KR20010086147A - Process for preparation of magnet having an inclined magnetic force line and magnetic motor utilizing it - Google Patents
Process for preparation of magnet having an inclined magnetic force line and magnetic motor utilizing it Download PDFInfo
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- KR20010086147A KR20010086147A KR1020017008952A KR20017008952A KR20010086147A KR 20010086147 A KR20010086147 A KR 20010086147A KR 1020017008952 A KR1020017008952 A KR 1020017008952A KR 20017008952 A KR20017008952 A KR 20017008952A KR 20010086147 A KR20010086147 A KR 20010086147A
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F7/00—Magnets
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K53/00—Alleged dynamo-electric perpetua mobilia
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F13/00—Apparatus or processes for magnetising or demagnetising
- H01F13/003—Methods and devices for magnetising permanent magnets
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- 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
- H01F41/0273—Imparting anisotropy
- H01F41/028—Radial anisotropy
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K1/00—Details of the magnetic circuit
- H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
- H02K1/12—Stationary parts of the magnetic circuit
- H02K1/17—Stator cores with permanent magnets
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K1/00—Details of the magnetic circuit
- H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
- H02K1/22—Rotating parts of the magnetic circuit
- H02K1/27—Rotor cores with permanent magnets
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K49/00—Dynamo-electric clutches; Dynamo-electric brakes
- H02K49/10—Dynamo-electric clutches; Dynamo-electric brakes of the permanent-magnet type
- H02K49/104—Magnetic couplings consisting of only two coaxial rotary elements, i.e. the driving element and the driven element
- H02K49/106—Magnetic couplings consisting of only two coaxial rotary elements, i.e. the driving element and the driven element with a radial air gap
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K49/00—Dynamo-electric clutches; Dynamo-electric brakes
- H02K49/10—Dynamo-electric clutches; Dynamo-electric brakes of the permanent-magnet type
- H02K49/104—Magnetic couplings consisting of only two coaxial rotary elements, i.e. the driving element and the driven element
- H02K49/108—Magnetic couplings consisting of only two coaxial rotary elements, i.e. the driving element and the driven element with an axial air gap
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Manufacturing & Machinery (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Permanent Field Magnets Of Synchronous Machinery (AREA)
Abstract
Description
종래의 자석은 자력선이 N,S극과 모두 수직방향으로 자화되어 있고 따라서 자장은 좌우 N,S극의 직선방향과 그 직선방향의 좌우 방사상으로만 형성되어 있다.In the conventional magnets, the magnetic force lines are magnetized in both the N and S poles in the vertical direction, and thus the magnetic field is formed only in the linear direction of the left and right N and S poles and in the left and right radial directions thereof.
그러므로 자력에 의해 작동되는 모터와 같은 동력장치에 있어서는 천연자석이나 인공 자석 또는 전자석이나를 막론하고 자력에 의한 동력장치의 고정자와 회전자는 상호 대향되는 동일한 극이 되도록 장착하여야 하기 때문에 자석에 의한 모터와 같은 동력장치를 제작하는데에는 구조적으로 한계가 있었다.Therefore, in a power device such as a motor operated by magnetic force, the stator and the rotor of the power device by magnetic force, whether natural or artificial magnets or electromagnets, should be mounted to be the same poles facing each other. There was a structural limitation in manufacturing the same power unit.
예컨데 수직 또는 수평 어느 한 방향으로만 자력선을 가진 자석으로 모터와 같은 동력장치를 제작하려면 고정자와 회전자의 대향되는 외주면 전체가 수직이나 수평 방향으로 서로 배타적인 동일한 극, 예컨데 N,N극 이나 S,S극을 띄도록 설치하여야 했었다.For example, to manufacture a motor-driven device with magnets with magnetic lines in either the vertical or horizontal direction, the same poles, such as N, N or S, whose entire outer circumferential surface of the stator and rotor are mutually exclusive in each other in the vertical or horizontal direction It had to be installed so that it had a S pole.
그러나 상기와 같은 종래의 수직방향으로만 자력선을 형성한 자석에 의한 동력장치는 인공자석이나 천연자석 또는 전자석을 막론하고 순전히 동일극의 서로 배타적인 반발력에만 의존하고 있어서 그 장치의 회전 가속도에 의한 추진력이 없기 때문에 자력소모가 심하면서도 동력은 약한 결점이 있었다. 예컨데 전자석인 경우 전기력이 갑자기 단절되면 동력장치 자체의 가속도와 추진력이 전혀 없기 때문에 갑자기 동력장치가 중단되는 등의 폐단이 있었다.However, such a power unit by a magnet having a magnetic field line formed only in the vertical direction as described above relies solely on mutually exclusive repulsive forces of the same pole regardless of artificial magnets, natural magnets, or electromagnets, and thus the driving force due to the rotational acceleration of the device. Because of this lack of self-consumption but weak power. For example, in the case of electromagnets, when the electric force was suddenly disconnected, there was a sudden breakdown of the power unit because there was no acceleration and propulsion of the power unit itself.
본원은 상기와 같은 종래 수직방향 자력선을 갖는 자석의 자력을 이용한 모터와 같은 동력장치의 결점을 개량한 것으로서, 특히 자력선을 편향되게(경사지게) 자화시킨 자석의 동일극을 마주보게 설치하여 그 동일극의 배타적인 자체 반발력에 의한 회전력에, 편향된 자력선을 가진 자석의 편향된 방향으로의 회전력에 의해 발생되는 가속도가 추가되어 자체 자력에 의한 회전력보다 훨씬 강한 회전력을 갖도록한 자석을 제조하고 그 자석을 이용한 동력장치인 자석모터를 제공코저하는 것으로서 이를 첨부된 도면을 참조하여 상세히 설명하면 다음과 같다.The present application improves the shortcomings of a power device such as a motor using a magnetic force of a magnet having a conventional vertical magnetic force line as described above. In particular, the same pole is installed to face the same pole of a magnet magnetized to be deflected (inclined). In addition to the rotational force due to the exclusive self-repulsion force of, the acceleration generated by the rotational force of the magnet with the deflected magnetic lines in the deflected direction is added to produce a magnet having a rotational force that is much stronger than the rotational force by its own magnetic force, The present invention provides a magnet motor as a device, which will be described in detail with reference to the accompanying drawings.
본 발명은 자력선이 편향되게, 즉 경사지게 형성되도록 자화시킨 자석을 제조하는 방법과 그 자석에 의한 자석모터를 제공코저하는 것이다.The present invention provides a method of manufacturing a magnet that is magnetized so that magnetic lines of force are deflected, that is, inclined, and a magnet motor by the magnet.
도 1(a) 은 본 발명에 따른 높이가 높은 원통형의 자화된 자석과 자화할 자석의 평면 구성도.Figure 1 (a) is a plan view of a high height cylindrical magnetized magnet and a magnet to magnetize according to the present invention.
도 1(b) 는 도1(a)의 A-A'선 종단면도.Fig. 1 (b) is a longitudinal cross-sectional view taken along the line A-A 'of Fig. 1 (a).
도 2 는 도1(a)와 같은 방법으로 제조된 자석을 이용한 원통형 모터의 측단면도.Figure 2 is a side cross-sectional view of a cylindrical motor using a magnet manufactured by the same method as in Figure 1 (a).
도 3(a) 는 본 발명에 따른 원판형의 자화된 자석과 자화할 자석의 종단면도.Figure 3 (a) is a longitudinal cross-sectional view of a disk-shaped magnetized magnet and a magnet to be magnetized in accordance with the present invention.
도 3(b) 는 도 3(a)의 B-B'선 종단면도.(B) is B-B 'longitudinal cross-sectional view of FIG.
도 4(a) 는 도3(a)의 방법으로 제조한 원판형 자석을 이용한 자석 모터의 횡단면도.Figure 4 (a) is a cross-sectional view of a magnet motor using a disk-shaped magnet manufactured by the method of Figure 3 (a).
도 4(b) 는 도4(a)모터의 측면도.4 (b) is a side view of the motor of FIG. 4 (a).
도 5(a) 는 원통형 자석모터에서 고정자와 회전자의 상하 양단이 동일극으로 형성된 예의 측면도.Figure 5 (a) is a side view of an example in which the upper and lower ends of the stator and the rotor are formed in the same pole in the cylindrical magnet motor.
도 5(b) 는 도 5(a)의 C-C'선 횡단면도.Fig. 5 (b) is a cross-sectional view taken along the line C-C 'in Fig. 5 (a).
도 6 은 상하 양단이 동일극으로 형성된 여러개의 호형 단편자석을 결합한 원통형자석 모터의 측면도.Figure 6 is a side view of a cylindrical magnet motor that combines a plurality of arc-shaped fractional magnets, both upper and lower ends formed in the same pole.
도1(a)(b)에 도시된 바와같이, 원주전체에 걸쳐 남극(S)(1)과 북극(N)(2)으로된 다수개의 호형단편 자석을 반복적으로 형성하도록 자화시켜서된 대직경의 원통형 자석(3)을 외각에 위치시키고 그 내측에 만들고저 하는 원통형 자석의 두께만큼의 간격(5)을 유지하면서 상기 대직경의 원통형 자석과 동일방법으로 제작한 동일형태의 소직경의 원통형 자석(4)을 축(6)을 중심으로 고정시키되, 대직경의 원통형 자석(3)의 남북극(1)(2)의 경계면(8)과 소직경의 원통형자석(4)의 남북극(1')(2')의 경계면(8a)이 서로 엇갈리도록 위치시킨 상태에서 상기 대직경의원통형 자석(3)과 소직경의 원통형자석(4)사이의 간격(5)에 자석용 철광(페라이트) 분말을 충전한 다음 압착하여 통상의 자석 제조방법으로 자석을 제조하므로써 그 자석이 대직경의 원통형 자석(3)내면과 접한 외주면은 그 대직경 자석의 극과 동일극이 되고, 소직경의 원통형 자석(4)외주면과 접한 내주면은 그 소직경 자석의 극과 동일극이 되어 N-S자력선이 편향되게 자화된 자석을 얻거나, 이와 유사한 방법으로 도3에서 참조되는 바와같이 수직방향으로 남북극(1a)(2a)의 자력선이 형성된 원판형 자석(3a)(4a)및(5a)를 만들고져 하는 원판형 자석의 높이만큼의 간격(6a)(7a)들을 두고 배치 고정하되, 상기 원판형자석(3a)(4a)및(5a)의 중심(9)(9a)및(9b)를 각각 엇갈리게 금형(9')(9a')(9b')내에 배열하여 상기 간격(6a)(7a)들 내에 자석용 철광분말을 충전한 다음 압착하여 통상의 자석 제조방법으로 자석을 제조하므로써, 그 자석의 상하가 상기 원판형 자석(3a)(4a) 및(5a)와 맞닿는 면의 극과 동일한 극이 되게하여 N-S자력선이 편향되게 자화된 원판형자석을 제조한다.As shown in Fig. 1 (a) (b), a large diameter magnetized to repeatedly form a plurality of arc-shaped fragment magnets consisting of the south pole (S) (1) and the north pole (N) (2) throughout the circumference. Small diameter cylindrical magnets of the same type manufactured in the same manner as the large diameter cylindrical magnets while maintaining the distance 5 as the thickness of the cylindrical magnets to be placed on the outer shell of the cylindrical magnet 3 (4) is fixed about the axis (6), but the interface (8) of the north and south poles (1) and (2) of the large diameter cylindrical magnets (3) and the north and south poles (1 ') of the small diameter cylindrical magnets (4). Iron ferrite (ferrite) powder for magnets is placed in the interval 5 between the large diameter cylindrical magnet 3 and the small diameter cylindrical magnet 4 in a state where the interface 8a of 2 'is staggered. After charging, the magnet is manufactured by the normal magnet manufacturing method, and the magnet is brought into contact with the inner surface of a large diameter cylindrical magnet (3). The surface becomes the same pole as the pole of the large diameter magnet, and the inner circumferential surface in contact with the outer circumferential surface of the small diameter cylindrical magnet 4 becomes the same pole as the pole of the small diameter magnet to obtain a magnetized magnet such that the NS magnetic lines are deflected, or In a similar manner, as shown in Fig. 3, the distance of the disc magnets 3a, 4a, and 5a in which the magnetic lines of the north and south poles 1a, 2a are formed in the vertical direction is made. (6a) (7a) to be fixed in place, the center of the disc magnet (3a) (4a) and (5a) of the center (9) (9a) and (9b) of the stagger respectively mold (9 ') (9a') By arranging in (9b ') and filling the iron iron powder for magnets in the gaps 6a and 7a, and then compressing them to produce magnets by a conventional magnet manufacturing method, the magnets are arranged in the disc-shaped magnets 3a. Disc-shaped magnets magnetized so that NS magnetic lines are deflected are made to be the same poles as the poles of the surfaces in contact with (4a) and (5a).
이상과 같은 자석제조방법으로 도5에서 참조되는 바와같이 원통형 자석의 상부가 모두 N극이나 S극 중 어느 하나의 극만으로 자화되고 자석 하부는 모두 상기 상부극과 반대극인 S극이나 N극중 어느 하나의 극만으로 자화되면서 상기 상하의 N극이나 S극 각각은 자력선이 편향되게 자화되도록 자석을 제조하거나, 상,하부에 N,S극이 형성된 원통형 자석을 원통의 높이 방향으로 다수개 분할한 것과같은 분할편들(Se)을 다수개 접합시켜서 원통형 자석을 만들 수도 있다.As shown in FIG. 5, the upper part of the cylindrical magnet is magnetized with only one pole of the N pole or the S pole, and the lower part of the magnet is any one of the S pole or the N pole which is opposite to the upper pole. Each of the upper and lower N poles or S poles is magnetized to produce a magnet such that the magnetic lines of force are deflected while the magnets are magnetized only at the poles of the poles. A plurality of pieces Se may be joined to form a cylindrical magnet.
이상과 같이 본 발명 방법에 따라 제조되는 자력선이 편향되게 자화된 자석을 이용하여 동력모터를 제작하고져 할때는, 도2에 도시된 바와같이 원주 전체에 걸쳐 남극(1)과 북극(2)이 반복되게 자화된 대직경 원통형 자석(3)으로된 원통형고정자(F)내에, 원통의 내외면으로도 극이 서로 상반되고 원주방향으로 인접한 극과도 각각 극이 서로 상반되면서 N-S자력선이 편향되게 형성된 다수개의 자석으로 구성되는 소직경 원통형 자석으로된 회전자(R)를, 상기 원통형 고정자(F)와 일정간격을 유지하도록 중심축(6)을 중심으로 장착하여 자력에 의한 동력장치를 구성하거나, 도4(a) 종단면도에서 참조되는 바와같이, V자형으로 자력선을 형성하도록 두개의 원판형 자석(Fa1+Fa2)을 맞물리게한 다수개의 원판형 고정자(Fa)를 축(10)을 중심으로 일정간격(11)을 두고 간헐적으로 고정시킨 다음 상기 고정자의 자력선과 반대방향의 V자형 자력선을 형성하도록 두개의 원판형자석(Ra1+ Ra2)을 맞물리게한 원판형 회전자(Ra)를 상기 간격(11)사이에 상기 고정자(Fa)와 동일 축상에 장착하여 상기 원판형 회전자(Ra)가 원판형 고정자(Fa)와 동일극의 경사진(편향된)자력선에 의하여 배타적으로 회전되게한 자력에 의한 동력장치를 구성하거나, 도5에서와 같이 N,S극이 상하로 형성되면서 자력선이 경사(편향)지게 자화된 대.소 직경의 원통형 자석으로된 원통형 고정자(FB)와 원통형 회전자(RB)를 상기와 같은 동일한 방법으로 대형 고정자(FB)내에 소형회전자(RB)를 중심축(6')으로 고정 장착하여 자력에 의한 동력장치를 구성하거나, 또는 상기 상하가 N,S극으로된 대.소직경의 원통형 자석인 고정자와 회전자에 의해서 구동되는 동력장치에서 대소직경의 원통형자석들을 높이 방향으로 다수개로 분할한 것과 같은 분할편(Se)(Se')을 결합하되 대직경의 원통형(FC)고정자내에 소직경의 원통형 회전자(RC)를 중심축(6")에 고정하여 자력에 의한 동력장치를 구성할 수도 있다.As described above, when a power motor is manufactured using a magnetized magnet in which a magnetic force line manufactured according to the present invention is deflected, the south pole 1 and the north pole 2 are repeated throughout the circumference as shown in FIG. 2. In the cylindrical stator (F) made of a magnetized large diameter cylindrical magnet (3), the poles are opposite to each other in the inner and outer surfaces of the cylinder and the poles adjacent to each other in the circumferential direction, respectively, so that the NS magnetic lines are deflected. A rotor R made of a small diameter cylindrical magnet composed of magnets is mounted about the central shaft 6 so as to maintain a constant distance from the cylindrical stator F, thereby configuring a power unit by magnetic force, or FIG. 4. (a) As referred to in the longitudinal section, a plurality of disc stators Fa interlocking two disc magnets Fa 1 + Fa 2 to form a magnetic field line in a V shape with respect to the axis 10. At intervals (11) Wherein between immobilized by heoljeok then the two disk-like magnet (Ra 1 + Ra 2) to form a magnetic line of force and the V-shaped lines of magnetic force in the opposite direction of the stator into engagement han disk-shaped rotor the gap 11, the (Ra) It is constructed on the same axis as the stator Fa and constitutes a power unit by a magnetic force that causes the disc-shaped rotor Ra to be exclusively rotated by the inclined (deflected) magnetic lines of the same pole as the disc-shaped stator Fa. 5, the cylindrical stator (FB) and the cylindrical rotor (RB) made of large and small diameter cylindrical magnets in which the magnetic force lines are inclined (deflected) while the N and S poles are formed up and down as shown in FIG. The small rotor RB is fixedly mounted to the central shaft 6 'in the large stator FB to form a power unit by magnetic force, or the large and small diameter cylinder whose upper and lower sides are N and S poles. Power field driven by a stator and rotor, which are magnets To combine the large-diameter cylindrical magnets (Se) (Se '), which are divided into a plurality of cylindrical magnets in the height direction, the central axis of the cylindrical rotor (RC) in the large-diameter cylindrical (FC) stator It can also be fixed to (6 ") to form a magnetic power unit.
이상과 같이 본 발명 자력에 의한 동력장치는 편향되게 자력선이 자화된 자석을 좌우, 상하 및 수평방향등으로 동일한 N 또는 S극이 배타적으로 맞물리도록 배치하였으므로 자석 자체의 반발력에 의해 동력이 발생함은 물론이고 고정자와 회전자의 동일극이 맞나는 지점에서 발생되는 노즐형태의 편향된(경사진)자력선에 의해 원심력이 발생하게 되어 상기 자석원래의 자력과 원심력에 의하여 가속도가 추가되므로 수직방향으로만 자화된 자력에 의한 동력보다는 훨씬 많은 양의 에너지(동력)을 발생할 수 있게 되는 것이다.As described above, in the power device according to the present invention, since the magnets in which the magnetic force lines are magnetized so as to be deflected are arranged such that the same N or S poles are exclusively engaged in the left, right, up, down and horizontal directions, the power is generated by the repulsive force of the magnet itself. Of course, the centrifugal force is generated by the deflected (inclined) magnetic lines of the nozzle type generated at the same pole of the stator and the rotor, and the acceleration is added by the magnetic force and the centrifugal force of the magnet. It is possible to generate much more energy (power) than the power generated by magnetic force.
본 발명의 편향된 자력선을가진 자석을 이용한 자석 모터와 같은 동력장치는 편향된 자력선의 원심력에 의한 가속도에 의해 적은힘으로 많은양의 동력을 얻을 수 있는 효과가 있음은 물론이고 자력이 완전 소진되거나 전자력을 단절하지 않는한 거의 무한대로 동력을 발생시킬 수 있는 효과가 있다.The power unit such as a magnet motor using a magnet having a deflected magnetic force line of the present invention has the effect of obtaining a large amount of power with a small force by the acceleration by the centrifugal force of the deflected magnetic force line. Unless disconnected, there is an effect that can generate power to almost infinity.
Claims (8)
Applications Claiming Priority (3)
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KR1019990011933 | 1999-04-06 | ||
KR1019990011933A KR19990068325A (en) | 1999-04-06 | 1999-04-06 | Process for preparation of magnet having an inclined magnetic force line and magnetic motor utilizing it |
PCT/KR2000/000260 WO2000060618A1 (en) | 1999-04-06 | 2000-03-24 | A method for manufacturing magnets having inclined magnetic force lines and power plants using it |
Publications (2)
Publication Number | Publication Date |
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KR20010086147A true KR20010086147A (en) | 2001-09-08 |
KR100383576B1 KR100383576B1 (en) | 2003-05-16 |
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KR1019990011933A KR19990068325A (en) | 1999-04-06 | 1999-04-06 | Process for preparation of magnet having an inclined magnetic force line and magnetic motor utilizing it |
KR10-2001-7008952A KR100383576B1 (en) | 1999-04-06 | 2000-03-24 | Process for preparation of magnet having an inclined magnetic force line and power plants utilizing them |
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KR1019990011933A KR19990068325A (en) | 1999-04-06 | 1999-04-06 | Process for preparation of magnet having an inclined magnetic force line and magnetic motor utilizing it |
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KR (2) | KR19990068325A (en) |
AU (1) | AU3462000A (en) |
WO (1) | WO2000060618A1 (en) |
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US6552090B1 (en) * | 1997-09-15 | 2003-04-22 | 3M Innovative Properties Company | Perfluoroalkyl haloalkyl ethers and compositions and applications thereof |
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1999
- 1999-04-06 KR KR1019990011933A patent/KR19990068325A/en not_active Application Discontinuation
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2000
- 2000-03-24 KR KR10-2001-7008952A patent/KR100383576B1/en active IP Right Grant
- 2000-03-24 WO PCT/KR2000/000260 patent/WO2000060618A1/en not_active Application Discontinuation
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WO2000060618A1 (en) | 2000-10-12 |
AU3462000A (en) | 2000-10-23 |
KR100383576B1 (en) | 2003-05-16 |
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