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JP7632200B2 - Core structure and transformer - Google Patents
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JP7632200B2 - Core structure and transformer - Google Patents

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JP7632200B2
JP7632200B2 JP2021151686A JP2021151686A JP7632200B2 JP 7632200 B2 JP7632200 B2 JP 7632200B2 JP 2021151686 A JP2021151686 A JP 2021151686A JP 2021151686 A JP2021151686 A JP 2021151686A JP 7632200 B2 JP7632200 B2 JP 7632200B2
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core
iron core
ferrite cores
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慎矢 高橋
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Description

本発明は、高周波大容量の変圧器の鉄心、特に、フェライトコアからなる鉄心の構造に関する。 The present invention relates to the structure of the iron core of a high-frequency, large-capacity transformer, in particular, an iron core made of a ferrite core.

大容量の変圧器の鉄心は、一般的に、例えばフェライトコアからなる板状の磁性体を額縁状に配置したものを一方向に積層した構造を成す(特許文献1,2)。 The core of a large-capacity transformer is generally constructed by stacking plate-shaped magnetic bodies, such as ferrite cores, in a frame-like arrangement in one direction (Patent Documents 1 and 2).

実全昭58-12915号公報Jitszen No. 58-12915 Publication 特開平5-326289号公報Japanese Patent Application Publication No. 5-326289

フェライトコアが積層された鉄心は、隣り合うフェライトコアのギャップ(間隙)に起因する磁気抵抗により、特に鉄心の巻線巻回部と非巻線巻回部との接合部における磁束が鉄心の内周側に集中し、また、鉄損も当該内周側に集中して起こる。 In an iron core made of laminated ferrite cores, magnetic resistance caused by the gaps between adjacent ferrite cores causes magnetic flux to concentrate on the inner circumference of the iron core, especially at the joints between the winding and non-winding parts of the iron core, and iron loss also concentrates on this inner circumference.

本発明は、以上の事情を鑑み、フェライトコアからなる鉄心の巻線巻回部と非巻線巻回部との接合部の内周側への磁束集中及び鉄損の緩和を図ることを課題とする。 In view of the above circumstances, the present invention aims to reduce magnetic flux concentration and iron loss on the inner side of the joint between the winding portion and non-winding portion of an iron core made of a ferrite core.

そこで、本発明の一態様は、鉄心構造であって、フェライトコアからなる鉄心の巻線巻回部と非巻線巻回部との接合部は横断面の異なる前記フェライトコアが配される。 Therefore, one aspect of the present invention is an iron core structure in which the ferrite core has a different cross section at the joint between the winding portion and the non-winding portion of the iron core.

本発明の一態様は、前記鉄心構造において、前記横断面は前記鉄心の外周側から内周側にかけて小さくなる。 In one aspect of the present invention, in the core structure, the cross section becomes smaller from the outer periphery to the inner periphery of the core.

本発明の一態様は、上記の鉄心構造を有する変圧器である。 One aspect of the present invention is a transformer having the above-mentioned core structure.

以上の本発明によれば、フェライトコアからなる鉄心の巻線巻回部と非巻線巻回部との接合部の内周側への磁束集中及び鉄損の緩和を図ることができる。 According to the present invention, it is possible to reduce magnetic flux concentration and iron loss on the inner side of the joint between the winding portion and the non-winding portion of the iron core made of a ferrite core.

本発明の実施形態1の変圧器における鉄心構造の横断面図。FIG. 2 is a cross-sectional view of a core structure in the transformer according to the first embodiment of the present invention. 変圧器の鉄心の外層、中層及び内層を模した磁気回路の磁気抵抗の説明図。FIG. 2 is an explanatory diagram of the magnetic resistance of a magnetic circuit simulating the outer, middle and inner layers of a transformer core.

以下に図面を参照しながら本発明の実施形態について説明する。 The following describes an embodiment of the present invention with reference to the drawings.

図1に示された実施形態1の鉄心構造は例えば内鉄形の変圧器1に適用される。 The core structure of embodiment 1 shown in FIG. 1 is applied to, for example, a core-type transformer 1.

変圧器1は、フェライトコア21~25からなる鉄心2と、この鉄心2に巻回される一次巻線3及び二次巻線4を備える。 The transformer 1 has an iron core 2 consisting of ferrite cores 21 to 25, and a primary winding 3 and a secondary winding 4 wound around this iron core 2.

鉄心2は、例えば同図に示したように、直方体状若しくは長板状のフェライトコア21~25が額縁状に配置されたものがさらに一方向に積層されて中空角柱状を成す。 As shown in the figure, the iron core 2 is a hollow rectangular column made up of rectangular or long plate-shaped ferrite cores 21-25 arranged in a frame shape and then stacked in one direction.

一次巻線3,二次巻線4が各々券回される鉄心2のレグ部に相当する巻線巻回部26、並びに、一次巻線3,二次巻線4が券回されない鉄心2のヨーク部に相当する非巻線巻回部27は、同一寸法のフェライトコア21が配置及び一方向に積層されて成る。隣接のフェライトコア21は鉄心製造分野において周知の接着法により接着される。 The winding section 26, which corresponds to the leg section of the iron core 2 around which the primary winding 3 and secondary winding 4 are wound, and the non-winding section 27, which corresponds to the yoke section of the iron core 2 around which the primary winding 3 and secondary winding 4 are not wound, are made by arranging ferrite cores 21 of the same size and stacking them in one direction. Adjacent ferrite cores 21 are bonded by a bonding method well known in the field of iron core manufacturing.

巻線巻回部26と非巻線巻回部27との接合部である鉄心2の角部28は、鉄心2の軸方向と直交する横断面の異なる複数のフェライトコア21~25が配置及び一方向に積層されて成る。前記横断面は鉄心2の外周側から内周側に連れて小さくなる。尚、隣接のフェライトコア21~25も前記周知の接着法により接着される。 The corner 28 of the core 2, which is the joint between the winding portion 26 and the non-winding portion 27, is formed by arranging and stacking in one direction a number of ferrite cores 21-25 with different cross sections perpendicular to the axial direction of the core 2. The cross sections become smaller from the outer periphery to the inner periphery of the core 2. Adjacent ferrite cores 21-25 are also bonded by the well-known bonding method.

図1に例示された三層の鉄心2の場合、接合部29は横断面の形状が略正方形を成す。そして、この接合部29の外層OUT(図2)には、通常寸法の横断面長方形のフェライトコア21及び当該通常寸法の略2/3である横断面長方形のフェライトコア22が配される。さらに、外層OUTよりも内周側の中層CEN(同図)には、フェライトコア21の略1/3若しくは略1/3~4/5の横断面のフェライトコア23,24が配される。そして、中層CENよりも内周側の内層IN(同図)には、フェライトコア21の略1/3若しくは略1/10の横断面のフェライトコア24,25が配される。 In the case of the three-layer core 2 illustrated in FIG. 1, the joint 29 has a substantially square cross section. The outer layer OUT (FIG. 2) of this joint 29 contains a ferrite core 21 with a rectangular cross section of normal dimensions and a ferrite core 22 with a rectangular cross section that is approximately 2/3 of the normal dimensions. Furthermore, the middle layer CEN (same figure) located more inward than the outer layer OUT contains ferrite cores 23 and 24 with a cross section that is approximately 1/3 or approximately 1/3 to 4/5 of the cross section of the ferrite core 21. The inner layer IN (same figure) located more inward than the middle layer CEN contains ferrite cores 24 and 25 with a cross section that is approximately 1/3 or approximately 1/10 of the cross section of the ferrite core 21.

特に、フェライトコア21~25は、鉄心2の内層IN、中層CEN及び外層OUTの磁気抵抗が略均等となるように配置及び積層される。すなわち、図2に例示した三層の鉄心2の内層INの磁気抵抗Rm_IN、中層CENの磁気抵抗Rm_CEN及び外層OUTの磁気抵抗Rm_OUTは、以下の式(1)~式(3)により示される(但し、μ:鉄心2の透磁率、lIN:内層INの磁路の長さ、lCEN:中層CENの磁路の長さ、lOUT:外層OUTの磁路の長さ、S:前記磁路の横断面積、μ0:真空の透磁率、lgap:内層IN,中層CEN,外層OUTにおいて隣接するフェライトコア21~25のギャップの長さ、Sgap:前記ギャップの断面積)。 In particular, the ferrite cores 21 to 25 are arranged and stacked so that the magnetic resistances of the inner layer IN, middle layer CEN, and outer layer OUT of the iron core 2 are approximately uniform. That is, the magnetic resistance Rm_IN of the inner layer IN, the magnetic resistance Rm_CEN of the middle layer CEN, and the magnetic resistance Rm_OUT of the outer layer OUT of the three-layer iron core 2 illustrated in Figure 2 are expressed by the following formulas (1) to (3) (where μ: magnetic permeability of the iron core 2, l IN : length of the magnetic path of the inner layer IN, l CEN : length of the magnetic path of the middle layer CEN, l OUT : length of the magnetic path of the outer layer OUT, S: cross-sectional area of the magnetic path, μ 0 : magnetic permeability of a vacuum, l gap : length of the gap between adjacent ferrite cores 21 to 25 in the inner layer IN, middle layer CEN, and outer layer OUT, S gap : cross-sectional area of the gap).

Figure 0007632200000001
Figure 0007632200000001

Figure 0007632200000002
Figure 0007632200000002

Figure 0007632200000003
Figure 0007632200000003

通常の磁気抵抗Rm_OUT、磁気抵抗Rm_CEN及び磁気抵抗Rm_INは、以下の式(4)により示される。 Normal magnetic resistance Rm_OUT, magnetic resistance Rm_CEN and magnetic resistance Rm_IN are shown by the following equation (4).

Figure 0007632200000004
Figure 0007632200000004

磁気抵抗Rm_OUT、磁気抵抗Rm_CEN及び磁気抵抗Rm_INは、フェライトコア21~25の磁気抵抗よりも、隣接するフェライトコア21~25のギャップの磁気抵抗が大きいので、当該ギャップの長さ及び数の調整により略均等に調整される。特に、磁気抵抗率μ(φ)は磁束φの関数であるので、磁気抵抗Rm_OUT、磁気抵抗Rm_CEN及び磁気抵抗Rm_INは以下の式(5)のように同等となるように有限要素法等の数値解析手法により前記ギャップの長さ及び数が調整される。 Since the magnetic resistance of the gaps between adjacent ferrite cores 21 to 25 is greater than the magnetic resistance of the ferrite cores 21 to 25, the magnetic resistances Rm_OUT, Rm_CEN, and Rm_IN are adjusted to be approximately equal by adjusting the length and number of the gaps. In particular, since the magnetic resistance rate μ(φ) is a function of the magnetic flux φ, the length and number of the gaps are adjusted by a numerical analysis method such as the finite element method so that the magnetic resistances Rm_OUT, Rm_CEN, and Rm_IN are equal as shown in the following formula (5).

Figure 0007632200000005
Figure 0007632200000005

以上のように角部28は、例えば、隣り合うフェライトコア21~25のギャップの長さが鉄心2の外周から内周に近づくに連れて小さくなるように、前記横断面の寸法が異なるフェライトコア21~25は配置及び積層される。これにより、フェライトコア21~25間のギャップの数が鉄心2の外側で少なく内側で多くなり、当該外側及び内側の磁気抵抗が均一となるので、鉄心2の角部28(巻線巻回部26と非巻線巻回部27との接合部)における磁束の集中が緩和される。 As described above, the ferrite cores 21 to 25 with different cross-sectional dimensions are arranged and stacked so that the gap length between adjacent ferrite cores 21 to 25 becomes smaller as the corners 28 approach from the outer periphery to the inner periphery of the iron core 2. As a result, the number of gaps between the ferrite cores 21 to 25 is smaller on the outside of the iron core 2 and larger on the inside, and the magnetic resistance on the outside and inside is uniform, so the concentration of magnetic flux at the corners 28 of the iron core 2 (the joints between the winding portion 26 and the non-winding portion 27) is mitigated.

鉄心2のフェライトコア21~25の大型化は技術的な制約があるが、入手可能なサイズのフェライトコアの配置及び積層により実現が可能である。特に前記ギャップの数の調整による磁気抵抗の均一化により、鉄心2の内周側に磁束が集中し、鉄損が冷却しにくい内側に集中することを回避できる。 There are technical constraints on enlarging the ferrite cores 21 to 25 of the iron core 2, but this can be achieved by arranging and stacking ferrite cores of available sizes. In particular, by equalizing the magnetic resistance by adjusting the number of gaps, it is possible to prevent magnetic flux from concentrating on the inner circumference of the iron core 2, which would otherwise cause iron loss to concentrate on the inside where it is difficult to cool.

尚、以上の実施形態の鉄心構造は内鉄形の変圧器に適用されたものであるが、本発明の鉄心構造は、外鉄形の変圧器にも適用しても当該実施形態と同様の効果が得られることは明らかである。また、鉄心2は三層の鉄心であるが、本発明の鉄心構造は四層以上の鉄心にも適用しても上記実施形態と同様の効果が得られることは明らかである。 The core structure of the above embodiment is applied to a core-type transformer, but it is clear that the same effect as the above embodiment can be obtained by applying the core structure of the present invention to a shell-type transformer as well. Also, while core 2 is a three-layer core, it is clear that the same effect as the above embodiment can be obtained by applying the core structure of the present invention to a core with four or more layers.

1…変圧器
2…鉄心、21~25…フェライトコア、26…巻線巻回部、27…非巻線巻回部、28…角部
3…一次巻線
4…二次巻線
1... transformer 2... iron core, 21 to 25... ferrite core, 26... winding portion, 27... non-winding portion, 28... corner portion 3... primary winding 4... secondary winding

Claims (2)

鉄心の巻線巻回部と非巻線巻回部との接合部が複数のフェライトコアから構成され、
前記接合部の外層から内層にかけて前記フェライトコアのギャップの長さが小さくなることを特徴とする鉄心構造。
The joint between the winding portion and the non-winding portion of the iron core is made of multiple ferrite cores,
An iron core structure, characterized in that the length of the gap of the ferrite core becomes smaller from the outer layer to the inner layer of the joint .
請求項に記載の鉄心構造を有する変圧器。 A transformer having the core structure according to claim 1 .
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Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003309017A (en) 2002-04-16 2003-10-31 Toyota Motor Corp Core and electromagnetic induction device including the core
JP2017204498A (en) 2016-05-09 2017-11-16 東芝産業機器システム株式会社 Wound core

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5812915U (en) * 1981-07-16 1983-01-27 勝山 慎治 Iron core for high frequency large capacity transformer
JPS63174303A (en) * 1987-01-14 1988-07-18 Mitsubishi Electric Corp Iron core for stationary induction apparatus
JPH05326289A (en) * 1992-05-18 1993-12-10 Matsushita Electric Ind Co Ltd Magnetic core, transformer, and magnetic core method

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003309017A (en) 2002-04-16 2003-10-31 Toyota Motor Corp Core and electromagnetic induction device including the core
JP2017204498A (en) 2016-05-09 2017-11-16 東芝産業機器システム株式会社 Wound core

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