ASTM D2029-1997(2008) Standard Test Methods for Water Vapor Content of Electrical Insulating Gases by Measurement of Dew Point《用露点法测定电绝缘气体中水蒸汽含量的标准试验方法》.pdf
《ASTM D2029-1997(2008) Standard Test Methods for Water Vapor Content of Electrical Insulating Gases by Measurement of Dew Point《用露点法测定电绝缘气体中水蒸汽含量的标准试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM D2029-1997(2008) Standard Test Methods for Water Vapor Content of Electrical Insulating Gases by Measurement of Dew Point《用露点法测定电绝缘气体中水蒸汽含量的标准试验方法》.pdf(6页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: D 2029 97 (Reapproved 2008)Standard Test Methods forWater Vapor Content of Electrical Insulating Gases byMeasurement of Dew Point1This standard is issued under the fixed designation D 2029; the number immediately following the designation indicates the year oforiginal adoption or, in th
2、e 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.This standard has been approved for use by agencies of the Department of Defense.1. Scope1.1 These
3、 test methods describe the determination of thewater vapor content of electrical insulating gases by direct orindirect measurement of the dew point and the calculation ofthe water vapor content.1.2 The following four test methods are provided:1.2.1 Method A describes the automatic chilled mirrormeth
4、od for measurement of dew point as low as 73C(99F).1.2.2 Method B describes the manual chilled mirror or dewcup method for measurement of dew point as low as 73C(99F).1.2.3 Method C describes the adiabatic expansion methodfor measurement of dew point as low as 62C (80F).1.2.4 Method D describes the
5、capacitance method for mea-surement of dew point as low as 110C (166F).1.3 This standard 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 th
6、e applica-bility of regulatory limitations prior to use. For specificwarnings, see 8.1.1, 9.2, 10.1.2 and 10.2.5.2. Referenced Documents2.1 ASTM Standards:2D 1933 Specification for Nitrogen Gas as an ElectricalInsulating MaterialD 2472 Specification for Sulfur HexafluorideD 3283 Specification for Ai
7、r as an Electrical InsulatingMaterial3. Terminology3.1 Definitions:3.1.1 dew point, nthe temperature to which a gas must becooled at constant pressure and constant water vapor content inorder for saturation to occur. Any further cooling usuallyresults in formation of the first drop of dew.3.1.2 hygr
8、oscopic, adjreadily taking up and retainingmoisture.4. Summary of Test Methods4.1 Method AThe automatic chilled mirror method usesthe chilled mirror dew point condensation principle to deter-mine the water vapor content in gas mixtures. An internalmirror, which is in the path of the test gas, is aut
9、omaticallycooled. Internal electronics sense the presence of moisture onthe mirror. The device then automatically brings itself toequilibrium and provides a direct reading of dew point tem-perature.4.2 Method BThis method uses the same basic condensa-tion principle in 4.1; however, the manual chille
10、d mirrormethod uses a mixture of acetone and ice or other coolingmedia to manually chill the dew cup polished surface whichacts as the mirror.4.3 Method CAdiabatic expansion uses a process inwhich the test gas is cooled rapidly to determine dew pointtemperature. This rapid exhausting of the test gas
11、 to atmo-sphere results in an expansion and cooling of the gas. If thecooling is sufficient to reduce the temperature of the gas to orbelow the dew point, water vapor will condense out in the formof a fine mist or fog. Successive trials will determine theminimum initial pressure that will produce a
12、fog. From this, thedew point temperature can be calculated.4.3.1 The relationship between pressure and temperatureduring adiabatic expansion is as follows:TF5 TIPF/PI#K21/Kwhere:K = ratio of specific heats for a given gas,TF= final temperature,TI= initial temperature,PF= final pressure, andPI= initi
13、al pressure.1These test methods are under the jurisdiction of ASTM Committee D27 onElectrical Insulating Liquids and Gases and are the direct responsibility ofSubcommittee D27.07 on Physical Test.Current edition approved Dec. 1, 2008. Published December 2008. Originallyapproved in 1964. Last previou
14、s edition approved in 2003 as D 2029 97 (2003).2For referenced ASTM standards, visit the ASTM 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.1Copyright AST
15、M International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.4.4 Method DThe capacitance method uses a moisturesensor, typically aluminum oxide or silicon oxide, whichchanges its electrical output with the amount of water vapor towhich it is exposed.5. Signifi
16、cance and Use5.1 Certain gases have excellent dielectric and electric arcinterruption characteristics which make their use in electricalinstallations very desirable.5.2 Water content, as the test parameter, is of great impor-tance in determining the dielectric effectiveness of the gas.Under certain
17、conditions, water may condense and become aconducting liquid resulting in a catastrophic dielectric break-down of the insulation. The water content of these insulatinggases as expressed by dew point is listed in SpecificationsD 1933, D 2473, and D 3283.5.3 Once the dew point is determined, a convers
18、ion tomoisture content may be performed using Table 1. Oncemoisture content is known, the lowest temperature at which gasinsulated equipment can be safely operated can usually bedetermined by reviewing manufacturers specifications for theequipment.5.4 The dew point of the test gas is independent of
19、the gastemperature but does depend on its pressure. Many moisturemeasurement test instruments are sensitive to pressure, anddisplay moisture values at the instrument inlet pressure and notnecessarily at the pressure of the system being sampled. It istherefore important to account for this condition
20、to avoidserious measurement errors.6. Interferences6.1 Tubing:6.1.1 Most new metal tubing contains oil deposits on theinterior walls due to the manufacturing process. This residueshould be removed before using these lines for gas sampling.6.1.2 Tubing should be free of leaks, since even a pinholelea
21、k will result in a false indication (higher dew point), due tothe partial pressure of water vapor in the atmosphere.6.1.3 When the gas being tested is extremely dry dew pointbelow approximately 40C (40F), results can be mislead-ing until the moisture adsorbed in the system (tubing, regula-tors, etc.
22、) has been removed by purging with the test gas. Atthis point, all moisture present within the system should be dueto that contained in the test gas.6.2 When testing gases that contain readily liquefiableimpurities, it must be kept in mind that the dew point that ismeasured by condensation type inst
23、ruments may be due tothese impurities rather than to water. Under these conditions,the measured dew point is not an indication of the watercontent of the gas.6.3 Measurement of water vapor in very dry gases iscomplicated by four considerations, as follows:6.3.1 For Methods A, B, and C, the relativel
24、y large volumeof gas required to deposit sufficient water vapor to create the“dew”.6.3.2 For Methods A, B, and C, that under very drycondition, the possibility exists to condense the test gas prior todeposition of moisture on the mirror.6.3.3 For Methods A, B, C, and D, that the measuringsystem (ins
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