ASTM D2477-2007(2012) Standard Test Method for Dielectric Breakdown Voltage and Dielectric Strength of Insulating Gases at Commercial Power Frequencies《商用电源频率下绝缘气体介电击穿电压和介电强度的标准试验方.pdf

《ASTM D2477-2007(2012) Standard Test Method for Dielectric Breakdown Voltage and Dielectric Strength of Insulating Gases at Commercial Power Frequencies《商用电源频率下绝缘气体介电击穿电压和介电强度的标准试验方.pdf》由会员分享，可在线阅读，更多相关《ASTM D2477-2007(2012) Standard Test Method for Dielectric Breakdown Voltage and Dielectric Strength of Insulating Gases at Commercial Power Frequencies《商用电源频率下绝缘气体介电击穿电压和介电强度的标准试验方.pdf（5页珍藏版）》请在麦多课文档分享上搜索。

1、Designation: D2477 07 (Reapproved 2012)Standard Test Method forDielectric Breakdown Voltage and Dielectric Strength ofInsulating Gases at Commercial Power Frequencies1This standard is issued under the fixed designation D2477; the number immediately following the designation indicates the year oforig

2、inal 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 the dielec-tric br

3、eakdown voltage and dielectric strength of insulatinggases used in transformers, circuit breakers, cables, and similarapparatus as an insulating medium. The test method is appli-cable only to gases with boiling points below room temperatureat atmospheric pressure.1.2 This standard may involve hazard

4、ous materials,operations, and equipment. This standard does not purport toaddress all of the safety concerns, if any, associated with itsuse. It is the responsibility of the user of this standard toestablish appropriate safety and health practices and deter-mine the applicability of regulatory limit

5、ations prior to use.1.3 Mercury has been designated by EPA and many stateagencies as a hazardous material that can cause centralnervous system, kidney and liver damage. Mercury, or itsvapor, may be hazardous to health and corrosive to materials.Caution should be taken when handling mercury and mercu

6、rycontaining products. See the applicable product MaterialSafety Data Sheet (MSDS) for details and EPAs website http:/www.epa.gov/mercury/faq.htm for additional informa-tion. Users should be aware that selling mercury and/ormercury containing products into your state may be prohibitedby state law.2.

7、 Referenced Documents2.1 ASTM Standards:2D2864 Terminology Relating to Electrical Insulating Liq-uids and Gases2.2 IEEE Standard:3No. 4 Standard Techniques for High Voltage Testing2.3 ASTM Adjuncts:Dielectric cell assembly and detail (2 drawings)43. Terminology3.1 Definitions:3.1.1 For definitions o

8、f terms used in this test method, referto Terminology D2864.4. Significance and Use4.1 The dielectric breakdown voltage and dielectric strengthof an insulating gas in a uniform field depends primarily on themolecular structure of the gas. As different gases are mixedeither by plan or by contaminatio

9、n, any change in dielectricbreakdown voltage and dielectric strength will depend on boththe nature and proportion of the individual gases. This testmethod uses plane and spherical electrodes which provide anearly uniform field (see Appendix) in the area of electricaldischarge. It is suitable for det

10、ermining the dielectric break-down voltage and dielectric strength of different gases andmixtures thereof for research and application evaluations andalso as a field test. A more complete discussion of thesignificance of the dielectric strength test is given in theAppendix.5. Apparatus5.1 Electrical

11、 Apparatus:5.1.1 Transformer The desired test voltage may be mostreadily obtained by a step-up transformer energized from avariable low-voltage commercial power frequency source. Thetransformer and controlling element shall be of such size anddesign that, with the test specimen in the circuit, the c

12、rest factor(ratio of maximum to mean effective) of the 60-Hz test voltagedoes not differ by more than 65 % from that of a sinusoidalwave over the upper half of the range of test voltage. The crestfactor may be checked by means of an oscilloscope, a spheregap, or a peak-reading voltmeter in conjuncti

13、on with an rmsvoltmeter. Where the waveform cannot be determinedconveniently, a transformer having a rating of not less than121This test method is under the jurisdiction of ASTM Committee D27 onElectrical Insulating Liquids and Gases and is the direct responsibility of Subcom-mittee D27.05 on Electr

14、ical Test.Current edition approved May 1, 2012. Published May 2012. Originallyapproved in 1966. Last previous edition approved in 2007 as D2477 07. DOI:10.1520/D2477-07R12.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For An

15、nual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.3Available from The Institute of Electrical and Electronic Engineers, Inc.(IEEE), 445 Hoes Ln., P.O. Box 1331, Piscataway, NJ 08854-1331.4Detailed drawings of this apparatus are available a

16、t a nominal cost from:ASTMInternational Headquarters. Order Adjunct No. ADJD2477.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States1kVA at the usual breakdown voltage shall be used. Transform-ers of larger kVA capacity may be used, but i

17、n no case shouldthe power frequency short circuit current in the specimencircuit be outside the range of 1 to 10 mA/kV of appliedvoltage. This limitation of current may be accomplished byusing a suitable external series resistor or by employing atransformer with sufficient inherent reactance.5.1.2 C

18、ircuit-Interrupting Equipment The test transformerprimary circuit shall be protected by an automatic circuit-breaking device capable of opening (as nearly instantaneouslyas possible) on the current produced by the breakdown of thetest specimen; a circuit breaker that opens within 5 cycles maybe used

19、 if the short-circuit current as described in 5.1.1 doesnot exceed 200 mA. A prolonged flow of current at the time ofbreakdown causes contamination of the gases and damage ofthe electrodes, thereby affecting the subsequent test results, andincreasing the electrode and test cell maintenance and time

20、oftesting.5.1.3 Voltage-Control EquipmentThe rate of voltage riseshall be12 kV/s 6 20 %. Voltage control may be secured by amotor-driven variable-ratio-autotransformer. Preference isgiven to equipment having an approximately straight-linevoltage-time curve over the desired operating range. Motordriv

21、e is preferred to manual drive because of the ease ofmaintaining a reasonably uniform rate-of-voltage rise with thistest method. The rate-of-voltage rise may be calculated frommeasurements of the time required to raise the voltage betweentwo prescribed values. When motor-driven equipment is used,cal

22、ibrate the speed control rheostat in terms of rate-of-voltagerise for the test transformer used.5.1.4 VoltmeterMeasure the voltage by a method thatfulfills the requirements of IEEE Standard No. 4, giving crestand also (if available) rms values, preferably by means of:5.1.4.1 Avoltmeter connected to

23、the secondary of a separatepotential transformer, or5.1.4.2 A voltmeter connected to a well-designed tertiarycoil in the test transformer, or5.1.4.3 A voltmeter connected to the low-voltage side of thetest transformer.5.1.5 AccuracyThe combined accuracy of the voltmeterand voltage divider circuit is

24、 not to exceed 5 % at the rate ofvoltage rise specified in 5.1.3.5.2 Evacuation and Filling Apparatus :5.2.1 Vacuum Pump The vacuum pump shall have suffi-cient pumping capacity to be able to evacuate the test cell to apressure below 0.133 kPa (1 torr).5.2.2 Vacuum and Pressure GageEither a mercuryma

25、nometer, or one or more gages, capable of measuringpressures below 0.133 kPa (1 torr) and also near atmosphericpressure. The manometer, or vacuum and pressure gages, shallbe calibrated in kPa or millimetres of mercury (torr).5.2.3 Connections Vacuum-tight tubing and valves shallbe used while evacuat

26、ing and purging the test cell and filling itwith the gas sample.5.3 Electrodes and Test Cell:45.3.1 The sphere and plane electrodes shall be mountedvertically as shown in Fig. 1. The sphere shall be a precisionsteel bearing ball 19.1 mm (0.75 in.) in diameter. The planeelectrode shall be of brass 38

27、.1 mm (1.50 in.) in diameter. Thegap setting shall be 2.54 6 0.025 mm (0.100 6 0.001 in.). Thetolerance of all dimensions is 62 %, unless otherwise stated.5.3.2 The cell shall consist of a borosilicate glass cylinderclamped by flanges to end plates which seal the cell andsupport the electrodes.5The

28、lower plane electrode shall befixed. The sphere electrode, held in place by a magnet, shall beadjustable by means of a micrometer screw suitably mountedthrough the top plate. The micrometer screw must be suitablefor setting the electrodes to within the specified tolerance. Thebottom plate shall have

29、 a valved port for evacuation andadmission of the sample. If considered more convenient, twoports, one in the top for evacuation and one in the bottom foradmission of the sample may be used. The dimensions areshown in Fig. 1.6. Sampling6.1 Obtain the gas sample from the gas cylinder or gas-filledequ

30、ipment through a pressure-reducing regulator valve so thatthe flow into the cell may be controlled. The sample and cellmust be at room temperature before the gas is admitted to thecell.7. Preparation of Cell7.1 Clean the cell except for the electrodes by washing withsoap or detergent, then rinse wit

31、h distilled or demineralizedwater and oven-dry. Clean the cell whenever necessary toremove detectable decomposition products formed by thebreakdown arc, or when testing different gases.7.2 Clean the electrodes with crocus cloth and naphtha.When the sphere electrode becomes pitted, it may be turned t

32、oa new position until it is necessary to replace it.7.3 Assemble the cell by positioning and tightening the twoend flanges and gaskets.7.4 Turn the micrometer screw until the sphere just touchesthe plane electrode. The point where contact is made is bestchecked by a continuity meter connected to the

33、 two electrodes.7.5 Note the reading on the micrometer, add 2.54 mm(0.100 in.), and adjust the micrometer to this new setting.8. Test Conditions8.1 The dielectric breakdown voltage of an insulating gasunder ambient conditions varies with temperature and pressure.The standard conditions for the test

34、are 101 kPa (760 torr) and25C. If the ambient temperature deviates slightly from 25Cadjust the gas pressure for the test as follows:P 5 2731T! 3101#/298where:P = gas pressure for the test, kPa, andT = ambient temperature, C.8.2 As an alternative to the pressure adjustment in 8.1 thetest may be made

35、at ambient temperature and pressure and the5Standard laboratory borosilicate glass pipe and connecting flanges may be used.D2477 07 (2012)2dielectric breakdown result multiplied by an approximatefactor, F, calculated as follows:F 5 2731T!/2.95 Pwhere:T = ambient temperature, C, andP = ambient gas pr

36、essure, kPa.8.3 The breakdown voltage of an insulating gas may beaffected by irradiation of the gas in the electrode gap. Suchirradiation can occur from random sources such as sunlight,artificial lights of various types, and nearby radioactive mate-rials. It is recommended that the test cell be shie

37、lded from suchsources as much as possible during test runs. See X1.4 andX1.5 for further discussion.9. Procedure9.1 Fill the cell as follows:9.1.1 Evacuate the cell to a pressure of less than 0.133 kPa(1 torr).9.1.2 Fill the cell with the gas to be tested to atmosphericpressure or slightly above.9.1

38、.3 Again evacuate the cell to a pressure of less than 0.133kPa (1 torr).9.1.4 Fill the cell with the gas to be tested to either thecalculated pressure as in 8.1 or to atmospheric pressure and usethe factor as calculated in 8.2.9.2 Apply the voltage by increasing from zero at the rate ofapproximately

39、12 kV/s until breakdown occurs as indicated byoperation of the circuit-interrupting equipment. Record thebreakdown voltage.9.3 Make five breakdowns on the one filling of the cell.9.4 To test a second sample, repeat the purging and filling asdescribed in 9.1.1-9.1.4.10. Report10.1 Report the followin

40、g information:10.1.1 Source of gas and its molecular identification,10.1.2 The five individual breakdown values and theiraverage, all multiplied by the factor, F, when the procedure in8.2 is followed,10.1.3 Ambient temperature and the pressure of the gaswhen tested, and10.1.4 Frequency of the voltag

41、e source.11. Precision and Bias11.1 The repeatability to be expected within a laboratoryand the agreement that should be obtained between laboratoriesare tabulated in Table 1 as a guide. The tabulated values areobtained from a cooperative test program involving ten labo-ratories each testing seven g

42、ases in test cells of same design.FIG. 1 Test CellD2477 07 (2012)312. Keywords12.1 breakdown voltage; dielectric strength; gases; insulat-ing gasesAPPENDIX(Nonmandatory Information)X1. SIGNIFICANCE OF THE DIELECTRIC STRENGTH TESTX1.1 Dielectric breakdown of an insulating gas occurswhen the gas is st

43、ressed in an electric field that exceeds thedielectric strength of the gas. An electric field can be applied toa gas by means of submerging two metal electrodes of oppositepolarity into the gas. As the voltage across the electrodes israised to a critical value, a spark jumps between the electrodesma

44、nifesting a dielectric breakdown of the gas. The dielectricbreakdown voltage, however, depends on the electric fieldproduced by the electrodes and the spacing between them. Fora given spacing, the highest breakdown voltage can beachieved when the field is uniform between the electrodes,such as that

45、produced by two parallel-plane electrodes ofinfinite size. The dielectric strength of a gas is then equal to thisvoltage at a unit spacing and is expressed as kilovolts percentimetre or per inch.X1.2 Since parallel-plane electrodes of infinite size areimpractical, parallel electrodes of finite dimen

46、sion have beendesigned with special contours at the electrode edges so thatthe breakdown spark takes place in the parallel-plane region,although the field outside this region is nonuniform. Rogowskiand Rengier6,7have utilized exponential and sinusoidalcontours, respectively, so that the electric str

47、ess is the highestbetween the planes. However, these electrodes are difficult tomanufacture and relatively bulky as compared to the sphere-to-plane electrode configuration used in this test method.X1.3 Although the field produced by the sphere-plane elec-trodes is largely nonuniform, yet in the limi

48、ted region at theminimum spacing, where sparking is observed in the dielectricbreakdown tests of insulating gases, the field is practicallyuniform. The dielectric strength (in terms of average electricalfield) of air determined with this test method is 30 kV/cm,which is the same as determined with t

49、he parallel-planeelectrodes. Consequently, this test method may be used fordetermining the dielectric strength as well as measuring thedielectric breakdown voltage of insulating gases.X1.4 The breakdown voltage of insulating gases may beaffected by irradiation of the gas in the electrode gap of the testcell. Random irradiation caused by sunlight, some artificiallight sources, and nearby radioactive materials, can causescatter in test results. It is recommended that reasonable care beused in shielding the test cell from such random sources.X1.5 The committee sp