(19) |
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EP 0 304 113 A1 |
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EUROPEAN PATENT APPLICATION |
(43) |
Date of publication: |
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22.02.1989 Bulletin 1989/08 |
(22) |
Date of filing: 03.08.1988 |
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(51) |
International Patent Classification (IPC)4: H01F 1/04 |
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Designated Contracting States: |
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AT CH DE FR GB IT LI NL SE |
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Priority: |
21.08.1987 NL 8701970
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Applicant: Philips Electronics N.V. |
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5621 BA Eindhoven (NL) |
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Inventors: |
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- De Mooij, Dirk Bastiaan
NL-5656 AA Eindhoven (NL)
- Van Mens, Reinoud
NL-5656 AA Eindhoven (NL)
- Buschow, Kurt Heinz Jürgen
NL-5656 AA Eindhoven (NL)
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Representative: Pennings, Johannes et al |
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INTERNATIONAAL OCTROOIBUREAU B.V.,
Prof. Holstlaan 6 5656 AA Eindhoven 5656 AA Eindhoven (NL) |
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(54) |
Starting material for permanent magnets |
(57) Hard-magnetic materials having a high crystal anisotropy on a carbide basis of the
general formula (RE
1-xNd
x) 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.
[0001] The invention relates to a hard-magnetic material which comprises neodymium and iron.
[0002] 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.
[0003] 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.
[0004] It has been found that this object can be achieved by means of a substance of the
following composition:
(RE
1-xNd
x) 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.
[0005] It has been found that the magnetic properties decrease substantially if x < 0.5
or if x > 0.8.
[0006] 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 |
[0007] 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.
[0008] Magnets in the form of shaped bodies can be sintered from the resulting material
after pulverisation in the manner conventional with Nd₂Fe₁₄B.
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.