From 293bfa04854dc76efd0dddfde27c8c0ddd20bbea Mon Sep 17 00:00:00 2001 From: Axel Kohlmeyer Date: Wed, 20 May 2020 23:28:07 -0400 Subject: [PATCH] fix typo --- doc/src/compute_gyration_shape_chunk.rst | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/doc/src/compute_gyration_shape_chunk.rst b/doc/src/compute_gyration_shape_chunk.rst index 50dd4822ce..94904f757d 100644 --- a/doc/src/compute_gyration_shape_chunk.rst +++ b/doc/src/compute_gyration_shape_chunk.rst @@ -37,7 +37,7 @@ and the relative shape anisotropy, k: b = & l_y - l_x \\ k = & \frac{3}{2} \frac{l_x^2+l_y^2+l_z^2}{(l_x+l_y+l_z)^2} - \frac{1}{2} -where :math:`l_x` <= :math:`l_y` <= :math`l_z` are the three eigenvalues of the gyration tensor. A general description +where :math:`l_x` <= :math:`l_y` <= :math:`l_z` are the three eigenvalues of the gyration tensor. A general description of these parameters is provided in :ref:`(Mattice) ` while an application to polymer systems can be found in :ref:`(Theodorou) `. The asphericity is always non-negative and zero only when the three principal moments are equal. This zero condition is met when the distribution