Stator Structure Using Forming Curved Wafer Thin Magnets From Rare Earth-Cobalt Alloy Powders

These and other objects and advantages of our invention will be better understood in view of a detailed description which follows. Reference will be made to the drawings in which:

FIG. 1 depicts an elevation in cross-section of an apparatus for axially compressing RE-Co powders into arcuate wafer thin shapes including the workpiece and compacting tool assembly of mandrel, mandrel restraint, die liners, punch and powder;

FIG. 2 is a sectional view of the apparatus of FIG. 1 along line 2--2;

FIG. 3 is a plan view showing the workpiece assembly positioned in a magnetizing apparatus with flux lines generated by the coils;

FIG. 4 depicts a section of an assembly of green compacts, forming mandrel and die spacers in an evacuated steel casing prior to isostatic compaction;

FIG. 5 is a sectional view of the assembly of FIG. 4 along line 5--5;

FIG. 6 is a split sectional view of the assembly of FIG. 4 along line 5--5 comparing the RE-Co compacts in the steel casing before and after hot isostatic compaction;

FIG. 7 is an axial sectional view of the motor casing; and

FIG. 8 is a cross sectional view of a finished steel motor casing containing two arcuate shaped wafer thin RE-Co magnets along line 8--8 of FIG. 7.

Long, thin RE-Co magnets having circular curvatures are particularly good pole magnets for small cylindrically shaped D.C. motors. In a preferred embodiment of the invention not only can such pole magnets be easily made but they can advantageously be compacted against and metallurgically bonded to the casings of such motors by hot isostatic compaction. Moreover, the casing can be constructed so that the armature and bushings can be inserted at the ends. The motor casing itself functions as the return flux path for the motor during operation.

For example, a small, thin window lift motor was constructed with SmCo.sub.5 magnets 42 formed against and metallurgically bonded to a tubular motor casing 30 as shown in FIGS. 7 and 8. It is seen that the magnets are spaced apart and diametrically opposed.

Referring to FIGS. 1 and 2, a ferromagnetic mandrel 10 is employed having opposing surface segments 11 defining circular arcs sized to form the inside curved surface of the magnet compacts to be formed. Since it is preferred to have symmetric die loads on the mandrel during compaction at least two magnet compacts are formed at a time. The mandrel is provided with opposing ribs 13 to separate the compacts. The mandrel is slidably retained in a tightly fitting annular restraint ring 12. Ring 12 has an upper annular shoulder 15. Semicircular nitrided steel die liners 14 enclose the mandrel as seen in FIG. 2 and define cavities between themselves and surfaces 11 forming two long, thin, curved cavities 16 (shown filled with RE-Co powder). The bottom of the cavity 16 is defined by shoulder 15. The upper boundary of the cavity 16 is defined by punch 24 which is slidable in liners 14 and bears down on mandrel 10 and powder cavity 16. This assembly is placed in a split die block 18 of a hydraulic press.

SmCo.sub.5 powder was poured into the cavities. The die was vibrated by means not shown to assist downward powder flow. The powder was then lightly compacted by downward movement of punch 24 to a density of about 40% of the theoretical. The assembly of the restraint ring 12, die liners 14 and compacted powder in cavity 16 was removed from the die block 18.

The assembly was then placed in a magnetizing fixture 17 shown in FIG. 3 to align the SmCo.sub.5 powder. The fixture included soft iron blocks 19, magnetizing coils 20 and soft iron spacers 21 to hold the coils and compaction assembly in place. A current was pulsed through the magnetizing coils 20 to create a strong magnetic field across the assembly as illustrated by the field lines 22. The mandrel 10 is chosen to be permeable to a magnetic field so that it does not interfere with the aligning magnetic field. The powder in the cavities was magnetically aligned by the pulse to a radial north-south polarity with respect to the magnet curvature.

The assembly was removed then from the magnetizing fixture 17 and replaced in the split die block 18 of the press. The punch 24 was forced downward pushing mandrel 10 through lower restraint ring 12, the punch 24 and the stationary shoulder 15 exerting an axial compacting force on the powder in the cavities 16. The punch was extracted and the die blocks 18 were separated to release the compact assembly. The die liners 14 were removed and the two relatively strong magnetic green compacts with a density of about 70% of the theoretical were slid off the mandrel 10.

Referring to FIGS. 4 and 5, the green compacts 44 were positioned against a stainless steel mandrel 28 in opposing surface segments defining circular arc segments 23 sized to define the interior curved surfaces of the finished magnets, said segments being separated by opposing ribs 25. Since it was desired to fabricate a full length motor casing, the mandrel was sized to be longer than the RE-Co compacts and stainless steel spacers 40 were inserted in the surface segments of the mandrel above and below the green compacts. The compacts, mandrel and spacers were placed in a closely fitting tubular steel casing 30. The casing was sealed at one end with a solid plug 32 and a vented plug at the other end 34. The casing was then evacuated through the vent 36 and sealed 38. The assembly was then placed in an autoclave for hot isostatic compaction (HIP).

The green compacts were densified as hot, pressurized argon gas in the autoclave pushed the casing against the compacts, spacers and mandrel. FIG. 6 shows the green RE-Co compacts 44 in the casing 30 before HIP and the densified magnets 42 after HIP. It is noted that the casing is extremely pliable at HIP temperature and pressures so the casing deforms to match the circular contour of mandrel and spacers and collapses inwardly towards the densified compacts. Under such conditions the RE-Co magnets also form metallurgical bonds with the casing metal.

After the compacts were densified to greater than 90% of the theoretical density and metallurgically bonded to the casing, the assembly was cooled. The caps, stainless steel mandrel and spacers were removed leaving the SmCo.sub.5 pole magnets 42 appropriately positioned on the tubular steel motor casing 30 as shown in FIGS. 7 and 8. The casing can be cut to length and the motor armature easily inserted between the pole magnets.

Our invention is further described by the following specific example.

Equal parts by weight of a commercial SmCo.sub.5 powder (34.6% by weight samarium) and a commercial samarium-cobalt sintering aid composition containing 36.5% by weight samarium were milled together. The resulting mixture had a nominal powder particle size of 7 microns. The powdered mixture was poured into molding cavities as described above in connection with FIGS. 1 and 2. The cavities were defined in this instance by opposing 114.degree. arcs having an inside radius of 27 mm and an outside radius of 28 mm and a cavity length of about 58 mm. The die was vibrated by mechanical means to assist in packing the powder in the mold before compressions. The powder was loosely compacted in the press to a density of about 40% of the theoretical.

The assembly of the mandrel, die liners and lower restraint ring was removed from the split die block to a magnetizing apparatus as illustrated in FIG. 3. A single pulse of current in the magnetizing coils generated a field of 25,000 Gauss which aligned the SmCo.sub.5 powder to a high degree in a north-south radial pole direction across the full 114.degree. of magnet arc.

The assembly was replaced in the die press and the powder was axially compacted with a die force of about 1300 MPa to a pack density of about 70%. The split die block was then separated to release the assembly. The die liners were removed and the magnetized green SmCo.sub.5 compacts were slid off the mandrel. Although the compacts were fragile, they were easily removed from the mandrel to which they were strongly magnetically attracted without breaking.

The green compacts were positioned on a forming mandrel of AISI 303 stainless steel coated with boron nitride to prevent the compacts from bonding to it during HIP. The compacts and mandrel were inserted into a closely fitting tubular casing of 9 gage AISI 1008 steel. Stainless steel spacers were inserted above and below the green compacts in the casing to maintain its cylindrical shape during HIP and the casing was plugged as shown in FIG. 4. The casing was heated to 475.degree. C. under vacuum and the vent was sealed when a pressure of 10.sup.-3 mm.sub.Hg was achieved.

The green compacts were densified to 97% of theoretical and bonded to the casing under isostatic gas pressure in an autoclave. The casing was heated in the argon atmosphere of the autoclave to a temperature of 1000.degree. C. and maintained at this temperature at a pressure of ten (10) MPa for 30 minutes.

The casing was cooled and the stainless steel mandrel and inserts were removed leaving a tubular structure with densified SmCo.sub.5 magnets bonded thereto particularly suited for use as a D.C. motor casing.

In the above example, steel was used for the motor casing. However, it will be appreciated that in other embodiments where a ferromagnetic backing layer is desired for RE-Co magnets, other metals such as alloys of iron, nickel and cobalt are also suitable. It is preferred to use steel because it is relatively inexpensive and readily available.

Our method has been illustrated in terms of using samarium-cobalt powder to make the permanent magnets. This is a preferred embodiment but other rare earth-cobalt compositions including any of the following are similarly useful: yttrium, lanthanum, cerium, praseodymium, neodymium, promethium, europium, gadolinium, terbium, dysprosium, holmium, erbium, thulium, ytterbium and lutetium. The rare earth constituent may also be in the form of misch metals, naturally occurring compositions. An exemplary misch metal is cerium misch metal which typically comprises by weight about 53% cerium, 24% lanthanum, 5% praseodymium, 16% neodymium, and 2% other rare earths. Moreover, as is known in the art, small percentages of elements such as copper or alumimum may be added to the RE-TM compositions to improve the coercivity of the magnets.

The green compacts were pressed in a split die block according to the example. However, a one piece die block may be used and the green compacts ejected from it by causing the upper punch to push the compacts, mandrel and lower restraint through the block.

The die press arrangement shown in FIG. 1 is particularly suited for axially compacting the RE-Co powders between the thin curved ends of the die cavities. In this arrangement, the floating mandrel serves to distribute the compacting force over the whole working surface area of the punch reducing the tendency of the punch to gall or warp in production. Therefore, high compaction forces can be applied to form strong green compacts without damaging the tools. Green compacts must have a pack density of at least 65% to be handled without breaking.

Densification of RE-Co powder compacts in the HIP occurs essentially by the radial inward displacement of the flexible casing around the green magnet compacts. The casing is pressed against the magnet compacts and the mandrel without buckling or creasing providing that the original pack density of the rare earth-cobalt powder in the green compacts approaches about 60% of theoretical. Also, a casing in which the green compacts and forming mandrel are placed must be such that it can be sealed and evacuated and maintain a good vacuum at pressures and temperatures reached during HIP. Moreover, it is important that the casing metal be flexible enough to deform around the magnets during hot isostatic compaction.

Although green compacts can be compressed in the same direction as the magnetic alignment of the powder, it is preferable to compact the powders in a direction perpendicular to their magnetic alignment. Commercial magnet producers have reported a 10 to 15% improvement in magnetic flux when cold pressing is done perpendicular to the magnetic alignment direction of SmCo.sub.5 powder. (Hitachi Magnets Corporation, Permanent Magnet Motor Seminar, Jan. 20-21, 1976, Grand Rapids, Michigan).

In the example only two magnets were compacted in one casing, however, numerous compacts can be positioned on a single, longer forming mandrel and placed in a suitably sized can. The maximum length of the casing is limited primarily by the size of the HIP apparatus and the ability to achieve a good vacuum in the casing.

The casing is evacuated to prevent the expansion of residual gases during HIP. Such gases would effectively decrease the externally applied fluid pressure during HIP and hinder magnet densification. Moreover, RE-Co powders are highly reactive at elevated HIP temperatures and the magnets would be contaminated if residual gases were present.

Hot isostatic compaction of RE metal-cobalt magnet compositions can be accomplished in any gas environment having an atmosphere nondestructive to the sealed casing at temperatures in the range of about 900.degree. to 1200.degree. C. and at pressures of from about three (3) to 200 MPa. A typical time for HIP is about 30 minutes, however, any time sufficient to densify magnets to a density greater than 90% and bond them to the backings is appropriate. Examination of magnets compacted by HIP showed good intermetallic bonds between rare earth-cobalt magnets and steel backings with little intermingling of the metals.

The mandrel used in the HIP process is preferably coated with a material that keeps it from bonding to the RE-Co compacts at high temperatures and pressures. Boron nitride is a suitable coating. Moreover, it is preferred that the forming mandrel have a coefficient of thermal expansion higher than that of the casing material and the RE-Co magnets so that when the assembly cools, the mandrel shrinks away from the metal backed magnets and can be easily removed from the casing and magnets.

Magnets made by the methods taught herein are particularly suitable for use in small D.C. motors such as those used in automobile window lift motors. Among the advantages of using this method are the easy handling extremely brittle compacts of rare earth-cobalt materials elimination of the necessity for diamond grinding flat magnets to achieve arcuate surfaces, and minimization of waste of expensive rare earth-cobalt powders. Moreover, the magnets are integrally bonded to a casing during the HIP process and the casing may serve directly as a motor casing providing a return pass for magnetic fluxes during motor operation.

While our invention has been disclosed in terms of specific embodiments, it will be appreciated that other forms could readily be adapted by one skilled in the art. Accordingly, the scope of our invention is to be considered limited only by the following claims.