From 055b20301e77fc2c25e05c43e149ad32f5d05e70 Mon Sep 17 00:00:00 2001
From: sjplimp <sjplimp@f3b2605a-c512-4ea7-a41b-209d697bcdaa>
Date: Mon, 9 May 2016 16:56:43 +0000
Subject: [PATCH] git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@14948
 f3b2605a-c512-4ea7-a41b-209d697bcdaa

---
 doc/compute_angle.rst    |  60 --------------
 doc/compute_dihedral.rst |  59 --------------
 doc/compute_improper.rst |  59 --------------
 doc/fix_shardlow.rst     | 115 ---------------------------
 doc/fix_smd.rst          | 168 ---------------------------------------
 5 files changed, 461 deletions(-)
 delete mode 100644 doc/compute_angle.rst
 delete mode 100644 doc/compute_dihedral.rst
 delete mode 100644 doc/compute_improper.rst
 delete mode 100644 doc/fix_shardlow.rst
 delete mode 100644 doc/fix_smd.rst

diff --git a/doc/compute_angle.rst b/doc/compute_angle.rst
deleted file mode 100644
index 91df79f906..0000000000
--- a/doc/compute_angle.rst
+++ /dev/null
@@ -1,60 +0,0 @@
-.. index:: compute angle
-
-compute angle command
-=====================
-
-Syntax
-""""""
-
-.. parsed-literal::
-
-   compute ID group-ID angle
-
-* ID, group-ID are documented in :doc:`compute <compute>` command
-* angle = style name of this compute command
-
-Examples
-""""""""
-
-.. parsed-literal::
-
-   compute 1 all angle
-
-Description
-"""""""""""
-
-Define a computation that extracts the angle energy calculated by each
-of the angle sub-styles used in the  "angle_style
-hybrid" angle_hybrid.html command.  These values are made accessible
-for output or further processing by other commands.  The group
-specified for this command is ignored.
-
-This compute is useful when using :doc:`angle_style hybrid <angle_hybrid>` if you want to know the portion of the total
-energy contributed by one or more of the hybrid sub-styles.
-
-**Output info:**
-
-This compute calculates a global vector of length N where N is the
-number of sub_styles defined by the :doc:`angle_style hybrid <angle_style>` command, which can be accessed by indices
-1-N.  These values can be used by any command that uses global scalar
-or vector values from a compute as input.  See :ref:`this section <howto_15>` for an overview of LAMMPS output
-options.
-
-The vector values are "extensive" and will be in energy
-:doc:`units <units>`.
-
-Restrictions
-""""""""""""
- none
-
-Related commands
-""""""""""""""""
-
-:doc:`compute pe <compute_pe>`, :doc:`compute pair <compute_pair>`
-
-**Default:** none
-
-
-.. _lws: http://lammps.sandia.gov
-.. _ld: Manual.html
-.. _lc: Section_commands.html#comm
diff --git a/doc/compute_dihedral.rst b/doc/compute_dihedral.rst
deleted file mode 100644
index 8c0281e409..0000000000
--- a/doc/compute_dihedral.rst
+++ /dev/null
@@ -1,59 +0,0 @@
-.. index:: compute dihedral
-
-compute dihedral command
-========================
-
-Syntax
-""""""
-
-.. parsed-literal::
-
-   compute ID group-ID dihedral
-
-* ID, group-ID are documented in :doc:`compute <compute>` command
-* dihedral = style name of this compute command
-
-Examples
-""""""""
-
-.. parsed-literal::
-
-   compute 1 all dihedral
-
-Description
-"""""""""""
-
-Define a computation that extracts the dihedral energy calculated by
-each of the dihedral sub-styles used in the :doc:`dihedral_style hybrid <dihedral_hybrid>` command.  These values are made
-accessible for output or further processing by other commands.  The
-group specified for this command is ignored.
-
-This compute is useful when using :doc:`dihedral_style hybrid <dihedral_hybrid>` if you want to know the portion of the
-total energy contributed by one or more of the hybrid sub-styles.
-
-**Output info:**
-
-This compute calculates a global vector of length N where N is the
-number of sub_styles defined by the :doc:`dihedral_style hybrid <dihedral_style>` command.  which can be accessed by indices
-1-N.  These values can be used by any command that uses global scalar
-or vector values from a compute as input.  See :ref:`this section <howto_15>` for an overview of LAMMPS output
-options.
-
-The vector values are "extensive" and will be in energy
-:doc:`units <units>`.
-
-Restrictions
-""""""""""""
- none
-
-Related commands
-""""""""""""""""
-
-:doc:`compute pe <compute_pe>`, :doc:`compute pair <compute_pair>`
-
-**Default:** none
-
-
-.. _lws: http://lammps.sandia.gov
-.. _ld: Manual.html
-.. _lc: Section_commands.html#comm
diff --git a/doc/compute_improper.rst b/doc/compute_improper.rst
deleted file mode 100644
index ade78d6cb7..0000000000
--- a/doc/compute_improper.rst
+++ /dev/null
@@ -1,59 +0,0 @@
-.. index:: compute improper
-
-compute improper command
-========================
-
-Syntax
-""""""
-
-.. parsed-literal::
-
-   compute ID group-ID improper
-
-* ID, group-ID are documented in :doc:`compute <compute>` command
-* improper = style name of this compute command
-
-Examples
-""""""""
-
-.. parsed-literal::
-
-   compute 1 all improper
-
-Description
-"""""""""""
-
-Define a computation that extracts the improper energy calculated by
-each of the improper sub-styles used in the :doc:`improper_style hybrid <improper_hybrid>` command.  These values are made
-accessible for output or further processing by other commands.  The
-group specified for this command is ignored.
-
-This compute is useful when using :doc:`improper_style hybrid <improper_hybrid>` if you want to know the portion of the
-total energy contributed by one or more of the hybrid sub-styles.
-
-**Output info:**
-
-This compute calculates a global vector of length N where N is the
-number of sub_styles defined by the :doc:`improper_style hybrid <improper_style>` command.  which can be accessed by indices
-1-N.  These values can be used by any command that uses global scalar
-or vector values from a compute as input.  See :ref:`this section <howto_15>` for an overview of LAMMPS output
-options.
-
-The vector values are "extensive" and will be in energy
-:doc:`units <units>`.
-
-Restrictions
-""""""""""""
- none
-
-Related commands
-""""""""""""""""
-
-:doc:`compute pe <compute_pe>`, :doc:`compute pair <compute_pair>`
-
-**Default:** none
-
-
-.. _lws: http://lammps.sandia.gov
-.. _ld: Manual.html
-.. _lc: Section_commands.html#comm
diff --git a/doc/fix_shardlow.rst b/doc/fix_shardlow.rst
deleted file mode 100644
index 560aaf5fa4..0000000000
--- a/doc/fix_shardlow.rst
+++ /dev/null
@@ -1,115 +0,0 @@
-.. index:: fix shardlow
-
-fix shardlow command
-====================
-
-Syntax
-""""""
-
-.. parsed-literal::
-
-   fix ID group-ID shardlow
-
-* ID, group-ID are documented in :doc:`fix <fix>` command
-* shardlow = style name of this fix command
-
-Examples
-""""""""
-
-.. parsed-literal::
-
-   fix 1 all shardlow
-
-Description
-"""""""""""
-
-Specifies that the Shardlow splitting algorithm (SSA) is to be used to
-integrate the DPD equations of motion.  The SSA splits the integration
-into a stochastic and deterministic integration step.  The fix
-*shardlow* performs the stochastic integration step and must be used
-in conjunction with a deterministic integrator (e.g. :doc:`fix nve <fix_nve>` or :doc:`fix nph <fix_nph>`).  The stochastic
-integration of the dissipative and random forces is performed prior to
-the deterministic integration of the conservative force. Further
-details regarding the method are provided in :ref:`(Lisal) <Lisal>` and
-:ref:`(Larentzos) <Larentzos>`.
-
-The fix *shardlow* must be used with the :doc:`pair_style dpd/fdt <pair_style>` or :doc:`pair_style dpd/fdt/energy <pair_style>` command to properly initialize the
-fluctuation-dissipation theorem parameter(s) sigma (and kappa, if
-necessary).
-
-Note that numerous variants of DPD can be specified by choosing an
-appropriate combination of the integrator and :doc:`pair_style dpd/fdt <pair_style>` command.  DPD under isothermal conditions can
-be specified by using fix *shardlow*, fix *nve* and pair_style
-*dpd/fdt*.  DPD under isoenergetic conditions can be specified by
-using fix *shardlow*, fix *nve* and pair_style *dpd/fdt/energy*.  DPD
-under isobaric conditions can be specified by using fix shardlow, fix
-*nph* and pair_style *dpd/fdt*.  DPD under isoenthalpic conditions can
-be specified by using fix shardlow, fix *nph* and pair_style
-*dpd/fdt/energy*.  Examples of each DPD variant are provided in the
-examples/USER/dpd directory.
-
-
-----------
-
-
-Restrictions
-""""""""""""
-
-
-This fix is only available if LAMMPS is built with the USER-DPD
-package.  See the :ref:`Making LAMMPS <start_3>` section
-for more info.
-
-This fix is currently limited to orthogonal simulation cell
-geometries.
-
-This fix must be used with an additional fix that specifies time
-integration, e.g. :doc:`fix nve <fix_nve>` or :doc:`fix nph <fix_nh>`.
-
-The Shardlow splitting algorithm requires the sizes of the sub-domain
-lengths to be larger than twice the cutoff+skin.  Generally, the
-domain decomposition is dependant on the number of processors
-requested.
-
-Related commands
-""""""""""""""""
-
-:doc:`pair_style dpd/fdt <pair_dpd_fdt>`, :doc:`fix eos/cv <fix_eos_cv>`
-
-**Default:** none
-
-
-----------
-
-
-.. _Lisal:
-
-
-
-**(Lisal)** M. Lisal, J.K. Brennan, J. Bonet Avalos, "Dissipative
-particle dynamics as isothermal, isobaric, isoenergetic, and
-isoenthalpic conditions using Shardlow-like splitting algorithms.",
-J. Chem. Phys., 135, 204105 (2011).
-
-.. _Larentzos:
-
-
-
-**(Larentzos)** J.P. Larentzos, J.K. Brennan, J.D. Moore, M. Lisal and
-W.D. Mattson, "Parallel Implementation of Isothermal and Isoenergetic
-Dissipative Particle Dynamics Using Shardlow-Like Splitting
-Algorithms", Comput. Phys. Commun., 185, 1987-1998 (2014).
-
-.. _Larentzos:
-
-
-
-**(Larentzos)** J.P. Larentzos, J.K. Brennan, J.D. Moore, and
-W.D. Mattson, "LAMMPS Implementation of Constant Energy Dissipative
-Particle Dynamics (DPD-E)", ARL-TR-6863, U.S. Army Research
-Laboratory, Aberdeen Proving Ground, MD (2014).
-
-
-.. _lws: http://lammps.sandia.gov
-.. _ld: Manual.html
-.. _lc: Section_commands.html#comm
diff --git a/doc/fix_smd.rst b/doc/fix_smd.rst
deleted file mode 100644
index 62d215a648..0000000000
--- a/doc/fix_smd.rst
+++ /dev/null
@@ -1,168 +0,0 @@
-.. index:: fix smd
-
-fix smd command
-===============
-
-Syntax
-""""""
-
-.. parsed-literal::
-
-   fix ID group-ID smd type values keyword values
-
-* ID, group-ID are documented in :doc:`fix <fix>` command
-* smd  = style name of this fix command
-* mode = *cvel* or *cfor* to select constant velocity or constant force SMD
-.. parsed-literal::
-
-     *cvel* values = K vel
-       K = spring constant (force/distance units)
-       vel = velocity of pulling (distance/time units) 
-     *cfor* values = force
-       force = pulling force (force units)
-
-* keyword = *tether* or *couple*
-.. parsed-literal::
-
-     *tether* values = x y z R0
-       x,y,z = point to which spring is tethered
-       R0 = distance of end of spring from tether point (distance units)
-     *couple* values = group-ID2 x y z R0
-       group-ID2 = 2nd group to couple to fix group with a spring
-       x,y,z = direction of spring, automatically computed with 'auto'
-       R0 = distance of end of spring (distance units)
-
-
-
-Examples
-""""""""
-
-.. parsed-literal::
-
-   fix  pull    cterm smd cvel 20.0 -0.00005 tether NULL NULL 100.0 0.0
-   fix  pull    cterm smd cvel 20.0 -0.0001 tether 25.0 25 25.0 0.0
-   fix  stretch cterm smd cvel 20.0  0.0001 couple nterm auto auto auto 0.0
-   fix  pull    cterm smd cfor  5.0 tether 25.0 25.0 25.0 0.0
-
-Description
-"""""""""""
-
-This fix implements several options of steered MD (SMD) as reviewed in
-:ref:`(Izrailev) <Izrailev>`, which allows to induce conformational changes
-in systems and to compute the potential of mean force (PMF) along the
-assumed reaction coordinate :ref:`(Park) <Park>` based on Jarzynski's
-equality :ref:`(Jarzynski) <Jarzynski>`.  This fix borrows a lot from :doc:`fix spring <fix_spring>` and :doc:`fix setforce <fix_setforce>`.
-
-You can apply a moving spring force to a group of atoms (*tether*
-style) or between two groups of atoms (*couple* style).  The spring
-can then be used in either constant velocity (*cvel*) mode or in
-constant force (*cfor*) mode to induce transitions in your systems.
-When running in *tether* style, you may need some way to fix some
-other part of the system (e.g. via :doc:`fix spring/self <fix_spring_self>`)
-
-The *tether* style attaches a spring between a point at a distance of
-R0 away from a fixed point *x,y,z* and the center of mass of the fix
-group of atoms.  A restoring force of magnitude K (R - R0) Mi / M is
-applied to each atom in the group where *K* is the spring constant, Mi
-is the mass of the atom, and M is the total mass of all atoms in the
-group.  Note that *K* thus represents the total force on the group of
-atoms, not a per-atom force.
-
-In *cvel* mode the distance R is incremented or decremented
-monotonously according to the pulling (or pushing) velocity.
-In *cfor* mode a constant force is added and the actual distance
-in direction of the spring is recorded.
-
-The *couple* style links two groups of atoms together.  The first
-group is the fix group; the second is specified by group-ID2.  The
-groups are coupled together by a spring that is at equilibrium when
-the two groups are displaced by a vector in direction *x,y,z* with
-respect to each other and at a distance R0 from that displacement.
-Note that *x,y,z* only provides a direction and will be internally
-normalized. But since it represents the *absolute* displacement of
-group-ID2 relative to the fix group, (1,1,0) is a different spring
-than (-1,-1,0).  For each vector component, the displacement can be
-described with the *auto* parameter. In this case the direction is
-recomputed in every step, which can be useful for steering a local
-process where the whole object undergoes some other change.  When the
-relative positions and distance between the two groups are not in
-equilibrium, the same spring force described above is applied to atoms
-in each of the two groups.
-
-For both the *tether* and *couple* styles, any of the x,y,z values can
-be specified as NULL which means do not include that dimension in the
-distance calculation or force application.
-
-For constant velocity pulling (*cvel* mode), the running integral 
-over the pulling force in direction of the spring is recorded and
-can then later be used to compute the potential of mean force (PMF) 
-by averaging over multiple independent trajectories along the same
-pulling path.
-
-Restart, fix_modify, output, run start/stop, minimize info
-""""""""""""""""""""""""""""""""""""""""""""""""""""""""""
-
-The fix stores the direction of the spring, current pulling target
-distance and the running PMF to :doc:`binary restart files <restart>`.
-See the :doc:`read_restart <read_restart>` command for info on how to
-re-specify a fix in an input script that reads a restart file, so that
-the operation of the fix continues in an uninterrupted fashion.
-
-None of the :doc:`fix_modify <fix_modify>` options are relevant to this
-fix.
-
-This fix computes a vector list of 7 quantities, which can be accessed
-by various :ref:`output commands <howto_15>`.  The
-quantities in the vector are in this order: the x-, y-, and
-z-component of the pulling force, the total force in direction of the
-pull, the equilibrium distance of the spring, the distance between the
-two reference points, and finally the accumulated PMF (the sum of
-pulling forces times displacement).
-
-The force is the total force on the group of atoms by the spring.  In
-the case of the *couple* style, it is the force on the fix group
-(group-ID) or the negative of the force on the 2nd group (group-ID2).
-The vector values calculated by this fix are "extensive".
-
-No parameter of this fix can be used with the *start/stop* keywords of
-the :doc:`run <run>` command.  This fix is not invoked during :doc:`energy minimization <minimize>`.
-
-Restrictions
-""""""""""""
-
-
-This fix is part of the USER-MISC package.  It is only enabled if
-LAMMPS was built with that package.  See the :ref:`Making LAMMPS <start_3>` section for more info.
-
-Related commands
-""""""""""""""""
-
-:doc:`fix drag <fix_drag>`, :doc:`fix spring <fix_spring>`, 
-:doc:`fix spring/self <fix_spring_self>`, 
-:doc:`fix spring/rg <fix_spring_rg>`
-
-**Default:** none
-
-
-----------
-
-
-.. _Israilev:
-
-
-
-**(Izrailev)** Izrailev, Stepaniants, Isralewitz, Kosztin, Lu, Molnar,
-Wriggers, Schulten. Computational Molecular Dynamics: Challenges,
-Methods, Ideas, volume 4 of Lecture Notes in Computational Science and
-Engineering, pp. 39-65. Springer-Verlag, Berlin, 1998.
-
-**(Park)**
-Park, Schulten, J. Chem. Phys. 120 (13), 5946 (2004)
-
-**(Jarzynski)**
-Jarzynski, Phys. Rev. Lett. 78, 2690 (1997)
-
-
-.. _lws: http://lammps.sandia.gov
-.. _ld: Manual.html
-.. _lc: Section_commands.html#comm
-- 
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