Standard Test Method for Alternating-Current Magnetic Properties of Amorphous Materials at Power Frequencies Using Wattmeter-Ammeter-Voltmeter Method with Sheet Specimens

SIGNIFICANCE AND USE
4.1 This test method provides a satisfactory means of determining various ac magnetic properties of amorphous magnetic materials. It was developed to supplement the testing of toroidal and Epstein specimens. For testing toroidal specimens of amorphous materials, refer to Test Method A912/A912M.  
4.2 The procedures described herein are suitable for use by manufacturers and users of amorphous magnetic materials for materials specification acceptance and manufacturing control.
Note 2: This test method has been principally applied to the magnetic testing of thermally, magnetically annealed, and flattened amorphous strip at 50 and 60 Hz. Specific core loss at 13 or 14 kG [1.3 or 1.4 T], specific exciting power at 13 or 14 kG [1.3 or 1.4 T], and the flux density, B, at 1 Oe [79.6 A/m] are the recommended parameters for evaluating power grade amorphous materials.
SCOPE
1.1 This test method covers tests for various magnetic properties of flat-cast amorphous magnetic materials at power frequencies (50 and 60 Hz) using sheet-type specimens in a yoke-type test fixture. It provides for testing using either single- or multiple-layer specimens.  
Note 1: This test method has been applied only at frequencies of 50 and 60 Hz, but with proper instrumentation and application of the principles of testing and calibration embodied in the test method, it is believed to be adaptable to testing at frequencies ranging from 25 to 400 Hz.  
1.2 This test method provides a test for specific core loss, specific exciting power and ac peak permeability at moderate and high flux densities, but is restricted to very soft magnetic materials with dc coercivities of 0.07 Oe [5.57 A/m] or less.  
1.3 The test method also provides procedures for calculating ac peak permeability from measured peak values of total exciting currents at magnetic field strengths up to about 2 Oe [159 A/m].  
1.4 Explanation of symbols and abbreviated definitions appear in the text of this test method. The official symbols and definitions are listed in Terminology A340.  
1.5 This test method shall be used in conjunction with Practice A34/A34M.  
1.6 The values stated in either customary (cgs-emu and inch-pound) or SI units are to be regarded separately as standard. Within this standard, SI units are shown in brackets. The values stated in each system 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 standard.  
1.7 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, health, and environmental practices and determine the applicability of regulatory limitations prior to use.  
1.8 This international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for the Development of International Standards, Guides and Recommendations issued by the World Trade Organization Technical Barriers to Trade (TBT) Committee.

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ASTM A932/A932M-01(2019) - Standard Test Method for Alternating-Current Magnetic Properties of Amorphous Materials at Power Frequencies Using Wattmeter-Ammeter-Voltmeter Method with Sheet Specimens
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This international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for the
Development of International Standards, Guides and Recommendations issued by the World Trade Organization Technical Barriers to Trade (TBT) Committee.
Designation: A932/A932M − 01 (Reapproved 2019)
Standard Test Method for
Alternating-Current Magnetic Properties of Amorphous
Materials at Power Frequencies Using Wattmeter-Ammeter-
Voltmeter Method with Sheet Specimens
This standard is issued under the fixed designationA932/A932M; the number immediately following the designation indicates the year
of original adoption or, in the case of revision, the year of last revision.Anumber in parentheses indicates the year of last reapproval.
A superscript epsilon (´) indicates an editorial change since the last revision or reapproval.
1. Scope responsibility of the user of this standard to establish appro-
priate safety, health, and environmental practices and deter-
1.1 This test method covers tests for various magnetic
mine the applicability of regulatory limitations prior to use.
properties of flat-cast amorphous magnetic materials at power
1.8 This international standard was developed in accor-
frequencies (50 and 60 Hz) using sheet-type specimens in a
dance with internationally recognized principles on standard-
yoke-type test fixture. It provides for testing using either
ization established in the Decision on Principles for the
single- or multiple-layer specimens.
Development of International Standards, Guides and Recom-
NOTE 1—This test method has been applied only at frequencies of 50
mendations issued by the World Trade Organization Technical
and 60 Hz, but with proper instrumentation and application of the
Barriers to Trade (TBT) Committee.
principles of testing and calibration embodied in the test method, it is
believed to be adaptable to testing at frequencies ranging from 25 to
2. Referenced Documents
400Hz.
2.1 ASTM Standards:
1.2 This test method provides a test for specific core loss,
A34/A34MPractice for Sampling and Procurement Testing
specific exciting power and ac peak permeability at moderate
of Magnetic Materials
and high flux densities, but is restricted to very soft magnetic
A340Terminology of Symbols and Definitions Relating to
materials with dc coercivities of 0.07 Oe [5.57 A/m] or less.
Magnetic Testing
1.3 Thetestmethodalsoprovidesproceduresforcalculating
A343/A343MTest Method for Alternating-Current Mag-
ac peak permeability from measured peak values of total
netic Properties of Materials at Power Frequencies Using
exciting currents at magnetic field strengths up to about 2 Oe
Wattmeter-Ammeter-Voltmeter Method and 25-cm Ep-
[159 A/m].
stein Test Frame
A876Specification for Flat-Rolled, Grain-Oriented, Silicon-
1.4 Explanation of symbols and abbreviated definitions
Iron, Electrical Steel, Fully Processed Types
appear in the text of this test method.The official symbols and
A901Specification for Amorphous Magnetic Core Alloys,
definitions are listed in Terminology A340.
Semi-Processed Types
1.5 This test method shall be used in conjunction with
A912/A912MTest Method for Alternating-Current Mag-
Practice A34/A34M.
netic Properties of Amorphous Materials at Power Fre-
1.6 The values stated in either customary (cgs-emu and
quencies Using Wattmeter-Ammeter-Voltmeter Method
inch-pound) or SI units are to be regarded separately as
with Toroidal Specimens
standard. Within this standard, SI units are shown in brackets.
3. Terminology
Thevaluesstatedineachsystemmaynotbeexactequivalents;
therefore,eachsystemshallbeusedindependentlyoftheother.
3.1 The definitions of terms, symbols, and conversion fac-
Combiningvaluesfromthetwosystemsmayresultinnoncon- tors relating to magnetic testing, used in this test method, are
formance with this standard.
found in Terminology A340.
1.7 This standard does not purport to address all of the
3.2 Definitions of Terms Specific to This Standard:
safety concerns, if any, associated with its use. It is the
3.2.1 sheet specimen—arectangularspecimencomprisedof
a single piece of material or parallel multiple strips of material
arranged in a single layer.
This test method is under the jurisdiction of ASTM Committee A06 on
MagneticPropertiesandisthedirectresponsibilityofSubcommitteeA06.01onTest
Methods. For referenced ASTM standards, visit the ASTM website, www.astm.org, or
Current edition approved Oct. 1, 2019. Published October 2019. Originally contact ASTM Customer Service at service@astm.org. For Annual Book of ASTM
approved in 1995. Last previous edition approved in 2012 as A932/A932M–01 Standards volume information, refer to the standard’s Document Summary page on
(2012). DOI:10.1520/A0932_A0932M-01R19. the ASTM website.
Copyright © ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States
A932/A932M − 01 (2019)
3.2.2 specimen stack—testspecimens(asin3.2.1)arranged additional strip in the stack. Moreover, the active length for
in a stack two or more layers high. stacked strips tends to vary from sample to sample. As the
stack height increases, the error as a result of cross-sectional
4. Significance and Use
variations diminishes but that as a result of length variations
increases with the overall optimum at about four to six layers.
4.1 This test method provides a satisfactory means of
The accuracy for stacked strips is never as good as for a single
determining various ac magnetic properties of amorphous
layer of smooth strip.
magneticmaterials.Itwasdevelopedtosupplementthetesting
of toroidal and Epstein specimens. For testing toroidal speci-
5.2 Some amorphous magnetic materials are highly magne-
mens of amorphous materials, refer to Test Method A912/
tostrictive. This is an additional potential source of error
A912M.
because even a small amount of surface loading, twisting, or
flattening will cause a noticeable change in the measured
4.2 The procedures described herein are suitable for use by
values.
manufacturers and users of amorphous magnetic materials for
materials specification acceptance and manufacturing control.
6. Basic Test Circuit
NOTE 2—This test method has been principally applied to the magnetic
6.1 Fig. 1 provides a schematic circuit diagram for the test
testingofthermally,magneticallyannealed,andflattenedamorphousstrip
method.Apowersourceofpreciselycontrollableacsinusoidal
at 50 and 60 Hz. Specific core loss at 13 or 14 kG [1.3 or 1.4 T], specific
voltage is used to energize the primary circuit. To minimize
exciting power at 13 or 14 kG [1.3 or 1.4 T], and the flux density, B,at1
flux-waveform distortion, current ratings of the power source
Oe [79.6 A/m] are the recommended parameters for evaluating power
grade amorphous materials. and of the wiring and switches in the primary circuit shall be
such as to provide very low impedance relative to the imped-
5. Interferences
ance arising from the test fixture and test specimen. Ratings of
switches and wiring in the secondary circuit also shall be such
5.1 Because amorphous magnetic strip is commonly less
than 0.0015 in. [0.04 mm] thick, surface roughness tends to astocausenegligiblevoltagedropbetweentheterminalsofthe
secondary test winding and the terminals of the measuring
have a large effect on the cross-sectional area and the cross
instruments.
sectioninsomeareascanbelessthanthecomputedaverage.In
suchcases,thetestresultsusingasingle-stripspecimencanbe
7. Apparatus
substantially different from that measured with a stack of
7.1 The test circuit shall incorporate as many of the follow-
several strips. One approach to minimize the error caused by
ing components as are required to perform the desired mea-
surface roughness is to use several strips in a stack to average
surements.
out the variations. The penalty for stacking is that the active
magnetic path length of the specimen stack becomes poorly 7.2 YokeTestFixture—Fig.2showsalinedrawingofayoke
defined. The variation of the active length increases with each fixture. Directions concerning the design, construction, and
FIG. 1 Basic Block Circuit Diagram of the Wattmeter Method
A932/A932M − 01 (2019)
ing voltmeter, with scale readings in average volts times π
.=2/4 so that its indications will be identical with those of a
true rms voltmeter on a pure sinusoidal voltage, shall be
provided for evaluating the peak value of the test flux density.
To produce the estimated precision of test under this test
method, the full-scale meter errors shall not exceed 0.25%
(Note3).Eitherdigitaloranalogfluxvoltmetersarepermitted.
Use of a digital flux voltmeter with high input impedance
(typically, 10 MΩ) is recommended to minimize loading
effects and to reduce instrument loss compensation. If an
analog flux voltmeter is used, its input resistance shall be
greaterthen10000Ω/Voffull-scaleindication.Voltageranges
FIG. 2 Single-Yoke Fixture (Exploded View)
and number of significant digits shall be consistent with the
accuracy specified above. Care shall be taken to avoid errors
caused by temperature and frequency effects in the instrument.
calibration of the fixture are given in 7.2.1, 7.2.2, Annex A1,
Annex A2, and Annex A3. NOTE3—Inaccuraciesinsettingthetestvoltageproduceerrorsapproxi-
mately two times as large in the specific core loss.
7.2.1 Yoke Structure—Various dimensions and fabrication
procedures in construction are permissible. Since the recom-
7.5 RMS Voltmeter, V —A true rms-indicating voltmeter
rms
mended calibration procedure requires correlation with the
shall be provided for evaluating the form factor of the voltage
25-cm Epstein test, the minimum inside dimension between
induced in the secondary winding of the test fixture and for
pole faces must be at least 22 cm [220 mm]. The thickness of
evaluating the instrument losses. The accuracy of the rms
the pole faces should be not less than 2.5 cm [25 mm]. To
voltmeter shall be the same as specified for the flux voltmeter.
minimize the influences of coil-end and pole-face effects, the
Either digital or analog rms voltmeters are permitted. The
yokes should be thicker than the recommended minimum. For
normally high input impedance of digital rms voltmeters is
calibrationpurposes,itissuggestedthatthewidthofthefixture
desirable to minimize loading effects and to reduce the mag-
be at least 12.0 cm [120 mm] which corresponds to the
nitude of instrument loss compensations. The input resistance
combined width of four Epstein-type specimens.
of an analog rms voltmeter shall not be less than 10000 Ω/V
7.2.2 Test Windings—The test windings, which shall consist
of full-scale indication.
of a primary (exciting) winding and a secondary (potential)
7.6 Wattmeter, W—The full-scale accuracy of the wattmeter
winding, shall be uniformly and closely wound on a
shall not be lower than 0.25% at the test frequency and unity
nonmagnetic, nonconducting coil form and each shall span the
power factor. The power factor encountered by a wattmeter
greatest possible distance between the pole faces of the yoke
during a core loss test on a specimen is always less than unity
fixture. It is recommended that the number of turns in the
and, at flux densities far above the knee of the magnetization
primaryandsecondarywindingsbeequal.Thenumberofturns
curve, approaches zero. The wattmeter must maintain 1.0%
may be chosen to suit the instrumentation, mass of specimen,
accuracy at the lowest power factor which is presented to it.
and test frequency. The secondary winding shall be the
Variablescalingdevicesmaybeusedtocausethewattmeterto
innermost winding. The primary and secondary turns shall be
indicatedirectlyinunitsofspecificcorelossifthecombination
wound in the same direction from a common starting point at
of basic instruments and scaling devices conforms to the
oneendofthecoilform.Also,tominimizeself-impedancesof
specifications stated here.
thewindings,theopeninginthecoilformshouldbenogreater
7.6.1 Electronic Digital Wattmeter—An electronic digital
than that required to allow easy insertion of the test specimen.
wattmeter is preferred in this test method because of its digital
Construction and mounting of the test coil assembly must be
readout and its capability for direct interfacing with electronic
such that the test specimen will be maintained without me-
data acquisition systems. A combination true rms voltmeter-
chanicaldistortionintheplaneestablishedbythepolefacesof
wattmeter-rms ammeter is acceptable to reduce the number of
the yoke(s) of the test fixture.
instruments connected in the test circuit.
7.3 Air-Flux Compensator—To provide a means of deter-
7.6.1.1 The voltage input circuitry of the electronic digital
mining intrinsic flux density in the test specimen, an air-core
wattmeter must have an input impedance sufficiently high so
mutual inductor shall constitute part of the test-coil system.
that connection to the secondary winding of the test fixture
The respective primary and secondary windings of the air-core
during testing does not change the terminal voltage of the
inductorandthetest-specimencoilshallbeconnectedinseries
secondary by more than 0.05%. Also, the voltage input
andthevoltagepolaritiesofthesecondarywindingsshallbein
circuitry must be capable of accepting the maximum peak
opposition. By proper adjustment of the mutual inductance of
voltage which is induced in the secondary winding during
the air-core inductor, the average voltage developed across the
testing.
combined secondary windings is proportional to the intrinsic
7.6.1.2 The current input circuitry of the electronic digital
flux density in the test specimen. Directions for construction
wattmeter should have as low an input impedance as possible,
and adjustment of the air-core mutual inductor for air flux are
preferably no more than 0.1 Ω, otherwise the flux waveform
found in Annex A3.
distortion tends to be excessive. The effect of moderate
7.4 Flux Voltmeter, V—A full-wave, true average respond- waveform distortion is addressed in 10.3. The current input
f
A932/A932M − 01 (2019)
circuitry must be capable of accepting the maximum rms peak value of the voltage drop that results when the exciting
current and the maximum peak current drawn by the primary current flows through a standard resistance of low value
winding of the test transformer when core loss tests are being connected in series with the primary winding of the test
performed. In particular, since the primary current will be very transformer. This peak-to-peak reading voltmeter shall have a
nonsinusoidal (peaked) if core loss tests are performed on a nominalfull-scaleaccuracyofatleast3%atthetestfrequency
specimen at flux densities above the knee of the magnetization and be able to accommodate voltage with a crest factor of 5 or
curve, the crest factor capability of the
...

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