && world_me!=0)
init_ok=VashishtaMF.init(ntypes, inum, nall, 500, cell_size, gpu_split, screen,
host_map, nelements, host_elem2param, nparams,
cutsq, r0, gamma, eta, lam1inv,
lam4inv, zizj, mbigd, dvrc, big6w, heta, bigh, bigw,
c0, costheta, bigb, big2b, bigc);
VashishtaMF.device->gpu_barrier();
if (message)
fprintf(screen,"Done.\n");
}
if (message)
fprintf(screen,"\n");
if (init_ok==0)
VashishtaMF.estimate_gpu_overhead();
return init_ok;
}
void vashishta_gpu_clear() {
VashishtaMF.clear();
}
int ** vashishta_gpu_compute_n(const int ago, const int inum_full,
const int nall, double **host_x, int *host_type,
double *sublo, double *subhi, tagint *tag, int **nspecial,
tagint **special, const bool eflag, const bool vflag,
const bool eatom, const bool vatom, int &host_start,
int **ilist, int **jnum, const double cpu_time,
bool &success) {
return VashishtaMF.compute(ago, inum_full, nall, host_x, host_type, sublo,
subhi, tag, nspecial, special, eflag, vflag, eatom,
vatom, host_start, ilist, jnum, cpu_time, success);
}
void vashishta_gpu_compute(const int ago, const int nlocal, const int nall,
const int nlist, double **host_x, int *host_type,
int *ilist, int *numj, int **firstneigh, const bool eflag,
const bool vflag, const bool eatom, const bool vatom,
int &host_start, const double cpu_time, bool &success) {
VashishtaMF.compute(ago,nlocal,nall,nlist,host_x,host_type,ilist,numj,
firstneigh,eflag,vflag,eatom,vatom,host_start,cpu_time,success);
}
double vashishta_gpu_bytes() {
return VashishtaMF.host_memory_usage();
}

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@ -1,5 +1,53 @@
# Change Log
## [2.03.05](https://github.com/kokkos/kokkos/tree/2.03.05) (2017-05-27)
[Full Changelog](https://github.com/kokkos/kokkos/compare/2.03.00...2.03.05)
**Implemented enhancements:**
- Harmonize Custom Reductions over nesting levels [\#802](https://github.com/kokkos/kokkos/issues/802)
- Prevent users directly including KokkosCore\_config.h [\#815](https://github.com/kokkos/kokkos/issues/815)
- DualView aborts on concurrent host/device modify \(in debug mode\) [\#814](https://github.com/kokkos/kokkos/issues/814)
- Abort when running on a NVIDIA CC5.0 or higher architecture with code compiled for CC \< 5.0 [\#813](https://github.com/kokkos/kokkos/issues/813)
- Add "name" function to ExecSpaces [\#806](https://github.com/kokkos/kokkos/issues/806)
- Allow null Future in task spawn dependences [\#795](https://github.com/kokkos/kokkos/issues/795)
- Add Unit Tests for Kokkos::complex [\#785](https://github.com/kokkos/kokkos/issues/785)
- Add pow function for Kokkos::complex [\#784](https://github.com/kokkos/kokkos/issues/784)
- Square root of a complex [\#729](https://github.com/kokkos/kokkos/issues/729)
- Command line processing of --threads argument prevents users from having any commandline arguments starting with --threads [\#760](https://github.com/kokkos/kokkos/issues/760)
- Protected deprecated API with appropriate macro [\#756](https://github.com/kokkos/kokkos/issues/756)
- Allow task scheduler memory pool to be used by tasks [\#747](https://github.com/kokkos/kokkos/issues/747)
- View bounds checking on host-side performance: constructing a std::string [\#723](https://github.com/kokkos/kokkos/issues/723)
- Add check for AppleClang as compiler distinct from check for Clang. [\#705](https://github.com/kokkos/kokkos/issues/705)
- Uninclude source files for specific configurations to prevent link warning. [\#701](https://github.com/kokkos/kokkos/issues/701)
- Add --small option to snapshot script [\#697](https://github.com/kokkos/kokkos/issues/697)
- CMake Standalone Support [\#674](https://github.com/kokkos/kokkos/issues/674)
- CMake build unit test and install [\#808](https://github.com/kokkos/kokkos/issues/808)
- CMake: Fix having kokkos as a subdirectory in a pure cmake project [\#629](https://github.com/kokkos/kokkos/issues/629)
- Tribits macro assumes build directory is in top level source directory [\#654](https://github.com/kokkos/kokkos/issues/654)
- Use bin/nvcc\_wrapper, not config/nvcc\_wrapper [\#562](https://github.com/kokkos/kokkos/issues/562)
- Allow MemoryPool::allocate\(\) to be called from multiple threads per warp. [\#487](https://github.com/kokkos/kokkos/issues/487)
- Allow MemoryPool::allocate\\(\\) to be called from multiple threads per warp. [\#487](https://github.com/kokkos/kokkos/issues/487)
- Move OpenMP 4.5 OpenMPTarget backend into Develop [\#456](https://github.com/kokkos/kokkos/issues/456)
- Testing on ARM testbed [\#288](https://github.com/kokkos/kokkos/issues/288)
**Fixed bugs:**
- Fix label in OpenMP parallel\_reduce verify\_initialized [\#834](https://github.com/kokkos/kokkos/issues/834)
- TeamScratch Level 1 on Cuda hangs [\#820](https://github.com/kokkos/kokkos/issues/820)
- \[bug\] memory pool. [\#786](https://github.com/kokkos/kokkos/issues/786)
- Some Reduction Tests fail on Intel 18 with aggressive vectorization on [\#774](https://github.com/kokkos/kokkos/issues/774)
- Error copying dynamic view on copy of memory pool [\#773](https://github.com/kokkos/kokkos/issues/773)
- CUDA stack overflow with TaskDAG test [\#758](https://github.com/kokkos/kokkos/issues/758)
- ThreadVectorRange Customized Reduction Bug [\#739](https://github.com/kokkos/kokkos/issues/739)
- set\_scratch\_size overflows [\#726](https://github.com/kokkos/kokkos/issues/726)
- Get wrong results for compiler checks in Makefile on OS X. [\#706](https://github.com/kokkos/kokkos/issues/706)
- Fix check if multiple host architectures enabled. [\#702](https://github.com/kokkos/kokkos/issues/702)
- Threads Backend Does not Pass on Cray Compilers [\#609](https://github.com/kokkos/kokkos/issues/609)
- Rare bug in memory pool where allocation can finish on superblock in empty state [\#452](https://github.com/kokkos/kokkos/issues/452)
- LDFLAGS in core/unit\_test/Makefile: potential "undefined reference" to pthread lib [\#148](https://github.com/kokkos/kokkos/issues/148)
## [2.03.00](https://github.com/kokkos/kokkos/tree/2.03.00) (2017-04-25)
[Full Changelog](https://github.com/kokkos/kokkos/compare/2.02.15...2.03.00)

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