--- trunk/tengDissertation/Introduction.tex	2006/06/21 16:28:25	2872
+++ trunk/tengDissertation/Introduction.tex	2006/06/21 16:43:07	2874
@@ -1110,7 +1110,7 @@ g(r) = \frac{V}{{N^2 }}\left\langle {\sum\limits_i {\s
 particle $j$ in the system
 \[
 g(r) = \frac{V}{{N^2 }}\left\langle {\sum\limits_i {\sum\limits_{j
-\ne i} {\delta (r - r_{ij} )} } } \right\rangle = \fract{\rho
+\ne i} {\delta (r - r_{ij} )} } } \right\rangle = \frac{\rho
 (r)}{\rho}.
 \]
 Note that the delta function can be replaced by a histogram in
@@ -1568,7 +1568,7 @@ coordinates ($x_ \apha$) and the system coordinate ($x
 \Delta U =  - \sum\limits_{\alpha  = 1}^N {g_\alpha  x_\alpha  x}
 \]
 where $g_\alpha$ are the coupling constants between the bath
-coordinates ($x_ \apha$) and the system coordinate ($x$).
+coordinates ($x_ \alpha$) and the system coordinate ($x$).
 Introducing
 \[
 W(x) = U(x) - \sum\limits_{\alpha  = 1}^N {\frac{{g_\alpha ^2
