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JP7768026B2 - Iron core structure and static winding equipment - Google Patents
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JP7768026B2 - Iron core structure and static winding equipment - Google Patents

Iron core structure and static winding equipment

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Publication number
JP7768026B2
JP7768026B2 JP2022072906A JP2022072906A JP7768026B2 JP 7768026 B2 JP7768026 B2 JP 7768026B2 JP 2022072906 A JP2022072906 A JP 2022072906A JP 2022072906 A JP2022072906 A JP 2022072906A JP 7768026 B2 JP7768026 B2 JP 7768026B2
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iron core
leg portion
core
depth direction
core structure
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JP2023162535A (en
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幹弥 石橋
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Meidensha Corp
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Meidensha Corp
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  • Soft Magnetic Materials (AREA)

Description

本発明は、変圧器、リアクトル等の静止巻線機器の技術に係り、フェライトなどの複数のブロックコアを積層した鉄心を有する変圧器及びリアクトルに関する。 The present invention relates to technology for static winding devices such as transformers and reactors, and relates to transformers and reactors having an iron core made of multiple stacked block cores such as ferrite.

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 generally has a structure in which plate-shaped magnetic bodies, such as ferrite cores, are arranged in a frame-like configuration and stacked in one direction (Patent Documents 1 and 2).

特願昭58-12915号公報Patent Application No. 12915/1983 特開平5-326289号公報Japanese Patent Application Publication No. 5-326289

図4に示されたブロックコア10を積層して成る鉄心1は、ブロックコア10間にギャップ13を確保する際に横断面に対してギャップ13の幅を均等に設定される。これにより、図2(a)のようにレグ部11の奥行き方向で前後中央の各磁路の磁気抵抗は均一となる。また、ギャップ13を確保しない場合でも、これらの磁路の磁気抵抗は均一となるので、レグ部11の磁束密度は均一化される。 The iron core 1 shown in Figure 4 is made by stacking block cores 10, and when gaps 13 are secured between the block cores 10, the width of the gaps 13 is set uniformly across the cross section. This ensures uniform magnetic resistance in each magnetic path at the front and rear center in the depth direction of the leg portion 11, as shown in Figure 2(a). Furthermore, even when gaps 13 are not secured, the magnetic resistance of these magnetic paths is uniform, so the magnetic flux density in the leg portion 11 is uniform.

しかしながら、図3(a)のように、空冷において冷却的に不利となるレグ部11の中央付近の温度が高くなり、ホットスポットが生じる。 However, as shown in Figure 3(a), the temperature near the center of the leg portion 11, which is disadvantageous for air cooling, becomes high, resulting in hot spots.

本発明は、以上の事情を鑑み、鉄心のレグ部の冷却に不利な部位の磁束密度を低減して鉄心の最大温度上昇の低減を図ることを課題とする。 In consideration of the above circumstances, the present invention aims to reduce the magnetic flux density in areas of the leg portion of the iron core that are unfavorable for cooling, thereby reducing the maximum temperature rise of the iron core.

そこで、本発明の一態様は、鉄心のレグ部の奥行方向に三つ以上積層されるブロックコアを有し、前記ブロックコア間のギャップは、前記レグ部の奥行方向で長さが異なり、奥行方向中央の前記ブロックコア間のギャップは、奥行方向前後の前記ブロックコア間のギャップよりも長大であることを特徴とする鉄心構造である。 One aspect of the present invention is an iron core structure that has three or more block cores stacked in the depth direction of the leg portion of the iron core, the gaps between the block cores vary in length in the depth direction of the leg portion, and the gap between the block cores in the center in the depth direction is longer than the gaps between the block cores at the front and rear in the depth direction.

本発明の一態様は、上記の鉄心構造を有する静止巻線機器である。 One aspect of the present invention is a static winding device having the above-mentioned core structure.

以上の本発明によれば、鉄心のレグ部の冷却に不利な部位の磁束密度が低減し、鉄心の最大温度上昇を低減できる。 According to the present invention, the magnetic flux density in the leg portion of the core, which is unfavorable for cooling, is reduced, thereby reducing the maximum temperature rise of the core.

(a)本発明の一態様である鉄心の正面図、(b)当該鉄心の上面図、(c)当該鉄心の側面図、(d)当該鉄心のA,C断面図、(e)当該鉄心のB断面図。(a) Front view of an iron core according to one embodiment of the present invention, (b) top view of the iron core, (c) side view of the iron core, (d) cross-sectional views A and C of the iron core, and (e) cross-sectional view B of the iron core. (a)従来の鉄心の磁束密度分布、(b)本発明の鉄心の磁束密度分布。(a) Magnetic flux density distribution of a conventional iron core, (b) Magnetic flux density distribution of an iron core of the present invention. (a)従来の鉄心の温度分布、(b)本発明の鉄心の温度分布。(a) Temperature distribution of a conventional iron core, (b) Temperature distribution of an iron core of the present invention. (a)従来の鉄心の正面図、(b)当該鉄心の上面図、(c)当該鉄心の側面図。1A is a front view of a conventional iron core, FIG. 1B is a top view of the iron core, and FIG. 1C is a side view of the iron 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。 Embodiments of the present invention will be described below with reference to the drawings.

図1に示された本発明の鉄心構造の一態様である鉄心1は、例えば、内鉄形若しくは外鉄形の変圧器、リアクトル等の静止巻線機器に適用される。 The core 1 shown in Figure 1, which is one embodiment of the core structure of the present invention, is applied to static winding devices such as core-type or shell-type transformers and reactors.

鉄心1は、一次巻線,二次巻線等の巻線が券回されるレグ部11と、当該巻線が券回されないヨーク部12と、を有する。 The core 1 has a leg portion 11 around which windings such as the primary winding and secondary winding are wound, and a yoke portion 12 around which the windings are not wound.

鉄心1は、奥行方向に三つ以上積層したブロックコア10から成る。鉄心1のレグ部11のブロックコア10間にはギャップ13が確保される。 The core 1 consists of three or more block cores 10 stacked in the depth direction. Gaps 13 are maintained between the block cores 10 in the leg portion 11 of the core 1.

ギャップ13は、レグ部11の奥行方向で長さが異なるように確保される。特に、図3(a)のホットスポットを生じやすい鉄心1のレグ部11の奥行方向中央にギャップ13が確保される。 The gap 13 is ensured to have different lengths in the depth direction of the leg portion 11. In particular, the gap 13 is ensured in the center of the depth direction of the leg portion 11 of the iron core 1, which is prone to hot spots as shown in Figure 3(a).

すなわち、図1のように、レグ部11の奥行方向中央のギャップ13は奥行方向前後のギャップ13よりも長大に設定される。但し、奥行方向中央と奥行方向前後のギャップ13の長さの差が大きくなり過ぎると、奥行方向前後の磁束密度が高くなり過ぎ、発熱が大きくなることから、磁束密度及び温度の低減効果が得られなくなる。 That is, as shown in Figure 1, the gap 13 at the center of the depth direction of the leg portion 11 is set to be longer than the gaps 13 at the front and rear of the depth direction. However, if the difference in length between the gaps 13 at the center of the depth direction and the front and rear of the depth direction becomes too large, the magnetic flux density at the front and rear of the depth direction becomes too high, resulting in increased heat generation, and the effect of reducing magnetic flux density and temperature cannot be obtained.

以上の鉄心1の構造によれば、レグ部11の奥行方向中央のギャップ13の長さが奥行方向前後のギャップ13の長さよりも大きく設定することで、レグ部11の奥行方向中央のブロックコア10の磁束密度を低減できる。そして、これにより、レグ部11の奥行方向中央のブロックコア10の損失密度も低減できる。また、レグ部11の奥行方向中央のブロックコア10は奥行方向前後のブロックコア10と比較して冷却条件が厳しいが、以上の動作によって最大温度を下げることができる。 With the above-described core 1 structure, the length of the gap 13 at the depth center of the leg portion 11 is set to be longer than the length of the gap 13 at the front and rear ends in the depth direction, thereby reducing the magnetic flux density of the block core 10 at the depth center of the leg portion 11. This also reduces the loss density of the block core 10 at the depth center of the leg portion 11. Furthermore, although the cooling conditions for the block core 10 at the depth center of the leg portion 11 are stricter than those for the block cores 10 at the front and rear ends in the depth direction, the maximum temperature can be reduced by the above-described operation.

図2,3を参照して鉄心1の具体的な作用効果について説明する。 The specific effects of iron core 1 will be explained with reference to Figures 2 and 3.

図2(a)は従来の鉄心1の磁束密度分布、同図(b)は本発明の鉄心1の磁束密度分布を示す。この両者の磁束密度分布の比較から明らかなように、本発明の鉄心1の構造によれば、従来の鉄心1と比べて鉄心1の奥行方向中央のブロックコア10の磁束密度を低減でき、当該中央のブロックコア10の損失密度も低減できることが示された。 Figure 2(a) shows the magnetic flux density distribution of a conventional iron core 1, and Figure 2(b) shows the magnetic flux density distribution of an iron core 1 of the present invention. As is clear from comparing the magnetic flux density distributions of the two, the structure of the iron core 1 of the present invention makes it possible to reduce the magnetic flux density of the block core 10 at the center in the depth direction of the iron core 1 compared to the conventional iron core 1, and it was also shown that the loss density of this central block core 10 can be reduced.

図3(a)は従来の鉄心1の温度分布、同図(b)は本発明の鉄心1の温度分布を示す。この両者の温度分布の比較から明らかなように、本発明の鉄心1の構造によれば、従来の鉄心1に比べて冷却的に不利なレグ部11の中央の温度を低減できることが示された。特に、鉄心1の奥行方向にブロックコア10を三つ以上配置し、レグ部11のヒートスポット付近にギャップ13を確保する場合に温度低減の効果があることが示された。 Figure 3(a) shows the temperature distribution of a conventional core 1, and Figure 3(b) shows the temperature distribution of an iron core 1 of the present invention. As is clear from comparing the two temperature distributions, the structure of the iron core 1 of the present invention can reduce the temperature in the center of the leg portion 11, which is less favorable for cooling than the conventional core 1. In particular, it was shown that there is a temperature reduction effect when three or more block cores 10 are arranged in the depth direction of the core 1 and gaps 13 are secured near the heat spots of the leg portion 11.

1…鉄心、10…ブロックコア、11…レグ部、12…ヨーク部、13…ギャップ 1...Iron core, 10...Block core, 11...Leg section, 12...Yoke section, 13...Gap

Claims (2)

巻線が巻回されるレグ部と、
前記巻線が巻回されないヨーク部と、
を有し、
前記レグ部と前記ヨーク部との間及び当該レグ部のブロックコア間にギャップが確保され、
前記レグ部及び前記ヨーク部のブロックコアは、当該レグ部及び当該ヨーク部の奥行方向に三つ以上積層され、
前記ブロックコア間のギャップは、前記レグ部の奥行方向で長さが異なり、
奥行方向中央の前記ブロックコア間のギャップは、奥行方向前後の前記ブロックコア間のギャップよりも長大であること
を特徴とする鉄心構造。
a leg portion around which the winding is wound;
a yoke portion on which the winding is not wound;
and
Gaps are secured between the leg portion and the yoke portion and between the block cores of the leg portion,
Three or more block cores of the leg portion and the yoke portion are stacked in the depth direction of the leg portion and the yoke portion,
the gap between the block cores has a different length in the depth direction of the leg portion;
An iron core structure characterized in that the gap between the block cores at the center in the depth direction is longer than the gaps between the block cores at the front and rear in the depth direction.
請求項1に記載の鉄心構造を有する静止巻線機器。 A static winding device having the core structure described in claim 1.
JP2022072906A 2022-04-27 2022-04-27 Iron core structure and static winding equipment Active JP7768026B2 (en)

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Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN2569307Y (en) 2002-04-10 2003-08-27 林国良 Silicon steel core construction for transformers or choke coils
JP2006351920A (en) 2005-06-17 2006-12-28 Toyota Motor Corp Reactor
CN201478056U (en) 2009-03-16 2010-05-19 焦海波 Novel transformer magnetic core of high frequency and high power
JP2012146786A (en) 2011-01-11 2012-08-02 Tabuchi Electric Co Ltd Electromagnetic induction device and method of manufacturing the same
JP2017103417A (en) 2015-12-04 2017-06-08 東芝産業機器システム株式会社 Transformer core
CN110945608A (en) 2017-08-18 2020-03-31 通用电器技术有限公司 Electric reactor

Family Cites Families (1)

* 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

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN2569307Y (en) 2002-04-10 2003-08-27 林国良 Silicon steel core construction for transformers or choke coils
JP2006351920A (en) 2005-06-17 2006-12-28 Toyota Motor Corp Reactor
CN201478056U (en) 2009-03-16 2010-05-19 焦海波 Novel transformer magnetic core of high frequency and high power
JP2012146786A (en) 2011-01-11 2012-08-02 Tabuchi Electric Co Ltd Electromagnetic induction device and method of manufacturing the same
JP2017103417A (en) 2015-12-04 2017-06-08 東芝産業機器システム株式会社 Transformer core
CN110945608A (en) 2017-08-18 2020-03-31 通用电器技术有限公司 Electric reactor

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