fix up some more package designations and clean up some legacy formatting
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@ -55,7 +55,7 @@ shell of distances in 3d and a thin ring of distances in 2d.
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command, and means those pairwise interactions do not appear in the
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neighbor list. Because this fix uses a neighbor list, it also means
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those pairs will not be included in the RDF. This does not apply when
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using long-range coulomb interactions (\ *coul/long*\ , *coul/msm*\ ,
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using long-range coulomb interactions (\ *coul/long*, *coul/msm*,
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*coul/wolf* or similar. One way to get around this would be to set
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special_bond scaling factors to very tiny numbers that are not exactly
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zero (e.g. 1.0e-50). Another workaround is to write a dump file, and
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@ -94,7 +94,7 @@ The *itypeN* and *jtypeN* arguments are optional. These arguments
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must come in pairs. If no pairs are listed, then a single histogram
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is computed for g(r) between all atom types. If one or more pairs are
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listed, then a separate histogram is generated for each
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*itype*\ ,\ *jtype* pair.
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*itype*,\ *jtype* pair.
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The *itypeN* and *jtypeN* settings can be specified in one of two
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ways. An explicit numeric value can be used, as in the fourth example
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@ -156,13 +156,13 @@ Output info
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"""""""""""
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This compute calculates a global array with the number of rows =
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*Nbins*\ , and the number of columns = 1 + 2\*Npairs, where Npairs is the
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*Nbins*, and the number of columns = 1 + 2\*Npairs, where Npairs is the
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number of I,J pairings specified. The first column has the bin
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coordinate (center of the bin), Each successive set of 2 columns has
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the g(r) and coord(r) values for a specific set of *itypeN* versus
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*jtypeN* interactions, as described above. These values can be used
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by any command that uses a global values from a compute as input. See
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the :doc:`Howto output <Howto_output>` doc page for an overview of
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the :doc:`Howto output <Howto_output>` page for an overview of
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LAMMPS output options.
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The array values calculated by this compute are all "intensive".
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@ -186,7 +186,7 @@ your model. The definition of g(r) used by LAMMPS is only appropriate
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for characterizing atoms that are uniformly distributed throughout the
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simulation cell. In such cases, the coordination number is still
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correct and meaningful. As an example, if a large simulation cell
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contains only one atom of type *itypeN* and one of *jtypeN*\ , then g(r)
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contains only one atom of type *itypeN* and one of *jtypeN*, then g(r)
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will register an arbitrarily large spike at whatever distance they
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happen to be at, and zero everywhere else. Coord(r) will show a step
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change from zero to one at the location of the spike in g(r).
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