TECHNICAL FIELD
[0001] The present invention relates to a method for producing a sintered rare-earth magnet,
such as a sintered Nd-Fe-B magnet or sintered Sm-Co magnet.
BACKGROUND ART
[0002] Sintered rare-earth magnets are commonly used as permanent magnets capable of creating
strong magnetic fields. In particular, sintered Nd-Fe-B magnets are commonly used
in motors for hybrid cars or electric vehicles, compact motors for hard-disk drives,
large-sized industrial motors, power generators and other applications.
[0003] In such motors or generators, a sintered rare-earth magnet is used as the rotor and
an electromagnet as the stator. The electromagnet is operated to create a rotating
magnetic field for revolving the rotor. In this process, an eddy current is generated
in the sintered rare-earth magnet, causing a loss of energy or overheating of the
motor. A technique for solving this problem is disclosed in Patent Document 1, in
which a plurality of slits are formed on the surface of the sintered rare-earth magnet
to prevent the generation of eddy currents.
[0004] In the case of producing a sintered Nd-Fe-B magnet (neodymium magnet), an alloy powder
having a portion of Nd replaced by Dy and/or Tb is used to increase the coercive force
of the magnet. However, since Dy and Tb are both expensive and rare elements, this
technique increases the production cost and negatively affects the stable supply of
the magnet. Another drawback of this technique is the decrease in the maximum energy
product. A conventional technique for solving these problems is the grain boundary
diffusion, which includes applying Dy and/or Tb to the surface of a sintered compact
of Nd-Fe-B alloy containing neither Dy nor Tb and heating it to a temperature within
a range from 700 to 1000 degrees Celsius, whereby Dy and/or Tb is transferred through
the boundaries of alloy particles into deeper regions of the sintered compact to create
a product containing Dy and/or Tb only in the vicinity of the surfaces of the alloy
particles. This technique has the effect of achieving a high coercive force while
preventing a significant decrease in the maximum energy product as well as decreasing
the usage of Dy and Tb. Patent Document 2 discloses the technique of efficiently injecting
Dy and/or Tb into the vicinity of the surfaces of alloy particles by forming slits
on the surface of the sintered compact of an Nd-Fe-B alloy and diffusing Dy and/or
Tb from those slits into the grain boundaries.
BACKGROUND ART DOCUMENT
PATENT DOCUMENT
DISCLOSURE OF THE INVENTION
PROBLEM TO BE SOLVED BY THE INVENTION
[0006] In any of the methods described in Patent Documents 1 and 2, the slits are formed
by a machining process using a cutter, wire saw or similar tool. The use of a machining
process inevitably increases the production cost since it requires a considerable
amount of labor and time, with heavy consumption of the tool. Furthermore, the slits
created by such a machining process cannot be very thin and hence considerably lower
the ratio of the actual volume of the magnet (i.e. the volume of the sintered portion)
to its outside volume. As a result, the performance of the product as the magnet substantially
deteriorates.
[0007] In the case where the slits are formed on a compressed compact by machining before
sintering, there will be another problem that the alloy powder remaining in the slits
cannot be easily removed. If a compact with an alloy powder remaining in the slits
is heated for sintering, the alloy powder will partially clog the slits, compromising
the effect of preventing the generation of eddy currents. Furthermore, Dy and/or Tb
is prevented from sufficiently reaching deep regions in the grain boundary diffusion
process.
Subjecting a compressed compact to machine work may also cause the additional problems
of chipping or cracking.
[0008] Thus, the problem to be solved by the present invention is to provide an easy and
inexpensive method for producing a sintered rare-earth magnet having cavities (e.g.
slits or holes) for making the magnet less likely to be influenced from eddy currents
and/or for performing the grain boundary diffusion process.
MEANS FOR SOLVING THE PROBLEMS
[0009] A method for producing a sintered rare-earth magnet according to the present invention
aimed at solving the aforementioned problem is characterized in that a sintered rare-earth
magnet having a cavity is produced by performing the following successive processes:
- a) a filling process for filling a powder of rare-earth magnet alloy into a powder-filling
container together with a cavity-forming member;
- b) an aligning process for aligning the rare-earth magnet alloy powder in a magnetic
field; and
- c) a sintering process for sintering the rare-earth magnet alloy powder by heating
the rare-earth magnet alloy powder in a state of being held in the powder-filling
container, wherein
- d) the cavity-forming member is removed after the aligning process is completed and
before the rare-earth magnet alloy powder begins to be sintered.
[0010] According to the present invention, a sintered rare-earth magnet having a cavity
can be easily produced by a simple method including filling a powder of rare-earth
magnet alloy into the powder-filling container together with a cavity-forming member
and then removing the cavity-forming member before the rare-earth magnet alloy begins
to be sintered. Thus, in the present invention, no machining is necessary to create
the cavity and a sintered rare-earth magnet having a cavity can be produced at a low
cost.
[0011] In most of the conventional methods for producing sintered rare-earth magnets, the
compression-molding and aligning of a rare-earth magnet alloy powder is achieved by
filling the powder into a container and applying a magnetic field to the powder while
compressing it. By contrast, the inventor of the present patent application discovered
the fact that a sintered rare-earth magnet could be created by filling a rare-earth
magnet alloy powder into a powder-filling container, aligning the rare-earth magnet
alloy powder without compression-molding this powder, and heating the powder in a
state of being held in the powder-filling container. (This technique is called a press-less
method. Refer to
JP-A 2006-019521.) In the present invention, since the press-less method is used, the cavity-forming
member undergoes no pressure even if this member is put in the powder-filling container
together with the rare-earth magnet alloy powder.
[0012] As a result of the aligning process in the magnetic field, the particles of the rare-earth
magnet alloy powder held in the powder-filling container magnetically attract each
other. In the present invention, since the cavity-forming member is removed after
the aligning process, the cavity will not be destroyed when the cavity-forming member
is removed.
[0013] When the rare-earth magnet alloy powder is heated to higher temperatures in the sintering
process, the powder begins to be sintered when its temperature exceeds a specific
level (e.g. approximately 600 degrees Celsius for a sintered Nd-Fe-B magnet), after
which the sintered compact shrinks as the sintering process continues. To avoid impeding
this shrinkage, the cavity-forming member used in the present invention is removed
before the rare-earth magnet alloy powder begins to be sintered.
[0014] The removal of the cavity-forming member may be performed before the sintering process
is initiated. This is desirable in that it eliminates the necessity of considering
the heat resistance of the cavity-forming member or the reactivity between the cavity-forming
member and the rare-earth magnet alloy powder.
[0015] It is possible to use a cavity-forming member that liquefies or vaporizes at a temperature
lower than the temperature at which the sintering begins. In this case, the cavity-forming
member will be removed after the temperature begins to increase for the sintering
and before the sintering actually begins.
[0016] If the aforementioned rare-earth magnet alloy is an alloy of a sintered Nd-Fe-B magnet,
Dy and/or Tb can be diffused into the sintered compact by injecting a substance containing
Dy and/or Tb into the cavity of the sintered compact obtained by the sintering process.
[0017] If slits for preventing the influence of eddy currents need to be formed on the sintered
rare-earth magnet, a plate-shaped member can be used as the cavity-forming member.
If the grain boundary diffusion is of primary importance, a rod-shaped member may
be used. In the latter case, a large number of rod-shaped cavity-forming members may
be arranged in the form of a matrix, whereby Dy and/or Tb can be uniformly diffused
from a large number of holes. The cross-sectional shape of the rod-shaped cavity-forming
member is not specifically limited; for example, it may be circular, quadrilateral
or hexagonal.
[0018] If a plate-shaped or rod-shaped cavity-forming member is used as the cavity-forming
member, it is preferable to align the rare-earth magnet alloy powder in a magnetic
field parallel to the cavity-forming member in the aligning process. The particles
of the rare-earth magnet alloy powder forms a chain-like structure extending in the
direction parallel to the cavity-forming member. Therefore, even if the cavity-forming
member is removed in this state, the chain-like structure will not be broken off and
the cavity will remain undestroyed.
[0019] To assuredly prevent the destruction of the cavity, the rare-earth magnet alloy powder
may be mixed with a binder when it is filled into the powder-filling container. Examples
of the binder include methyl cellulose, polyacrylamide, polyvinyl alcohol, paraffin
wax, polyethylene glycol, polyvinyl pyrrolidone, hydroxypropyl cellulose, hydroxypropyl
methylcellulose, ethyl cellulose, acetyl cellulose, nitrocellulose, and polyvinyl
acetate resin. (Refer to
JP-A 10-270278.)
[0020] When the rare-earth magnet alloy powder is filled into the powder-filling container
together with the cavity-forming member, it is possible to simultaneously put both
the powder of rare-earth magnet alloy and the cavity-forming member into the powder-filling
container or to separately and sequentially fill them into the container.
[0021] The cavity formed in the sintered compact by the production method according to the
present invention is mechanically weak and rather fragile if left in its original
state. Furthermore, the cavity may retain moisture and cause corrosion or mechanical
destruction of the product. To avoid these problems, an embedding member, such as
epoxy resin, may be filled into the cavity to increase its mechanical strength and
prevent the retention of moisture. The process of filling the embedding member is
performed after the removal of the cavity-forming member. If the embedding member
is an epoxy resin or similar material whose heat-resistant temperature is lower than
the sintering temperature of the rare-earth magnet, the filling process is performed
after the sintering process. If the diffusion process is additionally performed, the
filling process is performed after the diffusion process. The embedding member should
desirably be made of an insulating material to prevent the influence of eddy currents.
EFFECT OF THE INVENTION
[0022] With the present invention, a cavity can be formed by a simple method including filling
a powder of rare-earth magnet alloy into a powder-filling container together with
a cavity-forming member, aligning the powder in a magnetic field, and removing the
cavity-forming member. By this method, a sintered rear-earth magnet having a cavity
can be easily produced at a low cost since no machining is required.
BRIEF DESCRIPTION OF THE DRAWINGS
[0023]
Fig. 1 shows vertical-sectional views of the first embodiment of the mold, a lid for
this mold, and a cavity-forming member used in a method for producing a sintered rare-earth
magnet according to the present invention, as well as a top view of the aforementioned
lid.
Fig. 2 is a schematic diagram showing the first embodiment of the method for producing
a sintered rare-earth magnet according to the present invention.
Fig. 3 shows vertical-sectional views of the second embodiment of the mold, a lid
for this mold, and a cavity-forming member used in a method for producing a sintered
rare-earth magnet according to the present invention, as well as a bottom view of
the aforementioned mold.
Fig. 4 is a schematic diagram showing the second embodiment of the method for producing
a sintered rare-earth magnet according to the present invention.
Fig. 5 shows vertical-sectional views of another example of the mold and a lid for
this mold in the present invention.
Fig. 6 is a perspective view showing one embodiment of the rod-shaped cavity-forming
member.
Fig. 7 is a schematic diagram showing one embodiment of the grain boundary diffusion
process in the present invention.
Fig. 8 is a schematic diagram showing one embodiment of the process for filling an
embedding member into the cavities.
Fig. 9 is a perspective view of a sintered rare-earth magnet created by the method
according to Embodiment 1.
Fig. 10 shows vertical-sectional views of the mold, a lid for this mold, and a cavity-forming
member used in Example 3-1, as well as a top view of the aforementioned lid.
Fig. 11 shows vertical-sectional views of the mold, a lid for this mold, and a cavity-forming
member used in Example 3-2, as well as a top view of the aforementioned lid.
BEST MODES FOR CARRYING OUT THE INVENTION
[0024] Embodiments of the method for producing a sintered rare-earth magnet according to
the present invention are hereinafter described by means of Figs. 1-11.
Figs. 1 and 2 show the first embodiment of the present invention. The method according
to the first embodiment uses a mold (powder-filling container) 10 and a cavity-forming
member 14 shown in Fig. 1. The mold 10, which is designed for creating a plate-shaped
magnet, has a rectangular-parallelepiped receiving section 11, into which a powder
of rare-earth magnet alloy is to be filled. This receiving section 11 has an opening
on its upper side, thus allowing the filling of the rare-earth magnet alloy powder
and removal of a sintered rare-earth magnet after the sintering process. A lid 13
for closing this opening is attached thereto. Examples of the materials available
for the mold 10 and the lid 13 include magnetic stainless steel, non-magnetic stainless
steel, and some types of carbon that are heat-resistant to temperatures equal to or
higher than the sintering temperature used for creating the sintered rare-earth magnet.
The lid 13 has two insertion openings 131 extending parallel to each other in the
longitudinal direction of the rectangular-parallelepiped receiving section 11. Each
insertion opening 131 allows the insertion of a plate-shaped cavity-forming member
14, which is slightly smaller than the insertion opening 131 in both width and length.
Examples of the materials available for the cavity-forming member 14 include various
kinds of metal, carbon and plastic (which do not need to be heat-resistant in the
present embodiment). There are two cavity-forming members 14 standing on a plate-shaped
attachment base 15, with the same interval as the two insertion openings 131.
[0025] The method for producing a sintered rare-earth magnet according to the present embodiment
is hereinafter described by means of Fig. 2. Initially, a rare-earth magnet alloy
powder 19 is filled in the receiving section 11 (Fig. 2(a)). In this step, the rare-earth
magnet alloy powder 19 in a pure form may be used, or a binder may be mixed with the
rare-earth magnet alloy powder 19. The filling density should preferably be within
a range from 40 to 50 % of the true density of the rare-earth magnet alloy powder.
Next, the lid 13 is attached to the mold 10, and the cavity-forming members 14 are
inserted through the insertion openings 131 into the rare-earth magnet alloy powder
19 held in the receiving section 11 (Fig. 2(b)). Subsequently, the mold 10 is set
into a magnetic-field generation coil 17, and a pulsed magnetic field parallel to
the cavity-forming members 14 (and perpendicular to the lid 13) is applied to align
the rare-earth magnet alloy powder 19 (Fig. 2(c)). The strength of this magnetic field
should be within a range from 3 to 10 T, and more preferably from 4 to 8 T. While
the magnetic field is applied, the lid 13 should be securely pressed onto the mold
10 to prevent the rare-earth magnet alloy powder 19 from escaping. After the aligning
process in the magnetic field, the cavity-forming members 14 are pulled out from the
rare-earth magnet alloy powder 19 and the insertion openings 131 (Fig. 2(d)). Thus,
slit-shaped cavities 18 are formed in the compact of the rare-earth magnet alloy powder
19. As a result of the aligning process in the magnetic field, the fine particles
of the powder magnetically attract each other and hence will barely fall into the
cavities 18. Subsequently, the rare-earth magnet alloy powder 19 in a state of being
held in the receiving section 11 is heated (Fig. 2(e)). Thus, a sintered rare-earth
magnet having slit-shaped cavities is obtained. During the sintering process, water
and other substances that are inevitably present in the rare-earth magnet alloy powder
19 vaporize, and the generated gas is discharged through the insertion openings 131
to the outside of the mold.
[0026] By this method, the slits can be created at a much lower cost than in the case of
performing machine work using a wire saw or similar tool after the sintering process.
Furthermore, a narrow slit that cannot be created by machining can be created. The
obtained slits are completely free from any unwanted matter (e.g. residual powder
inside the slits) which lowers the functionalities of the slits. Thus, a high-quality
slit can be obtained.
[0027] Figs. 3 and 4 show the second embodiment of the present invention. The method according
to the second embodiment uses a mold 20 shown in Fig. 3 and a cavity-forming member
24 shown in Fig. 4. Similar to the mold 10 used in the first embodiment, the mold
20 has a receiving section 21 to which a lid 23 can be attached. A difference from
the first example exists in that two insertion openings 221 are formed in the bottom
of the mold 20. No insertion opening is formed in the lid 23. Similar to the first
embodiment, the cavity-forming members 24 fixed to a cavity-forming member attachment
base 25 can be inserted into the insertion openings 221.
[0028] The method for producing a sintered rare-earth magnet according to the second embodiment
is hereinafter described by means of Fig. 4. Initially, the cavity-forming members
24 are inserted into the insertion openings 221 of the mold 20 (Fig. 4(a)). Next,
a rare-earth magnet alloy powder 29 is filled in the receiving section 21, and the
lid 23 is attached (Fig. 4(b)). Thus, the insertion of the cavity-forming member and
the filling of the rare-earth magnet alloy powder are performed in reverse order as
compared to the first embodiment. Next, the mold 20 is set into a magnetic-field generation
coil 27, and a pulsed magnetic field parallel to the cavity-forming members 24 (and
perpendicular to the lid 23) is applied to align the rare-earth magnet alloy powder
29 (Fig. 4(c)). Subsequently, the cavity-forming members 24 are pulled out from the
rare-earth magnet alloy powder 29 and the insertion openings 221 to form cavities
28 (Fig. 4(d)), and the rare-earth magnet alloy powder 29 in a state of being held
in the receiving section 21 is sintered by heat (Fig. 4(e)).
[0029] Fig. 5 shows another example of the mold. Unlike the mold 10 shown in Fig. 1 in which
the cavity-forming members 14 are fixed to the cavity-forming member attachment base
15 prepared separately from the lid 13, the cavity-forming members 14A in the present
example are directly fixed to the lid 13A (Fig. 5(a)). If this lid 13A is used, the
lid 13A is detached from the mold after the aligning process in order to remove the
cavity-forming members 14.
[0030] The previous descriptions pertained to the cases where the cavity-forming members
are removed after the aligning process. On the other hand, if the cavity-forming members
are made of a material that liquefies or vaporizes at a temperature lower than the
sintering temperature of the rare-earth magnet alloy powder, it is possible to remove
the cavity-forming members, without pulling them out, by heating them together with
the mold and rare-earth magnet alloy powder. In this case, the cavity-forming members
may be attached to the inside of the receiving section. Specific examples of the materials
available for such a cavity-forming member include polyvinyl alcohol or other plastic
materials that easily vaporize. Fig. 5(b) shows one example in which cavity-forming
members 14B stand at the bottom 12 of the receiving section 11.
[0031] The following description explains how to determine an appropriate thickness and
interval of the cavity-forming members as well as an appropriate depth by which these
members should be inserted into the rare-earth magnet alloy powder (which is hereinafter
called the "insertion depth").
Initially, an appropriate width, insertion depth, number and interval of the cavity-forming
members will be explained for the case where the primary purpose of the cavities is
to prevent eddy current during the usage of the sintered rare-earth magnet. In this
case, the intended objective, i.e. the prevention of the eddy currents, can be achieved
even if the slit is too narrow. Therefore, in order to improve the inherent performance
of the magnet, the slits formed in the sintered compact should be as narrow as possible.
This means that the cavity-forming members should be as thin as possible. For example,
in the case of using a member similar to a razor blade, which is a typical example
of the thin plate-shaped member, the lower limit of the thickness of the cavity-forming
member is approximately 0.05 mm. In this case, with the sintering shrinkage taken
into account, the width of the slit to be eventually formed in the sintered compact
will be approximately 0.04 mm. With respect to the insertion depth, it is preferable
to increase this depth to improve the effect of reducing the eddy currents. However,
to ensure an adequate mechanical strength of the sintered compact, the depth should
be smaller than the magnet's thickness in the direction of the insertion depth by
1 mm or more, and more preferably 2 mm or more.
If the cavity-forming member is excessively thick, the volume ratio of the magnet
(i.e. the ratio of the volume where the magnet actually exists to the outside volume
of the sintered magnet) will be too low and the magnetic properties of the product
will deteriorate. Accordingly, the thickness of the cavity-forming member should be
appropriately determined so that the volume ratio will be equal to or higher than
90 %.
With respect to the interval of the slits, or the interval of the cavity-forming members,
it is preferable to reduce this interval since the loss of energy due to the eddy
currents generated in the magnet is proportional to the second power of the magnet
size. However, increasing the number of slits reduces the volume ratio of the magnet.
Given these factors along with the aforementioned conditions relating to the thickness
and insertion depth, the interval and number of the cavity-forming members should
be determined so that the volume ratio will exceed the level where the required magnetic
properties are obtained.
[0032] Next, an appropriate width, insertion depth, number and interval of the cavity-forming
members will be explained for the case where the primary purpose of the cavities is
to help the grain boundary diffusion of Dy and/or Tb into the sintered compact. If
the cavity-forming member is too narrow, it is difficult to inject a substance containing
Dy and/or Tb into the slit formed in the sintered compact. Therefore, it is preferable
to form the slits with a width equal to or larger than 0.1 mm. If the interval of
the slits is too large, the effect of grain boundary diffusion cannot extend over
the entirety of the sintered magnet, causing the resulting product to have uneven
magnetic properties. Accordingly, the interval of the slits, or the interval of the
cavity-forming members, should preferably be equal to or smaller than 6 mm, and more
preferably equal to or smaller than 5 mm. With respect to the insertion depth, the
difference between this depth and the magnet's thickness in the direction of the insertion
depth should preferably be equal to or smaller than 6 mm, and more preferably equal
to or smaller than 5 mm. However, to ensure an adequate mechanical strength of the
sintered compact, the difference should preferably be equal to or larger than 1 mm,
and more preferably equal to or larger than 2 mm. Additionally, as in the previous
case where the primary purpose was to prevent the eddy current, the thickness, insertion
depth, number and interval of the cavity-forming members should be determined so that
the volume ratio of the product will exceed the level where the required magnetic
properties are obtained.
[0033] The previous examples illustrated the case of using a plate-shaped cavity-forming
member. If the primary purpose is to help the grain boundary diffusion, it is possible
to use a rod-shaped cavity-forming member. Fig. 6 shows one example, in which a large
number of rod-shaped cavity-forming members 34 are arrayed in rows and columns in
the form of a matrix on a plate-shaped attachment base 35. The use of such a large
number of rod-shaped cavity-forming members 34 in the form of a matrix results in
a sintered compact having a large number of fine pores (cavities). When a grain boundary
diffusion process is performed to create a sintered Nd-Fe-B magnet, Dy and/or Tb can
be efficiently diffused through these fine pores into the sintered compact.
[0034] To ensure the injection of a substance containing Dy and/or Tb, the diameter of the
fine pores formed in the sintered compact should preferably be equal to or larger
than 0.2 mm, and more preferably equal to or larger than 0.3 mm. The interval of the
cavity-forming members 34 should preferably be equal to or smaller than 6 mm, and
more preferably equal to or smaller than 6 mm, to diffuse Dy and/or Tb over the entirety
of the sintered magnet. The conditions to be considered for the insertion depth are
the same as in the case of the plate-shaped cavity-forming member.
[0035] The diffusion process includes filling a powder containing Dy and/or Tb into the
cavities 18 and then heating the filled powder (Fig. 7). The heating temperature is
typically within a range from 700 to 1000 degrees Celsius. The Dy/Tb-containing substance
to be injected into the cavities may be a fluoride, oxide, acid fluoride or hydride
of Dy or Tb, an alloy of Dy or Tb and another kind of metal, or a hydride of such
an alloy. Examples of the alloy of Dy or Tb and another kind of metal include alloys
of Ty or Tb and an iron group transition metal (e.g. Fe, Co or Ni), B, Al or Cu. The
grain boundary diffusion process can be effectively performed by mixing the aforementioned
substances in an organic or similar solvent to prepare a slurry, injecting this slurry
into the cavities, and heating the slurry. This slurry may be injected into the cavities
only, or it may be additionally applied to the surface of the sintered compact. In
latter case, the grain boundary diffusion takes place from both the cavities and the
surface of the sintered compact. After the slurry is injected into the cavities of
the sintered compact (and applied to its surface in some cases), the grain boundary
diffusion process is performed by heating the sintered compact at 700 to 1000 degrees
Celsius for one to twenty hours under vacuum or in an inert-gas atmosphere. This grain
boundary diffusion process uses only a small amount of Dy and/or Tb and yet can effectively
increase the coercive force of the sintered Nd-Fe-B magnet without significantly decreasing
its residual flux density even if the magnet has a substantially large thickness of
5 mm or larger.
[0036] In the case where the cavities are formed for both purposes of helping the grain
boundary diffusion process and reducing the loss of energy due to eddy currents, if
the aforementioned slurry is used in the grain boundary diffusion process, it is necessary
to control the amount of the slurry so that an electrically conductive component of
the injected slurry will not fill the cavity.
[0037] In any of the previously described embodiments, it is possible to fill the cavities
with an epoxy resin or similar embedding member to prevent a decrease in the mechanical
strength of the product due to the presence of the cavities and the corrosion or other
problems due to retention of moisture in the cavities. In this case, an epoxy resin
in a liquid state is injected into the cavities 18 and then cured at room temperature
or by heat (Fig. 8). For some type of material of the embedding member, this embedding
process can be performed before the sintering process. In the case of using an epoxy
resin or similar adhesive resin, this process is performed after the sintering process.
If the diffusion process is additionally performed, the embedding process is performed
after the diffusion process.
EXAMPLE 1
[0038] A strip-cast alloy of an Nd-Fe-B rare-earth magnet was subjected to hydrogen pulverization
and then a jet-mill process using nitrogen gas, to obtain a rare-earth magnet powder
with an average particle size of 5 µm. The composition of this rare-earth magnet powder
ratio was Nd: 25.8%, Pr: 4.3%, Dy: 2.5%, Al: 0.23%, Cu: 0.1%, and Fe: the rest. The
average particle size of the rare-earth magnet powder was measured with a laser-type
particle-size analyzer.
[0039] This powder was filled into the mold 10 of the first embodiment to an apparent density
of 3.5 g/cm
3, after which the lid 13 was put on the mold 10. Subsequently, the cavity-forming
members 14 were inserted through the insertion openings 131. After the mold 10 was
fixed in a magnetic-field generation coil, a pulsed magnetic field of 5 T was applied
three times in the direction parallel to the cavity-forming members 14 and perpendicular
to the bottom of the mold 10 so as to align the rare-earth magnet powder in the magnetic
field. Subsequently, the cavity-forming members 14 were pulled out from the mold 10,
and then the mold 10 was put into a sintering furnace. The entire process from the
filling of the powder to the putting of the mold into the furnace was carried out
in an argon-gas atmosphere. The sintering process was performed under vacuum at 1010
degrees Celsius for two hours. In this example, the mold 10 and the lid 13 were made
of carbon and the cavity-forming members 14 were made of non-magnetic stainless steel.
The thickness of the cavity-forming members 14 was 0.5 mm.
[0040] The sintered compact created by the previously described process had a density of
7.56 g/cm
3, which is as high as the density of a sintered Nd-Fe-B magnet created by a normal
pressing method. The obtained sintered compact 31 (Fig. 9) had the shape of a rectangular
parallelepiped having a short-side length of 37 mm, a long-side length of 39 mm and
a height of 8.6 mm, with two slits 32 extending parallel to the shorter sides and
at an interval of 12 mm on the top face. No noticeable deformation in the outside
shape of the sintered compact or the slits 32 was recognized. The slits 32 had a width
of approximately 0.4 mm and a depth of 6.2 mm. For inspection, a metallic foil having
a thickness of 0.3 mm was inserted into each slit 32. The result confirmed that none
of these slits 32 was clogged or closed with foreign matter.
EXAMPLE 2
[0041] Using the same powder as used in Example 1, a sintered Nd-Fe-B magnet with slits
was created by using the mold 20 and the cavity-forming members 24 of the second embodiment.
When the mold 20 of the second embodiment is used, the powder needs to be filled into
the mold 20 with the cavity-forming members 24 attached thereto. In filling the powder,
it is necessary to carefully fill it so that the powder will be uniformly put into
the entire receiving section 21. The filling density was 3.6 g/cm
3. After the powder was filled, the lid 23 was put on the mold 20. Subsequently, the
aligning process in the magnetic field and the removal of the cavity-forming members
24 were performed under the same conditions as in Example 1, and then the sintering
process was performed under the same conditions as in Example 1. After the sintering
process, the sintered compact was removed from the mold. Similar to the product created
in Example 1, the obtained sintered compact had a high density and no deformation
in its shape. The slits were also found to be high-quality slits free from clogging
or closing. The outside shape of the sintered compact, the interval of the slits,
the width and other sizes of each slit were approximately the same as those of Example
1.
EXAMPLE 3
[0042] A sintered compact with cavities (slits or fine pores) was created by using the molds
and cavity-forming members shown in Figs. 10 and 11. The mold 40 shown in Fig. 10
has a rectangular-parallelepiped receiving section 41 having square-shaped top and
bottom sides. A lid 43 can be attached to the top side. This lid 43 has two insertion
openings 431 for allowing the insertion of two plate-shaped cavity-forming members
44. The mold used in the example shown in Fig. 11 is the same as this mold 40. A lid
53 to be attached to the mold 40 in the latter example has four insertion openings
531 arranged in the form of a square, thus allowing the insertion of four rod-shaped
cavity-forming members 54.
[0043] Using the same rare-earth magnet powder and method as used in Example 1, a sintered
compact with slits (Example 3-1) and a sintered compact with fine pores (Example 3-2)
were created by using the cavity-forming members 44 and 54, respectively. Both sintered
compacts had a cubic outside shape with one side approximately measuring 11 mm. The
slits formed in the former sintered compact had a width of 0.4 mm and a depth of 5.9
mm, and were spaced by an interval of 3.3 mm. The fine pores formed in the latter
sintered compact had a diameter of 0.5 mm and a depth of 7.2 mm. For comparison, another
sintered compact having a rectangular-parallelepiped shape with neither slits nor
fine pores (Comparative Example 1) was also created under the same conditions as used
in the present Example (and Example 1) except that the insertion and removal of the
cavity-forming members 44 were omitted. Each of the three types of sintered compacts
was shaped into a cube with one side accurately measuring 10 mm by using a surface
grinder. The obtained cubes were then subjected to alkaline cleaning, acid cleaning
and pure-water cleaning processes followed by a drying process.
[0044] For these samples, a grain boundary diffusion process using a Dy-containing alloy
powder was performed as follows: Initially, a Dy-containing alloy having a composition
by atomic ratio of Dy: 80%, Ni: 14%, Al: 4%, and other kinds metals and impurities:
2 % was pulverized to an average particle size of 9 µm with a jet mill to obtain a
Dy-containing alloy powder. Next, this powder was mixed with ethanol by 50 % by weight
and stirred. The obtained mixture was vacuum-impregnated into the slits of the sample
of Example 3-1 and the fine pores of the sample of Example 3-2, and then dried. Subsequently,
the Dy-containing powder was applied to the surface of each of the magnets of Examples
3-1, 3-2 and Comparative Example. These three types of sintered compacts were put
into a vacuum furnace and heated at 900 degrees Celsius for three hours. After that,
they were rapidly cooled to room temperature, then heated to 500 degrees Celsius,
and again rapidly cooled to room temperature. The magnetic properties of the three
samples created in this manner are shown in Table 1. In this table, Comparative Example
1-1 was obtained by performing the aforementioned grain boundary diffusion process
on the sintered compact of Comparative Example 1. Comparative Example 1-2 was obtained
by heating the sintered compact of Comparative Example 1, without any Dy-containing
alloy powder applied to its surface, in the same manner as in the grain boundary diffusion
process.
[0045]
TABLE 1
|
Residual Flux Density Br[kG] |
Coercive Force HcJ [kOe] |
Maximum Energy Product (BH)max [MGOe] |
Ratio of Br to Saturated Magnetization Br/Js [%] |
Squareness Hk/HcJ [%] |
Example 3-1 |
12.7 |
28.6 |
39.8 |
94.3 |
93.7 |
Example 3-2 |
12.8 |
28.2 |
40.0 |
94.5 |
95.2 |
Comparative Example 1-1 |
13.0 |
24.6 |
41.2 |
94.3 |
72.2 |
Comparative Example 1-2 |
13.0 |
21.6 |
41.4 |
94.4 |
94.3 |
[0046] As compared to the sample of Comparative Example 1-1, for which the grain boundary
diffusion process was performed with neither slits nor fine pores, the samples of
Examples 3-1 and 3-2 had higher coercive forces H
cJ and higher squareness H
k/H
cJ of magnetization curves. Their coercive forces H
cJ were also higher than that of the sample of Comparative Example 1-2, for which no
grain boundary diffusion process was performed. These results demonstrate that the
method according to the present invention, which is an inexpensive method that does
not include the expensive machining process for forming slits after the sintering
process, is effective for enhancing the coercive force of a sintered Nd-Fe-B magnet
by grain boundary diffusion even in the case where the magnet is large sized, like
the 10-mm cube, for which the grain boundary diffusion process has not been effective
before.
EXPLANATION OF NUMERALS
[0047]
- 10, 20, 40
- Mold (Powder-Filling Container)
- 11, 21, 41
- Receiving Section of Mold
- 12
- Bottom of Mold
- 13, 23, 53
- Lid of Mold
- 131, 221, 431, 531
- Insertion Opening
- 14, 24, 34, 44, 54
- Cavity-Forming Member
- 15, 25, 35
- Attachment Base for Cavity-Forming Members
- 17, 27
- Magnetic-Field Generation Coil
- 18,28
- Cavity
- 19, 29
- Rare-Earth Magnet Alloy Powder
- 31
- Sintered Compact
1. A method for producing a sintered rare-earth magnet,
characterized in that a sintered rare-earth magnet having a cavity is produced by performing following
successive processes:
a) a filling process for filling a powder of rare-earth magnet alloy into a powder-filling
container together with a cavity-forming member;
b) an aligning process for aligning the rare-earth magnet alloy powder in a magnetic
field; and
c) a sintering process for sintering the rare-earth magnet alloy powder by heating
the rare-earth magnet alloy powder in a state of being held in the powder-filling
container, wherein
d) the cavity-forming member is removed after the aligning process is completed and
before the rare-earth magnet alloy powder begins to be sintered.
2. The method for producing a sintered rare-earth magnet according to claim 1, characterized in that the removal of the cavity-forming member is performed before the sintering process
is initiated.
3. The method for producing a sintered rare-earth magnet according to claim 1 or 2, characterized in that the cavity-forming member is a plate-shaped member or a rod-shaped member.
4. The method for producing a sintered rare-earth magnet according to claim 3, characterized in that the rare-earth magnet alloy powder is aligned in a magnetic field parallel to the
cavity-forming member in the aligning process.
5. The method for producing a sintered rare-earth magnet according to one of claims 1-4,
characterized in that a binder is filled into the powder-filling container together with the rare-earth
magnet alloy powder in the filling process.
6. The method for producing a sintered rare-earth magnet according to one of claims 1-5,
characterized in that an embedding member is filled into the cavity after the removal of the cavity-forming
member.
7. The method for producing a sintered rare-earth magnet according to one of claims 1-5,
characterized in that:
the rare-earth magnet alloy is an Nd-Fe-B magnet alloy; and
a diffusing process for diffusing Dy and/or Tb into the sintered compact is performed
by injecting a substance containing Dy and/or Tb into the cavity of the sintered compact
obtained by the sintering process.
8. The method for producing a sintered rare-earth magnet according to claim 7, characterized in that an embedding member is filled into the cavity after the diffusing process.
9. The method for producing a sintered rare-earth magnet according to claim 6 or 8, characterized in that the embedding member is made of an insulating material.
10. The method for producing a sintered rare-earth magnet according to one of claims 1-9,
characterized in that the filling process includes inserting the cavity-forming member into the powder-filling
container through an insertion opening formed in either the powder-filling container
or a lid of the powder-filling container, and the removal process includes pulling
out the cavity-forming member from the insertion opening.
11. A powder-filling container for producing a sintered rare-earth magnet,
characterized by comprising:
a mold into which a powder of rare-earth magnet alloy is to filled;
a lid to be attached to the mold; and
an insertion opening, formed in either the mold or the lid, for allowing insertion
of a cavity-forming member.
12. A powder-filling container for producing a sintered rare-earth magnet,
characterized by comprising:
a mold into which a powder of rare-earth magnet alloy is to be filled;
a lid to be attached to the mold; and
a cavity-forming member provided on either the mold or the lid.