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Synteza układów kompensacji

CHHTE3 CHCTEM KOMIIEHCAUHtt

AJIA HEKOTOPŁDC KJ1ACCOB TPfiX<J>A3HHX UEIIEfl

P 8 3 B w e

B paÓOTe, Ha ocnoBe opToronajibHoro pasji o*QHna Tona TpexiJ>a3Horo npHSuHHKa b KenoTopoM THJibÓepTOBou npoaTpaaaTBa L^(0;T) aro Tp8x BaanMHo opToroHajnbHHX cjiaraeiibDC npoBOflHTCH chht©3 crpyitryp KouiieHCHpyjoąicc peaKTHBHyD oocTaB^asmyc tokb _r ąjifl Tpex$aaHbtx cKCTeii Óea ojieKTpoiiarHHTHott CBaan, a TaKjce qaaTHmiyD KOMneHcaUHH) ąji& CHOreu c ajieKTpouarHHTHOft CBaabD. Ajia ouohkh CTeneHH KouneHcaij^HH peaKTHBHoro TOKa _pi ■ (_ri_lf rⁱ2^#rⁱ3^ ^e L₃(0|T) bboahtch Koa^HuneHT £ _f 3HaqeHne KOToporo rjul KOHKpeTHboc cipyKTyp onpeAejmeT ąejiecooÓpasHocTb nojmoH KOHneHcaunu aToro Tona.

SYNTHESIS OF COMPENSATION NETWORKS FOR SOME CLASSES OF 3-PHASE NETWORKS

S u m m a r y

The eyntheele of the networks used for the compeneation of the reactance component _ri^ , <*e{l,2,3} of the load current with arbitrary number of harmonice hae been carried out in the paper* The syntheeie ie baeed on the orthogonal decomposition of the current of 3-phaee load in the chooeen Hilbert space L^(0;T) into 3 orthogonal componente* Complete compeneation of the current i. in 3-phaee networks with no magnetic coupling and partial compeneation of the reactance component of _r i^ in 3-phaee networks with magnetic coupling hae been done*

The coefficient E, hae been introducec ae a measure of the degree of compeneation of the reactance current _ri » (_fi_{lf r}ⁱ2^# r¹3^ ^& L₃(0>T) in the networks with magnetic coupling*

The coefficient £ will be ueed for the eetimation of the usefulnese of complete compeneation of thie current*