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Merge branch 'master' of https://www.github.com/lammps/lammps into port-enforce2d-kokkos

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This commit is contained in:
Stefan Paquay
2018-08-06 10:25:22 -04:00
parent 446a8da8e7 e88311235f
commit c1dffe40dc
1464 changed files with 168247 additions and 27758 deletions
Download Patch File Download Diff File Expand all files Collapse all files

14
.github/CODEOWNERS vendored
View File

@ -16,6 +16,8 @@ src/COMPRESS/* @akohlmey
src/GPU/* @ndtrung81
src/KOKKOS/* @stanmoore1
src/KIM/* @ellio167
src/LATTE/* @cnegre
src/SPIN/* @julient31
src/USER-CGDNA/* @ohenrich
src/USER-CGSDK/* @akohlmey
src/USER-COLVARS/* @giacomofiorin
@ -43,3 +45,15 @@ src/USER-MISC/*_grem.* @dstelter92
# tools
tools/msi2lmp/* @akohlmey
tools/emacs/* @HaoZeke
# cmake
cmake/* @junghans @rbberger
# python
python/* @rbberger
# docs
doc/utils/*/* @rbberger
doc/Makefile @rbberger
doc/README @rbberger

2
README
View File

@ -25,7 +25,7 @@ The LAMMPS distribution includes the following files and directories:
README this file
LICENSE the GNU General Public License (GPL)
bench benchmark problems
couple code coupling examples using LAMMPS as a library
cmake CMake build system
doc documentation
examples simple test problems
lib libraries LAMMPS can be linked with

490
cmake/CMakeLists.txt
View File

@ -6,11 +6,13 @@ cmake_minimum_required(VERSION 2.8.12)
project(lammps CXX)
set(SOVERSION 0)
set(LAMMPS_SOURCE_DIR ${CMAKE_CURRENT_SOURCE_DIR}/../src)
set(LAMMPS_LIB_SOURCE_DIR ${CMAKE_CURRENT_SOURCE_DIR}/../lib)
set(LAMMPS_LIB_BINARY_DIR ${CMAKE_BINARY_DIR}/lib)
get_filename_component(LAMMPS_SOURCE_DIR ${CMAKE_CURRENT_SOURCE_DIR}/../src ABSOLUTE)
get_filename_component(LAMMPS_LIB_SOURCE_DIR ${CMAKE_CURRENT_SOURCE_DIR}/../lib ABSOLUTE)
get_filename_component(LAMMPS_LIB_BINARY_DIR ${CMAKE_BINARY_DIR}/lib ABSOLUTE)
get_filename_component(LAMMPS_DOC_DIR ${CMAKE_CURRENT_SOURCE_DIR}/../doc ABSOLUTE)
#To not conflict with old Makefile build system, we build everything here
# To avoid conflicts with the conventional Makefile build system, we build everything here
file(GLOB LIB_SOURCES ${LAMMPS_SOURCE_DIR}/*.cpp)
file(GLOB LMP_SOURCES ${LAMMPS_SOURCE_DIR}/main.cpp)
list(REMOVE_ITEM LIB_SOURCES ${LMP_SOURCES})
@ -23,21 +25,23 @@ if(NOT CMAKE_BUILD_TYPE AND NOT CMAKE_CXX_FLAGS)
set(CMAKE_BUILD_TYPE Release CACHE STRING "Choose the type of build, options are: None Debug Release RelWithDebInfo MinSizeRel." FORCE)
endif(NOT CMAKE_BUILD_TYPE AND NOT CMAKE_CXX_FLAGS)
file(GLOB SRC_FILES ${LAMMPS_SOURCE_DIR}/*.cpp)
list(SORT SRC_FILES)
# check for files installed by make-based buildsystem
# only run this time consuming check if there are new files
if(NOT SRC_FILES STREQUAL SRC_FILES_CACHED)
file(GLOB SRC_PKG_FILES ${LAMMPS_SOURCE_DIR}/*/*.cpp)
message(STATUS "Running check for installed package (this might take a while)")
foreach(_SRC SRC_PKG_FILES)
get_filename_component(FILENAME "${_SRC}" NAME)
if(EXISTS ${LAMMPS_SOURCE_DIR}/${FILENAME})
message(FATAL_ERROR "Found packages installed by the make-based buildsystem, please run 'make -C ${LAMMPS_SOURCE_DIR} no-all purge'")
endif()
endforeach()
set(SRC_FILES_CACHED "${SRC_FILES}" CACHE INTERNAL "List of file in LAMMPS_SOURCE_DIR" FORCE)
endif()
# check for files auto-generated by make-based buildsystem
# this is fast, so check for it all the time
message(STATUS "Running check for auto-generated files from make-based build system")
file(GLOB SRC_AUTOGEN_FILES ${LAMMPS_SOURCE_DIR}/style_*.h)
list(APPEND SRC_AUTOGEN_FILES ${LAMMPS_SOURCE_DIR}/lmpinstalledpkgs.h)
foreach(_SRC ${SRC_AUTOGEN_FILES})
get_filename_component(FILENAME "${_SRC}" NAME)
if(EXISTS ${LAMMPS_SOURCE_DIR}/${FILENAME})
message(FATAL_ERROR "\n########################################################################\n"
"Found header file(s) generated by the make-based build system\n"
"\n"
"Please run\n"
"make -C ${LAMMPS_SOURCE_DIR} purge\n"
"to remove\n"
"########################################################################")
endif()
endforeach()
######################################################################
# compiler tests
@ -49,13 +53,59 @@ if (${CMAKE_CXX_COMPILER_ID} STREQUAL "Intel")
set (CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -restrict")
endif()
# GNU compiler features
if (${CMAKE_CXX_COMPILER_ID} STREQUAL "GNU")
option(ENABLE_COVERAGE "Enable code coverage" OFF)
mark_as_advanced(ENABLE_COVERAGE)
if(ENABLE_COVERAGE)
set (CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} --coverage")
endif()
option(ENABLE_SANITIZE_ADDRESS "Enable address sanitizer" OFF)
mark_as_advanced(ENABLE_SANITIZE_ADDRESS)
if(ENABLE_SANITIZE_ADDRESS)
set (CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -fsanitize=address")
endif()
option(ENABLE_SANITIZE_UNDEFINED "Enable undefined behavior sanitizer" OFF)
mark_as_advanced(ENABLE_SANITIZE_UNDEFINED)
if(ENABLE_SANITIZE_UNDEFINED)
set (CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -fsanitize=undefined")
endif()
option(ENABLE_SANITIZE_THREAD "Enable thread sanitizer" OFF)
mark_as_advanced(ENABLE_SANITIZE_THREAD)
if(ENABLE_SANITIZE_THREAD)
set (CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -fsanitize=thread")
endif()
endif()
########################################################################
# User input options #
########################################################################
option(BUILD_SHARED_LIBS "Build shared libs" OFF)
if(BUILD_SHARED_LIBS) # for all pkg libs, mpi_stubs and linalg
set(CMAKE_POSITION_INDEPENDENT_CODE ON)
option(BUILD_EXE "Build lmp binary" ON)
if(BUILD_EXE)
set(LAMMPS_MACHINE "" CACHE STRING "Suffix to append to lmp binary (WON'T enable any features automatically")
mark_as_advanced(LAMMPS_MACHINE)
if(LAMMPS_MACHINE)
set(LAMMPS_MACHINE "_${LAMMPS_MACHINE}")
endif()
endif()
option(BUILD_LIB "Build LAMMPS library" OFF)
if(BUILD_LIB)
option(BUILD_SHARED_LIBS "Build shared library" OFF)
if(BUILD_SHARED_LIBS) # for all pkg libs, mpi_stubs and linalg
set(CMAKE_POSITION_INDEPENDENT_CODE ON)
endif()
set(LIB_SUFFIX "" CACHE STRING "Suffix to append to liblammps and pkg-config file")
mark_as_advanced(LIB_SUFFIX)
if(LIB_SUFFIX)
set(LIB_SUFFIX "_${LIB_SUFFIX}")
endif()
endif()
if(NOT BUILD_EXE AND NOT BUILD_LIB)
message(FATAL_ERROR "You need to at least enable one of two following options: BUILD_LIB or BUILD_EXE")
endif()
option(DEVELOPER_MODE "Enable developer mode" OFF)
mark_as_advanced(DEVELOPER_MODE)
option(CMAKE_VERBOSE_MAKEFILE "Generate verbose Makefiles" OFF)
@ -88,8 +138,11 @@ set_property(CACHE LAMMPS_SIZE_LIMIT PROPERTY STRINGS LAMMPS_SMALLBIG LAMMPS_BIG
add_definitions(-D${LAMMPS_SIZE_LIMIT})
set(LAMMPS_API_DEFINES "${LAMMPS_API_DEFINES} -D${LAMMPS_SIZE_LIMIT}")
set(LAMMPS_MEMALIGN "64" CACHE STRING "enables the use of the posix_memalign() call instead of malloc() when large chunks or memory are allocated by LAMMPS")
add_definitions(-DLAMMPS_MEMALIGN=${LAMMPS_MEMALIGN})
# posix_memalign is not available on Windows
if(NOT ${CMAKE_SYSTEM_NAME} STREQUAL "Windows")
set(LAMMPS_MEMALIGN "64" CACHE STRING "enables the use of the posix_memalign() call instead of malloc() when large chunks or memory are allocated by LAMMPS")
add_definitions(-DLAMMPS_MEMALIGN=${LAMMPS_MEMALIGN})
endif()
option(LAMMPS_EXCEPTIONS "enable the use of C++ exceptions for error messages (useful for library interface)" OFF)
if(LAMMPS_EXCEPTIONS)
@ -97,12 +150,6 @@ if(LAMMPS_EXCEPTIONS)
set(LAMMPS_API_DEFINES "${LAMMPS_API_DEFINES} -DLAMMPS_EXCEPTIONS")
endif()
set(LAMMPS_MACHINE "" CACHE STRING "Suffix to append to lmp binary and liblammps (WON'T enable any features automatically")
mark_as_advanced(LAMMPS_MACHINE)
if(LAMMPS_MACHINE)
set(LAMMPS_MACHINE "_${LAMMPS_MACHINE}")
endif()
option(CMAKE_VERBOSE_MAKEFILE "Verbose makefile" OFF)
option(ENABLE_TESTING "Enable testing" OFF)
@ -110,19 +157,17 @@ if(ENABLE_TESTING)
enable_testing()
endif(ENABLE_TESTING)
option(ENABLE_ALL "Build all default packages" OFF)
set(DEFAULT_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS CORESHELL DIPOLE GRANULAR
KSPACE MANYBODY MC MEAM MISC MOLECULE PERI QEQ
REAX REPLICA RIGID SHOCK SNAP SRD)
set(OTHER_PACKAGES KIM PYTHON MSCG MPIIO VORONOI POEMS LATTE
USER-ATC USER-AWPMD USER-BOCS USER-CGDNA USER-MESO
USER-CGSDK USER-COLVARS USER-DIFFRACTION USER-DPD USER-DRUDE USER-EFF
USER-FEP USER-H5MD USER-LB USER-MANIFOLD USER-MEAMC USER-MGPT USER-MISC
set(DEFAULT_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS DIPOLE GRANULAR
KSPACE MANYBODY MC MEAM MISC MOLECULE PERI REAX REPLICA RIGID SHOCK SPIN SNAP
SRD KIM PYTHON MSCG MPIIO VORONOI POEMS LATTE USER-ATC USER-AWPMD USER-BOCS
USER-CGDNA USER-MESO USER-CGSDK USER-COLVARS USER-DIFFRACTION USER-DPD USER-DRUDE
USER-EFF USER-FEP USER-H5MD USER-LB USER-MANIFOLD USER-MEAMC USER-MGPT USER-MISC
USER-MOFFF USER-MOLFILE USER-NETCDF USER-PHONON USER-QTB USER-REAXC USER-SMD
USER-SMTBQ USER-SPH USER-TALLY USER-UEF USER-VTK USER-QUIP USER-QMMM)
set(ACCEL_PACKAGES USER-OMP KOKKOS OPT USER-INTEL GPU)
set(OTHER_PACKAGES CORESHELL QEQ)
foreach(PKG ${DEFAULT_PACKAGES})
option(PKG_${PKG} "Build ${PKG} Package" ${ENABLE_ALL})
option(PKG_${PKG} "Build ${PKG} Package" OFF)
endforeach()
foreach(PKG ${ACCEL_PACKAGES} ${OTHER_PACKAGES})
option(PKG_${PKG} "Build ${PKG} Package" OFF)
@ -134,36 +179,24 @@ macro(pkg_depends PKG1 PKG2)
endif()
endmacro()
# "hard" dependencies between packages resulting
# in an error instead of skipping over files
pkg_depends(MPIIO MPI)
pkg_depends(QEQ MANYBODY)
pkg_depends(USER-ATC MANYBODY)
pkg_depends(USER-LB MPI)
pkg_depends(USER-MISC MANYBODY)
pkg_depends(USER-PHONON KSPACE)
pkg_depends(CORESHELL KSPACE)
######################################################
# packages with special compiler needs or external libs
######################################################
if(PKG_REAX OR PKG_MEAM OR PKG_USER-QUIP OR PKG_USER-QMMM OR PKG_LATTE)
enable_language(Fortran)
list(APPEND LAMMPS_LINK_LIBS ${CMAKE_Fortran_IMPLICIT_LINK_LIBRARIES})
endif()
if(PKG_MEAM OR PKG_USER-H5MD OR PKG_USER-QMMM)
enable_language(C)
endif()
if(PKG_MSCG)
if (CMAKE_VERSION VERSION_LESS "3.1")
message(FATAL_ERROR "For the MSCG package you need at least cmake-3.1")
endif()
# starting with CMake 3.1 this is all you have to do to enforce C++11
set(CMAKE_CXX_STANDARD 11) # C++11...
set(CMAKE_CXX_STANDARD_REQUIRED ON) #...is required...
set(CMAKE_CXX_EXTENSIONS OFF) #...without compiler extensions like gnu++11
endif()
find_package(OpenMP QUIET)
option(BUILD_OMP "Build with OpenMP support" ${OpenMP_FOUND})
if(BUILD_OMP OR PKG_USER-OMP OR PKG_KOKKOS OR PKG_USER-INTEL)
@ -207,7 +240,7 @@ if(PKG_MSCG OR PKG_USER-ATC OR PKG_USER-AWPMD OR PKG_USER-QUIP OR PKG_LATTE)
find_package(LAPACK)
if(NOT LAPACK_FOUND)
enable_language(Fortran)
file(GLOB LAPACK_SOURCES ${LAMMPS_LIB_SOURCE_DIR}/linalg/*.f)
file(GLOB LAPACK_SOURCES ${LAMMPS_LIB_SOURCE_DIR}/linalg/*.[fF])
add_library(linalg STATIC ${LAPACK_SOURCES})
set(LAPACK_LIBRARIES linalg)
endif()
@ -219,7 +252,7 @@ if(PKG_PYTHON)
add_definitions(-DLMP_PYTHON)
include_directories(${PYTHON_INCLUDE_DIR})
list(APPEND LAMMPS_LINK_LIBS ${PYTHON_LIBRARY})
if(BUILD_SHARED_LIBS)
if(BUILD_LIB AND BUILD_SHARED_LIBS)
if(NOT PYTHON_INSTDIR)
execute_process(COMMAND ${PYTHON_EXECUTABLE}
-c "import distutils.sysconfig as cg; print(cg.get_python_lib(1,0,prefix='${CMAKE_INSTALL_PREFIX}'))"
@ -302,8 +335,8 @@ if(PKG_LATTE)
message(STATUS "LATTE not found - we will build our own")
include(ExternalProject)
ExternalProject_Add(latte_build
URL https://github.com/lanl/LATTE/archive/v1.1.1.tar.gz
URL_MD5 cb86f1d2473ce00aa61ff6a023154b03
URL https://github.com/lanl/LATTE/archive/v1.2.1.tar.gz
URL_MD5 85ac414fdada2d04619c8f936344df14
SOURCE_SUBDIR cmake
CMAKE_ARGS -DCMAKE_INSTALL_PREFIX=<INSTALL_DIR> -DCMAKE_POSITION_INDEPENDENT_CODE=${CMAKE_POSITION_INDEPENDENT_CODE}
)
@ -340,13 +373,10 @@ if(PKG_USER-SMD)
ExternalProject_Add(Eigen3_build
URL http://bitbucket.org/eigen/eigen/get/3.3.4.tar.gz
URL_MD5 1a47e78efe365a97de0c022d127607c3
CMAKE_ARGS -DCMAKE_INSTALL_PREFIX=<INSTALL_DIR> -DEIGEN_TEST_NOQT=ON
-DCMAKE_DISABLE_FIND_PACKAGE_LAPACK=ON -DCMAKE_DISABLE_FIND_PACKAGE_Cholmod=ON -DCMAKE_DISABLE_FIND_PACKAGE_Umfpack=ON -DCMAKE_DISABLE_FIND_PACKAGE_SuperLU=ON
-DCMAKE_DISABLE_FIND_PACKAGE_PASTIX=ON -DCMAKE_DISABLE_FIND_PACKAGE_SPQR=ON -DCMAKE_DISABLE_FIND_PACKAGE_Boost=ON -DCMAKE_DISABLE_FIND_PACKAGE_CUDA=ON
-DCMAKE_DISABLE_FIND_PACKAGE_FFTW=ON -DCMAKE_DISABLE_FIND_PACKAGE_MPFR=ON -DCMAKE_DISABLE_FIND_PACKAGE_OpenGL=ON
)
ExternalProject_get_property(Eigen3_build INSTALL_DIR)
set(EIGEN3_INCLUDE_DIR ${INSTALL_DIR}/include/eigen3)
CONFIGURE_COMMAND "" BUILD_COMMAND "" INSTALL_COMMAND ""
)
ExternalProject_get_property(Eigen3_build SOURCE_DIR)
set(EIGEN3_INCLUDE_DIR ${SOURCE_DIR})
list(APPEND LAMMPS_DEPS Eigen3_build)
else()
find_package(Eigen3)
@ -402,26 +432,36 @@ endif()
if(PKG_MSCG)
find_package(GSL REQUIRED)
set(LAMMPS_LIB_MSCG_BIN_DIR ${LAMMPS_LIB_BINARY_DIR}/mscg)
set(MSCG_TARBALL ${LAMMPS_LIB_MSCG_BIN_DIR}/MS-CG-master.zip)
set(LAMMPS_LIB_MSCG_BIN_DIR ${LAMMPS_LIB_MSCG_BIN_DIR}/MSCG-release-master/src)
if(NOT EXISTS ${LAMMPS_LIB_MSCG_BIN_DIR})
if(NOT EXISTS ${MSCG_TARBALL})
message(STATUS "Downloading ${MSCG_TARBALL}")
file(DOWNLOAD
https://github.com/uchicago-voth/MSCG-release/archive/master.zip
${MSCG_TARBALL} SHOW_PROGRESS) #EXPECTED_MD5 cannot be due due to master
option(DOWNLOAD_MSCG "Download latte (instead of using the system's one)" OFF)
if(DOWNLOAD_MSCG)
include(ExternalProject)
if(NOT LAPACK_FOUND)
set(EXTRA_MSCG_OPTS "-DLAPACK_LIBRARIES=${CMAKE_CURRENT_BINARY_DIR}/liblinalg.a")
endif()
ExternalProject_Add(mscg_build
URL https://github.com/uchicago-voth/MSCG-release/archive/1.7.3.1.tar.gz
URL_MD5 8c45e269ee13f60b303edd7823866a91
SOURCE_SUBDIR src/CMake
CMAKE_ARGS -DCMAKE_INSTALL_PREFIX=<INSTALL_DIR> -DCMAKE_POSITION_INDEPENDENT_CODE=${CMAKE_POSITION_INDEPENDENT_CODE} ${EXTRA_MSCG_OPTS}
BUILD_COMMAND make mscg INSTALL_COMMAND ""
)
ExternalProject_get_property(mscg_build BINARY_DIR)
set(MSCG_LIBRARIES ${BINARY_DIR}/libmscg.a)
ExternalProject_get_property(mscg_build SOURCE_DIR)
set(MSCG_INCLUDE_DIRS ${SOURCE_DIR}/src)
list(APPEND LAMMPS_DEPS mscg_build)
if(NOT LAPACK_FOUND)
file(MAKE_DIRECTORY ${MSCG_INCLUDE_DIRS})
add_dependencies(mscg_build linalg)
endif()
else()
find_package(MSCG)
if(NOT MSCG_FOUND)
message(FATAL_ERROR "MSCG not found, help CMake to find it by setting MSCG_LIBRARY and MSCG_INCLUDE_DIRS, or set DOWNLOAD_MSCG=ON to download it")
endif()
message(STATUS "Unpacking ${MSCG_TARBALL}")
execute_process(COMMAND ${CMAKE_COMMAND} -E tar xvf ${MSCG_TARBALL}
WORKING_DIRECTORY ${LAMMPS_LIB_BINARY_DIR}/mscg)
endif()
file(GLOB MSCG_SOURCES ${LAMMPS_LIB_MSCG_BIN_DIR}/*.cpp)
add_library(mscg STATIC ${MSCG_SOURCES})
list(APPEND LAMMPS_LINK_LIBS mscg)
target_compile_options(mscg PRIVATE -DDIMENSION=3 -D_exclude_gromacs=1)
target_include_directories(mscg PUBLIC ${LAMMPS_LIB_MSCG_BIN_DIR})
target_link_libraries(mscg ${GSL_LIBRARIES} ${LAPACK_LIBRARIES})
list(APPEND LAMMPS_LINK_LIBS ${MSCG_LIBRARIES} ${GSL_LIBRARIES} ${LAPACK_LIBRARIES})
include_directories(${MSCG_INCLUDE_DIRS})
endif()
if(PKG_COMPRESS)
@ -430,6 +470,11 @@ if(PKG_COMPRESS)
list(APPEND LAMMPS_LINK_LIBS ${ZLIB_LIBRARIES})
endif()
# the windows version of LAMMPS requires a couple extra libraries
if(${CMAKE_SYSTEM_NAME} STREQUAL "Windows")
list(APPEND LAMMPS_LINK_LIBS -lwsock32 -lpsapi)
endif()
########################################################################
# Basic system tests (standard libraries, headers, functions, types) #
########################################################################
@ -444,6 +489,9 @@ endforeach(HEADER)
set(MATH_LIBRARIES "m" CACHE STRING "math library")
mark_as_advanced( MATH_LIBRARIES )
include(CheckLibraryExists)
if (CMAKE_VERSION VERSION_LESS "3.4")
enable_language(C) # check_library_exists isn't supported without a c compiler before v3.4
endif()
foreach(FUNC sin cos)
check_library_exists(${MATH_LIBRARIES} ${FUNC} "" FOUND_${FUNC}_${MATH_LIBRARIES})
if(NOT FOUND_${FUNC}_${MATH_LIBRARIES})
@ -461,23 +509,14 @@ RegisterStyles(${LAMMPS_SOURCE_DIR})
##############################################
# add sources of enabled packages
############################################
foreach(PKG ${DEFAULT_PACKAGES} ${OTHER_PACKAGES})
foreach(PKG ${DEFAULT_PACKAGES})
set(${PKG}_SOURCES_DIR ${LAMMPS_SOURCE_DIR}/${PKG})
# ignore PKG files which were manually installed in src folder
# headers are ignored during RegisterStyles
file(GLOB ${PKG}_SOURCES ${${PKG}_SOURCES_DIR}/*.cpp)
file(GLOB ${PKG}_HEADERS ${${PKG}_SOURCES_DIR}/*.h)
foreach(PKG_FILE in ${${PKG}_SOURCES})
get_filename_component(FNAME ${PKG_FILE} NAME)
list(REMOVE_ITEM LIB_SOURCES ${LAMMPS_SOURCE_DIR}/${FNAME})
endforeach()
foreach(PKG_FILE in ${${PKG}_HEADERS})
get_filename_component(FNAME ${PKG_FILE} NAME)
DetectAndRemovePackageHeader(${LAMMPS_SOURCE_DIR}/${FNAME})
endforeach()
# check for package files in src directory due to old make system
DetectBuildSystemConflict(${LAMMPS_SOURCE_DIR} ${${PKG}_SOURCES} ${${PKG}_HEADERS})
if(PKG_${PKG})
# detects styles in package and adds them to global list
@ -488,6 +527,17 @@ foreach(PKG ${DEFAULT_PACKAGES} ${OTHER_PACKAGES})
endif()
endforeach()
# dedicated check for entire contents of accelerator packages
foreach(PKG ${ACCEL_PACKAGES})
set(${PKG}_SOURCES_DIR ${LAMMPS_SOURCE_DIR}/${PKG})
file(GLOB ${PKG}_SOURCES ${${PKG}_SOURCES_DIR}/*.cpp)
file(GLOB ${PKG}_HEADERS ${${PKG}_SOURCES_DIR}/*.h)
# check for package files in src directory due to old make system
DetectBuildSystemConflict(${LAMMPS_SOURCE_DIR} ${${PKG}_SOURCES} ${${PKG}_HEADERS})
endforeach()
##############################################
# add lib sources of (simple) enabled packages
############################################
@ -533,6 +583,41 @@ endif()
# packages which selectively include variants based on enabled styles
# e.g. accelerator packages
######################################################################
if(PKG_CORESHELL)
set(CORESHELL_SOURCES_DIR ${LAMMPS_SOURCE_DIR}/CORESHELL)
set(CORESHELL_SOURCES)
set_property(GLOBAL PROPERTY "CORESHELL_SOURCES" "${CORESHELL_SOURCES}")
# detects styles which have a CORESHELL version
RegisterStylesExt(${CORESHELL_SOURCES_DIR} cs CORESHELL_SOURCES)
get_property(CORESHELL_SOURCES GLOBAL PROPERTY CORESHELL_SOURCES)
list(APPEND LIB_SOURCES ${CORESHELL_SOURCES})
include_directories(${CORESHELL_SOURCES_DIR})
endif()
# Fix qeq/fire requires MANYBODY (i.e. COMB and COMB3) to be installed
if(PKG_QEQ)
set(QEQ_SOURCES_DIR ${LAMMPS_SOURCE_DIR}/QEQ)
file(GLOB QEQ_HEADERS ${QEQ_SOURCES_DIR}/fix*.h)
file(GLOB QEQ_SOURCES ${QEQ_SOURCES_DIR}/fix*.cpp)
if(NOT PKG_MANYBODY)
list(REMOVE_ITEM QEQ_HEADERS ${QEQ_SOURCES_DIR}/fix_qeq_fire.h)
list(REMOVE_ITEM QEQ_SOURCES ${QEQ_SOURCES_DIR}/fix_qeq_fire.cpp)
endif()
set_property(GLOBAL PROPERTY "QEQ_SOURCES" "${QEQ_SOURCES}")
foreach(MY_HEADER ${QEQ_HEADERS})
AddStyleHeader(${MY_HEADER} FIX)
endforeach()
get_property(QEQ_SOURCES GLOBAL PROPERTY QEQ_SOURCES)
list(APPEND LIB_SOURCES ${QEQ_SOURCES})
include_directories(${QEQ_SOURCES_DIR})
endif()
if(PKG_USER-OMP)
set(USER-OMP_SOURCES_DIR ${LAMMPS_SOURCE_DIR}/USER-OMP)
set(USER-OMP_SOURCES ${USER-OMP_SOURCES_DIR}/thr_data.cpp
@ -544,8 +629,31 @@ if(PKG_USER-OMP)
# detects styles which have USER-OMP version
RegisterStylesExt(${USER-OMP_SOURCES_DIR} omp OMP_SOURCES)
get_property(USER-OMP_SOURCES GLOBAL PROPERTY OMP_SOURCES)
# manually add package dependent source files from USER-OMP that do not provide styles
if(PKG_ASPHERE)
list(APPEND USER-OMP_SOURCES ${USER-OMP_SOURCES_DIR}/fix_nh_asphere_omp.cpp)
endif()
if(PKG_RIGID)
list(APPEND USER-OMP_SOURCES ${USER-OMP_SOURCES_DIR}/fix_rigid_nh_omp.cpp)
endif()
if(PKG_USER-REAXC)
list(APPEND USER-OMP_SOURCES ${USER-OMP_SOURCES_DIR}/reaxc_bond_orders_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_hydrogen_bonds_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_nonbonded_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_bonds_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_init_md_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_torsion_angles_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_forces_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_multi_body_omp.cpp
${USER-OMP_SOURCES_DIR}/reaxc_valence_angles_omp.cpp)
endif()
list(APPEND LIB_SOURCES ${USER-OMP_SOURCES})
include_directories(${USER-OMP_SOURCES_DIR})
endif()
@ -622,6 +730,10 @@ if(PKG_USER-INTEL)
message(FATAL_ERROR "USER-INTEL is needed at least 2016 intel compiler, found ${CMAKE_CXX_COMPILER_VERSION}")
endif()
endif()
option(INJECT_KNL_FLAG "Inject flags for KNL build" OFF)
if(INJECT_KNL_FLAG)
set(CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -xMIC-AVX512")
endif()
option(INJECT_INTEL_FLAG "Inject OMG fast flags for USER-INTEL" ON)
if(INJECT_INTEL_FLAG AND CMAKE_CXX_COMPILER_ID STREQUAL "Intel")
if(CMAKE_CXX_COMPILER_VERSION VERSION_EQUAL 17.3 OR CMAKE_CXX_COMPILER_VERSION VERSION_EQUAL 17.4)
@ -686,8 +798,7 @@ if(PKG_GPU)
endif()
option(CUDPP_OPT "Enable CUDPP_OPT" ON)
set(GPU_ARCH "sm_30" CACHE STRING "LAMMPS GPU CUDA SM architecture")
set_property(CACHE GPU_ARCH PROPERTY STRINGS sm_10 sm_20 sm_30 sm_60)
set(GPU_ARCH "sm_30" CACHE STRING "LAMMPS GPU CUDA SM architecture (e.g. sm_60)")
file(GLOB GPU_LIB_CU ${LAMMPS_LIB_SOURCE_DIR}/gpu/*.cu ${CMAKE_CURRENT_SOURCE_DIR}/gpu/*.cu)
list(REMOVE_ITEM GPU_LIB_CU ${LAMMPS_LIB_SOURCE_DIR}/gpu/lal_pppm.cu)
@ -796,36 +907,173 @@ GenerateStyleHeaders(${LAMMPS_STYLE_HEADERS_DIR})
include_directories(${LAMMPS_SOURCE_DIR})
include_directories(${LAMMPS_STYLE_HEADERS_DIR})
######################################
# Generate lmpinstalledpkgs.h
######################################
set(temp "#ifndef LMP_INSTALLED_PKGS_H\n#define LMP_INSTALLED_PKGS_H\n")
set(temp "${temp}const char * LAMMPS_NS::LAMMPS::installed_packages[] = {\n")
foreach(PKG ${DEFAULT_PACKAGES} ${ACCEL_PACKAGES} ${OTHER_PACKAGES})
if(PKG_${PKG})
set(temp "${temp} \"${PKG}\",\n")
endif()
endforeach()
set(temp "${temp} NULL\n};\n#endif\n\n")
message(STATUS "Generating lmpinstalledpkgs.h...")
file(WRITE "${LAMMPS_STYLE_HEADERS_DIR}/lmpinstalledpkgs.h.tmp" "${temp}" )
execute_process(COMMAND ${CMAKE_COMMAND} -E copy_if_different "${LAMMPS_STYLE_HEADERS_DIR}/lmpinstalledpkgs.h.tmp" "${LAMMPS_STYLE_HEADERS_DIR}/lmpinstalledpkgs.h")
###########################################
# Actually add executable and lib to build
############################################
add_library(lammps ${LIB_SOURCES})
get_property(LANGUAGES GLOBAL PROPERTY ENABLED_LANGUAGES)
list (FIND LANGUAGES "Fortran" _index)
if (${_index} GREATER -1)
list(APPEND LAMMPS_LINK_LIBS ${CMAKE_Fortran_IMPLICIT_LINK_LIBRARIES})
endif()
list(REMOVE_DUPLICATES LAMMPS_LINK_LIBS)
target_link_libraries(lammps ${LAMMPS_LINK_LIBS})
if(LAMMPS_DEPS)
add_dependencies(lammps ${LAMMPS_DEPS})
endif()
set_target_properties(lammps PROPERTIES OUTPUT_NAME lammps${LAMMPS_MACHINE})
if(BUILD_SHARED_LIBS)
set_target_properties(lammps PROPERTIES SOVERSION ${SOVERSION})
install(TARGETS lammps LIBRARY DESTINATION ${CMAKE_INSTALL_LIBDIR} ARCHIVE DESTINATION ${CMAKE_INSTALL_LIBDIR})
install(FILES ${LAMMPS_SOURCE_DIR}/library.h DESTINATION ${CMAKE_INSTALL_INCLUDEDIR}/lammps)
configure_file(pkgconfig/liblammps.pc.in ${CMAKE_CURRENT_BINARY_DIR}/liblammps${LAMMPS_MACHINE}.pc @ONLY)
install(FILES ${CMAKE_CURRENT_BINARY_DIR}/liblammps${LAMMPS_MACHINE}.pc DESTINATION ${CMAKE_INSTALL_LIBDIR}/pkgconfig)
if(BUILD_LIB)
add_library(lammps ${LIB_SOURCES})
target_link_libraries(lammps ${LAMMPS_LINK_LIBS})
if(LAMMPS_DEPS)
add_dependencies(lammps ${LAMMPS_DEPS})
endif()
set_target_properties(lammps PROPERTIES OUTPUT_NAME lammps${LIB_SUFFIX})
if(BUILD_SHARED_LIBS)
set_target_properties(lammps PROPERTIES SOVERSION ${SOVERSION})
install(TARGETS lammps LIBRARY DESTINATION ${CMAKE_INSTALL_LIBDIR} ARCHIVE DESTINATION ${CMAKE_INSTALL_LIBDIR})
install(FILES ${LAMMPS_SOURCE_DIR}/library.h DESTINATION ${CMAKE_INSTALL_INCLUDEDIR}/lammps)
configure_file(pkgconfig/liblammps.pc.in ${CMAKE_CURRENT_BINARY_DIR}/liblammps${LIB_SUFFIX}.pc @ONLY)
install(FILES ${CMAKE_CURRENT_BINARY_DIR}/liblammps${LIB_SUFFIX}.pc DESTINATION ${CMAKE_INSTALL_LIBDIR}/pkgconfig)
endif()
else()
list(APPEND LMP_SOURCES ${LIB_SOURCES})
endif()
add_executable(lmp ${LMP_SOURCES})
target_link_libraries(lmp lammps)
set_target_properties(lmp PROPERTIES OUTPUT_NAME lmp${LAMMPS_MACHINE})
install(TARGETS lmp DESTINATION ${CMAKE_INSTALL_BINDIR})
if(ENABLE_TESTING)
add_test(ShowHelp lmp${LAMMPS_MACHINE} -help)
if(BUILD_EXE)
add_executable(lmp ${LMP_SOURCES})
if(BUILD_LIB)
target_link_libraries(lmp lammps)
else()
target_link_libraries(lmp ${LAMMPS_LINK_LIBS})
if(LAMMPS_DEPS)
add_dependencies(lmp ${LAMMPS_DEPS})
endif()
endif()
set_target_properties(lmp PROPERTIES OUTPUT_NAME lmp${LAMMPS_MACHINE})
install(TARGETS lmp DESTINATION ${CMAKE_INSTALL_BINDIR})
if(ENABLE_TESTING)
add_test(ShowHelp lmp${LAMMPS_MACHINE} -help)
endif()
endif()
##################################
###############################################################################
# Build documentation
###############################################################################
option(BUILD_DOC "Build LAMMPS documentation" OFF)
if(BUILD_DOC)
include(ProcessorCount)
ProcessorCount(NPROCS)
find_package(PythonInterp 3 REQUIRED)
set(VIRTUALENV ${PYTHON_EXECUTABLE} -m virtualenv)
file(GLOB DOC_SOURCES ${LAMMPS_DOC_DIR}/src/*.txt)
file(GLOB PDF_EXTRA_SOURCES ${LAMMPS_DOC_DIR}/src/lammps_commands*.txt ${LAMMPS_DOC_DIR}/src/lammps_support.txt ${LAMMPS_DOC_DIR}/src/lammps_tutorials.txt)
list(REMOVE_ITEM DOC_SOURCES ${PDF_EXTRA_SOURCES})
add_custom_command(
OUTPUT docenv
COMMAND ${VIRTUALENV} docenv
)
set(DOCENV_BINARY_DIR ${CMAKE_BINARY_DIR}/docenv/bin)
add_custom_command(
OUTPUT requirements.txt
DEPENDS docenv
COMMAND ${CMAKE_COMMAND} -E copy ${LAMMPS_DOC_DIR}/utils/requirements.txt requirements.txt
COMMAND ${DOCENV_BINARY_DIR}/pip install -r requirements.txt --upgrade
COMMAND ${DOCENV_BINARY_DIR}/pip install --upgrade ${LAMMPS_DOC_DIR}/utils/converters
)
set(RST_FILES "")
set(RST_DIR ${CMAKE_BINARY_DIR}/rst)
file(MAKE_DIRECTORY ${RST_DIR})
foreach(TXT_FILE ${DOC_SOURCES})
get_filename_component(FILENAME ${TXT_FILE} NAME_WE)
set(RST_FILE ${RST_DIR}/${FILENAME}.rst)
list(APPEND RST_FILES ${RST_FILE})
add_custom_command(
OUTPUT ${RST_FILE}
DEPENDS requirements.txt docenv ${TXT_FILE}
COMMAND ${DOCENV_BINARY_DIR}/txt2rst -o ${RST_DIR} ${TXT_FILE}
)
endforeach()
add_custom_command(
OUTPUT html
DEPENDS ${RST_FILES}
COMMAND ${CMAKE_COMMAND} -E copy_directory ${LAMMPS_DOC_DIR}/src ${RST_DIR}
COMMAND ${DOCENV_BINARY_DIR}/sphinx-build -j ${NPROCS} -b html -c ${LAMMPS_DOC_DIR}/utils/sphinx-config -d ${CMAKE_BINARY_DIR}/doctrees ${RST_DIR} html
)
add_custom_target(
doc ALL
DEPENDS html
SOURCES ${LAMMPS_DOC_DIR}/utils/requirements.txt ${DOC_SOURCES}
)
install(DIRECTORY ${CMAKE_BINARY_DIR}/html DESTINATION ${CMAKE_INSTALL_DOCDIR})
endif()
###############################################################################
# Install potential files in data directory
###############################################################################
set(LAMMPS_POTENTIALS_DIR ${CMAKE_INSTALL_FULL_DATADIR}/lammps/potentials)
install(DIRECTORY ${LAMMPS_SOURCE_DIR}/../potentials DESTINATION ${CMAKE_INSTALL_DATADIR}/lammps/potentials)
configure_file(etc/profile.d/lammps.sh.in ${CMAKE_BINARY_DIR}/etc/profile.d/lammps.sh @ONLY)
configure_file(etc/profile.d/lammps.csh.in ${CMAKE_BINARY_DIR}/etc/profile.d/lammps.csh @ONLY)
install(
FILES ${CMAKE_BINARY_DIR}/etc/profile.d/lammps.sh
${CMAKE_BINARY_DIR}/etc/profile.d/lammps.csh
DESTINATION ${CMAKE_INSTALL_SYSCONFDIR}/profile.d
)
###############################################################################
# Testing
#
# Requires latest gcovr (for GCC 8.1 support):#
# pip install git+https://github.com/gcovr/gcovr.git
###############################################################################
if(ENABLE_COVERAGE)
find_program(GCOVR_BINARY gcovr)
find_package_handle_standard_args(GCOVR DEFAULT_MSG GCOVR_BINARY)
if(GCOVR_FOUND)
get_filename_component(ABSOLUTE_LAMMPS_SOURCE_DIR ${LAMMPS_SOURCE_DIR} ABSOLUTE)
add_custom_target(
gen_coverage_xml
COMMAND ${GCOVR_BINARY} -s -x -r ${ABSOLUTE_LAMMPS_SOURCE_DIR} --object-directory=${CMAKE_BINARY_DIR} -o coverage.xml
WORKING_DIRECTORY ${CMAKE_BINARY_DIR}
COMMENT "Generating XML Coverage Report..."
)
add_custom_target(
gen_coverage_html
COMMAND ${GCOVR_BINARY} -s --html --html-details -r ${ABSOLUTE_LAMMPS_SOURCE_DIR} --object-directory=${CMAKE_BINARY_DIR} -o coverage.html
WORKING_DIRECTORY ${CMAKE_BINARY_DIR}
COMMENT "Generating HTML Coverage Report..."
)
endif()
endif()
###############################################################################
# Print package summary
##################################
foreach(PKG ${DEFAULT_PACKAGES} ${OTHER_PACKAGES} ${ACCEL_PACKAGES})
###############################################################################
foreach(PKG ${DEFAULT_PACKAGES} ${ACCEL_PACKAGES})
if(PKG_${PKG})
message(STATUS "Building package: ${PKG}")
endif()
@ -834,7 +1082,7 @@ endforeach()
string(TOUPPER "${CMAKE_BUILD_TYPE}" BTYPE)
get_directory_property(CPPFLAGS DIRECTORY ${CMAKE_SOURCE_DIR} COMPILE_DEFINITIONS)
include(FeatureSummary)
feature_summary(INCLUDE_QUIET_PACKAGES WHAT ALL)
feature_summary(DESCRIPTION "The following packages have been found:" WHAT PACKAGES_FOUND)
message(STATUS "<<< Build configuration >>>
Build type ${CMAKE_BUILD_TYPE}
Install path ${CMAKE_INSTALL_PREFIX}
@ -872,13 +1120,17 @@ message(STATUS "Link libraries: ${LAMMPS_LINK_LIBS}")
if(BUILD_MPI)
message(STATUS "Using mpi with headers in ${MPI_CXX_INCLUDE_PATH} and ${MPI_CXX_LIBRARIES}")
endif()
if(ENABLED_GPU)
if(PKG_GPU)
message(STATUS "GPU Api: ${GPU_API}")
if(GPU_API STREQUAL "CUDA")
message(STATUS "GPU Arch: ${GPU_ARCH}")
elseif(GPU_API STREQUAL "OpenCL")
message(STATUS "OCL Tune: ${OCL_TUNE}")
endif()
message(STATUS "GPU Precision: ${GPU_PREC}")
endif()
if(PKG_KOKKOS)
message(STATUS "Kokkos Arch: ${KOKKOS_ARCH}")
endif()
if(PKG_KSPACE)
message(STATUS "Using ${FFT} as FFT")

22
cmake/Modules/FindMSCG.cmake Normal file
View File

@ -0,0 +1,22 @@
# - Find mscg
# Find the native MSCG headers and libraries.
#
# MSCG_INCLUDE_DIRS - where to find mscg.h, etc.
# MSCG_LIBRARIES - List of libraries when using mscg.
# MSCG_FOUND - True if mscg found.
#
find_path(MSCG_INCLUDE_DIR mscg.h PATH_SUFFIXES mscg)
find_library(MSCG_LIBRARY NAMES mscg)
set(MSCG_LIBRARIES ${MSCG_LIBRARY})
set(MSCG_INCLUDE_DIRS ${MSCG_INCLUDE_DIR})
include(FindPackageHandleStandardArgs)
# handle the QUIETLY and REQUIRED arguments and set MSCG_FOUND to TRUE
# if all listed variables are TRUE
find_package_handle_standard_args(MSCG DEFAULT_MSG MSCG_LIBRARY MSCG_INCLUDE_DIR)
mark_as_advanced(MSCG_INCLUDE_DIR MSCG_LIBRARY )

57
cmake/Modules/StyleHeaderUtils.cmake
View File

@ -45,14 +45,10 @@ function(FindStyleHeadersExt path style_class extension headers sources)
endfunction(FindStyleHeadersExt)
function(CreateStyleHeader path filename)
math(EXPR N "${ARGC}-2")
set(temp "")
if(N GREATER 0)
math(EXPR ARG_END "${ARGC}-1")
foreach(IDX RANGE 2 ${ARG_END})
list(GET ARGV ${IDX} FNAME)
if(ARGC GREATER 2)
list(REMOVE_AT ARGV 0 1)
foreach(FNAME ${ARGV})
get_filename_component(FNAME ${FNAME} NAME)
set(temp "${temp}#include \"${FNAME}\"\n")
endforeach()
@ -107,35 +103,6 @@ function(RegisterStyles search_path)
FindStyleHeaders(${search_path} REGION_CLASS region_ REGION ) # region ) # domain
endfunction(RegisterStyles)
function(RemovePackageHeader headers pkg_header)
get_property(hlist GLOBAL PROPERTY ${headers})
list(REMOVE_ITEM hlist ${pkg_header})
set_property(GLOBAL PROPERTY ${headers} "${hlist}")
endfunction(RemovePackageHeader)
function(DetectAndRemovePackageHeader fname)
RemovePackageHeader(ANGLE ${fname})
RemovePackageHeader(ATOM_VEC ${fname})
RemovePackageHeader(BODY ${fname})
RemovePackageHeader(BOND ${fname})
RemovePackageHeader(COMMAND ${fname})
RemovePackageHeader(COMPUTE ${fname})
RemovePackageHeader(DIHEDRAL ${fname})
RemovePackageHeader(DUMP ${fname})
RemovePackageHeader(FIX ${fname})
RemovePackageHeader(IMPROPER ${fname})
RemovePackageHeader(INTEGRATE ${fname})
RemovePackageHeader(KSPACE ${fname})
RemovePackageHeader(MINIMIZE ${fname})
RemovePackageHeader(NBIN ${fname})
RemovePackageHeader(NPAIR ${fname})
RemovePackageHeader(NSTENCIL ${fname})
RemovePackageHeader(NTOPO ${fname})
RemovePackageHeader(PAIR ${fname})
RemovePackageHeader(READER ${fname})
RemovePackageHeader(REGION ${fname})
endfunction(DetectAndRemovePackageHeader)
function(RegisterStylesExt search_path extension sources)
FindStyleHeadersExt(${search_path} ANGLE_CLASS ${extension} ANGLE ${sources})
FindStyleHeadersExt(${search_path} ATOM_CLASS ${extension} ATOM_VEC ${sources})
@ -181,3 +148,21 @@ function(GenerateStyleHeaders output_path)
GenerateStyleHeader(${output_path} READER reader ) # read_dump
GenerateStyleHeader(${output_path} REGION region ) # domain
endfunction(GenerateStyleHeaders)
function(DetectBuildSystemConflict lammps_src_dir)
if(ARGC GREATER 1)
list(REMOVE_AT ARGV 0)
foreach(SRC_FILE ${ARGV})
get_filename_component(FILENAME ${SRC_FILE} NAME)
if(EXISTS ${lammps_src_dir}/${FILENAME})
message(FATAL_ERROR "\n########################################################################\n"
"Found package(s) installed by the make-based build system\n"
"\n"
"Please run\n"
"make -C ${lammps_src_dir} no-all purge\n"
"to uninstall\n"
"########################################################################")
endif()
endforeach()
endif()
endfunction(DetectBuildSystemConflict)

1670
cmake/README.md
View File

File diff suppressed because it is too large Load Diff

2
cmake/etc/profile.d/lammps.csh.in Normal file
View File

@ -0,0 +1,2 @@
# set environment for LAMMPS executables to find potential files
if ( "$?LAMMPS_POTENTIALS" == 0 ) setenv LAMMPS_POTENTIALS @LAMMPS_POTENTIALS_DIR@

2
cmake/etc/profile.d/lammps.sh.in Normal file
View File

@ -0,0 +1,2 @@
# set environment for LAMMPS executables to find potential files
export LAMMPS_POTENTIALS=${LAMMPS_POTENTIALS-@LAMMPS_POTENTIALS_DIR@}

2
cmake/pkgconfig/liblammps.pc.in
View File

@ -13,6 +13,6 @@ Description: Large-scale Atomic/Molecular Massively Parallel Simulator Library
URL: http://lammps.sandia.gov
Version:
Requires:
Libs: -L${libdir} -llammps@LAMMPS_MACHINE@
Libs: -L${libdir} -llammps@LIB_SUFFIX@@
Libs.private: -lm
Cflags: -I${includedir} @LAMMPS_API_DEFINES@

22
cmake/presets/all_off.cmake Normal file
View File

@ -0,0 +1,22 @@
set(STANDARD_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS CORESHELL DIPOLE GPU
GRANULAR KIM KOKKOS KSPACE LATTE MANYBODY MC MEAM MISC
MOLECULE MPIIO MSCG OPT PERI POEMS
PYTHON QEQ REAX REPLICA RIGID SHOCK SNAP SRD VORONOI)
set(USER_PACKAGES USER-ATC USER-AWPMD USER-BOCS USER-CGDNA USER-CGSDK USER-COLVARS
USER-DIFFRACTION USER-DPD USER-DRUDE USER-EFF USER-FEP USER-H5MD
USER-INTEL USER-LB USER-MANIFOLD USER-MEAMC USER-MESO
USER-MGPT USER-MISC USER-MOFFF USER-MOLFILE
USER-NETCDF USER-OMP USER-PHONON USER-QMMM USER-QTB
USER-QUIP USER-REAXC USER-SMD USER-SMTBQ USER-SPH USER-TALLY
USER-UEF USER-VTK)
set(PACKAGES_WITH_LIB COMPRESS GPU KIM KOKKOS LATTE MEAM MPIIO MSCG POEMS PYTHON REAX VORONOI
USER-ATC USER-AWPMD USER-COLVARS USER-H5MD USER-LB USER-MOLFILE
USER-NETCDF USER-QMMM USER-QUIP USER-SMD USER-VTK)
set(ALL_PACKAGES ${STANDARD_PACKAGES} ${USER_PACKAGES})
foreach(PKG ${ALL_PACKAGES})
set(PKG_${PKG} OFF CACHE BOOL "" FORCE)
endforeach()

22
cmake/presets/all_on.cmake Normal file
View File

@ -0,0 +1,22 @@
set(STANDARD_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS CORESHELL DIPOLE GPU
GRANULAR KIM KOKKOS KSPACE LATTE MANYBODY MC MEAM MISC
MOLECULE MPIIO MSCG OPT PERI POEMS
PYTHON QEQ REAX REPLICA RIGID SHOCK SNAP SRD VORONOI)
set(USER_PACKAGES USER-ATC USER-AWPMD USER-BOCS USER-CGDNA USER-CGSDK USER-COLVARS
USER-DIFFRACTION USER-DPD USER-DRUDE USER-EFF USER-FEP USER-H5MD
USER-INTEL USER-LB USER-MANIFOLD USER-MEAMC USER-MESO
USER-MGPT USER-MISC USER-MOFFF USER-MOLFILE
USER-NETCDF USER-OMP USER-PHONON USER-QMMM USER-QTB
USER-QUIP USER-REAXC USER-SMD USER-SMTBQ USER-SPH USER-TALLY
USER-UEF USER-VTK)
set(PACKAGES_WITH_LIB COMPRESS GPU KIM KOKKOS LATTE MEAM MPIIO MSCG POEMS PYTHON REAX VORONOI
USER-ATC USER-AWPMD USER-COLVARS USER-H5MD USER-LB USER-MOLFILE
USER-NETCDF USER-QMMM USER-QUIP USER-SMD USER-VTK)
set(ALL_PACKAGES ${STANDARD_PACKAGES} ${USER_PACKAGES})
foreach(PKG ${ALL_PACKAGES})
set(PKG_${PKG} ON CACHE BOOL "" FORCE)
endforeach()

69
cmake/presets/manual_selection.cmake Normal file
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@ -0,0 +1,69 @@
set(PKG_ASPHERE OFF CACHE BOOL "" FORCE)
set(PKG_BODY OFF CACHE BOOL "" FORCE)
set(PKG_CLASS2 OFF CACHE BOOL "" FORCE)
set(PKG_COLLOID OFF CACHE BOOL "" FORCE)
set(PKG_COMPRESS OFF CACHE BOOL "" FORCE)
set(PKG_CORESHELL OFF CACHE BOOL "" FORCE)
set(PKG_DIPOLE OFF CACHE BOOL "" FORCE)
set(PKG_GPU OFF CACHE BOOL "" FORCE)
set(PKG_GRANULAR OFF CACHE BOOL "" FORCE)
set(PKG_KIM OFF CACHE BOOL "" FORCE)
set(PKG_KOKKOS OFF CACHE BOOL "" FORCE)
set(PKG_KSPACE OFF CACHE BOOL "" FORCE)
set(PKG_LATTE OFF CACHE BOOL "" FORCE)
set(PKG_LIB OFF CACHE BOOL "" FORCE)
set(PKG_MANYBODY OFF CACHE BOOL "" FORCE)
set(PKG_MC OFF CACHE BOOL "" FORCE)
set(PKG_MEAM OFF CACHE BOOL "" FORCE)
set(PKG_MISC OFF CACHE BOOL "" FORCE)
set(PKG_MOLECULE OFF CACHE BOOL "" FORCE)
set(PKG_MPIIO OFF CACHE BOOL "" FORCE)
set(PKG_MSCG OFF CACHE BOOL "" FORCE)
set(PKG_OPT OFF CACHE BOOL "" FORCE)
set(PKG_PERI OFF CACHE BOOL "" FORCE)
set(PKG_POEMS OFF CACHE BOOL "" FORCE)
set(PKG_PYTHOFF OFF CACHE BOOL "" FORCE)
set(PKG_QEQ OFF CACHE BOOL "" FORCE)
set(PKG_REAX OFF CACHE BOOL "" FORCE)
set(PKG_REPLICA OFF CACHE BOOL "" FORCE)
set(PKG_RIGID OFF CACHE BOOL "" FORCE)
set(PKG_SHOCK OFF CACHE BOOL "" FORCE)
set(PKG_SNAP OFF CACHE BOOL "" FORCE)
set(PKG_SRD OFF CACHE BOOL "" FORCE)
set(PKG_VOROFFOI OFF CACHE BOOL "" FORCE)
set(PKG_USER OFF CACHE BOOL "" FORCE)
set(PKG_USER-ATC OFF CACHE BOOL "" FORCE)
set(PKG_USER-AWPMD OFF CACHE BOOL "" FORCE)
set(PKG_USER-BOCS OFF CACHE BOOL "" FORCE)
set(PKG_USER-CGDNA OFF CACHE BOOL "" FORCE)
set(PKG_USER-CGSDK OFF CACHE BOOL "" FORCE)
set(PKG_USER-COLVARS OFF CACHE BOOL "" FORCE)
set(PKG_USER-DIFFRACTIOFF OFF CACHE BOOL "" FORCE)
set(PKG_USER-DPD OFF CACHE BOOL "" FORCE)
set(PKG_USER-DRUDE OFF CACHE BOOL "" FORCE)
set(PKG_USER-EFF OFF CACHE BOOL "" FORCE)
set(PKG_USER-FEP OFF CACHE BOOL "" FORCE)
set(PKG_USER-H5MD OFF CACHE BOOL "" FORCE)
set(PKG_USER-INTEL OFF CACHE BOOL "" FORCE)
set(PKG_USER-LB OFF CACHE BOOL "" FORCE)
set(PKG_USER-MANIFOLD OFF CACHE BOOL "" FORCE)
set(PKG_USER-MEAMC OFF CACHE BOOL "" FORCE)
set(PKG_USER-MESO OFF CACHE BOOL "" FORCE)
set(PKG_USER-MGPT OFF CACHE BOOL "" FORCE)
set(PKG_USER-MISC OFF CACHE BOOL "" FORCE)
set(PKG_USER-MOFFF OFF CACHE BOOL "" FORCE)
set(PKG_USER-MOLFILE OFF CACHE BOOL "" FORCE)
set(PKG_USER-NETCDF OFF CACHE BOOL "" FORCE)
set(PKG_USER-OMP OFF CACHE BOOL "" FORCE)
set(PKG_USER-PHOFFOFF OFF CACHE BOOL "" FORCE)
set(PKG_USER-QMMM OFF CACHE BOOL "" FORCE)
set(PKG_USER-QTB OFF CACHE BOOL "" FORCE)
set(PKG_USER-QUIP OFF CACHE BOOL "" FORCE)
set(PKG_USER-REAXC OFF CACHE BOOL "" FORCE)
set(PKG_USER-SMD OFF CACHE BOOL "" FORCE)
set(PKG_USER-SMTBQ OFF CACHE BOOL "" FORCE)
set(PKG_USER-SPH OFF CACHE BOOL "" FORCE)
set(PKG_USER-TALLY OFF CACHE BOOL "" FORCE)
set(PKG_USER-UEF OFF CACHE BOOL "" FORCE)
set(PKG_USER-VTK OFF CACHE BOOL "" FORCE)

22
cmake/presets/nolib.cmake Normal file
View File

@ -0,0 +1,22 @@
set(STANDARD_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS CORESHELL DIPOLE GPU
GRANULAR KIM KOKKOS KSPACE LATTE MANYBODY MC MEAM MISC
MOLECULE MPIIO MSCG OPT PERI POEMS
PYTHON QEQ REAX REPLICA RIGID SHOCK SNAP SRD VORONOI)
set(USER_PACKAGES USER-ATC USER-AWPMD USER-BOCS USER-CGDNA USER-CGSDK USER-COLVARS
USER-DIFFRACTION USER-DPD USER-DRUDE USER-EFF USER-FEP USER-H5MD
USER-INTEL USER-LB USER-MANIFOLD USER-MEAMC USER-MESO
USER-MGPT USER-MISC USER-MOFFF USER-MOLFILE
USER-NETCDF USER-OMP USER-PHONON USER-QMMM USER-QTB
USER-QUIP USER-REAXC USER-SMD USER-SMTBQ USER-SPH USER-TALLY
USER-UEF USER-VTK)
set(PACKAGES_WITH_LIB COMPRESS GPU KIM KOKKOS LATTE MEAM MPIIO MSCG POEMS PYTHON REAX VORONOI
USER-ATC USER-AWPMD USER-COLVARS USER-H5MD USER-LB USER-MOLFILE
USER-NETCDF USER-QMMM USER-QUIP USER-SMD USER-VTK)
set(ALL_PACKAGES ${STANDARD_PACKAGES} ${USER_PACKAGES})
foreach(PKG ${PACKAGES_WITH_LIB})
set(PKG_${PKG} OFF CACHE BOOL "" FORCE)
endforeach()

22
cmake/presets/std.cmake Normal file
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@ -0,0 +1,22 @@
set(STANDARD_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS CORESHELL DIPOLE GPU
GRANULAR KIM KOKKOS KSPACE LATTE MANYBODY MC MEAM MISC
MOLECULE MPIIO MSCG OPT PERI POEMS
PYTHON QEQ REAX REPLICA RIGID SHOCK SNAP SRD VORONOI)
set(USER_PACKAGES USER-ATC USER-AWPMD USER-BOCS USER-CGDNA USER-CGSDK USER-COLVARS
USER-DIFFRACTION USER-DPD USER-DRUDE USER-EFF USER-FEP USER-H5MD
USER-INTEL USER-LB USER-MANIFOLD USER-MEAMC USER-MESO
USER-MGPT USER-MISC USER-MOFFF USER-MOLFILE
USER-NETCDF USER-OMP USER-PHONON USER-QMMM USER-QTB
USER-QUIP USER-REAXC USER-SMD USER-SMTBQ USER-SPH USER-TALLY
USER-UEF USER-VTK)
set(PACKAGES_WITH_LIB COMPRESS GPU KIM KOKKOS LATTE MEAM MPIIO MSCG POEMS PYTHON REAX VORONOI
USER-ATC USER-AWPMD USER-COLVARS USER-H5MD USER-LB USER-MOLFILE
USER-NETCDF USER-QMMM USER-QUIP USER-SMD USER-VTK)
set(ALL_PACKAGES ${STANDARD_PACKAGES} ${USER_PACKAGES})
foreach(PKG ${STANDARD_PACKAGES})
set(PKG_${PKG} ON CACHE BOOL "" FORCE)
endforeach()

26
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@ -0,0 +1,26 @@
set(STANDARD_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS CORESHELL DIPOLE GPU
GRANULAR KIM KOKKOS KSPACE LATTE MANYBODY MC MEAM MISC
MOLECULE MPIIO MSCG OPT PERI POEMS
PYTHON QEQ REAX REPLICA RIGID SHOCK SNAP SRD VORONOI)
set(USER_PACKAGES USER-ATC USER-AWPMD USER-BOCS USER-CGDNA USER-CGSDK USER-COLVARS
USER-DIFFRACTION USER-DPD USER-DRUDE USER-EFF USER-FEP USER-H5MD
USER-INTEL USER-LB USER-MANIFOLD USER-MEAMC USER-MESO
USER-MGPT USER-MISC USER-MOFFF USER-MOLFILE
USER-NETCDF USER-OMP USER-PHONON USER-QMMM USER-QTB
USER-QUIP USER-REAXC USER-SMD USER-SMTBQ USER-SPH USER-TALLY
USER-UEF USER-VTK)
set(PACKAGES_WITH_LIB COMPRESS GPU KIM KOKKOS LATTE MEAM MPIIO MSCG POEMS PYTHON REAX VORONOI
USER-ATC USER-AWPMD USER-COLVARS USER-H5MD USER-LB USER-MOLFILE
USER-NETCDF USER-QMMM USER-QUIP USER-SMD USER-VTK)
set(ALL_PACKAGES ${STANDARD_PACKAGES} ${USER_PACKAGES})
foreach(PKG ${STANDARD_PACKAGES})
set(PKG_${PKG} ON CACHE BOOL "" FORCE)
endforeach()
foreach(PKG ${PACKAGES_WITH_LIB})
set(PKG_${PKG} OFF CACHE BOOL "" FORCE)
endforeach()

22
cmake/presets/user.cmake Normal file
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@ -0,0 +1,22 @@
set(STANDARD_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS CORESHELL DIPOLE GPU
GRANULAR KIM KOKKOS KSPACE LATTE MANYBODY MC MEAM MISC
MOLECULE MPIIO MSCG OPT PERI POEMS
PYTHON QEQ REAX REPLICA RIGID SHOCK SNAP SRD VORONOI)
set(USER_PACKAGES USER-ATC USER-AWPMD USER-BOCS USER-CGDNA USER-CGSDK USER-COLVARS
USER-DIFFRACTION USER-DPD USER-DRUDE USER-EFF USER-FEP USER-H5MD
USER-INTEL USER-LB USER-MANIFOLD USER-MEAMC USER-MESO
USER-MGPT USER-MISC USER-MOFFF USER-MOLFILE
USER-NETCDF USER-OMP USER-PHONON USER-QMMM USER-QTB
USER-QUIP USER-REAXC USER-SMD USER-SMTBQ USER-SPH USER-TALLY
USER-UEF USER-VTK)
set(PACKAGES_WITH_LIB COMPRESS GPU KIM KOKKOS LATTE MEAM MPIIO MSCG POEMS PYTHON REAX VORONOI
USER-ATC USER-AWPMD USER-COLVARS USER-H5MD USER-LB USER-MOLFILE
USER-NETCDF USER-QMMM USER-QUIP USER-SMD USER-VTK)
set(ALL_PACKAGES ${STANDARD_PACKAGES} ${USER_PACKAGES})
foreach(PKG ${USER_PACKAGES})
set(PKG_${PKG} ON CACHE BOOL "" FORCE)
endforeach()

15
doc/Makefile
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@ -9,6 +9,7 @@ TXT2RST = $(VENV)/bin/txt2rst
ANCHORCHECK = $(VENV)/bin/doc_anchor_check
PYTHON = $(shell which python3)
VIRTUALENV = virtualenv
HAS_PYTHON3 = NO
HAS_VIRTUALENV = NO
@ -16,7 +17,13 @@ ifeq ($(shell which python3 >/dev/null 2>&1; echo $$?), 0)
HAS_PYTHON3 = YES
endif
ifeq ($(shell which virtualenv-3 >/dev/null 2>&1; echo $$?), 0)
VIRTUALENV = virtualenv-3
HAS_VIRTUALENV = YES
endif
ifeq ($(shell which virtualenv >/dev/null 2>&1; echo $$?), 0)
VIRTUALENV = virtualenv
HAS_VIRTUALENV = YES
endif
@ -42,11 +49,11 @@ help:
# ------------------------------------------
clean-all:
clean-all: clean
rm -rf $(BUILDDIR)/* utils/txt2html/txt2html.exe
clean:
rm -rf $(RSTDIR) html
rm -rf $(RSTDIR) html old epub
rm -rf spelling
clean-spelling:
@ -150,7 +157,7 @@ $(RSTDIR)/%.rst : src/%.txt $(TXT2RST)
@(\
mkdir -p $(RSTDIR) ; \
. $(VENV)/bin/activate ;\
txt2rst $< > $@ ;\
txt2rst -v $< > $@ ;\
deactivate ;\
)
@ -158,7 +165,7 @@ $(VENV):
@if [ "$(HAS_PYTHON3)" == "NO" ] ; then echo "Python3 was not found! Please check README.md for further instructions" 1>&2; exit 1; fi
@if [ "$(HAS_VIRTUALENV)" == "NO" ] ; then echo "virtualenv was not found! Please check README.md for further instructions" 1>&2; exit 1; fi
@( \
virtualenv -p $(PYTHON) $(VENV); \
$(VIRTUALENV) -p $(PYTHON) $(VENV); \
. $(VENV)/bin/activate; \
pip install Sphinx; \
pip install sphinxcontrib-images; \

51
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@ -0,0 +1,51 @@
"Previous Section"_Run.html - "LAMMPS WWW Site"_lws -
"LAMMPS Documentation"_ld - "LAMMPS Commands"_lc - "Next
Section"_Packages.html :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html#comm)
:line
Commands :h2
These pages describe how a LAMMPS input script is formatted and the
commands in it are used to define a LAMMPS simulation.
<!-- RST
.. toctree::
Commands_input
Commands_parse
Commands_structure
Commands_category
.. toctree::
Commands_all
Commands_fix
Commands_compute
Commands_pair
Commands_bond
Commands_kspace
END_RST -->
<!-- HTML_ONLY -->
"LAMMPS input scripts"_Commands_input.html
"Parsing rules for input scripts"_Commands_parse.html
"Input script structure"_Commands_structure.html
"Commands by category"_Commands_category.html :all(b)
"All commands"_Commands_all.html
"Fix commands"_Commands_fix.html
"Compute commands"_Commands_compute.html
"Pair commands"_Commands_pair.html
"Bond, angle, dihedral, improper commands"_Commands_bond.html
"KSpace solvers"_Commands_kspace.html :all(b)
<!-- END_HTML_ONLY -->

128
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"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
"All commands"_Commands_all.html,
"Fix styles"_Commands_fix.html,
"Compute styles"_Commands_compute.html,
"Pair styles"_Commands_pair.html,
"Bond styles"_Commands_bond.html,
"Angle styles"_Commands_bond.html#angle,
"Dihedral styles"_Commands_bond.html#dihedral,
"Improper styles"_Commands_bond.html#improper,
"KSpace styles"_Commands_kspace.html :tb(c=3,ea=c)
All commands :h3
An alphabetic list of all LAMMPS commmands.
"angle_coeff"_angle_coeff.html,
"angle_style"_angle_style.html,
"atom_modify"_atom_modify.html,
"atom_style"_atom_style.html,
"balance"_balance.html,
"bond_coeff"_bond_coeff.html,
"bond_style"_bond_style.html,
"bond_write"_bond_write.html,
"boundary"_boundary.html,
"box"_box.html,
"change_box"_change_box.html,
"clear"_clear.html,
"comm_modify"_comm_modify.html,
"comm_style"_comm_style.html,
"compute"_compute.html,
"compute_modify"_compute_modify.html,
"create_atoms"_create_atoms.html,
"create_bonds"_create_bonds.html,
"create_box"_create_box.html,
"delete_atoms"_delete_atoms.html,
"delete_bonds"_delete_bonds.html,
"dielectric"_dielectric.html,
"dihedral_coeff"_dihedral_coeff.html,
"dihedral_style"_dihedral_style.html,
"dimension"_dimension.html,
"displace_atoms"_displace_atoms.html,
"dump"_dump.html,
"dump image"_dump_image.html,
"dump_modify"_dump_modify.html,
"dump movie"_dump_image.html,
"dump netcdf"_dump_netcdf.html,
"dump netcdf/mpiio"_dump_netcdf.html,
"dump vtk"_dump_vtk.html,
"echo"_echo.html,
"fix"_fix.html,
"fix_modify"_fix_modify.html,
"group"_group.html,
"group2ndx"_group2ndx.html,
"if"_if.html,
"info"_info.html,
"improper_coeff"_improper_coeff.html,
"improper_style"_improper_style.html,
"include"_include.html,
"jump"_jump.html,
"kspace_modify"_kspace_modify.html,
"kspace_style"_kspace_style.html,
"label"_label.html,
"lattice"_lattice.html,
"log"_log.html,
"mass"_mass.html,
"minimize"_minimize.html,
"min_modify"_min_modify.html,
"min_style"_min_style.html,
"molecule"_molecule.html,
"ndx2group"_group2ndx.html,
"neb"_neb.html,
"neigh_modify"_neigh_modify.html,
"neighbor"_neighbor.html,
"newton"_newton.html,
"next"_next.html,
"package"_package.html,
"pair_coeff"_pair_coeff.html,
"pair_modify"_pair_modify.html,
"pair_style"_pair_style.html,
"pair_write"_pair_write.html,
"partition"_partition.html,
"prd"_prd.html,
"print"_print.html,
"processors"_processors.html,
"python"_python.html,
"quit"_quit.html,
"read_data"_read_data.html,
"read_dump"_read_dump.html,
"read_restart"_read_restart.html,
"region"_region.html,
"replicate"_replicate.html,
"rerun"_rerun.html,
"reset_ids"_reset_ids.html,
"reset_timestep"_reset_timestep.html,
"restart"_restart.html,
"run"_run.html,
"run_style"_run_style.html,
"set"_set.html,
"shell"_shell.html,
"special_bonds"_special_bonds.html,
"suffix"_suffix.html,
"tad"_tad.html,
"temper"_temper.html,
"temper/grem"_temper_grem.html,
"temper/npt"_temper_npt.html,
"thermo"_thermo.html,
"thermo_modify"_thermo_modify.html,
"thermo_style"_thermo_style.html,
"timer"_timer.html,
"timestep"_timestep.html,
"uncompute"_uncompute.html,
"undump"_undump.html,
"unfix"_unfix.html,
"units"_units.html,
"variable"_variable.html,
"velocity"_velocity.html,
"write_coeff"_write_coeff.html,
"write_data"_write_data.html,
"write_dump"_write_dump.html,
"write_restart"_write_restart.html :tb(c=6,ea=c)

124
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@ -0,0 +1,124 @@
"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
"All commands"_Commands_all.html,
"Fix styles"_Commands_fix.html,
"Compute styles"_Commands_compute.html,
"Pair styles"_Commands_pair.html,
"Bond styles"_Commands_bond.html,
"Angle styles"_Commands_bond.html#angle,
"Dihedral styles"_Commands_bond.html#dihedral,
"Improper styles"_Commands_bond.html#improper,
"KSpace styles"_Commands_kspace.html :tb(c=3,ea=c)
Bond, angle, dihedral, and improper commands :h3
:line
Bond_style potentials :h3,link(bond)
All LAMMPS "bond_style"_bond_style.html commands. Some styles have
accelerated versions. This is indicated by additional letters in
parenthesis: g = GPU, i = USER-INTEL, k = KOKKOS, o = USER-OMP, t =
OPT.
"none"_bond_none.html,
"zero"_bond_zero.html,
"hybrid"_bond_hybrid.html :tb(c=3,ea=c)
"class2 (ko)"_bond_class2.html,
"fene (iko)"_bond_fene.html,
"fene/expand (o)"_bond_fene_expand.html,
"gromos (o)"_bond_gromos.html,
"harmonic (ko)"_bond_harmonic.html,
"harmonic/shift (o)"_bond_harmonic_shift.html,
"harmonic/shift/cut (o)"_bond_harmonic_shift_cut.html,
"morse (o)"_bond_morse.html,
"nonlinear (o)"_bond_nonlinear.html,
"oxdna/fene"_bond_oxdna.html,
"oxdna2/fene"_bond_oxdna.html,
"quartic (o)"_bond_quartic.html,
"table (o)"_bond_table.html :tb(c=4,ea=c)
:line
Angle_style potentials :h3,link(angle)
All LAMMPS "angle_style"_angle_style.html commands. Some styles have
accelerated versions. This is indicated by additional letters in
parenthesis: g = GPU, i = USER-INTEL, k = KOKKOS, o = USER-OMP, t =
OPT.
"none"_angle_none.html,
"zero"_angle_zero.html,
"hybrid"_angle_hybrid.html :tb(c=3,ea=c)
"charmm (ko)"_angle_charmm.html,
"class2 (ko)"_angle_class2.html,
"cosine (o)"_angle_cosine.html,
"cosine/delta (o)"_angle_cosine_delta.html,
"cosine/periodic (o)"_angle_cosine_periodic.html,
"cosine/shift (o)"_angle_cosine_shift.html,
"cosine/shift/exp (o)"_angle_cosine_shift_exp.html,
"cosine/squared (o)"_angle_cosine_squared.html,
"dipole (o)"_angle_dipole.html,
"fourier (o)"_angle_fourier.html,
"fourier/simple (o)"_angle_fourier_simple.html,
"harmonic (iko)"_angle_harmonic.html,
"quartic (o)"_angle_quartic.html,
"sdk"_angle_sdk.html,
"table (o)"_angle_table.html :tb(c=4,ea=c)
:line
Dihedral_style potentials :h3,link(dihedral)
All LAMMPS "dihedral_style"_dihedral_style.html commands. Some styles
have accelerated versions. This is indicated by additional letters in
parenthesis: g = GPU, i = USER-INTEL, k = KOKKOS, o = USER-OMP, t =
OPT.
"none"_dihedral_none.html,
"zero"_dihedral_zero.html,
"hybrid"_dihedral_hybrid.html :tb(c=3,ea=c)
"charmm (iko)"_dihedral_charmm.html,
"charmmfsw"_dihedral_charmm.html,
"class2 (ko)"_dihedral_class2.html,
"cosine/shift/exp (o)"_dihedral_cosine_shift_exp.html,
"fourier (io)"_dihedral_fourier.html,
"harmonic (io)"_dihedral_harmonic.html,
"helix (o)"_dihedral_helix.html,
"multi/harmonic (o)"_dihedral_multi_harmonic.html,
"nharmonic (o)"_dihedral_nharmonic.html,
"opls (iko)"_dihedral_opls.htm;,
"quadratic (o)"_dihedral_quadratic.html,
"spherical (o)"_dihedral_spherical.html,
"table (o)"_dihedral_table.html,
"table/cut"_dihedral_table_cut.html :tb(c=4,ea=c)
:line
Improper_style potentials :h3,link(improper)
All LAMMPS "improper_style"_improper_style.html commands. Some styles
have accelerated versions. This is indicated by additional letters in
parenthesis: g = GPU, i = USER-INTEL, k = KOKKOS, o = USER-OMP, t =
OPT.
"none"_improper_none.html,
"zero"_improper_zero.html,
"hybrid"_improper_hybrid.html :tb(c=3,ea=c)
"class2 (ko)"_improper_class2.html,
"cossq (o)"_improper_cossq.html,
"cvff (io)"_improper_cvff.html,
"distance"_improper_distance.html,
"fourier (o)"_improper_fourier.html,
"harmonic (iko)"_improper_harmonic.html,
"ring (o)"_improper_ring.html,
"umbrella (o)"_improper_umbrella.html :tb(c=4,ea=c)

141
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@ -0,0 +1,141 @@
"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Commands by category :h3
This page lists most of the LAMMPS commands, grouped by category. The
"Commands all"_Commands_all.html doc page lists all commands
alphabetically. It also includes long lists of style options for
entries that appear in the following categories as a single command
(fix, compute, pair, etc).
Initialization:
"newton"_newton.html,
"package"_package.html,
"processors"_processors.html,
"suffix"_suffix.html,
"units"_units.html :ul
Setup simulation box:
"boundary"_boundary.html,
"box"_box.html,
"change_box"_change_box.html,
"create_box"_create_box.html,
"dimension"_dimension.html,
"lattice"_lattice.html,
"region"_region.html :ul
Setup atoms:
"atom_modify"_atom_modify.html,
"atom_style"_atom_style.html,
"balance"_balance.html,
"create_atoms"_create_atoms.html,
"create_bonds"_create_bonds.html,
"delete_atoms"_delete_atoms.html,
"delete_bonds"_delete_bonds.html,
"displace_atoms"_displace_atoms.html,
"group"_group.html,
"mass"_mass.html,
"molecule"_molecule.html,
"read_data"_read_data.html,
"read_dump"_read_dump.html,
"read_restart"_read_restart.html,
"replicate"_replicate.html,
"set"_set.html,
"velocity"_velocity.html :ul
Force fields:
"angle_coeff"_angle_coeff.html,
"angle_style"_angle_style.html,
"bond_coeff"_bond_coeff.html,
"bond_style"_bond_style.html,
"bond_write"_bond_write.html,
"dielectric"_dielectric.html,
"dihedral_coeff"_dihedral_coeff.html,
"dihedral_style"_dihedral_style.html,
"improper_coeff"_improper_coeff.html,
"improper_style"_improper_style.html,
"kspace_modify"_kspace_modify.html,
"kspace_style"_kspace_style.html,
"pair_coeff"_pair_coeff.html,
"pair_modify"_pair_modify.html,
"pair_style"_pair_style.html,
"pair_write"_pair_write.html,
"special_bonds"_special_bonds.html :ul
Settings:
"comm_modify"_comm_modify.html,
"comm_style"_comm_style.html,
"info"_info.html,
"min_modify"_min_modify.html,
"min_style"_min_style.html,
"neigh_modify"_neigh_modify.html,
"neighbor"_neighbor.html,
"partition"_partition.html,
"reset_timestep"_reset_timestep.html,
"run_style"_run_style.html,
"timer"_timer.html,
"timestep"_timestep.html :ul
Operations within timestepping (fixes) and diagnostics (computes):
"compute"_compute.html,
"compute_modify"_compute_modify.html,
"fix"_fix.html,
"fix_modify"_fix_modify.html,
"uncompute"_uncompute.html,
"unfix"_unfix.html :ul
Output:
"dump image"_dump_image.html,
"dump movie"_dump_image.html,
"dump"_dump.html,
"dump_modify"_dump_modify.html,
"restart"_restart.html,
"thermo"_thermo.html,
"thermo_modify"_thermo_modify.html,
"thermo_style"_thermo_style.html,
"undump"_undump.html,
"write_coeff"_write_coeff.html,
"write_data"_write_data.html,
"write_dump"_write_dump.html,
"write_restart"_write_restart.html :ul
Actions:
"minimize"_minimize.html,
"neb"_neb.html,
"prd"_prd.html,
"rerun"_rerun.html,
"run"_run.html,
"tad"_tad.html,
"temper"_temper.html :ul
Input script control:
"clear"_clear.html,
"echo"_echo.html,
"if"_if.html,
"include"_include.html,
"jump"_jump.html,
"label"_label.html,
"log"_log.html,
"next"_next.html,
"print"_print.html,
"python"_python.html,
"quit"_quit.html,
"shell"_shell.html,
"variable"_variable.html :ul

153
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@ -0,0 +1,153 @@
"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
"All commands"_Commands_all.html,
"Fix styles"_Commands_fix.html,
"Compute styles"_Commands_compute.html,
"Pair styles"_Commands_pair.html,
"Bond styles"_Commands_bond.html,
"Angle styles"_Commands_bond.html#angle,
"Dihedral styles"_Commands_bond.html#dihedral,
"Improper styles"_Commands_bond.html#improper,
"KSpace styles"_Commands_kspace.html :tb(c=3,ea=c)
Compute commands :h3
An alphabetic list of all LAMMPS "compute"_compute.html commands.
Some styles have accelerated versions. This is indicated by
additional letters in parenthesis: g = GPU, i = USER-INTEL, k =
KOKKOS, o = USER-OMP, t = OPT.
"ackland/atom"_compute_ackland_atom.html,
"aggregate/atom"_compute_cluster_atom.html,
"angle"_compute_angle.html,
"angle/local"_compute_angle_local.html,
"angmom/chunk"_compute_angmom_chunk.html,
"basal/atom"_compute_basal_atom.html,
"body/local"_compute_body_local.html,
"bond"_compute_bond.html,
"bond/local"_compute_bond_local.html,
"centro/atom"_compute_centro_atom.html,
"chunk/atom"_compute_chunk_atom.html,
"cluster/atom"_compute_cluster_atom.html,
"cna/atom"_compute_cna_atom.html,
"cnp/atom"_compute_cnp_atom.html,
"com"_compute_com.html,
"com/chunk"_compute_com_chunk.html,
"contact/atom"_compute_contact_atom.html,
"coord/atom"_compute_coord_atom.html,
"damage/atom"_compute_damage_atom.html,
"dihedral"_compute_dihedral.html,
"dihedral/local"_compute_dihedral_local.html,
"dilatation/atom"_compute_dilatation_atom.html,
"dipole/chunk"_compute_dipole_chunk.html,
"displace/atom"_compute_displace_atom.html,
"dpd"_compute_dpd.html,
"dpd/atom"_compute_dpd_atom.html,
"edpd/temp/atom"_compute_edpd_temp_atom.html,
"entropy/atom"_compute_entropy_atom.html,
"erotate/asphere"_compute_erotate_asphere.html,
"erotate/rigid"_compute_erotate_rigid.html,
"erotate/sphere"_compute_erotate_sphere.html,
"erotate/sphere/atom"_compute_erotate_sphere_atom.html,
"event/displace"_compute_event_displace.html,
"fep"_compute_fep.html,
"force/tally"_compute_tally.html,
"fragment/atom"_compute_cluster_atom.html,
"global/atom"_compute_global_atom.html,
"group/group"_compute_group_group.html,
"gyration"_compute_gyration.html,
"gyration/chunk"_compute_gyration_chunk.html,
"heat/flux"_compute_heat_flux.html,
"heat/flux/tally"_compute_tally.html,
"hexorder/atom"_compute_hexorder_atom.html,
"improper"_compute_improper.html,
"improper/local"_compute_improper_local.html,
"inertia/chunk"_compute_inertia_chunk.html,
"ke"_compute_ke.html,
"ke/atom"_compute_ke_atom.html,
"ke/atom/eff"_compute_ke_atom_eff.html,
"ke/eff"_compute_ke_eff.html,
"ke/rigid"_compute_ke_rigid.html,
"meso/e/atom"_compute_meso_e_atom.html,
"meso/rho/atom"_compute_meso_rho_atom.html,
"meso/t/atom"_compute_meso_t_atom.html,
"msd"_compute_msd.html,
"msd/chunk"_compute_msd_chunk.html,
"msd/nongauss"_compute_msd_nongauss.html,
"omega/chunk"_compute_omega_chunk.html,
"orientorder/atom"_compute_orientorder_atom.html,
"pair"_compute_pair.html,
"pair/local"_compute_pair_local.html,
"pe"_compute_pe.html,
"pe/atom"_compute_pe_atom.html,
"pe/mol/tally"_compute_tally.html,
"pe/tally"_compute_tally.html,
"plasticity/atom"_compute_plasticity_atom.html,
"pressure"_compute_pressure.html,
"pressure/uef"_compute_pressure_uef.html,
"property/atom"_compute_property_atom.html,
"property/chunk"_compute_property_chunk.html,
"property/local"_compute_property_local.html,
"rdf"_compute_rdf.html,
"reduce"_compute_reduce.html,
"reduce/region"_compute_reduce.html,
"rigid/local"_compute_rigid_local.html,
"saed"_compute_saed.html,
"slice"_compute_slice.html,
"smd/contact/radius"_compute_smd_contact_radius.html,
"smd/damage"_compute_smd_damage.html,
"smd/hourglass/error"_compute_smd_hourglass_error.html,
"smd/internal/energy"_compute_smd_internal_energy.html,
"smd/plastic/strain"_compute_smd_plastic_strain.html,
"smd/plastic/strain/rate"_compute_smd_plastic_strain_rate.html,
"smd/rho"_compute_smd_rho.html,
"smd/tlsph/defgrad"_compute_smd_tlsph_defgrad.html,
"smd/tlsph/dt"_compute_smd_tlsph_dt.html,
"smd/tlsph/num/neighs"_compute_smd_tlsph_num_neighs.html,
"smd/tlsph/shape"_compute_smd_tlsph_shape.html,
"smd/tlsph/strain"_compute_smd_tlsph_strain.html,
"smd/tlsph/strain/rate"_compute_smd_tlsph_strain_rate.html,
"smd/tlsph/stress"_compute_smd_tlsph_stress.html,
"smd/triangle/mesh/vertices"_compute_smd_triangle_mesh_vertices.html,
"smd/ulsph/num/neighs"_compute_smd_ulsph_num_neighs.html,
"smd/ulsph/strain"_compute_smd_ulsph_strain.html,
"smd/ulsph/strain/rate"_compute_smd_ulsph_strain_rate.html,
"smd/ulsph/stress"_compute_smd_ulsph_stress.html,
"smd/vol"_compute_smd_vol.html,
"sna/atom"_compute_sna_atom.html,
"snad/atom"_compute_sna_atom.html,
"snav/atom"_compute_sna_atom.html,
"spin"_compute_spin.html,
"stress/atom"_compute_stress_atom.html,
"stress/tally"_compute_tally.html,
"tdpd/cc/atom"_compute_tdpd_cc_atom.html,
"temp (k)"_compute_temp.html,
"temp/asphere"_compute_temp_asphere.html,
"temp/body"_compute_temp_body.html,
"temp/chunk"_compute_temp_chunk.html,
"temp/com"_compute_temp_com.html,
"temp/deform"_compute_temp_deform.html,
"temp/deform/eff"_compute_temp_deform_eff.html,
"temp/drude"_compute_temp_drude.html,
"temp/eff"_compute_temp_eff.html,
"temp/partial"_compute_temp_partial.html,
"temp/profile"_compute_temp_profile.html,
"temp/ramp"_compute_temp_ramp.html,
"temp/region"_compute_temp_region.html,
"temp/region/eff"_compute_temp_region_eff.html,
"temp/rotate"_compute_temp_rotate.html,
"temp/sphere"_compute_temp_sphere.html,
"temp/uef"_compute_temp_uef.html,
"ti"_compute_ti.html,
"torque/chunk"_compute_torque_chunk.html,
"vacf"_compute_vacf.html,
"vcm/chunk"_compute_vcm_chunk.html,
"voronoi/atom"_compute_voronoi_atom.html,
"xrd"_compute_xrd.html :tb(c=6,ea=c)

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@ -0,0 +1,229 @@
"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
"All commands"_Commands_all.html,
"Fix styles"_Commands_fix.html,
"Compute styles"_Commands_compute.html,
"Pair styles"_Commands_pair.html,
"Bond styles"_Commands_bond.html,
"Angle styles"_Commands_bond.html#angle,
"Dihedral styles"_Commands_bond.html#dihedral,
"Improper styles"_Commands_bond.html#improper,
"KSpace styles"_Commands_kspace.html :tb(c=3,ea=c)
Fix commands :h3
An alphabetic list of all LAMMPS "fix"_fix.html commands. Some styles
have accelerated versions. This is indicated by additional letters in
parenthesis: g = GPU, i = USER-INTEL, k = KOKKOS, o = USER-OMP, t =
OPT.
"adapt"_fix_adapt.html,
"adapt/fep"_fix_adapt_fep.html,
"addforce"_fix_addforce.html,
"addtorque"_fix_addtorque.html,
"append/atoms"_fix_append_atoms.html,
"atc"_fix_atc.html,
"atom/swap"_fix_atom_swap.html,
"ave/atom"_fix_ave_atom.html,
"ave/chunk"_fix_ave_chunk.html,
"ave/correlate"_fix_ave_correlate.html,
"ave/correlate/long"_fix_ave_correlate_long.html,
"ave/histo"_fix_ave_histo.html,
"ave/histo/weight"_fix_ave_histo.html,
"ave/time"_fix_ave_time.html,
"aveforce"_fix_aveforce.html,
"balance"_fix_balance.html,
"bond/break"_fix_bond_break.html,
"bond/create"_fix_bond_create.html,
"bond/react"_fix_bond_react.html,
"bond/swap"_fix_bond_swap.html,
"box/relax"_fix_box_relax.html,
"cmap"_fix_cmap.html,
"colvars"_fix_colvars.html,
"controller"_fix_controller.html,
"deform (k)"_fix_deform.html,
"deposit"_fix_deposit.html,
"dpd/energy (k)"_fix_dpd_energy.html,
"drag"_fix_drag.html,
"drude"_fix_drude.html,
"drude/transform/direct"_fix_drude_transform.html,
"drude/transform/reverse"_fix_drude_transform.html,
"dt/reset"_fix_dt_reset.html,
"edpd/source"_fix_dpd_source.html,
"efield"_fix_efield.html,
"ehex"_fix_ehex.html,
"enforce2d (k)"_fix_enforce2d.html,
"eos/cv"_fix_eos_cv.html,
"eos/table"_fix_eos_table.html,
"eos/table/rx (k)"_fix_eos_table_rx.html,
"evaporate"_fix_evaporate.html,
"external"_fix_external.html,
"filter/corotate"_fix_filter_corotate.html,
"flow/gauss"_fix_flow_gauss.html,
"freeze"_fix_freeze.html,
"gcmc"_fix_gcmc.html,
"gld"_fix_gld.html,
"gle"_fix_gle.html,
"gravity (o)"_fix_gravity.html,
"grem"_fix_grem.html,
"halt"_fix_halt.html,
"heat"_fix_heat.html,
"imd"_fix_imd.html,
"indent"_fix_indent.html,
"ipi"_fix_ipi.html,
"langevin (k)"_fix_langevin.html,
"langevin/drude"_fix_langevin_drude.html,
"langevin/eff"_fix_langevin_eff.html,
"langevin/spin"_fix_langevin_spin.html,
"latte"_fix_latte.html,
"lb/fluid"_fix_lb_fluid.html,
"lb/momentum"_fix_lb_momentum.html,
"lb/pc"_fix_lb_pc.html,
"lb/rigid/pc/sphere"_fix_lb_rigid_pc_sphere.html,
"lb/viscous"_fix_lb_viscous.html,
"lineforce"_fix_lineforce.html,
"manifoldforce"_fix_manifoldforce.html,
"meso"_fix_meso.html,
"meso/stationary"_fix_meso_stationary.html,
"momentum (k)"_fix_momentum.html,
"move"_fix_move.html,
"mscg"_fix_mscg.html,
"msst"_fix_msst.html,
"mvv/dpd"_fix_mvv_dpd.html,
"mvv/edpd"_fix_mvv_dpd.html,
"mvv/tdpd"_fix_mvv_dpd.html,
"neb"_fix_neb.html,
"nph (ko)"_fix_nh.html,
"nph/asphere (o)"_fix_nph_asphere.html,
"nph/body"_fix_nph_body.html,
"nph/eff"_fix_nh_eff.html,
"nph/sphere (o)"_fix_nph_sphere.html,
"nphug (o)"_fix_nphug.html,
"npt (kio)"_fix_nh.html,
"npt/asphere (o)"_fix_npt_asphere.html,
"npt/body"_fix_npt_body.html,
"npt/eff"_fix_nh_eff.html,
"npt/sphere (o)"_fix_npt_sphere.html,
"npt/uef"_fix_nh_uef.html,
"nve (kio)"_fix_nve.html,
"nve/asphere (i)"_fix_nve_asphere.html,
"nve/asphere/noforce"_fix_nve_asphere_noforce.html,
"nve/body"_fix_nve_body.html,
"nve/dot"_fix_nve_dot.html,
"nve/dotc/langevin"_fix_nve_dotc_langevin.html,
"nve/eff"_fix_nve_eff.html,
"nve/limit"_fix_nve_limit.html,
"nve/line"_fix_nve_line.html,
"nve/manifold/rattle"_fix_nve_manifold_rattle.html,
"nve/noforce"_fix_nve_noforce.html,
"nve/sphere (o)"_fix_nve_sphere.html,
"nve/spin"_fix_nve_spin.html,
"nve/tri"_fix_nve_tri.html,
"nvk"_fix_nvk.html,
"nvt (iko)"_fix_nh.html,
"nvt/asphere (o)"_fix_nvt_asphere.html,
"nvt/body"_fix_nvt_body.html,
"nvt/eff"_fix_nh_eff.html,
"nvt/manifold/rattle"_fix_nvt_manifold_rattle.html,
"nvt/sllod (io)"_fix_nvt_sllod.html,
"nvt/sllod/eff"_fix_nvt_sllod_eff.html,
"nvt/sphere (o)"_fix_nvt_sphere.html,
"nvt/uef"_fix_nh_uef.html,
"oneway"_fix_oneway.html,
"orient/bcc"_fix_orient.html,
"orient/fcc"_fix_orient.html,
"phonon"_fix_phonon.html,
"pimd"_fix_pimd.html,
"planeforce"_fix_planeforce.html,
"poems"_fix_poems.html,
"pour"_fix_pour.html,
"precession/spin"_fix_precession_spin.html,
"press/berendsen"_fix_press_berendsen.html,
"print"_fix_print.html,
"property/atom (k)"_fix_property_atom.html,
"python/invoke"_fix_python_invoke.html,
"python/move"_fix_python_move.html,
"qbmsst"_fix_qbmsst.html,
"qeq/comb (o)"_fix_qeq_comb.html,
"qeq/dynamic"_fix_qeq.html,
"qeq/fire"_fix_qeq.html,
"qeq/point"_fix_qeq.html,
"qeq/reax (ko)"_fix_qeq_reax.html,
"qeq/shielded"_fix_qeq.html,
"qeq/slater"_fix_qeq.html,
"qmmm"_fix_qmmm.html,
"qtb"_fix_qtb.html,
"rattle"_fix_shake.html,
"reax/bonds"_fix_reax_bonds.html,
"reax/c/bonds (k)"_fix_reax_bonds.html,
"reax/c/species (k)"_fix_reaxc_species.html,
"recenter"_fix_recenter.html,
"restrain"_fix_restrain.html,
"rhok"_fix_rhok.html,
"rigid (o)"_fix_rigid.html,
"rigid/nph (o)"_fix_rigid.html,
"rigid/npt (o)"_fix_rigid.html,
"rigid/nve (o)"_fix_rigid.html,
"rigid/nvt (o)"_fix_rigid.html,
"rigid/small (o)"_fix_rigid.html,
"rigid/small/nph"_fix_rigid.html,
"rigid/small/npt"_fix_rigid.html,
"rigid/small/nve"_fix_rigid.html,
"rigid/small/nvt"_fix_rigid.html,
"rx (k)"_fix_rx.html,
"saed/vtk"_fix_saed_vtk.html,
"setforce (k)"_fix_setforce.html,
"shake"_fix_shake.html,
"shardlow (k)"_fix_shardlow.html,
"smd"_fix_smd.html,
"smd/adjust/dt"_fix_smd_adjust_dt.html,
"smd/integrate/tlsph"_fix_smd_integrate_tlsph.html,
"smd/integrate/ulsph"_fix_smd_integrate_ulsph.html,
"smd/move/triangulated/surface"_fix_smd_move_triangulated_surface.html,
"smd/setvel"_fix_smd_setvel.html,
"smd/wall/surface"_fix_smd_wall_surface.html,
"spring"_fix_spring.html,
"spring/chunk"_fix_spring_chunk.html,
"spring/rg"_fix_spring_rg.html,
"spring/self"_fix_spring_self.html,
"srd"_fix_srd.html,
"store/force"_fix_store_force.html,
"store/state"_fix_store_state.html,
"tdpd/source"_fix_dpd_source.html,
"temp/berendsen"_fix_temp_berendsen.html,
"temp/csld"_fix_temp_csvr.html,
"temp/csvr"_fix_temp_csvr.html,
"temp/rescale"_fix_temp_rescale.html,
"temp/rescale/eff"_fix_temp_rescale_eff.html,
"tfmc"_fix_tfmc.html,
"thermal/conductivity"_fix_thermal_conductivity.html,
"ti/spring"_fix_ti_spring.html,
"tmd"_fix_tmd.html,
"ttm"_fix_ttm.html,
"ttm/mod"_fix_ttm.html,
"tune/kspace"_fix_tune_kspace.html,
"vector"_fix_vector.html,
"viscosity"_fix_viscosity.html,
"viscous"_fix_viscous.html,
"wall/body/polygon"_fix_wall_body_polygon.html,
"wall/body/polyhedron"_fix_wall_body_polyhedron.html,
"wall/colloid"_fix_wall.html,
"wall/ees"_fix_wall_ees.html,
"wall/gran"_fix_wall_gran.html,
"wall/gran/region"_fix_wall_gran_region.html,
"wall/harmonic"_fix_wall.html,
"wall/lj1043"_fix_wall.html,
"wall/lj126"_fix_wall.html,
"wall/lj93 (k)"_fix_wall.html,
"wall/piston"_fix_wall_piston.html,
"wall/reflect (k)"_fix_wall_reflect.html,
"wall/region"_fix_wall_region.html,
"wall/region/ees"_fix_wall_ees.html,
"wall/srd"_fix_wall_srd.html :tb(c=8,ea=c)

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"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
LAMMPS input scripts :h3
LAMMPS executes by reading commands from a input script (text file),
one line at a time. When the input script ends, LAMMPS exits. Each
command causes LAMMPS to take some action. It may set an internal
variable, read in a file, or run a simulation. Most commands have
default settings, which means you only need to use the command if you
wish to change the default.
In many cases, the ordering of commands in an input script is not
important. However the following rules apply:
(1) LAMMPS does not read your entire input script and then perform a
simulation with all the settings. Rather, the input script is read
one line at a time and each command takes effect when it is read.
Thus this sequence of commands:
timestep 0.5
run 100
run 100 :pre
does something different than this sequence:
run 100
timestep 0.5
run 100 :pre
In the first case, the specified timestep (0.5 fs) is used for two
simulations of 100 timesteps each. In the 2nd case, the default
timestep (1.0 fs) is used for the 1st 100 step simulation and a 0.5 fs
timestep is used for the 2nd one.
(2) Some commands are only valid when they follow other commands. For
example you cannot set the temperature of a group of atoms until atoms
have been defined and a group command is used to define which atoms
belong to the group.
(3) Sometimes command B will use values that can be set by command A.
This means command A must precede command B in the input script if it
is to have the desired effect. For example, the
"read_data"_read_data.html command initializes the system by setting
up the simulation box and assigning atoms to processors. If default
values are not desired, the "processors"_processors.html and
"boundary"_boundary.html commands need to be used before read_data to
tell LAMMPS how to map processors to the simulation box.
Many input script errors are detected by LAMMPS and an ERROR or
WARNING message is printed. The "Errors"_Errors.html doc page gives
more information on what errors mean. The documentation for each
command lists restrictions on how the command can be used.

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"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands.html)
:line
"All commands"_Commands_all.html,
"Fix styles"_Commands_fix.html,
"Compute styles"_Commands_compute.html,
"Pair styles"_Commands_pair.html,
"Bond styles"_Commands_bond.html,
"Angle styles"_Commands_bond.html#angle,
"Dihedral styles"_Commands_bond.html#dihedral,
"Improper styles"_Commands_bond.html#improper,
"KSpace styles"_Commands_kspace.html :tb(c=3,ea=c)
KSpace solvers :h3
All LAMMPS "kspace_style"_kspace_style.html solvers. Some styles have
accelerated versions. This is indicated by additional letters in
parenthesis: g = GPU, i = USER-INTEL, k = KOKKOS, o = USER-OMP, t =
OPT.
"ewald (o)"_kspace_style.html,
"ewald/disp"_kspace_style.html,
"msm (o)"_kspace_style.html,
"msm/cg (o)"_kspace_style.html,
"pppm (gok)"_kspace_style.html,
"pppm/cg (o)"_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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"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
"All commands"_Commands_all.html,
"Fix styles"_Commands_fix.html,
"Compute styles"_Commands_compute.html,
"Pair styles"_Commands_pair.html,
"Bond styles"_Commands_bond.html,
"Angle styles"_Commands_bond.html#angle,
"Dihedral styles"_Commands_bond.html#dihedral,
"Improper styles"_Commands_bond.html#improper,
"KSpace styles"_Commands_kspace.html :tb(c=3,ea=c)
Pair_style potentials :h3
All LAMMPS "pair_style"_pair_style.html commands. Some styles have
accelerated versions. This is indicated by additional letters in
parenthesis: g = GPU, i = USER-INTEL, k = KOKKOS, o = USER-OMP, t =
OPT.
"none"_pair_none.html,
"zero"_pair_zero.html,
"hybrid"_pair_hybrid.html,
"hybrid/overlay (k)"_pair_hybrid.html :tb(c=4,ea=c)
"adp (o)"_pair_adp.html,
"agni (o)"_pair_agni.html,
"airebo (oi)"_pair_airebo.html,
"airebo/morse (oi)"_pair_airebo.html,
"awpmd/cut"_pair_awpmd.html,
"beck (go)"_pair_beck.html,
"body/nparticle"_pair_body_nparticle.html,
"body/rounded/polygon"_pair_body_rounded_polygon.html,
"body/rounded/polyhedron"_pair_body_rounded_polyhedron.html,
"bop"_pair_bop.html,
"born (go)"_pair_born.html,
"born/coul/dsf"_pair_born.html,
"born/coul/dsf/cs"_pair_born.html,
"born/coul/long (go)"_pair_born.html,
"born/coul/long/cs"_pair_born.html,
"born/coul/msm (o)"_pair_born.html,
"born/coul/wolf (go)"_pair_born.html,
"born/coul/wolf/cs"_pair_born.html,
"brownian (o)"_pair_brownian.html,
"brownian/poly (o)"_pair_brownian.html,
"buck (giko)"_pair_buck.html,
"buck/coul/cut (giko)"_pair_buck.html,
"buck/coul/long (giko)"_pair_buck.html,
"buck/coul/long/cs"_pair_buck.html,
"buck/coul/msm (o)"_pair_buck.html,
"buck/long/coul/long (o)"_pair_buck_long.html,
"buck/mdf"_pair_mdf.html,
"colloid (go)"_pair_colloid.html,
"comb (o)"_pair_comb.html,
"comb3"_pair_comb.html,
"coul/cut (gko)"_pair_coul.html,
"coul/cut/soft (o)"_pair_lj_soft.html,
"coul/debye (gko)"_pair_coul.html,
"coul/diel (o)"_pair_coul_diel.html,
"coul/dsf (gko)"_pair_coul.html,
"coul/long (gko)"_pair_coul.html,
"coul/long/cs"_pair_coul.html,
"coul/long/soft (o)"_pair_lj_soft.html,
"coul/msm"_pair_coul.html,
"coul/shield"_pair_coul_shield.html,
"coul/streitz"_pair_coul.html,
"coul/wolf (ko)"_pair_coul.html,
"coul/wolf/cs"_pair_coul.html,
"dpd (gio)"_pair_dpd.html,
"dpd/fdt"_pair_dpd_fdt.html,
"dpd/fdt/energy (k)"_pair_dpd_fdt.html,
"dpd/tstat (go)"_pair_dpd.html,
"dsmc"_pair_dsmc.html,
"eam (gikot)"_pair_eam.html,
"eam/alloy (gikot)"_pair_eam.html,
"eam/cd (o)"_pair_eam.html,
"eam/fs (gikot)"_pair_eam.html,
"edip (o)"_pair_edip.html,
"edip/multi"_pair_edip.html,
"edpd"_pair_meso.html,
"eff/cut"_pair_eff.html,
"eim (o)"_pair_eim.html,
"exp6/rx (k)"_pair_exp6_rx.html,
"extep"_pair_extep.html,
"gauss (go)"_pair_gauss.html,
"gauss/cut"_pair_gauss.html,
"gayberne (gio)"_pair_gayberne.html,
"gran/hertz/history (o)"_pair_gran.html,
"gran/hooke (o)"_pair_gran.html,
"gran/hooke/history (o)"_pair_gran.html,
"gw"_pair_gw.html,
"gw/zbl"_pair_gw.html,
"hbond/dreiding/lj (o)"_pair_hbond_dreiding.html,
"hbond/dreiding/morse (o)"_pair_hbond_dreiding.html,
"ilp/graphene/hbn"_pair_ilp_graphene_hbn.html,
"kim"_pair_kim.html,
"kolmogorov/crespi/full"_pair_kolmogorov_crespi_full.html,
"kolmogorov/crespi/z"_pair_kolmogorov_crespi_z.html,
"lcbop"_pair_lcbop.html,
"lennard/mdf"_pair_mdf.html,
"line/lj"_pair_line_lj.html,
"list"_pair_list.html,
"lj/charmm/coul/charmm (iko)"_pair_charmm.html,
"lj/charmm/coul/charmm/implicit (ko)"_pair_charmm.html,
"lj/charmm/coul/long (giko)"_pair_charmm.html,
"lj/charmm/coul/long/soft (o)"_pair_charmm.html,
"lj/charmm/coul/msm"_pair_charmm.html,
"lj/charmmfsw/coul/charmmfsh"_pair_charmm.html,
"lj/charmmfsw/coul/long"_pair_charmm.html,
"lj/class2 (gko)"_pair_class2.html,
"lj/class2/coul/cut (ko)"_pair_class2.html,
"lj/class2/coul/long (gko)"_pair_class2.html,
"lj/cubic (go)"_pair_lj_cubic.html,
"lj/cut (gikot)"_pair_lj.html,
"lj/cut/coul/cut (gko)"_pair_lj.html,
"lj/cut/coul/cut/soft (o)"_pair_lj_soft.html,
"lj/cut/coul/debye (gko)"_pair_lj.html,
"lj/cut/coul/dsf (gko)"_pair_lj.html,
"lj/cut/coul/long (gikot)"_pair_lj.html,
"lj/cut/coul/long/cs"_pair_lj.html,
"lj/cut/coul/long/soft (o)"_pair_lj_soft.html,
"lj/cut/coul/msm (go)"_pair_lj.html,
"lj/cut/coul/wolf (o)"_pair_lj.html,
"lj/cut/dipole/cut (go)"_pair_dipole.html,
"lj/cut/dipole/long"_pair_dipole.html,
"lj/cut/dipole/sf (go)"_pair_dipole.html,
"lj/cut/soft (o)"_pair_lj_soft.html,
"lj/cut/thole/long (o)"_pair_thole.html,
"lj/cut/tip4p/cut (o)"_pair_lj.html,
"lj/cut/tip4p/long (ot)"_pair_lj.html,
"lj/cut/tip4p/long/soft (o)"_pair_lj_soft.html,
"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 (io)"_pair_lj_long.html,
"lj/long/dipole/long"_pair_dipole.html,
"lj/long/tip4p/long"_pair_lj_long.html,
"lj/mdf"_pair_mdf.html,
"lj/sdk (gko)"_pair_sdk.html,
"lj/sdk/coul/long (go)"_pair_sdk.html,
"lj/sdk/coul/msm (o)"_pair_sdk.html,
"lj/smooth (o)"_pair_lj_smooth.html,
"lj/smooth/linear (o)"_pair_lj_smooth_linear.html,
"lj96/cut (go)"_pair_lj96.html,
"lubricate (o)"_pair_lubricate.html,
"lubricate/poly (o)"_pair_lubricate.html,
"lubricateU"_pair_lubricateU.html,
"lubricateU/poly"_pair_lubricateU.html,
"mdpd"_pair_meso.html,
"mdpd/rhosum"_pair_meso.html,
"meam"_pair_meam.html,
"meam/c"_pair_meam.html,
"meam/spline (o)"_pair_meam_spline.html,
"meam/sw/spline"_pair_meam_sw_spline.html,
"mgpt"_pair_mgpt.html,
"mie/cut (o)"_pair_mie.html,
"momb"_pair_momb.html,
"morse (gkot)"_pair_morse.html,
"morse/smooth/linear"_pair_morse.html,
"morse/soft"_pair_morse.html,
"multi/lucy"_pair_multi_lucy.html,
"multi/lucy/rx (k)"_pair_multi_lucy_rx.html,
"nb3b/harmonic (o)"_pair_nb3b_harmonic.html,
"nm/cut (o)"_pair_nm.html,
"nm/cut/coul/cut (o)"_pair_nm.html,
"nm/cut/coul/long (o)"_pair_nm.html,
"oxdna/coaxstk"_pair_oxdna.html,
"oxdna/excv"_pair_oxdna.html,
"oxdna/hbond"_pair_oxdna.html,
"oxdna/stk"_pair_oxdna.html,
"oxdna/xstk"_pair_oxdna.html,
"oxdna2/coaxstk"_pair_oxdna2.html,
"oxdna2/dh"_pair_oxdna2.html,
"oxdna2/excv"_pair_oxdna2.html,
"oxdna2/stk"_pair_oxdna2.html,
"peri/eps"_pair_peri.html,
"peri/lps (o)"_pair_peri.html,
"peri/pmb (o)"_pair_peri.html,
"peri/ves"_pair_peri.html,
"polymorphic"_pair_polymorphic.html,
"python"_pair_python.html,
"quip"_pair_quip.html,
"reax"_pair_reax.html,
"reax/c (ko)"_pair_reaxc.html,
"rebo (oi)"_pair_airebo.html,
"resquared (go)"_pair_resquared.html,
"smd/hertz"_pair_smd_hertz.html,
"smd/tlsph"_pair_smd_tlsph.html,
"smd/triangulated/surface"_pair_smd_triangulated_surface.html,
"smd/ulsph"_pair_smd_ulsph.html,
"smtbq"_pair_smtbq.html,
"snap (k)"_pair_snap.html,
"snap (k)"_pair_snap.html,
"soft (go)"_pair_soft.html,
"sph/heatconduction"_pair_sph_heatconduction.html,
"sph/idealgas"_pair_sph_idealgas.html,
"sph/lj"_pair_sph_lj.html,
"sph/rhosum"_pair_sph_rhosum.html,
"sph/taitwater"_pair_sph_taitwater.html,
"sph/taitwater/morris"_pair_sph_taitwater_morris.html,
"spin/dmi"_pair_spin_dmi.html,
"spin/exchange"_pair_spin_exchange.html,
"spin/magelec"_pair_spin_magelec.html,
"spin/neel"_pair_spin_neel.html,
"srp"_pair_srp.html,
"sw (giko)"_pair_sw.html,
"table (gko)"_pair_table.html,
"table/rx (k)"_pair_table_rx.html,
"tdpd"_pair_meso.html,
"tersoff (giko)"_pair_tersoff.html,
"tersoff/mod (gko)"_pair_tersoff_mod.html,
"tersoff/mod/c (o)"_pair_tersoff_mod.html,
"tersoff/table (o)"_pair_tersoff.html,
"tersoff/zbl (gko)"_pair_tersoff_zbl.html,
"thole"_pair_thole.html,
"tip4p/cut (o)"_pair_coul.html,
"tip4p/long (o)"_pair_coul.html,
"tip4p/long/soft (o)"_pair_lj_soft.html,
"tri/lj"_pair_tri_lj.html,
"ufm (got)"_pair_ufm.html,
"vashishta (ko)"_pair_vashishta.html,
"vashishta/table (o)"_pair_vashishta.html,
"yukawa (gok)"_pair_yukawa.html,
"yukawa/colloid (go)"_pair_yukawa_colloid.html,
"zbl (gok)"_pair_zbl.html :tb(c=4,ea=c)

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@ -0,0 +1,136 @@
"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Parsing rules for input scripts :h3
Each non-blank line in the input script is treated as a command.
LAMMPS commands are case sensitive. Command names are lower-case, as
are specified command arguments. Upper case letters may be used in
file names or user-chosen ID strings.
Here are 6 rulse for how each line in the input script is parsed by
LAMMPS:
(1) If the last printable character on the line is a "&" character,
the command is assumed to continue on the next line. The next line is
concatenated to the previous line by removing the "&" character and
line break. This allows long commands to be continued across two or
more lines. See the discussion of triple quotes in (6) for how to
continue a command across multiple line without using "&" characters.
(2) All characters from the first "#" character onward are treated as
comment and discarded. See an exception in (6). Note that a
comment after a trailing "&" character will prevent the command from
continuing on the next line. Also note that for multi-line commands a
single leading "#" will comment out the entire command.
(3) The line is searched repeatedly for $ characters, which indicate
variables that are replaced with a text string. See an exception in
(6).
If the $ is followed by curly brackets, then the variable name is the
text inside the curly brackets. If no curly brackets follow the $,
then the variable name is the single character immediately following
the $. Thus $\{myTemp\} and $x refer to variable names "myTemp" and
"x".
How the variable is converted to a text string depends on what style
of variable it is; see the "variable"_variable.html doc page for details.
It can be a variable that stores multiple text strings, and return one
of them. The returned text string can be multiple "words" (space
separated) which will then be interpreted as multiple arguments in the
input command. The variable can also store a numeric formula which
will be evaluated and its numeric result returned as a string.
As a special case, if the $ is followed by parenthesis, then the text
inside the parenthesis is treated as an "immediate" variable and
evaluated as an "equal-style variable"_variable.html. This is a way
to use numeric formulas in an input script without having to assign
them to variable names. For example, these 3 input script lines:
variable X equal (xlo+xhi)/2+sqrt(v_area)
region 1 block $X 2 INF INF EDGE EDGE
variable X delete :pre
can be replaced by
region 1 block $((xlo+xhi)/2+sqrt(v_area)) 2 INF INF EDGE EDGE :pre
so that you do not have to define (or discard) a temporary variable X.
Additionally, the "immediate" variable expression may be followed by a
colon, followed by a C-style format string, e.g. ":%f" or ":%.10g".
The format string must be appropriate for a double-precision
floating-point value. The format string is used to output the result
of the variable expression evaluation. If a format string is not
specified a high-precision "%.20g" is used as the default.
This can be useful for formatting print output to a desired precion:
print "Final energy per atom: $(pe/atoms:%10.3f) eV/atom" :pre
Note that neither the curly-bracket or immediate form of variables can
contain nested $ characters for other variables to substitute for.
Thus you cannot do this:
variable a equal 2
variable b2 equal 4
print "B2 = $\{b$a\}" :pre
Nor can you specify this $($x-1.0) for an immediate variable, but
you could use $(v_x-1.0), since the latter is valid syntax for an
"equal-style variable"_variable.html.
See the "variable"_variable.html command for more details of how
strings are assigned to variables and evaluated, and how they can be
used in input script commands.
(4) The line is broken into "words" separated by whitespace (tabs,
spaces). Note that words can thus contain letters, digits,
underscores, or punctuation characters.
(5) The first word is the command name. All successive words in the
line are arguments.
(6) If you want text with spaces to be treated as a single argument,
it can be enclosed in either single or double or triple quotes. A
long single argument enclosed in single or double quotes can span
multiple lines if the "&" character is used, as described above. When
the lines are concatenated together (and the "&" characters and line
breaks removed), the text will become a single line. If you want
multiple lines of an argument to retain their line breaks, the text
can be enclosed in triple quotes, in which case "&" characters are not
needed. For example:
print "Volume = $v"
print 'Volume = $v'
if "$\{steps\} > 1000" then quit
variable a string "red green blue &
purple orange cyan"
print """
System volume = $v
System temperature = $t
""" :pre
In each case, the single, double, or triple quotes are removed when
the single argument they enclose is stored internally.
See the "dump modify format"_dump_modify.html, "print"_print.html,
"if"_if.html, and "python"_python.html commands for examples.
A "#" or "$" character that is between quotes will not be treated as a
comment indicator in (2) or substituted for as a variable in (3).
NOTE: If the argument is itself a command that requires a quoted
argument (e.g. using a "print"_print.html command as part of an
"if"_if.html or "run every"_run.html command), then single, double, or
triple quotes can be nested in the usual manner. See the doc pages
for those commands for examples. Only one of level of nesting is
allowed, but that should be sufficient for most use cases.

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"Higher level section"_Commands.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Input script structure :h3
This page describes the structure of a typical LAMMPS input script.
The examples directory in the LAMMPS distribution contains many sample
input scripts; it is discussed on the "Examples"_Examples.html doc
page.
A LAMMPS input script typically has 4 parts:
Initialization
Atom definition
Settings
Run a simulation :ol
The last 2 parts can be repeated as many times as desired. I.e. run a
simulation, change some settings, run some more, etc. Each of the 4
parts is now described in more detail. Remember that almost all
commands need only be used if a non-default value is desired.
(1) Initialization
Set parameters that need to be defined before atoms are created or
read-in from a file.
The relevant commands are "units"_units.html,
"dimension"_dimension.html, "newton"_newton.html,
"processors"_processors.html, "boundary"_boundary.html,
"atom_style"_atom_style.html, "atom_modify"_atom_modify.html.
If force-field parameters appear in the files that will be read, these
commands tell LAMMPS what kinds of force fields are being used:
"pair_style"_pair_style.html, "bond_style"_bond_style.html,
"angle_style"_angle_style.html, "dihedral_style"_dihedral_style.html,
"improper_style"_improper_style.html.
(2) Atom definition
There are 3 ways to define atoms in LAMMPS. Read them in from a data
or restart file via the "read_data"_read_data.html or
"read_restart"_read_restart.html commands. These files can contain
molecular topology information. Or create atoms on a lattice (with no
molecular topology), using these commands: "lattice"_lattice.html,
"region"_region.html, "create_box"_create_box.html,
"create_atoms"_create_atoms.html. The entire set of atoms can be
duplicated to make a larger simulation using the
"replicate"_replicate.html command.
(3) Settings
Once atoms and molecular topology are defined, a variety of settings
can be specified: force field coefficients, simulation parameters,
output options, etc.
Force field coefficients are set by these commands (they can also be
set in the read-in files): "pair_coeff"_pair_coeff.html,
"bond_coeff"_bond_coeff.html, "angle_coeff"_angle_coeff.html,
"dihedral_coeff"_dihedral_coeff.html,
"improper_coeff"_improper_coeff.html,
"kspace_style"_kspace_style.html, "dielectric"_dielectric.html,
"special_bonds"_special_bonds.html.
Various simulation parameters are set by these commands:
"neighbor"_neighbor.html, "neigh_modify"_neigh_modify.html,
"group"_group.html, "timestep"_timestep.html,
"reset_timestep"_reset_timestep.html, "run_style"_run_style.html,
"min_style"_min_style.html, "min_modify"_min_modify.html.
Fixes impose a variety of boundary conditions, time integration, and
diagnostic options. The "fix"_fix.html command comes in many flavors.
Various computations can be specified for execution during a
simulation using the "compute"_compute.html,
"compute_modify"_compute_modify.html, and "variable"_variable.html
commands.
Output options are set by the "thermo"_thermo.html, "dump"_dump.html,
and "restart"_restart.html commands.
(4) Run a simulation
A molecular dynamics simulation is run using the "run"_run.html
command. Energy minimization (molecular statics) is performed using
the "minimize"_minimize.html command. A parallel tempering
(replica-exchange) simulation can be run using the
"temper"_temper.html command.

2
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@ -476,7 +476,7 @@ is the name of the class. This code allows LAMMPS to find your fix
when it parses input script. In addition, your fix header must be
included in the file "style\_fix.h". In case if you use LAMMPS make,
this file is generated automatically - all files starting with prefix
fix\_ are included, so call your header the same way. Otherwise, don<EFBFBD>t
fix\_ are included, so call your header the same way. Otherwise, don't
forget to add your include into "style\_fix.h".
Let's write a simple fix which will print average velocity at the end

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm,tikz}
\usetikzlibrary{automata,arrows,shapes,snakes}
\begin{document}
\begin{varwidth}{50in}
\begin{tikzpicture}
%Global
\node (v1) at (0,6.0) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] { $\bm{v} \leftarrow \bm{v}+L_v.\Delta t/2$ };
\node (s1) at (0,4.5) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] { $\bm{s} \leftarrow \bm{s}+L_s.\Delta t/2$ };
\node (r) at (0,3.0) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] { $\bm{r} \leftarrow \bm{r}+L_r.\Delta t$ };
\node (s2) at (0,1.5) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] { $\bm{s} \leftarrow \bm{s}+L_s.\Delta t/2$ };
\node (v2) at (0,0.0) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] { $\bm{v} \leftarrow \bm{v}+L_v.\Delta t/2$ };
\draw[line width=2pt, ->] (v1) -- (s1);
\draw[line width=2pt, ->] (s1) -- (r);
\draw[line width=2pt, ->] (r) -- (s2);
\draw[line width=2pt, ->] (s2) -- (v2);
%Spin
\node (s01) at (6,6.0) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] {$\bm{s}_0 \leftarrow \bm{s}_0+L_{s_0}.\Delta t/4$ };
\node (sN1) at (6,4.5) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] {$\bm{s}_{\rm N-1}\leftarrow\bm{s}_{\rm N-1}+L_{s_{\rm N-1}}.\Delta t/4$};
\node (sN) at (6,3.0) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] {$\bm{s}_{\rm N} \leftarrow \bm{s}_{\rm N}+L_{s_{\rm N}}.\Delta t/2$ };
\node (sN2) at (6,1.5) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] {$\bm{s}_{\rm N-1}\leftarrow\bm{s}_{\rm N-1}+L_{s_{\rm N-1}}.\Delta t/4$};
\node (s02) at (6,0.0) [draw,thick,minimum width=0.2cm,minimum height=0.2cm] {$\bm{s}_0 \leftarrow \bm{s}_0+L_{s_0}.\Delta t/4$ };
\draw[line width=2pt,dashed, ->] (s01) -- (sN1);
\draw[line width=2pt, ->] (sN1) -- (sN);
\draw[line width=2pt, ->] (sN) -- (sN2);
\draw[line width=2pt,dashed, ->] (sN2) -- (s02);
%from Global to Spin
\draw[line width=2pt, dashed, ->] (s1) -- (s01.west);
\draw[line width=2pt, dashed, ->] (s1) -- (s02.west);
\end{tikzpicture}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath, amssymb, graphics, setspace}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\frac{d \vec{s}_{i}}{dt} = \frac{1}{\left(1+\lambda^2 \right)} \left( \left(
\vec{\omega}_{i} +\vec{\eta} \right) \times \vec{s}_{i} + \lambda\, \vec{s}_{i}
\times\left( \vec{\omega}_{i} \times\vec{s}_{i} \right) \right), \nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\bm{H}_{aniso} = -\sum_{{ i}=1}^{N} K_{an}(\bm{r}_{i})\, \left( \vec{s}_{i} \cdot \vec{n}_{i} \right)^2, \nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\bm{H}_{zeeman} = -\mu_{B}\mu_0\sum_{i=0}^{N}g_{i} \vec{s}_{i} \cdot \vec{H}_{ext} \nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentstyle[12pt]{article}
\begin{document}
\begin{eqnarray*}
F_n &=& k_n \delta_n - c_n v_n, \qquad \delta_n \le 0 \\
&=& -k_{na} \delta_n - c_n v_n, \qquad 0 < \delta_n \le r_c \\
&=& 0 \qquad \qquad \qquad \qquad \delta_n > r_c \\
F_t &=& \mu k_n \delta_n - c_t v_t, \qquad \delta_n \le 0 \\
&=& 0 \qquad \qquad \qquad \qquad \delta_n > 0
\end{eqnarray*}
\end{document}

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\documentclass[12pt]{article}
\begin{document}
\thispagestyle{empty}
$$
s_S^i=-2\pi\rho k_B \int\limits_0^{r_m} \left [ g(r) \ln g(r) - g(r) + 1 \right ] r^2 dr ,
$$
\end{document}

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\documentclass[12pt]{article}
\begin{document}
\thispagestyle{empty}
$$
g_m^i(r) = \frac{1}{4 \pi \rho r^2} \sum\limits_{j} \frac{1}{\sqrt{2 \pi \sigma^2}} e^{-(r-r_{ij})^2/(2\sigma^2)} ,
$$
\end{document}

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\documentclass[12pt]{article}
\begin{document}
\thispagestyle{empty}
$$
\bar{s}_S^i = \frac{\sum_j s_S^j + s_S^i}{N + 1} ,
$$
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\vec{\omega}_i = -\frac{1}{\hbar} \sum_{j}^{Neighb} \vec{s}_{j}\times \left(\vec{e}_{ij}\times \vec{D} \right)
~~{\rm and}~~
\vec{F}_i = -\sum_{j}^{Neighb} \frac{1}{r_{ij}} \vec{D} \times \left( \vec{s}_{i}\times \vec{s}_{j} \right)
, \nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\bm{H}_{dm} = \sum_{{ i,j}=1,i\neq j}^{N}
\left( \vec{e}_{ij} \times \vec{D} \right)
\cdot\left(\vec{s}_{i}\times \vec{s}_{j}\right),
\nonumber
\end{equation}
\end{varwidth}
\end{document}
\vec{D}\left(r_{ij}\right)
{\rm ~and~} \vec{D}\left(r_{ij}\right) = \vec{e}_{ij} \times \vec{D}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\vec{\omega}_{i} = \frac{1}{\hbar} \sum_{j}^{Neighb} {J}
\left(r_{ij} \right)\,\vec{s}_{j}
~~{\rm and}~~
\vec{F}_{i} = \sum_{j}^{Neighb} \frac{\partial {J} \left(r_{ij} \right)}{
\partial r_{ij}} \left( \vec{s}_{i}\cdot \vec{s}_{j} \right) \vec{e}_{ij}
\nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath, amssymb, graphics, setspace}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
{J}\left( r_{ij} \right) = 4 a \left( \frac{r_{ij}}{d} \right)^2 \left( 1 - b \left( \frac{r_{ij}}{d} \right)^2 \right) e^{-\left( \frac{r_{ij}}{d}
\right)^2 }\Theta (R_c - r_{ij}) \nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\bm{H}_{ex} ~=~ -\sum_{i,j,i\neq j}^{N} {J} \left(r_{ij} \right)\, \vec{s}_{i}\cdot \vec{s}_{j} \nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\vec{F}^{i} = -\sum_{j}^{Neighbor} \left( \vec{s}_{i}\times \vec{s}_{j} \right)
\times \vec{E} ~~{\rm and}~~ \vec{\omega}^{i} = -\frac{1}{\hbar}
\sum_{j}^{Neighbor} \vec{s}_j \times \left(\vec{E}\times r_{ij} \right),\nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\vec{\omega}_i = -\frac{1}{\hbar} \sum_{j}^{Neighb} \vec{s}_{j}\times\vec{D}(r_{ij}) ~~{\rm and}~~
\vec{F}_i = -\sum_{j}^{Neighb} \frac{\partial D(r_{ij})}{\partial r_{ij}} \left(\vec{s}_{i}\times \vec{s}_{j} \right) \cdot \vec{r}_{ij}, \nonumber
\end{equation}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{eqnarray}
g_1(r_{ij}) &=& g(r_{ij}) + \frac{12}{35} q(r_{ij}) \nonumber \\
q_1(r_{ij}) &=& \frac{9}{5} q(r_{ij}) \nonumber \\
q_2(r_{ij}) &=& - \frac{2}{5} q(r_{ij}) \nonumber
\end{eqnarray}
\end{varwidth}
\end{document}

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\documentclass[preview]{standalone}
\usepackage{varwidth}
\usepackage[utf8x]{inputenc}
\usepackage{amsmath,amssymb,amsthm,bm}
\begin{document}
\begin{varwidth}{50in}
\begin{equation}
\mathcal{H}_{N\acute{e}el}=-\sum_{{ i,j=1,i\neq j}}^N g_1(r_{ij})\left(({\bm e}_{ij}\cdot {\bm s}_{i})({\bm e}_{ij}
\cdot {\bm s}_{j})-\frac{{\bm s}_{i}\cdot{\bm s}_{j}}{3} \right)
+q_1(r_{ij})\left( ({\bm e}_{ij}\cdot {\bm s}_{i})^2 -\frac{{\bm s}_{i}\cdot{\bm s}_{j}}{3}\right)
\left( ({\bm e}_{ij}\cdot {\bm s}_{i})^2 -\frac{{\bm s}_{i}\cdot{\bm s}_{j}}{3} \right)
+ q_2(r_{ij}) \Big( ({\bm e}_{ij}\cdot {\bm s}_{i}) ({\bm e}_{ij}\cdot {\bm s}_{j})^3 + ({\bm e}_{ij}\cdot
{\bm s}_{j}) ({\bm e}_{ij}\cdot {\bm s}_{i})^3\Big) \nonumber
\end{equation}
\end{varwidth}
\end{document}

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"Previous Section"_Python.html - "LAMMPS WWW Site"_lws -
"LAMMPS Documentation"_ld - "LAMMPS Commands"_lc - "Next
Section"_Manual.html :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Errors :h2
These doc pages describe the errors you can encounter when using
LAMMPS. The common problems include conceptual issues. The messages
and warnings doc pages give complete lists of all the messages the
code may generate (except those generated by USER packages), with
additional details for many of them.
<!-- RST
.. toctree::
Errors_common
Errors_bugs
Errors_messages
Errors_warnings
END_RST -->
<!-- HTML_ONLY -->
"Common problems"_Errors_common.html
"Reporting bugs"_Errors_bugs.html
"Error messages"_Errors_messages.html
"Warning messages"_Errors_warnings.html :all(b)
<!-- END_HTML_ONLY -->

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"Higher level section"_Errors.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Reporting bugs :h3
If you are confident that you have found a bug in LAMMPS, follow these
steps.
Check the "New features and bug
fixes"_http://lammps.sandia.gov/bug.html section of the "LAMMPS WWW
site"_lws to see if the bug has already been reported or fixed or the
"Unfixed bug"_http://lammps.sandia.gov/unbug.html to see if a fix is
pending.
Check the "mailing list"_http://lammps.sandia.gov/mail.html to see if
it has been discussed before.
If not, send an email to the mailing list describing the problem with
any ideas you have as to what is causing it or where in the code the
problem might be. The developers will ask for more info if needed,
such as an input script or data files.
The most useful thing you can do to help us fix the bug is to isolate
the problem. Run it on the smallest number of atoms and fewest number
of processors and with the simplest input script that reproduces the
bug and try to identify what command or combination of commands is
causing the problem.
NOTE: this page needs to have GitHub issues info added

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"Higher level section"_Errors.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Common problems :h3
If two LAMMPS runs do not produce the exact same answer on different
machines or different numbers of processors, this is typically not a
bug. In theory you should get identical answers on any number of
processors and on any machine. In practice, numerical round-off can
cause slight differences and eventual divergence of molecular dynamics
phase space trajectories within a few 100s or few 1000s of timesteps.
However, the statistical properties of the two runs (e.g. average
energy or temperature) should still be the same.
If the "velocity"_velocity.html command is used to set initial atom
velocities, a particular atom can be assigned a different velocity
when the problem is run on a different number of processors or on
different machines. If this happens, the phase space trajectories of
the two simulations will rapidly diverge. See the discussion of the
{loop} option in the "velocity"_velocity.html command for details and
options that avoid this issue.
Similarly, the "create_atoms"_create_atoms.html command generates a
lattice of atoms. For the same physical system, the ordering and
numbering of atoms by atom ID may be different depending on the number
of processors.
Some commands use random number generators which may be setup to
produce different random number streams on each processor and hence
will produce different effects when run on different numbers of
processors. A commonly-used example is the "fix
langevin"_fix_langevin.html command for thermostatting.
A LAMMPS simulation typically has two stages, setup and run. Most
LAMMPS errors are detected at setup time; others like a bond
stretching too far may not occur until the middle of a run.
LAMMPS tries to flag errors and print informative error messages so
you can fix the problem. For most errors it will also print the last
input script command that it was processing. Of course, LAMMPS cannot
figure out your physics or numerical mistakes, like choosing too big a
timestep, specifying erroneous force field coefficients, or putting 2
atoms on top of each other! If you run into errors that LAMMPS
doesn't catch that you think it should flag, please send an email to
the "developers"_http://lammps.sandia.gov/authors.html.
If you get an error message about an invalid command in your input
script, you can determine what command is causing the problem by
looking in the log.lammps file or using the "echo command"_echo.html
to see it on the screen. If you get an error like "Invalid ...
style", with ... being fix, compute, pair, etc, it means that you
mistyped the style name or that the command is part of an optional
package which was not compiled into your executable. The list of
available styles in your executable can be listed by using "the -h
command-line argument"_Section_start.html#start_6. The installation
and compilation of optional packages is explained in the "installation
instructions"_Section_start.html#start_3.
For a given command, LAMMPS expects certain arguments in a specified
order. If you mess this up, LAMMPS will often flag the error, but it
may also simply read a bogus argument and assign a value that is
valid, but not what you wanted. E.g. trying to read the string "abc"
as an integer value of 0. Careful reading of the associated doc page
for the command should allow you to fix these problems. In most cases,
where LAMMPS expects to read a number, either integer or floating point,
it performs a stringent test on whether the provided input actually
is an integer or floating-point number, respectively, and reject the
input with an error message (for instance, when an integer is required,
but a floating-point number 1.0 is provided):
ERROR: Expected integer parameter in input script or data file :pre
Some commands allow for using variable references in place of numeric
constants so that the value can be evaluated and may change over the
course of a run. This is typically done with the syntax {v_name} for a
parameter, where name is the name of the variable. On the other hand,
immediate variable expansion with the syntax ${name} is performed while
reading the input and before parsing commands,
NOTE: Using a variable reference (i.e. {v_name}) is only allowed if
the documentation of the corresponding command explicitly says it is.
Generally, LAMMPS will print a message to the screen and logfile and
exit gracefully when it encounters a fatal error. Sometimes it will
print a WARNING to the screen and logfile and continue on; you can
decide if the WARNING is important or not. A WARNING message that is
generated in the middle of a run is only printed to the screen, not to
the logfile, to avoid cluttering up thermodynamic output. If LAMMPS
crashes or hangs without spitting out an error message first then it
could be a bug (see "this section"_#err_2) or one of the following
cases:
LAMMPS runs in the available memory a processor allows to be
allocated. Most reasonable MD runs are compute limited, not memory
limited, so this shouldn't be a bottleneck on most platforms. Almost
all large memory allocations in the code are done via C-style malloc's
which will generate an error message if you run out of memory.
Smaller chunks of memory are allocated via C++ "new" statements. If
you are unlucky you could run out of memory just when one of these
small requests is made, in which case the code will crash or hang (in
parallel), since LAMMPS doesn't trap on those errors.
Illegal arithmetic can cause LAMMPS to run slow or crash. This is
typically due to invalid physics and numerics that your simulation is
computing. If you see wild thermodynamic values or NaN values in your
LAMMPS output, something is wrong with your simulation. If you
suspect this is happening, it is a good idea to print out
thermodynamic info frequently (e.g. every timestep) via the
"thermo"_thermo.html so you can monitor what is happening.
Visualizing the atom movement is also a good idea to insure your model
is behaving as you expect.
In parallel, one way LAMMPS can hang is due to how different MPI
implementations handle buffering of messages. If the code hangs
without an error message, it may be that you need to specify an MPI
setting or two (usually via an environment variable) to enable
buffering or boost the sizes of messages that can be buffered.

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"Higher level section"_Errors.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Warning messages :h3
This is an alphabetic list of the WARNING messages LAMMPS prints out
and the reason why. If the explanation here is not sufficient, the
documentation for the offending command may help. Warning messages
also list the source file and line number where the warning was
generated. For example, a message lile this:
WARNING: Bond atom missing in box size check (domain.cpp:187) :pre
means that line #187 in the file src/domain.cpp generated the error.
Looking in the source code may help you figure out what went wrong.
Note that warning messages from "user-contributed
packages"_Packages_user.html are not listed here. If such a warning
occurs and is not self-explanatory, you'll need to look in the source
code or contact the author of the package.
Doc page with "ERROR messages"_Errors_messages.html
:line
:dlb
{Adjusting Coulombic cutoff for MSM, new cutoff = %g} :dt
The adjust/cutoff command is turned on and the Coulombic cutoff has been
adjusted to match the user-specified accuracy. :dd
{Angle atoms missing at step %ld} :dt
One or more of 3 atoms needed to compute a particular angle are
missing on this processor. Typically this is because the pairwise
cutoff is set too short or the angle has blown apart and an atom is
too far away. :dd
{Angle style in data file differs from currently defined angle style} :dt
Self-explanatory. :dd
{Atom style in data file differs from currently defined atom style} :dt
Self-explanatory. :dd
{Bond atom missing in box size check} :dt
The 2nd atoms needed to compute a particular bond is missing on this
processor. Typically this is because the pairwise cutoff is set too
short or the bond has blown apart and an atom is too far away. :dd
{Bond atom missing in image check} :dt
The 2nd atom in a particular bond is missing on this processor.
Typically this is because the pairwise cutoff is set too short or the
bond has blown apart and an atom is too far away. :dd
{Bond atoms missing at step %ld} :dt
The 2nd atom needed to compute a particular bond is missing on this
processor. Typically this is because the pairwise cutoff is set too
short or the bond has blown apart and an atom is too far away. :dd
{Bond style in data file differs from currently defined bond style} :dt
Self-explanatory. :dd
{Bond/angle/dihedral extent > half of periodic box length} :dt
This is a restriction because LAMMPS can be confused about which image
of an atom in the bonded interaction is the correct one to use.
"Extent" in this context means the maximum end-to-end length of the
bond/angle/dihedral. LAMMPS computes this by taking the maximum bond
length, multiplying by the number of bonds in the interaction (e.g. 3
for a dihedral) and adding a small amount of stretch. :dd
{Both groups in compute group/group have a net charge; the Kspace boundary correction to energy will be non-zero} :dt
Self-explanatory. :dd
{Calling write_dump before a full system init.} :dt
The write_dump command is used before the system has been fully
initialized as part of a 'run' or 'minimize' command. Not all dump
styles and features are fully supported at this point and thus the
command may fail or produce incomplete or incorrect output. Insert
a "run 0" command, if a full system init is required. :dd
{Cannot count rigid body degrees-of-freedom before bodies are fully initialized} :dt
This means the temperature associated with the rigid bodies may be
incorrect on this timestep. :dd
{Cannot count rigid body degrees-of-freedom before bodies are initialized} :dt
This means the temperature associated with the rigid bodies may be
incorrect on this timestep. :dd
{Cannot include log terms without 1/r terms; setting flagHI to 1} :dt
Self-explanatory. :dd
{Cannot include log terms without 1/r terms; setting flagHI to 1.} :dt
Self-explanatory. :dd
{Charges are set, but coulombic solver is not used} :dt
Self-explanatory. :dd
{Charges did not converge at step %ld: %lg} :dt
Self-explanatory. :dd
{Communication cutoff is too small for SNAP micro load balancing, increased to %lf} :dt
Self-explanatory. :dd
{Compute cna/atom cutoff may be too large to find ghost atom neighbors} :dt
The neighbor cutoff used may not encompass enough ghost atoms
to perform this operation correctly. :dd
{Computing temperature of portions of rigid bodies} :dt
The group defined by the temperature compute does not encompass all
the atoms in one or more rigid bodies, so the change in
degrees-of-freedom for the atoms in those partial rigid bodies will
not be accounted for. :dd
{Create_bonds max distance > minimum neighbor cutoff} :dt
This means atom pairs for some atom types may not be in the neighbor
list and thus no bond can be created between them. :dd
{Delete_atoms cutoff > minimum neighbor cutoff} :dt
This means atom pairs for some atom types may not be in the neighbor
list and thus an atom in that pair cannot be deleted. :dd
{Dihedral atoms missing at step %ld} :dt
One or more of 4 atoms needed to compute a particular dihedral are
missing on this processor. Typically this is because the pairwise
cutoff is set too short or the dihedral has blown apart and an atom is
too far away. :dd
{Dihedral problem} :dt
Conformation of the 4 listed dihedral atoms is extreme; you may want
to check your simulation geometry. :dd
{Dihedral problem: %d %ld %d %d %d %d} :dt
Conformation of the 4 listed dihedral atoms is extreme; you may want
to check your simulation geometry. :dd
{Dihedral style in data file differs from currently defined dihedral style} :dt
Self-explanatory. :dd
{Dump dcd/xtc timestamp may be wrong with fix dt/reset} :dt
If the fix changes the timestep, the dump dcd file will not
reflect the change. :dd
{Energy due to X extra global DOFs will be included in minimizer energies} :dt
When using fixes like box/relax, the potential energy used by the minimizer
is augmented by an additional energy provided by the fix. Thus the printed
converged energy may be different from the total potential energy. :dd
{Energy tally does not account for 'zero yes'} :dt
The energy removed by using the 'zero yes' flag is not accounted
for in the energy tally and thus energy conservation cannot be
monitored in this case. :dd
{Estimated error in splitting of dispersion coeffs is %g} :dt
Error is greater than 0.0001 percent. :dd
{Ewald/disp Newton solver failed, using old method to estimate g_ewald} :dt
Self-explanatory. Choosing a different cutoff value may help. :dd
{FENE bond too long} :dt
A FENE bond has stretched dangerously far. It's interaction strength
will be truncated to attempt to prevent the bond from blowing up. :dd
{FENE bond too long: %ld %d %d %g} :dt
A FENE bond has stretched dangerously far. It's interaction strength
will be truncated to attempt to prevent the bond from blowing up. :dd
{FENE bond too long: %ld %g} :dt
A FENE bond has stretched dangerously far. It's interaction strength
will be truncated to attempt to prevent the bond from blowing up. :dd
{Fix SRD walls overlap but fix srd overlap not set} :dt
You likely want to set this in your input script. :dd
{Fix bond/swap will ignore defined angles} :dt
See the doc page for fix bond/swap for more info on this
restriction. :dd
{Fix deposit near setting < possible overlap separation %g} :dt
This test is performed for finite size particles with a diameter, not
for point particles. The near setting is smaller than the particle
diameter which can lead to overlaps. :dd
{Fix evaporate may delete atom with non-zero molecule ID} :dt
This is probably an error, since you should not delete only one atom
of a molecule. :dd
{Fix gcmc using full_energy option} :dt
Fix gcmc has automatically turned on the full_energy option since it
is required for systems like the one specified by the user. User input
included one or more of the following: kspace, triclinic, a hybrid
pair style, an eam pair style, or no "single" function for the pair
style. :dd
{Fix property/atom mol or charge w/out ghost communication} :dt
A model typically needs these properties defined for ghost atoms. :dd
{Fix qeq CG convergence failed (%g) after %d iterations at %ld step} :dt
Self-explanatory. :dd
{Fix qeq has non-zero lower Taper radius cutoff} :dt
Absolute value must be <= 0.01. :dd
{Fix qeq has very low Taper radius cutoff} :dt
Value should typically be >= 5.0. :dd
{Fix qeq/dynamic tolerance may be too small for damped dynamics} :dt
Self-explanatory. :dd
{Fix qeq/fire tolerance may be too small for damped fires} :dt
Self-explanatory. :dd
{Fix rattle should come after all other integration fixes} :dt
This fix is designed to work after all other integration fixes change
atom positions. Thus it should be the last integration fix specified.
If not, it will not satisfy the desired constraints as well as it
otherwise would. :dd
{Fix recenter should come after all other integration fixes} :dt
Other fixes may change the position of the center-of-mass, so
fix recenter should come last. :dd
{Fix srd SRD moves may trigger frequent reneighboring} :dt
This is because the SRD particles may move long distances. :dd
{Fix srd grid size > 1/4 of big particle diameter} :dt
This may cause accuracy problems. :dd
{Fix srd particle moved outside valid domain} :dt
This may indicate a problem with your simulation parameters. :dd
{Fix srd particles may move > big particle diameter} :dt
This may cause accuracy problems. :dd
{Fix srd viscosity < 0.0 due to low SRD density} :dt
This may cause accuracy problems. :dd
{Fix thermal/conductivity comes before fix ave/spatial} :dt
The order of these 2 fixes in your input script is such that fix
thermal/conductivity comes first. If you are using fix ave/spatial to
measure the temperature profile induced by fix viscosity, then this
may cause a glitch in the profile since you are averaging immediately
after swaps have occurred. Flipping the order of the 2 fixes
typically helps. :dd
{Fix viscosity comes before fix ave/spatial} :dt
The order of these 2 fixes in your input script is such that
fix viscosity comes first. If you are using fix ave/spatial
to measure the velocity profile induced by fix viscosity, then
this may cause a glitch in the profile since you are averaging
immediately after swaps have occurred. Flipping the order
of the 2 fixes typically helps. :dd
{Fixes cannot send data in Kokkos communication, switching to classic communication} :dt
This is current restriction with Kokkos. :dd
{For better accuracy use 'pair_modify table 0'} :dt
The user-specified force accuracy cannot be achieved unless the table
feature is disabled by using 'pair_modify table 0'. :dd
{Geometric mixing assumed for 1/r^6 coefficients} :dt
Self-explanatory. :dd
{Group for fix_modify temp != fix group} :dt
The fix_modify command is specifying a temperature computation that
computes a temperature on a different group of atoms than the fix
itself operates on. This is probably not what you want to do. :dd
{H matrix size has been exceeded: m_fill=%d H.m=%d\n} :dt
This is the size of the matrix. :dd
{Ignoring unknown or incorrect info command flag} :dt
Self-explanatory. An unknown argument was given to the info command.
Compare your input with the documentation. :dd
{Improper atoms missing at step %ld} :dt
One or more of 4 atoms needed to compute a particular improper are
missing on this processor. Typically this is because the pairwise
cutoff is set too short or the improper has blown apart and an atom is
too far away. :dd
{Improper problem: %d %ld %d %d %d %d} :dt
Conformation of the 4 listed improper atoms is extreme; you may want
to check your simulation geometry. :dd
{Improper style in data file differs from currently defined improper style} :dt
Self-explanatory. :dd
{Inconsistent image flags} :dt
The image flags for a pair on bonded atoms appear to be inconsistent.
Inconsistent means that when the coordinates of the two atoms are
unwrapped using the image flags, the two atoms are far apart.
Specifically they are further apart than half a periodic box length.
Or they are more than a box length apart in a non-periodic dimension.
This is usually due to the initial data file not having correct image
flags for the 2 atoms in a bond that straddles a periodic boundary.
They should be different by 1 in that case. This is a warning because
inconsistent image flags will not cause problems for dynamics or most
LAMMPS simulations. However they can cause problems when such atoms
are used with the fix rigid or replicate commands. Note that if you
have an infinite periodic crystal with bonds then it is impossible to
have fully consistent image flags, since some bonds will cross
periodic boundaries and connect two atoms with the same image
flag. :dd
{KIM Model does not provide 'energy'; Potential energy will be zero} :dt
Self-explanatory. :dd
{KIM Model does not provide 'forces'; Forces will be zero} :dt
Self-explanatory. :dd
{KIM Model does not provide 'particleEnergy'; energy per atom will be zero} :dt
Self-explanatory. :dd
{KIM Model does not provide 'particleVirial'; virial per atom will be zero} :dt
Self-explanatory. :dd
{Kspace_modify slab param < 2.0 may cause unphysical behavior} :dt
The kspace_modify slab parameter should be larger to insure periodic
grids padded with empty space do not overlap. :dd
{Less insertions than requested} :dt
The fix pour command was unsuccessful at finding open space
for as many particles as it tried to insert. :dd
{Library error in lammps_gather_atoms} :dt
This library function cannot be used if atom IDs are not defined
or are not consecutively numbered. :dd
{Library error in lammps_scatter_atoms} :dt
This library function cannot be used if atom IDs are not defined or
are not consecutively numbered, or if no atom map is defined. See the
atom_modify command for details about atom maps. :dd
{Lost atoms via change_box: original %ld current %ld} :dt
The command options you have used caused atoms to be lost. :dd
{Lost atoms via displace_atoms: original %ld current %ld} :dt
The command options you have used caused atoms to be lost. :dd
{Lost atoms: original %ld current %ld} :dt
Lost atoms are checked for each time thermo output is done. See the
thermo_modify lost command for options. Lost atoms usually indicate
bad dynamics, e.g. atoms have been blown far out of the simulation
box, or moved further than one processor's sub-domain away before
reneighboring. :dd
{MSM mesh too small, increasing to 2 points in each direction} :dt
Self-explanatory. :dd
{Mismatch between velocity and compute groups} :dt
The temperature computation used by the velocity command will not be
on the same group of atoms that velocities are being set for. :dd
{Mixing forced for lj coefficients} :dt
Self-explanatory. :dd
{Molecule attributes do not match system attributes} :dt
An attribute is specified (e.g. diameter, charge) that is
not defined for the specified atom style. :dd
{Molecule has bond topology but no special bond settings} :dt
This means the bonded atoms will not be excluded in pair-wise
interactions. :dd
{Molecule template for create_atoms has multiple molecules} :dt
The create_atoms command will only create molecules of a single type,
i.e. the first molecule in the template. :dd
{Molecule template for fix gcmc has multiple molecules} :dt
The fix gcmc command will only create molecules of a single type,
i.e. the first molecule in the template. :dd
{Molecule template for fix shake has multiple molecules} :dt
The fix shake command will only recognize molecules of a single
type, i.e. the first molecule in the template. :dd
{More than one compute centro/atom} :dt
It is not efficient to use compute centro/atom more than once. :dd
{More than one compute cluster/atom} :dt
It is not efficient to use compute cluster/atom more than once. :dd
{More than one compute cna/atom defined} :dt
It is not efficient to use compute cna/atom more than once. :dd
{More than one compute contact/atom} :dt
It is not efficient to use compute contact/atom more than once. :dd
{More than one compute coord/atom} :dt
It is not efficient to use compute coord/atom more than once. :dd
{More than one compute damage/atom} :dt
It is not efficient to use compute ke/atom more than once. :dd
{More than one compute dilatation/atom} :dt
Self-explanatory. :dd
{More than one compute erotate/sphere/atom} :dt
It is not efficient to use compute erorate/sphere/atom more than once. :dd
{More than one compute hexorder/atom} :dt
It is not efficient to use compute hexorder/atom more than once. :dd
{More than one compute ke/atom} :dt
It is not efficient to use compute ke/atom more than once. :dd
{More than one compute orientorder/atom} :dt
It is not efficient to use compute orientorder/atom more than once. :dd
{More than one compute plasticity/atom} :dt
Self-explanatory. :dd
{More than one compute sna/atom} :dt
Self-explanatory. :dd
{More than one compute snad/atom} :dt
Self-explanatory. :dd
{More than one compute snav/atom} :dt
Self-explanatory. :dd
{More than one fix poems} :dt
It is not efficient to use fix poems more than once. :dd
{More than one fix rigid} :dt
It is not efficient to use fix rigid more than once. :dd
{Neighbor exclusions used with KSpace solver may give inconsistent Coulombic energies} :dt
This is because excluding specific pair interactions also excludes
them from long-range interactions which may not be the desired effect.
The special_bonds command handles this consistently by insuring
excluded (or weighted) 1-2, 1-3, 1-4 interactions are treated
consistently by both the short-range pair style and the long-range
solver. This is not done for exclusions of charged atom pairs via the
neigh_modify exclude command. :dd
{New thermo_style command, previous thermo_modify settings will be lost} :dt
If a thermo_style command is used after a thermo_modify command, the
settings changed by the thermo_modify command will be reset to their
default values. This is because the thermo_modify command acts on
the currently defined thermo style, and a thermo_style command creates
a new style. :dd
{No Kspace calculation with verlet/split} :dt
The 2nd partition performs a kspace calculation so the kspace_style
command must be used. :dd
{No automatic unit conversion to XTC file format conventions possible for units lj} :dt
This means no scaling will be performed. :dd
{No fixes defined, atoms won't move} :dt
If you are not using a fix like nve, nvt, npt then atom velocities and
coordinates will not be updated during timestepping. :dd
{No joints between rigid bodies, use fix rigid instead} :dt
The bodies defined by fix poems are not connected by joints. POEMS
will integrate the body motion, but it would be more efficient to use
fix rigid. :dd
{Not using real units with pair reax} :dt
This is most likely an error, unless you have created your own ReaxFF
parameter file in a different set of units. :dd
{Number of MSM mesh points changed to be a multiple of 2} :dt
MSM requires that the number of grid points in each direction be a multiple
of two and the number of grid points in one or more directions have been
adjusted to meet this requirement. :dd
{OMP_NUM_THREADS environment is not set.} :dt
This environment variable must be set appropriately to use the
USER-OMP package. :dd
{One or more atoms are time integrated more than once} :dt
This is probably an error since you typically do not want to
advance the positions or velocities of an atom more than once
per timestep. :dd
{One or more chunks do not contain all atoms in molecule} :dt
This may not be what you intended. :dd
{One or more dynamic groups may not be updated at correct point in timestep} :dt
If there are other fixes that act immediately after the initial stage
of time integration within a timestep (i.e. after atoms move), then
the command that sets up the dynamic group should appear after those
fixes. This will insure that dynamic group assignments are made
after all atoms have moved. :dd
{One or more respa levels compute no forces} :dt
This is computationally inefficient. :dd
{Pair COMB charge %.10f with force %.10f hit max barrier} :dt
Something is possibly wrong with your model. :dd
{Pair COMB charge %.10f with force %.10f hit min barrier} :dt
Something is possibly wrong with your model. :dd
{Pair brownian needs newton pair on for momentum conservation} :dt
Self-explanatory. :dd
{Pair dpd needs newton pair on for momentum conservation} :dt
Self-explanatory. :dd
{Pair dsmc: num_of_collisions > number_of_A} :dt
Collision model in DSMC is breaking down. :dd
{Pair dsmc: num_of_collisions > number_of_B} :dt
Collision model in DSMC is breaking down. :dd
{Pair style in data file differs from currently defined pair style} :dt
Self-explanatory. :dd
{Pair style restartinfo set but has no restart support} :dt
This pair style has a bug, where it does not support reading and
writing information to a restart file, but does not set the member
variable "restartinfo" to 0 as required in that case. :dd
{Particle deposition was unsuccessful} :dt
The fix deposit command was not able to insert as many atoms as
needed. The requested volume fraction may be too high, or other atoms
may be in the insertion region. :dd
{Proc sub-domain size < neighbor skin, could lead to lost atoms} :dt
The decomposition of the physical domain (likely due to load
balancing) has led to a processor's sub-domain being smaller than the
neighbor skin in one or more dimensions. Since reneighboring is
triggered by atoms moving the skin distance, this may lead to lost
atoms, if an atom moves all the way across a neighboring processor's
sub-domain before reneighboring is triggered. :dd
{Reducing PPPM order b/c stencil extends beyond nearest neighbor processor} :dt
This may lead to a larger grid than desired. See the kspace_modify overlap
command to prevent changing of the PPPM order. :dd
{Reducing PPPMDisp Coulomb order b/c stencil extends beyond neighbor processor} :dt
This may lead to a larger grid than desired. See the kspace_modify overlap
command to prevent changing of the PPPM order. :dd
{Reducing PPPMDisp dispersion order b/c stencil extends beyond neighbor processor} :dt
This may lead to a larger grid than desired. See the kspace_modify overlap
command to prevent changing of the PPPM order. :dd
{Replacing a fix, but new group != old group} :dt
The ID and style of a fix match for a fix you are changing with a fix
command, but the new group you are specifying does not match the old
group. :dd
{Replicating in a non-periodic dimension} :dt
The parameters for a replicate command will cause a non-periodic
dimension to be replicated; this may cause unwanted behavior. :dd
{Resetting reneighboring criteria during PRD} :dt
A PRD simulation requires that neigh_modify settings be delay = 0,
every = 1, check = yes. Since these settings were not in place,
LAMMPS changed them and will restore them to their original values
after the PRD simulation. :dd
{Resetting reneighboring criteria during TAD} :dt
A TAD simulation requires that neigh_modify settings be delay = 0,
every = 1, check = yes. Since these settings were not in place,
LAMMPS changed them and will restore them to their original values
after the PRD simulation. :dd
{Resetting reneighboring criteria during minimization} :dt
Minimization requires that neigh_modify settings be delay = 0, every =
1, check = yes. Since these settings were not in place, LAMMPS
changed them and will restore them to their original values after the
minimization. :dd
{Restart file used different # of processors} :dt
The restart file was written out by a LAMMPS simulation running on a
different number of processors. Due to round-off, the trajectories of
your restarted simulation may diverge a little more quickly than if
you ran on the same # of processors. :dd
{Restart file used different 3d processor grid} :dt
The restart file was written out by a LAMMPS simulation running on a
different 3d grid of processors. Due to round-off, the trajectories
of your restarted simulation may diverge a little more quickly than if
you ran on the same # of processors. :dd
{Restart file used different boundary settings, using restart file values} :dt
Your input script cannot change these restart file settings. :dd
{Restart file used different newton bond setting, using restart file value} :dt
The restart file value will override the setting in the input script. :dd
{Restart file used different newton pair setting, using input script value} :dt
The input script value will override the setting in the restart file. :dd
{Restrain problem: %d %ld %d %d %d %d} :dt
Conformation of the 4 listed dihedral atoms is extreme; you may want
to check your simulation geometry. :dd
{Running PRD with only one replica} :dt
This is allowed, but you will get no parallel speed-up. :dd
{SRD bin shifting turned on due to small lamda} :dt
This is done to try to preserve accuracy. :dd
{SRD bin size for fix srd differs from user request} :dt
Fix SRD had to adjust the bin size to fit the simulation box. See the
cubic keyword if you want this message to be an error vs warning. :dd
{SRD bins for fix srd are not cubic enough} :dt
The bin shape is not within tolerance of cubic. See the cubic
keyword if you want this message to be an error vs warning. :dd
{SRD particle %d started inside big particle %d on step %ld bounce %d} :dt
See the inside keyword if you want this message to be an error vs
warning. :dd
{SRD particle %d started inside wall %d on step %ld bounce %d} :dt
See the inside keyword if you want this message to be an error vs
warning. :dd
{Shake determinant < 0.0} :dt
The determinant of the quadratic equation being solved for a single
cluster specified by the fix shake command is numerically suspect. LAMMPS
will set it to 0.0 and continue. :dd
{Shell command '%s' failed with error '%s'} :dt
Self-explanatory. :dd
{Shell command returned with non-zero status} :dt
This may indicate the shell command did not operate as expected. :dd
{Should not allow rigid bodies to bounce off relecting walls} :dt
LAMMPS allows this, but their dynamics are not computed correctly. :dd
{Should not use fix nve/limit with fix shake or fix rattle} :dt
This will lead to invalid constraint forces in the SHAKE/RATTLE
computation. :dd
{Simulations might be very slow because of large number of structure factors} :dt
Self-explanatory. :dd
{Slab correction not needed for MSM} :dt
Slab correction is intended to be used with Ewald or PPPM and is not needed by MSM. :dd
{System is not charge neutral, net charge = %g} :dt
The total charge on all atoms on the system is not 0.0.
For some KSpace solvers this is only a warning. :dd
{Table inner cutoff >= outer cutoff} :dt
You specified an inner cutoff for a Coulombic table that is longer
than the global cutoff. Probably not what you wanted. :dd
{Temperature for MSST is not for group all} :dt
User-assigned temperature to MSST fix does not compute temperature for
all atoms. Since MSST computes a global pressure, the kinetic energy
contribution from the temperature is assumed to also be for all atoms.
Thus the pressure used by MSST could be inaccurate. :dd
{Temperature for NPT is not for group all} :dt
User-assigned temperature to NPT fix does not compute temperature for
all atoms. Since NPT computes a global pressure, the kinetic energy
contribution from the temperature is assumed to also be for all atoms.
Thus the pressure used by NPT could be inaccurate. :dd
{Temperature for fix modify is not for group all} :dt
The temperature compute is being used with a pressure calculation
which does operate on group all, so this may be inconsistent. :dd
{Temperature for thermo pressure is not for group all} :dt
User-assigned temperature to thermo via the thermo_modify command does
not compute temperature for all atoms. Since thermo computes a global
pressure, the kinetic energy contribution from the temperature is
assumed to also be for all atoms. Thus the pressure printed by thermo
could be inaccurate. :dd
{The fix ave/spatial command has been replaced by the more flexible fix ave/chunk and compute chunk/atom commands -- fix ave/spatial will be removed in the summer of 2015} :dt
Self-explanatory. :dd
{The minimizer does not re-orient dipoles when using fix efield} :dt
This means that only the atom coordinates will be minimized,
not the orientation of the dipoles. :dd
{Too many common neighbors in CNA %d times} :dt
More than the maximum # of neighbors was found multiple times. This
was unexpected. :dd
{Too many inner timesteps in fix ttm} :dt
Self-explanatory. :dd
{Too many neighbors in CNA for %d atoms} :dt
More than the maximum # of neighbors was found multiple times. This
was unexpected. :dd
{Triclinic box skew is large} :dt
The displacement in a skewed direction is normally required to be less
than half the box length in that dimension. E.g. the xy tilt must be
between -half and +half of the x box length. You have relaxed the
constraint using the box tilt command, but the warning means that a
LAMMPS simulation may be inefficient as a result. :dd
{Use special bonds = 0,1,1 with bond style fene} :dt
Most FENE models need this setting for the special_bonds command. :dd
{Use special bonds = 0,1,1 with bond style fene/expand} :dt
Most FENE models need this setting for the special_bonds command. :dd
{Using a manybody potential with bonds/angles/dihedrals and special_bond exclusions} :dt
This is likely not what you want to do. The exclusion settings will
eliminate neighbors in the neighbor list, which the manybody potential
needs to calculated its terms correctly. :dd
{Using compute temp/deform with inconsistent fix deform remap option} :dt
Fix nvt/sllod assumes deforming atoms have a velocity profile provided
by "remap v" or "remap none" as a fix deform option. :dd
{Using compute temp/deform with no fix deform defined} :dt
This is probably an error, since it makes little sense to use
compute temp/deform in this case. :dd
{Using fix srd with box deformation but no SRD thermostat} :dt
The deformation will heat the SRD particles so this can
be dangerous. :dd
{Using kspace solver on system with no charge} :dt
Self-explanatory. :dd
{Using largest cut-off for lj/long/dipole/long long long} :dt
Self-explanatory. :dd
{Using largest cutoff for buck/long/coul/long} :dt
Self-explanatory. :dd
{Using largest cutoff for lj/long/coul/long} :dt
Self-explanatory. :dd
{Using largest cutoff for pair_style lj/long/tip4p/long} :dt
Self-explanatory. :dd
{Using package gpu without any pair style defined} :dt
Self-explanatory. :dd
{Using pair potential shift with pair_modify compute no} :dt
The shift effects will thus not be computed. :dd
{Using pair tail corrections with nonperiodic system} :dt
This is probably a bogus thing to do, since tail corrections are
computed by integrating the density of a periodic system out to
infinity. :dd
{Using pair tail corrections with pair_modify compute no} :dt
The tail corrections will thus not be computed. :dd
{pair style reax is now deprecated and will soon be retired. Users should switch to pair_style reax/c} :dt
Self-explanatory. :dd
:dle

14
doc/src/Section_example.txt → doc/src/Examples.txt
View File

@ -1,12 +1,14 @@
"Previous Section"_Section_howto.html - "LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc - "Next Section"_Section_perf.html :c
"Previous Section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc - "Next
Section"_Tools.html :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Section_commands.html#comm)
:link(lc,Commands_all.html)
:line
7. Example problems :h2
Example scripts :h3
The LAMMPS distribution includes an examples sub-directory with many
sample problems. Many are 2d models that run quickly are are
@ -46,7 +48,7 @@ Lists of both kinds of directories are given below.
:line
Lowercase directories :h3
Lowercase directories :h4
accelerate: run with various acceleration options (OpenMP, GPU, Phi)
airebo: polyethylene with AIREBO potential
@ -122,7 +124,7 @@ browser.
:line
Uppercase directories :h3
Uppercase directories :h4
ASPHERE: various aspherical particle models, using ellipsoids, rigid bodies, line/triangle particles, etc
COUPLE: examples of how to use LAMMPS as a library
@ -141,5 +143,5 @@ The USER directory has a large number of sub-directories which
correspond by name to a USER package. They contain scripts that
illustrate how to use the command(s) provided in that package. Many
of the sub-directories have their own README files which give further
instructions. See the "Section 4"_Section_packages.html doc
instructions. See the "Packages_details"_Packages_details.html doc
page for more info on specific USER packages.

128
doc/src/Howto.txt Normal file
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@ -0,0 +1,128 @@
"Previous Section"_Performance.html - "LAMMPS WWW Site"_lws -
"LAMMPS Documentation"_ld - "LAMMPS Commands"_lc - "Next
Section"_Examples.html :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands.html#comm)
:line
How to discussions :h2
These doc pages describe how to perform various tasks with LAMMPS,
both for users and developers. The
"glossary"_http://lammps.sandia.gov website page also lists MD
terminology with links to corresponding LAMMPS manual pages.
The example input scripts included in the examples dir of the LAMMPS
distribution and highlighted on the "Examples"_Examples.html doc page
also show how to setup and run various kinds of simulations.
<!-- RST
.. toctree::
Howto_github
Howto_pylammps
Howto_bash
.. toctree::
Howto_restart
Howto_viz
Howto_multiple
Howto_replica
Howto_library
Howto_couple
.. toctree::
Howto_output
Howto_chunk
.. toctree::
Howto_2d
Howto_triclinic
Howto_walls
Howto_nemd
Howto_granular
Howto_spherical
Howto_dispersion
.. toctree::
Howto_temperature
Howto_thermostat
Howto_barostat
Howto_elastic
Howto_kappa
Howto_viscosity
Howto_diffusion
.. toctree::
Howto_bioFF
Howto_tip3p
Howto_tip4p
Howto_spc
.. toctree::
Howto_body
Howto_polarizable
Howto_coreshell
Howto_drude
Howto_drude2
Howto_manifold
Howto_spins
END_RST -->
<!-- HTML_ONLY -->
"Using GitHub with LAMMPS"_Howto_github.html
"PyLAMMPS interface to LAMMPS"_Howto_pylammps.html
"Using LAMMPS with bash on Windows"_Howto_bash.html
"Restart a simulation"_Howto_restart.html
"Visualize LAMMPS snapshots"_Howto_viz.html
"Run multiple simulations from one input script"_Howto_multiple.html
"Multi-replica simulations"_Howto_replica.html
"Library interface to LAMMPS"_Howto_library.html
"Couple LAMMPS to other codes"_Howto_couple.html :all(b)
"Output from LAMMPS (thermo, dumps, computes, fixes, variables)"_Howto_output.html
"Use chunks to calculate system properties"_Howto_chunk.html :all(b)
"2d simulations"_Howto_2d.html
"Triclinic (non-orthogonal) simulation boxes"_Howto_triclinic.html
"Walls"_Howto_walls.html
"NEMD simulations"_Howto_nemd.html
"Granular models"_Howto_granular.html
"Finite-size spherical and aspherical particles"_Howto_spherical.html
"Long-range dispersion settings"_Howto_dispersion.html :all(b)
"Calculate temperature"_Howto_temperature.html
"Thermostats"_Howto_thermostat.html
"Barostats"_Howto_barostat.html
"Calculate elastic constants"_Howto_elastic.html
"Calculate thermal conductivity"_Howto_kappa.html
"Calculate viscosity"_Howto_viscosity.html
"Calculate a diffusion coefficient"_Howto_diffusion.html :all(b)
"CHARMM, AMBER, and DREIDING force fields"_Howto_bioFF.html
"TIP3P water model"_Howto_tip3p.html
"TIP4P water model"_Howto_tip4p.html
"SPC water model"_Howto_spc.html :all(b)
"Body style particles"_Howto_body.html
"Polarizable models"_Howto_polarizable.html
"Adiabatic core/shell model"_Howto_coreshell.html
"Drude induced dipoles"_Howto_drude.html
"Drude induced dipoles (extended)"_Howto_drude2.html :all(b)
"Manifolds (surfaces)"_Howto_manifold.html
"Magnetic spins"_Howto_spins.html
<!-- END_HTML_ONLY -->

48
doc/src/Howto_2d.txt Normal file
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@ -0,0 +1,48 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
2d simulations :h3
Use the "dimension"_dimension.html command to specify a 2d simulation.
Make the simulation box periodic in z via the "boundary"_boundary.html
command. This is the default.
If using the "create box"_create_box.html command to define a
simulation box, set the z dimensions narrow, but finite, so that the
create_atoms command will tile the 3d simulation box with a single z
plane of atoms - e.g.
"create box"_create_box.html 1 -10 10 -10 10 -0.25 0.25 :pre
If using the "read data"_read_data.html command to read in a file of
atom coordinates, set the "zlo zhi" values to be finite but narrow,
similar to the create_box command settings just described. For each
atom in the file, assign a z coordinate so it falls inside the
z-boundaries of the box - e.g. 0.0.
Use the "fix enforce2d"_fix_enforce2d.html command as the last
defined fix to insure that the z-components of velocities and forces
are zeroed out every timestep. The reason to make it the last fix is
so that any forces induced by other fixes will be zeroed out.
Many of the example input scripts included in the LAMMPS distribution
are for 2d models.
NOTE: Some models in LAMMPS treat particles as finite-size spheres, as
opposed to point particles. See the "atom_style
sphere"_atom_style.html and "fix nve/sphere"_fix_nve_sphere.html
commands for details. By default, for 2d simulations, such particles
will still be modeled as 3d spheres, not 2d discs (circles), meaning
their moment of inertia will be that of a sphere. If you wish to
model them as 2d discs, see the "set density/disc"_set.html command
and the {disc} option for the "fix nve/sphere"_fix_nve_sphere.html,
"fix nvt/sphere"_fix_nvt_sphere.html, "fix
nph/sphere"_fix_nph_sphere.html, "fix npt/sphere"_fix_npt_sphere.html
commands.

75
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@ -0,0 +1,75 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Barostats :h3
Barostatting means controlling the pressure in an MD simulation.
"Thermostatting"_Howto_thermostat.html means controlling the
temperature of the particles. Since the pressure includes a kinetic
component due to particle velocities, both these operations require
calculation of the temperature. Typically a target temperature (T)
and/or pressure (P) is specified by the user, and the thermostat or
barostat attempts to equilibrate the system to the requested T and/or
P.
Barostatting in LAMMPS is performed by "fixes"_fix.html. Two
barosttating methods are currently available: Nose-Hoover (npt and
nph) and Berendsen:
"fix npt"_fix_nh.html
"fix npt/sphere"_fix_npt_sphere.html
"fix npt/asphere"_fix_npt_asphere.html
"fix nph"_fix_nh.html
"fix press/berendsen"_fix_press_berendsen.html :ul
The "fix npt"_fix_nh.html commands include a Nose-Hoover thermostat
and barostat. "Fix nph"_fix_nh.html is just a Nose/Hoover barostat;
it does no thermostatting. Both "fix nph"_fix_nh.html and "fix
press/berendsen"_fix_press_berendsen.html can be used in conjunction
with any of the thermostatting fixes.
As with the "thermostats"_Howto_thermostat.html, "fix npt"_fix_nh.html
and "fix nph"_fix_nh.html only use translational motion of the
particles in computing T and P and performing thermo/barostatting.
"Fix npt/sphere"_fix_npt_sphere.html and "fix
npt/asphere"_fix_npt_asphere.html thermo/barostat using not only
translation velocities but also rotational velocities for spherical
and aspherical particles.
All of the barostatting fixes use the "compute
pressure"_compute_pressure.html compute to calculate a current
pressure. By default, this compute is created with a simple "compute
temp"_compute_temp.html (see the last argument of the "compute
pressure"_compute_pressure.html command), which is used to calculated
the kinetic component of the pressure. The barostatting fixes can
also use temperature computes that remove bias for the purpose of
computing the kinetic component which contributes to the current
pressure. See the doc pages for the individual fixes and for the
"fix_modify"_fix_modify.html command for instructions on how to assign
a temperature or pressure compute to a barostatting fix.
NOTE: As with the thermostats, the Nose/Hoover methods ("fix
npt"_fix_nh.html and "fix nph"_fix_nh.html) perform time integration.
"Fix press/berendsen"_fix_press_berendsen.html does NOT, so it should
be used with one of the constant NVE fixes or with one of the NVT
fixes.
Thermodynamic output, which can be setup via the
"thermo_style"_thermo_style.html command, often includes pressure
values. As explained on the doc page for the
"thermo_style"_thermo_style.html command, the default pressure is
setup by the thermo command itself. It is NOT the presure associated
with any barostatting fix you have defined or with any compute you
have defined that calculates a presure. The doc pages for the
barostatting fixes explain the ID of the pressure compute they create.
Thus if you want to view these pressurse, you need to specify them
explicitly via the "thermo_style custom"_thermo_style.html command.
Or you can use the "thermo_modify"_thermo_modify.html command to
re-define what pressure compute is used for default thermodynamic
output.

3
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@ -2,7 +2,7 @@
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Section_commands.html#comm)
:link(lc,Commands_all.html)
:line
@ -10,6 +10,7 @@ Using LAMMPS with Bash on Windows :h3
[written by Richard Berger]
:line
Starting with Windows 10 you can install Linux tools directly in Windows. This
allows you to compile LAMMPS following the same procedure as on a real Ubuntu
Linux installation. Software can be easily installed using the package manager

101
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@ -0,0 +1,101 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
CHARMM, AMBER, and DREIDING force fields :h3
A force field has 2 parts: the formulas that define it and the
coefficients used for a particular system. Here we only discuss
formulas implemented in LAMMPS that correspond to formulas commonly
used in the CHARMM, AMBER, and DREIDING force fields. Setting
coefficients is done in the input data file via the
"read_data"_read_data.html command or in the input script with
commands like "pair_coeff"_pair_coeff.html or
"bond_coeff"_bond_coeff.html. See the "Tools"_Tools.html doc page for
additional tools that can use CHARMM or AMBER to assign force field
coefficients and convert their output into LAMMPS input.
See "(MacKerell)"_#howto-MacKerell for a description of the CHARMM force
field. See "(Cornell)"_#howto-Cornell for a description of the AMBER force
field.
:link(charmm,http://www.scripps.edu/brooks)
:link(amber,http://amber.scripps.edu)
These style choices compute force field formulas that are consistent
with common options in CHARMM or AMBER. See each command's
documentation for the formula it computes.
"bond_style"_bond_harmonic.html harmonic
"angle_style"_angle_charmm.html charmm
"dihedral_style"_dihedral_charmm.html charmmfsh
"dihedral_style"_dihedral_charmm.html charmm
"pair_style"_pair_charmm.html lj/charmmfsw/coul/charmmfsh
"pair_style"_pair_charmm.html lj/charmmfsw/coul/long
"pair_style"_pair_charmm.html lj/charmm/coul/charmm
"pair_style"_pair_charmm.html lj/charmm/coul/charmm/implicit
"pair_style"_pair_charmm.html lj/charmm/coul/long :ul
"special_bonds"_special_bonds.html charmm
"special_bonds"_special_bonds.html amber :ul
NOTE: For CHARMM, newer {charmmfsw} or {charmmfsh} styles were
released in March 2017. We recommend they be used instead of the
older {charmm} styles. See discussion of the differences on the "pair
charmm"_pair_charmm.html and "dihedral charmm"_dihedral_charmm.html
doc pages.
DREIDING is a generic force field developed by the "Goddard
group"_http://www.wag.caltech.edu at Caltech and is useful for
predicting structures and dynamics of organic, biological and
main-group inorganic molecules. The philosophy in DREIDING is to use
general force constants and geometry parameters based on simple
hybridization considerations, rather than individual force constants
and geometric parameters that depend on the particular combinations of
atoms involved in the bond, angle, or torsion terms. DREIDING has an
"explicit hydrogen bond term"_pair_hbond_dreiding.html to describe
interactions involving a hydrogen atom on very electronegative atoms
(N, O, F).
See "(Mayo)"_#howto-Mayo for a description of the DREIDING force field
These style choices compute force field formulas that are consistent
with the DREIDING force field. See each command's
documentation for the formula it computes.
"bond_style"_bond_harmonic.html harmonic
"bond_style"_bond_morse.html morse :ul
"angle_style"_angle_harmonic.html harmonic
"angle_style"_angle_cosine.html cosine
"angle_style"_angle_cosine_periodic.html cosine/periodic :ul
"dihedral_style"_dihedral_charmm.html charmm
"improper_style"_improper_umbrella.html umbrella :ul
"pair_style"_pair_buck.html buck
"pair_style"_pair_buck.html buck/coul/cut
"pair_style"_pair_buck.html buck/coul/long
"pair_style"_pair_lj.html lj/cut
"pair_style"_pair_lj.html lj/cut/coul/cut
"pair_style"_pair_lj.html lj/cut/coul/long :ul
"pair_style"_pair_hbond_dreiding.html hbond/dreiding/lj
"pair_style"_pair_hbond_dreiding.html hbond/dreiding/morse :ul
"special_bonds"_special_bonds.html dreiding :ul
:line
:link(howto-MacKerell)
[(MacKerell)] MacKerell, Bashford, Bellott, Dunbrack, Evanseck, Field,
Fischer, Gao, Guo, Ha, et al, J Phys Chem, 102, 3586 (1998).
:link(howto-Mayo)
[(Mayo)] Mayo, Olfason, Goddard III, J Phys Chem, 94, 8897-8909
(1990).

280
doc/src/body.txt → doc/src/Howto_body.txt
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@ -1,24 +1,24 @@
"LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc :c
"Higher level section"_Howto.html - "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)
:link(lc,Commands_all.html)
:line
Body particles :h2
Body particles :h3
[Overview:]
This doc page is not about a LAMMPS input script command, but about
body particles, which are generalized finite-size particles.
In LAMMPS, body particles are generalized finite-size particles.
Individual body particles can represent complex entities, such as
surface meshes of discrete points, collections of sub-particles,
deformable objects, etc. Note that other kinds of finite-size
spherical and aspherical particles are also supported by LAMMPS, such
as spheres, ellipsoids, line segments, and triangles, but they are
simpler entities that body particles. See "Section
6.14"_Section_howto.html#howto_14 for a general overview of all
simpler entities that body particles. See the "Howto
spherical"_Howto_spherical.html doc page for a general overview of all
these particle types.
Body particles are used via the "atom_style body"_atom_style.html
@ -27,19 +27,17 @@ styles supported by LAMMPS are as follows. The name in the first
column is used as the {bstyle} argument for the "atom_style
body"_atom_style.html command.
{nparticle} | rigid body with N sub-particles |
{rounded/polygon} | 2d convex polygon with N vertices :tb(c=2,s=|)
{nparticle} : rigid body with N sub-particles
{rounded/polygon} : 2d polygons with N vertices
{rounded/polyhedron} : 3d polyhedra with N vertices, E edges and F faces :tb(s=:)
The body style determines what attributes are stored for each body and
thus how they can be used to compute pairwise body/body or
bond/non-body (point particle) interactions. More details of each
style are described below.
NOTE: The rounded/polygon style listed in the table above and
described below has not yet been relesed in LAMMPS. It will be soon.
We hope to add more styles in the future. See "Section
10.12"_Section_modify.html#mod_12 for details on how to add a new body
More styles may be added in the future. See the "Modify
body"_Modify_body.html doc page for details on how to add a new body
style to the code.
:line
@ -61,7 +59,7 @@ the simple particles.
By contrast, when body particles are used, LAMMPS treats an entire
body as a single particle for purposes of computing pairwise
interactions, building neighbor lists, migrating particles between
processors, outputting particles to a dump file, etc. This means that
processors, output of particles to a dump file, etc. This means that
interactions between pairs of bodies or between a body and non-body
(point) particle need to be encoded in an appropriate pair style. If
such a pair style were to mimic the "fix rigid"_fix_rigid.html model,
@ -72,17 +70,20 @@ single body/body interaction was computed.
Thus it only makes sense to use body particles and develop such a pair
style, when particle/particle interactions are more complex than what
the "fix rigid"_fix_rigid.html command can already calculate. For
example, if particles have one or more of the following attributes:
example, consider particles with one or more of the following
attributes:
represented by a surface mesh
represented by a collection of geometric entities (e.g. planes + spheres)
deformable
internal stress that induces fragmentation :ul
then the interaction between pairs of particles is likely to be more
complex than the summation of simple sub-particle interactions. An
example is contact or frictional forces between particles with planar
surfaces that inter-penetrate.
For these models, the interaction between pairs of particles is likely
to be more complex than the summation of simple pairwise interactions.
An example is contact or frictional forces between particles with
planar surfaces that inter-penetrate. Likewise, the body particle may
store internal state, such as a stress tensor used to compute a
fracture criterion.
These are additional LAMMPS commands that can be used with body
particles of different styles
@ -130,7 +131,9 @@ x1 y1 z1
...
xN yN zN :pre
N is the number of sub-particles in the body particle. M = 6 + 3*N.
where M = 6 + 3*N, and N is the number of sub-particles in the body
particle.
The integer line has a single value N. The floating point line(s)
list 6 moments of inertia followed by the coordinates of the N
sub-particles (x1 to zN) as 3N values. These values can be listed on
@ -148,8 +151,8 @@ center-of-mass position of the particle is specified by the x,y,z
values in the {Atoms} section of the data file, as is the total mass
of the body particle.
The "pair_style body"_pair_body.html command can be used with this
body style to compute body/body and body/non-body interactions.
The "pair_style body/nparticle"_pair_body_nparticle.html command can be used
with this body style to compute body/body and body/non-body interactions.
For output purposes via the "compute
body/local"_compute_body_local.html and "dump local"_dump.html
@ -175,15 +178,18 @@ The {bflag2} argument is ignored.
[Specifics of body style rounded/polygon:]
NOTE: Aug 2016 - This body style has not yet been added to LAMMPS.
The info below is a placeholder.
The {rounded/polygon} body style represents body particles as a 2d
polygon with a variable number of N vertices. This style can only be
used for 2d models; see the "boundary"_boundary.html command. See the
"pair_style body/rounded/polygon" doc page for a diagram of two
squares with rounded circles at the vertices. Special cases for N = 1
(circle) and N = 2 (rod with rounded ends) can also be specified.
The {rounded/polygon} body style represents body particles as a convex
polygon with a variable number N > 2 of vertices, which can only be
used for 2d models. One example use of this body style is for 2d
discrete element models, as described in "Fraige"_#Fraige. Similar to
body style {nparticle}, the atom_style body command for this body
style takes two additional arguments:
One use of this body style is for 2d discrete element models, as
described in "Fraige"_#body-Fraige.
Similar to body style {nparticle}, the atom_style body command for
this body style takes two additional arguments:
atom_style body rounded/polygon Nmin Nmax
Nmin = minimum # of vertices in any body in the system
@ -203,17 +209,20 @@ x1 y1 z1
...
xN yN zN
i j j k k ...
radius :pre
diameter :pre
N is the number of vertices in the body particle. M = 6 + 3*N + 2*N +
1. The integer line has a single value N. The floating point line(s)
where M = 6 + 3*N + 2*N + 1, and N is the number of vertices in the
body particle.
The integer line has a single value N. The floating point line(s)
list 6 moments of inertia followed by the coordinates of the N
vertices (x1 to zN) as 3N values, followed by 2N vertex indices
corresponding to the end points of the N edges, followed by a single
radius value = the smallest circle encompassing the polygon. That
last value is used to facilitate the body/body contact detection.
These floating-point values can be listed on as many lines as you
wish; see the "read_data"_read_data.html command for more details.
vertices (x1 to zN) as 3N values (with z = 0.0 for each), followed by
2N vertex indices corresponding to the end points of the N edges,
followed by a single diameter value = the rounded diameter of the
circle that surrounds each vertex. The diameter value can be different
for each body particle. These floating-point values can be listed on
as many lines as you wish; see the "read_data"_read_data.html command
for more details.
The 6 moments of inertia (ixx,iyy,izz,ixy,ixz,iyz) should be the
values consistent with the current orientation of the rigid body
@ -225,8 +234,11 @@ from the center-of-mass of the body particle. The center-of-mass
position of the particle is specified by the x,y,z values in the
{Atoms} section of the data file.
For example, the following information would specify a square
particles whose edge length is sqrt(2):
For example, the following information would specify a square particle
whose edge length is sqrt(2) and rounded diameter is 1.0. The
orientation of the square is aligned with the xy coordinate axes which
is consistent with the 6 moments of inertia: ixx iyy izz ixy ixz iyz =
1 1 4 0 0 0. Note that only Izz matters in 2D simulations.
3 1 27
4
@ -235,12 +247,178 @@ particles whose edge length is sqrt(2):
-0.7071 0.7071 0
0.7071 0.7071 0
0.7071 -0.7071 0
0 1 1 2 2 3 3 0
0 1
1 2
2 3
3 0
1.0 :pre
A rod in 2D, whose length is 4.0, mass 1.0, rounded at two ends
by circles of diameter 0.5, is specified as follows:
1 1 13
2
1 1 1.33333 0 0 0
-2 0 0
2 0 0
0.5 :pre
A disk, whose diameter is 3.0, mass 1.0, is specified as follows:
1 1 10
1
1 1 4.5 0 0 0
0 0 0
3.0 :pre
The "pair_style body/rounded/polygon"_pair_body_rounded_polygon.html
command can be used with this body style to compute body/body
interactions.
interactions. The "fix wall/body/polygon"_fix_wall_body_polygon.html
command can be used with this body style to compute the interaction of
body particles with a wall.
:line
[Specifics of body style rounded/polyhedron:]
The {rounded/polyhedron} body style represents body particles as a 3d
polyhedron with a variable number of N vertices, E edges and F faces.
This style can only be used for 3d models; see the
"boundary"_boundary.html command. See the "pair_style
body/rounded/polygon" doc page for a diagram of a two 2d squares with
rounded circles at the vertices. A 3d cube with rounded spheres at
the 8 vertices and 12 rounded edges would be similar. Special cases
for N = 1 (sphere) and N = 2 (rod with rounded ends) can also be
specified.
This body style is for 3d discrete element models, as described in
"Wang"_#body-Wang.
Similar to body style {rounded/polygon}, the atom_style body command
for this body style takes two additional arguments:
atom_style body rounded/polyhedron Nmin Nmax
Nmin = minimum # of vertices in any body in the system
Nmax = maximum # of vertices in any body in the system :pre
The Nmin and Nmax arguments are used to bound the size of data
structures used internally by each particle.
When the "read_data"_read_data.html command reads a data file for this
body style, the following information must be provided for each entry
in the {Bodies} section of the data file:
atom-ID 3 M
N E F
ixx iyy izz ixy ixz iyz
x1 y1 z1
...
xN yN zN
0 1
1 2
2 3
...
0 1 2 -1
0 2 3 -1
...
1 2 3 4
diameter :pre
where M = 6 + 3*N + 2*E + 4*F + 1, and N is the number of vertices in
the body particle, E = number of edges, F = number of faces.
The integer line has three values: number of vertices (N), number of
edges (E) and number of faces (F). The floating point line(s) list 6
moments of inertia followed by the coordinates of the N vertices (x1
to zN) as 3N values, followed by 2N vertex indices corresponding to
the end points of the E edges, then 4*F vertex indices defining F
faces. The last value is the diameter value = the rounded diameter of
the sphere that surrounds each vertex. The diameter value can be
different for each body particle. These floating-point values can be
listed on as many lines as you wish; see the
"read_data"_read_data.html command for more details. Because the
maxmimum vertices per face is hard-coded to be 4
(i.e. quadrilaterals), faces with more than 4 vertices need to be
split into triangles or quadrilaterals. For triangular faces, the
last vertex index should be set to -1.
The ordering of the 4 vertices within a face should follow
the right-hand rule so that the normal vector of the face points
outwards from the center of mass.
The 6 moments of inertia (ixx,iyy,izz,ixy,ixz,iyz) should be the
values consistent with the current orientation of the rigid body
around its center of mass. The values are with respect to the
simulation box XYZ axes, not with respect to the principal axes of the
rigid body itself. LAMMPS performs the latter calculation internally.
The coordinates of each vertex are specified as its x,y,z displacement
from the center-of-mass of the body particle. The center-of-mass
position of the particle is specified by the x,y,z values in the
{Atoms} section of the data file.
For example, the following information would specify a cubic particle
whose edge length is 2.0 and rounded diameter is 0.5.
The orientation of the cube is aligned with the xyz coordinate axes
which is consistent with the 6 moments of inertia: ixx iyy izz ixy ixz
iyz = 0.667 0.667 0.667 0 0 0.
1 3 79
8 12 6
0.667 0.667 0.667 0 0 0
1 1 1
1 -1 1
-1 -1 1
-1 1 1
1 1 -1
1 -1 -1
-1 -1 -1
-1 1 -1
0 1
1 2
2 3
3 0
4 5
5 6
6 7
7 4
0 4
1 5
2 6
3 7
0 1 2 3
4 5 6 7
0 1 5 4
1 2 6 5
2 3 7 6
3 0 4 7
0.5 :pre
A rod in 3D, whose length is 4.0, mass 1.0 and rounded at two ends
by circles of diameter 0.5, is specified as follows:
1 1 13
2
0 1.33333 1.33333 0 0 0
-2 0 0
2 0 0
0.5 :pre
A sphere whose diameter is 3.0 and mass 1.0, is specified as follows:
1 1 10
1
0.9 0.9 0.9 0 0 0
0 0 0
3.0 :pre
The "pair_style
body/rounded/polhedron"_pair_body_rounded_polyhedron.html command can
be used with this body style to compute body/body interactions. The
"fix wall/body/polyhedron"_fix_wall_body_polygon.html command can be
used with this body style to compute the interaction of body particles
with a wall.
:line
For output purposes via the "compute
body/local"_compute_body_local.html and "dump local"_dump.html
@ -257,10 +435,10 @@ the body particle itself. These values are calculated using the
current COM and orientation of the body particle.
For images created by the "dump image"_dump_image.html command, if the
{body} keyword is set, then each body particle is drawn as a convex
polygon consisting of N line segments. Note that the line segments
are drawn between the N vertices, which does not correspond exactly to
the physical extent of the body (because the "pair_style
{body} keyword is set, then each body particle is drawn as a polygon
consisting of N line segments. Note that the line segments are drawn
between the N vertices, which does not correspond exactly to the
physical extent of the body (because the "pair_style
rounded/polygon"_pair_body_rounded_polygon.html defines finite-size
spheres at those point and the line segments between the spheres are
tangent to the spheres). The drawn diameter of each line segment is
@ -269,6 +447,10 @@ determined by the {bflag1} parameter for the {body} keyword. The
:line
:link(Fraige)
:link(body-Fraige)
[(Fraige)] F. Y. Fraige, P. A. Langston, A. J. Matchett, J. Dodds,
Particuology, 6, 455 (2008).
:link(body-Wang)
[(Wang)] J. Wang, H. S. Yu, P. A. Langston, F. Y. Fraige, Granular
Matter, 13, 1 (2011).

166
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@ -0,0 +1,166 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Use chunks to calculate system properties :h3
In LAMMS, "chunks" are collections of atoms, as defined by the
"compute chunk/atom"_compute_chunk_atom.html command, which assigns
each atom to a chunk ID (or to no chunk at all). The number of chunks
and the assignment of chunk IDs to atoms can be static or change over
time. Examples of "chunks" are molecules or spatial bins or atoms
with similar values (e.g. coordination number or potential energy).
The per-atom chunk IDs can be used as input to two other kinds of
commands, to calculate various properties of a system:
"fix ave/chunk"_fix_ave_chunk.html
any of the "compute */chunk"_compute.html commands :ul
Here, each of the 3 kinds of chunk-related commands is briefly
overviewed. Then some examples are given of how to compute different
properties with chunk commands.
Compute chunk/atom command: :h4
This compute can assign atoms to chunks of various styles. Only atoms
in the specified group and optional specified region are assigned to a
chunk. Here are some possible chunk definitions:
atoms in same molecule | chunk ID = molecule ID |
atoms of same atom type | chunk ID = atom type |
all atoms with same atom property (charge, radius, etc) | chunk ID = output of compute property/atom |
atoms in same cluster | chunk ID = output of "compute cluster/atom"_compute_cluster_atom.html command |
atoms in same spatial bin | chunk ID = bin ID |
atoms in same rigid body | chunk ID = molecule ID used to define rigid bodies |
atoms with similar potential energy | chunk ID = output of "compute pe/atom"_compute_pe_atom.html |
atoms with same local defect structure | chunk ID = output of "compute centro/atom"_compute_centro_atom.html or "compute coord/atom"_compute_coord_atom.html command :tb(s=|,c=2)
Note that chunk IDs are integer values, so for atom properties or
computes that produce a floating point value, they will be truncated
to an integer. You could also use the compute in a variable that
scales the floating point value to spread it across multiple integers.
Spatial bins can be of various kinds, e.g. 1d bins = slabs, 2d bins =
pencils, 3d bins = boxes, spherical bins, cylindrical bins.
This compute also calculates the number of chunks {Nchunk}, which is
used by other commands to tally per-chunk data. {Nchunk} can be a
static value or change over time (e.g. the number of clusters). The
chunk ID for an individual atom can also be static (e.g. a molecule
ID), or dynamic (e.g. what spatial bin an atom is in as it moves).
Note that this compute allows the per-atom output of other
"computes"_compute.html, "fixes"_fix.html, and
"variables"_variable.html to be used to define chunk IDs for each
atom. This means you can write your own compute or fix to output a
per-atom quantity to use as chunk ID. See the "Modify"_Modify.html
doc pages for info on how to do this. You can also define a "per-atom
variable"_variable.html in the input script that uses a formula to
generate a chunk ID for each atom.
Fix ave/chunk command: :h4
This fix takes the ID of a "compute
chunk/atom"_compute_chunk_atom.html command as input. For each chunk,
it then sums one or more specified per-atom values over the atoms in
each chunk. The per-atom values can be any atom property, such as
velocity, force, charge, potential energy, kinetic energy, stress,
etc. Additional keywords are defined for per-chunk properties like
density and temperature. More generally any per-atom value generated
by other "computes"_compute.html, "fixes"_fix.html, and "per-atom
variables"_variable.html, can be summed over atoms in each chunk.
Similar to other averaging fixes, this fix allows the summed per-chunk
values to be time-averaged in various ways, and output to a file. The
fix produces a global array as output with one row of values per
chunk.
Compute */chunk commands: :h4
Currently the following computes operate on chunks of atoms to produce
per-chunk values.
"compute com/chunk"_compute_com_chunk.html
"compute gyration/chunk"_compute_gyration_chunk.html
"compute inertia/chunk"_compute_inertia_chunk.html
"compute msd/chunk"_compute_msd_chunk.html
"compute property/chunk"_compute_property_chunk.html
"compute temp/chunk"_compute_temp_chunk.html
"compute torque/chunk"_compute_vcm_chunk.html
"compute vcm/chunk"_compute_vcm_chunk.html :ul
They each take the ID of a "compute
chunk/atom"_compute_chunk_atom.html command as input. As their names
indicate, they calculate the center-of-mass, radius of gyration,
moments of inertia, mean-squared displacement, temperature, torque,
and velocity of center-of-mass for each chunk of atoms. The "compute
property/chunk"_compute_property_chunk.html command can tally the
count of atoms in each chunk and extract other per-chunk properties.
The reason these various calculations are not part of the "fix
ave/chunk command"_fix_ave_chunk.html, is that each requires a more
complicated operation than simply summing and averaging over per-atom
values in each chunk. For example, many of them require calculation
of a center of mass, which requires summing mass*position over the
atoms and then dividing by summed mass.
All of these computes produce a global vector or global array as
output, wih one or more values per chunk. They can be used
in various ways:
As input to the "fix ave/time"_fix_ave_time.html command, which can
write the values to a file and optionally time average them. :ulb,l
As input to the "fix ave/histo"_fix_ave_histo.html command to
histogram values across chunks. E.g. a histogram of cluster sizes or
molecule diffusion rates. :l
As input to special functions of "equal-style
variables"_variable.html, like sum() and max(). E.g. to find the
largest cluster or fastest diffusing molecule. :l
:ule
Example calculations with chunks :h4
Here are examples using chunk commands to calculate various
properties:
(1) Average velocity in each of 1000 2d spatial bins:
compute cc1 all chunk/atom bin/2d x 0.0 0.1 y lower 0.01 units reduced
fix 1 all ave/chunk 100 10 1000 cc1 vx vy file tmp.out :pre
(2) Temperature in each spatial bin, after subtracting a flow
velocity:
compute cc1 all chunk/atom bin/2d x 0.0 0.1 y lower 0.1 units reduced
compute vbias all temp/profile 1 0 0 y 10
fix 1 all ave/chunk 100 10 1000 cc1 temp bias vbias file tmp.out :pre
(3) Center of mass of each molecule:
compute cc1 all chunk/atom molecule
compute myChunk all com/chunk cc1
fix 1 all ave/time 100 1 100 c_myChunk\[*\] file tmp.out mode vector :pre
(4) Total force on each molecule and ave/max across all molecules:
compute cc1 all chunk/atom molecule
fix 1 all ave/chunk 1000 1 1000 cc1 fx fy fz file tmp.out
variable xave equal ave(f_1\[2\])
variable xmax equal max(f_1\[2\])
thermo 1000
thermo_style custom step temp v_xave v_xmax :pre
(5) Histogram of cluster sizes:
compute cluster all cluster/atom 1.0
compute cc1 all chunk/atom c_cluster compress yes
compute size all property/chunk cc1 count
fix 1 all ave/histo 100 1 100 0 20 20 c_size mode vector ave running beyond ignore file tmp.histo :pre

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Adiabatic core/shell model :h3
The adiabatic core-shell model by "Mitchell and
Fincham"_#MitchellFincham is a simple method for adding polarizability
to a system. In order to mimic the electron shell of an ion, a
satellite particle is attached to it. This way the ions are split into
a core and a shell where the latter is meant to react to the
electrostatic environment inducing polarizability. See the "Howto
polarizable"_Howto_polarizable.html doc page for a discussion of all
the polarizable models available in LAMMPS.
Technically, shells are attached to the cores by a spring force f =
k*r where k is a parametrized spring constant and r is the distance
between the core and the shell. The charges of the core and the shell
add up to the ion charge, thus q(ion) = q(core) + q(shell). This
setup introduces the ion polarizability (alpha) given by
alpha = q(shell)^2 / k. In a
similar fashion the mass of the ion is distributed on the core and the
shell with the core having the larger mass.
To run this model in LAMMPS, "atom_style"_atom_style.html {full} can
be used since atom charge and bonds are needed. Each kind of
core/shell pair requires two atom types and a bond type. The core and
shell of a core/shell pair should be bonded to each other with a
harmonic bond that provides the spring force. For example, a data file
for NaCl, as found in examples/coreshell, has this format:
432 atoms # core and shell atoms
216 bonds # number of core/shell springs :pre
4 atom types # 2 cores and 2 shells for Na and Cl
2 bond types :pre
0.0 24.09597 xlo xhi
0.0 24.09597 ylo yhi
0.0 24.09597 zlo zhi :pre
Masses # core/shell mass ratio = 0.1 :pre
1 20.690784 # Na core
2 31.90500 # Cl core
3 2.298976 # Na shell
4 3.54500 # Cl shell :pre
Atoms :pre
1 1 2 1.5005 0.00000000 0.00000000 0.00000000 # core of core/shell pair 1
2 1 4 -2.5005 0.00000000 0.00000000 0.00000000 # shell of core/shell pair 1
3 2 1 1.5056 4.01599500 4.01599500 4.01599500 # core of core/shell pair 2
4 2 3 -0.5056 4.01599500 4.01599500 4.01599500 # shell of core/shell pair 2
(...) :pre
Bonds # Bond topology for spring forces :pre
1 2 1 2 # spring for core/shell pair 1
2 2 3 4 # spring for core/shell pair 2
(...) :pre
Non-Coulombic (e.g. Lennard-Jones) pairwise interactions are only
defined between the shells. Coulombic interactions are defined
between all cores and shells. If desired, additional bonds can be
specified between cores.
The "special_bonds"_special_bonds.html command should be used to
turn-off the Coulombic interaction within core/shell pairs, since that
interaction is set by the bond spring. This is done using the
"special_bonds"_special_bonds.html command with a 1-2 weight = 0.0,
which is the default value. It needs to be considered whether one has
to adjust the "special_bonds"_special_bonds.html weighting according
to the molecular topology since the interactions of the shells are
bypassed over an extra bond.
Note that this core/shell implementation does not require all ions to
be polarized. One can mix core/shell pairs and ions without a
satellite particle if desired.
Since the core/shell model permits distances of r = 0.0 between the
core and shell, a pair style with a "cs" suffix needs to be used to
implement a valid long-range Coulombic correction. Several such pair
styles are provided in the CORESHELL package. See "this doc
page"_pair_cs.html for details. All of the core/shell enabled pair
styles require the use of a long-range Coulombic solver, as specified
by the "kspace_style"_kspace_style.html command. Either the PPPM or
Ewald solvers can be used.
For the NaCL example problem, these pair style and bond style settings
are used:
pair_style born/coul/long/cs 20.0 20.0
pair_coeff * * 0.0 1.000 0.00 0.00 0.00
pair_coeff 3 3 487.0 0.23768 0.00 1.05 0.50 #Na-Na
pair_coeff 3 4 145134.0 0.23768 0.00 6.99 8.70 #Na-Cl
pair_coeff 4 4 405774.0 0.23768 0.00 72.40 145.40 #Cl-Cl :pre
bond_style harmonic
bond_coeff 1 63.014 0.0
bond_coeff 2 25.724 0.0 :pre
When running dynamics with the adiabatic core/shell model, the
following issues should be considered. The relative motion of
the core and shell particles corresponds to the polarization,
hereby an instantaneous relaxation of the shells is approximated
and a fast core/shell spring frequency ensures a nearly constant
internal kinetic energy during the simulation.
Thermostats can alter this polarization behaviour, by scaling the
internal kinetic energy, meaning the shell will not react freely to
its electrostatic environment.
Therefore it is typically desirable to decouple the relative motion of
the core/shell pair, which is an imaginary degree of freedom, from the
real physical system. To do that, the "compute
temp/cs"_compute_temp_cs.html command can be used, in conjunction with
any of the thermostat fixes, such as "fix nvt"_fix_nh.html or "fix
langevin"_fix_langevin. This compute uses the center-of-mass velocity
of the core/shell pairs to calculate a temperature, and insures that
velocity is what is rescaled for thermostatting purposes. This
compute also works for a system with both core/shell pairs and
non-polarized ions (ions without an attached satellite particle). The
"compute temp/cs"_compute_temp_cs.html command requires input of two
groups, one for the core atoms, another for the shell atoms.
Non-polarized ions which might also be included in the treated system
should not be included into either of these groups, they are taken
into account by the {group-ID} (2nd argument) of the compute. The
groups can be defined using the "group {type}"_group.html command.
Note that to perform thermostatting using this definition of
temperature, the "fix modify temp"_fix_modify.html command should be
used to assign the compute to the thermostat fix. Likewise the
"thermo_modify temp"_thermo_modify.html command can be used to make
this temperature be output for the overall system.
For the NaCl example, this can be done as follows:
group cores type 1 2
group shells type 3 4
compute CSequ all temp/cs cores shells
fix thermoberendsen all temp/berendsen 1427 1427 0.4 # thermostat for the true physical system
fix thermostatequ all nve # integrator as needed for the berendsen thermostat
fix_modify thermoberendsen temp CSequ
thermo_modify temp CSequ # output of center-of-mass derived temperature :pre
The pressure for the core/shell system is computed via the regular
LAMMPS convention by "treating the cores and shells as individual
particles"_#MitchellFincham2. For the thermo output of the pressure
as well as for the application of a barostat, it is necessary to
use an additional "pressure"_compute_pressure compute based on the
default "temperature"_compute_temp and specifying it as a second
argument in "fix modify"_fix_modify.html and
"thermo_modify"_thermo_modify.html resulting in:
(...)
compute CSequ all temp/cs cores shells
compute thermo_press_lmp all pressure thermo_temp # pressure for individual particles
thermo_modify temp CSequ press thermo_press_lmp # modify thermo to regular pressure
fix press_bar all npt temp 300 300 0.04 iso 0 0 0.4
fix_modify press_bar temp CSequ press thermo_press_lmp # pressure modification for correct kinetic scalar :pre
If "compute temp/cs"_compute_temp_cs.html is used, the decoupled
relative motion of the core and the shell should in theory be
stable. However numerical fluctuation can introduce a small
momentum to the system, which is noticable over long trajectories.
Therefore it is recommendable to use the "fix
momentum"_fix_momentum.html command in combination with "compute
temp/cs"_compute_temp_cs.html when equilibrating the system to
prevent any drift.
When initializing the velocities of a system with core/shell pairs, it
is also desirable to not introduce energy into the relative motion of
the core/shell particles, but only assign a center-of-mass velocity to
the pairs. This can be done by using the {bias} keyword of the
"velocity create"_velocity.html command and assigning the "compute
temp/cs"_compute_temp_cs.html command to the {temp} keyword of the
"velocity"_velocity.html command, e.g.
velocity all create 1427 134 bias yes temp CSequ
velocity all scale 1427 temp CSequ :pre
To maintain the correct polarizability of the core/shell pairs, the
kinetic energy of the internal motion shall remain nearly constant.
Therefore the choice of spring force and mass ratio need to ensure
much faster relative motion of the 2 atoms within the core/shell pair
than their center-of-mass velocity. This allows the shells to
effectively react instantaneously to the electrostatic environment and
limits energy transfer to or from the core/shell oscillators.
This fast movement also dictates the timestep that can be used.
The primary literature of the adiabatic core/shell model suggests that
the fast relative motion of the core/shell pairs only allows negligible
energy transfer to the environment.
The mentioned energy transfer will typically lead to a small drift
in total energy over time. This internal energy can be monitored
using the "compute chunk/atom"_compute_chunk_atom.html and "compute
temp/chunk"_compute_temp_chunk.html commands. The internal kinetic
energies of each core/shell pair can then be summed using the sum()
special function of the "variable"_variable.html command. Or they can
be time/averaged and output using the "fix ave/time"_fix_ave_time.html
command. To use these commands, each core/shell pair must be defined
as a "chunk". If each core/shell pair is defined as its own molecule,
the molecule ID can be used to define the chunks. If cores are bonded
to each other to form larger molecules, the chunks can be identified
by the "fix property/atom"_fix_property_atom.html via assigning a
core/shell ID to each atom using a special field in the data file read
by the "read_data"_read_data.html command. This field can then be
accessed by the "compute property/atom"_compute_property_atom.html
command, to use as input to the "compute
chunk/atom"_compute_chunk_atom.html command to define the core/shell
pairs as chunks.
For example if core/shell pairs are the only molecules:
read_data NaCl_CS_x0.1_prop.data
compute prop all property/atom molecule
compute cs_chunk all chunk/atom c_prop
compute cstherm all temp/chunk cs_chunk temp internal com yes cdof 3.0 # note the chosen degrees of freedom for the core/shell pairs
fix ave_chunk all ave/time 10 1 10 c_cstherm file chunk.dump mode vector :pre
For example if core/shell pairs and other molecules are present:
fix csinfo all property/atom i_CSID # property/atom command
read_data NaCl_CS_x0.1_prop.data fix csinfo NULL CS-Info # atom property added in the data-file
compute prop all property/atom i_CSID
(...) :pre
The additional section in the date file would be formatted like this:
CS-Info # header of additional section :pre
1 1 # column 1 = atom ID, column 2 = core/shell ID
2 1
3 2
4 2
5 3
6 3
7 4
8 4
(...) :pre
:line
:link(MitchellFincham)
[(Mitchell and Fincham)] Mitchell, Fincham, J Phys Condensed Matter,
5, 1031-1038 (1993).
:link(MitchellFincham2)
[(Fincham)] Fincham, Mackrodt and Mitchell, J Phys Condensed Matter,
6, 393-404 (1994).

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Coupling LAMMPS to other codes :h3
LAMMPS is designed to allow it to be coupled to other codes. For
example, a quantum mechanics code might compute forces on a subset of
atoms and pass those forces to LAMMPS. Or a continuum finite element
(FE) simulation might use atom positions as boundary conditions on FE
nodal points, compute a FE solution, and return interpolated forces on
MD atoms.
LAMMPS can be coupled to other codes in at least 3 ways. Each has
advantages and disadvantages, which you'll have to think about in the
context of your application.
(1) Define a new "fix"_fix.html command that calls the other code. In
this scenario, LAMMPS is the driver code. During its timestepping,
the fix is invoked, and can make library calls to the other code,
which has been linked to LAMMPS as a library. This is the way the
"POEMS"_poems package that performs constrained rigid-body motion on
groups of atoms is hooked to LAMMPS. See the "fix
poems"_fix_poems.html command for more details. See the
"Modify"_Modify.html doc pages for info on how to add a new fix to
LAMMPS.
:link(poems,http://www.rpi.edu/~anderk5/lab)
(2) Define a new LAMMPS command that calls the other code. This is
conceptually similar to method (1), but in this case LAMMPS and the
other code are on a more equal footing. Note that now the other code
is not called during the timestepping of a LAMMPS run, but between
runs. The LAMMPS input script can be used to alternate LAMMPS runs
with calls to the other code, invoked via the new command. The
"run"_run.html command facilitates this with its {every} option, which
makes it easy to run a few steps, invoke the command, run a few steps,
invoke the command, etc.
In this scenario, the other code can be called as a library, as in
(1), or it could be a stand-alone code, invoked by a system() call
made by the command (assuming your parallel machine allows one or more
processors to start up another program). In the latter case the
stand-alone code could communicate with LAMMPS thru files that the
command writes and reads.
See the "Modify command"_Modify_command.html doc page for info on how
to add a new command to LAMMPS.
(3) Use LAMMPS as a library called by another code. In this case the
other code is the driver and calls LAMMPS as needed. Or a wrapper
code could link and call both LAMMPS and another code as libraries.
Again, the "run"_run.html command has options that allow it to be
invoked with minimal overhead (no setup or clean-up) if you wish to do
multiple short runs, driven by another program.
Examples of driver codes that call LAMMPS as a library are included in
the examples/COUPLE directory of the LAMMPS distribution; see
examples/COUPLE/README for more details:
simple: simple driver programs in C++ and C which invoke LAMMPS as a
library :ulb,l
lammps_quest: coupling of LAMMPS and "Quest"_quest, to run classical
MD with quantum forces calculated by a density functional code :l
lammps_spparks: coupling of LAMMPS and "SPPARKS"_spparks, to couple
a kinetic Monte Carlo model for grain growth using MD to calculate
strain induced across grain boundaries :l
:ule
:link(quest,http://dft.sandia.gov/Quest)
:link(spparks,http://www.sandia.gov/~sjplimp/spparks.html)
"This section"_Section_start.html#start_5 of the documentation
describes how to build LAMMPS as a library. Once this is done, you
can interface with LAMMPS either via C++, C, Fortran, or Python (or
any other language that supports a vanilla C-like interface). For
example, from C++ you could create one (or more) "instances" of
LAMMPS, pass it an input script to process, or execute individual
commands, all by invoking the correct class methods in LAMMPS. From C
or Fortran you can make function calls to do the same things. See the
"Python"_Python.html doc pages for a description of the Python wrapper
provided with LAMMPS that operates through the LAMMPS library
interface.
The files src/library.cpp and library.h contain the C-style interface
to LAMMPS. See the "Howto library"_Howto_library.html doc page for a
description of the interface and how to extend it for your needs.
Note that the lammps_open() function that creates an instance of
LAMMPS takes an MPI communicator as an argument. This means that
instance of LAMMPS will run on the set of processors in the
communicator. Thus the calling code can run LAMMPS on all or a subset
of processors. For example, a wrapper script might decide to
alternate between LAMMPS and another code, allowing them both to run
on all the processors. Or it might allocate half the processors to
LAMMPS and half to the other code and run both codes simultaneously
before syncing them up periodically. Or it might instantiate multiple
instances of LAMMPS to perform different calculations.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Calculate a diffusion coefficient :h3
The diffusion coefficient D of a material can be measured in at least
2 ways using various options in LAMMPS. See the examples/DIFFUSE
directory for scripts that implement the 2 methods discussed here for
a simple Lennard-Jones fluid model.
The first method is to measure the mean-squared displacement (MSD) of
the system, via the "compute msd"_compute_msd.html command. The slope
of the MSD versus time is proportional to the diffusion coefficient.
The instantaneous MSD values can be accumulated in a vector via the
"fix vector"_fix_vector.html command, and a line fit to the vector to
compute its slope via the "variable slope"_variable.html function, and
thus extract D.
The second method is to measure the velocity auto-correlation function
(VACF) of the system, via the "compute vacf"_compute_vacf.html
command. The time-integral of the VACF is proportional to the
diffusion coefficient. The instantaneous VACF values can be
accumulated in a vector via the "fix vector"_fix_vector.html command,
and time integrated via the "variable trap"_variable.html function,
and thus extract D.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Long-raage dispersion settings :h3
The PPPM method computes interactions by splitting the pair potential
into two parts, one of which is computed in a normal pairwise fashion,
the so-called real-space part, and one of which is computed using the
Fourier transform, the so called reciprocal-space or kspace part. For
both parts, the potential is not computed exactly but is approximated.
Thus, there is an error in both parts of the computation, the
real-space and the kspace error. The just mentioned facts are true
both for the PPPM for Coulomb as well as dispersion interactions. The
deciding difference - and also the reason why the parameters for
pppm/disp have to be selected with more care - is the impact of the
errors on the results: The kspace error of the PPPM for Coulomb and
dispersion interaction and the real-space error of the PPPM for
Coulomb interaction have the character of noise. In contrast, the
real-space error of the PPPM for dispersion has a clear physical
interpretation: the underprediction of cohesion. As a consequence, the
real-space error has a much stronger effect than the kspace error on
simulation results for pppm/disp. Parameters must thus be chosen in a
way that this error is much smaller than the kspace error.
When using pppm/disp and not making any specifications on the PPPM
parameters via the kspace modify command, parameters will be tuned
such that the real-space error and the kspace error are equal. This
will result in simulations that are either inaccurate or slow, both of
which is not desirable. For selecting parameters for the pppm/disp
that provide fast and accurate simulations, there are two approaches,
which both have their up- and downsides.
The first approach is to set desired real-space an kspace accuracies
via the {kspace_modify force/disp/real} and {kspace_modify
force/disp/kspace} commands. Note that the accuracies have to be
specified in force units and are thus dependent on the chosen unit
settings. For real units, 0.0001 and 0.002 seem to provide reasonable
accurate and efficient computations for the real-space and kspace
accuracies. 0.002 and 0.05 work well for most systems using lj
units. PPPM parameters will be generated based on the desired
accuracies. The upside of this approach is that it usually provides a
good set of parameters and will work for both the {kspace_modify diff
ad} and {kspace_modify diff ik} options. The downside of the method
is that setting the PPPM parameters will take some time during the
initialization of the simulation.
The second approach is to set the parameters for the pppm/disp
explicitly using the {kspace_modify mesh/disp}, {kspace_modify
order/disp}, and {kspace_modify gewald/disp} commands. This approach
requires a more experienced user who understands well the impact of
the choice of parameters on the simulation accuracy and
performance. This approach provides a fast initialization of the
simulation. However, it is sensitive to errors: A combination of
parameters that will perform well for one system might result in
far-from-optimal conditions for other simulations. For example,
parameters that provide accurate and fast computations for
all-atomistic force fields can provide insufficient accuracy or
united-atomistic force fields (which is related to that the latter
typically have larger dispersion coefficients).
To avoid inaccurate or inefficient simulations, the pppm/disp stops
simulations with an error message if no action is taken to control the
PPPM parameters. If the automatic parameter generation is desired and
real-space and kspace accuracies are desired to be equal, this error
message can be suppressed using the {kspace_modify disp/auto yes}
command.
A reasonable approach that combines the upsides of both methods is to
make the first run using the {kspace_modify force/disp/real} and
{kspace_modify force/disp/kspace} commands, write down the PPPM
parameters from the outut, and specify these parameters using the
second approach in subsequent runs (which have the same composition,
force field, and approximately the same volume).
Concerning the performance of the pppm/disp there are two more things
to consider. The first is that when using the pppm/disp, the cutoff
parameter does no longer affect the accuracy of the simulation
(subject to that gewald/disp is adjusted when changing the cutoff).
The performance can thus be increased by examining different values
for the cutoff parameter. A lower bound for the cutoff is only set by
the truncation error of the repulsive term of pair potentials.
The second is that the mixing rule of the pair style has an impact on
the computation time when using the pppm/disp. Fastest computations
are achieved when using the geometric mixing rule. Using the
arithmetic mixing rule substantially increases the computational cost.
The computational overhead can be reduced using the {kspace_modify
mix/disp geom} and {kspace_modify splittol} commands. The first
command simply enforces geometric mixing of the dispersion
coefficients in kspace computations. This introduces some error in
the computations but will also significantly speed-up the
simulations. The second keyword sets the accuracy with which the
dispersion coefficients are approximated using a matrix factorization
approach. This may result in better accuracy then using the first
command, but will usually also not provide an equally good increase of
efficiency.
Finally, pppm/disp can also be used when no mixing rules apply.
This can be achieved using the {kspace_modify mix/disp none} command.
Note that the code does not check automatically whether any mixing
rule is fulfilled. If mixing rules do not apply, the user will have
to specify this command explicitly.

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@ -0,0 +1,77 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Drude induced dipoles :h3
The thermalized Drude model represents induced dipoles by a pair of
charges (the core atom and the Drude particle) connected by a harmonic
spring. See the "Howto polarizable"_Howto_polarizable.html doc page
for a discussion of all the polarizable models available in LAMMPS.
The Drude model has a number of features aimed at its use in
molecular systems ("Lamoureux and Roux"_#howto-Lamoureux):
Thermostating of the additional degrees of freedom associated with the
induced dipoles at very low temperature, in terms of the reduced
coordinates of the Drude particles with respect to their cores. This
makes the trajectory close to that of relaxed induced dipoles. :ulb,l
Consistent definition of 1-2 to 1-4 neighbors. A core-Drude particle
pair represents a single (polarizable) atom, so the special screening
factors in a covalent structure should be the same for the core and
the Drude particle. Drude particles have to inherit the 1-2, 1-3, 1-4
special neighbor relations from their respective cores. :l
Stabilization of the interactions between induced dipoles. Drude
dipoles on covalently bonded atoms interact too strongly due to the
short distances, so an atom may capture the Drude particle of a
neighbor, or the induced dipoles within the same molecule may align
too much. To avoid this, damping at short range can be done by Thole
functions (for which there are physical grounds). This Thole damping
is applied to the point charges composing the induced dipole (the
charge of the Drude particle and the opposite charge on the core, not
to the total charge of the core atom). :l,ule
A detailed tutorial covering the usage of Drude induced dipoles in
LAMMPS is on the "Howto drude2e"_Howto_drude2.html doc page.
As with the core-shell model, the cores and Drude particles should
appear in the data file as standard atoms. The same holds for the
springs between them, which are described by standard harmonic bonds.
The nature of the atoms (core, Drude particle or non-polarizable) is
specified via the "fix drude"_fix_drude.html command. The special
list of neighbors is automatically refactored to account for the
equivalence of core and Drude particles as regards special 1-2 to 1-4
screening. It may be necessary to use the {extra/special/per/atom}
keyword of the "read_data"_read_data.html command. If using "fix
shake"_fix_shake.html, make sure no Drude particle is in this fix
group.
There are two ways to thermostat the Drude particles at a low
temperature: use either "fix langevin/drude"_fix_langevin_drude.html
for a Langevin thermostat, or "fix
drude/transform/*"_fix_drude_transform.html for a Nose-Hoover
thermostat. The former requires use of the command "comm_modify vel
yes"_comm_modify.html. The latter requires two separate integration
fixes like {nvt} or {npt}. The correct temperatures of the reduced
degrees of freedom can be calculated using the "compute
temp/drude"_compute_temp_drude.html. This requires also to use the
command {comm_modify vel yes}.
Short-range damping of the induced dipole interactions can be achieved
using Thole functions through the "pair style
thole"_pair_thole.html in "pair_style hybrid/overlay"_pair_hybrid.html
with a Coulomb pair style. It may be useful to use {coul/long/cs} or
similar from the CORESHELL package if the core and Drude particle come
too close, which can cause numerical issues.
:line
:link(howto-Lamoureux)
[(Lamoureux and Roux)] G. Lamoureux, B. Roux, J. Chem. Phys 119, 3025 (2003)

2
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@ -9,7 +9,7 @@
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Section_commands.html#comm)
:link(lc,Commands_all.html)
:line

47
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@ -0,0 +1,47 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Calculate elastic constants :h3
Elastic constants characterize the stiffness of a material. The formal
definition is provided by the linear relation that holds between the
stress and strain tensors in the limit of infinitesimal deformation.
In tensor notation, this is expressed as s_ij = C_ijkl * e_kl, where
the repeated indices imply summation. s_ij are the elements of the
symmetric stress tensor. e_kl are the elements of the symmetric strain
tensor. C_ijkl are the elements of the fourth rank tensor of elastic
constants. In three dimensions, this tensor has 3^4=81 elements. Using
Voigt notation, the tensor can be written as a 6x6 matrix, where C_ij
is now the derivative of s_i w.r.t. e_j. Because s_i is itself a
derivative w.r.t. e_i, it follows that C_ij is also symmetric, with at
most 7*6/2 = 21 distinct elements.
At zero temperature, it is easy to estimate these derivatives by
deforming the simulation box in one of the six directions using the
"change_box"_change_box.html command and measuring the change in the
stress tensor. A general-purpose script that does this is given in the
examples/elastic directory described on the "Examples"_Examples.html
doc page.
Calculating elastic constants at finite temperature is more
challenging, because it is necessary to run a simulation that perfoms
time averages of differential properties. One way to do this is to
measure the change in average stress tensor in an NVT simulations when
the cell volume undergoes a finite deformation. In order to balance
the systematic and statistical errors in this method, the magnitude of
the deformation must be chosen judiciously, and care must be taken to
fully equilibrate the deformed cell before sampling the stress
tensor. Another approach is to sample the triclinic cell fluctuations
that occur in an NPT simulation. This method can also be slow to
converge and requires careful post-processing "(Shinoda)"_#Shinoda1
:line
:link(Shinoda1)
[(Shinoda)] Shinoda, Shiga, and Mikami, Phys Rev B, 69, 134103 (2004).

10
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@ -2,7 +2,7 @@
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Section_commands.html#comm)
:link(lc,Commands_all.html)
:line
@ -26,7 +26,7 @@ work required by the LAMMPS developers. Consequently, creating a pull
request will increase your chances to have your contribution included
and will reduce the time until the integration is complete. For more
information on the requirements to have your code included into LAMMPS
please see "Section 10.15"_Section_modify.html#mod_15
please see the "Modify contribute"_Modify_contribute.html doc page.
:line
@ -124,7 +124,7 @@ unrelated feature, you should switch branches!
After everything is done, add the files to the branch and commit them:
$ git add doc/src/tutorial_github.txt
$ git add doc/src/Howto_github.txt
$ git add doc/src/JPG/tutorial*.png :pre
IMPORTANT NOTE: Do not use {git commit -a} (or {git add -A}). The -a
@ -318,7 +318,7 @@ Because the changes are OK with us, we are going to merge by clicking on
Now, since in the meantime our local text for the tutorial also changed,
we need to pull Axel's change back into our branch, and merge them:
$ git add tutorial_github.txt
$ git add Howto_github.txt
$ git add JPG/tutorial_reverse_pull_request*.png
$ git commit -m "Updated text and images on reverse pull requests"
$ git pull :pre
@ -331,7 +331,7 @@ With Axel's changes merged in and some final text updates, our feature
branch is now perfect as far as we are concerned, so we are going to
commit and push again:
$ git add tutorial_github.txt
$ git add Howto_github.txt
$ git add JPG/tutorial_reverse_pull_request6.png
$ git commit -m "Merged Axel's suggestions and updated text"
$ git push git@github.com:Pakketeretet2/lammps :pre

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@ -0,0 +1,57 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Granular models :h3
Granular system are composed of spherical particles with a diameter,
as opposed to point particles. This means they have an angular
velocity and torque can be imparted to them to cause them to rotate.
To run a simulation of a granular model, you will want to use
the following commands:
"atom_style sphere"_atom_style.html
"fix nve/sphere"_fix_nve_sphere.html
"fix gravity"_fix_gravity.html :ul
This compute
"compute erotate/sphere"_compute_erotate_sphere.html :ul
calculates rotational kinetic energy which can be "output with
thermodynamic info"_Howto_output.html.
Use one of these 3 pair potentials, which compute forces and torques
between interacting pairs of particles:
"pair_style"_pair_style.html gran/history
"pair_style"_pair_style.html gran/no_history
"pair_style"_pair_style.html gran/hertzian :ul
These commands implement fix options specific to granular systems:
"fix freeze"_fix_freeze.html
"fix pour"_fix_pour.html
"fix viscous"_fix_viscous.html
"fix wall/gran"_fix_wall_gran.html :ul
The fix style {freeze} zeroes both the force and torque of frozen
atoms, and should be used for granular system instead of the fix style
{setforce}.
For computational efficiency, you can eliminate needless pairwise
computations between frozen atoms by using this command:
"neigh_modify"_neigh_modify.html exclude :ul
NOTE: By default, for 2d systems, granular particles are still modeled
as 3d spheres, not 2d discs (circles), meaning their moment of inertia
will be the same as in 3d. If you wish to model granular particles in
2d as 2d discs, see the note on this topic on the "Howto 2d"_Howto_2d
doc page, where 2d simulations are discussed.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Calculate thermal conductivity :h3
The thermal conductivity kappa of a material can be measured in at
least 4 ways using various options in LAMMPS. See the examples/KAPPA
directory for scripts that implement the 4 methods discussed here for
a simple Lennard-Jones fluid model. Also, see the "Howto
viscosity"_Howto_viscosity.html doc page for an analogous discussion
for viscosity.
The thermal conductivity tensor kappa is a measure of the propensity
of a material to transmit heat energy in a diffusive manner as given
by Fourier's law
J = -kappa grad(T)
where J is the heat flux in units of energy per area per time and
grad(T) is the spatial gradient of temperature. The thermal
conductivity thus has units of energy per distance per time per degree
K and is often approximated as an isotropic quantity, i.e. as a
scalar.
The first method is to setup two thermostatted regions at opposite
ends of a simulation box, or one in the middle and one at the end of a
periodic box. By holding the two regions at different temperatures
with a "thermostatting fix"_Howto_thermostat.html, the energy added to
the hot region should equal the energy subtracted from the cold region
and be proportional to the heat flux moving between the regions. See
the papers by "Ikeshoji and Hafskjold"_#howto-Ikeshoji and
"Wirnsberger et al"_#howto-Wirnsberger for details of this idea. Note
that thermostatting fixes such as "fix nvt"_fix_nh.html, "fix
langevin"_fix_langevin.html, and "fix
temp/rescale"_fix_temp_rescale.html store the cumulative energy they
add/subtract.
Alternatively, as a second method, the "fix heat"_fix_heat.html or
"fix ehex"_fix_ehex.html commands can be used in place of thermostats
on each of two regions to add/subtract specified amounts of energy to
both regions. In both cases, the resulting temperatures of the two
regions can be monitored with the "compute temp/region" command and
the temperature profile of the intermediate region can be monitored
with the "fix ave/chunk"_fix_ave_chunk.html and "compute
ke/atom"_compute_ke_atom.html commands.
The third method is to perform a reverse non-equilibrium MD simulation
using the "fix thermal/conductivity"_fix_thermal_conductivity.html
command which implements the rNEMD algorithm of Muller-Plathe.
Kinetic energy is swapped between atoms in two different layers of the
simulation box. This induces a temperature gradient between the two
layers which can be monitored with the "fix
ave/chunk"_fix_ave_chunk.html and "compute
ke/atom"_compute_ke_atom.html commands. The fix tallies the
cumulative energy transfer that it performs. See the "fix
thermal/conductivity"_fix_thermal_conductivity.html command for
details.
The fourth method is based on the Green-Kubo (GK) formula which
relates the ensemble average of the auto-correlation of the heat flux
to kappa. The heat flux can be calculated from the fluctuations of
per-atom potential and kinetic energies and per-atom stress tensor in
a steady-state equilibrated simulation. This is in contrast to the
two preceding non-equilibrium methods, where energy flows continuously
between hot and cold regions of the simulation box.
The "compute heat/flux"_compute_heat_flux.html command can calculate
the needed heat flux and describes how to implement the Green_Kubo
formalism using additional LAMMPS commands, such as the "fix
ave/correlate"_fix_ave_correlate.html command to calculate the needed
auto-correlation. See the doc page for the "compute
heat/flux"_compute_heat_flux.html command for an example input script
that calculates the thermal conductivity of solid Ar via the GK
formalism.
:line
:link(howto-Ikeshoji)
[(Ikeshoji)] Ikeshoji and Hafskjold, Molecular Physics, 81, 251-261
(1994).
:link(howto-Wirnsberger)
[(Wirnsberger)] Wirnsberger, Frenkel, and Dellago, J Chem Phys, 143, 124104
(2015).

208
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@ -0,0 +1,208 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Library interface to LAMMPS :h3
As described in "Section 2.5"_Section_start.html#start_5, LAMMPS can
be built as a library, so that it can be called by another code, used
in a "coupled manner"_Howto_couple.html with other codes, or driven
through a "Python interface"_Python.html.
All of these methodologies use a C-style interface to LAMMPS that is
provided in the files src/library.cpp and src/library.h. The
functions therein have a C-style argument list, but contain C++ code
you could write yourself in a C++ application that was invoking LAMMPS
directly. The C++ code in the functions illustrates how to invoke
internal LAMMPS operations. Note that LAMMPS classes are defined
within a LAMMPS namespace (LAMMPS_NS) if you use them from another C++
application.
The examples/COUPLE and python/examples directories have example C++
and C and Python codes which show how a driver code can link to LAMMPS
as a library, run LAMMPS on a subset of processors, grab data from
LAMMPS, change it, and put it back into LAMMPS.
The file src/library.cpp contains the following functions for creating
and destroying an instance of LAMMPS and sending it commands to
execute. See the documentation in the src/library.cpp file for
details.
NOTE: You can write code for additional functions as needed to define
how your code talks to LAMMPS and add them to src/library.cpp and
src/library.h, as well as to the "Python interface"_Python.html. The
added functions can access or change any internal LAMMPS data you
wish.
void lammps_open(int, char **, MPI_Comm, void **)
void lammps_open_no_mpi(int, char **, void **)
void lammps_close(void *)
int lammps_version(void *)
void lammps_file(void *, char *)
char *lammps_command(void *, char *)
void lammps_commands_list(void *, int, char **)
void lammps_commands_string(void *, char *)
void lammps_free(void *) :pre
The lammps_open() function is used to initialize LAMMPS, passing in a
list of strings as if they were "command-line
arguments"_Section_start.html#start_6 when LAMMPS is run in
stand-alone mode from the command line, and a MPI communicator for
LAMMPS to run under. It returns a ptr to the LAMMPS object that is
created, and which is used in subsequent library calls. The
lammps_open() function can be called multiple times, to create
multiple instances of LAMMPS.
LAMMPS will run on the set of processors in the communicator. This
means the calling code can run LAMMPS on all or a subset of
processors. For example, a wrapper script might decide to alternate
between LAMMPS and another code, allowing them both to run on all the
processors. Or it might allocate half the processors to LAMMPS and
half to the other code and run both codes simultaneously before
syncing them up periodically. Or it might instantiate multiple
instances of LAMMPS to perform different calculations.
The lammps_open_no_mpi() function is similar except that no MPI
communicator is passed from the caller. Instead, MPI_COMM_WORLD is
used to instantiate LAMMPS, and MPI is initialized if necessary.
The lammps_close() function is used to shut down an instance of LAMMPS
and free all its memory.
The lammps_version() function can be used to determined the specific
version of the underlying LAMMPS code. This is particularly useful
when loading LAMMPS as a shared library via dlopen(). The code using
the library interface can than use this information to adapt to
changes to the LAMMPS command syntax between versions. The returned
LAMMPS version code is an integer (e.g. 2 Sep 2015 results in
20150902) that grows with every new LAMMPS version.
The lammps_file(), lammps_command(), lammps_commands_list(), and
lammps_commands_string() functions are used to pass one or more
commands to LAMMPS to execute, the same as if they were coming from an
input script.
Via these functions, the calling code can read or generate a series of
LAMMPS commands one or multiple at a time and pass it thru the library
interface to setup a problem and then run it in stages. The caller
can interleave the command function calls with operations it performs,
calls to extract information from or set information within LAMMPS, or
calls to another code's library.
The lammps_file() function passes the filename of an input script.
The lammps_command() function passes a single command as a string.
The lammps_commands_list() function passes multiple commands in a
char** list. In both lammps_command() and lammps_commands_list(),
individual commands may or may not have a trailing newline. The
lammps_commands_string() function passes multiple commands
concatenated into one long string, separated by newline characters.
In both lammps_commands_list() and lammps_commands_string(), a single
command can be spread across multiple lines, if the last printable
character of all but the last line is "&", the same as if the lines
appeared in an input script.
The lammps_free() function is a clean-up function to free memory that
the library allocated previously via other function calls. See
comments in src/library.cpp file for which other functions need this
clean-up.
The file src/library.cpp also contains these functions for extracting
information from LAMMPS and setting value within LAMMPS. Again, see
the documentation in the src/library.cpp file for details, including
which quantities can be queried by name:
int lammps_extract_setting(void *, char *)
void *lammps_extract_global(void *, char *)
void lammps_extract_box(void *, double *, double *,
double *, double *, double *, int *, int *)
void *lammps_extract_atom(void *, char *)
void *lammps_extract_compute(void *, char *, int, int)
void *lammps_extract_fix(void *, char *, int, int, int, int)
void *lammps_extract_variable(void *, char *, char *) :pre
The extract_setting() function returns info on the size
of data types (e.g. 32-bit or 64-bit atom IDs) used
by the LAMMPS executable (a compile-time choice).
The other extract functions return a pointer to various global or
per-atom quantities stored in LAMMPS or to values calculated by a
compute, fix, or variable. The pointer returned by the
extract_global() function can be used as a permanent reference to a
value which may change. For the extract_atom() method, see the
extract() method in the src/atom.cpp file for a list of valid per-atom
properties. New names could easily be added if the property you want
is not listed. For the other extract functions, the underlying
storage may be reallocated as LAMMPS runs, so you need to re-call the
function to assure a current pointer or returned value(s).
double lammps_get_thermo(void *, char *)
int lammps_get_natoms(void *) :pre
int lammps_set_variable(void *, char *, char *)
void lammps_reset_box(void *, double *, double *, double, double, double) :pre
The lammps_get_thermo() function returns the current value of a thermo
keyword as a double precision value.
The lammps_get_natoms() function returns the total number of atoms in
the system and can be used by the caller to allocate memory for the
lammps_gather_atoms() and lammps_scatter_atoms() functions.
The lammps_set_variable() function can set an existing string-style
variable to a new string value, so that subsequent LAMMPS commands can
access the variable.
The lammps_reset_box() function resets the size and shape of the
simulation box, e.g. as part of restoring a previously extracted and
saved state of a simulation.
void lammps_gather_atoms(void *, char *, int, int, void *)
void lammps_gather_atoms_concat(void *, char *, int, int, void *)
void lammps_gather_atoms_subset(void *, char *, int, int, int, int *, void *)
void lammps_scatter_atoms(void *, char *, int, int, void *)
void lammps_scatter_atoms_subset(void *, char *, int, int, int, int *, void *) :pre
void lammps_create_atoms(void *, int, tagint *, int *, double *, double *,
imageint *, int) :pre
The gather functions collect peratom info of the requested type (atom
coords, atom types, forces, etc) from all processors, and returns the
same vector of values to each callling processor. The scatter
functions do the inverse. They distribute a vector of peratom values,
passed by all calling processors, to invididual atoms, which may be
owned by different processos.
The lammps_gather_atoms() function does this for all N atoms in the
system, ordered by atom ID, from 1 to N. The
lammps_gather_atoms_concat() function does it for all N atoms, but
simply concatenates the subset of atoms owned by each processor. The
resulting vector is not ordered by atom ID. Atom IDs can be requetsed
by the same function if the caller needs to know the ordering. The
lammps_gather_subset() function allows the caller to request values
for only a subset of atoms (identified by ID).
For all 3 gather function, per-atom image flags can be retrieved in 2 ways.
If the count is specified as 1, they are returned
in a packed format with all three image flags stored in a single integer.
If the count is specified as 3, the values are unpacked into xyz flags
by the library before returning them.
The lammps_scatter_atoms() function takes a list of values for all N
atoms in the system, ordered by atom ID, from 1 to N, and assigns
those values to each atom in the system. The
lammps_scatter_atoms_subset() function takes a subset of IDs as an
argument and only scatters those values to the owning atoms.
The lammps_create_atoms() function takes a list of N atoms as input
with atom types and coords (required), an optionally atom IDs and
velocities and image flags. It uses the coords of each atom to assign
it as a new atom to the processor that owns it. This function is
useful to add atoms to a simulation or (in tandem with
lammps_reset_box()) to restore a previously extracted and saved state
of a simulation. Additional properties for the new atoms can then be
assigned via the lammps_scatter_atoms() or lammps_extract_atom()
functions.

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@ -2,11 +2,11 @@
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Section_commands.html#comm)
:link(lc,Commands_all.html)
:line
Manifolds (surfaces) :h2
Manifolds (surfaces) :h3
[Overview:]

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Run multiple simulations from one input script :h3
This can be done in several ways. See the documentation for
individual commands for more details on how these examples work.
If "multiple simulations" means continue a previous simulation for
more timesteps, then you simply use the "run"_run.html command
multiple times. For example, this script
units lj
atom_style atomic
read_data data.lj
run 10000
run 10000
run 10000
run 10000
run 10000 :pre
would run 5 successive simulations of the same system for a total of
50,000 timesteps.
If you wish to run totally different simulations, one after the other,
the "clear"_clear.html command can be used in between them to
re-initialize LAMMPS. For example, this script
units lj
atom_style atomic
read_data data.lj
run 10000
clear
units lj
atom_style atomic
read_data data.lj.new
run 10000 :pre
would run 2 independent simulations, one after the other.
For large numbers of independent simulations, you can use
"variables"_variable.html and the "next"_next.html and
"jump"_jump.html commands to loop over the same input script
multiple times with different settings. For example, this
script, named in.polymer
variable d index run1 run2 run3 run4 run5 run6 run7 run8
shell cd $d
read_data data.polymer
run 10000
shell cd ..
clear
next d
jump in.polymer :pre
would run 8 simulations in different directories, using a data.polymer
file in each directory. The same concept could be used to run the
same system at 8 different temperatures, using a temperature variable
and storing the output in different log and dump files, for example
variable a loop 8
variable t index 0.8 0.85 0.9 0.95 1.0 1.05 1.1 1.15
log log.$a
read data.polymer
velocity all create $t 352839
fix 1 all nvt $t $t 100.0
dump 1 all atom 1000 dump.$a
run 100000
clear
next t
next a
jump in.polymer :pre
All of the above examples work whether you are running on 1 or
multiple processors, but assumed you are running LAMMPS on a single
partition of processors. LAMMPS can be run on multiple partitions via
the "-partition" command-line switch as described in "this
section"_Section_start.html#start_6 of the manual.
In the last 2 examples, if LAMMPS were run on 3 partitions, the same
scripts could be used if the "index" and "loop" variables were
replaced with {universe}-style variables, as described in the
"variable"_variable.html command. Also, the "next t" and "next a"
commands would need to be replaced with a single "next a t" command.
With these modifications, the 8 simulations of each script would run
on the 3 partitions one after the other until all were finished.
Initially, 3 simulations would be started simultaneously, one on each
partition. When one finished, that partition would then start
the 4th simulation, and so forth, until all 8 were completed.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
NEMD simulations :h3
Non-equilibrium molecular dynamics or NEMD simulations are typically
used to measure a fluid's rheological properties such as viscosity.
In LAMMPS, such simulations can be performed by first setting up a
non-orthogonal simulation box (see the preceding Howto section).
A shear strain can be applied to the simulation box at a desired
strain rate by using the "fix deform"_fix_deform.html command. The
"fix nvt/sllod"_fix_nvt_sllod.html command can be used to thermostat
the sheared fluid and integrate the SLLOD equations of motion for the
system. Fix nvt/sllod uses "compute
temp/deform"_compute_temp_deform.html to compute a thermal temperature
by subtracting out the streaming velocity of the shearing atoms. The
velocity profile or other properties of the fluid can be monitored via
the "fix ave/chunk"_fix_ave_chunk.html command.
As discussed in the previous section on non-orthogonal simulation
boxes, the amount of tilt or skew that can be applied is limited by
LAMMPS for computational efficiency to be 1/2 of the parallel box
length. However, "fix deform"_fix_deform.html can continuously strain
a box by an arbitrary amount. As discussed in the "fix
deform"_fix_deform.html command, when the tilt value reaches a limit,
the box is flipped to the opposite limit which is an equivalent tiling
of periodic space. The strain rate can then continue to change as
before. In a long NEMD simulation these box re-shaping events may
occur many times.
In a NEMD simulation, the "remap" option of "fix
deform"_fix_deform.html should be set to "remap v", since that is what
"fix nvt/sllod"_fix_nvt_sllod.html assumes to generate a velocity
profile consistent with the applied shear strain rate.
An alternative method for calculating viscosities is provided via the
"fix viscosity"_fix_viscosity.html command.
NEMD simulations can also be used to measure transport properties of a fluid
through a pore or channel. Simulations of steady-state flow can be performed
using the "fix flow/gauss"_fix_flow_gauss.html command.

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@ -0,0 +1,307 @@
"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Output from LAMMPS (thermo, dumps, computes, fixes, variables) :h3
There are four basic kinds of LAMMPS output:
"Thermodynamic output"_thermo_style.html, which is a list
of quantities printed every few timesteps to the screen and logfile. :ulb,l
"Dump files"_dump.html, which contain snapshots of atoms and various
per-atom values and are written at a specified frequency. :l
Certain fixes can output user-specified quantities to files: "fix
ave/time"_fix_ave_time.html for time averaging, "fix
ave/chunk"_fix_ave_chunk.html for spatial or other averaging, and "fix
print"_fix_print.html for single-line output of
"variables"_variable.html. Fix print can also output to the
screen. :l
"Restart files"_restart.html. :l
:ule
A simulation prints one set of thermodynamic output and (optionally)
restart files. It can generate any number of dump files and fix
output files, depending on what "dump"_dump.html and "fix"_fix.html
commands you specify.
As discussed below, LAMMPS gives you a variety of ways to determine
what quantities are computed and printed when the thermodynamics,
dump, or fix commands listed above perform output. Throughout this
discussion, note that users can also "add their own computes and fixes
to LAMMPS"_Modify.html which can then generate values that can then be
output with these commands.
The following sub-sections discuss different LAMMPS command related
to output and the kind of data they operate on and produce:
"Global/per-atom/local data"_#global
"Scalar/vector/array data"_#scalar
"Thermodynamic output"_#thermo
"Dump file output"_#dump
"Fixes that write output files"_#fixoutput
"Computes that process output quantities"_#computeoutput
"Fixes that process output quantities"_#fixprocoutput
"Computes that generate values to output"_#compute
"Fixes that generate values to output"_#fix
"Variables that generate values to output"_#variable
"Summary table of output options and data flow between commands"_#table :ul
Global/per-atom/local data :h4,link(global)
Various output-related commands work with three different styles of
data: global, per-atom, or local. A global datum is one or more
system-wide values, e.g. the temperature of the system. A per-atom
datum is one or more values per atom, e.g. the kinetic energy of each
atom. Local datums are calculated by each processor based on the
atoms it owns, but there may be zero or more per atom, e.g. a list of
bond distances.
Scalar/vector/array data :h4,link(scalar)
Global, per-atom, and local datums can each come in three kinds: a
single scalar value, a vector of values, or a 2d array of values. The
doc page for a "compute" or "fix" or "variable" that generates data
will specify both the style and kind of data it produces, e.g. a
per-atom vector.
When a quantity is accessed, as in many of the output commands
discussed below, it can be referenced via the following bracket
notation, where ID in this case is the ID of a compute. The leading
"c_" would be replaced by "f_" for a fix, or "v_" for a variable:
c_ID | entire scalar, vector, or array
c_ID\[I\] | one element of vector, one column of array
c_ID\[I\]\[J\] | one element of array :tb(s=|)
In other words, using one bracket reduces the dimension of the data
once (vector -> scalar, array -> vector). Using two brackets reduces
the dimension twice (array -> scalar). Thus a command that uses
scalar values as input can typically also process elements of a vector
or array.
Thermodynamic output :h4,link(thermo)
The frequency and format of thermodynamic output is set by the
"thermo"_thermo.html, "thermo_style"_thermo_style.html, and
"thermo_modify"_thermo_modify.html commands. The
"thermo_style"_thermo_style.html command also specifies what values
are calculated and written out. Pre-defined keywords can be specified
(e.g. press, etotal, etc). Three additional kinds of keywords can
also be specified (c_ID, f_ID, v_name), where a "compute"_compute.html
or "fix"_fix.html or "variable"_variable.html provides the value to be
output. In each case, the compute, fix, or variable must generate
global values for input to the "thermo_style custom"_dump.html
command.
Note that thermodynamic output values can be "extensive" or
"intensive". The former scale with the number of atoms in the system
(e.g. total energy), the latter do not (e.g. temperature). The
setting for "thermo_modify norm"_thermo_modify.html determines whether
extensive quantities are normalized or not. Computes and fixes
produce either extensive or intensive values; see their individual doc
pages for details. "Equal-style variables"_variable.html produce only
intensive values; you can include a division by "natoms" in the
formula if desired, to make an extensive calculation produce an
intensive result.
Dump file output :h4,link(dump)
Dump file output is specified by the "dump"_dump.html and
"dump_modify"_dump_modify.html commands. There are several
pre-defined formats (dump atom, dump xtc, etc).
There is also a "dump custom"_dump.html format where the user
specifies what values are output with each atom. Pre-defined atom
attributes can be specified (id, x, fx, etc). Three additional kinds
of keywords can also be specified (c_ID, f_ID, v_name), where a
"compute"_compute.html or "fix"_fix.html or "variable"_variable.html
provides the values to be output. In each case, the compute, fix, or
variable must generate per-atom values for input to the "dump
custom"_dump.html command.
There is also a "dump local"_dump.html format where the user specifies
what local values to output. A pre-defined index keyword can be
specified to enumerate the local values. Two additional kinds of
keywords can also be specified (c_ID, f_ID), where a
"compute"_compute.html or "fix"_fix.html or "variable"_variable.html
provides the values to be output. In each case, the compute or fix
must generate local values for input to the "dump local"_dump.html
command.
Fixes that write output files :h4,link(fixoutput)
Several fixes take various quantities as input and can write output
files: "fix ave/time"_fix_ave_time.html, "fix
ave/chunk"_fix_ave_chunk.html, "fix ave/histo"_fix_ave_histo.html,
"fix ave/correlate"_fix_ave_correlate.html, and "fix
print"_fix_print.html.
The "fix ave/time"_fix_ave_time.html command enables direct output to
a file and/or time-averaging of global scalars or vectors. The user
specifies one or more quantities as input. These can be global
"compute"_compute.html values, global "fix"_fix.html values, or
"variables"_variable.html of any style except the atom style which
produces per-atom values. Since a variable can refer to keywords used
by the "thermo_style custom"_thermo_style.html command (like temp or
press) and individual per-atom values, a wide variety of quantities
can be time averaged and/or output in this way. If the inputs are one
or more scalar values, then the fix generate a global scalar or vector
of output. If the inputs are one or more vector values, then the fix
generates a global vector or array of output. The time-averaged
output of this fix can also be used as input to other output commands.
The "fix ave/chunk"_fix_ave_chunk.html command enables direct output
to a file of chunk-averaged per-atom quantities like those output in
dump files. Chunks can represent spatial bins or other collections of
atoms, e.g. individual molecules. The per-atom quantities can be atom
density (mass or number) or atom attributes such as position,
velocity, force. They can also be per-atom quantities calculated by a
"compute"_compute.html, by a "fix"_fix.html, or by an atom-style
"variable"_variable.html. The chunk-averaged output of this fix can
also be used as input to other output commands.
The "fix ave/histo"_fix_ave_histo.html command enables direct output
to a file of histogrammed quantities, which can be global or per-atom
or local quantities. The histogram output of this fix can also be
used as input to other output commands.
The "fix ave/correlate"_fix_ave_correlate.html command enables direct
output to a file of time-correlated quantities, which can be global
values. The correlation matrix output of this fix can also be used as
input to other output commands.
The "fix print"_fix_print.html command can generate a line of output
written to the screen and log file or to a separate file, periodically
during a running simulation. The line can contain one or more
"variable"_variable.html values for any style variable except the
vector or atom styles). As explained above, variables themselves can
contain references to global values generated by "thermodynamic
keywords"_thermo_style.html, "computes"_compute.html,
"fixes"_fix.html, or other "variables"_variable.html, or to per-atom
values for a specific atom. Thus the "fix print"_fix_print.html
command is a means to output a wide variety of quantities separate
from normal thermodynamic or dump file output.
Computes that process output quantities :h4,link(computeoutput)
The "compute reduce"_compute_reduce.html and "compute
reduce/region"_compute_reduce.html commands take one or more per-atom
or local vector quantities as inputs and "reduce" them (sum, min, max,
ave) to scalar quantities. These are produced as output values which
can be used as input to other output commands.
The "compute slice"_compute_slice.html command take one or more global
vector or array quantities as inputs and extracts a subset of their
values to create a new vector or array. These are produced as output
values which can be used as input to other output commands.
The "compute property/atom"_compute_property_atom.html command takes a
list of one or more pre-defined atom attributes (id, x, fx, etc) and
stores the values in a per-atom vector or array. These are produced
as output values which can be used as input to other output commands.
The list of atom attributes is the same as for the "dump
custom"_dump.html command.
The "compute property/local"_compute_property_local.html command takes
a list of one or more pre-defined local attributes (bond info, angle
info, etc) and stores the values in a local vector or array. These
are produced as output values which can be used as input to other
output commands.
Fixes that process output quantities :h4,link(fixprocoutput)
The "fix vector"_fix_vector.html command can create global vectors as
output from global scalars as input, accumulating them one element at
a time.
The "fix ave/atom"_fix_ave_atom.html command performs time-averaging
of per-atom vectors. The per-atom quantities can be atom attributes
such as position, velocity, force. They can also be per-atom
quantities calculated by a "compute"_compute.html, by a
"fix"_fix.html, or by an atom-style "variable"_variable.html. The
time-averaged per-atom output of this fix can be used as input to
other output commands.
The "fix store/state"_fix_store_state.html command can archive one or
more per-atom attributes at a particular time, so that the old values
can be used in a future calculation or output. The list of atom
attributes is the same as for the "dump custom"_dump.html command,
including per-atom quantities calculated by a "compute"_compute.html,
by a "fix"_fix.html, or by an atom-style "variable"_variable.html.
The output of this fix can be used as input to other output commands.
Computes that generate values to output :h4,link(compute)
Every "compute"_compute.html in LAMMPS produces either global or
per-atom or local values. The values can be scalars or vectors or
arrays of data. These values can be output using the other commands
described in this section. The doc page for each compute command
describes what it produces. Computes that produce per-atom or local
values have the word "atom" or "local" in their style name. Computes
without the word "atom" or "local" produce global values.
Fixes that generate values to output :h4,link(fix)
Some "fixes"_fix.html in LAMMPS produces either global or per-atom or
local values which can be accessed by other commands. The values can
be scalars or vectors or arrays of data. These values can be output
using the other commands described in this section. The doc page for
each fix command tells whether it produces any output quantities and
describes them.
Variables that generate values to output :h4,link(variable)
"Variables"_variable.html defined in an input script can store one or
more strings. But equal-style, vector-style, and atom-style or
atomfile-style variables generate a global scalar value, global vector
or values, or a per-atom vector, respectively, when accessed. The
formulas used to define these variables can contain references to the
thermodynamic keywords and to global and per-atom data generated by
computes, fixes, and other variables. The values generated by
variables can be used as input to and thus output by the other
commands described in this section.
Summary table of output options and data flow between commands :h4,link(table)
This table summarizes the various commands that can be used for
generating output from LAMMPS. Each command produces output data of
some kind and/or writes data to a file. Most of the commands can take
data from other commands as input. Thus you can link many of these
commands together in pipeline form, where data produced by one command
is used as input to another command and eventually written to the
screen or to a file. Note that to hook two commands together the
output and input data types must match, e.g. global/per-atom/local
data and scalar/vector/array data.
Also note that, as described above, when a command takes a scalar as
input, that could be an element of a vector or array. Likewise a
vector input could be a column of an array.
Command: Input: Output:
"thermo_style custom"_thermo_style.html: global scalars: screen, log file:
"dump custom"_dump.html: per-atom vectors: dump file:
"dump local"_dump.html: local vectors: dump file:
"fix print"_fix_print.html: global scalar from variable: screen, file:
"print"_print.html: global scalar from variable: screen:
"computes"_compute.html: N/A: global/per-atom/local scalar/vector/array:
"fixes"_fix.html: N/A: global/per-atom/local scalar/vector/array:
"variables"_variable.html: global scalars and vectors, per-atom vectors: global scalar and vector, per-atom vector:
"compute reduce"_compute_reduce.html: per-atom/local vectors: global scalar/vector:
"compute slice"_compute_slice.html: global vectors/arrays: global vector/array:
"compute property/atom"_compute_property_atom.html: per-atom vectors: per-atom vector/array:
"compute property/local"_compute_property_local.html: local vectors: local vector/array:
"fix vector"_fix_vector.html: global scalars: global vector:
"fix ave/atom"_fix_ave_atom.html: per-atom vectors: per-atom vector/array:
"fix ave/time"_fix_ave_time.html: global scalars/vectors: global scalar/vector/array, file:
"fix ave/chunk"_fix_ave_chunk.html: per-atom vectors: global array, file:
"fix ave/histo"_fix_ave_histo.html: global/per-atom/local scalars and vectors: global array, file:
"fix ave/correlate"_fix_ave_correlate.html: global scalars: global array, file:
"fix store/state"_fix_store_state.html: per-atom vectors: per-atom vector/array :tb(c=3,s=:)

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Polarizable models :h3
In polarizable force fields the charge distributions in molecules and
materials respond to their electrostatic environments. Polarizable
systems can be simulated in LAMMPS using three methods:
the fluctuating charge method, implemented in the "QEQ"_fix_qeq.html
package, :ulb,l
the adiabatic core-shell method, implemented in the
"CORESHELL"_Howto_coreshell.html package, :l
the thermalized Drude dipole method, implemented in the
"USER-DRUDE"_Howto_drude.html package. :l,ule
The fluctuating charge method calculates instantaneous charges on
interacting atoms based on the electronegativity equalization
principle. It is implemented in the "fix qeq"_fix_qeq.html which is
available in several variants. It is a relatively efficient technique
since no additional particles are introduced. This method allows for
charge transfer between molecules or atom groups. However, because the
charges are located at the interaction sites, off-plane components of
polarization cannot be represented in planar molecules or atom groups.
The two other methods share the same basic idea: polarizable atoms are
split into one core atom and one satellite particle (called shell or
Drude particle) attached to it by a harmonic spring. Both atoms bear
a charge and they represent collectively an induced electric dipole.
These techniques are computationally more expensive than the QEq
method because of additional particles and bonds. These two
charge-on-spring methods differ in certain features, with the
core-shell model being normally used for ionic/crystalline materials,
whereas the so-called Drude model is normally used for molecular
systems and fluid states.
The core-shell model is applicable to crystalline materials where the
high symmetry around each site leads to stable trajectories of the
core-shell pairs. However, bonded atoms in molecules can be so close
that a core would interact too strongly or even capture the Drude
particle of a neighbor. The Drude dipole model is relatively more
complex in order to remediate this and other issues. Specifically, the
Drude model includes specific thermostating of the core-Drude pairs
and short-range damping of the induced dipoles.
The three polarization methods can be implemented through a
self-consistent calculation of charges or induced dipoles at each
timestep. In the fluctuating charge scheme this is done by the matrix
inversion method in "fix qeq/point"_fix_qeq.html, but for core-shell
or Drude-dipoles the relaxed-dipoles technique would require an slow
iterative procedure. These self-consistent solutions yield accurate
trajectories since the additional degrees of freedom representing
polarization are massless. An alternative is to attribute a mass to
the additional degrees of freedom and perform time integration using
an extended Lagrangian technique. For the fluctuating charge scheme
this is done by "fix qeq/dynamic"_fix_qeq.html, and for the
charge-on-spring models by the methods outlined in the next two
sections. The assignment of masses to the additional degrees of
freedom can lead to unphysical trajectories if care is not exerted in
choosing the parameters of the polarizable models and the simulation
conditions.
In the core-shell model the vibration of the shells is kept faster
than the ionic vibrations to mimic the fast response of the
polarizable electrons. But in molecular systems thermalizing the
core-Drude pairs at temperatures comparable to the rest of the
simulation leads to several problems (kinetic energy transfer, too
short a timestep, etc.) In order to avoid these problems the relative
motion of the Drude particles with respect to their cores is kept
"cold" so the vibration of the core-Drude pairs is very slow,
approaching the self-consistent regime. In both models the
temperature is regulated using the velocities of the center of mass of
core+shell (or Drude) pairs, but in the Drude model the actual
relative core-Drude particle motion is thermostated separately as
well.

23
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@ -2,7 +2,7 @@
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Section_commands.html#comm)
:link(lc,Commands_all.html)
:line
@ -15,13 +15,19 @@ END_RST -->
Overview :h4
PyLammps is a Python wrapper class which can be created on its own or use an
existing lammps Python object. It creates a simpler, Python-like interface to
common LAMMPS functionality. Unlike the original flat C-types interface, it
exposes a discoverable API. It no longer requires knowledge of the underlying
C++ code implementation. Finally, the IPyLammps wrapper builds on top of
PyLammps and adds some additional features for IPython integration into IPython
notebooks, e.g. for embedded visualization output from dump/image.
PyLammps is a Python wrapper class which can be created on its own or
use an existing lammps Python object. It creates a simpler,
Python-like interface to common LAMMPS functionality, in contrast to
the lammps.py wrapper on the C-style LAMMPS library interface which is
written using Python ctypes. The lammps.py wrapper is discussed on
the "Python library"_Python_library.html doc page.
Unlike the flat ctypes interface, PyLammps exposes a discoverable API.
It no longer requires knowledge of the underlying C++ code
implementation. Finally, the IPyLammps wrapper builds on top of
PyLammps and adds some additional features for IPython integration
into IPython notebooks, e.g. for embedded visualization output from
dump/image.
Comparison of lammps and PyLammps interfaces :h5
@ -40,7 +46,6 @@ communication with LAMMPS is hidden from API user
shorter, more concise Python
better IPython integration, designed for quick prototyping :ul
Quick Start :h4
System-wide Installation :h5

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Multi-replica simulations :h3
Several commands in LAMMPS run mutli-replica simulations, meaning
that multiple instances (replicas) of your simulation are run
simultaneously, with small amounts of data exchanged between replicas
periodically.
These are the relevant commands:
"neb"_neb.html for nudged elastic band calculations
"prd"_prd.html for parallel replica dynamics
"tad"_tad.html for temperature accelerated dynamics
"temper"_temper.html for parallel tempering
"fix pimd"_fix_pimd.html for path-integral molecular dynamics (PIMD) :ul
NEB is a method for finding transition states and barrier energies.
PRD and TAD are methods for performing accelerated dynamics to find
and perform infrequent events. Parallel tempering or replica exchange
runs different replicas at a series of temperature to facilitate
rare-event sampling.
These commands 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.
PIMD runs different replicas whose individual particles are coupled
together by springs to model a system or ring-polymers.
This commands can only be used if LAMMPS was built with the USER-MISC
package. See the "Making LAMMPS"_Section_start.html#start_3 section
for more info on packages.
In all these cases, you must run with one or more processors per
replica. The processors assigned to each replica are determined at
run-time by using the "-partition command-line
switch"_Section_start.html#start_6 to launch LAMMPS on multiple
partitions, which in this context are the same as replicas. E.g.
these commands:
mpirun -np 16 lmp_linux -partition 8x2 -in in.temper
mpirun -np 8 lmp_linux -partition 8x1 -in in.neb :pre
would each run 8 replicas, on either 16 or 8 processors. Note the use
of the "-in command-line switch"_Section_start.html#start_6 to specify
the input script which is required when running in multi-replica mode.
Also note that with MPI installed on a machine (e.g. your desktop),
you can run on more (virtual) processors than you have physical
processors. Thus the above commands could be run on a
single-processor (or few-processor) desktop so that you can run
a multi-replica simulation on more replicas than you have
physical processors.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Restart a simulation :h3
There are 3 ways to continue a long LAMMPS simulation. Multiple
"run"_run.html commands can be used in the same input script. Each
run will continue from where the previous run left off. Or binary
restart files can be saved to disk using the "restart"_restart.html
command. At a later time, these binary files can be read via a
"read_restart"_read_restart.html command in a new script. Or they can
be converted to text data files using the "-r command-line
switch"_Section_start.html#start_6 and read by a
"read_data"_read_data.html command in a new script.
Here we give examples of 2 scripts that read either a binary restart
file or a converted data file and then issue a new run command to
continue where the previous run left off. They illustrate what
settings must be made in the new script. Details are discussed in the
documentation for the "read_restart"_read_restart.html and
"read_data"_read_data.html commands.
Look at the {in.chain} input script provided in the {bench} directory
of the LAMMPS distribution to see the original script that these 2
scripts are based on. If that script had the line
restart 50 tmp.restart :pre
added to it, it would produce 2 binary restart files (tmp.restart.50
and tmp.restart.100) as it ran.
This script could be used to read the 1st restart file and re-run the
last 50 timesteps:
read_restart tmp.restart.50 :pre
neighbor 0.4 bin
neigh_modify every 1 delay 1 :pre
fix 1 all nve
fix 2 all langevin 1.0 1.0 10.0 904297 :pre
timestep 0.012 :pre
run 50 :pre
Note that the following commands do not need to be repeated because
their settings are included in the restart file: {units, atom_style,
special_bonds, pair_style, bond_style}. However these commands do
need to be used, since their settings are not in the restart file:
{neighbor, fix, timestep}.
If you actually use this script to perform a restarted run, you will
notice that the thermodynamic data match at step 50 (if you also put a
"thermo 50" command in the original script), but do not match at step
100. This is because the "fix langevin"_fix_langevin.html command
uses random numbers in a way that does not allow for perfect restarts.
As an alternate approach, the restart file could be converted to a data
file as follows:
lmp_g++ -r tmp.restart.50 tmp.restart.data :pre
Then, this script could be used to re-run the last 50 steps:
units lj
atom_style bond
pair_style lj/cut 1.12
pair_modify shift yes
bond_style fene
special_bonds 0.0 1.0 1.0 :pre
read_data tmp.restart.data :pre
neighbor 0.4 bin
neigh_modify every 1 delay 1 :pre
fix 1 all nve
fix 2 all langevin 1.0 1.0 10.0 904297 :pre
timestep 0.012 :pre
reset_timestep 50
run 50 :pre
Note that nearly all the settings specified in the original {in.chain}
script must be repeated, except the {pair_coeff} and {bond_coeff}
commands since the new data file lists the force field coefficients.
Also, the "reset_timestep"_reset_timestep.html command is used to tell
LAMMPS the current timestep. This value is stored in restart files,
but not in data files.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
SPC water model :h3
The SPC water model specifies a 3-site rigid water molecule with
charges and Lennard-Jones parameters assigned to each of the 3 atoms.
In LAMMPS the "fix shake"_fix_shake.html command can be used to hold
the two O-H bonds and the H-O-H angle rigid. A bond style of
{harmonic} and an angle style of {harmonic} or {charmm} should also be
used.
These are the additional parameters (in real units) to set for O and H
atoms and the water molecule to run a rigid SPC model.
O mass = 15.9994
H mass = 1.008
O charge = -0.820
H charge = 0.410
LJ epsilon of OO = 0.1553
LJ sigma of OO = 3.166
LJ epsilon, sigma of OH, HH = 0.0
r0 of OH bond = 1.0
theta of HOH angle = 109.47 :all(b),p
Note that as originally proposed, the SPC model was run with a 9
Angstrom cutoff for both LJ and Coulommbic terms. It can also be used
with long-range Coulombics (Ewald or PPPM in LAMMPS), without changing
any of the parameters above, though it becomes a different model in
that mode of usage.
The SPC/E (extended) water model is the same, except
the partial charge assignments change:
O charge = -0.8476
H charge = 0.4238 :all(b),p
See the "(Berendsen)"_#howto-Berendsen reference for more details on both
the SPC and SPC/E models.
Wikipedia also has a nice article on "water
models"_http://en.wikipedia.org/wiki/Water_model.
:line
:link(howto-Berendsen)
[(Berendsen)] Berendsen, Grigera, Straatsma, J Phys Chem, 91,
6269-6271 (1987).

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Finite-size spherical and aspherical particles :h3
Typical MD models treat atoms or particles as point masses. Sometimes
it is desirable to have a model with finite-size particles such as
spheroids or ellipsoids or generalized aspherical bodies. The
difference is that such particles have a moment of inertia, rotational
energy, and angular momentum. Rotation is induced by torque coming
from interactions with other particles.
LAMMPS has several options for running simulations with these kinds of
particles. The following aspects are discussed in turn:
atom styles
pair potentials
time integration
computes, thermodynamics, and dump output
rigid bodies composed of finite-size particles :ul
Example input scripts for these kinds of models are in the body,
colloid, dipole, ellipse, line, peri, pour, and tri directories of the
"examples directory"_Examples.html in the LAMMPS distribution.
Atom styles :h4
There are several "atom styles"_atom_style.html that allow for
definition of finite-size particles: sphere, dipole, ellipsoid, line,
tri, peri, and body.
The sphere style defines particles that are spheriods and each
particle can have a unique diameter and mass (or density). These
particles store an angular velocity (omega) and can be acted upon by
torque. The "set" command can be used to modify the diameter and mass
of individual particles, after then are created.
The dipole style does not actually define finite-size particles, but
is often used in conjunction with spherical particles, via a command
like
atom_style hybrid sphere dipole :pre
This is because when dipoles interact with each other, they induce
torques, and a particle must be finite-size (i.e. have a moment of
inertia) in order to respond and rotate. See the "atom_style
dipole"_atom_style.html command for details. The "set" command can be
used to modify the orientation and length of the dipole moment of
individual particles, after then are created.
The ellipsoid style defines particles that are ellipsoids and thus can
be aspherical. Each particle has a shape, specified by 3 diameters,
and mass (or density). These particles store an angular momentum and
their orientation (quaternion), and can be acted upon by torque. They
do not store an angular velocity (omega), which can be in a different
direction than angular momentum, rather they compute it as needed.
The "set" command can be used to modify the diameter, orientation, and
mass of individual particles, after then are created. It also has a
brief explanation of what quaternions are.
The line style defines line segment particles with two end points and
a mass (or density). They can be used in 2d simulations, and they can
be joined together to form rigid bodies which represent arbitrary
polygons.
The tri style defines triangular particles with three corner points
and a mass (or density). They can be used in 3d simulations, and they
can be joined together to form rigid bodies which represent arbitrary
particles with a triangulated surface.
The peri style is used with "Peridynamic models"_pair_peri.html and
defines particles as having a volume, that is used internally in the
"pair_style peri"_pair_peri.html potentials.
The body style allows for definition of particles which can represent
complex entities, such as surface meshes of discrete points,
collections of sub-particles, deformable objects, etc. The body style
is discussed in more detail on the "Howto body"_Howto_body.html doc
page.
Note that if one of these atom styles is used (or multiple styles via
the "atom_style hybrid"_atom_style.html command), not all particles in
the system are required to be finite-size or aspherical.
For example, in the ellipsoid style, if the 3 shape parameters are set
to the same value, the particle will be a sphere rather than an
ellipsoid. If the 3 shape parameters are all set to 0.0 or if the
diameter is set to 0.0, it will be a point particle. In the line or
tri style, if the lineflag or triflag is specified as 0, then it
will be a point particle.
Some of the pair styles used to compute pairwise interactions between
finite-size particles also compute the correct interaction with point
particles as well, e.g. the interaction between a point particle and a
finite-size particle or between two point particles. If necessary,
"pair_style hybrid"_pair_hybrid.html can be used to insure the correct
interactions are computed for the appropriate style of interactions.
Likewise, using groups to partition particles (ellipsoids versus
spheres versus point particles) will allow you to use the appropriate
time integrators and temperature computations for each class of
particles. See the doc pages for various commands for details.
Also note that for "2d simulations"_dimension.html, atom styles sphere
and ellipsoid still use 3d particles, rather than as circular disks or
ellipses. This means they have the same moment of inertia as the 3d
object. When temperature is computed, the correct degrees of freedom
are used for rotation in a 2d versus 3d system.
Pair potentials :h4
When a system with finite-size particles is defined, the particles
will only rotate and experience torque if the force field computes
such interactions. These are the various "pair
styles"_pair_style.html that generate torque:
"pair_style gran/history"_pair_gran.html
"pair_style gran/hertzian"_pair_gran.html
"pair_style gran/no_history"_pair_gran.html
"pair_style dipole/cut"_pair_dipole.html
"pair_style gayberne"_pair_gayberne.html
"pair_style resquared"_pair_resquared.html
"pair_style brownian"_pair_brownian.html
"pair_style lubricate"_pair_lubricate.html
"pair_style line/lj"_pair_line_lj.html
"pair_style tri/lj"_pair_tri_lj.html
"pair_style body/nparticle"_pair_body_nparticle.html :ul
The granular pair styles are used with spherical particles. The
dipole pair style is used with the dipole atom style, which could be
applied to spherical or ellipsoidal particles. The GayBerne and
REsquared potentials require ellipsoidal particles, though they will
also work if the 3 shape parameters are the same (a sphere). The
Brownian and lubrication potentials are used with spherical particles.
The line, tri, and body potentials are used with line segment,
triangular, and body particles respectively.
Time integration :h4
There are several fixes that perform time integration on finite-size
spherical particles, meaning the integrators update the rotational
orientation and angular velocity or angular momentum of the particles:
"fix nve/sphere"_fix_nve_sphere.html
"fix nvt/sphere"_fix_nvt_sphere.html
"fix npt/sphere"_fix_npt_sphere.html :ul
Likewise, there are 3 fixes that perform time integration on
ellipsoidal particles:
"fix nve/asphere"_fix_nve_asphere.html
"fix nvt/asphere"_fix_nvt_asphere.html
"fix npt/asphere"_fix_npt_asphere.html :ul
The advantage of these fixes is that those which thermostat the
particles include the rotational degrees of freedom in the temperature
calculation and thermostatting. The "fix langevin"_fix_langevin
command can also be used with its {omgea} or {angmom} options to
thermostat the rotational degrees of freedom for spherical or
ellipsoidal particles. Other thermostatting fixes only operate on the
translational kinetic energy of finite-size particles.
These fixes perform constant NVE time integration on line segment,
triangular, and body particles:
"fix nve/line"_fix_nve_line.html
"fix nve/tri"_fix_nve_tri.html
"fix nve/body"_fix_nve_body.html :ul
Note that for mixtures of point and finite-size particles, these
integration fixes can only be used with "groups"_group.html which
contain finite-size particles.
Computes, thermodynamics, and dump output :h4
There are several computes that calculate the temperature or
rotational energy of spherical or ellipsoidal particles:
"compute temp/sphere"_compute_temp_sphere.html
"compute temp/asphere"_compute_temp_asphere.html
"compute erotate/sphere"_compute_erotate_sphere.html
"compute erotate/asphere"_compute_erotate_asphere.html :ul
These include rotational degrees of freedom in their computation. If
you wish the thermodynamic output of temperature or pressure to use
one of these computes (e.g. for a system entirely composed of
finite-size particles), then the compute can be defined and the
"thermo_modify"_thermo_modify.html command used. Note that by default
thermodynamic quantities will be calculated with a temperature that
only includes translational degrees of freedom. See the
"thermo_style"_thermo_style.html command for details.
These commands can be used to output various attributes of finite-size
particles:
"dump custom"_dump.html
"compute property/atom"_compute_property_atom.html
"dump local"_dump.html
"compute body/local"_compute_body_local.html :ul
Attributes include the dipole moment, the angular velocity, the
angular momentum, the quaternion, the torque, the end-point and
corner-point coordinates (for line and tri particles), and
sub-particle attributes of body particles.
Rigid bodies composed of finite-size particles :h4
The "fix rigid"_fix_rigid.html command treats a collection of
particles as a rigid body, computes its inertia tensor, sums the total
force and torque on the rigid body each timestep due to forces on its
constituent particles, and integrates the motion of the rigid body.
If any of the constituent particles of a rigid body are finite-size
particles (spheres or ellipsoids or line segments or triangles), then
their contribution to the inertia tensor of the body is different than
if they were point particles. This means the rotational dynamics of
the rigid body will be different. Thus a model of a dimer is
different if the dimer consists of two point masses versus two
spheroids, even if the two particles have the same mass. Finite-size
particles that experience torque due to their interaction with other
particles will also impart that torque to a rigid body they are part
of.
See the "fix rigid" command for example of complex rigid-body models
it is possible to define in LAMMPS.
Note that the "fix shake"_fix_shake.html command can also be used to
treat 2, 3, or 4 particles as a rigid body, but it always assumes the
particles are point masses.
Also note that body particles cannot be modeled with the "fix
rigid"_fix_rigid.html command. Body particles are treated by LAMMPS
as single particles, though they can store internal state, such as a
list of sub-particles. Individual body partices are typically treated
as rigid bodies, and their motion integrated with a command like "fix
nve/body"_fix_nve_body.html. Interactions between pairs of body
particles are computed via a command like "pair_style
body/nparticle"_pair_body_nparticle.html.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Magnetic spins :h3
The magnetic spin simualtions are enabled by the SPIN package, whose
implementation is detailed in "Tranchida"_#Tranchida7.
The model representents the simulation of atomic magnetic spins coupled
to lattice vibrations. The dynamics of those magnetic spins can be used
to simulate a broad range a phenomena related to magneto-elasticity, or
or to study the influence of defects on the magnetic properties of
materials.
The magnetic spins are interacting with each others and with the
lattice via pair interactions. Typically, the magnetic exchange
interaction can be defined using the
"pair/spin/exchange"_pair_spin_exchange.html command. This exchange
applies a magnetic torque to a given spin, considering the orientation
of its neighboring spins and their relative distances.
It also applies a force on the atoms as a function of the spin
orientations and their associated inter-atomic distances.
The command "fix precession/spin"_fix_precession_spin.html allows to
apply a constant magnetic torque on all the spins in the system. This
torque can be an external magnetic field (Zeeman interaction), or an
uniaxial magnetic anisotropy.
A Langevin thermostat can be applied to those magnetic spins using
"fix langevin/spin"_fix_langevin_spin.html. Typically, this thermostat
can be coupled to another Langevin thermostat applied to the atoms
using "fix langevin"_fix_langevin.html in order to simulate
thermostated spin-lattice system.
The magnetic Gilbert damping can also be applied using "fix
langevin/spin"_fix_langevin_spin.html. It allows to either dissipate
the thermal energy of the Langevin thermostat, or to perform a
relaxation of the magnetic configuration toward an equilibrium state.
All the computed magnetic properties can be outputed by two main
commands. The first one is "compute spin"_compute_spin.html, that
enables to evaluate magnetic averaged quantities, such as the total
magnetization of the system along x, y, or z, the spin temperature, or
the magnetic energy. The second command is "compute
property/atom"_compute_property_atom.html. It enables to output all the
per atom magnetic quantities. Typically, the orientation of a given
magnetic spin, or the magnetic force acting on this spin.
:line
:link(Tranchida7)
[(Tranchida)] Tranchida, Plimpton, Thibaudeau and Thompson,
arXiv preprint arXiv:1801.10233, (2018).

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Calcalate temperature :h3
Temperature is computed as kinetic energy divided by some number of
degrees of freedom (and the Boltzmann constant). Since kinetic energy
is a function of particle velocity, there is often a need to
distinguish between a particle's advection velocity (due to some
aggregate motion of particles) and its thermal velocity. The sum of
the two is the particle's total velocity, but the latter is often what
is wanted to compute a temperature.
LAMMPS has several options for computing temperatures, any of which can be used in "thermostatting"_Howto_thermostat.html and "barostatting"_Howto_barostat.html. These "compute commands"_compute.html calculate temperature:
"compute temp"_compute_temp.html
"compute temp/sphere"_compute_temp_sphere.html
"compute temp/asphere"_compute_temp_asphere.html
"compute temp/com"_compute_temp_com.html
"compute temp/deform"_compute_temp_deform.html
"compute temp/partial"_compute_temp_partial.html
"compute temp/profile"_compute_temp_profile.html
"compute temp/ramp"_compute_temp_ramp.html
"compute temp/region"_compute_temp_region.html :ul
All but the first 3 calculate velocity biases directly (e.g. advection
velocities) that are removed when computing the thermal temperature.
"Compute temp/sphere"_compute_temp_sphere.html and "compute
temp/asphere"_compute_temp_asphere.html compute kinetic energy for
finite-size particles that includes rotational degrees of freedom.
They both allow for velocity biases indirectly, via an optional extra
argument which is another temperature compute that subtracts a velocity bias.
This allows the translational velocity of spherical or aspherical
particles to be adjusted in prescribed ways.

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"Higher level section"_Howto.html - "LAMMPS WWW Site"_lws - "LAMMPS
Documentation"_ld - "LAMMPS Commands"_lc :c
:link(lws,http://lammps.sandia.gov)
:link(ld,Manual.html)
:link(lc,Commands_all.html)
:line
Thermostats :h3
Thermostatting means controlling the temperature of particles in an MD
simulation. "Barostatting"_Howto_barostat.html means controlling the
pressure. Since the pressure includes a kinetic component due to
particle velocities, both these operations require calculation of the
temperature. Typically a target temperature (T) and/or pressure (P)
is specified by the user, and the thermostat or barostat attempts to
equilibrate the system to the requested T and/or P.
Thermostatting in LAMMPS is performed by "fixes"_fix.html, or in one
case by a pair style. Several thermostatting fixes are available:
Nose-Hoover (nvt), Berendsen, CSVR, Langevin, and direct rescaling
(temp/rescale). Dissipative particle dynamics (DPD) thermostatting
can be invoked via the {dpd/tstat} pair style:
"fix nvt"_fix_nh.html
"fix nvt/sphere"_fix_nvt_sphere.html
"fix nvt/asphere"_fix_nvt_asphere.html
"fix nvt/sllod"_fix_nvt_sllod.html
"fix temp/berendsen"_fix_temp_berendsen.html
"fix temp/csvr"_fix_temp_csvr.html
"fix langevin"_fix_langevin.html
"fix temp/rescale"_fix_temp_rescale.html
"pair_style dpd/tstat"_pair_dpd.html :ul
"Fix nvt"_fix_nh.html only thermostats the translational velocity of
particles. "Fix nvt/sllod"_fix_nvt_sllod.html also does this, except
that it subtracts out a velocity bias due to a deforming box and
integrates the SLLOD equations of motion. See the "Howto
nemd"_Howto_nemd.html doc page for further details. "Fix
nvt/sphere"_fix_nvt_sphere.html and "fix
nvt/asphere"_fix_nvt_asphere.html thermostat not only translation
velocities but also rotational velocities for spherical and aspherical
particles.
DPD thermostatting alters pairwise interactions in a manner analogous
to the per-particle thermostatting of "fix
langevin"_fix_langevin.html.
Any of the thermostatting fixes can use "temperature
computes"_Howto_thermostat.html that remove bias which has two
effects. First, the current calculated temperature, which is compared
to the requested target temperature, is calculated with the velocity
bias removed. Second, the thermostat adjusts only the thermal
temperature component of the particle's velocities, which are the
velocities with the bias removed. The removed bias is then added back
to the adjusted velocities. See the doc pages for the individual
fixes and for the "fix_modify"_fix_modify.html command for
instructions on how to assign a temperature compute to a
thermostatting fix. For example, you can apply a thermostat to only
the x and z components of velocity by using it in conjunction with
"compute temp/partial"_compute_temp_partial.html. Of you could
thermostat only the thermal temperature of a streaming flow of
particles without affecting the streaming velocity, by using "compute
temp/profile"_compute_temp_profile.html.
NOTE: Only the nvt fixes perform time integration, meaning they update
the velocities and positions of particles due to forces and velocities
respectively. The other thermostat fixes only adjust velocities; they
do NOT perform time integration updates. Thus they should be used in
conjunction with a constant NVE integration fix such as these:
"fix nve"_fix_nve.html
"fix nve/sphere"_fix_nve_sphere.html
"fix nve/asphere"_fix_nve_asphere.html :ul
Thermodynamic output, which can be setup via the
"thermo_style"_thermo_style.html command, often includes temperature
values. As explained on the doc page for the
"thermo_style"_thermo_style.html command, the default temperature is
setup by the thermo command itself. It is NOT the temperature
associated with any thermostatting fix you have defined or with any
compute you have defined that calculates a temperature. The doc pages
for the thermostatting fixes explain the ID of the temperature compute
they create. Thus if you want to view these temperatures, you need to
specify them explicitly via the "thermo_style
custom"_thermo_style.html command. Or you can use the
"thermo_modify"_thermo_modify.html command to re-define what
temperature compute is used for default thermodynamic output.

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