JPH0461309A - Fabric structure inductance element - Google Patents
Fabric structure inductance elementInfo
- Publication number
- JPH0461309A JPH0461309A JP17309590A JP17309590A JPH0461309A JP H0461309 A JPH0461309 A JP H0461309A JP 17309590 A JP17309590 A JP 17309590A JP 17309590 A JP17309590 A JP 17309590A JP H0461309 A JPH0461309 A JP H0461309A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- inductance
- magnetic core
- thread
- latitude
- 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
- 239000004744 fabric Substances 0.000 title abstract description 3
- 239000004020 conductor Substances 0.000 claims abstract description 18
- 239000004753 textile Substances 0.000 claims description 15
- 230000005284 excitation Effects 0.000 claims description 9
- 230000006866 deterioration Effects 0.000 abstract description 4
- 230000002542 deteriorative effect Effects 0.000 abstract description 3
- 230000035699 permeability Effects 0.000 abstract description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 abstract description 2
- 230000015572 biosynthetic process Effects 0.000 abstract 1
- 229910052802 copper Inorganic materials 0.000 abstract 1
- 239000010949 copper Substances 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 9
- 239000002759 woven fabric Substances 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 239000003990 capacitor Substances 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 230000003313 weakening effect Effects 0.000 description 1
Landscapes
- Coils Or Transformers For Communication (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は、マイクロ化に好適する高周波数帯で用いる
インダクタやトランス等の織物構造インダクタンス素子
に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to textile structure inductance elements such as inductors and transformers used in high frequency bands suitable for micronization.
[従来の技術]
第4図は例えば特開昭61−219114号公報に示さ
れた、従来の織物構造インダクタンス素子の概略構成図
である。図中のインダクタンス素子には説明の便宜上、
インダクタを取り上げている。図中1は伸線が可能な金
属磁性線、2は1本あるいは複数本の磁性線1で構成さ
れる磁心であり、□織物構造の経糸となっている。3は
絶縁被覆された励磁導体線である。今、磁性線1を経糸
とし、励磁導体線3を緯糸として長尺の帯状の織布を作
製した後、所要の長さに磁性線1よりなる磁心2を切断
すれば容易にインダクタンスを作製できる。このインダ
クタンスにおいては図中の矢印iの方向に励磁導体線3
中を電流iが流れると、磁心2には矢印Hで示すように
隣接磁心2間で相互に逆向きに磁界が励起される。この
結果、各磁心2の先端からの婦洩磁束は点線の矢印Φで
示すように隣接磁心2の先端に容易に流入でき、全体的
には反磁界の小さい準閉磁路が磁性!111により形成
されていることになる。即ち磁心2の透磁率の増加にほ
ぼ比例して大きなインダクタンスを効果的を得ることが
できる。しかも磁心2を形成する磁性線1の直径を細く
すると磁心2を流れる渦電流を減少させ、損失を小さく
でき高周波帯での使用が可能となる。[Prior Art] FIG. 4 is a schematic diagram of a conventional textile structure inductance element disclosed in, for example, Japanese Unexamined Patent Publication No. 61-219114. For convenience of explanation, the inductance element in the figure is
We are talking about inductors. In the figure, 1 is a metal magnetic wire that can be drawn, 2 is a magnetic core composed of one or more magnetic wires 1, and □ serves as the warp of a woven fabric structure. 3 is an excitation conductor wire coated with insulation. Now, an inductance can be easily produced by making a long belt-shaped woven fabric using the magnetic wire 1 as the warp and the excitation conductor wire 3 as the weft, and then cutting the magnetic core 2 made of the magnetic wire 1 to the required length. . In this inductance, the excitation conductor wire 3 is directed in the direction of arrow i in the figure.
When a current i flows through the magnetic core 2, magnetic fields are excited in mutually opposite directions between adjacent magnetic cores 2, as shown by arrows H. As a result, the leakage magnetic flux from the tip of each magnetic core 2 can easily flow into the tip of the adjacent magnetic core 2 as shown by the dotted arrow Φ, and the quasi-closed magnetic path with a small demagnetizing field is magnetic! 111. That is, it is possible to effectively obtain a large inductance approximately in proportion to the increase in magnetic permeability of the magnetic core 2. Furthermore, by reducing the diameter of the magnetic wire 1 forming the magnetic core 2, the eddy current flowing through the magnetic core 2 is reduced, the loss can be reduced, and use in a high frequency band becomes possible.
[発明が解決しようとする課題]
織物構造において磁性線が長い場合には反磁界の影響を
無視することができ、磁心に励起される磁界により隣接
磁心間で相互に逆向きに励起されるため隣接磁心間で磁
性線にとり準閉磁路が形成される。しかし、マイクロ化
に伴いインダクタンス素子全体のサイズが小さくなった
場合には、磁性線の長さは短くなり従って反磁界の影響
を無視できなくなる。すなわち、反磁界が大きくなるた
め励起される磁界は弱められるためにインダクタンスが
劣化する問題があった。[Problem to be solved by the invention] When the magnetic wires are long in a textile structure, the influence of the demagnetizing field can be ignored, and the magnetic field excited by the magnetic cores causes adjacent magnetic cores to be excited in mutually opposite directions. A quasi-closed magnetic path is formed for the magnetic wire between adjacent magnetic cores. However, when the overall size of the inductance element becomes smaller due to miniaturization, the length of the magnetic wire becomes shorter, and therefore the influence of the demagnetizing field cannot be ignored. That is, since the demagnetizing field becomes larger, the excited magnetic field is weakened, resulting in a problem of deterioration of inductance.
そこで、本発明は上記の事情に鑑みてなされたもので、
サイズが小さくなった場合にも磁性線による反磁界の影
響を小さくしてインダクタンスの劣゛化を防止し得る織
物構造インダクタンス素子を提供することを目的とする
。Therefore, the present invention was made in view of the above circumstances.
It is an object of the present invention to provide a textile structure inductance element that can prevent deterioration of inductance by reducing the influence of demagnetizing fields caused by magnetic wires even when the size is reduced.
[課題を解決するための手段及び作用]本発明は上記課
題を解決するために、磁性線を経糸とし、絶縁膜で被覆
した励磁導体と磁性線とを緯糸として織物状に構成した
ことを特徴とするもので、緯糸を絶縁膜で被覆した励磁
導体と磁性線とで構成することにより、経糸磁心と緯糸
磁心により閉磁路を作るようにしたものである。[Means and Effects for Solving the Problems] In order to solve the above problems, the present invention is characterized in that the magnetic wire is used as the warp, and the excitation conductor coated with an insulating film and the magnetic wire are used as the weft in a woven fabric. By constructing an excitation conductor whose weft threads are covered with an insulating film and magnetic wires, a closed magnetic path is created by the warp thread magnetic core and the weft thread magnetic core.
[実施例] (実施例1) 第1図はこの発明の実施例1の概略図である。[Example] (Example 1) FIG. 1 is a schematic diagram of Embodiment 1 of the present invention.
以下図面を参照して詳細に説明する。説明の便宜上イン
ダクタンス素子としてインダクタを取り上げている。1
本あるいは複数本のアモルファス磁性線11を束ねて構
成した磁心12を経糸とし、絶縁膜としてホルマルを被
覆した銅線等の励磁導体線13と1本あるいは複数本の
アモルファス磁性線を束ねて構成した磁心14を緯糸と
して、織物状に構成したものである。このインダクタに
おいて図中の矢印iの方向に励磁導体線13中を電流i
が流れると経糸磁心12及び緯糸磁心14には矢印Hで
示すように磁界が励起される。この結果磁心12と14
間で閉磁路ができる。このことにより磁心12が短い場
合にもインダクタンスを劣化させず透磁率の増加にほぼ
比例して大きいインダクタンスが効果的に得られる。A detailed explanation will be given below with reference to the drawings. For convenience of explanation, an inductor is taken up as an inductance element. 1
A magnetic core 12 formed by bundling a book or a plurality of amorphous magnetic wires 11 is used as a warp, and an excitation conductor wire 13 such as a copper wire coated with formal as an insulating film is formed by bundling one or a plurality of amorphous magnetic wires. The magnetic core 14 is a weft and is constructed in the form of a woven fabric. In this inductor, a current i flows through the excitation conductor wire 13 in the direction of the arrow i in the figure.
Flows, a magnetic field is excited in the warp magnetic core 12 and the weft magnetic core 14 as shown by arrow H. As a result, magnetic cores 12 and 14
A closed magnetic path is created between the two. As a result, even when the magnetic core 12 is short, it is possible to effectively obtain a large inductance substantially proportional to an increase in magnetic permeability without deteriorating the inductance.
(実施例2)
第2図はこの発明に係わる実施例2の概略図である。緯
糸磁心141は連続的に接続していない場合においても
図中に矢印Hで示すように閉磁路ができるため第1図に
示す実施例の場合と同様の効果が得られる。第2図中、
第1図と同一部分は同一符号を付してその説明を省略す
る。(Embodiment 2) FIG. 2 is a schematic diagram of Embodiment 2 according to the present invention. Even when the weft magnetic cores 141 are not connected continuously, a closed magnetic path is formed as shown by arrow H in the figure, so that the same effect as in the embodiment shown in FIG. 1 can be obtained. In Figure 2,
The same parts as in FIG. 1 are given the same reference numerals, and the explanation thereof will be omitted.
(実施例3)
第3図は本発明の実施例3に係わるインダクタンス素子
のトランスの概略図である。第3図中、第1図と同一部
分は同一符号を付してその説明を省略する。即ち、′I
a3図は第1図の励磁導体線13を一次導体線131お
よび二次導体線132の二本に置き換え織物状に織った
トランスである。(Embodiment 3) FIG. 3 is a schematic diagram of a transformer of an inductance element according to Embodiment 3 of the present invention. In FIG. 3, the same parts as those in FIG. 1 are given the same reference numerals, and the explanation thereof will be omitted. That is, 'I
Figure a3 shows a transformer in which the excitation conductor wire 13 in Figure 1 is replaced with two wires, a primary conductor wire 131 and a secondary conductor wire 132, woven into a fabric.
また、2本の導体線131.132を直列に接続するこ
とにより、実施例1の約2倍のインダクタンスが得られ
る。このトランスにおいて実施例2と同様に緯糸磁心が
連続でない場合にも同様に実施できることが十分推察さ
れる。Furthermore, by connecting the two conductor wires 131 and 132 in series, an inductance approximately twice that of the first embodiment can be obtained. It is fully surmised that in this transformer, similar to the second embodiment, the present invention can be implemented in the same manner even when the weft magnetic core is not continuous.
以上のように導体線と磁性線とを同時に緯糸とすること
により、経糸磁心と緯糸磁心との間に閉磁路ができるた
めに、マイクロ化に伴うインダクタンスの劣化を防ぐこ
とができる。この織物構造インダクタンス素子はコンデ
ンサーや抵抗と集積化しても当然使用できる。この場合
、この織物構造インダクタンス素子は閉磁路構成になっ
ているために他の磁気的な外部条件の影響が少なく集積
化に好都合である。As described above, by simultaneously using the conductor wire and the magnetic wire as weft threads, a closed magnetic path is created between the warp thread magnetic core and the weft thread magnetic core, so that deterioration of inductance due to micronization can be prevented. Naturally, this textile structure inductance element can be used even if it is integrated with a capacitor or a resistor. In this case, since this textile structure inductance element has a closed magnetic circuit configuration, it is less affected by other magnetic external conditions and is convenient for integration.
[発明の効果]
以上述べたように本発明における織物構造インダクタン
ス素子によれば、磁性線の反磁界により磁心に励起され
る磁界が弱まりインダクタンスが劣化することを防ぐこ
とができる。従って、本発明は織物構造インダクタンス
素子のマイクロ化に非常に有用である。[Effects of the Invention] As described above, according to the textile structure inductance element of the present invention, the magnetic field excited in the magnetic core by the demagnetizing field of the magnetic wire can be prevented from weakening and the inductance from deteriorating. Therefore, the present invention is very useful for microfabrication of textile structure inductance elements.
第1図は本発明の実施例1における織物構造インダクタ
の構成を示す概略図、第2図は本発明の実施例2におけ
る織物構造インダクタの構成を示す概略図、第3図は本
発明の実施例3における織物構造トランスの構成を示す
概略図、第4図は従来の織物構造インダクタの構成を示
す概略図である。
1・・・磁性線、
2・・・経糸磁心、
13・・
は励磁
導体線、
14・・・緯糸磁心、
1・・・−次導体線、
32・・・二次導体線。FIG. 1 is a schematic diagram showing the configuration of a textile structure inductor in Example 1 of the present invention, FIG. 2 is a schematic diagram showing the configuration of a textile structure inductor in Example 2 of the invention, and FIG. 3 is a schematic diagram showing the configuration of a textile structure inductor in Example 2 of the present invention. FIG. 4 is a schematic diagram showing the configuration of a textile structure transformer in Example 3, and FIG. 4 is a schematic diagram showing the configuration of a conventional textile structure inductor. DESCRIPTION OF SYMBOLS 1...Magnetic wire, 2...Warp magnetic core, 13...Exciting conductor wire, 14...Weft magnetic core, 1...-Secondary conductor wire, 32...Secondary conductor wire.
Claims (1)
とを緯糸として織物状に構成したことを特徴とする織物
構造インダクタンス素子。A textile structure inductance element characterized in that it is constructed in the form of a textile, with magnetic wires as warp threads, and an excitation conductor coated with an insulating film and magnetic wires as weft threads.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17309590A JPH0461309A (en) | 1990-06-29 | 1990-06-29 | Fabric structure inductance element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17309590A JPH0461309A (en) | 1990-06-29 | 1990-06-29 | Fabric structure inductance element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0461309A true JPH0461309A (en) | 1992-02-27 |
Family
ID=15954100
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17309590A Pending JPH0461309A (en) | 1990-06-29 | 1990-06-29 | Fabric structure inductance element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0461309A (en) |
-
1990
- 1990-06-29 JP JP17309590A patent/JPH0461309A/en active Pending
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