GB2057194A - A method of producing a permanent anisotropic magnet - Google Patents
A method of producing a permanent anisotropic magnet Download PDFInfo
- Publication number
- GB2057194A GB2057194A GB8025362A GB8025362A GB2057194A GB 2057194 A GB2057194 A GB 2057194A GB 8025362 A GB8025362 A GB 8025362A GB 8025362 A GB8025362 A GB 8025362A GB 2057194 A GB2057194 A GB 2057194A
- Authority
- GB
- United Kingdom
- Prior art keywords
- magnetic
- magnet
- anisotropic
- convergent
- permanent
- 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.)
- Granted
Links
- 238000000034 method Methods 0.000 title claims abstract description 23
- 230000006698 induction Effects 0.000 claims abstract description 16
- 230000004907 flux Effects 0.000 claims abstract description 9
- 239000000696 magnetic material Substances 0.000 claims abstract description 8
- 238000004519 manufacturing process Methods 0.000 claims description 14
- 239000000463 material Substances 0.000 claims description 14
- 239000000843 powder Substances 0.000 claims description 5
- 230000005415 magnetization Effects 0.000 claims description 3
- 230000005389 magnetism Effects 0.000 claims description 2
- 239000011230 binding agent Substances 0.000 abstract description 2
- 230000008569 process Effects 0.000 description 5
- 239000012141 concentrate Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 239000002245 particle Substances 0.000 description 2
- SUBDBMMJDZJVOS-UHFFFAOYSA-N 5-methoxy-2-{[(4-methoxy-3,5-dimethylpyridin-2-yl)methyl]sulfinyl}-1H-benzimidazole Chemical compound N=1C2=CC(OC)=CC=C2NC=1S(=O)CC1=NC=C(C)C(OC)=C1C SUBDBMMJDZJVOS-UHFFFAOYSA-N 0.000 description 1
- 229910001047 Hard ferrite Inorganic materials 0.000 description 1
- 229910016629 MnBi Inorganic materials 0.000 description 1
- 229910002837 PtCo Inorganic materials 0.000 description 1
- 229910000828 alnico Inorganic materials 0.000 description 1
- 238000005266 casting Methods 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 238000002425 crystallisation Methods 0.000 description 1
- 230000008025 crystallization Effects 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000001125 extrusion Methods 0.000 description 1
- 238000009432 framing Methods 0.000 description 1
- 238000000227 grinding Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 238000003754 machining Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 238000005096 rolling process Methods 0.000 description 1
- 239000000523 sample Substances 0.000 description 1
- 238000005476 soldering Methods 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 239000007858 starting material Substances 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F7/00—Magnets
- H01F7/02—Permanent magnets [PM]
- H01F7/0205—Magnetic circuits with PM in general
- H01F7/021—Construction of PM
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/02—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
- H01F41/0253—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing permanent magnets
- H01F41/0286—Trimming
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Manufacturing & Machinery (AREA)
- Manufacturing Cores, Coils, And Magnets (AREA)
- Hard Magnetic Materials (AREA)
Abstract
In a method of producing a magnet with a convergent magnetic orientation to raise to magnetic induction by concentrating the magnetic flux into a reduced cross-section, anisotropic permanent magnetic material where the magnetic orientations converge to each other is combined, magnetisation being effected either before or after combination. The magnet may be pressed with a binder, sintered, cast in a mould or built up from separate, machined parts. <IMAGE>
Description
SPECIFICATION
A method of producing a permanent anisotropic magnet
The invention relates to a method of manufacturing an anisotropic permanent magnet, having a convergent controlled orientation throughout at least part of the magnet body.
Anisotropic permanent magnets have many uses where one desires rapid magnetic induction into an air gap or other portion of a magnetic circuit. The anisotropic magnets used at present are of the type where the directions of easy magnetization of the elementary magnet constituents (such as powder particles with pulverized materials or crystals with cast materials) are co-extensively oriented into the overall direction in which the complete permanent magnet is magnetized. In this way considerably higher values of remanence and (BH)max product are obtained, compared with isotropic non-oriented magnets.
In many cases it is preferable to apply magnets in the entire volume or in a part having an orientation of easy magnetization axes. This orientation is convergent at at least one pole surface. Thus, it is possible to raise substantially the magnetic induction value in the pole region, compared with existing homogeneously oriented magnets. The increase in magnetic induction present in the surrounding space is achieved over a smaller cross-section than that of the magnet itself. This effect is caused by the fact that the convergent orientation concentrates the magnetic flux, raises its density and reduces the flux of magnetic leakage.
Various processes can be used to achieve an homogeneous anisotropic structure with existing magnets, depending upon the material typeorientation of powder particles by a magnetic field, crystallization resulting from a directed temperature gradient, extrusion, rolling and other properties.
Present technology enables a series production of magnets, the homogeneous orientation of which is almost ideal.
To produce a convergent oriented structure that would raise the magnetic induction in a desired region is, as a rule, more difficult than to produce an orthodox homogeneous orientation, since specific processes for manufacturing permanent magnets with controlled convergent structure have not yet been developed. As a result, wide use of this type of magnet is impossible, in spite of the fact that in many applications, it would substantially improve the parameters of magnetic circuitry.
We have developed a magnet which can eliminate or reduce these drawbacks of the prior art.
Thus, the present invention consists in a method of producing a permanent anisotropic magnet having a convergent magnetic orientation throughout at least part of its body which raises magnetic induction by concentrating the magnetic flux into a reduced cross-section, which comprises combining anisotropic parts of magnetic material, to give a magnetic orientation comprising two or more con vergentconfigurations, magnetism being induced in the material either before or after combination.
The invention also consists in the magnet itself.
Forthe manufacture of conventional homogeneously oriented parts of the final magnet, it is possible to employ known processes for manufacturing anisotropic magnets. As an example there can be named processes for manufacturing an isotropic powdered magnets pressed in combination with a binder, or sintered, or cast anisotropic magnets. The desired shapes of the parts can be obtained either directly by using suitable press dies, casting moulds and like devices, or by dividing into parts, or by machining homogeneously oriented magnets of other forms as, e.g., by cutting and grinding. The parts can be fixed to one another to produce a final magnet having a convergent magnetic orientation; this can be effected by various mounting methods, such as encasing, screwing, framing, cementing and soldering.
It is to be understood that the parts can be combined together at different stages of the overall method. The parts can be either ready-to-use permanent magnets, orsemi-finished products. Thus, for instance, in the manufacture of sintered powder magnets, one can combine parts made of the final sintered material, or powder pressed pieces that are not sintered until they are fused into a complex.
Alternatively, one may use cast magnets wherein the parts can be combined with one another before or after heat treatment. Furthermore, the parts can be combined in the magnetized or unmagnetized state.
In the former case, repulsive forces have to be coped with, whereas in the latter it should be ensured that the final magnet be magnetised in accordance with a convergent orientation.
According to the invention, permanent magnets with convergent orientation can be made, preferably, from any of the known magnetically hard materials, such as magnetically hard ferrites, rare earth based materials, AlNiCo, PtCo, MnAI and
MnBi. The final magnets can be made in various forms, such as prisms, pyramids, cones, cylinders, annuli, rods, U-, C-, E-shapes, and in intricate or irregular forms with apertures, notches or projections.
Convergently oriented structures of magnets manufactured by the method of the invention can have various configurations. Particular structures may be designed according to the desired spatial distribution of magnetic induction to be supplied by the magnet into the surrounding space. The standard forms, dimensions and magnetic characteristics of materials used for manufacturing permanent magnets may be taken into consideration. Thus, for example, convergently oriented structures concentrate the magnetic flux into a larger or smaller region in the centre of area of one, two or more poles. The modification of the directions of orientation in the convergent structure in the magnet body can take place either continuously, or discretely.The anisotropic convergent structure can be produced in one or more parts, or throughout the entire magnet body, it can be linear, curvilinear, continuous, or stepwise, and it can be produced in two orthree dimensions. The shapes and dimensions of the individual parts will be selected so as to give, after the combination, a magnet having a desired form and size. The parts can have various forms, such as prisms, pyramids, cones, annuli, and other solids. To achieve a convergent magnetic structure which comprises two or more convergently oriented configurations, the parts should be oriented so that the orientations of adjacent pa rts are inclined towards each other, and are magnetized so thattheir like polarities point to the same pole.The inclination angles and the number of parts with convergent orientations will be chDsen according to the required degree of convergency and to the number of various orientation configurations in the convergent structure of the final magnet.
The invention is now further illustrated by the following example, with reference to the accompanying drawings, each of which depicts a magnet.
Example
A sintered ferrite magnet of convergent structure was made in theform of a right parallelepiped having the dimensions 2525,12 mm. The convergent structure raised the value of magnetic induction discharged by the 2 & 25 mm area of the S pole in the region of the axis passing through the centre of this area.
Figure 7a shows this anisotropic structure in a sectional view taken parallel to the magnet axis pointing to the pole, while
Figure ib is a view perpendicular to the pole area.
The magnet was made by combining three pieces of sintered, homogeneously oriented parts, shown separated in
Figure 2 which also shows their orientation.
Figure 3 shows the final magnet manufactured by combining these parts.
In this way a substantial increase in induction was achieved in the central part of the pole area, compared with conventional anisotropicpermanent magnets. By way of example, it is possible to refer to the value of magnetic induction present adjacent to the pole surface, measured by a Hall probe applied close to the centre of the pole area. The comparison was carried out by measuring reference magnet specimens made of the same material and having the same dimensions. A conventional homogenously oriented magnet in the central area region gave an induction of 0.125 T, and the magnet manufactured from parts as shown in Figures 2 and 3 gave an aimost double induction of 0.249 T.
The process of manufacturing magnets according to the invention has many advantages. It is particularly advantageous that various configurations of convergently oriented structures can be produced, according to the required characteristics of the final rnagnet. Among such structures there may also be some extreme cases, the manufacture of which in other ways would be very difficult, if not impossible.
An example of this is convergent orientations which concentrate the magnetic flux as much as possible into a narrow region, orto magnets having complicated shapes, or a plurality of poles.
As starting materials it is possible to use currently available anisotropic, magnetically hard materials,
or final magnets. Also the techniques for manufac
ture are relatively simple and inexpensive. For these
reasons, the method of the invention can be used by the magnet users themselves who are not equipped,
as a rule, with means for series production of
magnetically hard materials.
The magnets ofthe invention have many uses. An
increase in the magnetic induction at an air gap or at
any other parts of the magnetic circuit, compared to that of the conventional magnets, improves the
operation of, for example, motors, engines, drive
units and generators having permanent magnets,
microwave appliances, measuring apparatuses,
electroacoustictransducers, magnetic pick-ups, re
lays, bearings, clutches, separators and clamping
elements. The improvement can result from lower power demand, higher efficiency, output, torque,
attractive or repulsive force effects, sensitiveness
and accuracy, depending on the application. Another
merit of the present invention is the various possibi
lities of miniaturization of magnetic circuitry, reduction of material costs, longer lifetime and simplified structure.
Claims (10)
1. A method of producing a permanent anisotropic magnet having a convergent magneticorientation throughout at least part of its body which raises the magnetic induction by concentrating the magnetic flux, which comprises combining anisotropic magnetic material to give a magnetic orientation comprising two or more convergent configurations, magnetism being induced in the material either
before or after combination.
2. A method according to Claim 1, in which the magnet is a sintered powdered magnet.
3. A method according to Claim 2, in which sintered anisotropic magnetic material is combined.
4. A method according to Claim 2, in which unsintered powder pressed an isotropic magnetic material is combined, and the combination sintered.
5. A method according to Claim 1, in which cast anisotropic magnetic material is heat treated and then combined.
6. A method according to Claim 1, in which combined anisotropic magnetic material is heattreated.
7. A method of producing a permanent anisotropic magnet substantially as herein described with reference to any one of the accompanying drawings.
8. A permanent anisotropic magnet produced by a method according to any one of the preceding claims.
9. A permanent anisotropic magnet, comprising at least two pieces of magnetic material aligned to give a convergent magnetic orientation which raises magnetic induction by concentrating magnetic flux.
10. A method of manufacturing anisotropic permanent magnets with a convergent magnetic orientation in a part of or in the entire magnet body to raise the magnetic induction by concentrating the magnetic flux into a reduced cross-section, the method comprising manufacturing a final magnet by combining together anisotropic parts made of a permanent magnet material and complementing said parts, according to their shapes and dimensions, so as to give the final magnet of the desired shape and dimensions, the magnetic orientation which comprises two or more various convergent configurations, being produced in such a manner that at least with two adjacent parts, the magnetic orientations converge to each other, and their magnetization polarities point toward one and the same pole.
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CS537679A CS213750B1 (en) | 1979-08-03 | 1979-08-03 | Method of making the anizotropic permanent magnets |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| GB2057194A true GB2057194A (en) | 1981-03-25 |
| GB2057194B GB2057194B (en) | 1983-09-14 |
Family
ID=5398545
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| GB8025362A Expired GB2057194B (en) | 1979-08-03 | 1980-08-04 | Method of producing a permanent anisotropic magnet |
Country Status (5)
| Country | Link |
|---|---|
| JP (1) | JPS5654015A (en) |
| CS (1) | CS213750B1 (en) |
| DE (1) | DE3029380A1 (en) |
| FR (1) | FR2463494B1 (en) |
| GB (1) | GB2057194B (en) |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4536230A (en) * | 1979-03-13 | 1985-08-20 | Stani Vyzkumny Ustav Materialu | Anisotropic permanent magnets |
| EP0161832A1 (en) * | 1984-04-23 | 1985-11-21 | Field Effects, Inc. | Tunable segmented ring magnet and method of manufacture |
| US4710239A (en) * | 1984-09-14 | 1987-12-01 | General Motors Corporation | Hot pressed permanent magnet having high and low coercivity regions |
| EP0174735A3 (en) * | 1984-09-14 | 1988-01-20 | General Motors Corporation | Hot pressed permanent magnet having high and low coercivity regions |
| EP0393815A1 (en) * | 1989-04-15 | 1990-10-24 | Fuji Electrochemical Co.Ltd. | Method for packing permanent magnet powder |
| GB2311891A (en) * | 1996-04-04 | 1997-10-08 | Analytical Precision Ltd | A method of forming a magnetic body, e.g. for a mass spectrometer |
| GB2380309A (en) * | 2001-08-20 | 2003-04-02 | Richard Wolfe | Magnetic device for reduction of EMI in audio circuitry |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60214517A (en) * | 1984-04-10 | 1985-10-26 | Nissin Electric Co Ltd | Manufacture of ring permanent magnet magnetized in radial direction |
| JPS6424803U (en) * | 1987-08-06 | 1989-02-10 | ||
| DE19736295C1 (en) * | 1997-08-21 | 1999-06-02 | Freudenberg Carl Fa | Magnetic system, comprising one or more permanent magnets attached to a carrier body |
| JP2003197419A (en) * | 2001-12-27 | 2003-07-11 | Techno Takatsuki Co Ltd | Polar anisotropic magnet |
Family Cites Families (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| BE440964A (en) * | 1939-10-05 | |||
| FR1182885A (en) * | 1956-09-19 | 1959-06-30 | Philips Nv | Permanent magnet comprising on either side of a given line magnetic poles of opposite polarity |
| GB842531A (en) * | 1958-12-24 | 1960-07-27 | Mullard Ltd | Permanent magnets |
| US3334254A (en) * | 1965-06-03 | 1967-08-01 | Garrett Corp | Dynamoelectric machine |
| US3768054A (en) * | 1972-04-03 | 1973-10-23 | Gen Electric | Low flux leakage magnet construction |
| US4185262A (en) * | 1977-08-01 | 1980-01-22 | Matsushita Electric Industrial Co., Ltd. | Magnet device |
| JPS6028377B2 (en) * | 1979-02-08 | 1985-07-04 | 松下電器産業株式会社 | Manufacturing method for rolled magnets |
-
1979
- 1979-08-03 CS CS537679A patent/CS213750B1/en unknown
-
1980
- 1980-08-01 DE DE19803029380 patent/DE3029380A1/en active Granted
- 1980-08-01 FR FR8017088A patent/FR2463494B1/en not_active Expired
- 1980-08-04 JP JP10649880A patent/JPS5654015A/en active Pending
- 1980-08-04 GB GB8025362A patent/GB2057194B/en not_active Expired
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4536230A (en) * | 1979-03-13 | 1985-08-20 | Stani Vyzkumny Ustav Materialu | Anisotropic permanent magnets |
| EP0161832A1 (en) * | 1984-04-23 | 1985-11-21 | Field Effects, Inc. | Tunable segmented ring magnet and method of manufacture |
| US4710239A (en) * | 1984-09-14 | 1987-12-01 | General Motors Corporation | Hot pressed permanent magnet having high and low coercivity regions |
| EP0174735A3 (en) * | 1984-09-14 | 1988-01-20 | General Motors Corporation | Hot pressed permanent magnet having high and low coercivity regions |
| EP0393815A1 (en) * | 1989-04-15 | 1990-10-24 | Fuji Electrochemical Co.Ltd. | Method for packing permanent magnet powder |
| GB2311891A (en) * | 1996-04-04 | 1997-10-08 | Analytical Precision Ltd | A method of forming a magnetic body, e.g. for a mass spectrometer |
| GB2380309A (en) * | 2001-08-20 | 2003-04-02 | Richard Wolfe | Magnetic device for reduction of EMI in audio circuitry |
| GB2380309B (en) * | 2001-08-20 | 2005-04-06 | Richard Wolfe | Magnetic device for reduction of electromagnetic interference (EMI) in audio circuitry |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5654015A (en) | 1981-05-13 |
| GB2057194B (en) | 1983-09-14 |
| DE3029380A1 (en) | 1981-03-26 |
| FR2463494A1 (en) | 1981-02-20 |
| DE3029380C2 (en) | 1989-04-13 |
| CS213750B1 (en) | 1982-04-09 |
| FR2463494B1 (en) | 1987-01-23 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PCNP | Patent ceased through non-payment of renewal fee |
Effective date: 19920804 |