JPH03126204A - High frequency coil - Google Patents

High frequency coil

Info

Publication number
JPH03126204A
JPH03126204A JP26465889A JP26465889A JPH03126204A JP H03126204 A JPH03126204 A JP H03126204A JP 26465889 A JP26465889 A JP 26465889A JP 26465889 A JP26465889 A JP 26465889A JP H03126204 A JPH03126204 A JP H03126204A
Authority
JP
Japan
Prior art keywords
coil
foils
films
coils
frequency
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
JP26465889A
Other languages
Japanese (ja)
Inventor
Masao Hatami
播田実 正雄
Hiroaki Kobayashi
宏彰 小林
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP26465889A priority Critical patent/JPH03126204A/en
Publication of JPH03126204A publication Critical patent/JPH03126204A/en
Pending legal-status Critical Current

Links

Landscapes

  • Coils Or Transformers For Communication (AREA)

Abstract

PURPOSE:To suppress an increase in an effective resistance upon increase in a frequency and to increase a large current capacity by sequentially laminating substantially ringlike conductive films and insulating films in multiple layers, and connecting the conductive film ends in parallel. CONSTITUTION:For example, substantially rectangular copper foils 1a, 1b, 1c,..., and low dielectric constant insulating films 2a, 2b, 2c, ... are prepared. The foils 1a, 1b, 1c,... and the films 2a, 2b, 2c, ... are sequentially laminated, and integrated through adhesive or the like. The right and left ends of the foils 1a, 1b, 1c,... protrude from the right and left ends of the films 2a, 2b, 2c,.... Then, coils 7a, 7b are punched from the laminated multilayer board 9. The coils 7a, 7b are formed of substantially C-shaped rings 4a, 4b, legs 5a, 5b connected to the rings 4a, 4b, and terminals 6a, 6b made only of copper foils of the legs 5a, 5b, and the terminals 6a, 6b are integrally connected by soldering or the like. In this case, the substantially OMEGA-shaped coils 7a, 7b composed of the foils 1a, 1b, 1c are connected in parallel.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はスイッチングレギュレータ用トランスに用いて
好適な高周波コイルに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a high frequency coil suitable for use in a transformer for a switching regulator.

〔発明の概要〕[Summary of the invention]

本発明はスイッチングレギュレータ用トランスに用いて
好適な高周波コイルに関し、略リング状の導電性膜と絶
縁膜とを順次多層に積層し、リング状の導電性膜端末の
部分を並列接続させることで高周波化に伴う実効抵抗増
加を抑え、大電流容量化が同時に達成出来る様にしたも
のである。
The present invention relates to a high-frequency coil suitable for use in a transformer for a switching regulator.The present invention relates to a high-frequency coil suitable for use in a transformer for a switching regulator. This suppresses the increase in effective resistance that accompanies the increase in current capacity, and simultaneously achieves a large current capacity.

し従来の技術〕 従来からスイッチングレギュレータ用のトランスでは比
較的低電圧、大電流型のものが多く、然も高周波を扱う
ためにコア等に巻回するコイルのターン数は数百〜数十
ターンのものが多い。特に二次巻線ではそのターン数は
一次側とは逆にレギュレーションが最低の時を基準に設
定され、ターン数は数ターンで例えば、二次電流が10
A程度であればコイルの線径は2.3mm程度のものを
用いている。即ち、コアに巻回するコイルとして丸鋼単
線を使用し、電流許容量を上げるために線径を太くして
行くと、使用周波数帯域が上昇するにつれて、表皮効果
が無視出来なくなって来る。表皮効果は周波数が高くな
るにつれて、コイル導体に流れる電流が表面に集まり中
央部はど流れにくくなる現象で、表皮効果の大きさは次
式で与えられる。
Conventional technology] Traditionally, many of the transformers for switching regulators are relatively low voltage, high current types, and in order to handle high frequencies, the number of turns of the coil wound around the core etc. is several hundred to several tens of turns. There are many things. In particular, in the secondary winding, the number of turns is set based on the lowest regulation, contrary to the primary winding.
If it is about A, the wire diameter of the coil is about 2.3 mm. That is, when a round steel single wire is used as a coil wound around the core and the wire diameter is increased in order to increase the current capacity, the skin effect becomes impossible to ignore as the frequency band used increases. The skin effect is a phenomenon in which as the frequency increases, the current flowing through the coil conductor gathers at the surface and becomes difficult to flow through the center.The magnitude of the skin effect is given by the following equation.

ω・μ・k       ・・・・・・(1)ωは角周
波数(ω−2πf、 f :周波数)μは導体の透磁率 には導体の導電率 ここで、μ、には材料等が定まれば略一定であるので表
皮効果はωのみに依存するとみてよい。
ω・μ・k・・・・・・(1) ω is the angular frequency (ω-2πf, f: frequency) μ is the magnetic permeability of the conductor and the electrical conductivity of the conductor, where μ is determined by the material etc. If ω is approximately constant, it can be considered that the skin effect depends only on ω.

この様な表皮効果によって高周波では電流は導体の表面
だけにしか流れないので、コイルが有する抵抗分、即ち
銅損は増大する。そこで従来では銅損を少なくするため
に太い巻線を使用するか、更に高周波(VHF等の大電
力)になると、表面に銀鍍金を施したパイプ状の導線や
細い撚線を集めた導線を用いていた。
Due to such skin effect, current flows only on the surface of the conductor at high frequencies, so the resistance of the coil, ie, copper loss, increases. Therefore, in the past, thick winding wires were used to reduce copper loss, or, for higher frequencies (high power such as VHF), pipe-shaped conductors with silver plating on the surface or conductors made of thin stranded wires were used. I was using it.

更に、特開昭60−39743号公報に示されている様
に薄板状のフレキシブルプリント板上にコイルパターン
を一方向に順次に形成し、このフレキシブルプリント板
の対を重ね合せて筒状に形成したコイル等も知られてい
る。
Furthermore, as shown in Japanese Patent Application Laid-Open No. 60-39743, a coil pattern is sequentially formed in one direction on a thin flexible printed board, and a pair of the flexible printed boards are overlapped to form a cylindrical shape. Coils and the like are also known.

δ=(ω・μ・k)−*   ・・・・・・(2)で表
すことが出来る。例えば、ω=2πfの周波数f=IM
Hzの銅線の表皮深さδ=66μmで、これ以上の内部
では電流が流れなくなり、実効抵抗が増加する。即ち周
波数fの上昇と共に銅損が増加し、スイッチングレギュ
レータの二次巻線の様に大電流容量化と高周波化(例え
ばM Hz帯)に対応させる両立化が困難となる問題が
あった。
It can be expressed as δ=(ω・μ・k)−* (2). For example, the frequency f=IM of ω=2πf
When the skin depth δ of the Hz copper wire is 66 μm, current no longer flows inside the wire and the effective resistance increases. That is, as the frequency f increases, copper loss increases, and there is a problem in that it is difficult to simultaneously handle a large current capacity and a high frequency (for example, MHz band), as in the case of the secondary winding of a switching regulator.

本発明は叙上の問題点を解決するために成されたもので
、その目的とするところは高周波化に伴う実効抵抗増加
を抑え、大電流容量化が出来る高周波コイルを得る様に
したものである。
The present invention was made in order to solve the above-mentioned problems, and its purpose is to suppress the increase in effective resistance that accompanies higher frequencies and to obtain a high-frequency coil that can increase the current capacity. be.

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

コイルを形成した導体に上記した(1)式の大きさの表
皮効果が生じた場合に電流が導線の表面に集中する深さ
δは表皮効果の大きさを表す量であるから 〔課題を解決するための手段〕 本発明の高周波コイルはその例が第1図A、B。
When a skin effect with the magnitude of equation (1) above occurs in a conductor that forms a coil, the depth δ at which the current concentrates on the surface of the conductor is a quantity that represents the magnitude of the skin effect. Examples of the high-frequency coil of the present invention are shown in FIGS. 1A and 1B.

Cに示されている様に略リング状(4a) (4b)の
導電性膜(la) (lb) (lc)と絶縁膜(2a
) (2b) (2c) (2d)とを順次多層に積層
し、リング状(4a) (4b)の導電性膜の端末(6
a) (6b)の部分を並列接続して成るものである。
As shown in C, approximately ring-shaped (4a) (4b) conductive films (la) (lb) (lc) and insulating films (2a)
) (2b) (2c) (2d) are sequentially stacked in multiple layers to form terminals (6) of ring-shaped conductive films (4a) (4b).
a) This is made by connecting the parts in (6b) in parallel.

〔作用〕[Effect]

本発明の高周波コイルは表皮効果による表皮深さδ程度
の厚さの導電性膜と絶縁膜を交互にラミネートし、リン
グ状の1ターンコイルを形成しその端末を並列接続させ
たので高周波化に伴う表皮効果の影響を抑え、高周波領
域の低損失化と、大電流容量化を達成することが出来る
The high-frequency coil of the present invention is made by alternately laminating conductive films and insulating films with a thickness of about the skin depth δ due to the skin effect, forming a ring-shaped one-turn coil, and connecting the terminals in parallel, making it suitable for high frequencies. It is possible to suppress the influence of the accompanying skin effect and achieve low loss in the high frequency range and large current capacity.

〔実施例〕〔Example〕

以下、本発明の高周波コイルの一実施例を第1図及び第
2図について説明する。
An embodiment of the high frequency coil of the present invention will be described below with reference to FIGS. 1 and 2.

第1図A、B、Cは本発明の高周波コイルの形成工程を
説明するための説明図である。先ず第1図への様に、例
えば略長方形状の銅箔(la) (lb)(IC)・・
・・と、低誘導率の絶縁膜(2a) (2b) (2c
)・・・・を用意する。銅箔(la) (ib) (l
c)は第2式で示したδ−(ω・μ・k)−yの表皮効
果深さδ程度の厚さを有する。例えば、周aL]c f
がl M)Izでは60μm、5 MHzでは20 μ
m程度である。絶縁膜(2a) (2b)(2C)・・
・・は例えば、銅箔(la) (lb) (lc)・・
・・よりその左右端が小さく形成されている。この様な
銅箔(la) (lb) (lc) ・−・・と絶縁膜
(2a) (2b) (2c) = =を第1図已に示
すように順次ラミネートして、接着剤等を介して一体化
すると、銅箔(la) (lb) (lc)の左右端は
絶縁膜(2a) (2b) (2c)・・・・の左右端
より突出する。次に第1図Cの平面図に示す様に、ラミ
ネートされた多層板(9)からコイル(7a) (7b
)を打ち抜く、コイル(7a) (7’b)は略C状の
リング!(4a) (4b)とこのリング部(4a) 
(4b)に連通ずる脚部(5a) (5b)並にこの脚
部(5a) (5b)の銅箔だけよりなる端末(6a)
 (6b)より形成され、この端末(6a) (6b)
は半田等で一体に接続する。この場合各銅箔(la) 
(To)(IC)で構成した略Ω状のコイル(7a) 
(7b)は並列的に接続される。この様に打ち抜かれた
例えばコイル(7a)をスイッチングレキ−レータ用ト
ランスの二次巻線として用いるには第2囚人に示す様に
、例えば下側のE型コア(8a)の溝(10a) (1
0b)の底にコイル(7a)のC状のリング部(4a)
を充分深く沈め、このコイル(7a)の面に垂直に入射
する漏れ磁束(11) (第2図Bの組立断面参照)を
避ける様にすれば漏れ磁束(11)による渦電流損失も
抑えることが出来る。次に上側のE型コアを下側のE型
コアの上に乗せ一体化して、−次巻線等を巻回して、ス
イッチングレギュレータ用のトランスを構成させる。
FIGS. 1A, B, and C are explanatory diagrams for explaining the process of forming a high-frequency coil according to the present invention. First, as shown in Figure 1, for example, approximately rectangular copper foil (LA) (LB) (IC)...
...and low conductivity insulating films (2a) (2b) (2c
)... Prepare. Copper foil (la) (ib) (l
c) has a thickness of approximately the skin effect depth δ of δ−(ω·μ·k)−y shown in the second equation. For example, circumference aL] c f
is 60 μm at Iz and 20 μm at 5 MHz.
It is about m. Insulating film (2a) (2b) (2C)...
For example, copper foil (LA) (LB) (LC)...
...The left and right ends are smaller. Laminate such copper foils (la) (lb) (lc) ... and insulating films (2a) (2b) (2c) = = in sequence as shown in Figure 1, and apply adhesive etc. When integrated through the insulating films (2a), (2b), (2c), the left and right ends of the copper foils (la), (lb, and lc) protrude from the left and right ends of the insulating films (2a), (2b), (2c), and so on. Next, as shown in the plan view of Fig. 1C, coils (7a) (7b
) is punched out, the coil (7a) (7'b) is a substantially C-shaped ring! (4a) (4b) and this ring part (4a)
Legs (5a) (5b) communicating with (4b) and terminals (6a) made of only copper foil of these legs (5a) (5b)
(6b) and this terminal (6a) (6b)
are connected together with solder, etc. In this case each copper foil (la)
Approximately Ω-shaped coil (7a) composed of (To) (IC)
(7b) are connected in parallel. In order to use the thus punched coil (7a) as the secondary winding of a transformer for a switching regulator, for example, the groove (10a) of the lower E-shaped core (8a) must be cut out as shown in the second prisoner. (1
C-shaped ring part (4a) of the coil (7a) on the bottom of the coil (7a)
Eddy current loss due to leakage magnetic flux (11) can also be suppressed by sinking the coil (7a) sufficiently deeply to avoid leakage magnetic flux (11) that is incident perpendicularly to the surface of this coil (7a) (see assembled cross section in Figure 2B). I can do it. Next, the upper E-type core is placed on the lower E-type core and integrated, and the -order winding etc. are wound to form a transformer for a switching regulator.

この崖に構成された本例の高周波コイルによれば高周波
化に伴うコイルの実効抵抗(銅損)増加が少なくなり、
大電流容量に対応出来るので、スイッチングレギュレー
タ用のトランスの二次巻線の様に高周波、大電流容量の
ものでも高効率のトランスを得ることが出来る。
According to the high-frequency coil of this example configured on this cliff, the increase in effective resistance (copper loss) of the coil due to higher frequencies is reduced,
Since it can handle large current capacity, it is possible to obtain a highly efficient transformer even with high frequency and large current capacity, such as the secondary winding of a transformer for a switching regulator.

上述の実施例は1ターンのコイル(7a) (7b)に
ついて説明したが、第3図及び第4図で複数ターンの高
周波コイルの成形方法を説明する。第3図A。
In the above embodiment, the coils (7a) and (7b) each having one turn were explained, but a method for forming a high frequency coil having multiple turns will be explained with reference to FIGS. 3 and 4. Figure 3A.

B、Cは例えば2ターンの高周波コイルの形成方法を説
明するためのパターン説明図である。
B and C are pattern explanatory diagrams for explaining a method of forming, for example, a two-turn high-frequency coil.

この様なパターンを得るためには第1図A、 Bで説明
したと同様に銅箔(la) (lb) (lc)・・・
・と絶縁膜(2a) (2b) (2c)・・・・とを
ラミネートして一体化した多層板(9)を形成し、第3
図A、B並にCに示す様なパターンの第1乃至第3のコ
イル(12a) (12b)(12C)を打ち抜き形成
する。
In order to obtain such a pattern, copper foil (la) (lb) (lc)...
and the insulating films (2a), (2b), (2c), etc. are laminated to form an integrated multilayer board (9), and the third
First to third coils (12a), (12b), and (12C) having patterns as shown in Figures A, B, and C are punched out.

第1のコイル(12a)  は第3図Aに示す様に、略
C状のリング部(14a)  とこのリンク部(14a
)  の−端に連通ずる1本の脚部(13a)  と、
この脚部(13a)の端部に構成された銅箔だけでなり
複数銅箔が半田付され並列接続された端末(15a) 
 並にリング部(14a)  他側端に形成された中間
端子部(16a)  より構成されている。第2のコイ
ル(12b)  は13図Bに示す様に略C型のリング
部(14b)  の両側端に中間端子I(16b) (
16c)が形成され、更に第3のコイル(12c)  
は第3図Cに示す様に略半円状の半リング部(14c)
  と、この半リング部(14c)  の一端に連通ず
る1本の脚部(13b)  と、この脚部(13b) 
 の端部に構成された銅箔だけでなり、複数銅箔が半田
付されて並列接続された端末(15b) 並に半リング
8 (14c)他側端に形成された中間端子部(Ill
id)  より構成されている。この様に多層板(9)
から打ち抜かれた第1乃至第3のコイル(12a) (
12b) (12C)  はリング部(14a) (1
4b)及び半リング部(14C)  の中心○6,02
及び0.を中心にして第4図の様に積み重ねられる。そ
して第1のコイル(12a)  の中間端子部(16a
)  と第2のコイル(12b)  の中間端子部(1
6c) がスルホール加工と同様の方法で各銅箔(la
) (lb)・・・・間が互いに並列接合される。同様
に第2のコイル(12b)  と第3のコイル(12c
)  の中間端子部(16b)  と(16d)  と
が同じくスルホール加工と同様の方法で互に各銅箔(l
a) (lb)・・・・間が互に並列接続する様に一体
化される。上述の例では端末(15a) (15b)を
銅箔だけで構成するものについて説明したが、第4図の
様にこの部分も絶縁膜と銅箔を交互にラミネートシ、ス
ルホールを穿って、各銅箔(la) (lb)間を互に
並列接続する様にしてもよい。尚、第4図で(17a)
 (17b) (17c)  はスルホールに半田を充
填して中間端子部(16a)及び(16c)(16e)
及び(16d)並に端末(15a)或は(15b) の
銅箔(la) (lb)・・・・を一体化したものを示
している。
As shown in FIG. 3A, the first coil (12a) has a substantially C-shaped ring part (14a) and this link part (14a
) one leg (13a) communicating with the - end of the
A terminal (15a) consisting only of copper foil is formed at the end of this leg (13a), and a plurality of copper foils are soldered and connected in parallel.
It also includes a ring portion (14a) and an intermediate terminal portion (16a) formed at the other end. The second coil (12b) has intermediate terminals I (16b) (
16c) is formed, and a third coil (12c) is formed.
As shown in Fig. 3C, there is a semicircular half ring part (14c).
, one leg (13b) communicating with one end of this half ring part (14c), and this leg (13b)
There is a terminal (15b) consisting of only copper foil formed on the end of the ring, and a plurality of copper foils are soldered and connected in parallel, and a half ring 8 (14c).
id). Multilayer board like this (9)
The first to third coils (12a) punched from (
12b) (12C) is the ring part (14a) (1
4b) and the center of the half ring part (14C)○6,02
and 0. They are stacked as shown in Figure 4 with . and the intermediate terminal portion (16a) of the first coil (12a).
) and the intermediate terminal part (1) of the second coil (12b)
6c) Each copper foil (la
) (lb)... are connected in parallel to each other. Similarly, the second coil (12b) and the third coil (12c
) The intermediate terminal portions (16b) and (16d) of each copper foil (l
a) (lb)... are integrated so that they are connected in parallel with each other. In the above example, the terminals (15a) and (15b) were made of copper foil only, but as shown in Figure 4, this part is also laminated with an insulating film and copper foil alternately, and through holes are drilled in each part. The copper foils (la) and (lb) may be connected in parallel. In addition, in Figure 4 (17a)
(17b) (17c) Fill the through holes with solder and connect the intermediate terminal parts (16a) and (16c) (16e).
(16d) and the terminal (15a) or (15b) copper foil (la) (lb)... are shown integrated.

上述と同様の方法で3タ一ン以上の複数ターンの高周波
コイルを容易に得ることが出来る。
A high frequency coil with multiple turns of three or more turns can be easily obtained by the same method as described above.

本例は、スイッチングレギュレータ用のトランスの二次
コイルとして用いることで高能率なトランスを得ること
が出来る。
By using this example as a secondary coil of a transformer for a switching regulator, a highly efficient transformer can be obtained.

尚、上述例はスイッチングレギュレータ用のトランスの
高周波コイルとして説明したが、その用途はスイッチン
グレギュレータ用のトランスに限定され、るものでなく
、種々の高周波用コイルに利用出来る。又、多層板(9
)の製造方法も銅箔(1a)(lb) (lc)と絶縁
膜(2a) (2b) (2c) (2d)のラミネー
トに限定されることなく例えば、フレキシブルプリント
基板にパターニングされた略C状のコイル部をラミネー
トしたものを用いることも出来る等、本発明の要旨を逸
脱しない範囲で種々変更し得ることは明白である。
In addition, although the above-mentioned example was explained as a high frequency coil of a transformer for a switching regulator, its use is not limited to a transformer for a switching regulator, and can be used for various high frequency coils. Also, multilayer board (9
) is not limited to the laminate of copper foil (1a) (lb) (lc) and insulating film (2a) (2b) (2c) (2d). It is obvious that various modifications can be made without departing from the spirit of the present invention, such as the use of laminated coil portions.

〔発明の効果〕〔Effect of the invention〕

本発明によれば表皮効果の影響を抑え、高周波域で損失
の少ない、大電流容量の高周波コイルが得られる。
According to the present invention, it is possible to obtain a high-frequency coil that suppresses the influence of the skin effect, has low loss in the high-frequency range, and has a large current capacity.

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

第1図は本発明の高周波コイルの形成工程の説明図、第
2図は高周波コイルの組立状態図、第3図は本発明の高
周波コイルの他の実施例を示すコイルパターン図、第4
図は本発明の高周波コイルの池の実施例を示す組立側断
面図である。 (la) (lb) (lc)は銅箔、(2a) (2
b) (2c) (2d) f′!絶縁膜、(4a) 
(4b)はリング部、(7a) (7b)はコイル、(
9)は多層板、(8a) (8b)はE型コアである。 代 理 人 松 隈 秀 盛 91層板 本分明の高側渓コイ1しのガンA′玉8説り月圀第1図 20− $、定6月の高周波コイルしの碧]立イ人階化ろ第2図 木茫e月の高同及コイlしのイt!!n寅かと例と示す
コイIしへ°ターンBり本発明の市月j反コイJしのイ
亡の突7さ汀]乞示厚1且立押“珀斤屓汀口第4図
FIG. 1 is an explanatory diagram of the formation process of the high-frequency coil of the present invention, FIG. 2 is an assembly state diagram of the high-frequency coil, FIG. 3 is a coil pattern diagram showing another embodiment of the high-frequency coil of the present invention, and FIG.
The figure is an assembled side cross-sectional view showing an embodiment of the high-frequency coil pond of the present invention. (la) (lb) (lc) is copper foil, (2a) (2
b) (2c) (2d) f'! Insulating film, (4a)
(4b) is the ring part, (7a) (7b) is the coil, (
9) is a multilayer board, and (8a) and (8b) are E-type cores. Agent Hidemori Matsukuma 91-layer board Honbunmei's high side carp 1 gun A'ball 8 theory Tsukikuni 1st figure 20 - $, fixed June's high frequency coil Shino Aoi] Standing person floor stage 2nd map of the month of the month of high school and high school! ! n tiger or example carp I turn B turn the market of the present invention against carp

Claims (1)

【特許請求の範囲】[Claims]  略リング状の導電性膜と絶縁膜とを順次多層に積層し
、該リング状の導電性膜端末を並列接続して成ることを
特徴とする高周波コイル。
A high-frequency coil characterized in that a substantially ring-shaped conductive film and an insulating film are successively laminated in multiple layers, and terminals of the ring-shaped conductive films are connected in parallel.
JP26465889A 1989-10-11 1989-10-11 High frequency coil Pending JPH03126204A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26465889A JPH03126204A (en) 1989-10-11 1989-10-11 High frequency coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26465889A JPH03126204A (en) 1989-10-11 1989-10-11 High frequency coil

Publications (1)

Publication Number Publication Date
JPH03126204A true JPH03126204A (en) 1991-05-29

Family

ID=17406413

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26465889A Pending JPH03126204A (en) 1989-10-11 1989-10-11 High frequency coil

Country Status (1)

Country Link
JP (1) JPH03126204A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5578981A (en) * 1992-05-08 1996-11-26 Murata Manufacturing Co., Ltd. Laminated inductor
US6404317B1 (en) * 1990-05-31 2002-06-11 Kabushiki Kaisha Toshiba Planar magnetic element
JP2003510808A (en) * 1999-09-22 2003-03-18 エリクソン インコーポレイテッド Split inductor with partial winding in each winding and PCB containing the inductor
JP2009105159A (en) * 2007-10-22 2009-05-14 Tokyo Coil Engineering Kk Coil structure for inductor, and the inductor
JP2019149535A (en) * 2018-02-27 2019-09-05 国立大学法人信州大学 Inductor

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6404317B1 (en) * 1990-05-31 2002-06-11 Kabushiki Kaisha Toshiba Planar magnetic element
US5578981A (en) * 1992-05-08 1996-11-26 Murata Manufacturing Co., Ltd. Laminated inductor
JP2003510808A (en) * 1999-09-22 2003-03-18 エリクソン インコーポレイテッド Split inductor with partial winding in each winding and PCB containing the inductor
JP2009105159A (en) * 2007-10-22 2009-05-14 Tokyo Coil Engineering Kk Coil structure for inductor, and the inductor
JP2019149535A (en) * 2018-02-27 2019-09-05 国立大学法人信州大学 Inductor
JP2022172333A (en) * 2018-02-27 2022-11-15 国立大学法人信州大学 inductor

Similar Documents

Publication Publication Date Title
US6867678B2 (en) Transformer structure
CA2150953C (en) Flexible transformer apparatus particularly adapted for high voltage operation
US4201965A (en) Inductance fabricated on a metal base printed circuit board
EP0547120B1 (en) Power transformers and coupled inductors with optimum interleaving of windings
US4755783A (en) Inductive devices for printed wiring boards
US6577220B2 (en) Continuous multi-turn coils
EP0267108A1 (en) Miniaturized transformer
JP2008021788A (en) Multilayer inductor
KR101838225B1 (en) Double core planar transformer
JPH07263258A (en) Transformer
JP2770750B2 (en) Inductance element
KR100299893B1 (en) Transformer
US20030234436A1 (en) Semiconductor device with a spiral inductor and magnetic material
WO2017197550A1 (en) Electromagnetic induction device and manufacturing method therefor
KR101838227B1 (en) Common winding wire planar transformer
JPH056829A (en) Thin transformer
CN205542318U (en) Transformer winding and transformer based on flexible circuit board
JPH03126204A (en) High frequency coil
JPH10163039A (en) Thin transformer
JP2007317892A (en) Multilayered inductor
JPH06215962A (en) Transformer
Quilici Embedded magnetic power transformer
US7113066B2 (en) Electronic inductive and capacitive component
JPH03280409A (en) Flat transformer
JPH0227533Y2 (en)