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GB/T 3217-2013Permanent magnet (magnetically hard) materials -- Methods of measurement of magnetic properties (English PDF)

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Issued by

General Administration of Quality Supervision, Inspection and Quarantine

Level / Type

National · Recommended

Issue date

July 19, 2013

Implementation date

December 2, 2013

Scope

GB/T 3217-2013 (Permanent magnet (magnetically hard) materials -- Methods of measurement of magnetic properties) is available as an English-translated PDF.

GB/T 3217-2013 — This Standard specifies the methods of measurement of magnetic properties for permanent magnet (magnetically hard) materials.

This Standard applies to the measurement of magnetic properties of Al-Ni-Co permanent magnet, ferrite permanent magnet, Fe-Cr-Co permanent magnet, rare earth permanent magnet and other permanent magnet materials.

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Document preview — GB/T 3217-2013

National Standard of the People's Republic of China

ICS
29.030
Classification
K 14

Issued by: General Administration of Quality Supervision, Inspection and Quarantine

Contents

  • Foreword...3
  • 1 Scope...5
  • 2 Normative references...5
  • 3 Terms and definitions...5
  • 4 Measurement principle...7
  • 5 Magnetizing device...8
  • 6 Test specimen...10
  • 7 Measurement of the magnetic flux density...11
  • 8 Measurement of the magnetic polarization...12
  • 9 Measurement of the magnetic field intensity...14
  • 10 Determination of the demagnetization curve...14
  • 11 Determination of the principal characteristics...16
  • 12 Calibration of the test equipment...16
  • 13 Test report...17

Foreword

This Standard was drafted in accordance with the rules given in GB/T 1.1-2009.

This Standard replaces GB/T 3217-1992, Method of test of the magnetic properties of

permanent magnetic (magnetically hard) materials.

Compared with GB/T 3217-1992, the main changes of this Standard are as follows:

-- Add the content of terms;

-- Restructure according to the international standard;

-- Change the positions of diagrams and figures in accordance with the

international standard;

-- Add measurement principles in accordance with the international standard

(Chapter 4);

-- Delete the content of measuring demagnetization curve and recoil

permeability by impact method;

-- Delete Appendix A and Appendix B of the original standard; adjust Appendix

C of the original standard to Appendix B of this Standard and slightly modify

the content;

-- Add the influence of specimen temperature on measurement results

(Appendix A);

-- Add the corresponding chapter and article numbers of this Standard and IEC

60404-5:1993 Magnetic materials - Part 5: Permanent magnet (magnetically

hard) materials - Methods of measurement of magnetic properties and its 2006

amendment (1) (Appendix C);

-- Add the technical differences and their reasons between this Standard and IEC

60404-5:1993 Magnetic materials - Part 5: Permanent magnet (magnetically

hard) materials - Methods of measurement of magnetic properties and its 2006

amendment (1) (Appendix D).

This Standard modifies and adopts IEC 60404-5:1993 Magnetic materials - Part 5:

Permanent magnet (magnetically hard) materials - Methods of measurement of

magnetic properties and its 2006 amendment (1) by the redrafting method.

This Standard is partially restructured compared to IEC 60404-5:1993 and its 2006

amendment (1). Appendix C lists the comparison of chapter and clause numbers

between this Standard and IEC 60404-5:1993 and its 2006 amendment (1).

Permanent magnet (magnetically hard) materials - Methods

of measurement of magnetic properties

1 Scope

This Standard specifies the methods of measurement of magnetic properties for

permanent magnet (magnetically hard) materials.

This Standard applies to the measurement of magnetic properties of Al-Ni-Co

permanent magnet, ferrite permanent magnet, Fe-Cr-Co permanent magnet, rare earth

permanent magnet and other permanent magnet materials.

2 Normative references

The following referenced documents are indispensable for the application of this

document. For dated references, only the edition cited applies. For undated references,

the latest edition of the referenced document (including any amendments) applies.

GB/T 2900.4-2008, Electrotechnical terminology - Special alloys for electrical

equipment

GB/T 2900.60-2002, Electrotechnical terminology - Electromagnetism [eqv IEC

60050(121):1998]

GB/T 9637-2001, Electrotechnical terminology - Magnetic materials and

components [eqv IEC 60050(221):1990]

GB/T 24270-2009, Method of measurement of temperature coefficient of

magnetic properties of permanent magnetic materials

IEC60050(151), International electrotechnical vocabulary - Part 151: Electrical

and magnetic devices

3 Terms and definitions

For the purposes of this document, the terms and definitions given in GB/T 2900.4-

2008, GB/T 2900.60-2002, GB/T 9637-2001 and IEC 60050(151) as well as those given

below apply.

3.1

demagnetization curve

10.3.6 The J search coil can also be replaced by the B search coil and the B(H) curve

can be drawn according to the above method. However, the air gap between the

specimen and the B search coil must be small enough to reduce the measurement error.

11 Determination of the principal characteristics

11.1 Magnetic remanence, Br

After drawing the demagnetization curve, take the magnetic flux density value at the

intersection of the demagnetization curve and the B axis (see Figure 1).

11.2 Maximum BH product, (BH)max

The maximum BH product, (BH)max, is determined by the maximum value of the

corresponding product of B and H on the demagnetization curve, or by the method of

tangency of the demagnetization curve and the isomagnetic energy curve (see Figure

2).

11.3 Coercivity, HcB and intrinsic coercivity, HcJ

The magnetic field intensity value at the intersection of the B (H) demagnetization

curve and the B=0 straight line is HcB, and the magnetic field intensity value at the

intersection of the J (H) demagnetization curve and the J=0 straight line is HcJ (see

Figure 1).

11.4 Determination of the recoil line and the recoil permeability, µrec

Take a certain point A (Hrec, Brec), as required, on the demagnetization curve as the base

point of the recoil line (see Figure 1). When the measurement of the demagnetization

curve reaches point A (Hrec, Brec), change the direction of the magnetization field so that

the change amount is deltaH (reaching point C) and then return to point A (Hrec, Brec), to

obtain the recoil line. The recoil permeability µrec is obtained from the average slope of

the recoil line (see Figure 1).

Generally, µrec is not a constant along the demagnetization curve, so the corresponding

Hrec, Brec and deltaH values shall be indicated.

12 Calibration of the test equipment

12.1 The test equipment shall be calibrated regularly. The magnetic field detector, J

search coil, integrator, etc. used in the test equipment shall be sent to the metrology

department for calibration regularly.

12.2 To ensure the accuracy and consistency of the measurement of magnetic

parameters of permanent magnetic materials, use standard specimens verified by the

national metrology department to compare the measurement results of various magnetic

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This preview omits tables, figures, formulas and parts of the technical clauses. The complete document — 17 pages — is available in the English PDF.

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