ANSI ASTM D3426-1997 Standard Test Method for Dielectric Breakdown Voltage and Dielectric Strength of Solid Electrical Insulating Materials Using Impulse Waves《用冲击波测定电气固体绝缘材料的电介质击穿.pdf

《ANSI ASTM D3426-1997 Standard Test Method for Dielectric Breakdown Voltage and Dielectric Strength of Solid Electrical Insulating Materials Using Impulse Waves《用冲击波测定电气固体绝缘材料的电介质击穿.pdf》由会员分享，可在线阅读，更多相关《ANSI ASTM D3426-1997 Standard Test Method for Dielectric Breakdown Voltage and Dielectric Strength of Solid Electrical Insulating Materials Using Impulse Waves《用冲击波测定电气固体绝缘材料的电介质击穿.pdf（4页珍藏版）》请在麦多课文档分享上搜索。

1、Designation: D3426 97 (Reapproved 2012)Standard Test Method forDielectric Breakdown Voltage and Dielectric Strength ofSolid Electrical Insulating Materials Using Impulse Waves1This standard is issued under the fixed designation D3426; the number immediately following the designation indicates the ye

2、ar oforiginal adoption or, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method covers the determination of dielectri

3、cstrength of solid electrical insulating materials undersimulated-lightning impulse conditions.1.2 Procedures are given for tests using standard 1.2 by 50s full-wave impulses.1.3 This test method is intended for use in determining theimpulse dielectric strength of insulating materials, either usings

4、imple electrodes or functional models. It is not intended foruse in impulse testing of apparatus.1.4 This test method is similar to IEC Publication 243-3.Allprocedures in this test method are included in IEC 243-3.Differences between this test method and IEC 243-3 are largelyeditorial.1.5 This stand

5、ard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibility of the user of this standard to establish appro-priate safety and health practices and determine the applica-bility of regulatory limitations prior to use. Specific precautionstatement

6、s are given in Section 9.2. Referenced Documents2.1 ASTM Standards:2D149 Test Method for Dielectric Breakdown Voltage andDielectric Strength of Solid Electrical Insulating Materialsat Commercial Power FrequenciesD374 Test Methods for Thickness of Solid Electrical Insu-lation (Withdrawn 2013)3D2413 P

7、ractice for Preparation of Insulating Paper andBoard Impregnated with a Liquid Dielectric2.2 American National Standard:C 68.1 Techniques for Dielectric Tests (IEEE Standard No.4)42.3 IEC Standard:Pub 243-3 Methods of Test for Electric Strength of SolidInsulating MaterialsPart 3:Additional Requireme

8、nts forImpulse Tests43. Terminology3.1 Definitions:3.1.1 Reference should be made to Fig. 1 for the symbolsmentioned.3.1.2 full-impulse-voltage wave, nan aperiodic transientvoltage that rises rapidly to a maximum value, then falls lessrapidly to zero.3.1.3 peak value of an impulse voltage wave, n th

9、emaximum value of voltage.3.1.4 virtual-peak value of an impulse voltage wave, navalue derived from a recording of an impulse wave on whichhigh-frequency oscillations or overshoot of limited magnitudemay be present. If the oscillations have a magnitude of no morethan 5 % of the peak value and a freq

10、uency of at least 0.5 MHz,a mean curve may be drawn, the maximum amplitude of whichis the virtual-peak value. If the oscillations are of greatermagnitude, the voltage wave is not acceptable for standardtests.3.1.5 virtual-front time of an impulse voltage wave,nequal to 1.67 times the interval tfbetw

11、een the instants whenthe voltage is 0.3 and 0.9 times the peak value (t1, Fig. 1).3.1.6 virtual origin of an impulse voltage wave, nthe pointof intersection O1with the line of zero voltage of a line drawnthrough the points of 0.3 and 0.9 times the peak voltage on thefront of an impulse voltage wave.

12、3.1.7 virtual time to half-value of an impulse voltage wave,nthe time interval t2between the virtual origin O1and theinstant on the tail when the voltage has decreased to half thepeak value.1This test method is under the jurisdiction of ASTM Committee D09 onElectrical and Electronic Insulating Mater

13、ials and is the direct responsibility ofSubcommittee D09.12 on Electrical Tests.Current edition approved Nov. 1, 2012. Published November 2012. Originallyapproved in 1975. Last previous edition approved in 2004 as D3426 97(2004).DOI: 10.1520/D3426-97R12.2For referenced ASTM standards, visit the ASTM

14、 website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.3The last approved version of this historical standard is referenced onwww.astm.org.4Available from America

15、n National Standards Institute (ANSI), 25 W. 43rd St.,4th Floor, New York, NY 10036.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States14. Summary of Test Method4.1 A series of sets-of-three voltage waves of a specifiedshape (see 5.3) is

16、applied to the test specimen. The voltage ofsuccessive sets is increased in magnitude until breakdown ofthe test specimen occurs.4.2 The procedures for sampling and specimen preparationare as specified in the material specification or other documentcalling for the use of this test method. The surrou

17、ndingmedium (air or other gas, or oil or other liquid) is also asspecified if it differs from the medium in which the specimensare finally conditioned for test.5. Significance and Use5.1 Insulating materials used in high-voltage equipmentmay be subjected to transient voltage stresses, resulting from

18、such causes as nearby lightning strokes. This is particularlytrue of apparatus such as transformers and switchgear used inelectrical-power transmission and distribution systems. Theability of insulating materials to withstand these transientvoltages is important in establishing the reliability of ap

19、paratusinsulated with these materials.5.2 Transient voltages caused by lightning may be of eitherpositive or negative polarity. In a symmetrical field betweenidentical electrodes, the polarity has no effect on the break-down strength. However, with dissimilar electrodes there maybe a pronounced pola

20、rity effect. It is common practice whenusing dissimilar electrodes, to make negative that electrode atwhich the higher gradient will appear. When asymmetricalelectrodes are used for testing materials with which the testerhas no previous experience or knowledge, it is recommendedthat he make comparat

21、ive tests with positive polarity andnegative polarity applied to the higher gradient, or smallerelectrode, to determine which polarity produces the lowerbreakdown voltage.5.3 The standard wave shape is a 1.2 by 50-s wave,reaching peak voltage in approximately 1.2 s and decaying to50 % of peak voltag

22、e in approximately 50 s after thebeginning of the wave. This wave is intended to simulate alightning stroke that may strike a system without causingfailure on the system.5.4 For most materials, the impulse dielectric strength willbe higher than either its power frequency alternating voltage orits di

23、rect voltage dielectric strengths. Because of the short timeinvolved, dielectric heating and other thermal effects arelargely eliminated during impulse testing. Thus, the impulsetest gives values closer to the intrinsic breakdown strength thando longer time tests. From comparisons of the impulse die

24、lec-tric strength with the values obtained from longer time tests,FIG. 1 Full-Impulse Voltage WaveD3426 97 (2012)2inferences may be drawn as to the modes of failures under thevarious tests for a given material.Appendix X1 of Test MethodD149 should be referred to for further information on thissubjec

25、t.6. Apparatus6.1 Impulse Generator, capable of applying to the testspecimen a standard 1.2 by 50-s wave of either positive ornegative polarity. The virtual front time shall be 1.2 s 6 30 %and the virtual time to half value 50 s 6 20 %. The maximumvoltage and the energy-storage capability must be su

26、fficient toprovide impulse waves of the proper shape to any specimen tobe tested up to the breakdown voltage (or specified proofvoltage) of the material. The electrical characteristics (particu-larly capacitance) of the test specimen may have a significanteffect on the magnitude and shape of the app

27、lied voltage wave,especially when using generators having low energy-storagecapability. In such cases, provisions must be made for moni-toring and adjusting the voltage wave shape.6.2 Voltage-Measurement Equipment , meeting the require-ments of ANSI C68.1.6.3 Electrodes:6.3.1 Electrodes shall be as

28、defined in the specification ormethod in which reference is made to this test method. If noelectrodes are specified, one of the types listed in Table 1 ofTest Method D149 should be used when testing materials aslisted in Table 1 of Test Method D149.6.3.2 The surfaces of the electrodes must be polish

29、ed andfree of projecting irregularities resulting from previous tests.6.4 Surrounding Medium, as specified for the material beingtested. If the surrounding medium is not specified, refer to 8.2and 8.3 and to the section on Surrounding Medium in TestMethod D149 for guidance.7. Sampling7.1 Sample in a

30、ccordance with the requirements given in thedocument in which this test method is specified.7.2 Sample in such a manner as to permit preparation of testspecimens that are representative of the lot or other unit ofmaterial being evaluated.7.3 Handle and store the samples (and specimens preparedfrom t

31、he samples) in a manner to prevent alteration of theproperties of the material due to such handling and storage.8. Test Specimens8.1 Prepare specimens of sufficient number and size topermit making five valid tests (see 9.2.4).8.2 Prepare the specimens for test using procedures asspecified in the mat

32、erial specification. (In general, materialsshould be tested in the medium in which they are to be used,after conditioning in a manner representative of the manufac-turing methods to which they will be subjected.)8.3 When testing specimens in a surrounding medium otherthan air, do not remove them fro

33、m that surrounding mediumsubsequent to final conditioning for test until after completionof the test. As a specific example, when conditioning speci-mens for testing in oil by vacuum-impregnation with oil do notremove the specimen from oil even momentarily prior totesting.9. Procedure9.1 Warning Let

34、hal voltages are a potential hazard dur-ing the performance of this test. It is essential that the testapparatus, and all associated equipment electrically connectedto it, be properly designed and installed for safe operation.Solidly ground all electrically conductive parts which it ispossible for a

35、 person to contact during the test. Provide meansfor use at the completion of any test to ground any parts whichwere at high voltage during the test or have the potential foracquiring an induced charge during the test or retaining acharge even after disconnection of the voltage source. Thor-oughly i

36、nstruct all operators as to the correct procedures forperforming tests safely. When making high voltage tests,particularly in compressed gas or in oil, it is possible for theenergy released at breakdown to be sufficient to result in fire,explosion, or rupture of the test chamber. Design testequipmen

37、t, test chambers, and test specimens so as to minimizethe possibility of such occurrences and to eliminate thepossibility of personal injury. If the potential for fire exists,have fire suppression equipment available.9.2 Voltage Application:9.2.1 Place the specimen between the electrodes and applywa

38、ves of the polarity specified. The initial peak voltage shall beapproximately 70 % of the expected breakdown voltage.9.2.2 Apply the impulse waves in sets of three waves, eachset at successively increasing voltage levels until breakdownoccurs. Each level of peak voltage shall be higher than theprece

39、ding level by from 5 to 10 % of the crest voltage of theinitial level.9.2.3 The minimum time between successive voltage appli-cations is dependent upon the charging time constant of thegenerator and should be three times the time constant.9.2.4 A valid test is one in which impulse waves are appliedf

40、or at least two levels without breakdown before breakdownoccurs at the third or some higher voltage level.9.3 Criteria of Breakdown:9.3.1 Observation of actual rupture, either visually oraudibly, may be the most immediate indication of failure. Forsome specimen configurations, observation of the imp

41、ulsewave on an oscilloscope may be the most sensitive indication.A collapse of the voltage wave at any point is an indication offailure either by puncture or surface creepage.9.3.2 The impulse dielectric breakdown voltage is the peakvoltage that the wave causing breakdown would have reachedhad break

42、down not occurred.9.4 Thickness Measure the average thickness of the speci-men in the area between the electrodes, using procedures givenin Test Methods D374 for the material being tested.10. Calculation10.1 Calculate the impulse-withstand strength using thespecimen thickness and the value for the m

43、aximum level ofimpulse voltage that did not cause failure of the specimen.D3426 97 (2012)310.2 Calculate the impulse-breakdown dielectric strengthusing the specimen thickness and the value for impulsedielectric breakdown voltage.11. Report11.1 Report the following:11.1.1 Identification of test sampl

44、e,11.1.2 For each specimen:11.1.2.1 Average thickness,11.1.2.2 Maximum impulse-withstand voltage,11.1.2.3 Impulse dielectric breakdown voltage,NOTE 1It may in some cases be desirable to report which of the threeimpulse waves at the breakdown level resulted in failure.11.1.2.4 Impulse-withstand stren

45、gth,11.1.3 For each sample:11.1.3.1 Average impulse-withstand strength,11.1.3.2 Average impulse dielectric breakdown strength,11.1.3.3 Indication of variability, preferably the standarddeviation, from the average dielectric strengths,11.1.4 Conditioning or specimen preparation,11.1.5 Ambient atmosph

46、eric temperature,11.1.6 Surrounding medium,11.1.7 Test temperature,11.1.8 Impulse wave polarity,11.1.9 Initial voltage level and magnitude of voltage steps,and11.1.10 Date of test.12. Precision and Bias12.1 The precision and bias for this test method have notbeen established.12.2 Tests made by one o

47、perator in a single laboratory,using one test set over a period of 18 months, on 15 sets of 5randomized specimens from a single reference sample, resultedin a repeatability within 6 5 %. The sample was 0.002-in(50-m) thick high-density capacitor tissue. The specimenswere made up of three layers and

48、were impregnated with oilprior to test in accordance with Test Methods D2413. Thespecimens were tested under oil, using Type 1 electrodes. Theaverage impulse breakdown strength for the 15 sets of speci-mens ranged from 4200 to 4600 V/mil (165 to 181 kV/mm).13. Keywords13.1 dielectric breakdown; diel

49、ectric breakdown criteria;dielectric breakdown voltage; dielectric strength; full-impulse-voltage wave; impulse dielectric strength; impulse generator;impulse waves; lightning strokes; peak value; simulated-lightning impulse; solid insulating material; virtual front time;virtual origin; virtual peak value; virtual time to half-valueASTM International takes no position respecting the validity of any patent rights asserted in connection with any item mentionedin this standard. Users of this standard are expressly advised that determination of the validity of any su