diff --git a/doc/html/Section_packages.html b/doc/html/Section_packages.html index f882ee234b..fedd3cc1ae 100644 --- a/doc/html/Section_packages.html +++ b/doc/html/Section_packages.html @@ -493,7 +493,7 @@ name links to a sub-section below with more details.
compute myRDF all rdf 50
-fix 1 all ave/time 100 1 100 c_myRDF file tmp.rdf mode vector
+fix 1 all ave/time 100 1 100 c_myRDF[*] file tmp.rdf mode vector
Output info:
diff --git a/doc/html/fix_lb_pc.html b/doc/html/fix_lb_pc.html index 8a5281c6c3..4fe4f72ced 100644 --- a/doc/html/fix_lb_pc.html +++ b/doc/html/fix_lb_pc.html @@ -146,7 +146,7 @@Update the positions and velocities of the individual particles described by group-ID, experiencing velocity-dependent hydrodynamic -forces, using the integration algorithm described in Mackay et al.. This integration algorithm should only be used if a +forces, using the integration algorithm described in Mackay et al.. This integration algorithm should only be used if a user-specified value for the force-coupling constant used in fix lb/fluid has been set; do not use this integration algorithm if the force coupling constant has been set by default.
diff --git a/doc/html/pair_thole.html b/doc/html/pair_thole.html index b2742247f9..e3a5f8b9cb 100644 --- a/doc/html/pair_thole.html +++ b/doc/html/pair_thole.html @@ -189,8 +189,8 @@ short distances by a function \frac{s_{ij} r_{ij} }{2} \right) \exp \left( - s_{ij} r_{ij} \right) \end{equation}\]This function results from an adaptation to point charges -(Noskov) of the dipole screening scheme originally proposed -by Thole. The scaling coefficient \(s_{ij}\) is determined +(Noskov) of the dipole screening scheme originally proposed +by Thole. The scaling coefficient \(s_{ij}\) is determined by the polarizability of the atoms, \(\alpha_i\), and by a Thole damping parameter \(a\). This Thole damping parameter usually takes a value of 2.6, but in certain force fields the value can depend upon