fix typos
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@ -25,7 +25,7 @@ The *gaussian* angle style uses the potential:
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.. math::
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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)
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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)
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This analytical form is a suitable potential for obtaining
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mesoscale effective force fields which can reproduce target atomistic distributions :ref:`(Milano) <Milano1>`
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@ -34,7 +34,7 @@ The following coefficients must be defined for each angle type via the
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the data file or restart files read by the :doc:`read_data <read_data>`
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or :doc:`read_restart <read_restart>` commands:
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* T temperature at which the potential was derived
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* :math:`T` temperature at which the potential was derived
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* :math:`n` (integer >=1)
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* :math:`A_1` (-)
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* :math:`w_1` (-)
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@ -25,7 +25,7 @@ The *gaussian* bond style uses the potential:
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.. math::
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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)
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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)
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This analytical form is a suitable potential for obtaining
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mesoscale effective force fields which can reproduce target atomistic distributions :ref:`(Milano) <Milano0>`
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@ -35,7 +35,7 @@ The following coefficients must be defined for each bond type via the
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the data file or restart files read by the :doc:`read_data <read_data>`
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or :doc:`read_restart <read_restart>` commands:
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* T temperature at which the potential was derived
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* :math:`T` temperature at which the potential was derived
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* :math:`n` (integer >=1)
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* :math:`A_1` (-)
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* :math:`w_1` (-)
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