ANSI IEEE 1531-2003 Guide for Application and Specification of Harmonic Filters《谐波过滤器的使用和规范指南》.pdf
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1、IEEE Std 1531-2003IEEE Standards1531TMIEEE Guide for Application andSpecification of Harmonic FiltersPublished by The Institute of Electrical and Electronics Engineers, Inc.3 Park Avenue, New York, NY 10016-5997, USA24 November 2003IEEE Power Engineering SocietySponsored by theTransmission +1 978 75
2、0 8400. Permission to photocopy portions of any individual standard for educationalclassroom use can also be obtained through the Copyright Clearance Center.Authorized licensed use limited to: IHS Stephanie Dejesus. Downloaded on March 05,2010 at 13:56:43 EST from IEEE Xplore. Restrictions apply. iv
3、 Copyright 2003 IEEE. All rights reserved.Introduction(This introduction is not part of IEEE Std 1531-2003, IEEE Guide for Application and Specification of HarmonicFilters.)This guide addresses the specification of the (1) components, (2) protection, and (3) control of harmonic fil-ters. It does not
4、 address the proper sizing or configuration of harmonic filters to achieve desired perfor-mance. This document provides guidelines for passive shunt harmonic filters for use on 50 Hz and 60 Hzpower systems. No specific standards exist for harmonic filters, although standards do exist for virtually a
5、llof the components that are used in a filter.ParticipantsDuring the time this guide was being developed, the IEEE working group sponsored by the Capacitor Sub-committee of the Transmission and 8% or less for most user busses at less than 1 kV. The total demand current distortion at the point ofcomm
6、on coupling to the utility is limited to the range of 2.5% to 20%, depending upon the size of the cus-tomers harmonic-producing load and other factors. (See IEEE Std 519-1992 for details.) The document alsogives higher limits for conditions lasting less than 1 hour.4.2.2 Equipment withstand capabili
7、tiesSome of the withstand capabilities that are described in existing equipment standards are summarized in thissubclause.When transformers are operating at rated load, the total harmonic current distortion should be limited to 5%as defined in IEEE Std C57.12.00-2000 and IEEE Std C57.12.01-1998.12IE
8、EE Std C57.110-1998 definesthe method for derating transformers when supplying nonsinusoidal loads. UL 1561-1999 and UL 1562-1999 define the transformer K-rating that is intended for use in high harmonic environments.IEEE Std 18-200213states that capacitors are intended to be operated at or below th
9、eir rated voltage.Capacitors shall be capable of continuous operation under contingency system and bank conditions providedthat none of the following limitations are exceeded:a) 110% of rated rms root-mean-square voltageb) 120% of rated peak voltage, i.e., peak voltage not exceeding 1.2 x (square ro
10、ot of two) x rated rmsvoltage, including harmonics, but excluding transientsc) 135% of nominal rms current based on rated kvar and rated voltaged) 135% of rated kvarAdditional application guidelines for capacitors are given in IEEE Std 1036-1992. It should be noted thatcapacitor fuses should be rate
11、d for the voltage and current, including harmonics, in a filter application.The limitation to 135% of rated kvar in IEEE Std 18-2002 is based on dielectric heating at fundamental fre-quency and is based on the thermal stability test in that standard. The 135% limit in IEEE Std 18-2002 isbased on a m
12、aximum operating voltage of 110% of rated voltage and a maximum capacitance tolerance of+15% (the maximum allowable tolerance at the time the 135% limit was set). (1.12 , thus135%.)The total dielectric heating in a capacitor is a function of the force between the electrodes, the capacitance ofthe di
13、electric, and the number of force reversals per second.The force is the result of the attraction of the positive and negative charges on the electrodes. The magnitudeof the charge Q on each of the electrodes is proportional to the voltage difference V between the electrodes.The force is proportional
14、 to the product of the charge magnitudes. Because the positive and negative chargesare equal to each other and are proportional to the applied voltage, the force (and losses) varies as the squareof the applied voltage. 11This information is from the referenced standard(s) and does not transplant the
15、se limits to this guide. See the first paragraph ofClause 2.12See footnote 11.13This quotation is from the referenced standard(s) and does not transplant these limits to this guide.1.15 1.35Authorized licensed use limited to: IHS Stephanie Dejesus. Downloaded on March 05,2010 at 13:56:43 EST from IE
16、EE Xplore. Restrictions apply. IEEEStd 1531-2003 IEEE GUIDE FOR APPLICATION AND6 Copyright 2003 IEEE. All rights reserved.The total dielectric heating varies linearly with the capacitance of the dielectric. Changes in capacitance dueto change in area of the dielectric, thickness of the dielectric, a
17、nd changes in the dielectric constant due tosmall materials variations all affect the total heating linearly.The dc dielectric losses and resulting heating in a high voltage power capacitor are very small. The dielectriclosses are dominated by ac losses. Each time the force is reversed there is an a
18、mount of loss. The ac lossesare linear function of the applied frequency.Therefore, for a single frequency, the dielectric losses are proportional to the square of the applied voltage,the capacitance, and the frequency, as shown in Equation (1):(1)Note that, for a capacitor, the reactive power Q is(
19、2)(3)(4)Note the similarity in the expressions for dielectric loss and Q. For a single frequency, the dielectric heatingin the capacitor is proportional to the reactive power (measured in kilovars).For a capacitor in a filter, there are multiple frequencies generating the dielectric heating. For fil
20、ter applica-tions where (1) there is no significant dc voltage present, (2) the harmonic voltages across the capacitor aresmaller than the fundamental frequency voltage, and (3) the highest significant frequency is less than about1 kHz, the dielectric heating will be within the 135% limit if(5)or(6)
21、wheref is the rated frequency of the capacitor and system (Hz),C is the actual capacitance of the capacitor (F),h is the harmonic order, for all significant harmonics including the fundamental (h = 1),V(h) is the capacitor voltage (rms) at the h harmonic (kV),I(h) is the capacitor current (rms) at t
22、he h harmonic (A), Qratedis the capacitor rated reactive power (kvar).The inequality in Equation (6) is the one normally used to determine whether the dielectric heating is accept-able. While dc losses in a capacitor are small, the presence of dc voltage can increase the maximum chargeand significan
23、tly increase the ac losses. That increase is not reflected in the above inequalities, limiting theuse of these inequalities to applications where no significant dc voltage is present.Higher frequency currents may result in eddy current or induced losses in addition to the dielectric losses.Where the
24、 harmonic currents are smaller than the fundamental current, the error caused by ignoring theseDielectric Loss f CV2QV()I()=V()2 f CV()=2 f C V()2=2000 f C hV h()2()h1.35 QratedVh()Ih()h1.35 QratedAuthorized licensed use limited to: IHS Stephanie Dejesus. Downloaded on March 05,2010 at 13:56:43 EST
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