CS259355B1 - Wiring for real measurements of the AC component - Google Patents
Wiring for real measurements of the AC component Download PDFInfo
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- CS259355B1 CS259355B1 CS853866A CS386685A CS259355B1 CS 259355 B1 CS259355 B1 CS 259355B1 CS 853866 A CS853866 A CS 853866A CS 386685 A CS386685 A CS 386685A CS 259355 B1 CS259355 B1 CS 259355B1
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Abstract
Zapojenie rieši meranie reálnej zložky striedavého prúdu pre potřeby automatizácie technologických procesov. V zapojení je za meracím transformátorom prúdu kondenzátor, ktorý sa spínacími obvodmi zloženými zo spínacích diód, kondenzátorov a odporov nabíja na napatie úměrné reálnej zložke meraného prúdu.The circuit solves the measurement of the real component of alternating current for the needs of automation of technological processes. In the circuit, there is a capacitor after the measuring current transformer, which is charged to a voltage proportional to the real component of the measured current by switching circuits consisting of switching diodes, capacitors and resistors.
Description
259355259355
Vynález rieši meranie reálnej zložky e-lektrickěho striedavého prúdu jednoduchý-mi pasivnými obvodovými prvkami.The invention solves the measurement of the real component of the electric alternating current by simple passive circuit elements.
Doteraz sa reálna zložka prúdu meralavýchylkovými meracími prístrojmi, alebozložitými elektronickými zariadeniami pra-cujúcimi na principe vzorkovania vysokoufrekvenciou alebo spínanými odporovýmimostikmi. Výchylkové meracie přístroje sanedajú použit v automatickej regulácii, le-bo ich výstupom nie je elektrický signál. E-lektronické zariadenia sú zložité, rozměrnéa drahé. Meranie špinavými odporovýmimostikmi je zatažené chybou vznikajúcounelineárnou indukčnou záťažou.Until now, the real component of the current is a meter-based measuring instrument, or a complex electronic device operating on the principle of high-frequency or switched resistivity. The displacement measuring devices are used in automatic control as their output is not an electrical signal. Electronic devices are complex, expensive and expensive. The measurement by dirty resistance pulses is overridden by an error resulting from a linear inductive load.
Uvedené nedostatky odstraňuje zapojeniepodl'a vynálezu, ktorého podstata spočívá vtom, že do obvodu meraného prúdu je zapo-jený merací transformátor prúdu. Tentotransformátor je zatažený záťažným odpo-rom. Prvá svorka merácieho transformáto-ra je cez kondenzátor spojená s prvou vý-stupnou svorkou zapojenia. Druhá svorkamerácieho transformátora je priamo spoje-ná s druhou výstupnou svorkou zapojenia asúčasne so střednou svorkou napáťovéhotransformátora. Prvá výstupná svorka za-pojenia je cez prvú spínaciu diodu a para-lelné spojený druhý odpor s druhým kon-denzátorom spojená s prvou svorkou napa-ťového transformátora. Súčasne je prvávýstupná svorka zapojenia cez druhů spína-ciu diodu a paralelné spojený třetí odpors třetím kondenzátorom spojená s druhousvorkou napaťového transformátora. Výhody zapojenia podl'a vynálezu spočí-vajú v tom, že zapojenie je jednoduché anenáročné na súčiastky. Náklady na jehozhotovenie sú nízké. Tým, že zariadenievzorkuje prúd v čase, keď reaktačná zlož-ka prúdu je nulová, neovplyvňuje meraniejej nelinearita. Jednoduchost zapojenia adobrá kvalita výstupného signálu umožňu-jú aplikovat zapojenie v automatizácii a re-gulácii technologických procesov.The above mentioned drawbacks are eliminated by the connection of the invention, the principle being that a current measuring transformer is connected to the circuit of the measured current. This transformer is retracted by a load resistor. The first measuring transformer terminal is connected via a capacitor to the first output terminal of the connection. The second terminal transformer is directly connected to the second output terminal of the connection and simultaneously to the middle terminal of the transformer. The first output terminal of the connection is connected to the first terminal of the voltage transformer via a first switching diode and a parallel second second resistor to a second capacitor. At the same time, the first input terminal of the connection is a switching diode and a parallel connected third resistor through the third capacitor connected to the second terminal of the voltage transformer. Advantages of the connection according to the invention are that the connection is simple and not expensive for the components. The cost of making it is low. By plotting the current at a time when the reactant component of the current is zero, the device does not affect the measurement non-linearity. The simplicity of connection and the good quality of the output signal make it possible to apply wiring in automation and regulation of technological processes.
Na pripojenom výkrese je schéma zapoje-nia.In the attached drawing, there is a wiring diagram.
Prvá sekundárná svorka 11 meráciehotransformátoru 1 je cez kondenzátor C3 spo-jená s výstupnou svorkou 16 zapojenia. Dru-há sekundárná svorka 12 merácieho trans-formátora 1 je priamo spojená s druhou vý-stupnou svorkou 17 zapojenia a súčasne sostřednou svorkou 16 napaťového transfor-mátora 10. Prvá výstupná svorka 16 zapoje- nia je cez prvú spínaciu diodu 4 a paralel-né spojený druhý odpor R6 s druhým kon-denzátorom C8 spojená s prvou svorkou 14napaťového transformátora 10. Súčasne je prvá výstupná svorka 16 za-pojenia cez druhů spínaciu diodu 5 a para-lelné spojený třetí odpor R7 s třetím kon-denzátorom C9 spojená s druhou svorkou15 napaťového transformátora 10.The first secondary terminal 11 of the transformer 1 is coupled via the capacitor C3 to the output terminal 16 of the transformer. The second secondary terminal 12 of the measuring transformer 1 is directly connected to the second output terminal 17 of the wiring and simultaneously the center terminal 16 of the voltage transformer 10. The first output terminal 16 of the wiring is via the first switching diode 4 and parallel the second resistor R6 coupled to the second capacitor C8 coupled to the first terminal 14 of the voltage transformer 10. At the same time, the first output terminal 16 of the connection through the types is a switching diode 5 and a parallel third resistor R7 with a third capacitor C9 connected to the second terminal 15 voltage transformer 10.
Meraný prúd pretransformovaný meracímtransformátorom 1 vytvoří na zátažnom od-pore R2 zapojenom medzi svorky 11, 12 me·racieho transformátora 1 úbytok napátia ú-merný velkosti meraného prúdu. Vzorkomtohto napátia sa v čase maxima referenčné-ho napátia na napáťovom transformátore10 nabíja kondenzátor C3. Spínací obvodpre nabíjanie kondenzátora C3 tvoria spína-cie diody 4, 5, ktoré sú na krátký čas otvá-rané referenčným napátím zo svierok 13, 14a 14, 15 napaťového transformátora 10. Ot-váranie spínacích diód 4, 5 v okamihu ma-xima referenčného napátia zabezpečuje pro-tinapátie vznikajúce na kondenzátoroch C8,C9. Pomalé vybíjanie týchto kondenzátorovC8, C9 zabezpečujú odpory R6, R7. Vzorkanapátia, na ktorú sa nabíja kondenzátor C3je úměrná okamžitej hodnotě meraného prú-du v čase maxima referenčného napátia. Akreferenčně napátie je vo fáze s reálnouzložkou meraného prúdu a reálna zložkameraného prúdu má sinusový priebeh, takjednosměrné napátie na kondenzátore C3 jeprávě úměrné reálnej zložke meraného prú-du. Na výstupné svorky 16, 17 zapojenia sapripája analogovo digitálny převodník ale-bo regulačný obvod zo vstupným ^odporomR1S. Aby zariadenie podlá zapojenia spo-1'ahlivo fungovalo, musia hodnoty jeho ob-vodových prvkov splňať následovně pod-mienky: C3 C8C8 = C9R6 = R7 C3 . R18 > R6 . C8 > —- > C3 . R2 ω kde ω je kruhová frekvencia meraného prú-du.The measured current transformed by the measurement transformer 1 produces a voltage drop across the measuring resistor R2 connected between the measuring transformer terminals 11, 12, which is a measure of the measured current. The capacitance C3 is charged at the voltage reference voltage across the voltage transformer 10 at this time. The switching circuit for charging the capacitor C3 consists of switching diodes 4, 5, which are opened for a short time by a reference voltage from clamps 13, 14a 14, 15 of the voltage transformer 10. Opening of the switching diodes 4, 5 at the moment of reference reference the tension is provided by the capacitance generated by the capacitors C8, C9. Slow discharge of these capacitors C8, C9 provide resistors R6, R7. The sample voltage to which the capacitor C3 is charged is proportional to the instantaneous value of the measured current at the time of the maximum reference voltage. The accretion voltage is in the phase with the real component of the measured current and the real compound current is sinusoidal, so the unidirectional voltage on capacitor C3 is proportional to the real component of the measured current. An analog-to-digital converter or a control circuit with an input resistor R1S connects to the output terminals 16, 17. In order for the device to function reliably according to the connection, the values of its circumferential elements must satisfy the following conditions: C3 C8C8 = C9R6 = R7 C3. R18> R6. C8> -> C3. R2 ω where ω is the circular frequency of the measured current.
Zapojenie je vhodné aj pre meranie l'ubo-volných vektorových zložiek prúdu, ak dosměru vektoru meraného prúdu natočímefázovacím článkom vektor referenčného na-pátia.The connection is also suitable for measuring the free vector components of the current and for measuring the vector of the measured current by turning the reference vector of the reference vector.
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CS853866A CS259355B1 (en) | 1985-05-30 | 1985-05-30 | Wiring for real measurements of the AC component |
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CS853866A CS259355B1 (en) | 1985-05-30 | 1985-05-30 | Wiring for real measurements of the AC component |
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CS386685A1 CS386685A1 (en) | 1988-03-15 |
CS259355B1 true CS259355B1 (en) | 1988-10-14 |
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CS853866A CS259355B1 (en) | 1985-05-30 | 1985-05-30 | Wiring for real measurements of the AC component |
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1985
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