[0001] The invention relates to a boron-free hard magnetic material on the basis of neodymium,
iron and carbon, which comprises a hard magnetic tetragonal phase. The invention also
relates to a method of manufacturing such a material.
[0002] A known material of this type comprises Nd₂Fe₁₄B having a tetragonal crystal structure
as a hard magnetic phase. It is known that in this compound a partial substitution
of boron by carbon leads to an increased magnetic anisotropy (see, for example, Journal
de Physique Colloque C6, supplément au no. 9, T. 46, Sept. 1985, page C6-305/308:
" Magnetic Anisotropy of Carbon Doped Nd₂Fe₁₄B" by Bolzoni, Leccabue, Pareti and Sanchez).
In this article it is stated on page 306 that when boron is completely replaced by
carbon it is impossible to obtain a tetragonal phase which is required to obtain the
desired hard magnetic properties.
[0003] It is an object of the invention to provide a hard magnetic material having a high
crystal anisotropy, which comprises iron, neodymium and only carbon instead of boron.
[0004] It was found that this object can be achieved by a material having the following
overall composition, 11.2 to 15.2 at.% of Nd, 74.8 to 84.8 at.% of Fe and 4 to 10
at.% of C, a finely crystalline tetragonal phase having a grain size of 0.2 µm or
smaller and having the Nd₂Fe₁₄C structure being present in the material. This composition
range comprises material compositions having coercive forces µ
oH
c of 0.6 T or larger. It should be noted that materials having the highest coercive
force are obtained if the composition of the materials is selected as follows: Nd:
12 - 15 at.%, Fe: 75 - 84 at.% and C: 4.8 - 10 at.%. The magnetic properties of the
material improve, however, if the composition of the material is selected as follows,
Nd: 12.0 - 14.2 at.%, Fe: 76.6 - 83.2 at.% and C: 4.8 - 9.2 at.%, the Curie temperature
of these materials being in general 260°C or higher. However, sometimes the material
also contains a second soft magnetic phase. Substantially single-phase materials in
general have the following composition, Nd: 12 - 14 at.%, Fe: 78 - 81 at.% and C:
6 - 8 at.%. The compositions of the materials of the present invention possess the
known property of the Nd₂Fe₁₄B material that substitution of part of the iron by cobalt
increases the Curie temperature.
[0005] Finely crystalline is to be understood to mean herein that at least 90% of the crystallites
in the hard magnetic phase have a dimension of 0.2 µm or smaller. The hard magnetic
material according to the invention can be obtained by melting together the starting
elements, followed by melt spinning on a chill surface, for example the surface of
a rapidly rotating copper disc, which moves rapidly relative to the orifice.
[0006] A method of manufacturing a hard magnetic material in the form of a ribbon is known
from European Patent Application EP-A 108 474. In the known method, the moving chill
surface is formed by the circumferential surface of a disc of a material having a
high thermal conductivity such as copper coated with chromium.
[0007] This European Patent Application does not give any indication that the method can
also be used for the manufacture of boron-free finely crystalline hard magnetic materials
on the basis of neodymium and iron, provided that the method is suitably adapted.
For it has been found in the investigation leading to the invention that on rapidly
cooling carbon-containing, boron-free neodymium-iron alloys
no phase having the desired tetragonal crystal structure is formed. A suffiently rapid
cooling for the desired effect is obtained if, by a suitable choice of the spraying
pressure, the slot dimensions, the disc slot spacing and the speed of the disc, the
spraying process can be carried out such that ribbons or flakes having a thickness
of 30 µm or smaller are obtained. The ribbons or flakes formed comprise a microcrystalline
phase having a structure which resembles that of Nd₂Fe₁₇; the material is
not hard magnetic. It must be assumed that part of the carbon present is dissolved in
this phase. In this respect, the material according to the invention clearly differs
from boron-containing materials. Boron is substantially insoluble at the temperatures
used in the Nd₂Fe₁₇ phase.
[0008] According to another aspect of the invention, the desired hard magnetic properties
can be obtained if immediately after melt spinning the material is subjected to a
recrystallizing annealing treatment of short duration at a relatively low temperature.
[0009] Surprisingly, it has been found that in this annealing treatment a microcrystalline
phase having a tetragonal structure and substantially the composition Nd₂Fe₁₄C is
formed in the material, in which phase some extra carbon may possibly still be dissolved.
[0010] The annealing treatment is carried out at a temperature between 675 and 750°C, preferably
at a temperature between 685°C and 730°C. On heating to a temperature of 720°C the
desired finely crystalline tetragonal phase Nd₂Fe₁₄C is formed within a minute after
attaining the said temperature. The annealing duration necessary for the crystallization
can be established readily in an experimental way at any annealing temperature in
the indicated temperature range. A suitable annealing treatment consists in that the
material is maintained in a furnace for 1 to 5 minutes, the furnace being at a temperature
of 720°C. In practice, a dwell time of 2 to 3 minutes was found to be suitable. The
material thus obtained has suitable permanent magnetic properties. A saturation magnetization
µ
oM
sat of > 1.2 T, a remanence µ
oM
r of > 0.50 T and a coercive force µ
oH
c of > 1.0 T were measured. The particular thing about the new magnetic material is
that also after annealing for 6 days at 680°C it still has a relatively high coercive
force of µ
oH
c = 0.75 T. In the material according to the invention a marked grain growth occurs
when it is heated for a long time (360 hours) at 800°C, the grains being formed having
a dimension between 0.2 and 0.6 µm. In this process the coercive force decreases to
0.2 T. A further increase of the dimensions of the grains was observed when they were
heated at 850°C and 900°C for 15 days. Then, the most important phase is still the
Nd₂Fe₁₄C phase.
[0011] During the investigation leading to the invention, it was established that when material
compositions containing less than 11.2 at.% of neodymium are subjected to the annealing
treatment at 720°C a phase of more than 10% is formed having the α-Fe structure, in
which some carbon may possibly be dissolved; in which case roentgenographically no
traces of neodymium can be found. If the material contains more than 15.2 at.% of
neodymium, the tetragonal Nd₂Fe₁₄C phase is not formed or only to a small extent,
and the material is predominantly in a Nd₂Fe₁₇ phase having a rhombohedral structure,
in which the carbon is dissolved. Of course, also other techniques of rapidly cooling
a molten alloy can be used, which have the same result.
[0012] For the manufacture of magnets, the material in the form of flakes is compressed
in a hot condition, for example at 650°C, if necessary, after it has been powdered
or ground. The material in the form of flakes may alternatively be bound with a synthetic
resin, if necessary after it has been powdered or ground, and formed into a magnet.
[0013] An advantage of the new magnetic material is that during its manufacture it cannot
form toxic boron-containing compounds when it contacts water and/or hydrogen.
Exemplary embodiment 1:
[0014] 20 grams of an alloy having the following composition, neodymium 13.5 at.%, iron
79.6 at.% and carbon 6.9 at.% were melted by heating to a temperature of 1300°C. The
liquid alloy was sprayed onto a copper disc through an aperture of 0.4 x 10 mms. The
distance between the orifice and the disc was 0.2 mm, the spraying pressure was 2.10⁴
Pa and the disc had a speed of 28 m/s relative to the orifice. The flowing rate was
5 cm³/s, and spraying was carried out in an argon atmosphere. In this way, ribbons
having a width of approximately 10 mm, an average length of 10 mm and a thickness
of 20 µm were obtained. Subsequently, the flakes obtained were introduced into a furnace
which was heated to a temperature of 720°C, and they were maintained therein for 3
minutes. The material thus obtained had, predominantly, a finely crystalline tetragonal
structure (Nd₂Fe₁₄C). Crystallite dimension (more than 90%): 0.2 µm.
The following magnetic properties were measured: |
Coercive force µoHc) |
: |
1.02 T |
Saturation magnetization µoMsat) |
: |
1.34 T |
Remanence µoMr |
: |
0.72 T |
Curie temperature |
: |
269°C |
Exemplary embodiment 2:
[0015] The material compositions listed in the Table below were treated in a completely
analogous manner. The Table below lists the properties measured on the crystallized
material:
Material composition |
Coercive force |
Magnetization |
Remanence |
|
µoHc in T |
µoMsat in T |
µoMr in T |
Nd13.3Fe80.9C5.8 |
0.65 |
1.31 |
0.55 |
Nd13.5Fe77.7C8.8 |
0.60 |
1.33 |
0.64 |
Nd14.8Fe76.4C8.8 |
1.16 |
1.32 |
0.70 |
1. A boron-free hard magnetic material on the basis of neodymium, iron and carbon,
which comprises a hard magnetic, tetragonal phase, characterized in that the material
has the following overall composition, neodymium 11.2 - 15.2 at.%, iron 74.8 - 84.8
at.% and carbon 4 - 10 at.%, and that a finely crystalline tetragonal phase having
a grain size of 0.2 µm or smaller and having the Nd₂Fe₁₄C structure is present in
the material.
2. A boron-free hard magnetic material as claimed in Claim 1, characterized in that
the material has the following overall composition neodymium 12 - 15 at.%, iron 75
- 84 at.% and carbon 4.8 - 10 at.%.
3. A boron-free hard magnetic material as claimed in Claim 2, characterized in that
the material has the following overall composition, neodymium 12.0 - 14.2 at.%, iron
76.6 - 83.2 at.% and carbon 4.8 - 9.2 at.%.
4. A boron-free hard magnetic material as claimed in Claim 3, characterized in that
the material has the following overall composition, neodymium 12 - 14 at.%, iron 78
- 81 at.% and carbon 6 - 8 at.%.
5. A boron-free hard magnetic material as claimed in Claim 4, characterized in that
the material has the following overall composition, neodymium 13.5 at.%, iron 79.6
at.% and carbon 6.9 at.%.
6. A boron-free hardmagnetic material as claimed in any one of the preceding Claims,
characterized in that in the overall composition part of the iron is substituted by
cobalt in an amount sufficient to increase the Curie termperature.
7. A method of manufacturing a hard magnetic material on the basis of neodymium, iron
and carbon by spraying a molten alloy onto a rapidly moving chill surface and further
processing of the ribbons or flakes thus obtained, characterized in that the method
comprising the following steps,
ribbons or flakes having a thickness of 30 µm or less are manufactured from an alloy
having the following overall composition, neodymium 11.2 - 15.2 at.%, iron 74.8 -
84.8 at.% and carbon 4 - 10 at.%, the material obtained being annealed at a temperature
between 675 and 750°C.
8. A method as claimed in Claim 7, characterized in that the material is annealed
at 685 - 730°C.
9. A method as claimed in Claim 8, characterized in that the material is annealed
at 720°C.
10. A method as claimed in Claim 7, characterized in that an alloy having the following
overall composition is used, neodymium 12 - 15.2 at.%, iron 76.6 - 83.2 at.% and carbon
4.8 - 9.2 at.%.
11. A method as claimed in Claim 7, characterized in that an alloy having the following
overall composition is used, neodymium 12.0 -14.2 at.%, iron 76.6 - 83.2 at.% and
carbon 4.8 - 9.2 at.%.
12. A method as claimed in Claim 11, characterized in that an alloy having the following
overall composition is used, neodymium 12 - 14 at.%, iron 78 - 81 at.% and carbon
6 - 8 at.%.
13. A method as claimed in Claim 12, characterized in that an alloy having the following
overall composition is used, neodymium 13.5 at.%, iron 79.6 at.% and carbon 6.9 at.%.
14. A magnet of a material having the composition as claimed in Claims 1 - 6.
15. A magnet of a material obtained by using a material manufactured as claimed in
Claims 7 - 13.