New package DPD-BASIC with pair styles dpd, dpd/tstat, dpd/ext, dpd/ext/tstat
This commit is contained in:
@ -138,15 +138,84 @@ install(TARGETS lmp EXPORT LAMMPS_Targets DESTINATION ${CMAKE_INSTALL_BINDIR})
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option(CMAKE_VERBOSE_MAKEFILE "Generate verbose Makefiles" OFF)
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set(STANDARD_PACKAGES ASPHERE BODY CLASS2 COLLOID COMPRESS DIPOLE
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GRANULAR KSPACE LATTE MANYBODY MC MESSAGE MISC ML-IAP MOLECULE PERI POEMS
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PLUGIN QEQ REPLICA RIGID SHOCK SPIN ML-SNAP SRD KIM PYTHON MSCG MPIIO VORONOI
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ADIOS ATC AWPMD BOCS CG-DNA DPD-MESO CG-SDK
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COLVARS DIELECTRIC DIFFRACTION DPD-REACT DRUDE EFF FEP
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H5MD ML-HDNNP LATBOLTZ MANIFOLD MDI MEAM MESONT MGPT
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USER-MISC MOFFF MOLFILE NETCDF PHONON PLUMED PTM QTB
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ML-RANN REACTION REAXFF SCAFACOS DPD-SMOOTH MACHDYN SMTBQ SPH
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TALLY UEF VTK ML-QUIP QMMM YAFF ML-PACE BROWNIAN)
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set(STANDARD_PACKAGES
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ADIOS
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ASPHERE
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ATC
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AWPMD
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BOCS
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BODY
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BROWNIAN
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CG-DNA
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CG-SDK
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CLASS2
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COLLOID
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COLVARS
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COMPRESS
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DIELECTRIC
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DIFFRACTION
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DIPOLE
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DPD-BASIC
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DPD-MESO
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DPD-REACT
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DPD-SMOOTH
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DRUDE
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EFF
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FEP
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GRANULAR
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H5MD
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KIM
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KSPACE
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LATBOLTZ
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LATTE
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MACHDYN
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MANIFOLD
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MANYBODY
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MC
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MDI
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MEAM
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MESONT
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MESSAGE
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MGPT
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MISC
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ML-HDNNP
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ML-IAP
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ML-PACE
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ML-QUIP
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ML-RANN
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ML-SNAP
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MOFFF
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MOLECULE
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MOLFILE
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MPIIO
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MSCG
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NETCDF
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PERI
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PHONON
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PLUGIN
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PLUMED
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POEMS
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PTM
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PYTHON
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QEQ
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QMMM
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QTB
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REACTION
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REAXFF
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REPLICA
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RIGID
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SCAFACOS
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SHOCK
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SMTBQ
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SPH
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SPIN
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SRD
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TALLY
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UEF
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USER-MISC
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VORONOI
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VTK
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YAFF)
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set(SUFFIX_PACKAGES CORESHELL GPU KOKKOS OPT INTEL OPENMP)
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@ -19,6 +19,7 @@ set(ALL_PACKAGES
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DIELECTRIC
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DIFFRACTION
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DIPOLE
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DPD-BASIC
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DPD-MESO
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DPD-REACT
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DPD-SMOOTH
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@ -21,6 +21,7 @@ set(ALL_PACKAGES
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DIELECTRIC
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DIFFRACTION
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DIPOLE
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DPD-BASIC
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DPD-MESO
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DPD-REACT
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DPD-SMOOTH
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@ -15,6 +15,7 @@ set(WIN_PACKAGES
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DIELECTRIC
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DIFFRACTION
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DIPOLE
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DPD-BASIC
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DPD-MESO
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DPD-REACT
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DPD-SMOOTH
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@ -17,6 +17,7 @@ set(ALL_PACKAGES
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DIELECTRIC
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DIFFRACTION
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DIPOLE
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DPD-BASIC
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DPD-MESO
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DPD-REACT
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DPD-SMOOTH
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@ -43,6 +43,7 @@ page gives those details.
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* :ref:`DIELECTRIC <PKG-DIELECTRIC>`
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* :ref:`DIFFRACTION <PKG-DIFFRACTION>`
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* :ref:`DIPOLE <PKG-DIPOLE>`
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* :ref:`DPD-BASIC <PKG-DPD-BASIC>`
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* :ref:`DPD-MESO <PKG-DPD-MESO>`
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* :ref:`DPD-REACT <PKG-DPD-REACT>`
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* :ref:`DPD-SMOOTH <PKG-DPD-SMOOTH>`
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@ -560,6 +561,29 @@ short-range or long-range interactions.
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----------
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.. _PKG-DPD-BASIC:
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DPD-BASIC package
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--------------------
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**Contents:**
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Pair styles for the basic dissipative particle dynamics (DPD) method
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and DPD thermostatting.
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**Author:** Kurt Smith (U Pittsburgh), Martin Svoboda, Martin Lisal (ICPF and UJEP)
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**Supporting info:**
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* src/DPD-BASIC: filenames -> commands
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* :doc:`pair_style dpd <pair_dpd>`
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* :doc:`pair_style dpd/tstat <pair_dpd>`
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* :doc:`pair_style dpd/ext <pair_dpd_ext>`
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* :doc:`pair_style dpd/ext/tstat <pair_dpd_ext>`
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* examples/PACKAGES/dpd-basic
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----------
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.. _PKG-DPD-MESO:
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DPD-MESO package
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@ -113,6 +113,11 @@ whether an extra library is needed to build and use the package:
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- :doc:`pair_style lj/.../dipole <pair_dipole>`
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- dipole
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- no
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* - :ref:`DPD-BASIC <PKG-DPD-BASIC>`
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- basic DPD models
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- :doc:`pair_styles dpd dpd/tstat <pair_dpd>` :doc:`dpd/ext dpd/ext/tstat <pair_dpd_ext>`
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- PACKAGES/dpd-basic
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- no
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* - :ref:`DPD-MESO <PKG-DPD-MESO>`
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- mesoscale DPD models
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- :doc:`pair_style edpd <pair_mesodpd>`
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@ -154,14 +154,14 @@ These pair styles do not support the :doc:`pair_modify <pair_modify>`
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tail option for adding long-range tail corrections to energy and
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pressure.
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These pair styles writes their information to :doc:`binary restart files <restart>`, so pair_style and pair_coeff commands do not need
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to be specified in an input script that reads a restart file. Note
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that the user-specified random number seed is stored in the restart
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file, so when a simulation is restarted, each processor will
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re-initialize its random number generator the same way it did
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initially. This means the random forces will be random, but will not
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be the same as they would have been if the original simulation had
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continued past the restart time.
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These pair styles write their information to :doc:`binary restart files
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<restart>`, so pair_style and pair_coeff commands do not need to be
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specified in an input script that reads a restart file. Note that the
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user-specified random number seed is stored in the restart file, so when
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a simulation is restarted, each processor will re-initialize its random
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number generator the same way it did initially. This means the random
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forces will be random, but will not be the same as they would have been
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if the original simulation had continued past the restart time.
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These pair styles can only be used via the *pair* keyword of the
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:doc:`run_style respa <run_style>` command. They do not support the
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@ -177,22 +177,26 @@ this.
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Restrictions
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""""""""""""
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These styles are part of the DPD-BASIC package. They are only enabled if
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LAMMPS was built with that package. See the :doc:`Build package
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<Build_package>` doc page for more info.
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The default frequency for rebuilding neighbor lists is every 10 steps
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(see the :doc:`neigh_modify <neigh_modify>` command). This may be too
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infrequent for style *dpd* simulations since particles move rapidly
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and can overlap by large amounts. If this setting yields a non-zero
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number of "dangerous" reneighborings (printed at the end of a
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simulation), you should experiment with forcing reneighboring more
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often and see if system energies/trajectories change.
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infrequent for style *dpd* simulations since particles move rapidly and
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can overlap by large amounts. If this setting yields a non-zero number
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of "dangerous" reneighborings (printed at the end of a simulation), you
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should experiment with forcing reneighboring more often and see if
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system energies/trajectories change.
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These pair styles requires you to use the :doc:`comm_modify vel yes <comm_modify>` command so that velocities are stored by ghost
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atoms.
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These pair styles requires you to use the :doc:`comm_modify vel yes
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<comm_modify>` command so that velocities are stored by ghost atoms.
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These pair styles will not restart exactly when using the
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:doc:`read_restart <read_restart>` command, though they should provide
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statistically similar results. This is because the forces they
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compute depend on atom velocities. See the
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:doc:`read_restart <read_restart>` command for more details.
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statistically similar results. This is because the forces they compute
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depend on atom velocities. See the :doc:`read_restart <read_restart>`
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command for more details.
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Related commands
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""""""""""""""""
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@ -38,12 +38,19 @@ Examples
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Description
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"""""""""""
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The style *dpd/ext* computes an extended force field for dissipative particle dynamics (DPD) following the exposition in :ref:`(Groot) <Groot>`, :ref:`(Junghans) <Junghans>`.
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The style *dpd/ext* computes an extended force field for dissipative
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particle dynamics (DPD) following the exposition in :ref:`(Groot)
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<Groot>`, :ref:`(Junghans) <Junghans>`.
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Style *dpd/ext/tstat* invokes an extended DPD thermostat on pairwise interactions, equivalent to the non-conservative portion of the extended DPD force field. To use *dpd/ext/tstat* as a thermostat for another pair style, use the :doc:`pair_style hybrid/overlay <pair_hybrid>` command to compute both the desired pair interaction and the thermostat for each pair of particles.
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Style *dpd/ext/tstat* invokes an extended DPD thermostat on pairwise
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interactions, equivalent to the non-conservative portion of the extended
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DPD force field. To use *dpd/ext/tstat* as a thermostat for another pair
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style, use the :doc:`pair_style hybrid/overlay <pair_hybrid>` command to
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compute both the desired pair interaction and the thermostat for each
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pair of particles.
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For the style *dpd/ext*\ , the force on atom I due to atom J is given as a sum
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of 3 terms
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For the style *dpd/ext*\ , the force on atom I due to atom J is given as
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a sum of 3 terms
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.. math::
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@ -53,17 +60,51 @@ of 3 terms
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f^R = & \sigma_{\parallel} w_{\parallel}(r) \frac{\alpha}{\sqrt{\Delta t}} \hat{\mathbf{r}}_{ij} + \sigma_{\perp} w_{\perp} (r) ( \mathbf{I} - \hat{\mathbf{r}}_{ij} \hat{\mathbf{r}}_{ij}^{\rm T} ) \frac{\mathbf{\xi}_{ij}}{\sqrt{\Delta t}}\\
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w(r) = & 1 - r/r_c \\
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where :math:`\mathbf{f}^C` is a conservative force, :math:`\mathbf{f}^D` is a dissipative force, and :math:`\mathbf{f}^R` is a random force. :math:`A_{ij}` is the maximum repulsion between the two atoms, :math:`\hat{\mathbf{r}}_{ij}` is a unit vector in the direction :math:`\mathbf{r}_i - \mathbf{r}_j`, :math:`\mathbf{v}_{ij} = \mathbf{v}_i - \mathbf{v}_j` is the vector difference in velocities of the two atoms, :math:`\alpha` and :math:`\mathbf{\xi}_{ij}` are Gaussian random numbers with zero mean and unit variance, :math:`\Delta t` is the timestep, :math:`w (r) = 1 - r / r_c` is a weight function for the conservative interactions that varies between 0 and 1, :math:`r_c` is the corresponding cutoff, :math:`w_{\alpha} ( r ) = ( 1 - r / \bar{r}_c )^{s_{\alpha}}`, :math:`\alpha \equiv ( \parallel, \perp )`, are weight functions with coefficients :math:`s_\alpha` that vary between 0 and 1, :math:`\bar{r}_c` is the corresponding cutoff, :math:`\mathbf{I}` is the unit matrix, :math:`\sigma_{\alpha} = \sqrt{2 k T \gamma_{\alpha}}`, where :math:`k` is the Boltzmann constant and :math:`T` is the temperature in the pair\_style command.
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where :math:`\mathbf{f}^C` is a conservative force, :math:`\mathbf{f}^D`
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is a dissipative force, and :math:`\mathbf{f}^R` is a random
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force. :math:`A_{ij}` is the maximum repulsion between the two atoms,
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:math:`\hat{\mathbf{r}}_{ij}` is a unit vector in the direction
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:math:`\mathbf{r}_i - \mathbf{r}_j`, :math:`\mathbf{v}_{ij} =
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\mathbf{v}_i - \mathbf{v}_j` is the vector difference in velocities of
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the two atoms, :math:`\alpha` and :math:`\mathbf{\xi}_{ij}` are Gaussian
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random numbers with zero mean and unit variance, :math:`\Delta t` is the
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timestep, :math:`w (r) = 1 - r / r_c` is a weight function for the
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conservative interactions that varies between 0 and 1, :math:`r_c` is
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the corresponding cutoff, :math:`w_{\alpha} ( r ) = ( 1 - r / \bar{r}_c
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)^{s_{\alpha}}`, :math:`\alpha \equiv ( \parallel, \perp )`, are weight
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functions with coefficients :math:`s_\alpha` that vary between 0 and 1,
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:math:`\bar{r}_c` is the corresponding cutoff, :math:`\mathbf{I}` is the
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unit matrix, :math:`\sigma_{\alpha} = \sqrt{2 k T \gamma_{\alpha}}`,
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where :math:`k` is the Boltzmann constant and :math:`T` is the
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temperature in the pair\_style command.
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For the style *dpd/ext/tstat*\ , the force on atom I due to atom J is the same as the above equation, except that the conservative :math:`\mathbf{f}^C` term is dropped. Also, during the run, T is set each timestep to a ramped value from Tstart to Tstop.
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For the style *dpd/ext/tstat*\ , the force on atom I due to atom J is
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the same as the above equation, except that the conservative
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:math:`\mathbf{f}^C` term is dropped. Also, during the run, T is set
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each timestep to a ramped value from Tstart to Tstop.
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For the style *dpd/ext*\ , the pairwise energy associated with style *dpd/ext* is only due to the conservative force term :math:`\mathbf{f}^C`, and is shifted to be zero at the cutoff distance :math:`r_c`. The pairwise virial is calculated using all three terms. There is no pairwise energy for style *dpd/ext/tstat*, but the last two terms of the formula contribute the virial.
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For the style *dpd/ext*\ , the pairwise energy associated with style
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*dpd/ext* is only due to the conservative force term
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:math:`\mathbf{f}^C`, and is shifted to be zero at the cutoff distance
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:math:`r_c`. The pairwise virial is calculated using all three
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terms. There is no pairwise energy for style *dpd/ext/tstat*, but the
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last two terms of the formula contribute the virial.
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For the style *dpd/ext/tstat*, the force on atom I due to atom J is the same as the above equation, except that the conservative :math:`\mathbf{f}^C` term is dropped. Also, during the run, T is set each timestep to a ramped value from Tstart to Tstop.
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For the style *dpd/ext/tstat*, the force on atom I due to atom J is the
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same as the above equation, except that the conservative
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:math:`\mathbf{f}^C` term is dropped. Also, during the run, T is set
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each timestep to a ramped value from Tstart to Tstop.
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For the style *dpd/ext*\ , the pairwise energy associated with style *dpd/ext* is only due to the conservative force term :math:`\mathbf{f}^C`, and is shifted to be zero at the cutoff distance :math:`r_c`. The pairwise virial is calculated using all three terms. There is no pairwise energy for style *dpd/ext/tstat*, but the last two terms of the formula contribute the virial.
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For the style *dpd/ext*\ , the pairwise energy associated with style
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*dpd/ext* is only due to the conservative force term
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:math:`\mathbf{f}^C`, and is shifted to be zero at the cutoff distance
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:math:`r_c`. The pairwise virial is calculated using all three
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terms. There is no pairwise energy for style *dpd/ext/tstat*, but the
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last two terms of the formula contribute the virial.
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For the style *dpd/ext*, the following coefficients must be defined for each pair of atoms types via the :doc:`pair_coeff <pair_coeff>` command as in the examples above:
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For the style *dpd/ext*, the following coefficients must be defined for
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each pair of atoms types via the :doc:`pair_coeff <pair_coeff>` command
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as in the examples above:
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* A (force units)
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* :math:`\gamma_{\perp}` (force/velocity units)
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@ -72,35 +113,55 @@ For the style *dpd/ext*, the following coefficients must be defined for each pai
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* :math:`s_{\parallel}` (unitless)
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* :math:`r_c` (distance units)
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The last coefficient is optional. If not specified, the global DPD cutoff is used. Note that :math:`\sigma`'s are set equal to :math:`\sqrt{2 k T \gamma}`, where :math:`T` is the temperature set by the :doc:`pair_style <pair_style>` command so it does not need to be specified.
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The last coefficient is optional. If not specified, the global DPD
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cutoff is used. Note that :math:`\sigma`'s are set equal to
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:math:`\sqrt{2 k T \gamma}`, where :math:`T` is the temperature set by
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the :doc:`pair_style <pair_style>` command so it does not need to be
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specified.
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For the style *dpd/ext/tstat*, the coefficients defined for each pair of atoms types via the :doc:`pair_coeff <pair_coeff>` command is the same, except that A is not included.
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For the style *dpd/ext/tstat*, the coefficients defined for each pair of
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atoms types via the :doc:`pair_coeff <pair_coeff>` command is the same,
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except that A is not included.
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.. note::
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If you are modeling DPD polymer chains, you may want to use the :doc:`pair_style srp <pair_srp>` command in conjunction with these pair styles. It is a soft segmental repulsive potential (SRP) that can prevent DPD polymer chains from crossing each other.
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If you are modeling DPD polymer chains, you may want to use the
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:doc:`pair_style srp <pair_srp>` command in conjunction with these pair
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styles. It is a soft segmental repulsive potential (SRP) that can
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prevent DPD polymer chains from crossing each other.
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.. note::
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The virial calculation for pressure when using this pair style includes all the components of force listed above, including the random force.
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The virial calculation for pressure when using this pair style includes
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all the components of force listed above, including the random force.
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----------
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**Mixing, shift, table, tail correction, restart, rRESPA info**\ :
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The style *dpd/ext* does not support mixing. Thus, coefficients for all I,J pairs must be specified explicitly.
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The style *dpd/ext* does not support mixing. Thus, coefficients for all
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I,J pairs must be specified explicitly.
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The pair styles do not support the :doc:`pair_modify <pair_modify>` shift option for the energy of the pair interaction. Note that as discussed above, the energy due to the conservative :math:`\mathbf{f}^C` term is already shifted to be zero at the cutoff distance :math:`r_c`.
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The pair styles do not support the :doc:`pair_modify <pair_modify>`
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shift option for the energy of the pair interaction. Note that as
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discussed above, the energy due to the conservative :math:`\mathbf{f}^C`
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term is already shifted to be zero at the cutoff distance :math:`r_c`.
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The :doc:`pair_modify <pair_modify>` table option is not relevant for the style *dpd/ext*.
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The :doc:`pair_modify <pair_modify>` table option is not relevant for
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the style *dpd/ext*.
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The style *dpd/ext* does not support the :doc:`pair_modify <pair_modify>` tail option for adding long-range tail corrections to energy and pressure.
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||||
The style *dpd/ext* does not support the :doc:`pair_modify
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||||
<pair_modify>` tail option for adding long-range tail corrections to
|
||||
energy and pressure.
|
||||
|
||||
The pair styles can only be used via the pair keyword of the :doc:`run_style respa <run_style>` command. They do not support the *inner*\ , *middle*\ , and *outer*\ keywords.
|
||||
The pair styles can only be used via the pair keyword of the
|
||||
:doc:`run_style respa <run_style>` command. They do not support the
|
||||
*inner*\ , *middle*\ , and *outer*\ keywords.
|
||||
|
||||
The style *dpd/ext/tstat* can ramp its target temperature over multiple runs, using the start and stop keywords of the :doc:`run <run>` command. See the :doc:`run <run>` command for details of how to do this.
|
||||
The style *dpd/ext/tstat* can ramp its target temperature over multiple
|
||||
runs, using the start and stop keywords of the :doc:`run <run>`
|
||||
command. See the :doc:`run <run>` command for details of how to do this.
|
||||
|
||||
----------
|
||||
|
||||
@ -108,31 +169,42 @@ The style *dpd/ext/tstat* can ramp its target temperature over multiple runs, us
|
||||
Restrictions
|
||||
""""""""""""
|
||||
|
||||
The default frequency for rebuilding neighbor lists is every 10 steps (see the :doc:`neigh_modify <neigh_modify>` command). This may be too infrequent for style *dpd/ext* simulations since particles move rapidly and can overlap by large amounts. If this setting yields a non-zero number of \say{dangerous} reneighborings (printed at the end of a simulation), you should experiment with forcing reneighboring more often and see if system energies/trajectories change.
|
||||
These styles are part of the DPD-BASIC package. They are only enabled if
|
||||
LAMMPS was built with that package. See the :doc:`Build package
|
||||
<Build_package>` doc page for more info.
|
||||
|
||||
The pair styles require to use the :doc:`comm_modify vel yes <comm_modify>` command so that velocities are stored by ghost atoms.
|
||||
The default frequency for rebuilding neighbor lists is every 10 steps
|
||||
(see the :doc:`neigh_modify <neigh_modify>` command). This may be too
|
||||
infrequent for style *dpd/ext* simulations since particles move rapidly
|
||||
and can overlap by large amounts. If this setting yields a non-zero
|
||||
number of \say{dangerous} reneighborings (printed at the end of a
|
||||
simulation), you should experiment with forcing reneighboring more often
|
||||
and see if system energies/trajectories change.
|
||||
|
||||
The pair styles will not restart exactly when using the :doc:`read_restart <read_restart>` command, though they should provide statistically similar results. This is because the forces they compute depend on atom velocities. See the :doc:`read_restart <read_restart>` command for more details.
|
||||
The pair styles require to use the :doc:`comm_modify vel yes
|
||||
<comm_modify>` command so that velocities are stored by ghost atoms.
|
||||
|
||||
The pair styles will not restart exactly when using the
|
||||
:doc:`read_restart <read_restart>` command, though they should provide
|
||||
statistically similar results. This is because the forces they compute
|
||||
depend on atom velocities. See the :doc:`read_restart <read_restart>`
|
||||
command for more details.
|
||||
|
||||
Related commands
|
||||
""""""""""""""""
|
||||
|
||||
:doc:`pair_style dpd <pair_dpd>`, :doc:`pair_coeff <pair_coeff>`, :doc:`fix nvt <fix_nh>`, :doc:`fix langevin <fix_langevin>`, :doc:`pair_style srp <pair_srp>`
|
||||
:doc:`pair_style dpd <pair_dpd>`, :doc:`pair_coeff <pair_coeff>`,
|
||||
:doc:`fix nvt <fix_nh>`, :doc:`fix langevin <fix_langevin>`,
|
||||
:doc:`pair_style srp <pair_srp>`
|
||||
|
||||
**Default:** none
|
||||
|
||||
|
||||
----------
|
||||
|
||||
|
||||
.. _Groot:
|
||||
|
||||
|
||||
|
||||
**(Groot)** Groot and Warren, J Chem Phys, 107, 4423-35 (1997).
|
||||
|
||||
.. _Junghans:
|
||||
|
||||
|
||||
|
||||
**(Junghans)** Junghans, Praprotnik and Kremer, Soft Matter 4, 156, 1119-1128 (2008).
|
||||
|
||||
4
src/.gitignore
vendored
4
src/.gitignore
vendored
@ -1429,6 +1429,10 @@
|
||||
/pair_thole.h
|
||||
/pair_buck_mdf.cpp
|
||||
/pair_buck_mdf.h
|
||||
/pair_dpd.cpp
|
||||
/pair_dpd.h
|
||||
/pair_dpd_tstat.cpp
|
||||
/pair_dpd_tstat.h
|
||||
/pair_dpd_ext.cpp
|
||||
/pair_dpd_ext.h
|
||||
/pair_dpd_ext_tstat.cpp
|
||||
|
||||
@ -63,6 +63,7 @@ PACKAGE = \
|
||||
coreshell \
|
||||
diffraction \
|
||||
dipole \
|
||||
dpd-basic \
|
||||
dpd-meso \
|
||||
dpd-react \
|
||||
dpd-smooth \
|
||||
@ -148,6 +149,7 @@ PACKMOST = \
|
||||
coreshell \
|
||||
diffraction \
|
||||
dipole \
|
||||
dpd-basic \
|
||||
dpd-meso \
|
||||
dpd-react \
|
||||
dpd-smooth \
|
||||
|
||||
@ -51,6 +51,11 @@ lmpinstalledpkgs.h
|
||||
lmpgitversion.h
|
||||
mliap_model_python_couple.cpp
|
||||
mliap_model_python_couple.h
|
||||
# moved to DPD-BASIC package on 1 July 2021
|
||||
pair_dpd.cpp
|
||||
pair_dpd.h
|
||||
pair_dpd_tstat.cpp
|
||||
pair_dpd_tstat.h
|
||||
# removed on 14 May 2021
|
||||
nstencil_half_bin_2d_newton_ssa.cpp
|
||||
nstencil_half_bin_2d_newton_ssa.h
|
||||
|
||||
@ -89,8 +89,6 @@ pair_style coul/slater/long, Evangelos Voyiatzis, evoyiatzis at gmail.com, 26 Fe
|
||||
pair_style dipole/sf, Mario Orsi, orsimario at gmail.com, 8 Aug 11
|
||||
pair_style e3b, Steven Strong (U Chicago), stevene.strong at gmail dot com, 16 Apr 19
|
||||
pair_style drip, Mingjian Wen, University of Minnesota, wenxx151 at umn.edu, 17 Apr 19
|
||||
pair_style dpd/ext, Martin Svoboda, Karel Sindelka, Martin Lisal, ICPF and UJEP, svobod.martin at gmail dot com, 23 Apr 21
|
||||
pair_style dpd/ext/tstat, Martin Svoboda, Karel Sindelka, Martin Lisal, ICPF and UJEP , svobod.martin at gmail dot com, 23 Apr 21
|
||||
pair_style edip, Luca Ferraro, luca.ferraro at caspur.it, 15 Sep 11
|
||||
pair_style extep, Jaap Kroes (Radboud U), jaapkroes at gmail dot com, 28 Nov 17
|
||||
pair_style gauss/cut, Axel Kohlmeyer, akohlmey at gmail.com, 1 Dec 11
|
||||
|
||||
Reference in New Issue
Block a user