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\begin{center}
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\large{Additional documention for the Gay-Berne ellipsoidal potential \\
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\large{Additional documentation for the Gay-Berne ellipsoidal potential \\
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as implemented in LAMMPS}
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\end{center}
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@ -21,12 +21,12 @@ $$ U ( \mathbf{A}_1, \mathbf{A}_2, \mathbf{r}_{12} ) = U_r (
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\mathbf{A}_1, \mathbf{A}_2, \upsilon ) \cdot \chi_{12} ( \mathbf{A}_1,
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\mathbf{A}_2, \mathbf{r}_{12}, \mu ) $$
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where $\mathbf{A}_1$ and $\mathbf{A}_2$ are the transformation matrices
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from the simulation box frame to the body frame and $\mathbf{r}_{12}$
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is the center to center vectorb etween the particles.
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$U_r$ controls the shifted distance dependent
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interaction based on the distance of closest approach of the two
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particles ($h_{12}$) and the user-specified shift parameter gamma:
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where $\mathbf{A}_1$ and $\mathbf{A}_2$ are the transformation
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matrices from the simulation box frame to the body frame and
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$\mathbf{r}_{12}$ is the center to center vector between the
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particles. $U_r$ controls the shifted distance dependent interaction
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based on the distance of closest approach of the two particles
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($h_{12}$) and the user-specified shift parameter gamma:
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$$ U_r = 4 \epsilon ( \varrho^{12} - \varrho^6) $$
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\begin{center}
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\large{Additional documention for the RE-squared ellipsoidal potential \\
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\large{Additional documentation for the RE-squared ellipsoidal potential \\
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as implemented in LAMMPS}
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\end{center}
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