ASTM A773 A773M-2001(2009) Standard Test Method for dc Magnetic Properties of Materials Using Ring and Permeameter Procedures with dc Electronic Hysteresigraphs《使用DC电磁滞曲线记录仪的参数处理和环.pdf

《ASTM A773 A773M-2001(2009) Standard Test Method for dc Magnetic Properties of Materials Using Ring and Permeameter Procedures with dc Electronic Hysteresigraphs《使用DC电磁滞曲线记录仪的参数处理和环.pdf》由会员分享，可在线阅读，更多相关《ASTM A773 A773M-2001(2009) Standard Test Method for dc Magnetic Properties of Materials Using Ring and Permeameter Procedures with dc Electronic Hysteresigraphs《使用DC电磁滞曲线记录仪的参数处理和环.pdf（10页珍藏版）》请在麦多课文档分享上搜索。

1、Designation: A 773/A 773M 01 (Reapproved 2009)Standard Test Method fordc Magnetic Properties of Materials Using Ring andPermeameter Procedures with dc ElectronicHysteresigraphs1This standard is issued under the fixed designationA 773/A 773M; the number immediately following the designation indicates

2、 the yearof original adoption or, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval.A superscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method provides dc hysteresigraph pro

3、cedures(B-H loop methods) for the determination of basic magneticproperties of materials in the form of ring, toroidal, link,double-lapped Epstein cores, or other standard shapes that maybe cut, stamped, machined, or ground from cast, compacted,sintered, forged, or rolled materials. It includes test

4、s for normalinduction and hysteresis taken under conditions of continuoussweep magnetization. Rate of sweep may be varied, eithermanually or automatically at different portions of the curvesduring tracing. Total elapsed time for tracing a hysteresis loopis commonly 10 to 120 s per loop.1.2 The value

5、s stated in either SI units or inch-pound unitsare to be regarded separately as standard. The values stated ineach system may not be exact equivalents; therefore, eachsystem shall be used independently of the other. Combiningvalues from the two systems may result in non-conformancewith the standard.

6、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 the applica-bility of regulatory limitations prior to use.2. Referenced D

7、ocuments2.1 ASTM Standards:2A 34/A 34M Practice for Sampling and Procurement Test-ing of Magnetic MaterialsA 341/A 341M Test Method for Direct Current MagneticProperties of Materials Using D-C Permeameters and theBallistic Test MethodsA 343/A 343M Test Method for Alternating-Current Mag-netic Proper

8、ties of Materials at Power Frequencies UsingWattmeter-Ammeter-Voltmeter Method and 25-cm EpsteinTest FrameA 596/A 596M Test Method for Direct-Current MagneticProperties of Materials Using the Ballistic Method andRing Specimens2.2 Other:IEC Publication 404-4: Magnetic MaterialsPart 4: Meth-ods of Mea

9、surement of dc Magnetic Properties of Iron andSteel (1995)33. Summary of Test Method3.1 As in making most magnetic measurements, a specimenis wound with an exciting winding (the primary) and a searchcoil (the secondary) for measuring the change in flux. When anexciting current, I, is applied to the

10、primary winding, amagnetic field, H, is produced in the coil, and this in turnproduces magnetic flux f in the specimen. In uniform speci-mens that do not contain air gaps, such as ring samples, all ofthe exciting current is used to magnetize the specimen, and His proportional to I in accordance with

11、 the following equation:H 5 KI(1)where:H = magnetic field strength, Oe A/m;I = current in the exciting coil A; andK = constant determined by the number of primary turnsthe magnetic path length of the specimen and systemof units.3.1.1 The magnetic flux may be determined by integrationof the instantan

12、eous electromotive force that is induced in thesecondary coil when the flux is increased or decreased by avarying H. The instantaneous voltage, e, is equal to:e 52NK1dfdt(2)orf51K1N*edt1This test method is under the jurisdiction of ASTM Committee A06 onMagnetic Properties and is the direct responsib

13、ility of SubcommitteeA06.01 on TestMethods.Current edition approved May 1, 2009. Published August 2009. Originallyapproved in 1980. Last previous edition approved in 2001 as A 773/A 773M01.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at servic

14、eastm.org. For Annual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.3Available from American National Standards Institute, 25 W. 43rd St., 4thFloor, New York, NY 10036.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West

15、Conshohocken, PA 19428-2959, United States.where:dt = time differential,N = number of turns, andK1=108for cgs-emu system, or K1= 1 for SI system.The flux f can be obtained if *edt can be determined. Thiscan be accomplished by several means, as described in ASTMSTP 526. (1)4The most common method use

16、s an electronicintegrator consisting of a high-gain dc amplifier with resistive-capacitive feedback. The relationship to * edt is:E 51RC*edt (3)where:E = output voltage, V;R = input resistance of the integrator in the secondarycircuit, V; andC = the feedback capacitance, F.By combining the two equat

17、ions:f5ERCK1Nor E 5fNK1RC(4)If the voltage, E, is applied to the Y axis of an X-Y recorder,the Y deflection of the pen is proportional to the flux, f.3.1.2 Measurements of magnetic field strength and flux bythe hysteresigraph method is illustrated in the block diagram ofFig. 1. The system consists o

18、f a magnetizing power source, anexciting current controller, an electronic flux integrator, and adata recorder. As exciting current is applied to the coil, avoltage proportional to I is produced across the shunt resistorwhich is connected in series with the primary coil. This voltagedetermines the v

19、alue of H.3.1.3 In the testing of hard magnetic materials, or softmagnetic materials in the form of wire, bars or rods, it isusually necessary to use a permeameter. This is shown in theblock diagram of Fig. 2. When using permeameters, the valueof H in the gap is generally not proportional to I that

20、flowsthrough the exciting coil of the yoke. In these cases, the valueof H is determined by integration of the electromotive forcethat is induced in an H coil (or Chattock potentiometer) or fromthe signal developed by a Hall probe which is placed near thespecimen. When using an H coil, the determinat

21、ion of H isaccomplished with an H integrator in exactly the same manneras that used to determine flux with the B integrator described in3.1. When using a Hall sensor, the H values are determinedfrom the voltage output which is proportional to H. In somecases, the H versus I relationship may be suffi

22、ciently linearfrom 0 to the coercive field strength (Hc) of the material undertest. In such cases, it is acceptable to determine the secondquadrant of the hysteresis loop by determining H from thevalue of I in the exciting winding.4. Significance and Use4.1 Hysteresigraph testing permits more rapid

23、and efficientcollection of dc hysteresis (B-H loop) data as compared to thepoint by point ballistic Test Methods A 341/A 341M andA 596/A 596M. The accuracy and precision of testing iscomparable to the ballistic methods. Hysteresigraphs are par-ticularly desirable for testing of semihard and hard mag

24、neticmaterials where either the entire second quadrant (demagneti-zation curve) or entire hysteresis loop is of primary concern.4.2 Provided the test specimen is representative of the bulksample or lot, this test method is well suited for design,specification acceptance, service evaluation and resea

25、rch anddevelopment.5. Interferences5.1 Test methods using suitable ring-type specimens are thepreferred methods for determining the basic magnetic proper-ties of a material. However, this test method has severalimportant requirements. Unless adequate inside diameter tooutside diameter ratios are mai

26、ntained in the test specimens,the magnetic field strength will be excessively nonuniformthroughout the test material and the measured parameterscannot be represented as material properties. The basic qualityof materials having directional sensitive properties cannot betested satisfactorily with punc

27、hed rings or laminations. Withthem it is necessary to use Epstein specimens cut with their4The boldface numbers in parentheses refer to a list of references at the end ofthis standard.FIG. 1 Block Diagram of Ring Test ApparatusA 773/A 773M 01 (2009)2lengths in the direction of specific interest or u

28、se longlink-shaped or spirally wound core test specimens whose longdimensions are similarly oriented. The acceptable minimumwidth of strip used in such test specimens is also sensitive tothe material under test. At present, it is believed the siliconsteels should have a strip width of at least 3 cm

29、30 mm.Unless ring specimens are large, it is difficult to providesufficient magnetizing turns or current-carrying capacity toreach high magnetic field strengths. In general, magneticmaterials tend to have nonuniform properties throughout thebody of the test specimens; for this reason, uniformly dist

30、rib-uted test windings and uniform specimen cross-sectional areaare highly desirable to average nonuniform behavior to atolerable degree.5.2 When conducting permeameter tests on bars, rods, andother appropriate specimens, this test method covers a range ofmagnetic field strengths from about 0.05 Oe

31、4 A/m up toabout 20 000 Oe 1600 kA/m or more, depending on thespecimen geometry and the particular permeameter that isused. In general, the lower limit of magnetic field strength isdetermined by the area-turns of the H coil (or the sensitivity ofthe Hall probe if it is used), the sensitivity of the

32、integrator, andthe sensitivities of the measuring and recording components.The upper limitation in magnetic field strength is determinedby the type of permeameter appropriate for the specimen, thepower supply, and the heat generated in the yoke windings.Recommendations of the useful range of magneti

33、c fieldstrength for the various permeameters are shown in Table 1.Other types may be used with appropriate precautions.5.2.1 In general, permeameters do not maintain a uniformmagnetic field in either the axial or radial directions around thetest specimen. The field gradients in both of these directi

34、onswill differ in the various permeameters.Also the H-sensing andB-sensing coils of the different permeameters are not identicalin area, in turns, or in length or identically located. Althoughtest specimens are prepared to have uniform physical crosssection, they may have undetected nonuniform magne

35、tic prop-erties radially or axially along the specimen length adjacent tothe H or B coils. Some permeameters may also introduceclamping strains into the test specimen. For these reasons testresults obtained on a test specimen with one type of permeame-ter may not compare closely with those obtained

36、on the samespecimen from another type permeameter, and both may differfrom more precise testing methods.5.2.2 The limitation in the B measurement by this testmethod is determined by the number of turns on the specimen,the cross-sectional area, the permeability, and the sensitivitiesof the B integrat

37、or and X-Y recorder. In general, normalinduction and hysteresis data may be determined from a fluxlinkage corresponding to 1000 Maxwell turns 105Weberturns to an upper induction that corresponds to the intrinsicsaturation for most materials.5.2.3 Some permeameters use compensation coils and re-quire

38、 continual adjustment of the current flowing through thesecoils. This may not be compatible with commercially availablehysteresigraphs and can be a source of significant error.FIG. 2 Block Diagram of Permeator Test ApparatusTABLE 1 Permeameters Recommended for Use WithHysteresigraphsNOTEOther permea

39、meters may be suitable for use with dc hysteresi-graphs where appropriate modifications are made. Refer to Test MethodA 341/A 341M for other permeameters.Permeameter Magnetic Field Strength Range H MeasurementDeviceOe kA/mBabbit (2, 3) 40/100 3.2/8 current, H coilFahy Simplex (4-6) 0.1/300 0.008/24

40、H coilFahy Simplex SuperH Adapter (6)100/2500 8/200 H coilIEC Type A 12/2500 1/200 H coil, Hall probeIEC Type B 12/620 1/50 H coilIsthmus (6, 7) 100/20 000 + 8/1600 + H coil, Hall probeA 773/A 773M 01 (2009)35.2.4 The magnetic test results, particularly for high perme-ability alloys, may not exactly

41、 agree with test results obtainedby the ballistic methods, Test Methods A 341/A 341M andA 596/A 596M. This is due to the influence of eddy currentsand the different nature of the magnetizing waveform betweenhysteresigraph and ballistic testing.6. Apparatus6.1 The apparatus shall consist of as many o

42、f the compo-nents described in 6.2-6.6 as required to perform the tests.6.1.1 All apparatus used in this test method shall be cali-brated against known standards to ensure the accuracy limitsgiven below.6.2 Balance or Scales:6.2.1 The balance or scales used to weigh the test specimenshall be capable

43、 of weighing to an accuracy of 0.2 %.6.2.2 The micrometer or dimensional measuring scales usedto determine specimen dimensions for calculation of cross-sectional area shall be capable of measuring to an accuracy ofat least 0.1 %.6.3 Magnetizing Power SourceThe power source mayrange from simple batte

44、ries to sophisticated regulated, low-ripple, protected, programmable types. It shall have sufficientcapacity to produce the maximum currents required for mag-netization of the specimen under test.6.4 Exciting Current ControllerInstantaneous value ofmagnetizing current, and its rate of change, may be

45、 controlledentirely manually by means of rheostats, potentiometers,shunts, reversing switches, and so forth; semiautomatically bymeans of variable-speed motors or sweep generators, and soforth; or entirely automatic by means of rate sensors, and soforth. In all cases, components shall be capable of

46、carrying therequired currents without overheating, and controls shall be ofsuch design that magnetizing current may be increased ordecreased in a uniform manner so that smooth traces areplotted on the X-Y recorder.6.5 B or H IntegratorThe flux integrator(s) may be any ofthe types described in ASTM S

47、TP 526 (or other) and shouldhave sufficient sensitivity, stability, linearity, and freedom fromdrift to ensure an accuracy of at least 0.5 % of full scale.6.6 Data RecorderThe B and H values can be recordedand displayed by either analog or digital X-Y chart recorders,dataloggers, or computers. The r

48、ecording device shall becapable of resolving B or H values of 1 % of the full-scalevalue. For analog to digital converters, twelve-bit resolution isdesirable.7. Test Specimens for Ring-Type Measurements7.1 The specifications in 7.2-7.8 cover the general case forspecimens in which magnetic field stre

49、ngth is proportional tothe exciting current, that is, H = kI.7.2 When the test specimen represents a test lot of material,its selection shall conform to the requirements of PracticeA 34/A 34M or of an individual specification.7.3 To qualify as a test specimen suitable for evaluation ofmaterial properties, the effective ratio of mean diameter toradial width shall be not less than 10 to 1 (or an inside diameterto outside diameter ratio not less than 0.82). When the testspecimen has smaller ratios than the above requirements, thetest data should not be represented as