WO2013114993A1 - 磁気回路 - Google Patents
磁気回路 Download PDFInfo
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- WO2013114993A1 WO2013114993A1 PCT/JP2013/051104 JP2013051104W WO2013114993A1 WO 2013114993 A1 WO2013114993 A1 WO 2013114993A1 JP 2013051104 W JP2013051104 W JP 2013051104W WO 2013114993 A1 WO2013114993 A1 WO 2013114993A1
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- magnets
- magnetic circuit
- yoke
- magnetic
- magnet
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- 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
Definitions
- This invention relates to a long magnetic circuit.
- Patent Document 1 Japanese Patent Laid-Open No. 10-47651 (see Patent Document 1), a plurality of permanent magnets are arranged at intervals so that the surfaces of the same magnetic poles face each other, and a plurality of magnetic bodies are arranged between the permanent magnets.
- a long magnetic circuit is described in which a yoke is inserted and each permanent magnet and each magnetic yoke are brought into close contact with each other.
- Patent Document 2 discloses a magnetic adsorption member for a pipe provided in a magnetic suspension for a pipe that is attached to a ferromagnetic fixed object to suspend and support the pipe.
- the magnetic field strength of the magnetic circuit is enhanced by adopting a sandwich type magnetic circuit in which both sides of the magnetic pole direction of the permanent magnet are sandwiched between yokes.
- a sandwich type magnetic circuit in which both sides of the magnetic pole direction of the permanent magnet are sandwiched between yokes.
- a long permanent magnet is required, and it is difficult to process the permanent magnet, and there are problems such as being easily broken.
- the present invention has been made to solve the above-described problems, and uses a plurality of short magnets arranged in an array to obtain a long magnetic circuit having a uniform magnetic flux density distribution in the array direction of the array. For the purpose.
- a magnetic circuit according to the present invention includes a plurality of magnets provided in an array and a pair of yokes provided so as to sandwich the plurality of magnets, and the plurality of magnets are respectively predetermined in the array direction of the array.
- the pair of yokes is disposed below the gap, has one magnetic pole on one yoke side of the pair of yokes, and has the other magnetic pole on the other yoke side of the pair of yokes.
- the array includes a plurality of magnets arranged in an array with a predetermined gap or less and a yoke provided on the plurality of magnets.
- a uniform magnetic flux density can be obtained in the arrangement direction.
- FIG. Embodiment 1 is a side view showing a magnetic circuit according to the first embodiment of the present invention
- FIG. 2 is a perspective view showing the magnetic circuit according to the first embodiment of the present invention.
- 1 and 2 1 is a magnet body, 1a and 1b are magnets, and 2a and 2b are iron-based metallic yokes.
- the magnet body 1 includes a magnet 1a and a magnet 1b. Magnet 1a and magnet 1b are arranged with their magnetic poles oriented in the direction in which yoke 2a and yoke 2b are located. Further, the magnet 1a and the magnet 1b are arranged with the same magnetic poles directed in the same direction.
- the magnet 1a and the magnet 1b are arranged with the north pole on the side where the yoke 2a is installed and the south pole on the side where the yoke 2b is installed. Moreover, the magnet 1a and the magnet 1b are arrange
- an iron-based metallic yoke 2a is provided across the N pole of the magnet 1a and the N pole of the magnet 1b.
- the magnetic circuit is provided with an iron-based metallic yoke 2b across the S pole of the magnet 1a and the S pole of the magnet 1b.
- the yoke 2a and the yoke 2b are disposed so as to sandwich the magnet 1a and the magnet 1b together.
- the gap 3 between magnets may be a gap or may be filled with a resin such as an adhesive.
- FIG. 3A is a diagram showing a magnetic flux density distribution of the magnetic circuit according to the first embodiment of the present invention.
- the same components as those in FIG. 1 are denoted by the same reference numerals, and description thereof is omitted.
- 5 shows the distribution of the magnetic flux density in the axial direction of the magnetic circuit at a position 2.5 mm away from the magnet surface of the magnetic circuit in the direction perpendicular to the magnetic pole direction and the array arrangement direction (position of the measuring unit 4 shown in FIG. 3B). It is a graph to show.
- the vertical axis represents the magnetic flux density
- the horizontal axis represents the length of the magnetic circuit in the axial direction.
- the broken line shown in FIG. 3A shows the correspondence between the horizontal axis of the graph 5 and the magnetic circuit (that is, the magnetic circuit is located in the permanent magnet range shown in the graph 5).
- Graph 5 shows the distribution of magnetic flux density when the gap 3 between the magnets 1a and 1b is changed from 0 mm to 5 mm. Even if the gap 3 between magnets becomes large, the magnetic flux density around the gap 3 between magnets does not fluctuate greatly. Furthermore, the magnetic flux density around the gap 3 between the magnets hardly changes until the gap 3 between the magnets is 3 mm. A uniform magnetic flux density is obtained over the entire axial length of the magnetic circuit.
- FIG. 4 is a side view of the magnetic circuit obtained by removing the yokes 2a and 2b from the magnetic circuit according to the first embodiment of the present invention. 4, the same components as those in FIG. 1 are denoted by the same reference numerals, and the description thereof is omitted.
- FIG. 5A is a diagram showing a magnetic flux density distribution of the magnetic circuit obtained by removing the yoke from the magnetic circuit according to the first embodiment of the present invention.
- 5A and 5B the same components as those in FIG. 3 are denoted by the same reference numerals, and the description thereof is omitted.
- 51 shows the distribution of the magnetic flux density in the axial direction of the magnetic circuit at a position 2.5 mm away from the magnet surface of the magnetic circuit in the direction of the magnetic pole and in the direction orthogonal to the array direction of the array (position of the measuring unit 4 shown in FIG. 5B). It is a graph to show.
- the vertical axis represents the magnetic flux density
- the horizontal axis represents the longitudinal direction of the magnetic circuit.
- the broken line shown in FIG. 5A indicates the correspondence between the horizontal axis of the graph 51 and the magnetic circuit.
- the graph 51 shows the distribution of magnetic flux density when the gap 3 between the magnets 1a and 1b is changed from 0 mm to 5 mm. As the gap 3 between the magnets increases, the magnetic flux density around the gap 3 between the magnets varies greatly. It can be seen that the magnetic flux density around the gap 3 between the magnets varies greatly as the magnets 1a and 1b are separated.
- the iron-based metallic yokes 2a and 2b are extended over the magnet 1a and the magnet 1b without contacting the magnet 1a and the magnet 1b.
- produces between the magnet 1a and the magnet 1b as shown in FIG. 5 can be suppressed as shown in FIG. As a result, a uniform magnetic flux density can be obtained over the axial direction.
- Embodiment 1 of the present invention the case where two magnets are arranged in an array in the axial direction has been described. However, as shown in FIG. 6, three or more magnets are arranged in an array in the axial direction. A yoke may be provided over all the arranged magnets. The same effect as the above magnetic circuit can be obtained.
- FIG. Embodiment 2 of the present invention will be described with reference to the drawings.
- FIG. 7 is a perspective view of a magnetic circuit according to Embodiment 2 of the present invention.
- the same components as those in FIG. 2 are denoted by the same reference numerals, and the description thereof is omitted.
- the yokes 2a and 2b protrude from the planes (A (a) surface and A (b) surface) surrounded by the axial direction and the magnetic pole direction of each of the magnets 1a and 1b. It has become a shape.
- Magnetic field lines generated from the magnets 1a and 1b are collected by the yokes 2a and 2b through contact surfaces between the magnets 1a and 1b and the yokes 2a and 2b.
- the collected magnetic field lines draw a loop from the N pole at the tip of the protruding portion of the yoke 2a toward the S pole at the tip of the protruding portion of the yoke 2b.
- Protruding the yokes 2a and 2b from the magnets 1a and 1b has an effect of concentrating the magnetic flux on the yokes 2a and 2b and increasing the magnetic flux density.
- FIG. Embodiment 3 of the present invention will be described with reference to the drawings.
- FIG. 8 is a side view showing a magnetic circuit according to the third embodiment of the present invention.
- FIG. 9 is a perspective view showing a magnetic circuit according to Embodiment 3 of the present invention.
- the magnetic circuit according to Embodiment 3 of the present invention is a magnetic circuit in which an iron-based metallic yoke 2c is provided only on one magnetic pole side (for example, the N pole side).
- an iron-based metallic yoke 2c is provided only on one magnetic pole side (for example, the N pole side).
- Other configurations are the same as those of the magnetic circuit of the first embodiment.
- the yoke 2c is provided on the N pole side, but the yoke 2c may be provided on the S pole side instead of the N pole side.
- a graph 6 shown in FIG. 10A is a graph showing the distribution of magnetic flux density at a position 2 mm away from the magnet surface on the N pole side with the yoke 2c interposed therebetween (that is, the place where the measurement unit 4 shown in FIGS. 10A and 10B is located). It is.
- the broken line shown to FIG. 10A has shown the correspondence of the horizontal axis of the graph 6, and a magnetic circuit.
- the graph 6 shows the result of measurement by changing the gap 3 between the magnets from 0 mm to 5 mm in units of 1 mm.
- the vertical axis represents the magnetic flux density
- the horizontal axis represents the length of the magnetic circuit in the axial direction.
- the graph 61 shown in FIG. 11A is a result of measuring the magnetic flux density under the same conditions as the graph 6 shown in FIG. 10A (that is, the result of measuring the magnetic flux density at the location where the measuring unit 4 shown in FIGS. 11A and 11B is located). Is).
- the broken line shown to FIG. 11A has shown the correspondence of the horizontal axis of the graph 61, and a magnetic circuit.
- the graph 61 shows the measurement result obtained by changing the gap 3 between the magnets in units of 1 mm from 0 mm to 5 mm.
- the magnetic circuit of the third embodiment of the present invention even when the iron-based metallic yoke 2c is provided only on one magnetic pole side, it is the same as the magnetic circuit of the first embodiment. In addition, a uniform magnetic flux density can be obtained in the axial direction.
- the number of magnets to be arranged is not limited to two.
- the number of magnets to be arranged is not limited to two.
- FIG. Embodiment 4 of the present invention will be described with reference to the drawings.
- FIG. 13 is a side view showing a magnetic circuit according to Embodiment 4 of the present invention.
- FIG. 14 is a perspective view showing a magnetic circuit according to Embodiment 4 of the present invention.
- an iron-based metallic metal plate 9 is provided.
- the metal plate 9 is arranged in parallel with the arrangement direction of the magnets 1a and 1b (array arrangement direction). Further, the metal plate 9 is disposed at a position separated by a distance d from the outer surface of the yoke 2b so that the object 10 is positioned between the yoke 2b and the metal plate 9.
- the object 10 is an object to which the magnetic circuit has an influence of magnetism.
- the width w2 of the yoke 2a and the yoke 2b is shorter than the width w1 of the magnet 1a and the magnet 1b.
- Other configurations are the same as those of the magnetic circuit of the first embodiment.
- the metal plate 9 is provided on the S pole side, but the metal plate 9 may be provided on the N pole side instead of the S pole side. Further, it is possible to adopt a configuration in which the metal plate 9 is provided on both the N pole side and the S pole side.
- Graph 7 shown in FIG. 15A shows the magnetic flux density distribution at a position 2.5 mm away from the magnet surface on the S pole side with yoke 2b interposed therebetween (that is, where measurement unit 4 shown in FIGS. 15A and 15B is located). It is a graph to show.
- the broken line shown in FIG. 15A indicates the correspondence between the horizontal axis of the graph 7 and the magnetic circuit.
- the graph 7 shows the results of measurement with the gap 3 between the magnets changed from 0 mm to 5 mm in units of 1 mm.
- the vertical axis represents the magnetic flux density
- the horizontal axis represents the length of the magnetic circuit in the axial direction. It can be seen that the magnetic flux density around the gap 3 between magnets does not change greatly even if the gap 3 between magnets becomes large.
- a graph 71 shown in FIG. 16A is a result of measuring the magnetic flux density under the same conditions as the graph 7 shown in FIG. 15A (that is, a graph showing a result of measuring the magnetic flux density at the place where the measuring unit 4 shown in FIG. 16A is located). Is). 16A indicates the correspondence between the horizontal axis of the graph 71 and the magnetic circuit. Similarly to the graph 7, the graph 71 shows the measurement result obtained by changing the gap 3 between magnets from 0 mm to 5 mm in units of 1 mm. It can be seen that the magnetic flux density around the gap 3 between the magnets greatly changes as the gap 3 between the magnets increases. Thus, when the yoke 2a and the yoke 2b are not provided, it can be seen that the uniformity of the magnetic flux density around the gap 3 between magnets is not maintained.
- FIG. 17A, FIG. 17B, FIG. 18A, and FIG. 18B A measurement result is demonstrated using FIG. 17A, FIG. 17B, FIG. 18A, and FIG. 18B.
- FIG. 17A shows the result of measuring the magnetic flux density using the same configuration as the magnetic circuit shown in FIG. 15A.
- Graph 8 shown in FIG. 17A is a graph showing the distribution of magnetic flux density at a position 2.5 mm away from the sides of magnet 1a and magnet 1b (that is, where measurement unit 4 shown in FIGS. 17A and 17B is located).
- the broken line shown in FIG. 17A indicates the correspondence between the horizontal axis of the graph 8 and the magnetic circuit.
- the graph 8 shows the result of measurement with the gap 3 between the magnets changed from 0 mm to 5 mm in units of 1 mm. It can be seen that the magnetic flux density around the gap 3 between magnets does not change greatly even if the gap 3 between magnets becomes large.
- FIG. 18A shows the result of measurement using the same configuration as the magnetic circuit shown in FIG. 16A (that is, the magnetic circuit obtained by removing the yoke 2a and the yoke 2b from the magnetic circuit shown in FIG. 17A) and changing only the position of the measuring unit 4.
- FIG. A graph 81 shown in FIG. 18A is a graph showing a result of measuring the magnetic flux density of the magnetic circuit under the same conditions as the graph 8 shown in FIG. 17A (that is, at the place where the measuring unit 4 shown in FIGS. 18A and 18B is located). It is a graph which shows the result of having measured magnetic flux density).
- 18A indicates the correspondence between the horizontal axis of the graph 81 and the magnetic circuit.
- the result of measuring the gap 3 between the magnets in units of 1 mm from 0 mm to 5 mm is shown as in the graph 8.
- the magnetic flux density around the gap 3 between magnets greatly changes as the gap 3 between magnets increases.
- a uniform magnetic flux density can be obtained in the axial direction.
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- Electromagnetism (AREA)
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Abstract
Description
この発明の実施の形態1について図を用いて説明する。図1は、この発明の実施の形態1の磁気回路を示す側面図であり、図2は、この発明の実施の形態1の磁気回路を示す斜視図である。図1及び図2において、1は磁石体、1a、1bは磁石、2a、2bは鉄系金属性のヨークである。磁石体1は、磁石1aと磁石1bとから構成される。磁石1aと磁石1bは、ヨーク2aおよびヨーク2bが位置する方向に磁極を向け配置されている。また、磁石1aと磁石1bは、同じ方向に同じ磁極を向け配置されている。例えば、磁石1aと磁石1bは、ヨーク2aが設置された側にN極、ヨーク2bが設置された側にS極を向け配置されている。また、磁石1aと磁石1bは、軸方向にアレイ状に配置されている。磁石1aと磁石1bは例えば2mmの磁石間ギャップ3をもって配置されている。磁気回路には、磁石1aのN極と磁石1bのN極とに亘って鉄系金属性のヨーク2aが設けられている。また、磁気回路には、磁石1aのS極と磁石1bのS極とに亘って鉄系金属性のヨーク2bが設けられている。ヨーク2aとヨーク2bは、磁石1aおよび磁石1bを一体に挟むように配置されている。なお、磁石間ギャップ3は、空隙であってもよく、接着剤等の樹脂が充填されていても良い。
この発明の実施の形態2について図を用いて説明する。図7は、この発明の実施の形態2における磁気回路の斜視図である。図7において、図2と同一の構成要素には同一符号を付し、その説明を省略する。
この発明の実施の形態3について、図面を参照しながら説明する。図8は、この発明の実施の形態3の磁気回路を示す側面図である。また、図9はこの発明の実施の形態3の磁気回路を示す斜視図である。
この発明の実施の形態4について、図面を参照しながら説明する。図13は、この発明の実施の形態4の磁気回路を示す側面図である。また、図14はこの発明の実施の形態4の磁気回路を示す斜視図である。
Claims (5)
- アレイ状に設けられた複数の磁石と、
前記複数の磁石を挟むように設けられた一対のヨークと、を備え、
前記複数の磁石は、アレイの配列方向にそれぞれ所定の隙間以下で配置され、前記一対のヨークの一方のヨーク側に一方の磁極を有し、前記一対のヨークの他方のヨーク側に他方の磁極を有する磁気回路。 - 前記複数の磁石は、前記アレイの配列方向及び磁極方向で囲まれた平面を有し、該平面に対する側面に前記一対のヨークが設けられ、前記一対のヨークが、前記平面から突出している請求項1に記載の磁気回路。
- 前記複数の磁石は、前記アレイの配列方向に直交する方向の断面が矩形形状である請求項1又は請求項2に記載の磁気回路。
- 前記複数の磁石の配列方向と平行に配置された鉄系金属の金属板を備え、
前記金属板は、前記一対のヨークの一方と前記金属板との間に磁気の影響を与える対象となる物体が位置するよう、前記一対のヨークの一方と離間した位置に配置されている請求項1に記載の磁気回路。 - アレイ状に設けられた複数の磁石と、
前記複数の磁石すべてにわたって接するように設けられたヨークと、を備え、
前記複数の磁石は、アレイの配列方向にそれぞれ所定の隙間以下で配置されており、前記ヨークが位置する方向に一方の磁極を向けており、さらに、すべての磁石が同じ方向に同じ磁極を向けている磁気回路。
Priority Applications (7)
Application Number | Priority Date | Filing Date | Title |
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CN201380007289.3A CN104094368A (zh) | 2012-01-30 | 2013-01-21 | 磁路 |
EP13744110.1A EP2816573B1 (en) | 2012-01-30 | 2013-01-21 | Magnetic circuit |
JP2013556319A JP5951647B2 (ja) | 2012-01-30 | 2013-01-21 | 磁気回路 |
KR1020147019004A KR20140109427A (ko) | 2012-01-30 | 2013-01-21 | 자기회로 |
US14/369,772 US9691533B2 (en) | 2012-01-30 | 2013-01-21 | Magnetic circuit |
RU2014135402A RU2014135402A (ru) | 2012-01-30 | 2013-01-21 | Магнитная цепь |
US15/599,738 US10008315B2 (en) | 2012-01-30 | 2017-05-19 | Magnetic circuit |
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JP2012016847 | 2012-01-30 | ||
JP2012-016847 | 2012-01-30 |
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US14/369,772 A-371-Of-International US9691533B2 (en) | 2012-01-30 | 2013-01-21 | Magnetic circuit |
US15/599,738 Division US10008315B2 (en) | 2012-01-30 | 2017-05-19 | Magnetic circuit |
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WO2013114993A1 true WO2013114993A1 (ja) | 2013-08-08 |
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PCT/JP2013/051104 WO2013114993A1 (ja) | 2012-01-30 | 2013-01-21 | 磁気回路 |
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US (2) | US9691533B2 (ja) |
EP (1) | EP2816573B1 (ja) |
JP (1) | JP5951647B2 (ja) |
KR (1) | KR20140109427A (ja) |
CN (1) | CN104094368A (ja) |
RU (1) | RU2014135402A (ja) |
WO (1) | WO2013114993A1 (ja) |
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JP2016125861A (ja) * | 2014-12-26 | 2016-07-11 | セイコーNpc株式会社 | 磁気ラインセンサ |
WO2016125634A1 (ja) * | 2015-02-02 | 2016-08-11 | 三菱電機株式会社 | 磁気センサ装置 |
JP2019175902A (ja) * | 2018-03-27 | 2019-10-10 | 太陽誘電株式会社 | チップ部品の整列方法及び磁石 |
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US9870861B2 (en) * | 2015-09-21 | 2018-01-16 | Apple Inc. | Multiple step shifted-magnetizing method to improve performance of multi-pole array magnet |
US11004586B2 (en) * | 2017-09-15 | 2021-05-11 | Siemens Gamesa Renewable Energy A/S | Permanent magnet for a permanent magnet machine |
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JP7116470B2 (ja) | 2018-03-27 | 2022-08-10 | 太陽誘電株式会社 | チップ部品の整列方法 |
Also Published As
Publication number | Publication date |
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CN104094368A (zh) | 2014-10-08 |
EP2816573A4 (en) | 2015-12-02 |
RU2014135402A (ru) | 2016-03-27 |
US10008315B2 (en) | 2018-06-26 |
EP2816573A1 (en) | 2014-12-24 |
US20140354385A1 (en) | 2014-12-04 |
EP2816573B1 (en) | 2020-08-26 |
JPWO2013114993A1 (ja) | 2015-05-11 |
KR20140109427A (ko) | 2014-09-15 |
US9691533B2 (en) | 2017-06-27 |
US20170256347A1 (en) | 2017-09-07 |
JP5951647B2 (ja) | 2016-07-13 |
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