--- trunk/tengDissertation/Langevin.tex	2006/07/17 15:28:44	2938
+++ trunk/tengDissertation/Langevin.tex	2006/07/17 15:48:57	2939
@@ -278,9 +278,9 @@ arbitrary origin $O$ can be written as
 bead $i$ and origin $O$, the elements of resistance tensor at
 arbitrary origin $O$ can be written as
 \begin{eqnarray}
- \Xi _{}^{tt}  = \sum\limits_i {\sum\limits_j {C_{ij} } } \notag , \\
- \Xi _{}^{tr}  = \Xi _{}^{rt}  = \sum\limits_i {\sum\limits_j {U_i C_{ij} } } , \\
- \Xi _{}^{rr}  =  - \sum\limits_i {\sum\limits_j {U_i C_{ij} } } U_j. \notag \\
+ \Xi _{}^{tt}  & = & \sum\limits_i {\sum\limits_j {C_{ij} } } \notag , \\
+ \Xi _{}^{tr}  & = & \Xi _{}^{rt}  = \sum\limits_i {\sum\limits_j {U_i C_{ij} } } , \\
+ \Xi _{}^{rr}  & = &  - \sum\limits_i {\sum\limits_j {U_i C_{ij} } } U_j. \notag \\
 \label{introEquation:ResistanceTensorArbitraryOrigin}
 \end{eqnarray}
 The resistance tensor depends on the origin to which they refer. The
