From b4ad6888a0a0fca2a2ab6b972270fa9876ad6d9e Mon Sep 17 00:00:00 2001
From: sjplimp
Date: Tue, 21 Jul 2015 23:11:53 +0000
Subject: [PATCH] git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@13663
f3b2605a-c512-4ea7-a41b-209d697bcdaa
---
doc/Section_commands.html | 7 ++---
doc/Section_commands.txt | 5 +++-
doc/Section_packages.html | 19 ++++++++++++++
doc/Section_packages.txt | 19 ++++++++++++++
doc/compute_saed.html | 25 ++++++++++--------
doc/compute_saed.txt | 22 +++++++++-------
doc/compute_xrd.html | 54 +++++++++++++++++++++------------------
doc/compute_xrd.txt | 51 +++++++++++++++++++-----------------
doc/fix_ave_histo.html | 18 ++++++-------
doc/fix_ave_histo.txt | 18 ++++++-------
doc/fix_saed_vtk.html | 14 +++++-----
doc/fix_saed_vtk.txt | 6 ++---
12 files changed, 159 insertions(+), 99 deletions(-)
diff --git a/doc/Section_commands.html b/doc/Section_commands.html
index 87bc66cad9..550da65be9 100644
--- a/doc/Section_commands.html
+++ b/doc/Section_commands.html
@@ -436,8 +436,8 @@ package.
imd | ipi | langevin/eff | lb/fluid | lb/momentum | lb/pc |
lb/rigid/pc/sphere | lb/viscous | meso | meso/stationary | nph/eff | npt/eff |
nve/eff | nvt/eff | nvt/sllod/eff | phonon | pimd | qeq/reax |
-qmmm | reax/c/bonds | reax/c/species | smd | temp/rescale/eff | ti/rs |
-ti/spring | ttm/mod
+ |
qmmm | reax/c/bonds | reax/c/species | saed/vtk | smd | temp/rescale/eff |
+ti/rs | ti/spring | ttm/mod
|
@@ -472,7 +472,8 @@ package.
diff --git a/doc/Section_commands.txt b/doc/Section_commands.txt
index 8d026e861a..b6bcd79dee 100644
--- a/doc/Section_commands.txt
+++ b/doc/Section_commands.txt
@@ -624,6 +624,7 @@ package"_Section_start.html#start_3.
"qmmm"_fix_qmmm.html,
"reax/c/bonds"_fix_reax_bonds.html,
"reax/c/species"_fix_reaxc_species.html,
+"saed/vtk"_fix_saed_vtk.html,
"smd"_fix_smd.html,
"temp/rescale/eff"_fix_temp_rescale_eff.html,
"ti/rs"_fix_ti_rs.html,
@@ -721,10 +722,12 @@ package"_Section_start.html#start_3.
"meso_e/atom"_compute_meso_e_atom.html,
"meso_rho/atom"_compute_meso_rho_atom.html,
"meso_t/atom"_compute_meso_t_atom.html,
+"saed"_compute_saed.html,
"temp/eff"_compute_temp_eff.html,
"temp/deform/eff"_compute_temp_deform_eff.html,
"temp/region/eff"_compute_temp_region_eff.html,
-"temp/rotate"_compute_temp_rotate.html :tb(c=6,ea=c)
+"temp/rotate"_compute_temp_rotate.html,
+"xrd"_compute_xrd.html :tb(c=6,ea=c)
:line
diff --git a/doc/Section_packages.html b/doc/Section_packages.html
index ed2125d604..9295269d8f 100644
--- a/doc/Section_packages.html
+++ b/doc/Section_packages.html
@@ -126,6 +126,7 @@ on how to build LAMMPS with both kinds of auxiliary libraries.
USER-CG-CMM | coarse-graining model | Axel Kohlmeyer (Temple U) | pair_style lj/sdk | USER/cg-cmm | cg | - |
USER-COLVARS | collective variables | Fiorin & Henin & Kohlmeyer (3) | fix colvars | USER/colvars | colvars | lib/colvars |
USER-CUDA | NVIDIA GPU styles | Christian Trott (U Tech Ilmenau) | Section accelerate | USER/cuda | - | lib/cuda |
+USER-DIFFRACTION | virutal x-ray and electron diffraction | Shawn Coleman (ARL) | compute xrd | USER/diffraction | - | - |
USER-EFF | electron force field | Andres Jaramillo-Botero (Caltech) | pair_style eff/cut | USER/eff | eff | - |
USER-FEP | free energy perturbation | Agilio Padua (U Blaise Pascal Clermont-Ferrand) | compute fep | USER/fep | - | - |
USER-INTEL | Vectorized CPU and Intel(R) coprocessor styles | W. Michael Brown (Intel) | Section accelerate | examples/intel | - | - |
@@ -336,6 +337,24 @@ tu-ilmenau.de). Contact him directly if you have questions.
+USER-DIFFRACTION package
+
+This package contains the commands neeed to calculate x-ray and
+electron diffraction intensities based on kinematic diffraction
+theory.
+
+See these doc pages and their related commands to get started:
+
+
+The person who created this package is Shawn P. Coleman
+(shawn.p.coleman8.ctr at mail.mil) while at the University of
+Arkansas. Contact him directly if you have questions.
+
+
+
USER-EFF package
This package contains a LAMMPS implementation of the electron Force
diff --git a/doc/Section_packages.txt b/doc/Section_packages.txt
index 697339b662..13182ac008 100644
--- a/doc/Section_packages.txt
+++ b/doc/Section_packages.txt
@@ -118,6 +118,7 @@ USER-AWPMD, wave-packet MD, Ilya Valuev (JIHT), "pair_style awpmd/cut"_pair_awpm
USER-CG-CMM, coarse-graining model, Axel Kohlmeyer (Temple U), "pair_style lj/sdk"_pair_sdk.html, USER/cg-cmm, "cg"_cg, -
USER-COLVARS, collective variables, Fiorin & Henin & Kohlmeyer (3), "fix colvars"_fix_colvars.html, USER/colvars, "colvars"_colvars, lib/colvars
USER-CUDA, NVIDIA GPU styles, Christian Trott (U Tech Ilmenau), "Section accelerate"_accelerate_cuda.html, USER/cuda, -, lib/cuda
+USER-DIFFRACTION, virutal x-ray and electron diffraction, Shawn Coleman (ARL),"compute xrd"_compute_xrd.html, USER/diffraction, -, -
USER-EFF, electron force field, Andres Jaramillo-Botero (Caltech), "pair_style eff/cut"_pair_eff.html, USER/eff, "eff"_eff, -
USER-FEP, free energy perturbation, Agilio Padua (U Blaise Pascal Clermont-Ferrand), "compute fep"_compute_fep.html, USER/fep, -, -
USER-INTEL, Vectorized CPU and Intel(R) coprocessor styles, W. Michael Brown (Intel), "Section accelerate"_accelerate_intel.html, examples/intel, -, -
@@ -323,6 +324,24 @@ tu-ilmenau.de). Contact him directly if you have questions.
:line
+USER-DIFFRACTION package :h4
+
+This package contains the commands neeed to calculate x-ray and
+electron diffraction intensities based on kinematic diffraction
+theory.
+
+See these doc pages and their related commands to get started:
+
+"compute xrd"_compute_xrd.html
+"compute saed"_compute_saed.html
+"fix saed/vtk"_fix_saed_vtk.html :ul
+
+The person who created this package is Shawn P. Coleman
+(shawn.p.coleman8.ctr at mail.mil) while at the University of
+Arkansas. Contact him directly if you have questions.
+
+:line
+
USER-EFF package :h4
This package contains a LAMMPS implementation of the electron Force
diff --git a/doc/compute_saed.html b/doc/compute_saed.html
index 178de056b4..c8f4ad0cec 100644
--- a/doc/compute_saed.html
+++ b/doc/compute_saed.html
@@ -21,8 +21,7 @@
lambda = wavelength of incident radiation (length units)
-type1 type2 ... typeN = chemical symbol of each atom type (see valid
-options below)
+type1 type2 ... typeN = chemical symbol of each atom type (see valid options below)
zero or more keyword/value pairs may be appended
@@ -46,9 +45,9 @@ options below)
Examples:
-compute 1 all saed 0.0251 Al O Kmax 1.70 Zone 0 0 1 dR_Ewald 0.01 c 0.5 0.5 0.5
-compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo
-
+compute 1 all saed 0.0251 Al O Kmax 1.70 Zone 0 0 1 dR_Ewald 0.01 c 0.5 0.5 0.5
+compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo
+
fix saed/vtk 1 1 1 c_1 file Al2O3_001.saed
fix saed/vtk 1 1 1 c_2 file Ni_000.saed
@@ -71,8 +70,11 @@ position of each atom, fj are atomic scattering factors.
Diffraction intensities are calculated on a three-dimensional mesh of
reciprocal lattice nodes. The mesh spacing is defined either (I) by
-the entire simulation domain or (II) manually using selected values.
+the entire simulation domain or (II) manually using selected values as
+shown in the 2D diagram below.
+
+
For a mesh defined by the simulation domain, a rectilinear grid is
constructed with spacing c*inv(A) along each reciprocal lattice
axis. Where A are the vectors corresponding to the edges of the
@@ -100,8 +102,11 @@ increase the cost of computation. Otherwise, Zone parameters will
denote the z1=h, z2=k, and z3=l (in a global since) zone axis of an
intersecting Ewald sphere. Diffraction intensities will only be
computed at the intersection of the reciprocal lattice mesh and a
-dR_Ewald thick surface of the Ewald sphere.
+dR_Ewald thick surface of the Ewald sphere. See the example 3D
+intestiety data and the intersection of a 010 zone axis in the below image.
+
+
The atomic scattering factors, fj, accounts for the reduction in
diffraction intensity due to Compton scattering. Compute saed uses
analytical approximations of the atomic scattering factors that vary
@@ -159,12 +164,12 @@ options.
Related commands:
-fix saed_vtk
-compute xrd
+
fix saed_vtk, compute xrd
Default:
-The option defaults are Kmax = 1.70, Zone 1 0 0, c 1 1 1, dR_Ewald = 0.01
+
The option defaults are Kmax = 1.70, Zone 1 0 0, c 1 1 1, dR_Ewald =
+0.01.
diff --git a/doc/compute_saed.txt b/doc/compute_saed.txt
index d2aaae2056..9bf628f6f2 100644
--- a/doc/compute_saed.txt
+++ b/doc/compute_saed.txt
@@ -15,8 +15,7 @@ compute ID group-ID saed lambda type1 type2 ... typeN keyword value ... :pre
ID, group-ID are documented in "compute"_compute.html command :ulb,l
saed = style name of this compute command :l
lambda = wavelength of incident radiation (length units) :l
-type1 type2 ... typeN = chemical symbol of each atom type (see valid
-options below) :l
+type1 type2 ... typeN = chemical symbol of each atom type (see valid options below) :l
zero or more keyword/value pairs may be appended :l
keyword = {Kmax} or {Zone} or {dR_Ewald} or {c} or {manual} or {echo} :l
@@ -38,7 +37,7 @@ keyword = {Kmax} or {Zone} or {dR_Ewald} or {c} or {manual} or {echo} :l
[Examples:]
compute 1 all saed 0.0251 Al O Kmax 1.70 Zone 0 0 1 dR_Ewald 0.01 c 0.5 0.5 0.5
-compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo
+compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo :pre
fix saed/vtk 1 1 1 c_1 file Al2O3_001.saed
fix saed/vtk 1 1 1 c_2 file Ni_000.saed :pre
@@ -61,7 +60,10 @@ position of each atom, fj are atomic scattering factors.
Diffraction intensities are calculated on a three-dimensional mesh of
reciprocal lattice nodes. The mesh spacing is defined either (I) by
-the entire simulation domain or (II) manually using selected values.
+the entire simulation domain or (II) manually using selected values as
+shown in the 2D diagram below.
+
+:c,image(JPG/saed_mesh_small.jpg,saed_mesh.jpg)
For a mesh defined by the simulation domain, a rectilinear grid is
constructed with spacing {c}*inv(A) along each reciprocal lattice
@@ -90,7 +92,10 @@ increase the cost of computation. Otherwise, {Zone} parameters will
denote the z1=h, z2=k, and z3=l (in a global since) zone axis of an
intersecting Ewald sphere. Diffraction intensities will only be
computed at the intersection of the reciprocal lattice mesh and a
-{dR_Ewald} thick surface of the Ewald sphere.
+{dR_Ewald} thick surface of the Ewald sphere. See the example 3D
+intestiety data and the intersection of a [010] zone axis in the below image.
+
+:c,image(JPG/saed_ewald_intersect_small.jpg,saed_ewald_intersect.jpg)
The atomic scattering factors, fj, accounts for the reduction in
diffraction intensity due to Compton scattering. Compute saed uses
@@ -150,12 +155,12 @@ The compute_saed command does not work for triclinic cells.
[Related commands:]
-"fix saed_vtk"_fix_saed_vtk.html
-"compute xrd"_compute_xrd.html
+"fix saed_vtk"_fix_saed_vtk.html, "compute xrd"_compute_xrd.html
[Default:]
-The option defaults are Kmax = 1.70, Zone 1 0 0, c 1 1 1, dR_Ewald = 0.01
+The option defaults are Kmax = 1.70, Zone 1 0 0, c 1 1 1, dR_Ewald =
+0.01.
:line
@@ -170,4 +175,3 @@ Volume C: Mathematical and Chemical Tables, 554-95 (2004).
:link(Fox)
[(Fox)] Fox, O'Keefe, Tabbernor, Acta Crystallogr. A, 45, 786-93
(1989).
-
diff --git a/doc/compute_xrd.html b/doc/compute_xrd.html
index bbcd1ddfab..253f936a21 100644
--- a/doc/compute_xrd.html
+++ b/doc/compute_xrd.html
@@ -21,8 +21,7 @@
lambda = wavelength of incident radiation (length units)
-type1 type2 ... typeN = chemical symbol of each atom type (see valid
-options below)
+type1 type2 ... typeN = chemical symbol of each atom type (see valid options below)
zero or more keyword/value pairs may be appended
@@ -44,12 +43,12 @@ options below)
Examples:
-compute 1 all xrd 1.541838 Al O 2Theta 0.087 0.87 c 1 1 1 LP 1 echo
+
compute 1 all xrd 1.541838 Al O 2Theta 0.087 0.87 c 1 1 1 LP 1 echo
compute 2 all xrd 1.541838 Al O 2Theta 10 100 c 0.05 0.05 0.05 LP 1 manual
-
-fix 1 all ave/histo 1 1 1 0.087 0.87 250 c_11 mode vector weights c_12 file Rad2Theta.xrd
-fix 2 all ave/histo 1 1 1 10 100 250 c_21 mode vector weights c_22 file Deg2Theta.xrd
-
+
+fix 1 all ave/histo 1 1 1 0.087 0.87 250 c_1[1] mode vector weights c_1[2] file Rad2Theta.xrd
+fix 2 all ave/histo 1 1 1 10 100 250 c_2[1] mode vector weights c_2[2] file Deg2Theta.xrd
+
Description:
@@ -78,8 +77,11 @@ the LP switch.
Diffraction intensities are calculated on a three-dimensional mesh of
reciprocal lattice nodes. The mesh spacing is defined either (I)
-by the entire simulation domain or (II) manually using selected values.
+by the entire simulation domain or (II) manually using selected values as
+shown in the 2D diagram below.
+
+
For a mesh defined by the simulation domain, a rectilinear grid is
constructed with spacing c*inv(A) along each reciprocal lattice
axis. Where A are the vectors corresponding to the edges of the
@@ -89,23 +91,24 @@ average of the (inversed) box lengths with periodic boundary conditions.
Meshes defined by the simulation domain must contain at least one periodic
boundary.
-If the manual flag is included, the mesh of reciprocal lattice nodes
-will defined using the c values for the spacing along each reciprocal
-lattice axis. Note that manual mapping of the reciprocal space mesh is
-good for comparing diffraction results from multiple simulations; however
-it can reduce the likelihood that Bragg reflections will be satisfied
-unless small spacing parameters <0.05 Angstrom^(-1) are implemented.
-Meshes with manual spacing do not require a periodic boundary.
+
If the manual flag is included, the mesh of reciprocal lattice nodes
+will defined using the c values for the spacing along each
+reciprocal lattice axis. Note that manual mapping of the reciprocal
+space mesh is good for comparing diffraction results from multiple
+simulations; however it can reduce the likelihood that Bragg
+reflections will be satisfied unless small spacing parameters (< 0.05
+Angstrom^(-1)) are implemented. Meshes with manual spacing do not
+require a periodic boundary.
-The limits of the reciprocal lattice mesh are determined by range of
-scattering angles explored. The 2Theta parameters allows the user to
-reduce the scattering angle range to only the region of interest which
-reduces the cost of the computation.
+
The limits of the reciprocal lattice mesh are determined by range of
+scattering angles explored. The 2Theta parameters allows the user
+to reduce the scattering angle range to only the region of interest
+which reduces the cost of the computation.
-The atomic scattering factors, fj, accounts for the reduction in
-diffraction intensity due to Compton scattering. Compute xrd uses
-analytical approximations of the atomic scattering factors that vary
-for each atom type (type1 type2 ... typeN) and angle of diffraction.
+
The atomic scattering factors, fj, accounts for the reduction in
+diffraction intensity due to Compton scattering. Compute xrd uses
+analytical approximations of the atomic scattering factors that vary
+for each atom type (type1 type2 ... typeN) and angle of diffraction.
The analytic approximation is computed using the formula
(Colliex):
@@ -183,12 +186,13 @@ options.
Related commands:
-fix ave/histo
+
fix ave/histo,
compute saed
Default:
-The option defaults are 2Theta = 1 179 (degrees), c = 1 1 1, LP = 1, no manual flag, no echo flag
+
The option defaults are 2Theta = 1 179 (degrees), c = 1 1 1, LP = 1,
+no manual flag, no echo flag.
diff --git a/doc/compute_xrd.txt b/doc/compute_xrd.txt
index 4e03ef5709..486fd22951 100644
--- a/doc/compute_xrd.txt
+++ b/doc/compute_xrd.txt
@@ -15,8 +15,7 @@ compute ID group-ID xrd lambda type1 type2 ... typeN keyword value ... :pre
ID, group-ID are documented in "compute"_compute.html command :ulb,l
xrd = style name of this compute command :l
lambda = wavelength of incident radiation (length units) :l
-type1 type2 ... typeN = chemical symbol of each atom type (see valid
-options below) :l
+type1 type2 ... typeN = chemical symbol of each atom type (see valid options below) :l
zero or more keyword/value pairs may be appended :l
keyword = {2Theta} or {c} or {LP} or {manual} or {echo} :l
@@ -36,10 +35,10 @@ keyword = {2Theta} or {c} or {LP} or {manual} or {echo} :l
[Examples:]
compute 1 all xrd 1.541838 Al O 2Theta 0.087 0.87 c 1 1 1 LP 1 echo
-compute 2 all xrd 1.541838 Al O 2Theta 10 100 c 0.05 0.05 0.05 LP 1 manual
+compute 2 all xrd 1.541838 Al O 2Theta 10 100 c 0.05 0.05 0.05 LP 1 manual :pre
-fix 1 all ave/histo 1 1 1 0.087 0.87 250 c_1[1] mode vector weights c_1[2] file Rad2Theta.xrd
-fix 2 all ave/histo 1 1 1 10 100 250 c_2[1] mode vector weights c_2[2] file Deg2Theta.xrd
+fix 1 all ave/histo 1 1 1 0.087 0.87 250 c_1\[1\] mode vector weights c_1\[2\] file Rad2Theta.xrd
+fix 2 all ave/histo 1 1 1 10 100 250 c_2\[1\] mode vector weights c_2\[2\] file Deg2Theta.xrd :pre
:pre
@@ -66,7 +65,11 @@ the {LP} switch.
Diffraction intensities are calculated on a three-dimensional mesh of
reciprocal lattice nodes. The mesh spacing is defined either (I)
-by the entire simulation domain or (II) manually using selected values.
+by the entire simulation domain or (II) manually using selected values as
+shown in the 2D diagram below.
+
+:c,image(JPG/xrd_mesh_small.jpg,xrd_mesh.jpg)
+
For a mesh defined by the simulation domain, a rectilinear grid is
constructed with spacing {c}*inv(A) along each reciprocal lattice
@@ -77,23 +80,24 @@ average of the (inversed) box lengths with periodic boundary conditions.
Meshes defined by the simulation domain must contain at least one periodic
boundary.
-If the {manual} flag is included, the mesh of reciprocal lattice nodes
-will defined using the {c} values for the spacing along each reciprocal
-lattice axis. Note that manual mapping of the reciprocal space mesh is
-good for comparing diffraction results from multiple simulations; however
-it can reduce the likelihood that Bragg reflections will be satisfied
-unless small spacing parameters [<0.05 Angstrom^(-1)] are implemented.
-Meshes with manual spacing do not require a periodic boundary.
+If the {manual} flag is included, the mesh of reciprocal lattice nodes
+will defined using the {c} values for the spacing along each
+reciprocal lattice axis. Note that manual mapping of the reciprocal
+space mesh is good for comparing diffraction results from multiple
+simulations; however it can reduce the likelihood that Bragg
+reflections will be satisfied unless small spacing parameters (< 0.05
+Angstrom^(-1)) are implemented. Meshes with manual spacing do not
+require a periodic boundary.
-The limits of the reciprocal lattice mesh are determined by range of
-scattering angles explored. The {2Theta} parameters allows the user to
-reduce the scattering angle range to only the region of interest which
-reduces the cost of the computation.
+The limits of the reciprocal lattice mesh are determined by range of
+scattering angles explored. The {2Theta} parameters allows the user
+to reduce the scattering angle range to only the region of interest
+which reduces the cost of the computation.
-The atomic scattering factors, fj, accounts for the reduction in
-diffraction intensity due to Compton scattering. Compute xrd uses
-analytical approximations of the atomic scattering factors that vary
-for each atom type (type1 type2 ... typeN) and angle of diffraction.
+The atomic scattering factors, fj, accounts for the reduction in
+diffraction intensity due to Compton scattering. Compute xrd uses
+analytical approximations of the atomic scattering factors that vary
+for each atom type (type1 type2 ... typeN) and angle of diffraction.
The analytic approximation is computed using the formula
"(Colliex)"_#Colliex:
@@ -172,12 +176,13 @@ The compute_xrd command does not work for triclinic cells.
[Related commands:]
-"fix ave/histo"_compute_ave_histo.html
+"fix ave/histo"_compute_ave_histo.html,
"compute saed"_compute_saed.html
[Default:]
-The option defaults are 2Theta = 1 179 (degrees), c = 1 1 1, LP = 1, no manual flag, no echo flag
+The option defaults are 2Theta = 1 179 (degrees), c = 1 1 1, LP = 1,
+no manual flag, no echo flag.
:line
diff --git a/doc/fix_ave_histo.html b/doc/fix_ave_histo.html
index 7533cc70a5..d941762f0b 100644
--- a/doc/fix_ave_histo.html
+++ b/doc/fix_ave_histo.html
@@ -66,7 +66,7 @@
string = text to print as 2nd line of output file
title3 arg = string
string = text to print as 3rd line of output file, only for vector mode
- weights arg = c_ID, c_ID[N], f_ID, f_ID[N], v_name
+ weights arg = x, y, z, vx, vy, vz, fx, fy, fz, c_ID, c_ID[N], f_ID, f_ID[N], v_name
c_ID = scalar or vector calculated by a compute with ID
c_ID[I] = Ith component of vector or Ith column of array calculated by a compute with ID
f_ID = scalar or vector calculated by a fix with ID
@@ -294,14 +294,14 @@ describes the six values that are printed at the first of each section
of output. The third describes the 4 values printed for each bin in
the histogram.
-If the weights keyword is specified, the fix will compute a weighted
-histogram using per-bin weights specified by the weights argument. As
-normal, the bin locations will be will be generated based off value1.
-However, instead of each binned value contributing 1 to the bin
-location, the contributing ammount is assigned the weights
-argument. Only a single value1 and weights argument pair can be can be
-used for each fix ave/histo. The length of value1 must match the
-lenght of the weights arguemnt.
+
If the weights keyword is specified, the fix will generate a weighted
+histogram using data from the assigned value1 and weights argument.
+As normal, the bin locations will be will be generated based off value1.
+However, instead of each binned value contributing 1 to the bin location,
+the contributing ammount is assigned the weights argument. Only a single
+value1 and weights argument pair can be can be used for each fix
+ave/histo. The length of value1 must match the lenght of the weights
+arguemnt.
diff --git a/doc/fix_ave_histo.txt b/doc/fix_ave_histo.txt
index a954c29325..d5d5c095a2 100644
--- a/doc/fix_ave_histo.txt
+++ b/doc/fix_ave_histo.txt
@@ -52,7 +52,7 @@ keyword = {mode} or {file} or {ave} or {start} or {beyond} or {overwrite} or {ti
string = text to print as 2nd line of output file
{title3} arg = string
string = text to print as 3rd line of output file, only for vector mode
- {weights} arg = c_ID, c_ID\[N\], f_ID, f_ID\[N\], v_name
+ {weights} arg = x, y, z, vx, vy, vz, fx, fy, fz, c_ID, c_ID\[N\], f_ID, f_ID\[N\], v_name
c_ID = scalar or vector calculated by a compute with ID
c_ID\[I\] = Ith component of vector or Ith column of array calculated by a compute with ID
f_ID = scalar or vector calculated by a fix with ID
@@ -279,14 +279,14 @@ describes the six values that are printed at the first of each section
of output. The third describes the 4 values printed for each bin in
the histogram.
-If the {weights} keyword is specified, the fix will compute a weighted
-histogram using per-bin weights specified by the {weights} argument. As
-normal, the bin locations will be will be generated based off value1.
-However, instead of each binned value contributing 1 to the bin
-location, the contributing ammount is assigned the weights
-argument. Only a single value1 and weights argument pair can be can be
-used for each fix ave/histo. The length of value1 must match the
-lenght of the weights arguemnt.
+If the {weights} keyword is specified, the fix will generate a weighted
+histogram using data from the assigned value1 and weights argument.
+As normal, the bin locations will be will be generated based off value1.
+However, instead of each binned value contributing 1 to the bin location,
+the contributing ammount is assigned the weights argument. Only a single
+value1 and weights argument pair can be can be used for each fix
+ave/histo. The length of value1 must match the lenght of the weights
+arguemnt.
:line
diff --git a/doc/fix_saed_vtk.html b/doc/fix_saed_vtk.html
index 55c15e8893..370ebe7856 100644
--- a/doc/fix_saed_vtk.html
+++ b/doc/fix_saed_vtk.html
@@ -42,9 +42,9 @@
Examples:
-compute 1 all saed 0.0251 Al O Kmax 1.70 Zone 0 0 1 dR_Ewald 0.01 c 0.5 0.5 0.5
-compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo
-
+compute 1 all saed 0.0251 Al O Kmax 1.70 Zone 0 0 1 dR_Ewald 0.01 c 0.5 0.5 0.5
+compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo
+
fix saed/vtk 1 1 1 c_1 file Al2O3_001.saed
fix saed/vtk 1 1 1 c_2 file Ni_000.saed
@@ -69,11 +69,11 @@ specified values may represent calculations performed by saed computes
which store their own "group" definitions.
Fix saed/vtk is designed to work only with compute_saed
-values.
-
-compute 3 top saed 0.0251 Al O
-fix saed/vtk 1 1 1 c_3 file Al2O3_001.saed
+values, e.g.
+compute 3 top saed 0.0251 Al O
+fix saed/vtk 1 1 1 c_3 file Al2O3_001.saed
+
The Nevery, Nrepeat, and Nfreq arguments specify on what
diff --git a/doc/fix_saed_vtk.txt b/doc/fix_saed_vtk.txt
index 67c940b192..1f048e9c3a 100644
--- a/doc/fix_saed_vtk.txt
+++ b/doc/fix_saed_vtk.txt
@@ -35,7 +35,7 @@ keyword = {file} or {ave} or {start} or {file} or {overwrite}:l
[Examples:]
compute 1 all saed 0.0251 Al O Kmax 1.70 Zone 0 0 1 dR_Ewald 0.01 c 0.5 0.5 0.5
-compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo
+compute 2 all saed 0.0251 Ni Kmax 1.70 Zone 0 0 0 c 0.05 0.05 0.05 manual echo :pre
fix saed/vtk 1 1 1 c_1 file Al2O3_001.saed
fix saed/vtk 1 1 1 c_2 file Ni_000.saed :pre
@@ -61,10 +61,10 @@ specified values may represent calculations performed by saed computes
which store their own "group" definitions.
Fix saed/vtk is designed to work only with "compute_saed"_compute_saed.txt
-values.
+values, e.g.
compute 3 top saed 0.0251 Al O
-fix saed/vtk 1 1 1 c_3 file Al2O3_001.saed
+fix saed/vtk 1 1 1 c_3 file Al2O3_001.saed :pre
:line