EP0304113A1 - Starting material for permanent magnets - Google Patents

Starting material for permanent magnets Download PDF

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Publication number
EP0304113A1
EP0304113A1 EP88201675A EP88201675A EP0304113A1 EP 0304113 A1 EP0304113 A1 EP 0304113A1 EP 88201675 A EP88201675 A EP 88201675A EP 88201675 A EP88201675 A EP 88201675A EP 0304113 A1 EP0304113 A1 EP 0304113A1
Authority
EP
European Patent Office
Prior art keywords
starting material
permanent magnets
fe14c
hard
temperature
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP88201675A
Other languages
German (de)
French (fr)
Inventor
Dirk Bastiaan De Mooij
Reinoud Van Mens
Kurt Heinz Jürgen Buschow
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Koninklijke Philips NV
Original Assignee
Philips Gloeilampenfabrieken NV
Koninklijke Philips Electronics NV
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Philips Gloeilampenfabrieken NV, Koninklijke Philips Electronics NV filed Critical Philips Gloeilampenfabrieken NV
Publication of EP0304113A1 publication Critical patent/EP0304113A1/en
Withdrawn legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/047Alloys characterised by their composition
    • H01F1/053Alloys characterised by their composition containing rare earth metals
    • H01F1/055Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
    • H01F1/058Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IVa elements, e.g. Gd2Fe14C

Definitions

  • the invention relates to a hard-magnetic material which comprises neodymium and iron.
  • Nd2 Fe14 B having a tetragonal crystal structure. It is known that a substitution of B by C in this compound leads to a greater anisotropy (see, for example, Journal de Physique Colloque C6, supplpir au no. 9, T. 46, September, 1985, pages C6-­305/308: "Magnetic anisotropy of Carbon Doped Nd2Fe14B" by Bolzoni, Leccabue, Pareti and Sanchez). It is stated in this article on page 306 that it was not possible to obtain the tetragonal phase when borium was replaced entirely by carbon.
  • the Curie-temperature is between 500 and 600 K.
  • the hard-magnetic materials according to the invention can be obtained in the conventional manner by fusing starting materials suitable for that purpose succeeded by an annealing treatment in a protective gas or another vacuum. A number of materials which were obtained in this manner are collected in the following table which also states the Curie-temperature and the annealing temperature.
  • the magnetic properties are comparable to those of materials on the basis of Nd2Fe14B or better.
  • the absence of boron is an advantage since now poisonous volatile boron compounds cannot be formed in the preparation.
  • Magnets in the form of shaped bodies can be sintered from the resulting material after pulverisation in the manner conventional with Nd2Fe14B.

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Hard Magnetic Materials (AREA)

Abstract

Hard-magnetic materials having a high crystal anisotropy on a carbide basis of the general formula (RE1-xNdx) Fe₁₄C, wherein
RE is a rare earth metal having an atomic number exceeding 61 and 0.50 ≦ x ≦ 0.80 have a comparatively high Curie-­temperature.

Description

  • The invention relates to a hard-magnetic material which comprises neodymium and iron.
  • A known material of this type is the Nd₂ Fe₁₄ B having a tetragonal crystal structure. It is known that a substitution of B by C in this compound leads to a greater anisotropy (see, for example, Journal de Physique Colloque C6, supplément au no. 9, T. 46, September, 1985, pages C6-­305/308: "Magnetic anisotropy of Carbon Doped Nd₂Fe₁₄B" by Bolzoni, Leccabue, Pareti and Sanchez). It is stated in this article on page 306 that it was not possible to obtain the tetragonal phase when borium was replaced entirely by carbon.
  • It is the object of the invention to provide a hard-­magnetic material having a great crystal anisotropy which comprises only carbon instead of boron and also a comparatively high content of neodymium.
  • It has been found that this object can be achieved by means of a substance of the following composition:
    (RE1-xNdx) Fe₁₄C,
    wherein RE is one or more rare earth metals having an atomic number exceeding 61 (for example Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Lu) and
    0.5 ≦ x ≦ 0.80.
  • It has been found that the magnetic properties decrease substantially if x < 0.5 or if x > 0.8.
  • In all the combinations a carbide having a tetragonal crystal structure is found. The Curie-temperature is between 500 and 600 K. The hard-magnetic materials according to the invention can be obtained in the conventional manner by fusing starting materials suitable for that purpose succeeded by an annealing treatment in a protective gas or another vacuum. A number of materials which were obtained in this manner are collected in the following table which also states the Curie-temperature and the annealing temperature. Table
    Compound Curie-temperature (K) Annealing temperature (°C)
    TbNdFe₁₄C 560 850
    Tb0.5Nd1.5Fe₁₄C 550 800
    Dy0.5Nd1.5Fe₁₄C 545 850
    LuNdFe₁₄C 530 850
  • The magnetic properties are comparable to those of materials on the basis of Nd₂Fe₁₄B or better. The absence of boron is an advantage since now poisonous volatile boron compounds cannot be formed in the preparation.
  • Magnets in the form of shaped bodies can be sintered from the resulting material after pulverisation in the manner conventional with Nd₂Fe₁₄B.

Claims (2)

1. A hard-magnetic material which comprises neodymium and iron, characterized in that the material has the composition (RE1-xNdx) Fe₁₄C, wherein RE is Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm and/or Lu and
0.5 ≦ x ≦ 0.8.
2. A permanent magnet on the basis of a material as claimed in Claim 1.
EP88201675A 1987-08-21 1988-08-03 Starting material for permanent magnets Withdrawn EP0304113A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
NL8701970 1987-08-21
NL8701970 1987-08-21

Publications (1)

Publication Number Publication Date
EP0304113A1 true EP0304113A1 (en) 1989-02-22

Family

ID=19850485

Family Applications (1)

Application Number Title Priority Date Filing Date
EP88201675A Withdrawn EP0304113A1 (en) 1987-08-21 1988-08-03 Starting material for permanent magnets

Country Status (4)

Country Link
EP (1) EP0304113A1 (en)
JP (1) JPS6473051A (en)
KR (1) KR890004353A (en)
CN (1) CN1031443A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109881113B (en) * 2019-02-24 2020-05-19 东阳市宏丰磁业有限公司 Composite permanent magnetic material and preparation method thereof

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
JOURNAL OF APPLIED PHYSICS, Band 61, Nr. 8, 15. April 1987, Seiten 3574-3576, American Institute of Physics, New York, US; N.C. LIU et al.: "High intrinsic coercivities in iron-rare earth-carbon-boron alloys through the carbide or boro-carbide Fe14R2X(X=BxC1-x)" *
MATERIALS LETTERS, Band 4, Nrs. 8,9, August 1986, Seiten 377-380, Elsevier Science Publishers B.V., Amsterdam, NL; N.C. LIU et al.: "High coercivity permanent magnet materials based on iron-rare-earth-carbon alloys" *

Also Published As

Publication number Publication date
JPS6473051A (en) 1989-03-17
KR890004353A (en) 1989-04-21
CN1031443A (en) 1989-03-01

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