--- trunk/tengDissertation/LiquidCrystal.tex	2006/06/21 18:28:27	2875
+++ trunk/tengDissertation/LiquidCrystal.tex	2006/06/21 19:46:01	2876
@@ -276,19 +276,21 @@ by other researchers in liquid crystal studies\cite{Be
 arbitrary shape was introduce by Stone\cite{Stone1978} and adopted
 by other researchers in liquid crystal studies\cite{Berardi2000}.
 
-\begin{equation}
-S_{22}^{220} (r) = \frac{1}{{4\sqrt 5 }}\left\langle {\delta (r -
-r_{ij} )((\hat x_i  \cdot \hat x_j )^2  - (\hat x_i  \cdot \hat y_j
-)^2  - (\hat y_i  \cdot \hat x_j )^2  + (\hat y_i  \cdot \hat y_j
-)^2 ) - 2(\hat x_i  \cdot \hat y_j )(\hat y_i  \cdot \hat x_j ) -
+\begin{eqnarray}
+S_{22}^{220} (r) & = & \frac{1}{{4\sqrt 5 }}\left\langle {\delta (r
+- r_{ij} )((\hat x_i  \cdot \hat x_j )^2  - (\hat x_i  \cdot \hat
+y_j )^2  - (\hat y_i  \cdot \hat x_j )^2  + (\hat y_i  \cdot \hat
+y_j )^2 ) \\
+& & - 2(\hat x_i  \cdot \hat y_j )(\hat y_i  \cdot \hat x_j ) -
 2(\hat x_i  \cdot \hat x_j )(\hat y_i  \cdot \hat y_j ))}
 \right\rangle
-\end{equation}
+\end{eqnarray}
 
 \begin{equation}
 S_{00}^{221} (r) =  - \frac{{\sqrt 3 }}{{\sqrt {10} }}\left\langle
 {\delta (r - r_{ij} )((\hat z_i  \cdot \hat z_j )(\hat z_i  \cdot
-\hat z_j  \times \hat r_{ij} ))} \right\rangle s\end{equation}
+\hat z_j  \times \hat r_{ij} ))} \right\rangle
+\end{equation}
 
 \section{Results and Conclusion}
 \label{sec:results and conclusion}