JPH0810658B2 - Split coil type inductance element - Google Patents
Split coil type inductance elementInfo
- Publication number
- JPH0810658B2 JPH0810658B2 JP3129746A JP12974691A JPH0810658B2 JP H0810658 B2 JPH0810658 B2 JP H0810658B2 JP 3129746 A JP3129746 A JP 3129746A JP 12974691 A JP12974691 A JP 12974691A JP H0810658 B2 JPH0810658 B2 JP H0810658B2
- Authority
- JP
- Japan
- Prior art keywords
- coil
- inductance element
- skin depth
- split
- film
- 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.)
- Expired - Lifetime
Links
- 239000010408 film Substances 0.000 claims description 19
- 239000010409 thin film Substances 0.000 claims description 11
- 239000004020 conductor Substances 0.000 claims description 9
- 239000011810 insulating material Substances 0.000 claims 1
- 239000012212 insulator Substances 0.000 claims 1
- 239000010410 layer Substances 0.000 description 11
- 238000000034 method Methods 0.000 description 9
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 3
- 229910052802 copper Inorganic materials 0.000 description 3
- 239000010949 copper Substances 0.000 description 3
- 239000002356 single layer Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 229910004298 SiO 2 Inorganic materials 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000002500 effect on skin Effects 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 229920001187 thermosetting polymer Polymers 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Landscapes
- Coils Or Transformers For Communication (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は高周波薄膜インダクタン
ス素子に於いて、高周波領域でコイルの有効断面を増加
させるための励磁導体の改良に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high frequency thin film inductance element, and to an improvement of an exciting conductor for increasing an effective cross section of a coil in a high frequency region.
【0002】[0002]
【従来の技術】図7(a),(b)に従来検討されてい
る薄膜インダクタの渦巻状コイルもしくは櫛状コイルの
形状を示す。一般にこれらのコイルを絶縁膜を介して磁
心薄膜のまわりに配したり、これらのコイルの一面又は
両面に磁心を絶縁膜を介して配することにより、薄膜イ
ンダクタやトランス等のインダクタンス素子を作製して
いる。2. Description of the Related Art FIGS. 7A and 7B show the shape of a spiral coil or a comb coil of a thin film inductor which has been conventionally studied. Generally, by arranging these coils around a magnetic core thin film via an insulating film, or by arranging a magnetic core on one or both surfaces of these coils via an insulating film, an inductance element such as a thin film inductor or a transformer is manufactured. ing.
【0003】[0003]
【発明が解決しようとする課題】しかし、これらのイン
ダクタンス素子において高いインダクタンスを得るため
にコイルの巻数を増やさなければならないのが現状であ
る。此れにともないコイルの抵抗は増加し、インダクタ
ンス素子のQを下げる原因になっている。これを解消す
るためにコイル膜厚を厚くして抵抗を低減する方法も考
えられるが、高周波領域では表皮効果により単層で厚い
コイルを用いてもコイル断面全体を有効に利用出来な
い。従って、単に単層コイルの膜厚を厚くしてもコイル
の高周波領域での抵抗を低減出来ない。However, under the present circumstances, it is necessary to increase the number of turns of the coil in order to obtain a high inductance in these inductance elements. Along with this, the resistance of the coil increases, which causes the Q of the inductance element to decrease. In order to solve this, a method of increasing the coil film thickness to reduce the resistance may be considered, but in the high frequency region, the entire coil cross section cannot be effectively used even if a single layer thick coil is used due to the skin effect. Therefore, even if the film thickness of the single-layer coil is simply increased, the resistance of the coil in the high frequency region cannot be reduced.
【0004】本発明は上記の事情に鑑みてなされたもの
で、高周波薄膜インダクタンス素子において、高周波領
域でコイルの有効断面を増加させることにより、高周波
領域でのコイルの抵抗を低減し得る分割コイル型インダ
クタンス素子を提供することを目的する。The present invention has been made in view of the above circumstances, and in a high frequency thin film inductance element, by increasing the effective section of the coil in the high frequency region, the split coil type which can reduce the resistance of the coil in the high frequency region. An object is to provide an inductance element.
【0005】[0005]
【課題を解決するための手段】本発明は上記課題を解決
するために、薄膜磁性体のまわりに絶縁膜を介して励磁
導体を配するインダクタンス素子において、励磁導体を
絶縁物の介在した分割コイルとすることを特徴とするも
のである。In order to solve the above-mentioned problems, the present invention provides an inductance element in which an exciting conductor is arranged around a thin film magnetic body with an insulating film interposed therebetween. It is characterized by
【0006】[0006]
【作用】上記手段により、矩形断面を有するコイルの短
径が表皮深さ内の幅を有するように絶縁膜を挿んで二層
以上に多層分割化することにより励磁導体の高周波領域
でのコイルの有効断面積を増加させようとするもので、
高周波インダクタンス素子の高Q化に有用な手段であ
る。With the above-mentioned means, the insulating film is inserted so that the minor axis of the coil having the rectangular cross section has the width within the skin depth, and the coil is divided into two or more layers. To increase the effective area,
It is a useful means for increasing the Q of the high frequency inductance element.
【0007】[0007]
【実施例】以下図面を参照して本発明の実施例を詳細に
説明する。 実施例1Embodiments of the present invention will now be described in detail with reference to the drawings. Example 1
【0008】図1に本発明の一実施例を示し、図2に図
1のA−B線より断面した断面図を示す。説明の便宜
上、巻線型インダクタを例にとり説明する。絶縁基板1
の上には、薄膜磁性体よりなる磁心3のまわりに絶縁膜
4を介して励磁導体のコイル2を巻いた高周波薄膜イン
ダクタンス素子が形成される。図1においては煩雑を避
けるためにコイル2と磁心3間の絶縁膜4は省略してあ
る。前記コイル2は絶縁膜5を介して二層コイルを巻い
た構造になっている。コイル2を2層に分割した場合の
分割方法を図3,図4に示す。即ち、図3に示すよう
に、コイル2の長手方向に対して直角に切った矩形断面
の長径にほぼ平行(又はほぼ直角)に絶縁層5を挾む方
法である。この場合、分割されたコイル2の導体部分の
幅は次のようにして決定される。図5に示した銅の表皮
深さ、即ち、導体表面の電流密度に対してその値が1/
e=略1/2.7になる表皮からの深さと周波数の関係
より、インダクタンス素子の使用周波数に対応した銅の
表皮深さを知り得る。従って、コイル2の一層の膜厚を
この表皮深さの2倍程度の膜厚とする。又、導体間の絶
縁膜5は熱硬化したレジスト膜やSiO2 膜で行ってい
る。図2において平面方向のコイル2は二層であるが垂
直方向即ちコイル2の接合部分では単層なっているがサ
イズ的に結合部分のコイル長は全体のコイル長の1%以
下であるため全体として二層にした効果が充分発揮され
る。コイル2を図4のように、垂直方向即ちコイル2の
接合部分を絶縁膜5で分割した場合はコイル2全体が分
割コイルとなり高周波領域での抵抗の低減により有効で
ある。実施例2FIG. 1 shows an embodiment of the present invention, and FIG. 2 shows a sectional view taken along the line AB of FIG. For convenience of explanation, a winding type inductor will be described as an example. Insulating substrate 1
A high-frequency thin film inductance element in which a coil 2 of an exciting conductor is wound around a magnetic core 3 made of a thin film magnetic material via an insulating film 4 is formed on the above. In FIG. 1, the insulating film 4 between the coil 2 and the magnetic core 3 is omitted to avoid complication. The coil 2 has a structure in which a two-layer coil is wound with an insulating film 5 interposed therebetween. A method of dividing the coil 2 into two layers is shown in FIGS. That is, as shown in FIG. 3, this is a method in which the insulating layer 5 is sandwiched substantially parallel (or substantially at right angles) to the major axis of a rectangular cross section cut at right angles to the longitudinal direction of the coil 2. In this case, the width of the conductor portion of the divided coil 2 is determined as follows. The skin depth of copper shown in FIG. 5, that is, the value is 1 / with respect to the current density on the conductor surface.
From the relationship between the depth from the skin and the frequency at which e = approximately 1 / 2.7, the skin depth of copper corresponding to the operating frequency of the inductance element can be known. Therefore, the film thickness of one layer of the coil 2 is about twice the skin depth. The insulating film 5 between the conductors is made of a thermosetting resist film or SiO 2 film. In FIG. 2, the coil 2 in the plane direction has two layers, but the coil 2 in the vertical direction, that is, in the joint portion of the coil 2 has a single layer. As a result, the effect of forming two layers is sufficiently exhibited. As shown in FIG. 4, when the coil 2 is divided in the vertical direction, that is, the joint portion of the coil 2 is divided by the insulating film 5, the entire coil 2 becomes a divided coil, which is effective in reducing resistance in a high frequency region. Example 2
【0009】図6はコイルの他の分割方法を示す実施例
の断面概略図である。コイル2の中央部分のみに絶縁膜
5をはさんで多層化する方法である。この方法によれば
実施例1の結合部分も多層分割コイルになりよりいっそ
うの効果があり、高周波インダクタンス素子の高Q化に
効果的である。FIG. 6 is a schematic sectional view of an embodiment showing another method of dividing the coil. This is a method in which the insulating film 5 is sandwiched only in the central portion of the coil 2 to form a multilayer structure. According to this method, the coupling portion of the first embodiment also becomes a multi-layer split coil, which is more effective, and is effective in increasing the Q of the high frequency inductance element.
【0010】一般に低周波領域でコイルの膜厚を厚くす
ることにより抵抗の低減をはかっているが、高周波領域
ではたとえ厚膜コイルを用いても表皮深さにより有効に
利用されるコイル断面は限定され高周波領域でのコイル
の抵抗を低減することが困難であった。本発明における
インダクタンス素子ではコイルを表皮深さを考慮して分
割すること、即ち矩形断面コイルの短径を表皮深さ程度
に分割し表皮深さ内でコイルを有効に利用することによ
りインダクタンス素子の高Q化をはかるために非常に有
利である。なお上記の実施例では絶縁層を介して動体を
2層に分割する場合について示したが絶縁層の層数を増
やし、導体の厚みを増やせばさらに抵抗の低減が図ら
れ、より顕著な効果が得られる。In general, the resistance is reduced by increasing the film thickness of the coil in the low frequency region. However, in the high frequency region, even if a thick film coil is used, the coil cross section that is effectively used due to the skin depth is limited. It has been difficult to reduce the resistance of the coil in the high frequency region. In the inductance element according to the present invention, the coil is divided in consideration of the skin depth, that is, the minor axis of the rectangular cross-section coil is divided into about the skin depth and the coil is effectively used within the skin depth. It is very advantageous for achieving high Q. In the above embodiment, the case where the moving body is divided into two layers through the insulating layer has been shown, but if the number of insulating layers is increased and the thickness of the conductor is increased, the resistance is further reduced, and a more remarkable effect is obtained. can get.
【0011】[0011]
【発明の効果】以上述べたように本発明によれば、コイ
ルを分割することによりコイルの高周波領域での抵抗を
低減しインダクタの高Q化がはかれる利点がある。As described above, according to the present invention, by dividing the coil, the resistance of the coil in the high frequency region can be reduced and the Q of the inductor can be increased.
【図1】本発明の実施例1を示す概略斜視図である。FIG. 1 is a schematic perspective view showing a first embodiment of the present invention.
【図2】図1のA−B線断面図である。FIG. 2 is a sectional view taken along the line AB of FIG.
【図3】本発明に係るコイルの分割方法の一例を示す構
成説明図である。FIG. 3 is a configuration explanatory view showing an example of a coil dividing method according to the present invention.
【図4】本発明に係るコイルの分割方法の他の例を示す
構成説明図である。FIG. 4 is a structural explanatory view showing another example of the coil dividing method according to the present invention.
【図5】銅の表皮深さと周波数の関係を示す特性図であ
る。FIG. 5 is a characteristic diagram showing the relationship between the skin depth of copper and frequency.
【図6】本発明の実施例2におけるコイルの多層分割の
方法を示す斜視図である。FIG. 6 is a perspective view showing a method of dividing a coil into multiple layers according to a second embodiment of the present invention.
【図7】従来の平面コイルの概略図である。FIG. 7 is a schematic view of a conventional planar coil.
1…絶縁基板、2…コイル、3…磁心、4,5…絶縁
膜。1 ... Insulating substrate, 2 ... Coil, 3 ... Magnetic core, 4, 5 ... Insulating film.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 村上 孝一 宮城県仙台市青葉区小松島一丁目5−29 (56)参考文献 特開 平2−126610(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Koichi Murakami 1-29 Komatsushima 1-chome, Aoba-ku, Sendai City, Miyagi Prefecture (56) Reference JP-A-2-126610 (JP, A)
Claims (2)
磁導体のコイルを配するインダクタンス素子において、
表皮深さ内の厚みを有する薄膜コイル毎に絶縁物を挟み
積層する構成で、一本のコイルを絶縁物で表皮深さ内の
厚みの薄膜コイルに分割することを特徴とする分割コイ
ル型インダクタンス素子。1. An inductance element in which a coil of an exciting conductor is arranged around a thin film magnetic body via an insulating film,
An insulator is sandwiched between each thin-film coil having a thickness within the skin depth.
In the laminated structure, one coil is made of an insulating material within the skin depth.
A split coil type inductance element characterized by being split into thin film coils of thickness .
る各導体部分の矩形断面の短い辺の長さがインダクタン
ス素子の使用周波数に於ける表皮深さの2倍程度にする
ことを特徴とする請求項1記載の分割コイル型インダク
タンス素子。2. The length of the short side of the rectangular cross section of each conductor portion having the divided rectangular cross section of the split coil is about twice the skin depth at the operating frequency of the inductance element. The split coil type inductance element according to claim 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3129746A JPH0810658B2 (en) | 1991-05-31 | 1991-05-31 | Split coil type inductance element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3129746A JPH0810658B2 (en) | 1991-05-31 | 1991-05-31 | Split coil type inductance element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH06204041A JPH06204041A (en) | 1994-07-22 |
| JPH0810658B2 true JPH0810658B2 (en) | 1996-01-31 |
Family
ID=15017181
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3129746A Expired - Lifetime JPH0810658B2 (en) | 1991-05-31 | 1991-05-31 | Split coil type inductance element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0810658B2 (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5591804A (en) * | 1978-12-29 | 1980-07-11 | Tdk Corp | Chip type inductor |
| JPH01105516A (en) * | 1987-10-19 | 1989-04-24 | Fuji Elelctrochem Co Ltd | Manufacture of laminated chip inductor |
| JP3000579B2 (en) * | 1988-11-07 | 2000-01-17 | 株式会社村田製作所 | Manufacturing method of chip coil |
-
1991
- 1991-05-31 JP JP3129746A patent/JPH0810658B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH06204041A (en) | 1994-07-22 |
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