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[PSA] Chapter 8 - Generator Modeling

8.0 Introduction

  • Exciter : complete voltage control system, including an error detector, feedback loop, automatic voltage regulator(AVR)

8.1 Exciter System Block Diagram

Measurement block

  • Gain of measurement block is unity in steady-state

Amplifier block

  • Amplifier gain $K_A$ is typically in the range 25 to 400
  • $T_A$ in range 0.02 to 0.4 sec
  • Amplifier voltage has limitations (exciter field winding can supply limited voltage)

Exciter block

  • Voltage of dc generator is proprotional to product of speed times air-gap flux per pole
  • Due to saturation effect of magnetic circuit, the flux is a nonlinear function of dc generator field current

  • Consider inverse-relationship between $v_F $ and $i$
\[i = i_0 + f(v_F) = {1\over k} v_F + f(v_F) \tag{8.1}\] \[v_R = Ri + {d\lambda \over dt}\]
  • Assume that dc generator output voltage $v_F$ is proportional to dc generator air-gap flux,
\[v_F = \beta\lambda\]
  • We can get following equation by converting $v_F$ into $E_{fd}$
\[v_R = E_{fd} + E_{fd}S_E(E_{fd})+T_E{dE_{fd} \over dt}\]

Where $T_E \triangleq k/R\beta, S(v_F) \triangleq kf(v_F)/v_F$, Saturation function

8.2 Generator Models

Case I : Open Circuit

  • $I_a = 0$, we have $E’_a = E_a = V_a$
  • Recall relationship between $E’_a $ and $E_{fd}$
\[T'_{do} {d\vert E'_a \vert \over dt} + \vert E_a \vert = E_{fd}\]

We can substitute $E’_a $ with $E_a$

Can get transfer function

\[G_g(s) = {\vert \hat V_a\vert \over \hat E_{fd}}={1\over 1+sT'_{do}}\]

Case II : Impedance Load

  • Assume that isolated generator supplying an impedance load $Z$.
  • By considering relationships,
\[\vert E_a \vert = {1\over \sigma} \vert E_a' \vert \tag {8.13}\]

For inductive loads, $\sigma<1$

Can get desired transfer function by defining some auxiliary variables

\[G_g(s) = {k_v\sigma \over 1+s\sigma T'_{do}}\]

Where $k_v \triangleq \vert Z \vert \vert K \vert$, $K \triangleq K_q+jK_d$, $I_d = K_d\vert E’_a \vert, I_q = K_q\vert E’_a \vert$

8.3 Stability of Excitation System

  • higher loop gain → smaller voltage error
  • but consequently excitation system can be unstable
  • Solution : add rate feedback to exciter
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