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Revision 2883 by tim, Sun Jun 25 17:39:42 2006 UTC vs.
Revision 2884 by tim, Sun Jun 25 17:54:42 2006 UTC

# Line 69 | Line 69 | for molecule $i$ and molecule $j$ respectively.
69   where $r_{ij}$ is the vector between molecule $i$ and molecule $j$,
70   $\Omega _i$ and $\Omega _j$ are the orientational degrees of freedom
71   for molecule $i$ and molecule $j$ respectively.
72 < \[
73 < V_{LJ} (r_{ij} ) = 4\varepsilon _{ij} \left[ {\left( {\frac{{\sigma
74 < _{ij} }}{{r_{ij} }}} \right)^{12}  - \left( {\frac{{\sigma _{ij}
75 < }}{{r_{ij} }}} \right)^6 } \right]
76 < \]
77 < \[
78 < V_{dp} (r_{ij} ,\Omega _i ,\Omega _j ) = \frac{1}{{4\pi \varepsilon
79 < _0 }}\left[ {\frac{{\mu _i  \cdot \mu _j }}{{r_{ij}^3 }} -
80 < \frac{{3\left( {\mu _i  \cdot r_{ij} } \right)\left( {\mu _i  \cdot
81 < r_{ij} } \right)}}{{r_{ij}^5 }}} \right]
82 < \]
83 < \[
84 < V_{sticky} (r_{ij} ,\Omega _i ,\Omega _j ) = v_0 [s(r_{ij} )w(r_{ij}
85 < ,\Omega _i ,\Omega _j ) + s'(r_{ij} )w'(r_{ij} ,\Omega _i ,\Omega _j
86 < )]
87 < \]
72 > \begin{eqnarray*}
73 > V_{LJ} (r_{ij} ) &= &4\varepsilon _{ij} \left[ {\left(
74 > {\frac{{\sigma _{ij} }}{{r_{ij} }}} \right)^{12}  - \left(
75 > {\frac{{\sigma _{ij}
76 > }}{{r_{ij} }}} \right)^6 } \right], \\
77 > V_{dp} (r_{ij} ,\Omega _i ,\Omega _j ) &= &
78 > \frac{|\mu_i||\mu_j|}{4\pi\epsilon_{0}r_{ij}^{3}} \biggl[
79 > \hat{u}_{i} \cdot \hat{u}_{j} - 3(\hat{u}_i \cdot \hat{\mathbf{r}}_{ij}) %
80 > (\hat{u}_j \cdot \hat{\mathbf{r}}_{ij}) \biggr],\\
81 > V_{sticky} (r_{ij} ,\Omega _i ,\Omega _j ) &=& v_0 [s(r_{ij}
82 > )w(r_{ij} ,\Omega _i ,\Omega _j ) + s'(r_{ij} )w'(r_{ij} ,\Omega _i
83 > ,\Omega _j )].\\
84 > \end{eqnarray*}
85   where $v_0$ is a strength parameter, $s$ and $s'$ are cubic
86 < switching functions, while $w$   and $w'$  are responsible for the
86 > switching functions, while $w$ and $w'$  are responsible for the
87   tetrahedral potential and the short-range correction to the dipolar
88   interaction respectively.
89   \[

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