JPH01246808A - Electromagnetic device - Google Patents

Electromagnetic device

Info

Publication number
JPH01246808A
JPH01246808A JP7741988A JP7741988A JPH01246808A JP H01246808 A JPH01246808 A JP H01246808A JP 7741988 A JP7741988 A JP 7741988A JP 7741988 A JP7741988 A JP 7741988A JP H01246808 A JPH01246808 A JP H01246808A
Authority
JP
Japan
Prior art keywords
magnetic path
magnetic
inductance
recessed
parts
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
JP7741988A
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 JP7741988A priority Critical patent/JPH01246808A/en
Publication of JPH01246808A publication Critical patent/JPH01246808A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To increase the variable amount of inductance by a method wherein the title electromagnetic device is constituted in such a manner that the protruding part of the external magnetic path is positioned outside the protruding part of the internal magnetic path of a pot core, and the recessed part of the external magnetic path is positioned outside the recessed part of the inner magnetic path. CONSTITUTION:Pot cores 11 and 12 are composed of inner magnetic paths 13 and 15, which are through inside of a bobbin 10, and the external magnetic paths 14 and 16 which are fitted externally. The butting surfaces 17, 18, 19 and 20 of the inner magnetic paths 13 and 15 and outer magnetic paths 14 and 16 are divided into two parts in circumferential direction of protruding parts 21, 23, 25 and 27 and recessed parts 22, 24, 26 and 28, and the protruding parts 21 and 25, and 23 and 27 and the recessed parts 22 and 26, and 24 and 28 are opposingly positioned with each other. The more the distance between magnetic materials becomes smaller, the more magnetic reluctance becomes low, and also the more the opposing area becomes wider, the more magnetic resistance becomes lower. As a result, in the state of theta=0 (protruding parts 21 and 25, and 23 and 27 are opposing with each other, the magnetic resistance becomes larger in the order of theta=90 deg. and theta=180, and inductance becomes lower. At the same time, the variable amount of the inductance increases when compared with the device manufactured in the past in which recessed and protruding parts are formed on the inner magnetic path only and also the device in which the recessed and protruding parts of the inner and the outer magnetic paths are not opposingly positioned.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、高周波トランスおよびチョーク等の電磁装
置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to electromagnetic devices such as high frequency transformers and chokes.

〔従来の技術〕[Conventional technology]

従来、電話、電信用回路あるいはスイッチング電源、イ
ンバータ点灯回路等、10KHz以上で使用されている
高周波トランスおよびチョーク等の電磁装置がある。電
磁装置は、巻線と、巻線を囲む2個のコアからなる。コ
アは、円筒状のいわゆるポットコアが使用され、コイル
の周波数特性が高く、漏れ磁束が少ないことから、古く
から使用されているが、回路上、コイルのインダクタン
ス管理のニーズが非常に強い。例えば、LCの直列共振
回路で共振周波数を変化させる場合、耐圧の高い可変コ
ンデンサがない場合、可変インダクタンスを使用しなけ
ればならない。また、コアおよび巻線の製造のばらつき
のため、規格外のインダクタンスが大量に発生した際、
これを調整する必要が生じる。
2. Description of the Related Art Conventionally, there are electromagnetic devices such as high frequency transformers and chokes used at frequencies of 10 KHz or higher, such as telephones, electronic circuits, switching power supplies, inverter lighting circuits, and the like. The electromagnetic device consists of a winding and two cores surrounding the winding. The core used is a cylindrical pot core, which has been used for a long time because the coil has high frequency characteristics and low leakage magnetic flux, but there is a strong need for coil inductance management from a circuit standpoint. For example, when changing the resonant frequency in an LC series resonant circuit, a variable inductance must be used if there is no variable capacitor with high voltage resistance. Also, when a large amount of non-standard inductance occurs due to manufacturing variations in the core and windings,
This will need to be adjusted.

そこで、円筒状のポットコアを利用した可変インダクタ
ンス素子として、第12図ないし第14図に示すものが
ある。図において、50はボビンであり、51.52は
フェライト製の一対のコアである。各コア51.52の
ボビン50を通る内磁路53,54の付合せ面55.5
6は、凸部57゜58と凹部59,60とに2分割され
ている。上下のコア51.52を垂直軸回りに相対的に
回転して、付合せ面55.56の磁気抵抗を変化させ、
インダクタンスを変える。第15図ないし第18図を用
いて、回転による付合せ面55.56の磁束の変化につ
いて説明する。第15図および第16図の状態は、付合
せ面55.56の凸部57.58どうしおよび凹部59
,60どうしが向き合ったものである(回転角度θ−〇
°とする)。また、第17図および第18図の状態は、
第15図の状態に比べ、コア51とコア52を相対的に
90度面回転たものであり(θ=90°)、凸部57゜
58どうしの重なり面積は半分である。磁気抵抗は、磁
性体間距離が小さいほど、また対向する面積が大きいほ
ど小さくなるので、第17図の状態より第15図の状態
の方が磁気抵抗が小さく、インダクタンスが高くなる。
Therefore, there are variable inductance elements using a cylindrical pot core as shown in FIGS. 12 to 14. In the figure, 50 is a bobbin, and 51 and 52 are a pair of ferrite cores. A mating surface 55.5 of the inner magnetic paths 53, 54 passing through the bobbin 50 of each core 51.52
6 is divided into two parts: a convex portion 57°58 and a concave portion 59,60. The upper and lower cores 51.52 are rotated relatively around the vertical axis to change the magnetic resistance of the mating surfaces 55.56,
Change the inductance. Changes in the magnetic flux of the mating surfaces 55, 56 due to rotation will be explained using FIGS. 15 to 18. The states shown in FIGS. 15 and 16 are the convex portions 57 and 58 of the mating surfaces 55 and 56 and the concave portions 59.
, 60 face each other (rotation angle θ-〇°). In addition, the states shown in FIGS. 17 and 18 are as follows:
Compared to the state shown in FIG. 15, the cores 51 and 52 are relatively rotated by 90 degrees (θ=90 degrees), and the overlapping area of the convex portions 57 and 58 is half. The magnetic resistance decreases as the distance between the magnetic bodies becomes smaller and as the opposing area increases, so the magnetic resistance is smaller and the inductance is higher in the state shown in FIG. 15 than in the state shown in FIG. 17.

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

前述のように、コア51.52の回転を利用した可変イ
ンダクタンス素子はを望であるが、コア51.52の内
磁路53..54のみに凸部57゜58および凹部59
,60を設けただけでは、インダクタンスの可変量が小
さく、特に上下のコア51.52間にギヤラフを有する
ような電磁装置では、所定の可変量が得られないという
問題があった。
As mentioned above, it is desirable to have a variable inductance element that utilizes the rotation of the cores 51, 52, but the inner magnetic path 53. .. Convex portions 57° 58 and concave portions 59 only on 54
, 60, the amount of inductance variation is small, and particularly in an electromagnetic device having a gear rough between the upper and lower cores 51 and 52, there is a problem that a predetermined amount of variation cannot be obtained.

そこで、第19図ないし第21図に示すように、ポット
コア65.66の外付路67.68の付合せ面69.7
0にも、凸部7]、72と凹部73゜74を形成した電
磁装置が提案されている。外磁路67.68の凸部71
.72は、内磁路75゜76の凹部79,80の外側に
位置し、外磁路67゜68の凹部73,74は、内磁路
15.76の凸部77.78の外側に位置している。
Therefore, as shown in FIGS. 19 to 21, the mating surface 69.7 of the external passage 67.68 of the pot core 65.66 is
0 has also proposed an electromagnetic device in which convex portions 7], 72 and concave portions 73 and 74 are formed. Convex portion 71 of outer magnetic path 67,68
.. 72 is located outside the recesses 79, 80 of the inner magnetic path 75.76, and the recesses 73, 74 of the outer magnetic path 67.68 are located outside the convex portions 77.78 of the inner magnetic path 15.76. ing.

第22図ないし第25図は、ポットコア65゜66を垂
直軸回りに相対的に回転して磁気抵抗を変化させた状態
を示している。第22図および第23図の状態は、凸部
71,72,77、.78どうしおよび凹部73,74
,79.80どうしが向き合ったものであり(回転角度
θ=0°とする)、磁気抵抗が最小となり、インダクタ
ンスが最大となる。また、第24図および第25図の状
態は、ポットコア65.66を相対的に180度回転し
たものであり(θ−180’)、磁気抵抗が最大となり
、インダクタンスが最小となる。
FIGS. 22 to 25 show the pot core 65.degree. 66 rotated relative to each other about the vertical axis to change the magnetic resistance. The states shown in FIGS. 22 and 23 are the convex portions 71, 72, 77, . 78 and recesses 73 and 74
, 79.80 face each other (rotation angle θ=0°), magnetic resistance is minimized, and inductance is maximized. Further, in the states shown in FIGS. 24 and 25, the pot cores 65 and 66 are relatively rotated by 180 degrees (θ-180'), and the magnetic resistance is maximum and the inductance is minimum.

しかし、依然として、インダクタンスの変化量は小さい
However, the amount of change in inductance is still small.

したがって、この発明の目的は、インダクタンスの可変
量が増大した電磁装置を提供することである。
Therefore, it is an object of the present invention to provide an electromagnetic device with increased variable inductance.

〔課題を解決するための手段〕[Means to solve the problem]

この発明の電磁装置は、電線を巻回したボビンを設け、
このボビンに両端から挟んで取付けられ内磁路および外
磁路の付合せ面に各々周方向に並んで凹凸部を形成した
一対の筒状のポットコアを設けたものであり、前記内磁
路の凸部の外側に前記外磁路の凸部が位置し、かつ前記
内磁路の凹部の外側に前記外磁路の凹部が位置している
ことを特徴とするものである。
The electromagnetic device of this invention includes a bobbin wound with electric wire,
A pair of cylindrical pot cores are attached to the bobbin from both ends, and each of the mating surfaces of the inner magnetic path and the outer magnetic path is lined up in the circumferential direction and has concave and convex portions formed thereon. The convex portion of the outer magnetic path is located outside the convex portion, and the recessed portion of the outer magnetic path is located outside the recessed portion of the inner magnetic path.

(作 用) この発明の電磁装置によると、一対のポットコアの内磁
路および外磁路の付合せ面に各々周方向に並んで凹凸部
が形成されている。しかも、内磁路の凸部の外側に外磁
路の凸部が位置し、かつ内磁路の凹部の外側に外磁路の
凹部が位置している。
(Function) According to the electromagnetic device of the present invention, the uneven portions are formed on the mating surfaces of the inner magnetic path and the outer magnetic path of the pair of pot cores so as to be lined up in the circumferential direction. Furthermore, the convex portion of the outer magnetic path is located outside the convex portion of the inner magnetic path, and the concave portion of the outer magnetic path is located outside the concave portion of the inner magnetic path.

したがって、従来のように内磁路のみに凹凸部を形成し
たものや、内磁路と外磁路の各凹凸部が対応していない
ものに比べ、インダクタンスの可変量が増大する。
Therefore, the amount of variation in inductance increases compared to a conventional structure in which uneven portions are formed only in the inner magnetic path, or in which the uneven portions in the inner magnetic path and outer magnetic path do not correspond to each other.

〔実施例〕〔Example〕

この発明の一実施例を第1図ないし第9図に基づいて説
明する。
An embodiment of the present invention will be described based on FIGS. 1 to 9.

第1図において、10はボビンであり、電線(図示せず
)を巻回する。また、11.12は円筒状に形成したフ
ェライト類のポットコアである。
In FIG. 1, 10 is a bobbin around which an electric wire (not shown) is wound. Further, 11 and 12 are ferrite pot cores formed into a cylindrical shape.

ポットコア11(第2図参照)およびポットコア12は
、共にボビン10内を通る内磁路13,15と、ボビン
10に外嵌する外磁路14,16とから構成されている
。内磁路13,15および外磁路14,16の互いの付
合せ面17.1B、19゜20は、それぞれ凸部21,
23,25.27と凹部22,24,26.28に周方
向に2分割されている。しかも、内磁路13,15の凸
部21゜23と外磁路14,16の凸部25.27は同
一側に位置し、かつ凹部22,24と凹部26,28も
同一側に位置している。
Both the pot core 11 (see FIG. 2) and the pot core 12 are composed of inner magnetic paths 13 and 15 passing through the bobbin 10 and outer magnetic paths 14 and 16 that are fitted onto the bobbin 10. The mating surfaces 17.1B, 19° 20 of the inner magnetic paths 13, 15 and the outer magnetic paths 14, 16 are formed by convex portions 21, 19, 20, respectively.
It is divided into two in the circumferential direction into recesses 23, 25 and 27 and recesses 22, 24 and 26 and 28. Furthermore, the convex portions 21, 23 of the inner magnetic paths 13, 15 and the convex portions 25, 27 of the outer magnetic paths 14, 16 are located on the same side, and the concave portions 22, 24 and the concave portions 26, 28 are also located on the same side. ing.

次に、第4図ないし第8図を用いて、ポットコア11.
12の回転による付合せ面17.18゜19.20の磁
束の変化について説明する。第4図および第5図は、ポ
ットコア11の凸部21゜25とポンドコア12の凸部
23.27どうしが完全に向き合った状態であり(回転
角度θ−〇。
Next, using FIGS. 4 to 8, pot core 11.
The change in the magnetic flux of the mating surfaces 17.18° and 19.20° due to the rotation of 12 will be explained. 4 and 5 show a state in which the convex portions 21.25 of the pot core 11 and the convex portions 23.27 of the pound core 12 are completely facing each other (rotation angle θ-〇).

)、第6図は第4図の状態から90度回転したIJ態で
あり(θ−90”)、第7図および第8図はポットコア
11の凸部21.25とポットコア12の凹部24,2
8どうしが完全に向き合った状態を示している(θ−1
80°)。磁気抵抗は磁性体間距離が小さいほど、対向
する面積が広いほど低くなるので、θ=0″の状態、θ
−90’の状態、θ=180@の状態の順に大きくなる
。また、インダクタンスは磁気抵抗とは逆の順序に高く
なる。
), FIG. 6 shows the IJ state rotated by 90 degrees from the state shown in FIG. 4 (θ-90''), and FIGS. 2
8 are completely facing each other (θ-1
80°). Magnetic resistance decreases as the distance between magnetic bodies decreases and as the opposing area increases, so when θ=0'', θ
It increases in the order of -90' state and θ=180@ state. Also, inductance increases in the opposite order to magnetic resistance.

このように構成された電磁装置によると、ポットコア1
1,12の内磁路13,15と外磁路14゜16の両方
の付合せ面17.18,19.20に凸部21,23,
25.27と凹部22,24゜26.28を形成したの
で、内磁路のみに凹凸部を形成した従来例に比べ、イン
ダクタンスの変化量が大きくなる。また、第19図に示
したような、内磁路と外磁路の凹凸部が逆に位置してい
る電磁装置に比べても、インダクタンスの変化量は太き
(なる。すなわち、第9図に示すように、横軸にポット
コアの相対的回転角度θを取り、縦軸にインダクタンス
の変化率ΔL/Lを取ると、第1図ないし第3図のよう
な内磁路13,15と外磁路14.16の凸部21,2
3,25.27どうしおよび凹部22,24,26.2
8どうしが同一側に位置している電磁装置は実線Aで示
すようになり、第19図ないし第21図のような内磁路
75゜76の凸部77.78ならびに凹部79,80が
外磁路67.68の凹部73,74ならびに凸部71.
72に対応している電磁装置は破線Bで示すようになる
。このグラフからも判るように、内磁IPI13.15
の凸部21.23および凹部22゜24を外磁路14.
16の凸部25.27および凹部26,2Bに対応させ
た方が、インダクタンスの変化量が大きくなる。以上の
ことから、広範囲にインダクタンスを可変可能な可変イ
ンダクタンス素子を実現でき、インダクタンス製造に伴
う部品のばらつきを吸収できる。また、インダクタンス
素子に接続される他部品(例えばコンデンサやトランジ
スタ等)のばらつきも、インダクタンス可変により補正
することができる。しかも、LC共振回路において、広
範囲な周波数特性の管理が可能となる。
According to the electromagnetic device configured in this way, the pot core 1
Convex portions 21, 23,
Since the concave portions 22, 24° and 26.28 are formed, the amount of change in inductance is larger than in the conventional example in which concave and convex portions are formed only in the inner magnetic path. Furthermore, compared to an electromagnetic device in which the concave and convex portions of the inner magnetic path and the outer magnetic path are located oppositely, as shown in FIG. 19, the amount of change in inductance is large (i.e. As shown in Figures 1 to 3, if the horizontal axis represents the relative rotation angle θ of the pot core, and the vertical axis represents the inductance change rate ΔL/L, the inner magnetic paths 13 and 15 and the outer magnetic paths as shown in Figures 1 to 3 are Convex portions 21, 2 of magnetic path 14.16
3, 25.27 and recesses 22, 24, 26.2
8 are located on the same side, as shown by the solid line A, and the convex portions 77, 78 and concave portions 79, 80 of the internal magnetic path 75° 76 as shown in FIGS. 19 to 21 are located on the outside. Concave portions 73, 74 and convex portions 71. of the magnetic paths 67, 68.
An electromagnetic device compatible with 72 is shown by a broken line B. As you can see from this graph, the internal magnetic IPI is 13.15.
The convex portions 21, 23 and concave portions 22, 24 of the outer magnetic path 14.
The amount of change in inductance becomes larger when the convex portions 25 and 27 and the concave portions 26 and 2B of No. 16 are made to correspond to each other. From the above, it is possible to realize a variable inductance element whose inductance can be varied over a wide range, and it is possible to absorb variations in components caused by inductance manufacturing. Furthermore, variations in other components (for example, capacitors, transistors, etc.) connected to the inductance element can also be corrected by varying the inductance. Furthermore, it is possible to manage a wide range of frequency characteristics in the LC resonant circuit.

この発明の他の実施例を、第10図および第11図に示
す。第10図の例のポットコア30は、内磁路31の付
合せ面33を4分割して、交互に凸部34と凹部35を
形成すると共に、外EfHIR39の付合せ面36も4
分割して交互に凸部37と凹部38を形成したものであ
り、内磁路31の凸部34の外側には外磁路39の凸部
37が位置し、内磁路31の凹部35の外側には外磁路
39の凹部38が位置している。
Other embodiments of the invention are shown in FIGS. 10 and 11. In the pot core 30 of the example shown in FIG. 10, the mating surface 33 of the inner magnetic path 31 is divided into four to form convex portions 34 and recessed portions 35 alternately, and the mating surface 36 of the outer EfHIR 39 is also divided into four parts.
The convex portions 37 and concave portions 38 are formed alternately by dividing the convex portion 37 of the outer magnetic path 39 to the outside of the convex portion 34 of the inner magnetic path 31, and the convex portion 37 of the outer magnetic path 39 is located outside the convex portion 34 of the inner magnetic path 31. A recess 38 of the outer magnetic path 39 is located on the outside.

また、第11図の例のポットコア40は、内磁路41と
外磁路44の付合せ面をそれぞれ6分割し、交互に凸部
42.45と四部43.46を形成したものであり、凸
部42.45および凹部43゜46どうしが対応してい
る。
Further, in the pot core 40 of the example shown in FIG. 11, the mating surfaces of the inner magnetic path 41 and the outer magnetic path 44 are each divided into six parts, and convex parts 42.45 and four parts 43.46 are formed alternately. The convex portions 42, 45 and the concave portions 43, 46 correspond to each other.

〔発明の効果〕〔Effect of the invention〕

この発明の電磁装置によると、一対のポットコアの内磁
路および外磁路の付合せ面に各々周方向に並んで凹凸部
が形成されている。しかも、内(n路の凸部の外側に外
磁路の凸部が位置し、かつ内磁路の凹部の外側に外磁路
の凹部が位置している。
According to the electromagnetic device of the present invention, the uneven portions are formed on the mating surfaces of the inner magnetic path and the outer magnetic path of the pair of pot cores, respectively, in line with the circumferential direction. Moreover, the convex portion of the outer magnetic path is located outside the convex portion of the inner (n path), and the concave portion of the outer magnetic path is located outside the concave portion of the inner magnetic path.

したがって、従来のように内磁路のみに凹凸部を形成し
たものや、内磁路と外磁路の各凹凸部が対応していない
ものに比べ、インダクタンスの可変量が増大するという
効果が得られる。
Therefore, the effect of increasing the variable amount of inductance is obtained compared to the conventional case in which unevenness is formed only in the inner magnetic path, or in which the unevenness in the inner magnetic path and outer magnetic path do not correspond to each other. It will be done.

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

第1図はこの発明の一実施例の分解斜視図、第2図はそ
のポンドコアの斜視図、第3図はそのポットコアの断面
図、第4図ないし第8図はそのポットコアどうしを相対
的に回転した状態の説明図、第9図はそのポットコアの
回転角度とインダクタンスの変化率の関係を示したグラ
フ、第1O図はこの発明の他の実施例のポットコアの斜
視図、第11図はこの発明のさらに他の実施例のポット
コアのP[有]図、第12図は従来例の斜視図、第13
図はそのポットコアの斜視図、第14図はそのポットコ
アの断面図、第15図ないし第18図はそのポットコア
どうしを相対的に回転した状態の説明図、第19図は提
案例の分解斜視図、第20図はそのポットコアの斜視図
、第21図はそのボンドコアの断面図、第22図ないし
第25図はそのポンドコアどうしを相対的に回転した状
態の説明図である。 10・・・ボビン、11.12・・・ポットコア、13
゜15・・・内磁路、14.16・・・外磁路、17,
18゜19.20・・・付合せ面、21,23,25.
27・・・凸部、22,24,26.28・・・凹部特
許出願人  松下電工株式会社 第 1 図 第6図 第7図     第80 第9図 第10図      第11図 第12図         第14図 第15図 第19図 第20図 第21図 第22図 第24図 第23図 第25図
Fig. 1 is an exploded perspective view of an embodiment of the present invention, Fig. 2 is a perspective view of its pond core, Fig. 3 is a sectional view of its pot core, and Figs. 4 to 8 show the pot cores relative to each other. FIG. 9 is a graph showing the relationship between the rotation angle of the pot core and the rate of change in inductance. FIG. 10 is a perspective view of a pot core according to another embodiment of the present invention. FIG. FIG. 12 is a perspective view of a conventional example, and FIG.
Figure 14 is a perspective view of the pot core, Figure 14 is a sectional view of the pot core, Figures 15 to 18 are illustrations of the pot cores rotated relative to each other, and Figure 19 is an exploded perspective view of the proposed example. , FIG. 20 is a perspective view of the pot core, FIG. 21 is a cross-sectional view of the bond core, and FIGS. 22 to 25 are illustrations of the pound cores rotated relative to each other. 10...Bobbin, 11.12...Pot core, 13
゜15...Inner magnetic path, 14.16...Outer magnetic path, 17,
18°19.20... mating surface, 21, 23, 25.
27... Convex portion, 22, 24, 26. 28... Concave portion Patent applicant Matsushita Electric Works Co., Ltd. Fig. 1 Fig. 6 Fig. 7 Fig. 80 Fig. 9 Fig. 10 Fig. 11 Fig. 12 Fig. 14 Figure 15 Figure 19 Figure 20 Figure 21 Figure 22 Figure 24 Figure 23 Figure 25

Claims (1)

【特許請求の範囲】[Claims] 電線を巻回したボビンと、このボビンに両端から挟んで
取付けられ内磁路および外磁路の付合せ面に各々周方向
に並んで凹凸部を形成した一対の筒状のポットコアとを
備えた電磁装置であって、前記内磁路の凸部の外側に前
記外磁路の凸部が位置し、かつ前記内磁路の凹部の外側
に前記外磁路の凹部が位置していることを特徴とする電
磁装置。
It is equipped with a bobbin around which electric wire is wound, and a pair of cylindrical pot cores that are attached to the bobbin from both ends and have concavities and convexities aligned in the circumferential direction on the mating surfaces of the inner magnetic path and the outer magnetic path, respectively. In the electromagnetic device, a convex portion of the outer magnetic path is located outside a convex portion of the inner magnetic path, and a concave portion of the outer magnetic path is located outside a concave portion of the internal magnetic path. Features an electromagnetic device.
JP7741988A 1988-03-28 1988-03-28 Electromagnetic device Pending JPH01246808A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7741988A JPH01246808A (en) 1988-03-28 1988-03-28 Electromagnetic device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7741988A JPH01246808A (en) 1988-03-28 1988-03-28 Electromagnetic device

Publications (1)

Publication Number Publication Date
JPH01246808A true JPH01246808A (en) 1989-10-02

Family

ID=13633437

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7741988A Pending JPH01246808A (en) 1988-03-28 1988-03-28 Electromagnetic device

Country Status (1)

Country Link
JP (1) JPH01246808A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08213245A (en) * 1995-02-02 1996-08-20 Nec Corp Variable inductance element
JP2017502507A (en) * 2013-12-04 2017-01-19 エプコス アクチエンゲゼルシャフトEpcos Ag Transducer device with adjusted inductance

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08213245A (en) * 1995-02-02 1996-08-20 Nec Corp Variable inductance element
JP2017502507A (en) * 2013-12-04 2017-01-19 エプコス アクチエンゲゼルシャフトEpcos Ag Transducer device with adjusted inductance

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