git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@1619 f3b2605a-c512-4ea7-a41b-209d697bcdaa

doc/Section_commands.html

@@ -335,8 +335,8 @@ description:
 <DIV ALIGN=center><TABLE  BORDER=1 >
 <TR ALIGN="center"><TD ><A HREF = "compute_centro_atom.html">centro/atom</A></TD><TD ><A HREF = "compute_coord_atom.html">coord/atom</A></TD><TD ><A HREF = "compute_displace_atom.html">displace/atom</A></TD><TD ><A HREF = "compute_erotate_sphere.html">erotate/sphere</A></TD><TD ><A HREF = "compute_group_group.html">group/group</A></TD><TD ><A HREF = "compute_ke_atom.html">ke/atom</A></TD></TR>
 <TR ALIGN="center"><TD ><A HREF = "compute_pe.html">pe</A></TD><TD ><A HREF = "compute_pe_atom.html">pe/atom</A></TD><TD ><A HREF = "compute_pressure.html">pressure</A></TD><TD ><A HREF = "compute_reduce.html">reduce</A></TD><TD ><A HREF = "compute_stress_atom.html">stress/atom</A></TD><TD ><A HREF = "compute_temp.html">temp</A></TD></TR>
-<TR ALIGN="center"><TD ><A HREF = "compute_temp_asphere.html">temp/asphere</A></TD><TD ><A HREF = "compute_temp_com.html">temp/com</A></TD><TD ><A HREF = "compute_temp_deform.html">temp/deform</A></TD><TD ><A HREF = "compute_temp_dipole.html">temp/dipole</A></TD><TD ><A HREF = "compute_temp_partial.html">temp/partial</A></TD><TD ><A HREF = "compute_temp_ramp.html">temp/ramp</A></TD></TR>
+<TR ALIGN="center"><TD ><A HREF = "compute_temp_asphere.html">temp/asphere</A></TD><TD ><A HREF = "compute_temp_com.html">temp/com</A></TD><TD ><A HREF = "compute_temp_deform.html">temp/deform</A></TD><TD ><A HREF = "compute_temp_partial.html">temp/partial</A></TD><TD ><A HREF = "compute_temp_ramp.html">temp/ramp</A></TD><TD ><A HREF = "compute_temp_region.html">temp/region</A></TD></TR>
-<TR ALIGN="center"><TD ><A HREF = "compute_temp_region.html">temp/region</A></TD><TD ><A HREF = "compute_temp_sphere.html">temp/sphere</A> 
+<TR ALIGN="center"><TD ><A HREF = "compute_temp_sphere.html">temp/sphere</A> 
 </TD></TR></TABLE></DIV>
 
 <P>These are compute styles contributed by users, which can be used if

doc/compute_erotate_sphere.html

@@ -9,34 +9,43 @@
 
 <HR>
 
-<H3>compute rotate/dipole command 
+<H3>compute erotate/sphere command 
 </H3>
 <P><B>Syntax:</B>
 </P>
-<PRE>compute ID group-ID rotate/dipole 
+<PRE>compute ID group-ID erotate/sphere 
 </PRE>
 <UL><LI>ID, group-ID are documented in <A HREF = "compute.html">compute</A> command
-<LI>rotate/dipole = style name of this compute command 
+<LI>erotate/sphere = style name of this compute command 
 </UL>
 <P><B>Examples:</B>
 </P>
-<PRE>compute 1 all rotate/dipole 
+<PRE>compute 1 all erotate/sphere 
 </PRE>
 <P><B>Description:</B>
 </P>
-<P>Define a computation that calculates the total rotational energy of a
+<P>Define a computation that calculates the rotational kinetic energy of
-group of atoms with point dipole moments.
+a group of spherical particles.
 </P>
-<P>The rotational energy is calculated as the sum of 1/2 I w^2 over all
+<P>The rotational energy is computed as 1/2 I w^2, where I is the moment
-the atoms in the group, where I is the moment of inertia of a
+of inertia for a sphere and w is the particle's angular velocity.
-disk/spherical (2d/3d) particle, and w is its angular velocity.
+</P>
+<P>IMPORTANT NOTE: For <A HREF = "dimension.html">2d models</A>, particles are treated
+as spheres, not disks, meaning their moment of inertia will be the
+same as in 3d.
 </P>
 <P><B>Output info:</B>
 </P>
 <P>The scalar value calculated by this compute is "extensive", meaning it
 it scales with the number of atoms in the simulation.
 </P>
-<P><B>Restrictions:</B> none
+<P><B>Restrictions:</B>
+</P>
+<P>This compute requires that particles be represented as extended
+spheres and not point particles.  This means they will have an angular
+velocity and a diameter which is determined either by the
+<A HREF = "shape.html">shape</A> command or by each particle being assigned an
+individual radius, e.g. for <A HREF = "atom_style.html">atom_style granular</A>.
 </P>
 <P><B>Related commands:</B> none
 </P>

doc/compute_erotate_sphere.txt

@@ -6,34 +6,43 @@
 
 :line
 
-compute rotate/dipole command :h3
+compute erotate/sphere command :h3
 
 [Syntax:]
 
-compute ID group-ID rotate/dipole :pre
+compute ID group-ID erotate/sphere :pre
 
 ID, group-ID are documented in "compute"_compute.html command
-rotate/dipole = style name of this compute command :ul
+erotate/sphere = style name of this compute command :ul
 
 [Examples:]
 
-compute 1 all rotate/dipole :pre
+compute 1 all erotate/sphere :pre
 
 [Description:]
 
-Define a computation that calculates the total rotational energy of a
+Define a computation that calculates the rotational kinetic energy of
-group of atoms with point dipole moments.
+a group of spherical particles.
 
-The rotational energy is calculated as the sum of 1/2 I w^2 over all
+The rotational energy is computed as 1/2 I w^2, where I is the moment
-the atoms in the group, where I is the moment of inertia of a
+of inertia for a sphere and w is the particle's angular velocity.
-disk/spherical (2d/3d) particle, and w is its angular velocity.
+
+IMPORTANT NOTE: For "2d models"_dimension.html, particles are treated
+as spheres, not disks, meaning their moment of inertia will be the
+same as in 3d.
 
 [Output info:]
 
 The scalar value calculated by this compute is "extensive", meaning it
 it scales with the number of atoms in the simulation.
 
-[Restrictions:] none
+[Restrictions:]
+
+This compute requires that particles be represented as extended
+spheres and not point particles.  This means they will have an angular
+velocity and a diameter which is determined either by the
+"shape"_shape.html command or by each particle being assigned an
+individual radius, e.g. for "atom_style granular"_atom_style.html.
 
 [Related commands:] none
 

doc/compute_temp_asphere.html

@@ -53,7 +53,7 @@ particles, so they do not rotate.
 inertia tensor for the aspherical particle and w is its angular
 velocity, which is computed from its angular momentum.
 </P>
-<P>IMPORTANT NOTE: Fo <A HREF = "dimension.html">2d models</A>, particles are treated
+<P>IMPORTANT NOTE: For <A HREF = "dimension.html">2d models</A>, particles are treated
 as ellipsoids, not ellipses, meaning their moments of inertia will be
 the same as in 3d.
 </P>

doc/compute_temp_asphere.txt

@@ -50,7 +50,7 @@ The rotational kinetic energy is computed as 1/2 I w^2, where I is the
 inertia tensor for the aspherical particle and w is its angular
 velocity, which is computed from its angular momentum.
 
-IMPORTANT NOTE: Fo "2d models"_dimension.html, particles are treated
+IMPORTANT NOTE: For "2d models"_dimension.html, particles are treated
 as ellipsoids, not ellipses, meaning their moments of inertia will be
 the same as in 3d.
 

doc/compute_temp_sphere.html

@@ -39,7 +39,7 @@ degrees of freedom (2 translational, 1 rotational).
 moment of inertia for a sphere and w is the particle's angular
 velocity.
 </P>
-<P>IMPORTANT NOTE: Fo <A HREF = "dimension.html">2d models</A>, particles are treated
+<P>IMPORTANT NOTE: For <A HREF = "dimension.html">2d models</A>, particles are treated
 as spheres, not disks, meaning their moment of inertia will be the
 same as in 3d.
 </P>

doc/compute_temp_sphere.txt

@@ -36,7 +36,7 @@ The rotational kinetic energy is computed as 1/2 I w^2, where I is the
 moment of inertia for a sphere and w is the particle's angular
 velocity.
 
-IMPORTANT NOTE: Fo "2d models"_dimension.html, particles are treated
+IMPORTANT NOTE: For "2d models"_dimension.html, particles are treated
 as spheres, not disks, meaning their moment of inertia will be the
 same as in 3d.