diff --git a/DOCUMENTATION/SACAMOS_TheoryManual.pdf b/DOCUMENTATION/SACAMOS_TheoryManual.pdf
index 1773bd1..6838405 100644
Binary files a/DOCUMENTATION/SACAMOS_TheoryManual.pdf and b/DOCUMENTATION/SACAMOS_TheoryManual.pdf differ
diff --git a/DOCUMENTATION/THEORY_MANUAL/Tex/Laplace_Solver_Documentation.tex b/DOCUMENTATION/THEORY_MANUAL/Tex/Laplace_Solver_Documentation.tex
index 96c919c..b8ec4cd 100644
--- a/DOCUMENTATION/THEORY_MANUAL/Tex/Laplace_Solver_Documentation.tex
+++ b/DOCUMENTATION/THEORY_MANUAL/Tex/Laplace_Solver_Documentation.tex
@@ -110,7 +110,7 @@ Without an outer shield the electrostatic field is no longer confined to a bound
 
 %Of all available techniques we have chosen to truncate the domain by introducing a fictitious contour that encloses the domain of primary %interest and prescribe on it an asymptotic boundary condition which mimics the behaviour of the electrostatic potential in the region %outside the contour. Not only has it been shown that asymptotic boundaries give good results, the technique is relatively easy to implement %and preserves the sparsity of the finite element coefficient matrix which makes it a very efficient method as-well.\\
 
-In unshielded condcutor configurations a suitable boundary condition must be applied on the outer boundary of the problems space. The imposition of a boundary condition will necessarily have an effect on the fields within the Finite Element domain and hence the capacitance matrix to be calculated. Three possible boundary conditions are outlined here, the Dirichelet boundary condition ($\phi=0$), the Neumann boundary condition $\frac{\partial \phi(r) }{\partial r}=0$ and an asymptotic boundary condition,  
+In unshielded conductor configurations a suitable boundary condition must be applied on the outer boundary of the problems space. The imposition of a boundary condition will necessarily have an effect on the fields within the Finite Element domain and hence the capacitance matrix to be calculated. Three possible boundary conditions are outlined here, the Dirichelet boundary condition ($\phi=0$), the Neumann boundary condition $\frac{\partial \phi(r) }{\partial r}=0$ and an asymptotic boundary condition,  
 $\frac{\partial \phi(r) }{\partial r}=\frac{1}{r ln(r)}\phi(r)$. 
 
 \subsubsection{Dirichelet boundary conditions}
@@ -127,7 +127,7 @@ This boundary condition enforces a condition that the normal derivitive of the p
 
 \subsubsection{Asymptotic boundary conditions}
 
-For electrostatic problems, the potential in a point ${\bf{r}}$, can be written as\\
+For 2D electrostatic problems, the potential in a point ${\bf{r}}$, can be written as\\
 \\
 \begin{equation}\phi\left(\mathbf{r}\right)=\iint_{\Omega}\rho\left(\mathbf{r}'\right) G\left(\mathbf{r},\mathbf{r}'\right)d\mathbf{r}'\end{equation}
 \\
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