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Paul Cuffe edited Methodology.tex
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\section{Seperation of Power System Losses }
\subsection{Partitioning}
The $Y_{bus}$ is reordered, per [8], such that generator buses
(G (\textit{G} subscript) and load buses
(L) (\textit{L}) are grouped together:
\begin{equation}
\label{eq:YLL}
...
$I_{G}$ and $I_{L}$ are complex-valued vectors representing the nodal currents at generator and load buses, respectively, while $V_{G}$ and $V_{L}$ are corresponding complex nodal voltages.
From
(\ref{eq:YLL}):
\begin{equation}
\label{eq:IG}
I_{G} = Y_{GG}V_{G} + Y_{GL}V_{L}
\end{equation}
\begin{equation}
\label{eq:IL}
I_{L} = Y_{LG}V_{G} + Y_{LL}V_{L}
\end{equation}
Rearrange (\ref{eq:IL}) to find that:
\begin{equation}
\label{eq:VL}
V_{L} = Z_{LL}I_{L} - Z_{LL}Y_{LG}V_{G}
\end{equation}
Where $Z_{LL} = Y_{LL}^{-1}$. Substituting for $V_{L}$ in (\ref{eq:IG}):
\begin{equation}
\label{eq:IG2}
I_{G} = (Y_{GG}-Y_{GL}Z_{LL}Y_{LH})V_{G} + Y_{GL}Z_{LL}I_{L}
\end{equation}
Inspecting (\ref{eq:VL}) and (\ref{eq:IG2}) indicates that they (\ref{eq:YLL}) we can
be efficiently represented in block matrix form: derive:
\begin{equation}
\label{eq:YMod}