Update pair_ylz.rst
Corrected some typo in formulations
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@ -33,23 +33,21 @@ relative particle orientations via the formulas
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.. math::
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U ( \mathbf{r}_{ij}, \mathbf{n}_i, \mathbf{n}_j ) =\left\{\begin{matrix} \mathbf{u}_R(r)+\left [ 1-\phi (\mathbf{r\hat{}}_{ij}, \mathbf{n}_i, \mathbf{n}_j ) \right ]\epsilon, ~~ r<\mathbf{r}_{min} \\ \mathbf{u}_A(r)\phi (\mathbf{r\hat{}}_{ij}, \mathbf{n}_i, \mathbf{n}_j ),~~ \mathbf{r}_{min}<r<\mathbf{r}_{c} \\ \end{matrix}\right.\\\\ \phi (\mathbf{r\hat{}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )=1+\mu (a(\mathbf{r\hat{}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )-1) \\\\ a(\mathbf{r\hat{}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )=(\mathbf{n}_i\times\mathbf{r\hat{}}_{ij} )\cdot (\mathbf{n}_j\times\mathbf{r\hat{}}_{ij} )+sin\mathbf{\theta}_0(\mathbf{n}_i-\mathbf{n}_j)\cdot \mathbf{r\hat{}}_{ij}\\\\ \mathbf{u}_R(r)=\epsilon \left [ \left ( \frac{{r}_{min}}{r} \right )^{4}-2\left ( \frac{{r}_{min}}{r}\right )^{2} \right ] \\\\ \mathbf{u}_A(r)=-\epsilon\;cos^{2\zeta }\left ( \frac{\pi}{2}\frac{\left ( {r}-{r}_{min} \right )}{\left ( {r}_{c}-{r}_{min} \right )} \right ) \\
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U ( \mathbf{r}_{ij}, \mathbf{n}_i, \mathbf{n}_j ) =\left\{\begin{matrix} {u}_R(r)+\left [ 1-\phi (\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j ) \right ]\epsilon, ~~ r<{r}_{min} \\ {u}_A(r)\phi (\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j ),~~ {r}_{min}<r<{r}_{c} \\ \end{matrix}\right.\\\\ \phi (\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )=1+\left [ \mu (a(\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )-1) \right ] \\\\a(\mathbf{\hat{r}}_{ij}, \mathbf{n}_i, \mathbf{n}_j )=(\mathbf{n}_i\times\mathbf{\hat{r}}_{ij} )\cdot (\mathbf{n}_j\times\mathbf{\hat{r}}_{ij} )+{\beta}(\mathbf{n}_i-\mathbf{n}_j)\cdot \mathbf{\hat{r}}_{ij}-\beta^{2}\\\\ {u}_R(r)=\epsilon \left [ \left ( \frac{{r}_{min}}{r} \right )^{4}-2\left ( \frac{{r}_{min}}{r}\right )^{2} \right ] \\\\ {u}_A(r)=-\epsilon\;cos^{2\zeta }\left [ \frac{\pi}{2}\frac{\left ( {r}-{r}_{min} \right )}{\left ( {r}_{c}-{r}_{min} \right )} \right ]\\
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where :math:`r_{i}` and :math:`r_{j}` are the center position vectors of
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particles i and j, respectively, :math:`r_{ij}=r_{i}-r_{j}` is the
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inter-particle distance vector, :math:`r=\left|r_{ij} \right|` and
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:math:`{r\hat{}}_{ij}=\mathbf{r}_{ij}/r`. The unit vectors :math:`n_{i}`
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and :math:`n_{j}` represent the axes of symmetry of particles i and j,
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respectively. :math:`u_R` and :math:`u_A` are the repulsive and
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attractive potentials. :math:`\phi` is an angular function which depends
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on the relative orientation between pair particles. :math:`\mu` is the
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parameter related to bending rigidity, :math:`\theta_{0}` is the
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parameter related to the spontaneous curvature, and :math:`\epsilon` is
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the energy unit, respectively. The :math:`\zeta` controls the slope of
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the attractive branch and :math:`{r}_{c}`is the cutoff
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radius. :math:`r_{min}` is the distance which minimizes the potential
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energy :math:`u_{A}(r)`and :math:`r_{min}=2^{1/6}\sigma`, where
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:math:`\sigma` is the length unit.
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where :math:`\mathbf{r}_{i}` and :math:`\mathbf{r}_{j}` are the center position
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vectors of particles i and j, respectively, :math:`\mathbf{r}_{ij}=\mathbf{r}_{i}-\mathbf{r}_{j}`
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is the inter-particle distance vector, :math:`r=\left|\mathbf{r}_{ij} \right|` and
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:math:`{\hat{\mathbf{r}}}_{ij}=\mathbf{r}_{ij}/r`. The unit vectors
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:math:`\mathbf{n}_{i}` and :math:`\mathbf{n}_{j}` represent the axes of symmetry of
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particles i and j, respectively, :math:`u_R` and :math:`u_A` are the
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repulsive and attractive potentials, :math:`\phi` is an angular function which depends on
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the relative orientation between pair particles, :math:`\mu` is the parameter
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related to bending rigidity, :math:`\beta` is the parameter related to the spontaneous
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curvature, and :math:`\epsilon` is the energy unit, respectively. The :math:`\zeta` controls
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the slope of the attractive branch and :math:`{r}_{c}`is the cutoff radius. :math:`r_{min}`
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is the distance which minimizes the potential energy :math:`u_{A}(r)`and
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:math:`r_{min}=2^{1/6}\sigma`, where :math:`\sigma` is the length unit.
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Use of this pair style requires the NVE, NVT, or NPT fixes with the *asphere* extension (e.g. :doc:`fix nve/asphere <fix_nve_asphere>`) in order to integrate particle rotation. Additionally, :doc:`atom_style ellipsoid <atom_style>` should be used since it defines the rotational state of each particle.
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@ -59,7 +57,7 @@ The following coefficients must be defined for each pair of atoms types via the
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* :math:`\sigma` = minimum effective particle radii (distance units)
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* :math:`\zeta` = tune parameter for the slope of the attractive branch
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* :math:`\mu` = parameter related to bending rigidity
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* :math:`\sin(\theta _{0})` is the sine of parameter related to the spontaneous curvature
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* :math:`\beta` = parameter related to the spontaneous curvature
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* cutoff (distance units)
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The last coefficient is optional. If not specified, the global
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