Loading doc/src/compute_gyration_shape.txt +4 −4 Original line number Diff line number Diff line Loading @@ -32,8 +32,8 @@ and the relative shape anisotropy, k: :c,image(Eqs/compute_shape_parameters.jpg) where lx <= ly <= lz are the three eigenvalues of the gyration tensor. A general description of these parameters is provided in "(Mattice)"_#Mattice while an application to polymer systems can be found in "(Theodorou)"_#Theodorou. of these parameters is provided in "(Mattice)"_#Mattice1 while an application to polymer systems can be found in "(Theodorou)"_#Theodorou1. The asphericity is always non-negative and zero only when the three principal moments are equal. This zero condition is met when the distribution of particles is spherically symmetric (hence the name asphericity) but also whenever the particle Loading Loading @@ -83,9 +83,9 @@ package"_Build_package.html doc page for more info. :line :link(Mattice) :link(Mattice1) [(Mattice)] Mattice, Suter, Conformational Theory of Large Molecules, Wiley, New York, 1994. :link(Theodorou) :link(Theodorou1) [(Theodorou)] Theodorou, Suter, Macromolecules, 18, 1206 (1985). doc/src/compute_gyration_shape_chunk.txt +4 −4 Original line number Diff line number Diff line Loading @@ -32,8 +32,8 @@ and the relative shape anisotropy, k: :c,image(Eqs/compute_shape_parameters.jpg) where lx <= ly <= lz are the three eigenvalues of the gyration tensor. A general description of these parameters is provided in "(Mattice)"_#Mattice while an application to polymer systems can be found in "(Theodorou)"_#Theodorou. The asphericity is always non-negative and zero of these parameters is provided in "(Mattice)"_#Mattice2 while an application to polymer systems can be found in "(Theodorou)"_#Theodorou2. The asphericity is always non-negative and zero only when the three principal moments are equal. This zero condition is met when the distribution of particles is spherically symmetric (hence the name asphericity) but also whenever the particle distribution is symmetric with respect to the three coordinate axes, e.g., Loading Loading @@ -85,9 +85,9 @@ package"_Build_package.html doc page for more info. :line :link(Mattice) :link(Mattice2) [(Mattice)] Mattice, Suter, Conformational Theory of Large Molecules, Wiley, New York, 1994. :link(Theodorou) :link(Theodorou2) [(Theodorou)] Theodorou, Suter, Macromolecules, 18, 1206 (1985). Loading
doc/src/compute_gyration_shape.txt +4 −4 Original line number Diff line number Diff line Loading @@ -32,8 +32,8 @@ and the relative shape anisotropy, k: :c,image(Eqs/compute_shape_parameters.jpg) where lx <= ly <= lz are the three eigenvalues of the gyration tensor. A general description of these parameters is provided in "(Mattice)"_#Mattice while an application to polymer systems can be found in "(Theodorou)"_#Theodorou. of these parameters is provided in "(Mattice)"_#Mattice1 while an application to polymer systems can be found in "(Theodorou)"_#Theodorou1. The asphericity is always non-negative and zero only when the three principal moments are equal. This zero condition is met when the distribution of particles is spherically symmetric (hence the name asphericity) but also whenever the particle Loading Loading @@ -83,9 +83,9 @@ package"_Build_package.html doc page for more info. :line :link(Mattice) :link(Mattice1) [(Mattice)] Mattice, Suter, Conformational Theory of Large Molecules, Wiley, New York, 1994. :link(Theodorou) :link(Theodorou1) [(Theodorou)] Theodorou, Suter, Macromolecules, 18, 1206 (1985).
doc/src/compute_gyration_shape_chunk.txt +4 −4 Original line number Diff line number Diff line Loading @@ -32,8 +32,8 @@ and the relative shape anisotropy, k: :c,image(Eqs/compute_shape_parameters.jpg) where lx <= ly <= lz are the three eigenvalues of the gyration tensor. A general description of these parameters is provided in "(Mattice)"_#Mattice while an application to polymer systems can be found in "(Theodorou)"_#Theodorou. The asphericity is always non-negative and zero of these parameters is provided in "(Mattice)"_#Mattice2 while an application to polymer systems can be found in "(Theodorou)"_#Theodorou2. The asphericity is always non-negative and zero only when the three principal moments are equal. This zero condition is met when the distribution of particles is spherically symmetric (hence the name asphericity) but also whenever the particle distribution is symmetric with respect to the three coordinate axes, e.g., Loading Loading @@ -85,9 +85,9 @@ package"_Build_package.html doc page for more info. :line :link(Mattice) :link(Mattice2) [(Mattice)] Mattice, Suter, Conformational Theory of Large Molecules, Wiley, New York, 1994. :link(Theodorou) :link(Theodorou2) [(Theodorou)] Theodorou, Suter, Macromolecules, 18, 1206 (1985).
