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ASTM A340-03a

(Terminology)

Standard Terminology of Symbols and Definitions Relating to Magnetic Testing

Standard Terminology of Symbols and Definitions Relating to Magnetic Testing

General Information

Status
Historical
Publication Date
09-Jun-2003
ICS
29.030 - Magnetic materials
Technical Committee
A06 - Magnetic Properties
Drafting Committee
A06.92 - Terminology and Definitions
Current Stage
Ref Project

Relations

Replaces
ASTM A340-03 - Standard Terminology of Symbols and Definitions Relating to Magnetic Testing
Effective Date
10-Jun-2003
Replaced By
ASTM A340-03a(2011) - Standard Terminology of Symbols and Definitions Relating to Magnetic Testing
Effective Date
01-May-2011
Referred By
ASTM A904-20 - Standard Specification for 50 Nickel-50 Iron Powder Metallurgy Soft Magnetic Parts
Effective Date
10-Jun-2003
Referred By
ASTM A912/A912M-11(2019) - Standard Test Method for Alternating-Current Magnetic Properties of Amorphous Materials at Power Frequencies Using Wattmeter-Ammeter-Voltmeter Method with Toroidal Specimens
Effective Date
10-Jun-2003
Referred By
ASTM A726-18 - Standard Specification for Cold-Rolled Magnetic Lamination Quality Steel, Semiprocessed Types
Effective Date
10-Jun-2003
Referred By
ASTM A1101-16 - Standard Specification for Sintered and Fully Dense Neodymium Iron Boron (NdFeB) Permanent Magnets
Effective Date
10-Jun-2003
Referred By
ASTM A1070-16(2022) - Standard Specification for Cast and Sintered Alnico Permanent Magnets
Effective Date
10-Jun-2003
Referred By
ASTM A1013-00(2020) - Standard Test Method for High-Frequency (10 kHz-1 MHz) Core Loss of Soft Magnetic Core Components at Controlled Temperatures Using the Voltmeter-Ammeter-Wattmeter Method
Effective Date
10-Jun-2003
Referred By
ASTM A889/A889M-14(2020) - Standard Test Method for Alternating-Current Magnetic Properties of Materials at Low Magnetic Flux Density Using the Voltmeter-Ammeter-Wattmeter-Varmeter Method and 25-cm Epstein Frame
Effective Date
10-Jun-2003
Referred By
ASTM A677-16 - Standard Specification for Nonoriented Electrical Steel Fully Processed Types
Effective Date
10-Jun-2003
Referred By
ASTM A804/A804M-04(2021) - Standard Test Methods for Alternating-Current Magnetic Properties of Materials at Power Frequencies Using Sheet-Type Test Specimens
Effective Date
10-Jun-2003
Referred By
ASTM A1126-23 - Standard Specification for Magnetic Pure Iron
Effective Date
10-Jun-2003
Referred By
ASTM A598/A598M-02(2022) - Standard Test Method for Magnetic Properties of Magnetic Amplifier Cores
Effective Date
10-Jun-2003
Referred By
ASTM A345-19 - Standard Specification for Flat-Rolled Electrical Steels for Magnetic Applications
Effective Date
10-Jun-2003
Referred By
ASTM F2978-20 - Standards Guide to Optimize Scan Sequences for Clinical Diagnostic Evaluation of Metal-on-Metal Hip Arthroplasty Devices using Magnetic Resonance Imaging
Effective Date
10-Jun-2003

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ASTM A340-03a - Standard Terminology of Symbols and Definitions Relating to Magnetic TestingASTM A340-03a - Standard Terminology of Symbols and Definitions Relating to Magnetic Testing
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ASTM A340-03a - Standard Terminology of Symbols and Definitions Relating to Magnetic Testing
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Standards Content (Sample)

NOTICE: This standard has either been superseded and replaced by a new version or withdrawn.
Contact ASTM International (www.astm.org) for the latest information
Designation: A340 – 03a
Standard Terminology of
1
Symbols and Definitions Relating to Magnetic Testing
This standard is issued under the fixed designation A340; 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 (´) indicates an editorial change since the last revision or reapproval.
INTRODUCTION
In preparing this glossary of terms, an attempt has been made to avoid, where possible, vector
analysisanddifferentialequationssoastomakethedefinitionsmoreintelligibletotheaverageworker
in the field of magnetic testing. In some cases, rigorous treatment has been sacrificed to secure
simplicity, but it is believed that none of the definitions will prove to be misleading.
It is the intent of this glossary to be consistent in the use of symbols and units with those found in
ANSI/IEEE 260-1978 and USA Standard Y10.5-1968.
Part 1—Symbols Used in Magnetic Testing
Symbol Term H biasing magnetic field strength
b
H coercive field strength
c
a cross-sectional area of B coil H intrinsic coercive field strength
ci
A cross-sectional area of specimen H coercivity
cs
A8 solid area H demagnetizing field strength
d
H incremental magnetic field strength
magnetic induction D
H
B magnetic flux density H air gap magnetic field strength
g
H ac magnetic field strength (from an assumed
L
DB excursion range of induction
peak value of magnetizing current
B · biased induction
b
H maximum magnetic field strength in a
m
B remanent induction
d
hyster esis loop
B remanence
dm
H maximum magnetic field strength in a
max
B H energy product
d d
flux- current loop
(B H ) maximum energy product
d d m
H ac magnetic field strength (from a measured
p
B incremental induction
D
peak value of exciting current)
B intrinsic induction
i
H instantaneous magnetic field strength (coinci-
t
B maximum induction in a hysteresis loop
m
dent with B )
max
B maximum induction in a flux current loop
max
H ac magnetic field strength force (from an as-
z
B residual induction
r
sumed peak value of exciting current)
B retentivity
rs
I ac exciting current (rms value)
B saturation induction
s
I ac core loss current (rms value)
c
cf crest factor
I constant current
dc
CM cyclically magnetized condition
I ac magnetizing current (rms value)
m
d lamination thickness
J magnetic polarization
D demagnetizing coefficient
B
k8 coupling coefficient
df distortion factor
, flux path length
D magnetic dissipation factor
m
, effective flux path length
1
E exciting voltage
, gap length
g
E induced primary voltage
1
+ (also f N) flux linkage
E induced secondary voltage
2
+ mutual flux linkage
m
E flux volts
f
L self inductance
f cyclic frequency in hertz
L core inductance
1
^ magnetomotive force
L incremental inductance
D
ff form factor
L intrinsic inductance
i
H magnetic field strength
L mutual inductance
m
DH excursion range of magnetic field strength
L initial inductance
0
L series inductance
s
L winding inductance
w
1
m magnetic moment
This terminology is under the jurisdiction of ASTM Committee A06 on
M magnetization
Magnetic Properties and is the direct responsibility of Subcommittee A06.92 on
m total mass of a specimen
Terminology and Definitions.
m active mass of a specimen
1
Current edition approved June 10, 2003. Published July 2003. Originally
N demagnetizing factor
D
approved in 1949. Last previous edition approved in 2003 as A340–03. DOI:
10.1520/A0340-03A.
Copyright © ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.
1

---------------------- Page: 1 ----------------------
A340 – 03a
N turns in a primary winding g proton gyromagnetic ratio
1 p
N turns in a secondary winding G magnetic constant
2 m
N I/, ac excitation d density
1 1
p magnetic pole strength k susceptibility
3 permeance ac Permeabilities:
P active (real) power µ ideal permeability
a
P apparent power µ inductance permeability
a L
P specific apparent power µ L incremental inductance permeability
a (B;f) D
µ initial dynamic permeability
0d
P total core loss µ peak permeability
c p
P specific core loss µ incremental peak permeability
c (B;f) Dp
µ instantaneous permeability
i
P incremental core loss µ impedance permeability
cD
z
P normal eddy current core loss
µ incremental impedance permeability
e Dz
P incremental eddy current core loss dc Permeabilities:
De
P normal hysteresis core loss µ normal permeability
h
P incremental hysteresis core loss µ absolute permeability
Dh abs
P reactive (quadrature) power µ differential permeability
q d
P residual core loss µ incremental permeability
r D
P winding loss (copper loss) µ effective circuit permeability
w eff
P exciting power
µ intrinsic permeability
z i
P specific exciting power µ incremental intrinsic permeabili
...

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1.1 This test method provides a means for determination of the impedance permeability (μz) of ferromagnetic materials under the condition of sinusoidal current (sinusoidal H) excitation. Test specimens in the form of laminated toroidal cores, tape-wound toroidal cores, and link-type laminated cores having uniform cross sections and closed flux paths (no air gaps) are used. The method is intended as a means for determining the magnetic performance of ferromagnetic strip having a thickness less than or equal to 0.025 in. [0.635 mm].  
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FIG. 1 Basic Circuit Using Permeameter  
Note 1:  
A1—Multirange ammeter (main current)
A2—Multirange ammeter (hysteresis current)
B—Magnetic flux density test position for Switch S3
F—Electronic Fluxmeter
H—Magnetic field strength test position for Switch S3
N1—Magnetizing coil
N2—Magnetic flux sensing (B) coil
N3—Magnetic field strength (H) sensing coil
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3.1 This test method is suitable for specification acceptance, design purposes, service evaluation, regulatory statutes, manufacturing control, and research and development.  
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1.1 These test methods cover four procedures for determination of the permeability [relative permeability]2 of materials having a relative permeability not exceeding 6.0.  
1.2 The test methods covered are as follows:  
1.2.1 Test Method 1—Fluxmetric Method is suitable for materials with relative permeabilities between 1.0 and 4.0. This method permits the user to select the magnetic field strength at which the permeability is to be measured.  
1.2.2 Test Method 2—Permeability of Paramagnetic Materials has been eliminated as an acceptable method of test.  
1.2.3 Test Method 3—Low Mu Permeability Indicator is suitable for measuring the permeability of a material as “less than” or “greater than” that of calibrated standard inserts with relative permeabilities between 1.01 and 6.0, as designated for use in a Low-Mu Permeability Indicator.3 In this method, a small volume of specimen is subjected to a local magnetic field that varies in magnitude and direction, so it is not possible to specify the magnetic field strength at which the measurement is made.  
1.2.4 Test Method 4—Flux Distortion is suitable for materials with relative permeabilities between 1.0 and 2.0. In this method, a small volume of specimen is subjected to a local magnetic field that varies in magnitude and direction, so it is not possible to specify the magnetic field strength at which the measurement is made.4  
1.2.5 Test Method 5—Vibrating Sample Magnetometry is suitable for materials with relative permeabilities between 1.0 and 4.0. This test method permits the user to select the magnetic field strength at which the permeability is to be measured.  
1.3 Materials typically tested by these methods such as austenitic stainless steels may be weakly ferromagnetic. That is, the magnetic permeability is dependent on the magnetic field strength. As a consequence, the results obtained using the different methods may not closely agree with each other. When using Methods 1 and 5, it is imperative to specify the magnetic field strength or range of magnetic field strengths at which the permeabilities have been determined.  
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1.5 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.  
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ASTM A773/A773M-21(Test Method)
Standard Test Method for Direct Current Magnetic Properties of Low Coercivity Magnetic Materials Using Hysteresigraphs

SIGNIFICANCE AND USE
5.1 Hysteresigraphs permit more rapid and efficient collection of data as compared to the point by point ballistic Test Methods A341/A341M and A596/A596M. The high measurement point density offered by computer-automated systems is often required for computer aided design of electrical components such as transformers, motors, and relays.  
5.2 Hysteresigraphs are particularly desirable for testing of semi-hard and hard magnetic materials, where either the entire second quadrant (demagnetization curve) or entire hysteresis loop is of primary concern. Test Method A977/A977M describes the special requirements for accurate measurement of hard magnetic (permanent magnet) materials.  
5.3 Hysteresigraphs are not recommended for measurement of initial permeability, µi, of materials with high magnetic permeability such as nickel-iron, amorphous, and nanocrystalline materials due to errors associated with integrator drift; in these cases, Test Method A596/A596M is a more appropriate method.  
5.4 Provided the test specimen is representative of the bulk sample or lot, this test method is well suited for design, specification acceptance, service evaluation, and research and development.
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1.2 The equipment and procedures described in this test method are most suited for soft and semi-hard materials with intrinsic coercivity less than about 100 Oersteds [8 kA/M]. Materials with higher intrinsic coercivities should be tested according to Test Method A977/A977M.  
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ASTM A596/A596M-21(Test Method)
Standard Test Method for Direct-Current Magnetic Properties of Materials Using the Point by Point (Ballistic) Method and Ring Specimens

SIGNIFICANCE AND USE
3.1 Test methods using suitable ring-type specimens4 are the preferred methods of determining the basic magnetic properties of a material caused by the absence of demagnetizing effects and are well suited for specification acceptance, service evaluation, and research and development.  
3.2 Provided the test specimen is representative of the bulk material as is usually the case for thin strip and wire, this test is also suitable for design purposes.  
3.3 When the test specimen is not necessarily representative of the bulk material such as a ring machined from a large forging or casting, the results of this test method may not be an accurate indicator of the magnetic properties of the bulk material. In such instances, the test results when viewed in context of past performance history will be useful for judging the suitability of the current material for the intended application.
SCOPE
1.1 This test method covers dc testing for the determination of basic magnetic properties of materials in the form of ring, toroidal, link, double-lapped Epstein cores, or other standard shapes which may be cut, stamped, machined, or ground from cast, compacted, sintered, forged, or rolled materials. It includes tests for determination of the normal magnetization curve and hysteresis loop taken under conditions of steep wavefront reversals of the direct-current magnetic field strength.  
1.2 This test method shall be used in conjunction with Practice A34/A34M.  
1.3 This test method is suitable for a testing range from very low magnetic field strength up to 200 or more Oe [15.9 or more kA/m]. The lower limit is determined by integrator sensitivity and the upper limit by heat generation in the magnetizing winding. Special techniques and short duration testing may extend the upper limit of magnetic field strength.  
1.4 Testing under this test method is inherently more accurate than other methods. When specified dimensional or shape requirements are observed, the measurements are a good approximation to absolute properties. Test accuracy available is primarily limited by the accuracy of instrumentation. In most cases, equivalent results may be obtained using Test Method A773/A773M or the test methods of IEC Publication 60404-4.  
1.5 This test method permits a choice of test specimen to permit measurement of properties in any desired direction relative to the direction of crystallographic orientation without interference from external yoke systems.  
1.6 The symbols and abbreviated definitions used in this test method appear in Fig. 1 and Sections 5, 6, 9, and 10. For the official definitions see Terminology A340.  
FIG. 1 Basic Circuit Using Ring-Type Cores  
Note 1:  
A1—Multirange ammeter, main-magnetizing current circuit
A2—Multirange ammeter, hysteresis-current circuit
N1—Magnetizing (primary) winding
N2—Flux-sensing (secondary) winding
F—Electronic integrator
  R1—Main current control rheostat
R2—Hysteresis current control rheostat
S1—Reversing switch
S2—Shunting switch for hysteresis current control rheostat  
1.7 Warning—Mercury has been designated by EPA and many state agencies as a hazardous material that can cause central nervous system, kidney, and liver damage. Mercury, or its vapor, may be hazardous to health and corrosive to materials. Caution should be taken when handling mercury and mercury-containing products. See the applicable product Material Safety Data Sheet (MSDS) for details and EPA’s website (http://www.epa.gov/mercury/faq.htm ) for additional information. Users should be aware that selling mercury or mercury-containing products, or both, in your state may be prohibited by state law.  
1.8 The values stated in either customary (cgs-emu and inch-pound) units or SI units are to be regarded separately as standard. Within this test method, the SI units are shown in brackets except for the sections concerning calculations where there are separate sections fo...

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ASTM
ASTM A34/A34M-06(2021)(Practice)
Standard Practice for Sampling and Procurement Testing of Magnetic Materials

SIGNIFICANCE AND USE
4.1 This practice defines test lots and describes the selection and preparation of test specimens used in the determination of magnetic properties of various materials.  
4.2 A method of calculating the density of iron-base electrical steels is given and a table of assumed densities for magnetic testing of commercial soft magnetic alloys is provided.
SCOPE
1.1 This practice covers sampling procedures and test practices for determination of various magnetic properties of both soft and hard magnetic materials.  
1.2 This practice may be used either in conjunction with, or independent of, the standard test methods and materials specifications under the jurisdiction of ASTM Committee A06. In the former situation, the sampling and testing procedures listed herein shall not supersede those found in the individual test methods and materials specifications. In the latter situation, the sampling and testing procedures listed herein shall strictly apply.  
1.3 The values and equations stated in 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 except for the sections concerning calculations where there are separate sections for the respective unit systems. 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.  
1.4 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.  
1.5 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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