diff --git a/doc/Section_errors.html b/doc/Section_errors.html
index a27f2b6065..0f73e09ff8 100644
--- a/doc/Section_errors.html
+++ b/doc/Section_errors.html
@@ -73,7 +73,7 @@ of the following cases:
 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.
+prwhich 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
diff --git a/doc/Section_history.html b/doc/Section_history.html
index 881d419cd3..996c175d62 100644
--- a/doc/Section_history.html
+++ b/doc/Section_history.html
@@ -35,8 +35,7 @@ time or interest; others are just a lot of work!
 <LI>torsional shear boundary conditions and temperature calculation
 <LI>bond creation potentials
 <LI>point dipole force fields
-<LI>many-body and bond-order potentials for materials like C, Si, or silica
-<LI>modified EAM (MEAM) potentials for metals
+<LI>REBO bond-order potential
 <LI>ReaxFF force field from Bill Goddard's group
 <LI>Parinello-Rahman non-rectilinear simulation box 
 </UL>
diff --git a/doc/Section_history.txt b/doc/Section_history.txt
index 5ddf6b7cd3..2979a6cd01 100644
--- a/doc/Section_history.txt
+++ b/doc/Section_history.txt
@@ -32,8 +32,7 @@ Monte Carlo bond-swapping for polymers (was in Fortran LAMMPS)
 torsional shear boundary conditions and temperature calculation
 bond creation potentials
 point dipole force fields
-many-body and bond-order potentials for materials like C, Si, or silica
-modified EAM (MEAM) potentials for metals
+REBO bond-order potential
 ReaxFF force field from Bill Goddard's group
 Parinello-Rahman non-rectilinear simulation box :ul
 
diff --git a/doc/Section_intro.html b/doc/Section_intro.html
index 81e6b50fbc..bbfd83cd43 100644
--- a/doc/Section_intro.html
+++ b/doc/Section_intro.html
@@ -28,8 +28,8 @@ the years.
 </H4>
 <P>LAMMPS is a classical molecular dynamics code that models an ensemble
 of particles in a liquid, solid, or gaseous state.  It can model
-atomic, polymeric, biological, metallic, or granular systems using a
-variety of force fields and boundary conditions.
+atomic, polymeric, biological, metallic, granular, and coarse-grained
+systems using a variety of force fields and boundary conditions.
 </P>
 <P>For examples of LAMMPS simulations, see the Publications page of the
 <A HREF = "http://lammps.sandia.gov">LAMMPS WWW Site</A>.
@@ -108,6 +108,7 @@ LAMMPS.
 <LI>  all-atom polymers, organic molecules, proteins, DNA
 <LI>  metals
 <LI>  granular materials
+<LI>  coarse-grained mesoscale models
 <LI>  hybrid systems 
 </UL>
 <H4>Force fields: 
@@ -117,8 +118,8 @@ LAMMPS.
 <A HREF = "improper_style.html">improper style</A>, <A HREF = "kspace_style.html">kspace style</A>
 commands)
 </P>
-<UL><LI>  pairwise potentials: Lennard-Jones, Coulombic, Buckingham, Morse,     Yukawa, embedded atom method (EAM, Finnis/Sinclair), frictional granular,
-<LI>    Debye, soft, DPD, class 2 (COMPASS), tabulated, hybrid
+<UL><LI>  pairwise potentials: Lennard-Jones, Coulombic, Buckingham, Morse,     Yukawa, frictional granular, Debye, soft, DPD, class 2 (COMPASS),     tabulated, hybrid
+<LI>  manybody potentials: EAM, Finnis/Sinclair, modified EAM (MEAM),     Stillinger-Weber, Tersoff
 <LI>  bond potentials: harmonic, FENE, Morse, nonlinear, class 2,     quartic (breakable), hybrid
 <LI>  angle potentials: harmonic, CHARMM, cosine, cosine/squared,     class 2 (COMPASS), hybrid
 <LI>  dihedral potentials: harmonic, CHARMM, multi-harmonic, helix,     class 2 (COMPASS), OPLS, hybrid	 
@@ -479,7 +480,16 @@ features in LAMMPS:
 <TR><TD >DCD and XTC dump styles</TD><TD > Naveen Michaud-Agrawal (Johns Hopkins U)</TD></TR>
 <TR><TD >breakable bond quartic potential</TD><TD > Chris Lorenz and Mark Stevens (SNL)</TD></TR>
 <TR><TD >faster pair hybrid potential</TD><TD > James Fischer   (High Performance Technologies, Inc), Vincent Natoli and   David Richie (Stone Ridge Technology)</TD></TR>
-<TR><TD >POEMS coupled rigid body integrator</TD><TD > Rudranarayan Mukherjee (RPI) 
+<TR><TD >POEMS coupled rigid body integrator</TD><TD > Rudranarayan Mukherjee (RPI)</TD></TR>
+<TR><TD >OPLS dihedral potential</TD><TD > Mark Stevens (Sandia)</TD></TR>
+<TR><TD >multi-letter variable names </TD><TD > Naveen Michaud-Agrawal (Johns Hopkins U)</TD></TR>
+<TR><TD >fix momentum and recenter </TD><TD > Naveen Michaud-Agrawal (Johns Hopkins U)</TD></TR>
+<TR><TD >LJ tail corrections for energy/pressure </TD><TD > Paul Crozier (Sandia)</TD></TR>
+<TR><TD >region prism </TD><TD > Pieter in't Veld (Sandia)</TD></TR>
+<TR><TD >Stillinger-Weber and Tersoff potentials </TD><TD > Aidan Thompson (Sandia)</TD></TR>
+<TR><TD >fix wall/lj126 </TD><TD > Mark Stevens (Sandia)</TD></TR>
+<TR><TD >optimized pair potentials for lj/cut, charmm/long, eam, morse </TD><TD > James Fischer (High Performance Tech), David Richie and Vincent Natol (Stone Ridge Technologies)</TD></TR>
+<TR><TD >MEAM potential </TD><TD > Greg Wagner (Sandia) 
 </TD></TR></TABLE></DIV>
 
 <P>Other CRADA partners involved in the design and testing of LAMMPS were
diff --git a/doc/Section_intro.txt b/doc/Section_intro.txt
index b7831926a9..8d988d6927 100644
--- a/doc/Section_intro.txt
+++ b/doc/Section_intro.txt
@@ -25,8 +25,8 @@ the years.
 
 LAMMPS is a classical molecular dynamics code that models an ensemble
 of particles in a liquid, solid, or gaseous state.  It can model
-atomic, polymeric, biological, metallic, or granular systems using a
-variety of force fields and boundary conditions.
+atomic, polymeric, biological, metallic, granular, and coarse-grained
+systems using a variety of force fields and boundary conditions.
 
 For examples of LAMMPS simulations, see the Publications page of the
 "LAMMPS WWW Site"_lws.
@@ -104,6 +104,7 @@ Kinds of systems LAMMPS can simulate: :h4
   all-atom polymers, organic molecules, proteins, DNA
   metals
   granular materials
+  coarse-grained mesoscale models
   hybrid systems :ul
 
 Force fields: :h4
@@ -113,8 +114,10 @@ Force fields: :h4
 commands)
 
   pairwise potentials: Lennard-Jones, Coulombic, Buckingham, Morse, \
-    Yukawa, embedded atom method (EAM, Finnis/Sinclair), frictional granular,
-    Debye, soft, DPD, class 2 (COMPASS), tabulated, hybrid
+    Yukawa, frictional granular, Debye, soft, DPD, class 2 (COMPASS), \
+    tabulated, hybrid
+  manybody potentials: EAM, Finnis/Sinclair, modified EAM (MEAM), \
+    Stillinger-Weber, Tersoff
   bond potentials: harmonic, FENE, Morse, nonlinear, class 2, \
     quartic (breakable), hybrid
   angle potentials: harmonic, CHARMM, cosine, cosine/squared, \
@@ -467,7 +470,16 @@ breakable bond quartic potential: Chris Lorenz and Mark Stevens (SNL)
 faster pair hybrid potential: James Fischer \
   (High Performance Technologies, Inc), Vincent Natoli and \
   David Richie (Stone Ridge Technology)
-POEMS coupled rigid body integrator: Rudranarayan Mukherjee (RPI) :tb(s=:)
+POEMS coupled rigid body integrator: Rudranarayan Mukherjee (RPI)
+OPLS dihedral potential: Mark Stevens (Sandia)
+multi-letter variable names : Naveen Michaud-Agrawal (Johns Hopkins U)
+fix momentum and recenter : Naveen Michaud-Agrawal (Johns Hopkins U)
+LJ tail corrections for energy/pressure : Paul Crozier (Sandia)
+region prism : Pieter in't Veld (Sandia)
+Stillinger-Weber and Tersoff potentials : Aidan Thompson (Sandia)
+fix wall/lj126 : Mark Stevens (Sandia)
+optimized pair potentials for lj/cut, charmm/long, eam, morse : James Fischer (High Performance Tech), David Richie and Vincent Natol (Stone Ridge Technologies)
+MEAM potential : Greg Wagner (Sandia) :tb(s=:)
 
 Other CRADA partners involved in the design and testing of LAMMPS were