address spelling issues
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@ -155,7 +155,7 @@ page on BPMs.
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If the *break* keyword is set to *no*, LAMMPS assumes bonds should not break
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during a simulation run. This will prevent some unnecessary calculation.
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The recommended bond communication distance no longer depends on bond failure
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coefficients (which are ignored) but instead corresponds to the typical heurestic
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coefficients (which are ignored) but instead corresponds to the typical heuristic
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maximum strain used by typical non-bpm bond styles. Similar behavior to *break no*
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can also be attained by setting arbitrarily high values for all four failure
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coefficients. One cannot use *break no* with *smooth yes*.
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@ -119,7 +119,7 @@ If the *break* keyword is set to *no*, LAMMPS assumes bonds should not break
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during a simulation run. This will prevent some unnecessary calculation.
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The recommended bond communication distance no longer depends on the value of
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:math:`\epsilon_c` (which is ignored) but instead corresponds to the typical
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heurestic maximum strain used by typical non-bpm bond styles. Similar behavior
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heuristic maximum strain used by typical non-bpm bond styles. Similar behavior
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to *break no* can also be attained by setting an arbitrarily high value of
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:math:`\epsilon_c`. One cannot use *break no* with *smooth yes*.
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@ -101,7 +101,7 @@ A modified form of Fickian particle shifting can be enabled with the
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more uniform spatial distribution. By default, shifting does not consider the
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type of a particle and therefore may be inappropriate in systems consisting
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of multiple atom types representing multiple fluid phases. However, two
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optional subarguments can follow the *shift* keyword, *exclude/type* and
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optional sub-arguments can follow the *shift* keyword, *exclude/type* and
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*scale/cross/type* to adjust shifting at fluid interfaces.
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The *exclude/type* option lets the user specify a list of atom types which
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@ -155,7 +155,7 @@ threshold for this classification is set by the numerical value of
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By default, RHEO integrates particles' densities using a mass diffusion
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equation. Alternatively, one can update densities every timestep by performing
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a kernel summation of the masses of neighboring particles by specifying the *rho/sum*
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keyword. Following this keyword, one may include the optional *self/mass* subargument
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keyword. Following this keyword, one may include the optional *self/mass* sub-argument
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which modifies the behavior of the density summation. Typically, the density
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:math:`\rho` of a particle is calculated as the sum over neighbors
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@ -2499,6 +2499,7 @@ neel
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Neel
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Neelov
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Negre
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Negrut
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nelem
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Nelement
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Nelements
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@ -3116,6 +3117,7 @@ Rafferty
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rahman
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Rahman
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Rajamanickam
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Rakhsha
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Ralf
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Raman
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ramped
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