文獻(xiàn)翻譯 組合數(shù)字電子式電流和電壓傳感器.doc
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1、 黃河科技學(xué)院畢業(yè)設(shè)計(jì)(文獻(xiàn)翻譯) 第21頁 組合數(shù)字電子式電流和電壓傳感器 作者:段雄英、鄒積巖、廖敏夫、張可衛(wèi) 摘 要 在電力系統(tǒng)中已開發(fā)出高性能的電流和電壓測量系統(tǒng)。該系統(tǒng)由兩部分組成:電流測量元件和電壓測量元件。洛高夫斯基線圈和電容分壓器分別用于為線電流和電壓測量。有源電子元件是電流互感器進(jìn)行在線檢測時(shí)為這些組件信號(hào)調(diào)制并提供電源的。測量信號(hào)通過光纖傳輸,光纖可以抗電磁干擾和噪聲干擾。通過精細(xì)的設(shè)計(jì)和對(duì)數(shù)字信號(hào)處理技術(shù)的應(yīng)用,整個(gè)系統(tǒng)的精度可以達(dá)到0.5%,配以高精度的供繼電保護(hù)設(shè)備可提供較大范圍的動(dòng)態(tài)檢測。 關(guān)鍵
2、詞:電子式電流傳感器(ECT),電子電壓互感器(EVT),洛高夫斯基(Rogowski)線圈,電容分壓器(CVD),光纖 1 簡 介 電流和電壓測量在測光、保護(hù)和電力系統(tǒng)控制中起著重要作用。隨著電力系統(tǒng)的發(fā)展,傳統(tǒng)的電流互感器(CT)和電壓互感器(PT)有著不能容忍的缺點(diǎn):絕緣結(jié)構(gòu)成本高且模式復(fù)雜,CT的飽和效應(yīng)和PT的鐵磁諧振效應(yīng)等影響。在過去的二十年中,大多興趣投入在光學(xué)電流互感器(OCT)和光學(xué)電壓互感器(OPT)的研究中。最常見的類型有利用法拉第效應(yīng)的OCT和利用普克爾斯效應(yīng)的OPT,它們都是使用光學(xué)晶體的傳感器。盡管一些成功的現(xiàn)場試驗(yàn)已經(jīng)完成,但在商業(yè)產(chǎn)品中OCT和OPT還不能
3、實(shí)現(xiàn)量產(chǎn),因?yàn)镺CT和OPT很容易受到環(huán)境溫度和機(jī)械擾動(dòng)[1~3]。近年來,麗思(Ritz)公司開發(fā)的以結(jié)合電子式電流和電壓傳感器利用洛高夫斯基(Rogowski)線圈和電容分壓器分別作為傳感器線電流和電壓測量[4]。基于這一概念,一種新型電流和電壓測量數(shù)字系統(tǒng)被開發(fā)出來了。 2 系統(tǒng)結(jié)構(gòu) 數(shù)字電流互感器的概念已經(jīng)提出了近半個(gè)世紀(jì),但因電子元件及常規(guī)繼電保護(hù)和測光模式的限制使其沒有得到很好的發(fā)展。可是現(xiàn)在基于數(shù)字技術(shù)及信息網(wǎng)絡(luò)的繼電保護(hù)和獨(dú)占地測光系統(tǒng)操作正在被廣泛應(yīng)用于配電系統(tǒng)。各種具有特殊功能的集成芯片投入市場。所有這些都可能使電子CT和PT產(chǎn)品基于數(shù)字調(diào)制。 合并后的電流和電壓測量
4、系統(tǒng)框圖如圖1所示。洛高夫斯基(Rogowski)線圈是用于使電流測量和電力CT符合電力線的。洛高夫斯基(Rogowski)線圈納入有源電子元件組成了整個(gè)電流變送器。這種發(fā)射器生成信息描述性測量電流和光信號(hào)編碼。整個(gè)電流發(fā)射器和電源部分都被放到一個(gè)抗電磁干擾(EMI)的鐵盒中。空心陶瓷絕緣體用于維持系統(tǒng)的高電壓的一部分。無論是光纖承載的電流信號(hào)還是電容分壓器都為通過絕緣體的電壓傳感器使用。電容分壓器的電壓信號(hào)也在絕緣體的底部調(diào)制成光信號(hào)。接著電流信號(hào)和電壓信號(hào)通過光纖傳輸?shù)綔y光和繼電保護(hù)遠(yuǎn)程控制室內(nèi)。 圖1 組合電子式電流和電壓測量系統(tǒng) 3 電流和電壓傳感器 在此,提出了一種洛高夫斯
5、基(Rogowski)線圈式電流傳感器。Rogowski線圈,這是一個(gè)電感無磁環(huán)形口,已用于測量電流一段時(shí)間[5]。圖2所示為一個(gè)矩形截面Rogowski線圈。 Rogowski線圈是基于載流導(dǎo)體的放置,線圈產(chǎn)生一個(gè)電壓E成正比,線圈交互M和電流變化的的速度為: (1) 由式(1)得: (2) 要獲取電流測量值,線圈的輸出電壓必須是完整的。這可以通過兩種常見的方法:(1)電子積分器的使用;(
6、2)在使用數(shù)值積分軟件之后線圈的輸出電壓是數(shù)字化的。本文圖3所示為積分器。該積分器的輸出為: (3) 其中,Vi是Rogowski線圈的輸出從目前可以得到以下等式: (4) 因?yàn)闆]有鐵芯飽和,Rogowski線圈有廣泛的測量范圍。同樣的線圈可用于測量從幾安培至數(shù)百千安培的電流。此外,他們具有較高的測量精度,也就是說可以精確至0.1%[6],而且它對(duì)溫度不敏感。電容分壓器(CV
7、D)技術(shù)已被廣泛應(yīng)用于高壓電力系統(tǒng)。影響CVD測量精度的主要因素是雜散電容和電容的溫度系數(shù)。精密電容分壓器技術(shù)用于提高測量精度。有效減小雜散電容的方法是全速淡化分頻器高度。本文中,主要是以充滿絕緣油的絕緣體來盡量減少它的高度。通過這種方法,雜散電容分壓器可以保持在較低水平,且位于高壓臂中的具有相同的溫度特性的串聯(lián)電容器可以被大大改善。分壓器終端置頂一個(gè)屏蔽電極以補(bǔ)償雜散電容的影響。 將電子電壓互感器(EVT)中CVD放在室外,強(qiáng)烈的溫度變化可能影響分壓器的誤差。正如微處理器基礎(chǔ)系統(tǒng)中的傳感器一樣,在EVT中的CVD是不同于常規(guī)CVD的。因其負(fù)荷小的特點(diǎn),故如圖4所示,特殊結(jié)構(gòu)的CVD可以消除
8、溫度的影響。 分壓器是由具有相同的電介質(zhì)、規(guī)模、價(jià)值和溫度系數(shù)的m+n個(gè)電容器Ci組成的。m個(gè)電容器串聯(lián)在系統(tǒng)中的值C1得滿足高壓臂中的要求:,低壓臂中的電容值C2 是由并聯(lián)電路得出的C2=nCi, 那么分壓比K″為: (5) 電容值C1由于溫度變化變?yōu)镃i +ΔC1,這時(shí)分壓比K″是: K″=C1/(C1+C2) =(1/m)(Ci+ΔC1)/[(1/m)(Ci+ΔC1)+n(Ci+ΔC1)] =1/(mn
9、+1) (6) 由式5和式6可知K= K″,通過這種方式,所有具有相同參數(shù)的電容Ci都可以消除溫度對(duì)分頻比率的影響。 4 信號(hào)處理 如圖5所示為一個(gè)信號(hào)處理框圖?,F(xiàn)在市場上發(fā)售有許多特殊的A / D芯片在。有多種方式可以從一個(gè)遠(yuǎn)程發(fā)射點(diǎn)傳達(dá)測量信息。電壓頻率調(diào)制是一個(gè)純粹的數(shù)字技術(shù),它可以提供無差錯(cuò)和無干擾的傳輸,因此,最適合在電力系統(tǒng)中使用。這項(xiàng)技術(shù)的基本概念是把測量信號(hào)轉(zhuǎn)換成PFM(脈沖頻率調(diào)制)信號(hào),其測量信號(hào)的頻率偏差與電流或電壓的大小成線性正比。 圖5 信號(hào)處理系統(tǒng) 式7闡述了這種關(guān)系:
10、 (7) 其中F0 是輸入直流電壓偏移設(shè)置的基本頻率,系數(shù)k是取決于實(shí)際電路。 LED(發(fā)光二極管低)直接由頻率脈沖驅(qū)動(dòng),然后信號(hào)調(diào)制成光脈沖。與LED匹配的光纖傳輸窗口具有850nm的中心波長。200μm多模光纖用來傳輸光信號(hào)。控制室接收器是一個(gè)光電二極管,即用于重建電頻率脈沖的驅(qū)動(dòng)放大器,之后把頻率信號(hào)發(fā)送到計(jì)算機(jī)用于解調(diào)。 由時(shí)間到其實(shí)是一個(gè)完整的頻率信號(hào)計(jì)數(shù)過程,并且計(jì)數(shù)值Y j i 為: Yji 是由計(jì)數(shù)器獲取的,所以:
11、 (8) 式8是由到的輸入脈沖信號(hào)的積分值, 它等于由信號(hào)曲線包圍的面積值。如果輸入信號(hào)的微小變化保持在與 之間, 或者采樣時(shí)間=–足夠短,其點(diǎn)的值可以是一個(gè)近似值。 (9) 由式8和9,我們可以得到: (10) 整合延遲效果所造成的錯(cuò)誤,可以通過軟件進(jìn)行修改。由于該系統(tǒng)采用光纖傳輸數(shù)字信號(hào),所以它是抗電磁干擾。 5 線電位編碼器電源 使用光纖實(shí)現(xiàn)高低電壓間的絕緣,但在高電壓上仍有些電源問題。有三
12、種方法可以設(shè)計(jì)一個(gè)電流驅(qū)動(dòng)的電力供應(yīng):電池,電流互感器,和光功率。常見的是電池的工作壽命為5?10年,平均修復(fù)時(shí)間為3年,動(dòng)力系統(tǒng)中是不行的。更重要的是,大尺寸的電池和其復(fù)雜的浮點(diǎn)充電電路是不可取的。一些先進(jìn)的電池成本高,如鋰或光電池成為應(yīng)用的障礙。在此提出了一種特殊設(shè)計(jì)的輔助CT是用來直接從生產(chǎn)線上獲取能量的。這種高壓CT的絕緣要求要比那些常規(guī)CT更簡單,并且輸出功率低,所以它比常規(guī)CT要小的多。 在電源CT設(shè)計(jì)中應(yīng)該考慮兩個(gè)關(guān)鍵問題。首先,電力CT應(yīng)為線電流盡提供可能低的所需的電壓和電流,也就是,在該系統(tǒng)運(yùn)行中實(shí)測線電流有一個(gè)最低值。其次,在故障電流中,電源CT能吸收多余的能量成為供應(yīng)電
13、子元器件的穩(wěn)定力量,且其本身不會(huì)被電場力所破壞。該電源系統(tǒng)的示意圖如圖6所示。從圖6,我們可以得到的: (11) 其中,Z0---控制阻抗,Z1----負(fù)載阻抗,I---線電流, ---負(fù)載電壓。 為了使負(fù)載電壓是常量,那么Z0必須隨線電流I的變化而變化,也就是說,如果我們能夠設(shè)計(jì)出隨線電流I變化的控制阻抗電路,我們可以得到一個(gè)穩(wěn)定的高能量輸出功率的電子元件。圖7說明了電源的設(shè)計(jì)運(yùn)行原則。能量由電源CT獲得。起初,電源穩(wěn)壓電路是唯一施加在電源變壓器的次級(jí)繞組的負(fù)載。當(dāng)所有的穩(wěn)壓電源電壓是指定的值時(shí),
14、當(dāng)前分支電路是停止電力供應(yīng)的進(jìn)一步補(bǔ)充。通過這種設(shè)計(jì)方法,該系統(tǒng)可以正常工作在5%到20的額定電流(400A)。 6 系統(tǒng)性能 用綜合電子式電流和電壓傳感器的單導(dǎo)線施工原型為110KV電力系統(tǒng)進(jìn)行測試,初步測試結(jié)果概述如下:電子式電流傳感器在室溫下的比率的誤差特性如圖8所示。 縱軸表示比率誤差,而橫軸表示初級(jí)電流流向?qū)w。這一數(shù)字表明RMS(均方根方)的光接口輸出波形的值和初級(jí)電流作為衡量一個(gè)0.2級(jí)線圈型CT的RMS的波形的值的關(guān)系。Rogowski線圈的輸出設(shè)計(jì)為400mV相對(duì)應(yīng)的初級(jí)電流400 A 的變動(dòng)率,和積分器的參數(shù)為:R= 10kΩ的中,C =0.1μF的。由數(shù)字可以看
15、出ECT的比率誤差范圍為1.0%。如上所述,通過軟件解調(diào)信號(hào),可以很方便地利用數(shù)字信號(hào)處理技術(shù)進(jìn)行錯(cuò)誤修改,并有望獲得更高的測量精度為0.5%。測量電流的相位誤差要好于20分鐘時(shí)電流過載50Hz的20%。圖9顯示電壓傳感器的測試結(jié)果。無論是高壓電容器系列和低電壓電容器聚丙烯電容器。該測試是在室溫下執(zhí)行的。這一數(shù)字表明在控制室的光纖接口輸出波形的RMS值和0.2級(jí)標(biāo)準(zhǔn)常規(guī)PT的高電壓波形的RMS值的關(guān)系??v坐標(biāo)軸表示低電壓,而橫坐標(biāo)軸表示高電壓。該電子電壓傳感器的線性測量滿足該測量系統(tǒng)精度的0.5%,當(dāng)電壓超過20%的滿量程時(shí),電壓的相位誤差要好于30分鐘的時(shí)候。 7 結(jié)束語 一個(gè)組合數(shù)字電
16、子電流和電壓測量系統(tǒng)相比與常規(guī)的CTs和PTs具有許多優(yōu)點(diǎn)。這些可以概括如下: (1) 高測量精度Rogowski線圈和精密電容分壓器可以通過軟件很方便的修改錯(cuò)誤。且該系統(tǒng)預(yù)計(jì)將擁有0.5%的精確度。 (2) 具有較寬的測量范圍和頻率范圍。因?yàn)闆]有鐵飽和 ,Rogowski線圈不直接測量電流,而不像CTs那樣,當(dāng)一個(gè)大的DC元件存在時(shí),可以精確地測量電流。 (3) 電流和電壓測量組合結(jié)構(gòu)體積小,重量輕,絕緣結(jié)構(gòu)簡單。 (4) 光纖高電壓具有電鍍絕緣帶。這構(gòu)成了可靠的低成本絕緣非接觸式測量系統(tǒng)和強(qiáng)大的抗電磁干擾性。 (5) 系統(tǒng)的溫度特性決定于該電子元件溫度敏感性,先進(jìn)的產(chǎn)品都小于
17、 5010-6/℃。 (6) 目前已開發(fā)增加相容性的新的電子繼電器和測光設(shè)備。未來工作重心著手將組合數(shù)字電流和電壓測量系統(tǒng)投入實(shí)際應(yīng)用中。 參考文獻(xiàn) [1]The Emerging Technologies Working Group. Optical current transducers for power systems: A review[J].IEEE Transactions on Power Delivery,1994,9(4):1778-1788. [2]Maffetone T D, McClelland T M.345kV Substation opti
18、cal current measurement system for revenue metering and protective relaying[J].IEEE Transactions on Power Delivery,1991,6(4):1430-1436. [3]Christensen Lars H. Design construction and test of a passive optical prototype high voltage instrument transformer [J].IEEE Trans. on PD,1995,10(3):1332-1337.
19、 [4]Instruction Book of Sensors [ M]. RITZ Messwandler Hamburg, Germany, Mar.1999. [5]Ramboz John D. Machinable Rogowski coils, design and calibration[J].IEEE Transactions on instrumentation and Measurement,1996,45(2):511-515. [6]Ljubomir Kojovic. Rogowski coils suit relay protection and measureme
20、nt[J].IEEE Computer Application in Power,July1997:47-52. 來源于:上海大學(xué)學(xué)報(bào)(英文版),2002,6(1):79?84 (黃河科技學(xué)院主頁 圖書館 維普期刊 搜索關(guān)鍵字 digital electric) 附:英文原文 Combined Digital Electronic Current and Voltage Transducer DUAN Xiong-Ying, ZOU Ji-Yan, LIAO Min-Fu, ZHANG Ke-Wei Abstract A high-
21、performance current and voltage measurement system has been developed in power system. The system is composed of two parts: one current measurement element and one voltage measurement element. A Rogowski coil and a capacitive voltage divider are used respectively for the line current and voltage mea
22、surements. Active electronic components are used to modulate signal,and power supply for these components is drawn from power line via an auxiliary current transformer. Measurement signal is transmitted by optical fibers, which is resistant to electromagnetic induction and noise. With careful design
23、 and the use of digital signal processing technology, the whole system can meet 0.5% accuracy for metering and provides large dynamic range coupled with good accuracy for protective relaying use. Key words: electronic current transducer (ECT), electronic voltage transducer (EVT), Rogowski coil, cap
24、acitive voltage divider(CVD), optical fiber. 1 Introduction Current and voltage measurements play an important role in metering, protection and control of electric power system. With the development of power system,the traditional current transformers (CT) and potential transformers (PT) show in
25、tolerant drawbacks: high cost and a complicated mode of insulation structure, the CT’s saturation effect and PT’s ferromagnetic resonance effect,et al.In past twenty years, considerable interest has been paid to the research on new optical current transformers (OCT) and optical potential transformer
26、s (OPT). The most common type of OCT utilizes the Farady effect, and OPTutilizes the Pockels effect. They use optical crystals as sensor. Though some successful field trials have been achieved, the large numbers of plentiful commercial products of OCTs and OPTs have not been attained, because OCT an
27、d OPT are susceptible to circumstance temperature and mechanical perturbations[1~3]. In recent years, Ritz Company developed combined electronic current and voltage transducer using Rogowski coil and a capacitive voltage divider as sensors for the line current and voltage measurements respectively[4
28、]. Based on this concept, a new type of digital system for current and voltage measurement are developed. 2 System Structure The concept of digital current transformer has been proposed for almost half century, but it is not well developed because of the limits of electronic components and convent
29、ional protective relaying and metering mode.Yet now protective relaying and metering system operate exclusively by digital technology and information network are being widely employed in power distribution system. All kinds of integrated chips for special function have come to markets.All of these m
30、ake it possible to make electronic CT and PT products based on digital modulation. A block diagram of the combined current and voltage measurement system is given in Fig.1. A Rogowski coil used for current measurement and a power supply CT are fitted to the power line. The Rogowski coil incorporate
31、d with active electronic components composes the whole current transmitter. This transmitter generates an optical signal encoded with information describing the measured current. The whole current transmitter and the power supply part are put into an iron box for electromagnetic interferenece(MEI) i
32、mmunity. A hollow ceramic insulator is used to sustain the high voltage part of the system. Both the optical fiber carrying the current signal and the capacitive voltage divider used as the voltage sensor traverse through the insulator. Voltage signal from the capacitive divider is also modulated in
33、to optical signal at the bottom part of the insulator. Then both the current signal and voltage signal are transmitted by means of optical fiber to the remote control room for metering and protective relaying. 3 Current and Voltage Sensor In this paper, a Rogowski coil is used as current sensor
34、. Rogowski coil, which is a non-magnetic toroid wound like an inductor, has been used for measuring current for some time[5]. A Rogowski coil with rectangular cross-section is showed in Fig.2. When the Rogowski coil is placed on a current-carrying conductor, the coil generates a voltage E proportion
35、al to the coil’s mutual M and the rate of current change di/dt, and it is given by: (1) From Eq.1, the current is derived by means of the relationship : (2) To obtain a measure of current, the coil’s
36、 output voltage must be integrated. This can be done by one of two common means: (1) by use of electronic integrator, (2) by using numerical integration in software after the coil’s output voltage is digitized. In this paper, an active integrator shown in Fig.3 is used. The output of the integrator
37、is : (3) where,Vi is the output of the Rogowski coil. From Eq. (1), Eq.(2), Eq.(3), the current can be obtained by the following equation: (4) Because there is no iron core to saturate, Rogowski coils have wide measurement range. The
38、 same coil can be used to measure currents from several amps to hundreds of kiloamps. Also they have high measurement accuracy, it is reported that they can be designed to be better accuracy than 0.1 percent, and it is insensitive to temperature[6]. Capacitive voltage divider (CVD) has been widely
39、used in high voltage power system. The main factors affecting the measurement accuracy of CVD are stray capacitance and the capacitor’s temperature coefficient. Here precise capacitive divider technology is used to improve measurement accuracy. The effective method to minish stray capacitance is to
40、play down the height of the divider at full steam. In this paper, the insulator is filled with oil as the main insulation to minimize its height. By this means, the stray capacitance of the divider can keep at a low level, and the identical temperature characteristic of the capacitors in series at t
41、he high voltage arm can be ameliorated greatly. A shielding electrode is also put on the top terminal of the divider to compensate the stray capacitance effect. The CVD in electronic voltage transducer (EVT) is put outdoors, great temperature change may affect the ratio error of the divider . As a
42、sensor used in microprocessor-based system, the CVD in EVT is different from those conventional CVD. It has a small load burden, so in this paper a special structure of the CVD shown in Fig.4 is used to eliminate the effect of temperature. The divider is composed of m + n capacitors Ci which have th
43、e identical dielectric, size, value and temperature coefficient. M capacitors are connected in series to produce the C1 value required for the capacitor in the high-voltage arm, C1=Ci/m, and the capacitor value C2 in the low-voltage arm is produced by n capacitors Ci in parallel, C2=n*Ci , then th
44、e divider ratio K is (5) When the capacitor value Ci becomes Ci+ΔCi because of the temperature change,the divider ratio K″ is K″=C1/(C1+C2) =(1/m)(Ci+ΔC1)/[(1/m)(Ci+ΔC1)+n(Ci+ΔC1)] =1/(mn+1) (6) Eq.5 and Eq.6 showK=K″. B
45、y this means, temperature effect on divider ratio can be eliminated provided that all capacitorsCihave the same parameters. 4 Signal Processing A block diagram of the signal processing is shown in Fig.5. Now there are many special A/D chips available in the market. Various methods can be used to
46、 convey measurement information from the transmitter to a remote point. Voltage to frequency modulation is a purely digital technique which can offer error-free and interference-free transmission, and therefor, is most attractive for use in power system. The basic concept of this technique is to con
47、vert the measurement signal into a PFM ( pulse frequency of modulated) signal whose frequency deviation is linearly proportional to the current or voltage magnitude. Eq.7 shows this relationship. (7) Where, F0 is the fundamental frequency which is set by a DC voltage offset a
48、t the input, the coefficient k is determined by the actual circuit. The frquency pulses drive the LED(low emitting diode) directly, and then the signal is modulated into optical pulse. The LED has a center wavelength of 850 nm, which matches the transmission window of the optical fiber. 200μm multi
49、mode fiber is used to transmit optical signal. The receiver in the control room is a photodiode, which drives an amplifier to reconstruct the electric frequency pulses, then the frequency signal is sent into computer for demodulating. It is actually an integral process to count the frequency signa
50、l from time ti to tj, and the count value Yji is: Yji is obtained from the counter, so: (8) The left side of Eq.8 is an integration value of the input pulse signal from ti to tj, and it equals the are value surrounded by the signal curve. If the input signal keeps small change during
51、ti to tj, or the sample time Tc=tj-ti is short enough, its value at point tj can be represented by an approximate value. (9) From Eq.8 and Eq.9, we get (10) The error caused by integration delay effect can be r
52、evised by software. Because the system uses optical fiber to transmit digital signal, it is resistant to EMI. 5 Line Potential Encoder Power Supply Optical fiber uses implements insulation between high voltage and low voltage, but this also brings the problem of power supply at the high voltage. T
53、hree methods are available for designing a current driven power supply: batteries, current transformer, and optical power. Commonly the working life of the batteries is 5~10 years, and the mean time to be repaired is 3 years, it can not be accepted by power system. What is more, the big size of batt
54、ery and its complicated floating charge circuit are undesirable.The high cost of some advanced batteries like lithium or optical batteries becomes obstacle for the application. In this paper, a special designed auxiliary CT is used to get enegy from the line directly. This CT is at the high voltage,
55、 and the insulation requirement is much simpler than those conventional CT, and the power output is low, so it has a rather smaller size than conventional CT. Two key problems should be considered during the power CT design. Firstly, the power CT should supply the required voltage and current from
56、a line current as low as possible, that is to say, the measured line current has a minimum value at which the system will operate. Second, at fault current, the power CT can absorb the unwanted energy to supply a stable power for electronic components, and itself will not be destroyed by electric fo
57、rce. The schematic of the power supply system is shown in Fig.6. From Fig.6, we can obtain that (11) Where, Z0—controlled impedance,Z1—the load impedance, I—line current, UL—load voltage. In order to keep the load voltage UL be constant, then Z0 must change as the change of lin
58、e current I, that is to say, if we can design a controlled impedance circuit changing with the line current I, we can obtain a stable power energy output for the high electronic components. A diagram is shown in Fig.7 for illustrating the operating principle of the power supply design. The energy
59、is obtained from line by power CT. At first , the power supply regulator circuit is the only load imposed on the power transformer’s secondary windings. When all regulated supply voltages are at their specified value, the current branch circuit is activated to stop further replenishment of power sup
60、ply.By this design method, the system can work normally at 5% to 20-fold of the rate current (400 A). 6 System Performance The prototype of a combined electronic current and voltage transducer for a single conductor construction was tested for a 110 kV power system. An overview of primary test re
61、sults is described below. The ratio error characteristics of electronic current transducer at room temperature is shown in Fig.8.The ratio error is represented on the vertical axis,while the primary current flowing to the conductor is represented on the abscissa. This figure indicates the relation
62、ship between the RMS(root-mean-square)value of the output waveform of the optical interface andthe RMS value of the waveform of the primary currentas measured by a 0.2 class coil-type CT. The output of Rogowski coil is designed to be 400 mV corresponding to the 400 A rate primary current, and the pa
63、rameters of integrator arer=10 kΩ,C=0.1μF. It may be seen from this figure that the ratio error of the ECT is at a range of1.0%. As discussed above,signal is demodulated by software, so it is convenient to revise error by using digital signal processing technique, and higher measurement accuracy of
64、0.5% is expected to obtain. The measured phase error of current is better than 20 minutes at twenty percent of full load current at 50 Hz. Fig.9 shows voltage transducer test results. Both the high voltage capacitors in series and the low voltage capacitors are polypropylene capacitors. The test
65、 was carried out at room temperature. This figure indicates the relationship between the RMS value of the output waveform of the optical interface in control room and the RMS value of the waveform of the high voltage as measured by a 0.2 class standard conventional PT. The low voltage is represented
66、 on the vertical axis, while the high voltage is represented on the abscissa. The linearity of the electronic voltage transducer was measured to meet the accuracy (0.5%) of the measurement system. The phase error of voltage is better than 30 minutes when the voltage is over than 20% percent of the full scale. 7 Conclusion A combined digital electronic current and voltage measurement system has been described, which offers many advantages compared with the conventional CTs and PTs. These ca
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