Unbalanced, Three phase, Three wire, Y Connected Load
For the system shown in Fig. 1, the required equations can be
derived by first applying Kirchhoff’s voltage law around each closed loop to produce
Substituting, we have
Applying Kirchhoff's current law at node $ n $ results in
Substituting for $ \mathbf{I}_{b n} $ in Eqs. (1) and (2) yields
which are rewritten as
Using determinants, we have
Applying Kirchhoff's voltage law to the line voltages:
Substituting for $ \left(\mathbf{E}_{A B}+\mathbf{E}_{C B}\right) $ in the above equation for $ \mathbf{I}_{a n} $ :
and
In the same manner, it can be shown that
Substituting Eq. (5) for $ \mathbf{I}_{c n} $ in the right-hand side of Eq. (2), we obtain
Fig. 1: Unbalanced, three-phase, three-wire, Y-connected load
$$\begin{array}{l}\mathbf{E}_{A B}-\mathbf{V}_{a n}+\mathbf{V}_{b n}=0 \\\mathbf{E}_{B C}-\mathbf{V}_{b n}+\mathbf{V}_{c n}=0 \\\mathbf{E}_{C A}-\mathbf{V}_{c n}+\mathbf{V}_{a n}=0\end{array}$$
$$\mathbf{V}_{a n}=\mathbf{I}_{a n} \mathbf{Z}_{1} \quad \mathbf{V}_{b n}=\mathbf{I}_{b n} \mathbf{Z}_{2} \quad \mathbf{V}_{c n}=\mathbf{I}_{c n} \mathbf{Z}_{3}$$
$$\begin{array}{l}
\bbox[10px,border:1px solid grey]{\mathbf{E}_{A B}=\mathbf{I}_{a n} \mathbf{Z}_{1}-\mathbf{I}_{b n} \mathbf{Z}_{2}} \quad \text{(1)}\\
\bbox[10px,border:1px solid grey]{\mathbf{E}_{B C}=\mathbf{I}_{b n} \mathbf{Z}_{2}-\mathbf{I}_{c n} \mathbf{Z}_{3}} \quad \text{(2)}\\
\bbox[10px,border:1px solid grey]{\mathbf{E}_{C A}=\mathbf{I}_{c n} \mathbf{Z}_{3}-\mathbf{I}_{a n} \mathbf{Z}_{1}} \quad \text{(3)}
\end{array}$$
$$\mathbf{I}_{a n}+\mathbf{I}_{b n}+\mathbf{I}_{c n}=0 \quad \text { and } \quad \mathbf{I}_{b n}=-\mathbf{I}_{a n}-\mathbf{I}_{c n}$$
$$\begin{array}{l}\mathbf{E}_{A B}=\mathbf{I}_{a n} \mathbf{Z}_{1}-\left[-\left(\mathbf{I}_{a n}+\mathbf{I}_{c n}\right)\right] \mathbf{Z}_{2} \\\mathbf{E}_{B C}=-\left(\mathbf{I}_{a n}+\mathbf{I}_{c n}\right) \mathbf{Z}_{2}-\mathbf{I}_{c n} \mathbf{Z}_{3}
\end{array}$$
$$\begin{array}{l}\mathbf{E}_{A B}=\mathbf{I}_{a n}\left(\mathbf{Z}_{1}+\mathbf{Z}_{2}\right)+\mathbf{I}_{c n} \mathbf{Z}_{2} \\\mathbf{E}_{B C}=\mathbf{I}_{a n}\left(-\mathbf{Z}_{2}\right)+\mathbf{I}_{c n}\left[-\left(\mathbf{Z}_{2}+\mathbf{Z}_{3}\right)\right]\end{array}$$
$$\begin{aligned}\mathbf{I}_{a n} &=\frac{\left|\begin{array}{cc}\mathbf{E}_{A B} & \mathbf{Z}_{2} \\\mathbf{E}_{B C} & -\left(\mathbf{Z}_{2}+\mathbf{Z}_{3}\right)\end{array}\right|}{\left|\begin{array}{cc}\mathbf{Z}_{1}+\mathbf{Z}_{2} & \mathbf{Z}_{2} \\-\mathbf{Z}_{2} & -\left(\mathbf{Z}_{2}+\mathbf{Z}_{3}\right)\end{array}\right|} \\&=\frac{-\left(\mathbf{Z}_{2}+\mathbf{Z}_{3}\right) \mathbf{E}_{A B}-\mathbf{E}_{B C} \mathbf{Z}_{2}}{-\mathbf{Z}_{1} \mathbf{Z}_{2}-\mathbf{Z}_{1} \mathbf{Z}_{3}-\mathbf{Z}_{2} \mathbf{Z}_{3}-\mathbf{Z}_{2}^{2}+\mathbf{Z}_{2}^{2}} \\\mathbf{I}_{a n} &=\frac{-\mathbf{Z}_{2}\left(\mathbf{E}_{A B}+\mathbf{E}_{B C}\right)-\mathbf{Z}_{3} \mathbf{E}_{A B}}{-\mathbf{Z}_{1} \mathbf{Z}_{2}-\mathbf{Z}_{1} \mathbf{Z}_{3}-\mathbf{Z}_{2} \mathbf{Z}_{3}}\end{aligned}$$
$$\mathbf{E}_{A B}+\mathbf{E}_{C A}+\mathbf{E}_{B C}=0 \text { or } \mathbf{E}_{A B}+\mathbf{E}_{B C}=-\mathbf{E}_{C A}$$
$$\mathbf{I}_{a n}=\frac{-\mathbf{Z}_{2}\left(-\mathbf{E}_{C A}\right)-\mathbf{Z}_{3} \mathbf{E}_{A B}}{-\mathbf{Z}_{1} \mathbf{Z}_{2}-\mathbf{Z}_{1} \mathbf{Z}_{3}-\mathbf{Z}_{2} \mathbf{Z}_{3}}$$
$$ \bbox[10px,border:1px solid grey]{\mathbf{I}_{a n}=\frac{\mathbf{E}_{A B} \mathbf{Z}_{3}-\mathbf{E}_{C A} \mathbf{Z}_{2}}{\mathbf{Z}_{1} \mathbf{Z}_{2}+\mathbf{Z}_{1} \mathbf{Z}_{3}+\mathbf{Z}_{2} \mathbf{Z}_{3}}} \tag{4}$$
$$\bbox[10px,border:1px solid grey]{\mathbf{I}_{c n}=\frac{\mathbf{E}_{C A} \mathbf{Z}_{2}-\mathbf{E}_{B C} \mathbf{Z}_{1}}{\mathbf{Z}_{1} \mathbf{Z}_{2}+\mathbf{Z}_{1} \mathbf{Z}_{3}+\mathbf{Z}_{2} \mathbf{Z}_{3}}} \tag{5}$$
$$\bbox[10px,border:1px solid grey]{\mathbf{I}_{b n}=\frac{\mathbf{E}_{B C} \mathbf{Z}_{1}-\mathbf{E}_{A B} \mathbf{Z}_{3}}{\mathbf{Z}_{1} \mathbf{Z}_{2}+\mathbf{Z}_{1} \mathbf{Z}_{3}+\mathbf{Z}_{2} \mathbf{Z}_{3}}}$$
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