Commit 6e8a68a4 authored by Axel Kohlmeyer's avatar Axel Kohlmeyer
Browse files

fix a bunch of typos and broken links as detected by ebook-convert

parent 11f04fde
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@@ -119,7 +119,7 @@ the core/shell pair, which is an imaginary degree of freedom, from the
real physical system.  To do that, the "compute
temp/cs"_compute_temp_cs.html command can be used, in conjunction with
any of the thermostat fixes, such as "fix nvt"_fix_nh.html or "fix
langevin"_fix_langevin.  This compute uses the center-of-mass velocity
langevin"_fix_langevin.html.  This compute uses the center-of-mass velocity
of the core/shell pairs to calculate a temperature, and insures that
velocity is what is rescaled for thermostatting purposes.  This
compute also works for a system with both core/shell pairs and
@@ -150,9 +150,9 @@ The pressure for the core/shell system is computed via the regular
LAMMPS convention by "treating the cores and shells as individual
particles"_#MitchellFincham2. For the thermo output of the pressure
as well as for the application of a barostat, it is necessary to
use an additional "pressure"_compute_pressure compute based on the
default "temperature"_compute_temp and specifying it as a second
argument in "fix modify"_fix_modify.html and
use an additional "pressure"_compute_pressure.html compute based on
the default "temperature"_compute_temp.html and specifying it as a
second argument in "fix modify"_fix_modify.html and
"thermo_modify"_thermo_modify.html resulting in:

(...)
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@@ -53,5 +53,5 @@ computations between frozen atoms by using this command:
NOTE: By default, for 2d systems, granular particles are still modeled
as 3d spheres, not 2d discs (circles), meaning their moment of inertia
will be the same as in 3d.  If you wish to model granular particles in
2d as 2d discs, see the note on this topic on the "Howto 2d"_Howto_2d
2d as 2d discs, see the note on this topic on the "Howto 2d"_Howto_2d.html
doc page, where 2d simulations are discussed.
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@@ -265,7 +265,7 @@ supports.

[Running on GPUs:]

Use the "-k" "command-line switch"_Run_options.thml to
Use the "-k" "command-line switch"_Run_options.html to
specify the number of GPUs per node. Typically the -np setting of the
mpirun command should set the number of MPI tasks/node to be equal to
the number of physical GPUs on the node.  You can assign multiple MPI
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@@ -76,7 +76,7 @@ command for the types of the two atoms is used. For the {radius}
setting, the sum of the radii of the two particles is used as a
cutoff.  For example, this is appropriate for granular particles which
only interact when they are overlapping, as computed by "granular pair
styles"_pair_gran.txt.  Note that if a granular model defines atom
styles"_pair_gran.html.  Note that if a granular model defines atom
types such that all particles of a specific type are monodisperse
(same diameter), then the two settings are effectively identical.

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@@ -132,7 +132,7 @@ between 1 and the number of bond types defined.
The {single/angle} style creates a single angle of type {atype}
between three atoms with IDs {aatom1}, {aatom2}, and {aatom3}.  The
ordering of the atoms is the same as in the {Angles} section of a data
file read by the "read_data"_read_data command.  I.e. the 3 atoms are
file read by the "read_data"_read_data.html command.  I.e. the 3 atoms are
ordered linearly within the angle; the central atom is {aatom2}.
{Atype} must be a value between 1 and the number of angle types
defined.
@@ -140,7 +140,7 @@ defined.
The {single/dihedral} style creates a single dihedral of type {btype}
between two atoms with IDs {batom1} and {batom2}.  The ordering of the
atoms is the same as in the {Dihedrals} section of a data file read by
the "read_data"_read_data command.  I.e. the 4 atoms are ordered
the "read_data"_read_data.html command.  I.e. the 4 atoms are ordered
linearly within the dihedral.  {Dtype} must be a value between 1 and
the number of dihedral types defined.

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