diff --git a/doc/pair_gayberne.html b/doc/pair_gayberne.html index 5397039504..c599878b25 100644 --- a/doc/pair_gayberne.html +++ b/doc/pair_gayberne.html @@ -59,7 +59,7 @@ be used since it defines the rotational state of the ellipsoidal particles.
More details of the Gay-Berne formulation are given in the references -listed below and in this supplementary +listed below and in this supplementary document.
The following coefficients must be defined for each pair of atoms diff --git a/doc/pair_gayberne.txt b/doc/pair_gayberne.txt index 31b82dd336..096027b442 100755 --- a/doc/pair_gayberne.txt +++ b/doc/pair_gayberne.txt @@ -57,7 +57,7 @@ particles. More details of the Gay-Berne formulation are given in the references listed below and in "this supplementary -document"_Eqs/pair_gayberne_extra.pdf. +document"_PDF/pair_gayberne_extra.pdf. The following coefficients must be defined for each pair of atoms types via the "pair_coeff"_pair_coeff.html command as in the examples diff --git a/doc/pair_resquared.html b/doc/pair_resquared.html index e0b6b619df..a21433f817 100644 --- a/doc/pair_resquared.html +++ b/doc/pair_resquared.html @@ -33,7 +33,7 @@ size sigma. The distinction is made to allow the pair style to make efficient calculations of ellipsoid/solvent interactions.
Details for the equations used are given in the references below and -in this supplementary document. +in this supplementary document.
Use of this pair style requires the NVE, NVT, or NPT fixes with the asphere extension (e.g. fix nve/asphere) in @@ -80,7 +80,7 @@ composing the ellipsoids and epsilon_LJ determines the interaction strength of the spherical particles.
For ellipsoid-LJ sphere interactions, A12 gives the energy prefactor -(see here for details: +(see here for details: