Read e-book online Analysis and Damping Control of Power System Low-frequency PDF

By Haifeng Wang, Wenjuan Du

ISBN-10: 1489976949

ISBN-13: 9781489976949

ISBN-10: 1489976965

ISBN-13: 9781489976963

This e-book provides the examine and improvement effects on strength structures oscillations in 3 different types of analytical tools. First is damping torque research which was once proposed in 1960’s, extra constructed among 1980-1990, and typical in undefined. moment is modal research which constructed among the 1980’s and 1990’s because the strongest procedure. ultimately the linearized equal-area criterion research that's proposed and constructed lately. The e-book covers 3 major forms of controllers: strength approach Stabilizer (PSS), evidence (Flexible AC Transmission structures) stabilizer, and ESS (Energy garage platforms) stabilizer. The ebook presents a scientific and certain advent at the topic because the reference for purposes and educational learn.

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Extra info for Analysis and Damping Control of Power System Low-frequency Oscillations

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3 wTi3 bpssÀ3 vi2 aT  i2 vi2 23À8 Àw M 2 3 vi1 6 7 0 Š4 vi2 5 vi3 ð2:83Þ i I À A33 ÞÀ1 bpssÀ3 ðk Design of PSS by Pole Assignment If the feedback signal and transfer function of the PSS to be designed is y and TPSS ðsÞ respectively, Eq. 78) can be written more generally as follows: sX ¼ AX þ bDupss y ¼ cT X Dupss ¼ Tpss ðsÞy ð2:84Þ Transfer function of open-loop system is as follows: GðsÞ ¼ cT ðsI À AÞÀ1 b ð2:85Þ Characteristic equation of closed-loop control system is as follows: 1 þ GðsÞTpss ðsÞ ¼ 0 ð2:86Þ If design of the PSS is to assign the electromechanical oscillation mode of the c ¼ Àn Æ jxc , single-machine infinite-bus power system to a target position, k c  kc must be the solution of the characteristic equation of closed-loop control system of Eq.

2 ð2:30Þ A Simplified Model of Single-Machine Infinite-Bus Power System For the single-machine infinite-bus power system shown in Fig. 6, from Eqs. 28), it can have vtd ¼ vd À xt iq ¼ xq iq vtq ¼ vq þ xt id ¼ Eq À xd id ¼ E0q À x0d id ð2:31Þ Thus, vd ¼ ðxt þ xq Þiq ¼ xqR iq vq ¼ Eq À ðxd þ xt Þid ¼ E0q À ðx0d þ xt Þid ¼ Eq À xdR id ¼ E0q À x0dR id ð2:32Þ 2 A Single-Machine Infinite-Bus Power System … 28 Fig. 8 Equivalent circuit model of single-machine infinite-bus power system id iq + + x dΣ (x dΣ ') x qΣ vq vd Eq (Eq ') d winding - Fig.

26) together with Eq. 3) forms the simplified third-order model of synchronous generator. 2) becomes wd ! xd xad ¼ wf xad xf wq ¼ Àxq iq ! Àid ! if ð2:27Þ From Eqs. 27), it can have vtd ¼ Àwq ¼ xq iq vtq ¼ wd ¼ xad if À xd id ¼ Eq À xd id ð2:28Þ From Eqs. 27), it can be obtained that E0q ¼ À Á xad xad x2 wf ¼ ðxf if À xad id Þ ¼ Eq À ad id ¼ Eq À xd À x0d id xf xf xf ð2:29Þ x2 where x0d ¼ xd À xadf , which is called the transient d-axis reactance. Thus, Eq. 2 ð2:30Þ A Simplified Model of Single-Machine Infinite-Bus Power System For the single-machine infinite-bus power system shown in Fig.

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Analysis and Damping Control of Power System Low-frequency Oscillations by Haifeng Wang, Wenjuan Du


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