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ASTM A341 – A341M – 95

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ASTM A341 – A341M – 95 Designation: A 341/A341M – 9500 An American National Standard Standard Test Method for Direct Current Magnetic Properties of Materials Using D-C Permeameters and the Ballistic Test Methods1 This standard is issued under the fixed designation A 341/A341M; the numb...
ASTM A341 – A341M – 95
Designation: A 341/A341M – 9500 An American National Standard Standard Test Method for Direct Current Magnetic Properties of Materials Using D-C Permeameters and the Ballistic Test Methods1 This standard is issued under the fixed designation A 341/A341M; the number immediately following the designation indicates the year of 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 (e) indicates an editorial change since the last revision or reapproval. 1. Scope 1.1 This test method provides dc permeameter tests for the basic magnetic properties of materials in the form of bars, rods, wire, or strip specimens which may be cut, machined, or ground from cast, compacted, sintered, forged, extruded, rolled, or other fabricated materials. It includes tests for determination of the normal induction under symmetrically cyclically magnetized (SCM) conditions and the hysteresis loop (B-H loop) taken under conditions of rapidly changing or steep wavefront reversals of the direct current magnetic field strength. 1.2 This test method shall be used in conjunction with Practice A 34/A 34M. 1.3 This test method covers a range of magnetic field strength in the specimen from about 0.05 Oe [4 A/m] up to above 5000 Oe [400 kA/M] through the use of several permeameters. The separate permeameters cover this test region in several overlapping ranges. 1.4 Normal induction and hysteresis properties may be determined over the flux density range from essentially zero to intrinsic saturation for most materials. 1 This test method is under the jurisdiction of ASTM Committee A-6 A06 on Magnetic Properties and is the direct responsibility of Subcommittee A06.01 on Test Methods. Current edition approved Feb. 15, 1995. Oct. 10, 2000. Published April 1995. December 2000. Originally published as A 341 – 69. Last previous edition A 341 – 89e 1 A 341/A 341M – 95. 1 This document is not an ASTM standard and is intended only to provide the user of an ASTM standard an indication of what changes have been made to the previous version. Because it may not be technically possible to adequately depict all changes accurately, ASTM recommends that users consult prior editions as appropriate. In all cases only the current version of the standard as published by ASTM is to be considered the official document. Copyright © ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States. 1.5 Recommendations of the useful magnetic field strength range for each of the permeameters are shown in Table 12. Also, see Sections 3 and 4 for general limitations relative to the use of permeameters. 1.6 The symbols and abbreviated definitions used in this test method appear with Fig. 1 and in appropriate sections of this document. For the official definitions, see Terminology A 340. Note that the term flux density used in this document is synonymous with the term magnetic induction. 1.7 The values and equations stated in either customary (absolute (or practical) cgs-emu and inch-pound) units inch-pound or SI units are to be regarded separately as standard. Within this test method, the standard, SI units are shown in brackets except for the sections concerning calculations where there are separate sections for the respective unit systems. The values stated in each system are may not be exact equivalents; therefore, each system shall be used independently of the other. Combining values from the two systems may result in nonconformance with this specification. standard. 1.8 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use. 2 use. 2 The boldface numbers in parentheses refer to a list of references at the end of this standard. A 341/A341M – 9500 2 2. Referenced Documents 2.1 ASTM Standards: A 34/A 34M Practice for Procurement, Testing and Sampling and Procurement Testing of Magnetic Materials3 A 340 Terminology of Symbols and Definitions Relating to Magnetic Testing3 A 596/A 596M Test Method for Direct-Current Magnetic Properties of Materials Using the Ballistic Method and Ring Specimens 3 A 773 Test Method for dc Magnetic Properties of Materials Using Ring and Permeameter Procedures with dc Electronic Hysteresigraphs Specimens3 2.2 IEC Standard: Publication 60404-4, Ed. 2.0 Magnetic Materials – Part 4: Methods of Measurement of the D-C D.C. Magnetic Properties of Solid Iron and Steel, IEC, 1982. 19954 2.3 Other Documents: 5 NIST Circular No. 74, pg. 269.5 3 Annual Book of ASTM Standards, Vol 03.04. 4 Available from American National Standards Institute, 11 W. 42nd St., 13th Floor, New York, NY 10036. 5 Available from National Institute of Standards and Technology, (NIST), Gaithersburg, MD 20899. TABLE 1 Permeameters Permeameter Useful Magnetizingc Foield Strcength Range A H Measuring Device B Reluctance Comp.ensation Magnetizing Coils Surrounds Specimen References 52 Oersteds kA/M m Babbit 40/1 000 3 200/80 000 I, HC yes yes (1,2) Babbit 40/1000 3.2/80 I, HC yes yes (1,2) Burroughs 0.1/300 8/24 000 I yes yes (1,3,4,5) Burroughs 0.1/300 0.008/24 I yes yes (1,3,4,5) Fahy Simplex C 0.1/300 8/24 000 HC no no (1,4,5,6,7) Fahy SimplexC 0.1/300 0.008/24 HC no no (1,4,5,6,7) Fahy Simplex Super H Adapter C 100/2 500 8 000/200 000 HC no no (1,3) Fahy Simplex Super H adapterC 100/2500 8/200 HC no no (1,3) Full Range 0.05/1 400 4/1 100 HC yes yes (1,8) Full range 0.05/1400 0.004/112 HC yes yes (1,8) High H D 100/5 000 8 000/400 000 FC yes no (1,5,7,9) High H 100/5000 8/400 FC yes no (1,5,7,9) Iliovici D 0.5/500 40/400 000 I, HC yes yes (4,10,11) Iliovici 0.5/500 0.04/400 I, HC yes yes (4,10,11) Isthmus 100/20 000 + 8 000/1 600 000 + HC, HP no yes IEC 60404-4 IEC Type A 0.1/2500 0.008/200 HC, HP no yes IEC 60404-4 IEC Type B 0.1/630 0.008/50 RCC no no IEC 60404-4 Isthmus 100/20 000+ 8/1600+ HC, HP no no (1,4,12,13) MH D 0.1/300 8/2 400 FC yes yes (1,6,14) MH 0.1/300 0.008/24 FC yes yes (1,6,14) NPL D 0.5/2 500 40/200 000 I, HC yes yes (15) NPL 0.5/2500 0.04/200 I, HC yes yes (15) Saturation 100/4 000 8 000/400 000 HC no yes (5,16,17) Saturation 100/4000 8/320 HC no yes (5,16,17) AAlthough the permeameters are capable of being used at the lower end of the measurement range, the measurement accuracy is reduced. Best overall accuracy is obtained for a combination of high flux density and high magnetic field strength such as is encountered in the testing of permanent magnet materials. B I—magnetizing current; HC—fixed H- coil; FC—flip coil; HP—Hall Probe.RCC—Rogowski-Chattock coil. C Fahy permeameters require a standard of known magnetic properties for calibration of the H- coil. D These permeameters are recommended by the International Electrotechnical Commission. A 341/A341M – 9500 3 NIST Scientific Paper 117, SPBTA5 3. Significance and Use 3.1 Permeameters require the use of yokes to complete the magnetic circuit and are therefore inherently less accurate than ring test methods. Refer to Test Method A 596/A 596M for further details on ring test methods. However, when testing certain shapes as bars or when magnetic field strength in excess of 200 Oe [15.9 or more kA/m] are required, permeameters are the only practical means of measuring magnetic properties. 3.2 This test method is suitable for specification acceptance, service evaluation, research and development and design. 3.3 When the test specimen is fabricated from a larger sample and is in the same condition as the larger sample, it may not exhibit magnetic properties representative of the original sample. In such instances the test results, when viewed in context of past performance history, will be useful for judging the suitability of the material for the intended application. 4. Interferences 4.1 In general, permeameters do not maintain a uniform magnetic field in either the axial or radial directions around the test specimen. The field gradients in both of these directions will differ in the various permeameters. Also the H-sensing and B-sensing coils of the different permeameters are not identical in area, in turns, or in length or identically located. Although test specimens are prepared to have uniform physical cross section, they may have undetected nonuniform magnetic properties radially or axially along the specimen length adjacent to the H- H or B- coils. Some permeameters may also introduce clamping strains into the test specimen. For the above reasons test results obtained on a test specimen with one type permeameter may not agree closely with those obtained on the same test specimen using another type of permeameter. 5. Apparatus 5.1 DBecause t of the differences in physical construction of the various permeameters listed in Table 1, no standard list of components is given. When used with a particular type of permeameter, the components should conform to the general requirements listed below. A basic schematic of a permeameter is shown in Fig. 1. 5.2 Permeameter—The particular permeameter used shall be of high quality construction. The yokes should be made of high permeability alloy such as oriented or nonoriented silicon iron or nickel-iron alloy, although low carbon steel or iron is acceptable in certain instances. The preferred yolk dimensions are listed in the appended references (see Table 1). Deviations from these dimensions should be such that the yolk is operating at or below the point of maximum permeability for the highest test flux densities encountered. Yoke construction may consist of either stacked laminations or stripwound C- cores suitably bolted or adhesive bonded together. 5.3 Power Supply—The magnetizing current shall be supplied by either storage batteries or dc power supplies. Bipolar programmable linear power supplies have been found to be well suited for this use. The source of dc current must be stable, have NOTE 1— A1—Multirange ammeter (main current) A2—Multirange ammeter (hysteresis current) B—Flux density test position for switch S3 F—Electronic Integrator H—Magnetic field strength test position for switch S3 N1—Magnetizing coil N2—Flux sensing (B) coil N3—Magnetic field strength sensing coil R1—Main current control rheostat R2—Hysteresis current control rheostat S1—Reversing switch for magnetizing current S2—Shunting switch for hysteresis current control rheostat S3—Integrator selector switch SP—Specimen FIG. 1 Basic Circuit Using Permeameter A 341/A341M – 9500 4 negligible ripple and be capable of quickly returning to the stable state after switching. When programmable power supplies are used, either digital or analog programming signals are permissible provided that equal but opposite polarity current cycling is possible. 5.4 Main-Current-Control Rheostats, R1—When used, these rheostats must have sufficient power rating and heat-dissipating capacity to handle the voltage and largest test current and must contain sufficient resistance to limit the test currents to those required for the lowest magnetic field strength to be used. 5.5 Hysteresis-Current-Control Rheostats, R2—When used, these rheostats must have the same characteristics as the main-current control rheostats. 5.6 Main-Current Ammeter, A1—Magnetizing current measurement shall be conducted using a digital ammeter or combination of a digital voltmeter and precision shunt resistor with an overall accuracy of better than 0.25 % when the magnetic field strength will be determined from the current. In those permeameters where the magnetic field strength is determined by other means, such as Hall probes or H- coils, lower accuracy analog instruments can be used. In such permeameters, the ammeter is used to prevent excessive currents from being applied and, based on past experience, to roughly establish the required magnetic field strength. 5.7 Hysteresis-Current- Ammeter, A2—The requirements of 5.6 shall apply. In general, a separate ammeter is not required. 5.8 Reversing Switch, S1—When nonprogrammable dc current sources such as storage batteries are used, a current reversing switch is required. The reversing switch should be either a high quality knife switch, mechanical or electrical solenoid-operated contractors or mercury switches having high current rating and the ability to maintain uniform contact resistance of equal magnitude in both current directions. Switches with contact bounce or other multiple contacting behavior on make or break must be avoided. Due to Because of the presence of leakage currents in the open condition, solid state relays are not permitted. 5.9 Hysteresis Switch, S2—This single pole switch must conform to the same requirements as the reversing s Switch, S1. 5.10 Integrator, F—Due to—Because of their superior accuracy, stability, and ease of operation, electronic charge integrators are the preferred means of measuring magnetic flux. Integrators using either operational amplifier and capacitor feedback (analog integrator) or pulse counting are permitted. The accuracy of the integrator must be better than 1 % full scale. If analog display meters are used to read the value of flux, the measurement should be made on the upper two-thirds of the scale. Analog integrators must have drift adjust circuitry and the drift should not exceed 100 Maxwell-turns [10−6 Wb-turns] per minute on the most sensitive range. It is also desirable that the integrator have appropriate scaling circuitry to permit direct reading of either flux (f) or flux density (B). Ballistic galvanometers or moving coil fluxmeters are permitted provided the 1 % full-scale accuracy requirement is met. Such devices require additional circuitry not shown in Fig. 1. Details may be found in the appropriate references appended to this test method. 5.11 B- Coils—Prewound fixed flux sensing coils are often used. When used, the cross-sectional area enclosed by the secondary winding and number of turns must be known to be better than 0.5 %. 5.12 Magnetic Field Strength Measuring Devices—Certain permeameters do not or cannot use the magnetizing current to accurately determine the magnetic field strength accurately. Such permeameters instead use stationary H- coils, flip- coils, or Hall probes. When such devices are used, they shall be capable of determining the apparent magnetic field strength to accuracy of 1.0 % or better. 6. Test Specimens 6.1 Test specimen area shall normally be determined from mass, length, and density as indicated in 9.1 and 10.1. When the test specimen is machined or ground to have a very smooth surface, the physical dimensions obtained from micrometer measurements may be used to calculate the cross-sectional area. 6.2 Test specimens in bar form may be of round, square, or rectangular cross-sectional shape. In some permeameters the bar specimen may be a half round or any shape having a uniform cross-sectional area. Certain permeameters must have a good magnetic joint between the ends of the test specimen and the permeameter yoke or pole faces. Pole shoes may be necessary to create this joint. Generally, to achieve a good magnetic joint, the test specimen must be of square or rectangular cross section and must be machined or ground to have straight and parallel surfaces. For permeameters using specimens butted to pole pieces, the specimen ends must be smooth and parallel. 6.3 When the material is in flat-rolled form and is to be evaluated as half transverse-half longitudinal, the specimen shall be sheared to have strips in multiples of four in accordance with Table 2. When material is to be evaluated in one direction, it shall conform to this table or to the requirements for best test quality in a particular permeameter. For gages No. 33 and thinner, the cross-sectional area shall be not less than 0.31 in.2 [200 mm2]] and not more than 0.62 in.2 [400 mm2]. ]. 6.4 When the test specimen for strip materials is to be half transverse and half longitudinal, the strips shall be positioned to be TABLE 2 Number of Test Strips Nominal Thickness Gage Number Number of Stripsin. mm 0.0100 to 0.0250 0.254 to 0.635 32 to 24, incl 12 0.0280 to 0.0435 0.711 to 1.105 23 to 19, incl 8 0.0500 and over 1.27 and over 18 and thicker 4 A 341/A341M – 9500 5 composed of alternately transverse and longitudinal throughout the specimen and a transverse strip shall be placed adjacent to the permeameter’s yoke or pole face. 6.5 For full testing accuracy, the length and size of the test specimen must meet the requirements of the permeameter being used. Generally, for most permeameters, a test specimen length of 10 in. [0.254 m] or more is required. Shorter specimens with some permeameters will require the use of pole-piece extensions, and may cause a reduction in testing accuracy. Other permeameters are designed for short specimens without loss of testing accuracy. 6.6 All test specimen forms shall be cut, machined, or ground to have a uniform cross-sectional area along the active length of the test specimen. The cross-sectional area shall be sufficiently uniform so that its nonuniformity will not materially affect the accuracy of establishing and measuring flux density in the test sample. 6.7 When required for development of material properties the test specimen shall have received a stress relief or other heat treatment after preparation. This anneal is subject to agreement between manufacturer and purchaser; manufacturer’s recommendation; or the recommended heat treatment provided by the appropriate ASTM standard for the material. The heat treatment used shall be reported with the magnitude test results. 6.8 Specimens of permanent-magnetic materials shall be processed prior to before testing in accordance with a procedure acceptable to both manufacturer and purchaser. The processing used shall be reported with the test results. 7. Calibration 7.1 Integrator—Practical operating experience has shown that provided a proper warmup period is allowed, electronic integrators require infrequent calibration and unlike ballistic galvanometers, calibration is not an integral part of this test method. When calibration is required, it can be accomplished with either a mutual inductor or a volt-second source. Due to Because of their traceability to the fundamental units of voltage and time, volt-second sources are the preferred means of calibration. The accuracy of either the mutual inductor or volt-second source must be better than the rated full scale accuracy of the integrator. 7.2 Fixed B- B and H- Coils—The effective area turns of such search coils can be determined by comparison with a coil of known area- turns or by individual calibration in a series of known magnetizing fields. Such fields can be obtained using either long solenoid electromagnetics or large Helmholtz coil systems. 7.3 Comparison Permeameters—Certain types of permeameters such as the Fahy permeameter require a standard specimen of known magnetic properties in order to derive the relationship between field sensor output and true magnetic field strength. Instead of nationally recognized standard specimens, a standard may be developed by mutual agreement between manufacturer and purchaser, and if possible, a referee laboratory. 8. Procedure 8.1 Most permeameters utilize use a compensating system of magnetizing coils to provide extra magnetomotive force to overcome the reluctance of the yokes and joints in the magnetic circuit. Hence, the detailed operation procedure will vary somewhat with the type of permeameter used. Detailed operating procedures can be found in the references appended to this test method. The procedure listed below is common to all types of permeameters. 8.2 In Fig. 1, the dc power source supplies testing current measured by ammeter
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