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GridKit/Model/PhasorDynamics/Exciter Expand file tree Collapse file tree Original file line number Diff line number Diff line change @@ -127,6 +127,17 @@ and when both saturation values are positive,
127127\end{aligned}
128128```
129129
130+ During initialization, the effective
131+ exciter constant is derived from the initial operating point:
132+
133+ ``` math
134+ K_E^{\mathrm{eff}} =
135+ \begin{cases}
136+ \dfrac{V_R^{\max}/10-s_e}{E_{\mathrm{fd}}'} & K_E=0 \\
137+ K_E & K_E\ne 0.
138+ \end{cases}
139+ ```
140+
130141## Model Ports
131142
132143Name | Port | Init | Description
@@ -317,12 +328,6 @@ routed through the gate:
317328 \dfrac{E_{\mathrm{fd}}}{1 + s_{\mathrm{spd}}\omega} \\
318329 s_e
319330 &\leftarrow S_B q\left(E_{\mathrm{fd}}' - S_A\right) \\
320- K_E^{\mathrm{eff}}
321- &\leftarrow
322- \begin{cases}
323- \dfrac{V_R^{\max}/10-s_e}{E_{\mathrm{fd}}'} & K_E=0 \\
324- K_E & K_E\ne 0
325- \end{cases} \\
326331 V_{\mathrm{FE}}
327332 &\leftarrow K_E^{\mathrm{eff}} E_{\mathrm{fd}}' + s_e \\
328333 V_R
Original file line number Diff line number Diff line change @@ -102,6 +102,17 @@ When both saturation values are positive, the non-extraneous solution is:
102102\end{aligned}
103103```
104104
105+ During initialization, the effective
106+ exciter constant is derived from the initial operating point:
107+
108+ ``` math
109+ K_E^{\mathrm{eff}} =
110+ \begin{cases}
111+ \dfrac{V_R^{\max}/10-k_\text{sat}}{E_{fd}'} & K_E=0 \\
112+ K_E & K_E\ne 0.
113+ \end{cases}
114+ ```
115+
105116## Model Variables
106117
107118### Internal Variables
@@ -201,11 +212,6 @@ with the current input values.
201212 E_{C,0} &:= \sqrt{V_r^2 + V_i^2} \\
202213 E_{fd}' &= \dfrac{E_{fd,0}}{1 + I_{\mathrm{spdlim}}\,\omega} \\
203214 k_\text{sat} &= S_B\, q(E_{fd}' - S_A) \\
204- K_E^{\mathrm{eff}} &\leftarrow
205- \begin{cases}
206- \dfrac{V_R^{\max}/10-k_\text{sat}}{E_{fd}'} & K_E=0 \\
207- K_E & K_E\ne 0
208- \end{cases} \\
209215 V_E &= k_\text{sat} \\
210216 V_R &= K_E^{\mathrm{eff}} E_{fd}' + V_E \\
211217 V_{tr} &= \dfrac{V_R}{K_A} \\
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