diff --git a/doc/src/bond_bpm_rotational.rst b/doc/src/bond_bpm_rotational.rst
index e4cfef3d51..cfbd01dd99 100644
--- a/doc/src/bond_bpm_rotational.rst
+++ b/doc/src/bond_bpm_rotational.rst
@@ -155,7 +155,7 @@ page on BPMs.
 If the *break* keyword is set to *no*, LAMMPS assumes bonds should not break
 during a simulation run. This will prevent some unnecessary calculation.
 The recommended bond communication distance no longer depends on bond failure
-coefficients (which are ignored) but instead corresponds to the typical heurestic
+coefficients (which are ignored) but instead corresponds to the typical heuristic
 maximum strain used by typical non-bpm bond styles. Similar behavior to *break no*
 can also be attained by setting arbitrarily high values for all four failure
 coefficients. One cannot use *break no* with *smooth yes*.
diff --git a/doc/src/bond_bpm_spring.rst b/doc/src/bond_bpm_spring.rst
index c868a47a12..0a43a62159 100644
--- a/doc/src/bond_bpm_spring.rst
+++ b/doc/src/bond_bpm_spring.rst
@@ -119,7 +119,7 @@ If the *break* keyword is set to *no*, LAMMPS assumes bonds should not break
 during a simulation run. This will prevent some unnecessary calculation.
 The recommended bond communication distance no longer depends on the value of
 :math:`\epsilon_c` (which is ignored) but instead corresponds to the typical
-heurestic maximum strain used by typical non-bpm bond styles. Similar behavior
+heuristic maximum strain used by typical non-bpm bond styles. Similar behavior
 to *break no* can also be attained by setting an arbitrarily high value of
 :math:`\epsilon_c`. One cannot use *break no* with *smooth yes*.
 
diff --git a/doc/src/fix_rheo.rst b/doc/src/fix_rheo.rst
index 6add84a5ca..ef18d19f82 100644
--- a/doc/src/fix_rheo.rst
+++ b/doc/src/fix_rheo.rst
@@ -101,7 +101,7 @@ A modified form of Fickian particle shifting can be enabled with the
 more uniform spatial distribution. By default, shifting does not consider the
 type of a particle and therefore may be inappropriate in systems consisting
 of multiple atom types representing multiple fluid phases. However, two
-optional subarguments can follow the *shift* keyword, *exclude/type* and
+optional sub-arguments can follow the *shift* keyword, *exclude/type* and
 *scale/cross/type* to adjust shifting at fluid interfaces.
 
 The *exclude/type* option lets the user specify a list of atom types which
@@ -155,7 +155,7 @@ threshold for this classification is set by the numerical value of
 By default, RHEO integrates particles' densities using a mass diffusion
 equation. Alternatively, one can update densities every timestep by performing
 a kernel summation of the masses of neighboring particles by specifying the *rho/sum*
-keyword. Following this keyword, one may include the optional *self/mass* subargument
+keyword. Following this keyword, one may include the optional *self/mass* sub-argument
 which modifies the behavior of the density summation. Typically, the density
 :math:`\rho` of a particle is calculated as the sum over neighbors
 
diff --git a/doc/utils/sphinx-config/false_positives.txt b/doc/utils/sphinx-config/false_positives.txt
index 8e601d6c16..67db18a17d 100644
--- a/doc/utils/sphinx-config/false_positives.txt
+++ b/doc/utils/sphinx-config/false_positives.txt
@@ -2499,6 +2499,7 @@ neel
 Neel
 Neelov
 Negre
+Negrut
 nelem
 Nelement
 Nelements
@@ -3116,6 +3117,7 @@ Rafferty
 rahman
 Rahman
 Rajamanickam
+Rakhsha
 Ralf
 Raman
 ramped