JP2522318B2 - Transformer - Google Patents

Transformer

Info

Publication number
JP2522318B2
JP2522318B2 JP62208929A JP20892987A JP2522318B2 JP 2522318 B2 JP2522318 B2 JP 2522318B2 JP 62208929 A JP62208929 A JP 62208929A JP 20892987 A JP20892987 A JP 20892987A JP 2522318 B2 JP2522318 B2 JP 2522318B2
Authority
JP
Japan
Prior art keywords
layer
conductor layer
magnetic
transformer
conductor
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.)
Expired - Lifetime
Application number
JP62208929A
Other languages
Japanese (ja)
Other versions
JPS6451648A (en
Inventor
達也 筧
好 ▲吉▼野
青  建一
一朗 伊澤
俊和 荒砂
博 桜井
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.)
Denso Corp
Original Assignee
NipponDenso Co 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 NipponDenso Co Ltd filed Critical NipponDenso Co Ltd
Priority to JP62208929A priority Critical patent/JP2522318B2/en
Publication of JPS6451648A publication Critical patent/JPS6451648A/en
Application granted granted Critical
Publication of JP2522318B2 publication Critical patent/JP2522318B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) この発明は変圧器に関するものである。TECHNICAL FIELD The present invention relates to a transformer.

(従来の技術及び問題点) 従来、変圧器は磁性コアとその磁性コアに巻かれた銅
線等により構成され、電子部品の中では比較的大きな体
積を要し、集積化が非常に困難であった。又、特開昭62
−88354号公報のように巻線形の集積化変圧器も提案さ
れているが、一次・二次間の導線の間隔を一定に保つこ
とが困難であるとともに磁路面積を大きくするには限界
があり結合効率を向上させることが困難であった。
(Prior Art and Problems) Conventionally, a transformer is composed of a magnetic core and a copper wire wound around the magnetic core, which requires a relatively large volume among electronic components and is extremely difficult to integrate. there were. In addition, JP-A-62
A winding type integrated transformer is also proposed as in Japanese Patent Publication No. 88354, but it is difficult to maintain a constant spacing between the primary and secondary conductors, and there is a limit to increasing the magnetic path area. Yes It was difficult to improve the coupling efficiency.

(発明の目的) この発明の目的は上記問題点を解消し、従来の変圧器
とは全く異なった構造を採用することにより集積化が可
能であるとともに結合効率を向上させることができる変
圧器を提供することにある。
(Object of the Invention) An object of the present invention is to solve the above problems and to adopt a transformer which can be integrated and improve the coupling efficiency by adopting a completely different structure from the conventional transformer. To provide.

(問題点を解決するための手段) この発明は上記目的を達成すべく、並設した第1及び
第2の導体層をそれぞれ絶縁体層にて覆うとともにそれ
ら絶縁層の外周を磁性体層で囲い、前記並設した第1及
び第2の導体層の両端間をそれぞれ一次側及び二次側と
した変圧器をその要旨とするものである。
(Means for Solving the Problems) In order to achieve the above object, the present invention covers the first and second conductor layers juxtaposed with each other with an insulating layer and surrounds the outer periphery of the insulating layer with a magnetic layer. The gist of the present invention is a transformer in which an enclosure and a first side and a second side of the first and second conductor layers, which are arranged side by side, are respectively set as a primary side and a secondary side.

(作用) 一次側に電圧を印加すると、第1の導体層に電流が流
れ、磁性体層に磁束が形成され、相互誘導作用により第
2の導体層に電圧が発生し二次側に出力される。
(Operation) When a voltage is applied to the primary side, a current flows in the first conductor layer, a magnetic flux is formed in the magnetic layer, and a voltage is generated in the second conductor layer due to the mutual induction action and is output to the secondary side. It

(実施例) 以下、この発明を具体化した一実施例を図面に従って
説明する。
(Embodiment) An embodiment of the present invention will be described below with reference to the drawings.

第1図に示すように、SiO2又はポリイミド系絶縁材料
(PIQ)よりなる基板1上には第1の磁性体層2が平面
略M字状に形成され、その第1の磁性体層2上には第1
の絶縁体層3が積層されている。第1の絶縁体層3の上
部には第1の導体層4が積層され、さらに、その第1の
導体層4の上面及び両側は第2の絶縁体層5が積層され
ている。
As shown in FIG. 1, a first magnetic layer 2 is formed on a substrate 1 made of SiO 2 or a polyimide-based insulating material (PIQ) in a substantially M-shape in a plane, and the first magnetic layer 2 is formed. First on top
Insulator layer 3 is laminated. The first conductor layer 4 is laminated on the first insulator layer 3, and the second insulator layer 5 is laminated on the upper surface and both sides of the first conductor layer 4.

前記第2の絶縁体層5の上面には第2の導体層6が積
層され、その第2の導体層6の上面及び両側は第3の絶
縁体層7が積層されている。この第3の絶縁体層7の上
面及び前記第1,第2,第3の絶縁体層3,5,7両側部は第2
の磁性体層8で覆われ、前記第1の磁性体層2と接続さ
れている。
A second conductor layer 6 is laminated on the upper surface of the second insulator layer 5, and a third insulator layer 7 is laminated on the upper surface and both sides of the second conductor layer 6. The upper surface of the third insulator layer 7 and both sides of the first, second and third insulator layers 3, 5, 7 are second
Of the magnetic material layer 8 and is connected to the first magnetic material layer 2.

よって、平面略M字状に延設された本実施例の変圧器
の断面において、並設された第1及び第2の導体層4,6
はそれぞれ周囲を第1,第2,第3の絶縁体層3,5,7で覆わ
れるとともに、その絶縁体層3,5,7の外周(全周)は第
1,第2の磁性体層2,8にて囲われている。
Therefore, in the cross section of the transformer of this embodiment extending in a substantially M shape in a plane, the first and second conductor layers 4 and 6 arranged in parallel are arranged.
Are covered with the first, second and third insulator layers 3, 5, 7 respectively, and the outer circumference (entire circumference) of the insulator layers 3, 5, 7 is the first.
It is surrounded by the first and second magnetic layers 2 and 8.

この第1及び第2の導体層4,6にはAl,Cu,Au等が使用
される。又、第1及び第2の磁性体層2,8はNi−Fe,Ni−
Co等のパーマロイ、又は、フェライト,アモルファス等
が使用される。さらに、これらの各層の積層は真空蒸着
やスパッタリング等により行なわれる。
Al, Cu, Au, etc. are used for the first and second conductor layers 4, 6. The first and second magnetic layers 2, 8 are made of Ni-Fe, Ni-
Permalloy such as Co, ferrite, amorphous or the like is used. Further, lamination of these layers is performed by vacuum vapor deposition, sputtering or the like.

そして、平面略M字状に延設された第1の導体層4の
両端4a,4b間を一次側とするとともに第2の導体層6の
両端6a,6b間を二次側とし、一次側(第1の導体層4の
両端4a,4b間)に交流電流又はパルスを入力すると、第
1及び第2の磁性体層2,8中の磁束が変化し相互誘導作
用により第2の導体層6の両端6a,6b間に起電力を発生
する。即ち、第2図に示すように、第1の導体層4に電
流I0が流れると、第1及び第2の磁性体層2,8に磁束Φ
の変化が生じる。その結果、第2の導体層6の両端6a,6
b間に電圧が発生し二次側に出力されることとなる。
The primary side is defined by the ends 4a, 4b of the first conductor layer 4 extending in a substantially M-shape on the plane, and the secondary side is defined by the ends 6a, 6b of the second conductor layer 6. When an alternating current or a pulse is applied to (between both ends 4a, 4b of the first conductor layer 4), the magnetic flux in the first and second magnetic material layers 2, 8 changes and the second conductor layer is induced by mutual induction. An electromotive force is generated between both ends 6a, 6b of 6. That is, as shown in FIG. 2, when the current I 0 flows through the first conductor layer 4, the magnetic flux Φ flows through the first and second magnetic layers 2, 8.
Changes occur. As a result, both ends 6a, 6 of the second conductor layer 6 are
A voltage is generated between points b and is output to the secondary side.

この際、磁路は閉じており、漏れ磁束を小さくするこ
とができる。又、磁束が断面積S,磁路長L,透磁率μの磁
気コアを通ると、磁気抵抗はR=L/μSであり、本実施
例の場合は、第2図で示す幅Waで、長さが平面略M字状
の全長Haであり、その断面積Sa(=Wa・Ha)は幅Waを大
きくするか、あるいは、全長Haを長くすることにより断
面積Saを大きくすることができる。さらに、磁路の長さ
は第1及び第2の磁性体層2,8の一周分であり(第2図
中、La)、短くすることができる。即ち、磁路長Laを小
さくできるとともに断面積Sa(=Wa・Ha)を大きくする
ことができることにより、磁気抵抗Ra(=La/μSa)を
小さくすることができ、第1の導体層4の両端4a,4b間
と第2の導体層6の両端6a,6b間の結合の程度を良くす
ることができることとなる。
At this time, the magnetic path is closed, and the leakage magnetic flux can be reduced. Further, when the magnetic flux passes through the magnetic core having the cross-sectional area S, the magnetic path length L and the magnetic permeability μ, the magnetic resistance is R = L / μS, and in the case of the present embodiment, the width Wa shown in FIG. The length is a substantially M-shaped total length Ha, and its cross-sectional area Sa (= Wa · Ha) can be increased by increasing the width Wa or by increasing the total length Ha. . Furthermore, the length of the magnetic path is one round of the first and second magnetic layers 2 and 8 (La in FIG. 2) and can be shortened. That is, since the magnetic path length La can be reduced and the cross-sectional area Sa (= Wa · Ha) can be increased, the magnetic resistance Ra (= La / μSa) can be reduced and the first conductor layer 4 The degree of coupling between both ends 4a and 4b and both ends 6a and 6b of the second conductor layer 6 can be improved.

又、薄膜で形成される変圧器であるためIC内に集積化
が可能となる。さらに、従来の巻線形構造の変圧器にお
いては、一次側・二次側の導線の間隔を一定に保つこと
が困難であったが、本実施例では第1の導体層4と第2
の導体層6とはその間隔はどの場所でも等しくすること
ができ結合効率を上げることができる。
In addition, since it is a thin film transformer, it can be integrated in an IC. Further, in the conventional winding type transformer, it was difficult to keep the distance between the primary side and secondary side conductors constant, but in the present embodiment, the first conductor layer 4 and the second conductor layer 4
The space between the conductor layer 6 and the conductor layer 6 can be made equal at any place, and the coupling efficiency can be improved.

尚、この発明は上記実施例に限定されるものではな
く、例えば第3図に示すように従来の変圧器での巻線比
を変えたものとすることができる。これは、導体層9を
一次側とするとともに、導体層10と11を直列にし二次側
としたものである。この場合、従来の変圧器における巻
数比1対2に相当する。
The present invention is not limited to the above-mentioned embodiment, but the winding ratio in the conventional transformer may be changed as shown in FIG. 3, for example. This is one in which the conductor layer 9 is the primary side and the conductor layers 10 and 11 are in series and are the secondary side. This case corresponds to a turns ratio of 1: 2 in the conventional transformer.

又、第4図は最初の実施例と同じく巻数比1対1に相
当するものであり、導体層12,13を同一面に並設し、導
体を多層にする必要をなくしたものである。
Also, FIG. 4 corresponds to a winding ratio of 1: 1 as in the first embodiment, and the conductor layers 12 and 13 are arranged in parallel on the same plane, thereby eliminating the need for a multilayer conductor.

発明の効果 以上詳述したようにこの発明によれば、従来の変圧器
とは全く異なった構造を採用することにより集積化でき
るとともに結合効率を向上させることができる優れた効
果を発揮する。
EFFECTS OF THE INVENTION As described in detail above, according to the present invention, by adopting a structure that is completely different from that of the conventional transformer, it is possible to achieve an excellent effect that it can be integrated and the coupling efficiency can be improved.

【図面の簡単な説明】[Brief description of drawings]

第1図はこの発明を具体化した変圧器を示す斜視図、第
2図は変圧器の要部を示す図、第3図は別例を示す変圧
器の断面図、第4図は他の別例の変圧器の断面図であ
る。 2は第1の磁性体層、3は第1の絶縁体層、4は第1の
導体層、5は第2の絶縁体層、6は第2の導体層、7は
第3の絶縁体層、8は第2の磁性体層、9は導体層、10
は導体層、11は導体層、12は導体層、13は導体層。
FIG. 1 is a perspective view showing a transformer embodying the present invention, FIG. 2 is a view showing a main part of the transformer, FIG. 3 is a sectional view of a transformer showing another example, and FIG. It is sectional drawing of the transformer of another example. 2 is a first magnetic layer, 3 is a first insulator layer, 4 is a first conductor layer, 5 is a second insulator layer, 6 is a second conductor layer, and 7 is a third insulator. Layer, 8 is the second magnetic layer, 9 is a conductor layer, 10
Is a conductor layer, 11 is a conductor layer, 12 is a conductor layer, and 13 is a conductor layer.

フロントページの続き (72)発明者 伊澤 一朗 愛知県刈谷市昭和町1丁目1番地 日本 電装株式会社内 (72)発明者 荒砂 俊和 愛知県刈谷市昭和町1丁目1番地 日本 電装株式会社内 (72)発明者 桜井 博 愛知県刈谷市昭和町1丁目1番地 日本 電装株式会社内 (56)参考文献 特開 昭63−110767(JP,A) 実開 昭58−3016(JP,U)Front Page Continuation (72) Inventor Ichiro Izawa 1-1 Showa-cho, Kariya Aichi Prefecture, Japan Denso Co., Ltd. (72) Inventor Toshikazu Arasa 1-1-Showa-cho Kariya, Aichi Prefecture Nippon Denso Co., Ltd. (72 ) Inventor Hiroshi Sakurai, 1-1, Showa-cho, Kariya city, Aichi Japan Denso Co., Ltd. (56) Reference JP-A-63-110767 (JP, A)

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】並設した第1及び第2の導体層をそれぞれ
絶縁体層にて覆うとともにそれら絶縁層の外周を磁性体
層で囲い、前記並設した第1及び第2の導体層の両端間
をそれぞれ一次側及び二次側としたことを特徴とする変
圧器。
1. A first conductor layer and a second conductor layer, which are arranged in parallel, are covered with an insulating layer, and the outer circumferences of the insulating layers are surrounded by a magnetic material layer. A transformer having a primary side and a secondary side between both ends.
JP62208929A 1987-08-21 1987-08-21 Transformer Expired - Lifetime JP2522318B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62208929A JP2522318B2 (en) 1987-08-21 1987-08-21 Transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62208929A JP2522318B2 (en) 1987-08-21 1987-08-21 Transformer

Publications (2)

Publication Number Publication Date
JPS6451648A JPS6451648A (en) 1989-02-27
JP2522318B2 true JP2522318B2 (en) 1996-08-07

Family

ID=16564464

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62208929A Expired - Lifetime JP2522318B2 (en) 1987-08-21 1987-08-21 Transformer

Country Status (1)

Country Link
JP (1) JP2522318B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH09213530A (en) * 1996-01-30 1997-08-15 Alps Electric Co Ltd Plane transformer

Also Published As

Publication number Publication date
JPS6451648A (en) 1989-02-27

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