JPS62101010A - Printed coil - Google Patents
Printed coilInfo
- Publication number
- JPS62101010A JPS62101010A JP24247285A JP24247285A JPS62101010A JP S62101010 A JPS62101010 A JP S62101010A JP 24247285 A JP24247285 A JP 24247285A JP 24247285 A JP24247285 A JP 24247285A JP S62101010 A JPS62101010 A JP S62101010A
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- spiral
- coil
- printed
- printed coil
- 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
Links
Abstract
Description
【発明の詳細な説明】
(発明の分野)
本発明は、これまで実用化が困難とされCいた誘電体基
板の表面に導体を固着させ〔なるプリントコイルに関す
る。DETAILED DESCRIPTION OF THE INVENTION (Field of the Invention) The present invention relates to a printed coil in which a conductor is fixed to the surface of a dielectric substrate, which has hitherto been considered difficult to put into practical use.
(従来の技術)
従来より、絶縁体基板ないし磁性体基板等の一方の表面
に渦巻形状な(八しジグザグ形状の導体を固着させ°C
なるブリイトコイルがある。(Prior art) Conventionally, a spiral-shaped (or zigzag-shaped conductor) is fixed to one surface of an insulating substrate or a magnetic substrate.
There is a Britcoil.
第4図(A) $−よび(B)は絶縁体基板の一方の表
面に渦巻形状の導体を固着させCなる従来のプリントコ
イルである。ただし、第4図(A)は平面図、第4図C
B)はその鎖線A=−A’ 部分の側断面図である。FIGS. 4(A) and 4(B) are conventional printed coils having a spiral conductor fixed to one surface of an insulating substrate. However, Fig. 4(A) is a plan view, Fig. 4C
B) is a side sectional view of the portion indicated by the chain line A=-A'.
このプリントコイルにおいC,1はセラミックスや樹脂
等からなる絶縁体基板である。2は渦巻形状の導体であ
り、絶縁体基板1の一方の表面に、導体ペーストを印刷
するなどの方法によつ゛C固着され°Cいる。このプリ
ントコイルは、導体2の一方の端部2aと他方の端部2
bとの間に所望のインダクタンス値を得ることができる
。In this printed coil, C,1 is an insulating substrate made of ceramics, resin, or the like. A spiral conductor 2 is fixed to one surface of the insulating substrate 1 by a method such as printing a conductive paste. This printed coil consists of one end 2a of the conductor 2 and the other end 2a of the conductor 2.
A desired inductance value can be obtained between the inductance and b.
また、従来よシ、絶縁体基板な(八し磁性体基板等の両
方の表面に渦巻形状ないしジグザグ形状の導体を固着さ
せCなるプリントコイルがある。Furthermore, conventionally, there is a printed coil (C) in which a spiral or zigzag conductor is fixed to both surfaces of an insulating substrate (eg, a magnetic substrate).
第5図(A)から<C)は、絶縁体基板の両方の表面に
渦巻形状の導体を固着させCなる従来のプリントコイル
である。ただし、第5図(A)は平面図、第5図(B)
はその鎖線B −B’部分の側断面図、第5図(C)は
底面図である。このプリントコイルにおいて、6はセラ
ミックスや樹脂等からなる絶縁体基板である。4は絶縁
体基板6を頁通し゛C形成されたスルーホールである。FIGS. 5A to 5C show conventional printed coils C in which spiral conductors are fixed to both surfaces of an insulating substrate. However, Figure 5 (A) is a plan view, Figure 5 (B)
is a side sectional view taken along the chain line B-B', and FIG. 5(C) is a bottom view. In this printed coil, 6 is an insulating substrate made of ceramics, resin, or the like. Reference numeral 4 denotes a through hole formed through the insulating substrate 6.
5は渦巻形状の導体であり、絶縁体基板6の両方の表面
に導体ペーストを印刷する等の方法によつ゛C固着され
′〔おり、一方の表面の渦巻形状と他方の表面の渦巻形
状とはスルーホール4を介し゛C電気的に接続され°C
いる。このプリントコイルは、導体5の絶縁本基板6の
一方の表面の渦巻形形状の端部5aと、他方の表面の渦
巻形状の端部5bとの間に所望のインダクタンス値を得
ることができる。Reference numeral 5 denotes a spiral-shaped conductor, which is fixed to both surfaces of the insulating substrate 6 by a method such as printing conductor paste, and has a spiral shape on one surface and a spiral shape on the other surface. is electrically connected to °C through through hole 4.
There is. This printed coil can obtain a desired inductance value between the spiral-shaped end 5a on one surface of the insulating main substrate 6 of the conductor 5 and the spiral-shaped end 5b on the other surface.
上述した2つの従来のプリントコイルは、絶縁体基板1
ないし6の代わりに磁性体基板等を用1^°Cも、同様
のプリントコイルを形成することができる。また、渦巻
形状の導体2ないし5の代わりにジグザグ形状の導体を
固着させ′Cも、同様のプリントコイルを形成すること
ができる。The two conventional printed coils mentioned above have an insulator substrate 1
A similar printed coil can be formed at 1^°C by using a magnetic substrate or the like instead of 6 to 6. Further, a similar printed coil can also be formed by fixing a zigzag-shaped conductor in place of the spiral-shaped conductors 2 to 5.
(発明の解決しようとする問題点)
しかしながら、誘遊体基板の表面に渦巻形状ないしジグ
ザグ形状の導体分固着させCなるプリントコイルは、以
下の理由によつC1これまで実用化が困難とされ〔いた
。(Problems to be Solved by the Invention) However, it has been difficult to put into practical use C1, which is a printed coil in which a spiral or zigzag conductor is fixed to the surface of a dielectric substrate, for the following reasons. there was.
すなわち、基板の表面に渦巻形状ないしジグザグ形状の
導体を固着させCなるプリントコイルの等価回路は、第
6図のように表わすことができる。That is, the equivalent circuit of a printed coil C in which a spiral or zigzag conductor is fixed to the surface of a substrate can be expressed as shown in FIG.
これは、基板の7方の表面に導体を固着さすたプリント
コイルの場合、導体の線間に浮遊容量Cpが入るため、
また基板の両方の表面に導体を固着させたプリントコイ
ルの場合、導体の線間、および一方の表面の導体と他方
の表面の導体との間に浮遊容量Cpが入るためである。This is because in the case of a printed coil with conductors fixed to seven surfaces of the board, there is stray capacitance Cp between the conductor lines.
Further, in the case of a printed coil in which conductors are fixed to both surfaces of the substrate, stray capacitance Cp occurs between the conductor lines and between the conductor on one surface and the conductor on the other surface.
基板とし′C絶縁体基板や磁性体基板を用いた場合、浮
遊容量Cpは小さいが、誘電体基板を用いると、浮遊容
量cpは当然のことながら非常に大きくなる。自己共振
周波数10は、
であるから、誘電体基板を用いることによつC浮遊容量
cpが大きくなると、自己共振周波数f0は低下しCし
まう。このプリントコイルは、自己共振周波数よりも高
い周波数ではコイルとし°C機−止せずコノデンサとし
°C機能しCしまうから、誘電体基板を用いることによ
つC自己共振周波数f0が低下すると、周波数特性が劣
下し・Cしまう。When a C insulator substrate or a magnetic substrate is used as the substrate, the stray capacitance Cp is small, but when a dielectric substrate is used, the stray capacitance Cp naturally becomes very large. The self-resonant frequency 10 is as follows. Therefore, when the C stray capacitance cp increases due to the use of a dielectric substrate, the self-resonant frequency f0 decreases and becomes C. This printed coil does not function as a coil at frequencies higher than the self-resonant frequency, but instead functions as a conode. Therefore, when the self-resonant frequency f0 is lowered by using a dielectric substrate, the frequency Characteristics deteriorate and C is removed.
つまり、誘電体基板の表面に渦巻形状ないしジグザグ形
状の導体を固着させCなるプリントコイルは、浮遊容量
Cpが大きいことにより、自己共振周波数f。が低く、
周波数特性が悪いため、実用化が困難だったのである。In other words, a printed coil C in which a spiral or zigzag conductor is fixed to the surface of a dielectric substrate has a self-resonant frequency f due to a large stray capacitance Cp. is low;
Its poor frequency characteristics made it difficult to put it into practical use.
これまで、比誘電率が20以上の誘電体基板の表面知渦
巻形状ないしジグザグ形状の導体を固着させ°Cなるプ
リントコイルは、はとんど実用化され′Cいない。Until now, printed coils made by fixing spiral or zigzag conductors on the surface of a dielectric substrate having a dielectric constant of 20 or more have hardly been put to practical use.
しかしながら、誘電体基板を用1八たLC複合部品等に
おlへ’(は、誘電体基板の表面にプリントコイルを形
成することが強く望゛まれ“Cいる。However, when a dielectric substrate is used for LC composite parts, etc., it is strongly desired to form a printed coil on the surface of the dielectric substrate.
(問題点を解決するだめの手段)
本発明は、これまで実用化が困難とされ゛〔いた、誘電
体基板の表面に渦巻形状な(八しジグザグ形状の導体を
固着させ°Cなるプリントコイルの実用化を目的とする
。(Means for Solving the Problems) The present invention is a printed coil that fixes a spiral (8-zigzag) conductor on the surface of a dielectric substrate, which has hitherto been difficult to put into practical use. The purpose is to put it into practical use.
その手段としC本発明のプリントコイルは、2個以上の
渦巻形状なl、−LLジグザグ形状を直列に接続した導
体を、誘電体基板の表面に固着させるようにした。すな
わち本発明のプリントコイルは、所望のインダクタンス
値を連続した1個の渦枠形状な(八しジグザグ形状の導
体によつ゛C形成するのではなく、直列に接続された2
個以上の渦巻形状な(八しジグザグ形状の導体に分割し
゛〔形成するようにしたのである。As a means for achieving this, the printed coil of the present invention has a conductor in which two or more spiral-shaped 1, -LL zigzag shapes are connected in series, and is fixed to the surface of a dielectric substrate. That is, in the printed coil of the present invention, a desired inductance value is not formed by one continuous vortex frame-shaped (or zigzag-shaped conductor), but by two conductors connected in series.
The conductor was divided into eight or more spiral-shaped (or zigzag-shaped) conductors.
たとえば、所望のインダクタンス値りを2個の渦巻形状
ないしジグザグ形状の導体からなる第1コイル部と第2
コイル部とに2等分割しC形成した場合、その等価回路
は第7図に示すようになる。For example, a desired inductance value can be obtained by connecting a first coil portion and a second coil portion each consisting of two spiral or zigzag conductors.
When the coil portion is equally divided into two parts to form a C, the equivalent circuit is shown in FIG.
ただし、Llは第1コイル部のインダクタンス値、L2
は第2コイル部のインダクタンス1直(L=L。However, Ll is the inductance value of the first coil section, L2
is the inductance of the second coil section (L=L).
+L2)、CpIは第1コイル部の浮遊容量、CF2は
第2コイル部の浮遊容量である。+L2), CpI is the stray capacitance of the first coil section, and CF2 is the stray capacitance of the second coil section.
ところで、このプリントコイルに総合的に入る浮遊容量
Cpと、インダクタンス値りを連続した1個の渦巻形状
ないしジグザグ形状の導体によつC形成したプリントコ
イルに入る浮遊容量Caとを比較すると、次のようにな
る。まず、インダクタンス値りを第1コイル部と第2コ
イル部とに2等分割しC形成すると、それぞれのコイル
部の導体の大きさは1個の導体で形成した場合の約%沈
なるため、浮遊容量(:、 plおよびCptは浮遊容
量Caの約!イになつCいる。一方、浮遊、g計Cpは
浮遊容量CplとCp、とを直列に接続したものである
が、同じ大きさの容量を2個直列に接続すると容量はイ
になるから、浮遊容−1cpは浮遊容量Cp、およ’0
” plの%になつCいる。したがつC1このプリント
コイルに総合的に入る浮遊容量CpI/′i、インダク
タンス値りを連続した1個の渦巻形状ないしジグザグ形
状の導体によつ′C形成したプリントコイルに入る浮遊
容tCaの約イになつCいる。By the way, if we compare the total stray capacitance Cp that enters this printed coil with the stray capacitance Ca that enters the printed coil whose inductance value is formed by a continuous spiral or zigzag conductor, we get the following. become that way. First, if the inductance value is divided into two equal parts, the first coil part and the second coil part, forming a C, the size of the conductor in each coil part will be about % smaller than if it were formed with one conductor. Stray capacitance (:, pl and Cpt are approximately equal to the stray capacitance Ca. On the other hand, the stray capacitance Cp is a series connection of the stray capacitances Cpl and Cp, but they have the same size) If two capacitors are connected in series, the capacitance becomes A, so the stray capacitance -1cp is the stray capacitance Cp, and '0
"C is % of pl. Therefore, C1 is the stray capacitance CpI/'i that enters this printed coil as a whole, and the inductance value is formed by one continuous spiral or zigzag conductor. The floating capacitance tCa entering the printed coil is approximately A.
つ−まり、本発明のプリントコイルは、所望のインダク
タンス値りを直列に接続された2個以上の渦巻形状ない
しジグザグ形状の導体に分割しC形成することによつご
、基板として誘電体基板を使用しCいるにもかかわらず
、浮遊容gapを極めC小さくおさえることが可能にな
つ′Cいる。したがつC1自己共撮周波数foの低下を
防上することができ、周波数特性が改善されCいる。In other words, the printed coil of the present invention is produced by dividing a desired inductance value into two or more spiral-shaped or zigzag-shaped conductors connected in series. Despite using C, it is possible to keep the floating capacitance gap extremely small. Therefore, it is possible to prevent the C1 self-photographing frequency fo from decreasing, and the frequency characteristics are improved.
(実施例の説明) 以下、図面とともに本発明の実施ff11を説明する。(Explanation of Examples) Hereinafter, implementation ff11 of the present invention will be described with reference to the drawings.
第1図(A)および(B)は、本発明の一実施例にかか
るプリントコイルを示しCいる。ただし、第1図(A)
は平面図、第1図(B)は鎖、I C−C’部分の側断
面図である。このプリントコイルにおいC16’tdセ
ラミツクスの誘電体基板であり、比誘電率240.1コ
イル部8分形成し、他方の渦巻形状が第2コイル部9を
形成しCいる。このプリントコイルは、導体7の一方の
端部7aと他方の端部7bとの間に所望のインダクタン
ス1直を得ることができる。FIGS. 1A and 1B show a printed coil according to an embodiment of the present invention. However, Fig. 1 (A)
1 is a plan view, and FIG. 1(B) is a side cross-sectional view of the chain and I CC' portion. In this printed coil, the dielectric substrate is made of C16'td ceramics, and has a dielectric constant of 240.1, forming eight coil parts, and the other spiral shape forms a second coil part 9. This printed coil can obtain a desired inductance between one end 7a and the other end 7b of the conductor 7.
一方、第2図(A)から(C)は、本発明の他の実施例
にかかるプリントコイルを示しCI/−する。ただし、
第2図LA)は平面図、第2図(B)はその鎖線D −
D’部分の側断面図、第21図(C)は底面図である。On the other hand, FIGS. 2A to 2C show printed coils according to other embodiments of the present invention. however,
Figure 2 (LA) is a plan view, Figure 2 (B) is its chain line D -
FIG. 21(C) is a side sectional view of portion D' and a bottom view.
このプリンコイルに、しlへC110はセラミックスの
誘電体基板であり、比誘電率240.厚さ0.411u
Iである。11および12はスルーホールであり、それ
ぞれ誘電体基板10を貫通し゛〔形成され〔いる。C110 is a ceramic dielectric substrate with a dielectric constant of 240. Thickness 0.411u
It is I. Reference numerals 11 and 12 indicate through holes, which are formed to penetrate through the dielectric substrate 10, respectively.
16は誘電体基板10の両方の表面にわたつC固着され
た導体であり、一方の表面からスルーホール11を介し
゛C他方の表面にわたつC形成された渦巻形状と、一方
の表面からスルーホール12を介し〔他方の表面にわた
つ〔形成された渦巻形状とを直列に接続したものである
。そしC1一方の渦を形状が第1コイル部14を形成し
、他方の渦き形状が第2コイル部15を形成しく1八る
。このプリントコイルは、導体16の一方の端部13a
と他方の端部13bとの間に所望のインダクタンス値を
得ることができる。A conductor 16 is fixed to both surfaces of the dielectric substrate 10, and has a spiral shape that extends from one surface to the other surface through the through hole 11, and from one surface to the other surface. The spiral shapes formed across the other surface are connected in series through the through holes 12. The shape of one vortex of C1 forms the first coil part 14, and the shape of the other vortex forms the second coil part 15. This printed coil is connected to one end 13a of the conductor 16.
A desired inductance value can be obtained between the end portion 13b and the other end portion 13b.
上述した2つの本発明にかかるプリントコイルは、いず
れも、所望のインダクタンス値を直列に接続された2個
の渦巻形状の導体に分割し〔形成したものであり、浮遊
容icpは極めC小さい。Both of the above-mentioned printed coils according to the present invention are formed by dividing a desired inductance value into two spiral-shaped conductors connected in series, and the stray capacitance icp is extremely small.
したがつC1自己共搗周波elfoは低下しCおらず、
充分実用的な周波数特性と得ることができる。Therefore, the C1 self-resonant frequency elfo decreases and C does not occur.
A sufficiently practical frequency characteristic can be obtained.
第6図は、比誘電率240、厚さ0.4aの誘11体基
板の一方の表面に2回巻、スルーホールを介しC他方の
表面に、2回をした渦を形状を2周面列に接続した導体
からなるインダクタンス/175nHの本発明にかかる
プリントコイルの周波数特性〔図中([L)で示す〕と
、一方の表面に5回巻、スルーホールを介しC開方の表
面に6回巻した渦巻形状の導体からなるインダクタンス
値75nHの本発明に属さないプリントコイルの周波数
特性〔図中(b)で示す〕とを比較したものである。こ
の図から、本発明によれば周波数!特性が改善され〔い
ることがわかる。Figure 6 shows a dielectric substrate with a relative dielectric constant of 240 and a thickness of 0.4a.The vortex is wound twice on one surface of the dielectric substrate and passed through a through hole to the other surface. The frequency characteristics of a printed coil according to the present invention with an inductance of 175 nH consisting of conductors connected in a row (indicated by [L] in the figure), and a winding of 5 turns on one surface and a C-opening surface through a through hole. A comparison is made with the frequency characteristics of a printed coil (shown in (b) in the figure), which does not belong to the present invention and has an inductance value of 75 nH and is made of a spiral conductor wound six times. From this figure, according to the invention, the frequency! It can be seen that the characteristics have been improved.
以上は本発明のプリントコイルの2つの実施例であり、
本発明の趣旨を屓なわない範囲内で設計変更をなしうろ
ことはいうまでもない。たとえば、誘電体基板6ないし
10の材質や比誘電率や厚みなどは任意であり、上記の
実施例のように限定されることはない。また、導体7な
いし1・6はeれぞれ2個の四角渦巻形状を直列に接続
し〔それぞれ2個のコイル部分を構成しCいるが、コイ
ル部分を構成する導体7な(八し16の形状は四角渦巻
形状に限定されることはなく、円渦静形状、ジグザブ形
状などであつCもよい。さらに、導体7ないし13によ
つ゛C溝成されるコイル部分の数は21固に限定される
ことはなく、21固以上であればよい。The above are two embodiments of the printed coil of the present invention,
It goes without saying that design changes may be made without departing from the spirit of the present invention. For example, the material, dielectric constant, thickness, etc. of the dielectric substrates 6 to 10 are arbitrary, and are not limited as in the above embodiments. In addition, the conductors 7 to 1 and 6 are connected in series with two rectangular spiral shapes each [each constitutes two coil parts], but the conductors 7 (e) constituting the coil part (e) The shape of the coil is not limited to a rectangular spiral shape, but may be a circular spiral shape, a zigzab shape, etc. Furthermore, the number of coil portions formed by the conductors 7 to 13 with the "C" groove is limited to 21. There is no limitation, and it may be 21 or more.
(発明の効果)
以上の説明からも明らかなように、本発明のプリントコ
イルは、2個以上の渦巻形状ないしジグザグ形状を直列
に接続した導体を、誘電体基板の表面に固着させるよう
にしだものである。この結果、本発明のプリントコイル
は、基板とし゛C誘゛厄体基板を使用しCいるにもかか
わらず、浮遊容量Cpが小さいため、自己共憑周波数f
。は低下しCおらず、充分実用的な周波数特性を得るこ
とができる。(Effects of the Invention) As is clear from the above explanation, the printed coil of the present invention has a conductor in which two or more spiral or zigzag shapes are connected in series and is fixed to the surface of a dielectric substrate. It is something. As a result, the printed coil of the present invention has a small stray capacitance Cp even though it uses a C attracting substrate as a substrate, so that the self-coherent frequency f
. There is no decrease in C, and sufficiently practical frequency characteristics can be obtained.
第1図(A)は本発明の一実施例にかかるプリントコイ
ルを示す平面図、第1図(B)はその鎖線C−C’部分
の側断面図、第2図(勾は本発明の他の実施例にかかる
プリントコイルを示す平面図、第2図中)はその鎖線D
−D’部分の側断面図、第2図(C)は底面図、第5図
は本発明にかかるプリントコイルの周波数特性と本発明
に属さないプリントコイルの周波数特性とを比較した図
、第4図(A)は従来のプリントコイルを示す平面図、
第4図(B)はその鎖線鎖線B−B’部分の側断面図、
第5図(C)はその底面図、第6図は従来のプリントコ
イルの等価回路図、第7図は本発明にかかるプリントコ
イルの等価回路図である。
6.10・・・・・・・・・誘電体基板、7.13・・
・・・・・・4朱8.14・・・・・・・・・第1コイ
ル部、9.15・・・・・・・・・第2コイル部。FIG. 1(A) is a plan view showing a printed coil according to an embodiment of the present invention, FIG. 1(B) is a side sectional view taken along the dashed line CC', and FIG. A plan view showing a printed coil according to another embodiment (in Fig. 2) is indicated by the chain line D.
- A side sectional view of the D' portion, FIG. 2(C) is a bottom view, FIG. Figure 4 (A) is a plan view showing a conventional printed coil;
FIG. 4(B) is a side sectional view taken along the chain line B-B',
FIG. 5(C) is a bottom view thereof, FIG. 6 is an equivalent circuit diagram of a conventional printed coil, and FIG. 7 is an equivalent circuit diagram of a printed coil according to the present invention. 6.10... Dielectric substrate, 7.13...
・・・・・・4 Red 8.14・・・・・・First coil part, 9.15・・・・・・Second coil part.
Claims (1)
イルにおいて、 導体が2個以上の渦巻形状ないしジグザグ形状を直列に
接続したものからなることを特徴とするプリントコイル
。[Claims] A printed coil comprising a conductor fixed to the surface of a dielectric substrate, characterized in that the conductor is composed of two or more spiral or zigzag shapes connected in series.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24247285A JPS62101010A (en) | 1985-10-28 | 1985-10-28 | Printed coil |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24247285A JPS62101010A (en) | 1985-10-28 | 1985-10-28 | Printed coil |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62101010A true JPS62101010A (en) | 1987-05-11 |
Family
ID=17089591
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP24247285A Pending JPS62101010A (en) | 1985-10-28 | 1985-10-28 | Printed coil |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62101010A (en) |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02128507A (en) * | 1988-11-09 | 1990-05-16 | Murata Mfg Co Ltd | Wide band amplifier |
JPH02146409U (en) * | 1989-05-16 | 1990-12-12 | ||
JPH0514007A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0514006A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line resonator and filter |
JPH0514010A (en) * | 1991-07-05 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0514008A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0514009A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0550803U (en) * | 1991-11-29 | 1993-07-02 | 東光株式会社 | Stripline filter |
JPH0550805U (en) * | 1991-12-04 | 1993-07-02 | 東光株式会社 | Stripline filter |
JP2002299130A (en) * | 2001-04-02 | 2002-10-11 | Densei Lambda Kk | Composite element for power source |
US6593841B1 (en) | 1990-05-31 | 2003-07-15 | Kabushiki Kaisha Toshiba | Planar magnetic element |
JP2012089700A (en) * | 2010-10-20 | 2012-05-10 | Asahi Kasei Electronics Co Ltd | Planar coil, method of manufacturing the same, and composite planar coil for actuator |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS57563U (en) * | 1980-05-30 | 1982-01-05 |
-
1985
- 1985-10-28 JP JP24247285A patent/JPS62101010A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS57563U (en) * | 1980-05-30 | 1982-01-05 |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02128507A (en) * | 1988-11-09 | 1990-05-16 | Murata Mfg Co Ltd | Wide band amplifier |
JPH02146409U (en) * | 1989-05-16 | 1990-12-12 | ||
US6593841B1 (en) | 1990-05-31 | 2003-07-15 | Kabushiki Kaisha Toshiba | Planar magnetic element |
JPH0514007A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0514006A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line resonator and filter |
JPH0514008A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0514009A (en) * | 1991-06-27 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0514010A (en) * | 1991-07-05 | 1993-01-22 | Toko Inc | Strip line filter |
JPH0550803U (en) * | 1991-11-29 | 1993-07-02 | 東光株式会社 | Stripline filter |
JPH0550805U (en) * | 1991-12-04 | 1993-07-02 | 東光株式会社 | Stripline filter |
JP2002299130A (en) * | 2001-04-02 | 2002-10-11 | Densei Lambda Kk | Composite element for power source |
JP2012089700A (en) * | 2010-10-20 | 2012-05-10 | Asahi Kasei Electronics Co Ltd | Planar coil, method of manufacturing the same, and composite planar coil for actuator |
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