diff --git a/doc/src/angle_gaussian.rst b/doc/src/angle_gaussian.rst index f0a50938e4..88f17092bc 100644 --- a/doc/src/angle_gaussian.rst +++ b/doc/src/angle_gaussian.rst @@ -25,7 +25,7 @@ The *gaussian* angle style uses the potential: .. math:: - E = -k_B T ln\left(\sum_{i=1}^{n} \frac{A_i}{w_i \sqrt{\pi/2}} exp\left( \frac{-(\theta-\theta_{i})^2}{w_i^2})\right) \right) + E = -k_B T ln\left(\sum_{i=1}^{n} \frac{A_i}{w_i \sqrt{\pi/2}} exp\left( \frac{-2(\theta-\theta_{i})^2}{w_i^2}\right) \right) This analytical form is a suitable potential for obtaining mesoscale effective force fields which can reproduce target atomistic distributions :ref:`(Milano) ` @@ -34,7 +34,7 @@ The following coefficients must be defined for each angle type via the the data file or restart files read by the :doc:`read_data ` or :doc:`read_restart ` commands: -* T temperature at which the potential was derived +* :math:`T` temperature at which the potential was derived * :math:`n` (integer >=1) * :math:`A_1` (-) * :math:`w_1` (-) diff --git a/doc/src/bond_gaussian.rst b/doc/src/bond_gaussian.rst index 9fbcf4778c..6ee15248ad 100644 --- a/doc/src/bond_gaussian.rst +++ b/doc/src/bond_gaussian.rst @@ -25,7 +25,7 @@ The *gaussian* bond style uses the potential: .. math:: - E = -k_B T ln\left(\sum_{i=1}^{n} \frac{A_i}{w_i \sqrt{\pi/2}} exp\left( \frac{-(r-r_{i})^2}{w_i^2})\right) \right) + E = -k_B T ln\left(\sum_{i=1}^{n} \frac{A_i}{w_i \sqrt{\pi/2}} exp\left( \frac{-2(r-r_{i})^2}{w_i^2}\right)\right) This analytical form is a suitable potential for obtaining mesoscale effective force fields which can reproduce target atomistic distributions :ref:`(Milano) ` @@ -35,7 +35,7 @@ The following coefficients must be defined for each bond type via the the data file or restart files read by the :doc:`read_data ` or :doc:`read_restart ` commands: -* T temperature at which the potential was derived +* :math:`T` temperature at which the potential was derived * :math:`n` (integer >=1) * :math:`A_1` (-) * :math:`w_1` (-)