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Function of excitation system and its transfer function

Short answer

The excitation system supplies DC field current, regulates terminal voltage, controls reactive power, and improves stability. With stabilizing transformer, Vt/Vref = K_AK_EK_G(1+sTF) / [(1+sTA)(1+sTE)(1+sTG)(1+sTF) + sKF K_AK_E(1+sTG) + K_AK_EK_G(1+sTF)].

What is the function of excitation system in generating station? Derive the transfer function of an excitation system with stabilizing transformer.

Function of excitation system

The excitation system supplies and controls the DC field current of a synchronous generator. Its functions are:

  • Supply DC current to the rotor field winding to produce the main flux.
  • Keep the terminal voltage constant as load changes (automatic voltage regulation).
  • Control the reactive power (VAr) output and share it correctly among parallel generators.
  • Improve transient and steady-state stability by fast field forcing during faults.
  • Provide protective limits (over/under-excitation limiters, V/Hz limiter).

Transfer function with stabilizing transformer

The system has four blocks: amplifier, exciter, generator field and a stabilizing transformer that feeds back the rate of change of exciter voltage to damp oscillations.

Vref +  e   +   +-----------+    +---------+  Efd
 --->(Σ)-->(Σ)-->| Amplifier |--->| Exciter |--+--+
      ^-    ^-   +-----------+    +---------+  |  |
      |     |     +---------------+            |  |
      |     +-----| Stab. transf. |<-----------+  |
      |           +---------------+               |
      |   Vt      +-----------+                   |
      +-----------| Generator |<------------------+
                  +-----------+

1. Amplifier: VR(s)Ve(s)=KA1+sTA\dfrac{V_R(s)}{V_e(s)} = \dfrac{K_A}{1+sT_A}

2. Exciter (field ReR_e, LeL_e; Efd=KieE_{fd} = K i_e): from vR=Reie+Lediedtv_R = R_e i_e + L_e \frac{di_e}{dt},

Efd(s)VR(s)=K/Re1+s(Le/Re)=KE1+sTE\frac{E_{fd}(s)}{V_R(s)} = \frac{K/R_e}{1+s(L_e/R_e)} = \frac{K_E}{1+sT_E}

3. Generator field (open circuit): Vt(s)Efd(s)=KG1+sTG\dfrac{V_t(s)}{E_{fd}(s)} = \dfrac{K_G}{1+sT_G}

4. Stabilizing transformer: primary (R1R_1, L1L_1) is across the exciter output; secondary (mutual inductance MM) is practically open-circuited by the high-impedance amplifier input.

Efd=R1i1+L1di1dt  ⇒  I1(s)=Efd(s)R1(1+sTF)VF=Mdi1dt  ⇒  VF(s)Efd(s)=sKF1+sTF\begin{aligned} E_{fd} &= R_1 i_1 + L_1 \frac{di_1}{dt} \;\Rightarrow\; I_1(s) = \frac{E_{fd}(s)}{R_1(1+sT_F)} \\ V_F &= M\frac{di_1}{dt} \;\Rightarrow\; \frac{V_F(s)}{E_{fd}(s)} = \frac{sK_F}{1+sT_F} \end{aligned}

where KF=M/R1K_F = M/R_1 and TF=L1/R1T_F = L_1/R_1.

5. Closed loop. Let G1=KAKE(1+sTA)(1+sTE)G_1 = \dfrac{K_A K_E}{(1+sT_A)(1+sT_E)}, HF=sKF1+sTFH_F = \dfrac{sK_F}{1+sT_F}, G2=KG1+sTGG_2 = \dfrac{K_G}{1+sT_G}. The minor loop gives G11+G1HF\dfrac{G_1}{1+G_1H_F}; with unity voltage feedback:

Vt(s)Vref(s)=G1G21+G1HF+G1G2\frac{V_t(s)}{V_{ref}(s)} = \frac{G_1G_2}{1+G_1H_F+G_1G_2}

Substituting and clearing fractions:

Vt(s)Vref(s)=KAKEKG(1+sTF)(1+sTA)(1+sTE)(1+sTG)(1+sTF)+sKFKAKE(1+sTG)+KAKEKG(1+sTF)\frac{V_t(s)}{V_{ref}(s)} = \frac{K_AK_EK_G(1+sT_F)}{(1+sT_A)(1+sT_E)(1+sT_G)(1+sT_F) + sK_FK_AK_E(1+sT_G) + K_AK_EK_G(1+sT_F)}

The sKFsK_F term adds damping, so a high loop gain (small steady-state error) can be used without oscillation.

✓ Answer checked by Claude Opus 5.5 (high effort)

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