@@ -59,3 +59,44 @@ with the following possible combinations of the {py:class}`associated phases <po
5959- Single phase to ground: ` a ` , ` b ` , ` c `
6060- Two phase: ` ab ` , ` bc ` , ` ac `
6161- Two phase to ground: ` ab ` , ` bc ` , ` ac `
62+
63+ ## Prefault voltages
64+
65+ IEC 60909 prescribes use of rated voltage of the fault node on the Thevenin equivalent of the grid impedance for
66+ calculation of $I_k^{\prime\prime}$.
67+ This isolates the short circuit calculations from the actual loading conditions of the grid.
68+
69+ PGM extends IEC 60909 to support simulation of multiple simultaneous faults for advanced use cases.
70+ Since IEC 60909 does not prescribe a method for this scenario,
71+ PGM deviates slightly from the standard to accommodate it.
72+ Prefault voltages and corresponding $I_k^{\prime\prime}$ deviate by an
73+ "equivalent transformation ratio" from all transformers.
74+
75+ An example is shown below to demonstrate this effect.
76+ In the following grid, lets say we assumed the rated voltage of the source and fault node is $u_ {rated-1}$ and
77+ $u_ {rated-2}$ respectively.
78+ The transformer has a $u1$/$u2$ transformation ratio.
79+ Let $z_k$ and $z_t$ denote the source and transformer impedances, respectively.
80+
81+ ``` {tikz}
82+ :alt: transformer
83+
84+ \draw (0,3) node[gridnode, anchor=east]{} to (1,3);
85+ \draw [black, ultra thick] (1,2) -- (1,4);
86+ \draw (1,3) to (2,3) [oosourcetrans] to (5,3);
87+ \draw [black, ultra thick] (5,2) -- (5,4);
88+ \draw[thick, ->] (5,1.4) +(0.05,0.5) -- +(-0.1,-0.1) -- +(0.1,0.1) -- +(0,-0.5);
89+ ```
90+
91+ IEC 60909 calculation should give $I_k^{\prime\prime} = \frac{u_ {rated-2}}{ \sqrt{3} \cdot (z_k + z_t)}$
92+
93+ PGM calculates short circuit by setting source voltage as $u_ {rated-1}$ instead. Hence
94+ $I_k^{\prime\prime} = \frac{u_ {rated-1} \cdot k}{ \sqrt{3} \cdot (z_k + z_t)}$
95+ where $k =\frac{u1 \cdot u_ {rated-2}}{u2 \cdot u_ {rated-1}} $
96+
97+ When the voltage rating of the transformer matches the rated voltage of the nodes, this factor is exactly ` 1.0 ` .
98+ In radial grids, it can be easily accumulated by multiplying the transformation ratios of all transformers
99+ ($k_ {t1} \cdot k_ {t2} \cdot k_ {t3} ...$) along the fault path to the source.
100+ However, when multiple sources and meshed networks are involved, the calculation becomes complex.
101+ This factor is roughly ` 0.97 ` to ` 1.03 ` on a practical grid.
102+ An easy approach is then to simply leave a margin of ~ ` 1.03 ` in the maximal short circuit current.
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