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JPS62176111A - High-frequency transformer - Google Patents

High-frequency transformer

Info

Publication number
JPS62176111A
JPS62176111A JP61018408A JP1840886A JPS62176111A JP S62176111 A JPS62176111 A JP S62176111A JP 61018408 A JP61018408 A JP 61018408A JP 1840886 A JP1840886 A JP 1840886A JP S62176111 A JPS62176111 A JP S62176111A
Authority
JP
Japan
Prior art keywords
conductor
radial
balancer
frequency transformer
back sides
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
JP61018408A
Other languages
Japanese (ja)
Inventor
Kenzo Tanabe
田辺 謙造
Yoshihiro Bessho
芳宏 別所
Joji Kane
丈二 加根
Koji Hashimoto
興二 橋本
Tomohiro Kimura
知弘 木村
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 Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP61018408A priority Critical patent/JPS62176111A/en
Publication of JPS62176111A publication Critical patent/JPS62176111A/en
Pending legal-status Critical Current

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  • Production Of Multi-Layered Print Wiring Board (AREA)
  • Parts Printed On Printed Circuit Boards (AREA)
  • Coils Or Transformers For Communication (AREA)

Abstract

PURPOSE:To make a balancer hard to be influenced strongly by a conductive layer for electromagnetic field, even if it is arranged in the vicinity of a toroidal type coil, and yet to enable a thin type electromagnetic shielding, by closely coupling a multiple number of thin toroidal type coils having a rectangular cross section, using either a both-side or multilayer circuit substrate. CONSTITUTION:In the balancer, for instance, the primary winding consists of radial conductors 3A, 4A, 3C, 4C, 3E, 4E, etc. and thru-holes 5A, 6A, 5C, 6C, 5E, 6E, etc., having their electrodes 7A, 7B. The secondary winding consists of radial conductors 3B, 4B, 3D, 4D, 3F, etc. and thru-holes 5B, 5B, 5D, 6D, 5F, 6F, etc., having their electrodes 7C, 7D (central tap electrode), 7E. As mentioned above, this balance is of a close coupling of two pairs of toroidal type coils having a rectangular cross section. The main magnetic flux generated by a current running through the primary and secondary windings composes a closed magnetic route and is confined in the insulator 2 parallel with the substrate surface and composing the substrate. For this reason, even arranging a conductive layer for electromagnetic shield in the vicinity of the balancer can hardly influence the balancer strongly.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は主として両面回路基板を利用した高周波トラン
ス、バラン(以下、両者を高周波トランスと総称する)
に関するものである。
[Detailed Description of the Invention] Industrial Field of Application The present invention mainly relates to a high-frequency transformer and balun (hereinafter, both are collectively referred to as high-frequency transformers) that utilize a double-sided circuit board.
It is related to.

従来の技術 近年、電子機器の小型、薄型化指向は著しく、そのため
それらの機器を構成する高周波回路ブロック、たとえば
受信機フロントエンド部、チェーナ部などの高周波回路
部に対する小型化、薄型化要望は掻めて強くなってきた
BACKGROUND OF THE INVENTION In recent years, there has been a marked trend toward smaller and thinner electronic devices, and as a result, there has been a strong demand for smaller and thinner high-frequency circuit blocks such as receiver front-end sections and chainer sections that make up these devices. I've become stronger.

これら高周波回路部を小型化、薄型化するための1つの
課題はコイル、高周波トランスを小型化、薄型化するこ
とおよび薄型TL磁シールドを可能ならしめることであ
る。この中でコイルについてはり一ドレスチノプコイル
あるいはプリントコイルとして近年、とみに小型化、薄
型化がはかられてきたが、高周波トランスについては未
だ十分な配慮がなされていない。
One of the challenges in making these high frequency circuit parts smaller and thinner is to make the coils and high frequency transformers smaller and thinner, and to make thin TL magnetic shields possible. Among these coils, efforts have been made in recent years to make them smaller and thinner as one-dress tinop coils or printed coils, but sufficient consideration has not yet been given to high frequency transformers.

本発明はプリントコイルを基にして、薄型シールドの可
能な高周波トランスの実現をはかるものであり、まず、
従来のプリントコイルにつき説明する。
The present invention aims to realize a high frequency transformer that can be thinly shielded based on a printed coil.
A conventional printed coil will be explained.

第5図は従来より高周波分野でよく用いられている平面
型プリントコイルのパターン図である。
FIG. 5 is a pattern diagram of a planar printed coil that has been commonly used in the high frequency field.

第4図において、11は回路基板、12はその表面に形
成された導体パターンでありプリントコイルとしての働
きを有する。12の導体パターンの中心部は、導体パタ
ーンの最外周の終端部と共にコイル端子となるため、使
用時にはスルーホールあるいはジャンパー線などを用い
て他の回路部と接続されるが、図ではそれらの詳細につ
いては省略する。
In FIG. 4, 11 is a circuit board, and 12 is a conductor pattern formed on its surface, which functions as a printed coil. The center of the 12 conductor patterns, together with the outermost end of the conductor pattern, becomes the coil terminal, so when in use it is connected to other circuit parts using through holes or jumper wires, but the details are not shown in the figure. will be omitted.

上記プリントコイルに関しては例えばH,G。Regarding the above-mentioned printed coils, for example, H and G.

Dill著デザイング インダクターズ フォア スイ
ンフィルム アプリケーションズ:エレクトリソク デ
ザイン 第52項1964年2月17日(Design
ing  Iudnctors  For  Thin
−Film  Applications:Elect
ronic  DesignP52  Feb、17.
1964に詳述されている。
Dill, Design Inductors for Spinfilm Applications: Electrison Design Section 52, February 17, 1964 (Design
ing Iudnctors For Thin
-Film Applications: Elect
ronic DesignP52 Feb, 17.
1964.

発明が解決しようとする問題点 第5図に示す平面型プリントコイルを基にして高周波ト
ランスを形成する場合の問題は、コイルに流れる電流に
より生ずる磁束の主要部が回路基板面と垂直の方向に生
ずるため、このコイルを基にして形成された高周波トラ
ンスを有する回路基板に近接して導体、磁性体を配置す
ると、その影響を強(受け、高周波トランスの1次、2
次側インダクタンス、Qが大幅に変化するため薄型電磁
シールドを施しにくいと云う点にある。
Problems to be Solved by the Invention The problem when forming a high-frequency transformer based on the planar printed coil shown in Figure 5 is that the main part of the magnetic flux generated by the current flowing through the coil is perpendicular to the surface of the circuit board. Therefore, if a conductor or magnetic material is placed close to a circuit board that has a high-frequency transformer formed based on this coil, the influence will be strong (and the primary and secondary parts of the high-frequency transformer will be
The problem is that it is difficult to provide a thin electromagnetic shield because the next-side inductance, Q, changes significantly.

問題点を解決するための手段 回路基板の両面に対向して夫に断続された放射状導体を
形成する際に、表裏面の各放射状導体の各始点が同一円
周上で対向し、上記放射状導体の各終点が上記の各始点
を結ぶ円周と同心状で異なる直径を有する同一円周上に
並べられ、がっ、表裏面の互いに対向している始点に対
応する終点が、表、裏面の天々Mコ(Mは2以上の正整
数)隣りの終点と対応するよう、表裏面の放射状導体を
形成し、表、裏面の放射状導体の対向している各始点、
終点を天々スルーホール接続することにより、矩形状断
面を有し、各巻線が互いに密に結合されているMコの独
立したトロイダル型コイルを形成し、Mコの独立したト
ロイダル型コイルを天々、−次S綿、二次巻線、・・・
・・・M次巻線として使用する。また、適宜、各巻線の
任意の所にタップを設け、バランなどを構成する。
Means for Solving the Problems When forming intermittent radial conductors facing both sides of a circuit board, each starting point of each radial conductor on the front and back sides faces on the same circumference, and the radial conductors The end points of are arranged on the same circumference that is concentric with the circumference connecting the above starting points and have different diameters, and the end points corresponding to the starting points facing each other on the front and back sides are Form radial conductors on the front and back surfaces so as to correspond to the adjacent end points (M is a positive integer of 2 or more), and each starting point of the radial conductors on the front and back surfaces facing each other,
By connecting the end points to each other through holes, M independent toroidal coils with a rectangular cross section and each winding are closely coupled to each other are formed. -Next S cotton, secondary winding,...
...Used as the Mth winding. Further, taps are provided at arbitrary locations on each winding to form a balun or the like.

さらに、多層回路基板の内層導体を利用して上記の高周
波トランスを形成し、それに近接する導体層を電磁シー
ルド用導体層として用いる。
Furthermore, the above-mentioned high frequency transformer is formed using the inner layer conductor of the multilayer circuit board, and the conductor layer adjacent thereto is used as a conductor layer for electromagnetic shielding.

作用 本発明は上記のような矩形状断面を有する薄型トロイダ
ル状コイルを複数固形成し、高周波トランスの機能を有
せしめるものであるが、コイルに流れる電流により生ず
る磁束の主要部を回路基板面と平行方向でかつ閉磁路を
構成するように生ぜしめることにより、近接して導体層
を配置してもそれにより受ける影響を少なくし、もって
薄型電磁シールドの可能な高周波トランスを実現する。
Function The present invention solidly forms a plurality of thin toroidal coils having a rectangular cross section as described above to have the function of a high frequency transformer. By creating a closed magnetic path in parallel directions, the influence of conductor layers even if they are placed close to each other is reduced, thereby realizing a high frequency transformer capable of thin electromagnetic shielding.

実施例 以下、本発明の一実施例につき、図面を参照しながら説
明する。
EXAMPLE Hereinafter, an example of the present invention will be described with reference to the drawings.

第1図は本発明の高周波トランスの構造をバランを例に
とり概念的に示す斜視図である。
FIG. 1 is a perspective view conceptually showing the structure of a high frequency transformer according to the present invention, taking a balun as an example.

第1図においてIA、18は天々両面回路基板の表面お
よび裏面導体層、2は絶縁体、実線で示す3A〜3uは
表面導体層に形成された放射状導体、点線で示す4A〜
4.は裏面導体層に形成された放射状導体、5A〜5.
および6A〜61.Iは夫々放射状導体の各ライン3A
〜3゜および4A〜匂の各始点、終点の端部を電気的に
接続するためのスルーホール、そして7A〜7Eはバラ
ンの各電極を示す。
In FIG. 1, IA, 18 are front and back conductor layers of a double-sided circuit board, 2 is an insulator, 3A to 3u shown by solid lines are radial conductors formed on the front conductor layer, and 4A to 4A shown by dotted lines are shown in FIG.
4. 5A to 5. are radial conductors formed on the back conductor layer.
and 6A-61. I is each line 3A of radial conductor
~3° and 4A~ Through holes for electrically connecting the ends of the starting and ending points, and 7A to 7E represent the electrodes of the balun.

第1図に示すバランでは一次巻線は放射状導体3A、4
A、3o、4c、36.4E、30゜4o、3..4.
.3..4に、3..4.およびスルーホールSA、6
A、5o、6o、58゜6゜、5o、6o、5..6.
.5に、6K。
In the balun shown in Figure 1, the primary winding consists of radial conductors 3A, 4
A, 3o, 4c, 36.4E, 30°4o, 3. .. 4.
.. 3. .. 4, 3. .. 4. and through hole SA, 6
A, 5o, 6o, 58°6°, 5o, 6o, 5. .. 6.
.. 5, 6K.

5、.6.で構成され7A、7Bはその電極となり、二
次巻線は放射状導体3B、4B、38゜4D・ 3F・
 4F・ 3H・ 4H・ 3J・ 4J・3L、4L
およびスルーホール58.6B、5.。
5. 6. 7A and 7B are the electrodes, and the secondary windings are radial conductors 3B, 4B, 38° 4D, 3F,
4F・3H・4H・3J・4J・3L, 4L
and through hole 58.6B, 5. .

6D・ 5F・ 6F・ 5H・ 6H・ 5J・ 6
J・5L、6Lで構成され7c、7[)、78はその電
極(7,は中央タップ電極)となる。
6D・5F・6F・5H・6H・5J・6
It is composed of J, 5L, and 6L, and 7c, 7[), and 78 are its electrodes (7, is the center tap electrode).

第1図より明らかなように、このバランは薄い矩形断面
を有するトロイダル型コイルを2組、密に結合したもの
となり、−次S線、2次巻線に流れる電流によって生ず
る主磁束は基板面と平行でかつ基板を構成する絶縁体内
に閉磁路を構成するようにして閉し込められるため、こ
のバランに近接して電磁シールド用導体層を配置しても
、バランはその影響を強く受けにくくなり、薄型電磁シ
ールドの施されたバランを作ることができる。第2図は
、第1図のバランを平面図として示すものであり、図に
付している各番号は第1図のそれと同じであるためこれ
以上の詳述は省略する。
As is clear from Figure 1, this balun consists of two sets of toroidal coils with a thin rectangular cross section, tightly coupled together, and the main magnetic flux generated by the current flowing through the -order S wire and the secondary winding is directed to the substrate surface. Since the balun is parallel to the balun and is confined to form a closed magnetic path within the insulator that makes up the board, even if an electromagnetic shielding conductor layer is placed close to the balun, the balun is not strongly affected by it. Therefore, it is possible to create a balun with a thin electromagnetic shield. FIG. 2 shows a plan view of the balun shown in FIG. 1, and since each number attached to the figure is the same as that in FIG. 1, further detailed explanation will be omitted.

第3図は4層回路基板を利用し、薄型を磁シールドの施
されたバランの構造を概念的に示す斜視図であり、第1
図と同じ番号を付している部分は、第1図のそれと同じ
機能、構造を有するものであるため、これ以上の詳述は
省略する。第3図において8A〜8Dは夫々多層回路基
板の第1.第2゜第3.第4導体層を示し、9A〜96
はバラン電極を外部にとり出すため、第1導体層と第2
導体層または第3導体層に形成された放射状導体を電気
的に接続するためのスルーホール。10A。
FIG. 3 is a perspective view conceptually showing the structure of a balun that uses a four-layer circuit board and is thin and magnetically shielded.
Portions designated by the same numbers as in the figures have the same functions and structures as those in FIG. 1, so further detailed description will be omitted. In FIG. 3, 8A to 8D are the first sections of the multilayer circuit board, respectively. 2nd゜3rd. Indicates the fourth conductor layer, 9A to 96
In order to take out the balun electrode to the outside, the first conductor layer and the second
A through hole for electrically connecting radial conductors formed in the conductor layer or the third conductor layer. 10A.

108は電磁シールド用として使用される第1導体層と
第4導体層とを電気的に接続するためのスルホール、そ
して20A〜208は、夫々電磁シールド用として使用
される第1i体層の一部が島状に除去された部分に設け
られたバラン用電極を示す。
108 is a through hole for electrically connecting the first conductor layer and the fourth conductor layer used for electromagnetic shielding, and 20A to 208 are parts of the 1i-th body layer used for electromagnetic shielding. This shows the balun electrode provided in the part where the island shape has been removed.

第4図は第3図に示す4層回路基板の内部にバランが形
成された場合の外観を斜視図的に示すものであり、第3
図と同じ番号を付している部分は第3図のそれと同じ機
能、構造を有するため、これ以上の詳述は省略する。
FIG. 4 is a perspective view showing the external appearance when a balun is formed inside the four-layer circuit board shown in FIG.
Since the parts designated by the same numbers as in the figures have the same functions and structures as those in FIG. 3, further detailed description will be omitted.

以上の説明においては、中央クソブ付き二次巻線を有す
るバランを例にとり説明したが、図より明らかなように
第3次巻線、第4次巻線を設けること、タップをなくし
たり、任意の巻線の任意の点に設けることなどが本発明
に含まれることは云うまでもない。
In the above explanation, a balun having a secondary winding with a center socket was used as an example. However, as is clear from the figure, it is possible to provide a tertiary winding, a quaternary winding, eliminate a tap, or Needless to say, the present invention includes the provision of the winding at any point of the winding.

また、各巻線のインダクタンス、Q、結合度を上界させ
るため、本発明の趣旨をふまえて回路基板の絶縁体内に
磁性体を王とするフィラーを導入したり、磁性体そのも
のを絶縁性をよくして導入するなど任意の工夫を施しう
るのは勿論である。
Furthermore, in order to increase the inductance, Q, and degree of coupling of each winding, based on the purpose of the present invention, a filler made of a magnetic material is introduced into the insulator of the circuit board, and the magnetic material itself has good insulation properties. Of course, it is possible to take any other measures, such as introducing the system.

発明の効果 以上のように本発明は両面回路基板、多層回路基板を用
い矩形断面を有する薄いトロイダル型ニイルを複数組、
密結合にすることにより高周波トランスを構成するもの
であり、トランスの各巻線に流れる電流によって生ずる
主磁束は基板面と平行でかつ基板を構成する絶縁体内に
閉磁路を構成して閉じ込められるため、この高周波トラ
ンスに近接して電磁シールド用導体層を配置しても、そ
の影響を強く受けにくくなり薄型電磁シールドの可能な
高周波トランスを得ることができる。
Effects of the Invention As described above, the present invention uses a double-sided circuit board, a multilayer circuit board, and a plurality of sets of thin toroidal type foils having a rectangular cross section.
A high-frequency transformer is constructed by tightly coupling the transformer, and the main magnetic flux generated by the current flowing through each winding of the transformer is parallel to the substrate surface and is confined by forming a closed magnetic path within the insulator that makes up the substrate. Even if a conductor layer for electromagnetic shielding is placed close to this high-frequency transformer, it is less susceptible to the influence, and a high-frequency transformer capable of thin electromagnetic shielding can be obtained.

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

第3図は4N回路基板を利用し薄型電磁シールドの施さ
れたバランの構造を概念的に示す斜視図、第4図は第3
図に示す4N回路基板の内部にバランが形成された場合
の外観を示す斜視図、第5図は従来の平面プリントコイ
ルを示す斜視図である。 IA、1.、・・・・・・両面回路基板の表面、裏面導
体層、2・・・・・・絶縁体、3A〜3工・・・・・・
表面導体層に形成された放射状導体、4A〜4゜・・・
・・・裏面導体層に形成された放射状導体、5A〜5゜
・・・・・・表面。 裏面の導体層間に形成された放射状、および・・・・・
・6A〜6o・・・・・・導体の各始点、および終点を
電気的に結合するスルーホール、7A〜78・・・・・
・バラン用電極、8A〜8.・・・・・・4層回路基板
の導体層、9A〜9E・・・・・・バラン電極を外部に
とり出すためのスルーホール、■OA、10B・・・・
・・電極シールド用導体間を接続するスルーホール、2
0A〜208・・・・・・バラン用電極、11・・・・
・・回路基板、12・・・・・・従来の平面型プリント
コイル導体パターン。 代理人の氏名 弁理士 中尾敏男 はか1名δA−−−
ヤ1キ住看 8B−一一す2 デ δ。−一−す3 ・ 第3図   δD−り→・ 9a−9E−−−+r才21iLiijlt1.rJI
ff;f焚:□、’H’;、:h&:!−;−L2θ〜
FOr−バラノ連Aへ
Figure 3 is a perspective view conceptually showing the structure of a balun that uses a 4N circuit board and is provided with a thin electromagnetic shield.
FIG. 5 is a perspective view showing the external appearance of a 4N circuit board shown in which a balun is formed inside the circuit board, and FIG. 5 is a perspective view showing a conventional planar printed coil. IA, 1. ,...Front surface of double-sided circuit board, back conductor layer, 2...Insulator, 3A to 3 construction...
Radial conductor formed on the surface conductor layer, 4A~4°...
. . . Radial conductor formed on the back conductor layer, 5A to 5° . . . Surface. The radial pattern formed between the conductor layers on the back side, and...
・6A to 6o...Through holes that electrically connect each starting point and end point of the conductor, 7A to 78...
- Balun electrode, 8A-8. ...Conductor layer of 4-layer circuit board, 9A to 9E...Through hole for taking out the balun electrode to the outside, ■OA, 10B...
・Through hole connecting between conductors for electrode shield, 2
0A~208...Balun electrode, 11...
...Circuit board, 12...Conventional planar printed coil conductor pattern. Name of agent: Patent attorney Toshio Nakao, 1 person δA ---
Ya 1 Ki Jukan 8B-11su 2 De δ. -1-su3・Figure 3 δD-ri→・9a-9E---+r21iLiijlt1. rJI
ff; f firing: □, 'H';, :h&:! -;-L2θ~
FOR-Barano Ren A

Claims (3)

【特許請求の範囲】[Claims] (1)回路基板の両面に対向して夫々断続された放射状
導体を形成する際に、表、裏面の各放射状導体の各始点
が同一円周上で対向し、表、裏面の各放射状導体の各終
点が上記の各始点を結ぶ円周と同心状で異なる直径を有
する同一円周上に並べられ、かつ、表、裏面の互いに対
向している始点に対応する終点が、表、裏面の夫々Mコ
(Mは2以上の正整数)隣りの終点と対応するよう、表
、裏面の放射状導体を形成し、表、裏面の放射状導体の
対向している各始点、終点を天々スルーホール接続する
ことにより矩形状断面を有し、各巻線が互いに密に結合
されているMコの独立したトロイダル型コイルを形成し
、Mコの独立したトロイダル型コイルを天々、M次巻線
(Mは1以上の正整数)として使用することを特徴とす
る高周波トランス。
(1) When forming interrupted radial conductors facing both sides of a circuit board, each starting point of each radial conductor on the front and back sides is opposite on the same circumference, and each radial conductor on the front and back sides is The end points are arranged on the same circumference that is concentric with the circumference connecting the above starting points and have different diameters, and the end points corresponding to the starting points facing each other on the front and back sides are on the front and back sides, respectively. Form radial conductors on the front and back surfaces so that they correspond to the adjacent end points (M is a positive integer of 2 or more), and connect the opposing starting and ending points of the radial conductors on the front and back sides through holes. By doing so, M independent toroidal coils having a rectangular cross section and each winding are tightly coupled to each other are formed. is a positive integer of 1 or more).
(2)Mコの各巻線の任意の位置にタップを設けること
を特徴とする特許請求の範囲第(1)項記載の高周波ト
ランス。
(2) A high-frequency transformer according to claim (1), characterized in that a tap is provided at an arbitrary position on each winding of M coils.
(3)表裏面の断続された放射状導体パターンが形成さ
れている全領域をおおって絶縁層を形成し、さらにそれ
をおおって導体層を形成し、この導体層を高周波トラン
スの電磁シールド用導体層として使用することを特徴と
する特許請求の範囲第(1)項記載の高周波トランス。
(3) Form an insulating layer covering the entire area where the interrupted radial conductor pattern is formed on the front and back surfaces, further cover it to form a conductor layer, and use this conductor layer as a conductor for electromagnetic shielding of a high frequency transformer. The high frequency transformer according to claim (1), which is used as a layer.
JP61018408A 1986-01-30 1986-01-30 High-frequency transformer Pending JPS62176111A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61018408A JPS62176111A (en) 1986-01-30 1986-01-30 High-frequency transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61018408A JPS62176111A (en) 1986-01-30 1986-01-30 High-frequency transformer

Publications (1)

Publication Number Publication Date
JPS62176111A true JPS62176111A (en) 1987-08-01

Family

ID=11970836

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61018408A Pending JPS62176111A (en) 1986-01-30 1986-01-30 High-frequency transformer

Country Status (1)

Country Link
JP (1) JPS62176111A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004259944A (en) * 2003-02-26 2004-09-16 Densei Lambda Kk Method for manufacturing inductance element
WO2005031765A1 (en) * 2003-09-29 2005-04-07 Tamura Corporation Laminated magnetic component
WO2005031766A1 (en) * 2003-09-29 2005-04-07 Tamura Corporation Multilayer board incorporating laminated magnetic components
JP2010516056A (en) * 2007-01-11 2010-05-13 プラナーマグ インコーポレイテッド Flat type wideband transformer
JP2010525576A (en) * 2007-04-19 2010-07-22 ハリス コーポレイション Embedded step-up toroidal transformer
WO2017079337A1 (en) * 2015-11-03 2017-05-11 Qualcomm Incorporated Toroid inductor with reduced electromagnetic field leakage
US10158293B2 (en) 2014-11-12 2018-12-18 Murata Manufacturing Co., Ltd. Power supply module and mounting structure therefor

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004259944A (en) * 2003-02-26 2004-09-16 Densei Lambda Kk Method for manufacturing inductance element
WO2005031765A1 (en) * 2003-09-29 2005-04-07 Tamura Corporation Laminated magnetic component
WO2005031766A1 (en) * 2003-09-29 2005-04-07 Tamura Corporation Multilayer board incorporating laminated magnetic components
JP2010516056A (en) * 2007-01-11 2010-05-13 プラナーマグ インコーポレイテッド Flat type wideband transformer
JP2010525576A (en) * 2007-04-19 2010-07-22 ハリス コーポレイション Embedded step-up toroidal transformer
US10158293B2 (en) 2014-11-12 2018-12-18 Murata Manufacturing Co., Ltd. Power supply module and mounting structure therefor
WO2017079337A1 (en) * 2015-11-03 2017-05-11 Qualcomm Incorporated Toroid inductor with reduced electromagnetic field leakage
US10170232B2 (en) 2015-11-03 2019-01-01 Qualcomm Incorporated Toroid inductor with reduced electromagnetic field leakage

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