JPH03141623A - Electromagnetic device - Google Patents

Electromagnetic device

Info

Publication number
JPH03141623A
JPH03141623A JP28148089A JP28148089A JPH03141623A JP H03141623 A JPH03141623 A JP H03141623A JP 28148089 A JP28148089 A JP 28148089A JP 28148089 A JP28148089 A JP 28148089A JP H03141623 A JPH03141623 A JP H03141623A
Authority
JP
Japan
Prior art keywords
core
shaped
yoke core
electromagnetic device
cores
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.)
Pending
Application number
JP28148089A
Other languages
Japanese (ja)
Inventor
Hidenori Kakehashi
英典 掛橋
Tomio Otoshi
大利 富夫
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP28148089A priority Critical patent/JPH03141623A/en
Publication of JPH03141623A publication Critical patent/JPH03141623A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To miniaturize and lighten it while maintaining high performance by providing bar-shaped exciting cores between the flanges of a yoke core whose section is H-shaped, and coiling the windings around exciting cores. CONSTITUTION:A yoke core 10 whose section is H-shaped and a pair of bar- shaped exciting cores 11 and 12 are both made of Mn-Zn ferrite. For the exciting cores 11 and 12, gaps 15 and 16 are made at both sides between itself and the flanges 13 and 14 of the yoke core 10. Furthermore, windings 17 and 18 are wound, through bobbins, around each exciting core 11 and 12, and currents are applied so that the magnetism may be reduced at the foot 9 of the yoke core 10. This way, an electromagnetic device, where bellow magnetic fluxes do not interfere with each other, can be constituted, and it can be miniaturized and lightened, with high performance maintained.

Description

【発明の詳細な説明】 〔産業上の利用分野] この発明は、スイッチング電源やインバータ点灯装置な
どのチョークやトランス等に用いられる電磁装置に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an electromagnetic device used for chokes, transformers, etc. in switching power supplies, inverter lighting devices, and the like.

〔従来の技術〕[Conventional technology]

近年、電子機器の小型、軽量化の要求に伴い、使用され
る電子部品においても、コンパクトで高品質のものが必
要となってきた。スイッチング電源やインバータ点灯装
置の分野でも同様で、特に主部品であるチョークやトラ
ンスへの要求が強い。
In recent years, with the demand for smaller and lighter electronic devices, there has been a need for compact and high quality electronic components. The same is true in the field of switching power supplies and inverter lighting devices, where there are particularly strong demands on the main components, chokes and transformers.

これらの部品は、通常複数個のインダクタンス素子が使
用されているが、これらを一体止して小型軽量化したい
という強いニーズがあった。
These parts usually use a plurality of inductance elements, but there has been a strong need to integrate them into one piece to make them smaller and lighter.

そこで、第11図に示すように、共にMn−Znフェラ
イト材料にて形成されたE型コア70とI型コア71を
組み合わせ、E型コア70の両側脚部72.73に巻線
74.75を巻回してなる2個のインダククン・ス素子
を一体化したli詰装置ある。各巻線74.75には、
誘起された磁束(図中矢印が磁束の流れを示す)がE型
コア70の中央脚部76で減磁性となるように通電され
る。
Therefore, as shown in FIG. 11, an E-type core 70 and an I-type core 71, both made of Mn-Zn ferrite material, are combined, and windings 74.75 are connected to both leg portions 72.73 of the E-type core 70. There is a lithium-ion packing device that integrates two inductance elements made by winding a. Each winding 74.75 has
Electricity is applied so that the induced magnetic flux (arrows in the figure indicate the flow of magnetic flux) becomes demagnetized at the central leg 76 of the E-shaped core 70.

このようにすると、中央脚部76の磁束密度が低減し、
中央脚部76の断面積を小さくすることができる。
In this way, the magnetic flux density of the central leg 76 is reduced,
The cross-sectional area of the central leg portion 76 can be reduced.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

第11図に示した電磁装置では、蓄積エネルギーが小さ
いという問題があった。そこで、第12図に示すように
、E型コア70とI型コア71の間にギャンプ77を形
成して蓄積エネルギーを大きくした電iff装置がある
。しかし、このような電磁装置では、ギヤ2177部分
の磁気抵抗が大きく、一方の側脚部72に流れる磁束の
一部が、他方の側脚部73に流れて、相互に干渉すると
いう問題があった。
The electromagnetic device shown in FIG. 11 has a problem in that the stored energy is small. Therefore, as shown in FIG. 12, there is an electric IF device in which a gap 77 is formed between an E-type core 70 and an I-type core 71 to increase the stored energy. However, in such an electromagnetic device, there is a problem that the magnetic resistance of the gear 2177 portion is large, and a part of the magnetic flux flowing to one side leg 72 flows to the other side leg 73, causing mutual interference. Ta.

そこで、第13図に示すように、E型コア78の側脚部
79.80のみにギヤノブ82を設け、中央脚部81と
I型コア71とは接合して、相互干渉を防止した電磁装
置がある。しかし、このような電磁装置では、十分な蓄
積エネルギーを得るため、ギヤツブ82が大きくなり過
ぎ、ギヤ、アブ82部分でのフリンジング磁束が巻線7
4.75と錯交し、銅損が著しく増加し、温度上昇も大
きくなるという新たな問題が発生してしまう。しかも、
中央脚部81と■型コア71の接合部には、微小ではあ
るがギャップが存在し、相互干渉の問題もあった。
Therefore, as shown in FIG. 13, a gear knob 82 is provided only on the side legs 79 and 80 of the E-shaped core 78, and the central leg 81 and the I-shaped core 71 are joined to prevent mutual interference in the electromagnetic device. There is. However, in such an electromagnetic device, in order to obtain sufficient stored energy, the gear knob 82 becomes too large, and the fringing magnetic flux at the gear and knob 82 portions is caused by the winding 7.
4.75, a new problem arises in that the copper loss increases significantly and the temperature rise also increases. Moreover,
There was a gap, although small, at the joint between the central leg portion 81 and the ■-shaped core 71, and there was also a problem of mutual interference.

以上のように、従来の電磁装置〃では、高い性能を維持
しながら小型、軽量化を図ることは困難であった。
As described above, it has been difficult to reduce the size and weight of conventional electromagnetic devices while maintaining high performance.

したがって、この発明の目的は、磁束どうしが相互干渉
しない電磁装置を提供するこごである。
Therefore, an object of the present invention is to provide an electromagnetic device in which magnetic fluxes do not interfere with each other.

[課題を解決するための手段] この発明のTi1ft装置は、断面H形のヨークコアと
、このヨークコアの鍔間に設けた複数の棒状の励磁コア
と、この励磁コアに巻回した巻線とを備えたものである
[Means for Solving the Problems] The Ti1ft device of the present invention includes a yoke core with an H-shaped cross section, a plurality of rod-shaped excitation cores provided between the flanges of this yoke core, and a winding wound around this excitation core. It is prepared.

〔作 用〕[For production]

この発明の電磁装置によると、断面II形のヨークコア
の鍔間に、複数の励磁コアを設けたものであり、ヨーク
コアは断面H形で脚部は鍔と一体であって磁束が相互干
渉しない。
According to the electromagnetic device of the present invention, a plurality of excitation cores are provided between the flanges of a yoke core with a II-shaped cross section.The yoke core has an H-shaped cross section and the legs are integral with the flanges, so that magnetic fluxes do not interfere with each other.

〔実施例〕〔Example〕

この発明の第1の実施例を第1図ないし第4図に基づい
て説明する。
A first embodiment of the present invention will be described based on FIGS. 1 to 4.

第3図および第4図は、コアの分解正面図ならびに平面
図を示している。図において、lOは断面H形のヨーク
コア、11.12は棒状の一対の励磁コアであり、共に
M’n−Zn系フェライト(日本フェライト製5B7C
)にて形成されている。
3 and 4 show an exploded front view and a plan view of the core. In the figure, IO is a yoke core with an H-shaped cross section, and 11.12 is a pair of rod-shaped excitation cores, both of which are made of M'n-Zn ferrite (5B7C manufactured by Nippon Ferrite).
).

励磁コア11.12は、第2図に示すように、両端にギ
ャップ15.16を形成してヨークコアlOの鍔13.
14間に設ける。さらに、各励磁コア11 12には、
第1図に示すようにボビン(図示せず)を介して巻線1
7.18を巻回し、ヨークコアlOの脚部19で減磁性
(図中の矢印が磁束の流れを示す)となるように通電す
る。
As shown in FIG. 2, the excitation cores 11.12 are connected to the collars 13.1 of the yoke cores 10 with gaps 15.16 formed at both ends.
Provided between 14. Furthermore, in each excitation core 11 12,
Winding 1 through a bobbin (not shown) as shown in Figure 1.
7.18 is wound and energized so that the leg portion 19 of the yoke core IO becomes demagnetized (arrows in the figure indicate the flow of magnetic flux).

今、仮に、ヨークコアIOならびに励磁コア11゜I2
の断面積を80(mnr〕、巻線17の端子間のインダ
クタンスを11:mH)、巻線18の端子間のインダク
タンスをQ、5(mH)と設定する。
Now, hypothetically, yoke core IO and excitation core 11°I2
The cross-sectional area of the winding 17 is set to 80 (mnr), the inductance between the terminals of the winding 17 is set to 11: mH), and the inductance between the terminals of the winding 18 is set to Q, 5 (mH).

そして、巻線18に電圧を印加し、巻線17のインダク
タンスを測定したところ、インダクタンスの値は変化せ
ず、相互干渉のないことが明らかとなった。さらに、巻
線17.t8へのフリンジング磁束の影響を調べるため
に、同一条件で電圧を印加し、従来のE]型ココア電1
置と比較したところ、約10度、温度上昇が低いことが
判明した。
Then, when a voltage was applied to the winding 18 and the inductance of the winding 17 was measured, it was found that the inductance value did not change and there was no mutual interference. Furthermore, winding 17. In order to investigate the influence of fringing magnetic flux on t8, we applied a voltage under the same conditions and
It was found that the temperature rise was approximately 10 degrees lower than the previous one.

このように構成された電磁装置によると、励磁コア11
 12の両・端にギャップ15.16を形成したので、
蓄積エネルギーが大きくなる。
According to the electromagnetic device configured in this way, the excitation core 11
Since gaps 15 and 16 were formed on both ends of 12,
The stored energy increases.

また、ヨークコアlOは断面1]形で、脚部19と鍔1
3.14とが一体に形成されているので、一方の磁束が
他方の磁路に流れて相互干渉することがない。
In addition, the yoke core lO has a cross section of 1] shape, and has a leg 19 and a collar 1.
3.14 are integrally formed, so that the magnetic flux of one does not flow into the magnetic path of the other and interfere with each other.

また、励磁コア11.12の両端にギャップ1516を
形成したので、各ギャップ15.16の大きさは従来の
片側のみに設けたのに比べ、小さくなり、フリンジング
磁束による巻線17.18の温度上昇が小さい。
In addition, since gaps 1516 are formed at both ends of the excitation core 11.12, the size of each gap 15.16 is smaller compared to the conventional case where it is provided only on one side, and the winding 17.18 due to fringing magnetic flux is Temperature rise is small.

また、励(イ■コア11.12をヨークコア10で覆っ
た磁気遮蔽構造となっており、外部への漏れ磁束がなく
、外部部品間の相互作用やノイズがなく、高密度実装が
できる。
In addition, it has a magnetic shielding structure in which the excitation cores 11 and 12 are covered with the yoke core 10, so there is no magnetic flux leaking to the outside, there is no interaction between external components, there is no noise, and high-density mounting is possible.

また、ヨークコアlOの脚部19には、減!■性の磁束
が流れるため磁束密度が低く、よって脚部19の断面積
を小さくでき、電磁装置の小型化が可能となる。
In addition, the leg portion 19 of the yoke core lO has a reduction! (2) Since the magnetic flux flows, the magnetic flux density is low, so the cross-sectional area of the leg portions 19 can be reduced, and the electromagnetic device can be made smaller.

さらに、ヨークコア10が断面H形で、鍔1314と脚
部19とが一体形成されており、従来のEl型コアに見
られるようなE型コアの中央脚部とI型コアとの付き合
わせの問題がなく、量産性に優れている。
Furthermore, the yoke core 10 has an H-shaped cross section, and the flange 1314 and the leg portion 19 are integrally formed, so that the central leg portion of the E-type core and the I-type core are matched with each other as seen in the conventional El-type core. There are no problems and it is suitable for mass production.

この発明の第2の実施例を、第5図ないし第6図に示す
。この実施例の電+f!装置は、断面H形のコークコア
20の鍔21.22の両端角部にテーパ23.24を形
成し、励磁コア25.26を断面円形の棒状としたもの
である。このように構成された電磁装置においても、第
1の実施例と同様の効果が得られる。
A second embodiment of the invention is shown in FIGS. 5 and 6. Electricity+f! of this example! In the device, tapers 23, 24 are formed at both end corners of the flanges 21, 22 of a coke core 20 with an H-shaped cross section, and the excitation core 25, 26 is shaped like a rod with a circular cross section. Even in the electromagnetic device configured in this way, the same effects as in the first embodiment can be obtained.

この発明の第3の実施例を、第7回および第8図に示す
。この実施例の電磁装置は、断面H形のヨークコア30
の鍔31.32間に、合計4個の励磁コア33.34.
35.36を両端にギャップ37.38を形成して設け
たものである。各励磁コア33〜36には、巻線39,
40.4142を巻回し、ヨークコア30の脚部43で
減磁性(図中矢印が磁束の流れを示す)となるように巻
線39〜42に通電する。
A third embodiment of this invention is shown in FIGS. 7 and 8. The electromagnetic device of this embodiment has a yoke core 30 with an H-shaped cross section.
A total of four excitation cores 33, 34.
35 and 36 with gaps 37 and 38 formed at both ends. Each excitation core 33 to 36 has a winding 39,
40.4142 is wound, and the windings 39 to 42 are energized so that the legs 43 of the yoke core 30 are demagnetized (arrows in the figure indicate the flow of magnetic flux).

このように4個のインダクタンス素子を一体化した電磁
装置においても、第1の実施例と同様の効果が得られる
。なお、励磁コアの数は4個に限らない。
Even in the electromagnetic device in which four inductance elements are integrated in this manner, the same effects as in the first embodiment can be obtained. Note that the number of excitation cores is not limited to four.

この発明の第4の実施例を、第9図および第10図に示
す。この実施例の電(n装置は、両鍔51゜52が円形
の断面H形のヨークコア50と、このヨークコア50の
鍔51.52間に両端にギャップ53.54を形成して
設けた4個の励磁コア55゜56.57.58と、各励
磁コア55〜58に巻回した巻線(図示せず)とからな
るものである。
A fourth embodiment of the invention is shown in FIGS. 9 and 10. The electromagnetic device of this embodiment includes a yoke core 50 having an H-shaped cross section with both flanges 51 and 52 circular, and four cores with gaps 53 and 54 formed at both ends between the flanges 51 and 52 of this yoke core 50. It consists of an excitation core 55 degrees 56, 57, 58, and a winding (not shown) wound around each excitation core 55 to 58.

なお、各巻線には、ヨークコア50の脚部59が減磁性
となるように通電される。
Note that each winding is energized so that the leg portion 59 of the yoke core 50 becomes demagnetized.

このように構成された電磁装置においても、第1の実施
例と同様の効果が得られる。
Even in the electromagnetic device configured in this way, the same effects as in the first embodiment can be obtained.

なお、前記各実施例の場合、励磁コア11.12゜25
.26,33,34,35,36,55,5657.5
8の両端にギャップ15.16.3738.53.64
を設けたが、ギャップを設けずにヨークコア10,20
.30.50に接合したものも、当然本発明に含まれる
In addition, in the case of each of the above embodiments, the excitation core is 11.12°25
.. 26, 33, 34, 35, 36, 55, 5657.5
Gap on both ends of 8 15.16.3738.53.64
However, the yoke cores 10 and 20 are connected without providing a gap.
.. Of course, those joined to 30.50 are also included in the present invention.

〔発明の効果〕・ この発明の電磁装置によると、断面H形のヨークコアの
鍔間に、複数の励磁コアを設けたものであり、ヨークコ
アは断面I]形で脚部は鍔と一体であって磁束が相互干
渉しないという効果が得られる。
[Effects of the Invention]- According to the electromagnetic device of the present invention, a plurality of excitation cores are provided between the flanges of a yoke core with an H-shaped cross section, and the yoke core has an I-shaped cross section and the legs are integral with the flanges. Therefore, the effect that the magnetic fluxes do not interfere with each other can be obtained.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の第1の実施例の断面図、第2図はそ
の部分正面図、第3図はその部分分解正面図、第4図は
その部分分解平面図、第5図はこの発明の部分正面図、
第6図はその部分平面図、第7図はこの発明の第3の実
施例の部分正面図、第8図はその断面図、第9図はこの
発明の第4の実施例の部分斜視図、堕10図はその部分
平面図、第11図は従来例の断面l、第12図は他の従
来例の断面図、第13図はさらに他の従来例の断面図で
ある。 10.20,30.50・・・ヨークコア、11゜12
.25.26,33,34,35,36.5556.5
7.58・・・励磁コア、13,14,2122.31
.32 51.52・・・鍔、17,1839.40.
41.42・・・巻線 第1図 第 7 図 第8 図 第11 図 第 2 図 憾
Fig. 1 is a sectional view of the first embodiment of the invention, Fig. 2 is a partial front view thereof, Fig. 3 is a partially exploded front view thereof, Fig. 4 is a partially exploded plan view thereof, and Fig. 5 is a partial front view thereof. A partial front view of the invention;
6 is a partial plan view thereof, FIG. 7 is a partial front view of the third embodiment of the present invention, FIG. 8 is a sectional view thereof, and FIG. 9 is a partial perspective view of the fourth embodiment of the present invention. , FIG. 10 is a partial plan view thereof, FIG. 11 is a cross-sectional view of the conventional example, FIG. 12 is a cross-sectional view of another conventional example, and FIG. 13 is a cross-sectional view of still another conventional example. 10.20, 30.50...Yoke core, 11°12
.. 25.26, 33, 34, 35, 36.5556.5
7.58... Excitation core, 13, 14, 2122.31
.. 32 51.52...Tsuba, 17,1839.40.
41.42... Winding Figure 1 Figure 7 Figure 8 Figure 11 Figure 2 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 断面H形のヨークコアと、このヨークコアの鍔間に設け
た複数の棒状の励磁コアと、この励磁コアに巻回した巻
線とを備えた電磁装置。
An electromagnetic device comprising a yoke core with an H-shaped cross section, a plurality of rod-shaped excitation cores provided between the flanges of the yoke core, and a winding wound around the excitation core.
JP28148089A 1989-10-26 1989-10-26 Electromagnetic device Pending JPH03141623A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28148089A JPH03141623A (en) 1989-10-26 1989-10-26 Electromagnetic device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28148089A JPH03141623A (en) 1989-10-26 1989-10-26 Electromagnetic device

Publications (1)

Publication Number Publication Date
JPH03141623A true JPH03141623A (en) 1991-06-17

Family

ID=17639771

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28148089A Pending JPH03141623A (en) 1989-10-26 1989-10-26 Electromagnetic device

Country Status (1)

Country Link
JP (1) JPH03141623A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06188132A (en) * 1992-12-18 1994-07-08 Toko Inc Boosting transformer
JP2005311227A (en) * 2004-04-26 2005-11-04 Sumida Corporation High-voltage transformer
CN109256266A (en) * 2017-07-12 2019-01-22 发那科株式会社 three-phase reactor

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06188132A (en) * 1992-12-18 1994-07-08 Toko Inc Boosting transformer
JP2005311227A (en) * 2004-04-26 2005-11-04 Sumida Corporation High-voltage transformer
CN109256266A (en) * 2017-07-12 2019-01-22 发那科株式会社 three-phase reactor
JP2019021673A (en) * 2017-07-12 2019-02-07 ファナック株式会社 Three-phase reactor
US10741319B2 (en) 2017-07-12 2020-08-11 Fanuc Corporation Three-phase reactor
CN109256266B (en) * 2017-07-12 2023-12-01 发那科株式会社 Three-phase reactor

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