JP2605565Y2 - Multilayer noise removal components - Google Patents

Multilayer noise removal components

Info

Publication number
JP2605565Y2
JP2605565Y2 JP1993024392U JP2439293U JP2605565Y2 JP 2605565 Y2 JP2605565 Y2 JP 2605565Y2 JP 1993024392 U JP1993024392 U JP 1993024392U JP 2439293 U JP2439293 U JP 2439293U JP 2605565 Y2 JP2605565 Y2 JP 2605565Y2
Authority
JP
Japan
Prior art keywords
laminated
noise
component
conductor
noise elimination
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
Application number
JP1993024392U
Other languages
Japanese (ja)
Other versions
JPH0682822U (en
Inventor
俊一 大野
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.)
Taiyo Yuden Co Ltd
Original Assignee
Taiyo Yuden Co 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
Family has litigation
First worldwide family litigation filed litigation Critical https://patents.darts-ip.com/?family=26352647&utm_source=google_patent&utm_medium=platform_link&utm_campaign=public_patent_search&patent=JP2605565(Y2) "Global patent litigation dataset” by Darts-ip is licensed under a Creative Commons Attribution 4.0 International License.
Application filed by Taiyo Yuden Co Ltd filed Critical Taiyo Yuden Co Ltd
Priority to JP1993024392U priority Critical patent/JP2605565Y2/en
Publication of JPH0682822U publication Critical patent/JPH0682822U/en
Application granted granted Critical
Publication of JP2605565Y2 publication Critical patent/JP2605565Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】[Detailed description of the invention]

【0001】[0001]

【産業上の利用分野】本考案は、ロスの少ない積層ノイ
ズ除去部品に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a laminated noise removing component having a small loss.

【0002】[0002]

【従来の技術】従来の積層ノイズ除去部品は、磁性セラ
ミック(フェライト)素体内に導体を埋設し、導体の端
末を該素体の両端面に形成された外部端子電極に接続し
た部品である。導体は直線で両端に亘って形成されたも
のが基本的な構成であるが、磁路長を長く取得する目的
で、コイル状に磁性体内を周回する構造のものも広く利
用されている。
2. Description of the Related Art A conventional laminated noise elimination component is a component in which a conductor is buried in a magnetic ceramic (ferrite) body and terminals of the conductor are connected to external terminal electrodes formed on both end surfaces of the body. The basic structure of the conductor is a straight line formed at both ends, but a coil having a structure of orbiting a magnetic body in a coil shape is widely used in order to obtain a long magnetic path length.

【0003】積層ノイズ除去部品は、電気回路中に接続
されて用いられ、回路中で発生したノイズを外部へ伝達
することのないように出力時に除去したり、また外部か
らの受信信号に重畳したノイズを除去してきれいな信号
として受信する作用を有する。
A laminated noise removing component is used by being connected to an electric circuit, and removes noise generated in the circuit at the time of output so as not to be transmitted to the outside, or superimposes the noise on an externally received signal. It has the effect of removing noise and receiving it as a clean signal.

【0004】例えば信号波形が幾何学的な矩形波である
として、この信号にノイズが重畳した時の信号波形の例
を図2の(a)に示す。特に同図の(b)は矩形波のか
どがとれて丸くひずんだいわゆるなまった波形を、同図
の(c)は波形が減衰的に振動するひずみでいわゆるリ
ンギングを生じた波形を示している。
For example, assuming that the signal waveform is a geometric rectangular wave, FIG. 2A shows an example of a signal waveform when noise is superimposed on this signal. In particular, FIG. 3B shows a so-called rounded waveform in which the shape of a rectangular wave is rounded and distorted, and FIG. .

【0005】このノイズを除去するために用いた積層ノ
イズ除去部品のインピーダンス(Z)を実数部(R)と
虚数部(XL )とで表わし、それらと周波数(f)との
関係を図3および図4を用いて以下に説明する。なお、
このZ−f曲線で除去できるノイズの周波数はR=XL
の周波数fR=XLを目安とし、これより高い周波数のノイ
ズが除去できるとされている。
[0005] represents leaving the impedance of the laminated noise removal component used for removing the noise (Z) the real part (R) and imaginary part and the (X L), 3 the relationship thereof with the frequency (f) This will be described below with reference to FIG. In addition,
The frequency of the noise that can be removed by this Zf curve is R = X L
It is said that the frequency f R = XL as a guide, and that noise of a higher frequency can be removed.

【0006】例えば、比較的高い透磁率(μ=800)
の磁性体を用いて巻数が少ない場合、ノイズが除去でき
ない領域があり好ましくないので巻数を増加させ曲線Z
のピーク値を高くする。巻数が増せばZが増加し、XL
部分が増し、曲線Zがノイズ除去帯域を覆うようにな
る。
For example, a relatively high magnetic permeability (μ = 800)
When the number of windings is small using the magnetic material of the above, there is a region where noise cannot be removed, which is not preferable.
The peak value of The number of turns is Z is increased if Maze, X L
The portion increases and the curve Z covers the noise removal band.

【0007】以上のことを図3の(a)〜(c)により
説明する。
The above will be described with reference to FIGS.

【0008】ノイズ減衰に要求される周波数の必要帯域
n とその時の必要なインピーダンスZ(R)が図3の
(a)の場合、同図の(b)に示すようなZ−f曲線を
有するインダクタを用いればfR =XL が所望帯域よりも
低い帯域にあってZ(R)も小さく、ノイズがとりきれ
ない領域4(ハッチングで示す)が生じる。
[0008] If the required bandwidth of a frequency required for noise attenuation f n and the time required impedance Z (R) is in FIG. 3 (a), a Z-f curve as shown in the same figure (b) If the inductor is used, fR = XL is in a band lower than the desired band, Z (R) is small, and a region 4 (shown by hatching) in which noise cannot be completely removed occurs.

【0009】そこで、同図(c)に示すように、巻数を
増して曲線Zのピーク値を高くすると、Z(R)が大き
くなって必要なf−Z(R)領域を確保できるようにな
る。
Therefore, as shown in FIG. 1C, when the number of turns is increased and the peak value of the curve Z is increased, Z (R) is increased so that a necessary fZ (R) region can be secured. Become.

【0010】しかしながら図3の(c)ではZ(R)が
余っている部分、必要以上のロスが発生しており、この
ため信号の立ち上がり、立ち下がりの応答性が劣化する
とともに巻数増によるRDCやXL の増大が信号系をも減
衰させるという影響が大きい。特にfR =XL が低いので
低周波でのXL が、透磁率の低い磁性体の場合よりも大
きい。この種の積層ノイズ除去部品の波形はなまった波
形となる。
However, in FIG. 3 (c), a portion where Z (R) is surplus and a loss more than necessary occur, so that the response of the rising and falling of the signal is deteriorated, and the R due to the increase in the number of turns is reduced. effect of increased DC and X L can also attenuate the signal system is large. Particularly X L in the low frequency because of the low f R = XL is larger than in the case of low magnetic permeability. The waveform of this type of laminated noise removing component is a blunt waveform.

【0011】そこで、透磁率の低い磁性体を選択して巻
数を少なくするとZのピークは高周波側に移動し、Zの
ピーク値が高くなる。この種の積層ノイズ除去部品の波
形はR部分が少なくなり波形のなまりは避けられるがリ
ンギングが増す。
Therefore, when a magnetic material having a low magnetic permeability is selected and the number of turns is reduced, the peak of Z moves to the high frequency side, and the peak value of Z increases. The waveform of this type of laminated noise removing component has a smaller R portion and can avoid rounding of the waveform, but increases ringing.

【0012】以上の場合を具体的に図4の(a)〜
(b)により説明する。
The above case is specifically shown in FIGS.
This will be described with reference to FIG.

【0013】ノイズ減衰に要求される周波数の必要帯域
とその時の必要なインピーダンスZ(R)を前記図3の
(a)と同じとして、図4の(a)に示すように、巻数
が少ないインダクタのf−Z曲線では、Z(R)の最大
値は十分であるが、Z曲線の山がするどすぎてとりきれ
ない領域4ができている。そこで図4の(b)のように
巻数を増し、Z(R)を大きくすると、必要なf−Z
(R)領域が確保される。
Assuming that the required band of the frequency required for noise attenuation and the necessary impedance Z (R) at that time are the same as those of FIG. 3A, as shown in FIG. In the fZ curve, the maximum value of Z (R) is sufficient, but an area 4 is formed where the peak of the Z curve is too small to be removed. Therefore, when the number of turns is increased and Z (R) is increased as shown in FIG.
(R) An area is secured.

【0014】しかしながら図4の(b)ではRDCやXL
が大きい上、特に透磁率の高い磁性体の場合に比してZ
(R)が大きいためZ(R)が余っている部分、必要以
上のロスが発生し、このため信号の立ち上がり(立ち下
がり)の応答性が劣化するようになる。これらはf
R =XL が高周波サイドにくるので必要な低周波までZ
(R)を伸ばすためZ(R)値を必要以上大きくとらざ
るを得ないためである。
However, in FIG. 4B, R DC and X L
Is large, and Z is particularly large compared to a magnetic material having a high magnetic permeability.
Since R (R) is large, a portion where Z (R) is surplus and loss more than necessary occurs, and as a result, the response of the rising (falling) of the signal deteriorates. These are f
R = XL is on the high frequency side, so Z is required until the required low frequency
This is because the Z (R) value must be unnecessarily large in order to extend (R).

【0015】[0015]

【考案が解決しようとする課題】以上のように、従来の
積層ノイズ除去部品においては、信号波形を無視しなま
りを避けるか、多少波形のなまりは承知の上でリンギン
グを避けるかは使用する側の判断でいずれかを選択し、
共に満足するものはないと無いという課題があった。
As described above, in the conventional laminated noise elimination component, whether the signal waveform is ignored and the rounding is avoided or the ringing is avoided with some knowledge of the waveform rounding depends on the side to be used. Choose one at your discretion,
There was a problem that there was no satisfaction with both.

【0016】 本考案は電気信号をなまらせるノイズや
電気信号をリンギングするノイズなどを取り除く目的か
ら開発されたものである。すなわち本考案の目的は簡単
にノイズを除去できる積層ノイズ除去部品を提供するこ
とにある。言い換えると本考案の目的は必要なノイズ除
去帯域をほぼ正確にカバーするロスの少ない積層ノイズ
除去部品を提供することにある。
The present invention has been developed for the purpose of removing noise that blunts an electric signal and noise that rings an electric signal. That is, an object of the present invention is to provide a laminated noise removing component that can easily remove noise. In other words, an object of the present invention is to provide a low-loss laminated noise elimination component that covers a required noise elimination band almost exactly.

【0017】[0017]

【課題を解決するための手段】 本考案者は従来の積層
ノイズ除去部品が単一種の磁性体で構成されていて必要
なノイズ除去帯域をカバーするためにはロスが大きいこ
とを知った。鋭意研究の結果、本考案者は透磁率の異な
る複数の磁性体でコイル導体を覆うようにした積層ノイ
ズ除去部品を開発した。したがって開発された積層ノイ
ズ除去部品の全体インピーダンスZのピーク周波数fは
透磁率の異なる複数の磁性体それぞれの各Zのピーク周
波数fの間に位置することになる。言い換えると開発さ
れた積層ノイズ除去部品のZ−f曲線のピークがブロー
ドになると共にZ−f曲線の立ち上がりが急峻になるこ
とになる。この結果、必要なノイズ除去帯域をほぼ正確
にカバーするロスの少ない積層ノイズ除去部品が得られ
ることを見出し本考案に到達した。
Means for Solving the Problems The present inventor has found that a conventional laminated noise elimination component is composed of a single kind of magnetic material, and that loss is large in order to cover a required noise elimination band. As a result of diligent research, the present inventor has developed a multilayer noise elimination component in which a coil conductor is covered with a plurality of magnetic materials having different magnetic permeability. Therefore, the peak frequency f of the total impedance Z of the developed laminated noise elimination component is located between the Z peak frequencies f of the plurality of magnetic materials having different magnetic permeability. In other words, the peak of the Zf curve of the developed laminated noise removing component becomes broad and the rise of the Zf curve becomes steep. As a result, the inventors have found that a laminated noise elimination component with a small loss that covers the required noise elimination band almost accurately can be obtained, and reached the present invention.

【0018】 したがって本考案は、セラミックの積層
体内に導体をコイル状に形成して当該導体の各端を前記
積層体の表面に導出した積層ノイズ除去部品であって当
該セラミック積層体が少なくとも、第1の透磁率ならび
に第1の導体ターン数を有して周波数変化による第1の
インピーダンス・ピークを持つ第1のセラミック積層部
と、第2の透磁率ならびに第2の導体ターン数を有して
周波数変化による第2のインピーダンス・ピークを持つ
第2のセラミック積層部と、を備えていることを特徴と
した積層ノイズ除去部品を提供するものである。
Therefore, the present invention is a laminated noise elimination component in which a conductor is formed in a coil shape in a ceramic laminate and each end of the conductor is led out to the surface of the laminate, wherein the ceramic laminate is at least a ceramic laminate. A first ceramic laminate having a first magnetic permeability and a first number of conductor turns and having a first impedance peak due to frequency change; and a second magnetic permeability and a second number of conductor turns. And a second ceramic laminated portion having a second impedance peak due to a frequency change.

【0019】[0019]

【作用】上述のように本考案の積層ノイズ除去部品では
異なる透磁率を有する複数の磁性体がコイル導体の周囲
を覆うことになる。したがって積層ノイズ除去部品のZ
−f曲線におけるインピーダンスZのピーク周波数fは
異なる材質の各Zのピーク周波数fの間に位置するよう
になる。このため本考案積層ノイズ除去部品のZ−f曲
線のピークがブロードになると共にZ−f曲線の立ち上
がりが急峻になる。すなわち本考案はZ−f曲線とノイ
ズ除去帯域との重なりが密になってロスの少ない積層ノ
イズ除去部品となる。
As described above, in the laminated noise elimination component of the present invention, a plurality of magnetic materials having different magnetic permeability cover the periphery of the coil conductor. Therefore, the Z
The peak frequency f of the impedance Z in the −f curve is located between the peak frequencies f of the respective materials Z of different materials. Therefore, the peak of the Zf curve of the laminated noise elimination component of the present invention becomes broad and the rise of the Zf curve becomes steep. That is, in the present invention, the overlap between the Zf curve and the noise elimination band is increased, and the laminated noise elimination component with less loss is obtained.

【0020】以上の作用効果を図1の(a)〜(d)に
より詳しく説明する。図1の(a)は前記図3の(a)
の場合と同じくノイズ減衰に要求される周波数の必要帯
域fn とその時の必要なインピーダンスを示すものであ
り図1の(b)に示すように、材質2として比較的高い
透磁率(μ=800)の磁性体を選び3ターンの導体を
内設した時のZ−f曲線では、材質2部分のZ(R)へ
の寄与は主に低周波域ノイズを減衰し、一方低い透磁率
(μ=120)の磁性体からなり2ターンの導体を内設
した時のZ−f曲線では、図1の(c)に見られるよう
に、材質1の部分のZ(R)への寄与は主に高周波域ノ
イズを減衰していることがわかる。
The above operation and effect will be described in detail with reference to FIGS. FIG. 1A shows the state of FIG.
And shows the necessary impedance at that time required band f n of frequencies also required to noise attenuation in the case of, as shown in (b) of FIG. 1, a relatively high permeability as the material 2 (mu = 800 In the Zf curve when the magnetic material of (3) is selected and a three-turn conductor is internally provided, the contribution of the material 2 to Z (R) mainly attenuates low-frequency noise while lowering magnetic permeability (μ) = 120), the Z-f curve when a two-turn conductor is internally provided, as shown in FIG. 1C, the contribution of the material 1 to Z (R) is mainly It can be seen that high frequency noise is attenuated.

【0021】上記材質1の積層体上に材質2の積層体を
重ねて一体化して5ターンの積層体にすると、図1の
(d)のに見られるように、巻数5ターンを保ったまま
必要な周波数帯域全体で必要なZ(R)値をクリアして
いて、Z−f曲線からわかるように余分なZが少なく、
前述のように信号の立ち上がり立ち下がり応答性がよ
く、従来例のような巻数の増加がないので、RDCやXL
が増大せず、信号ロスが少ない。
When the laminate of the material 2 is laminated on the laminate of the material 1 and integrated to form a 5-turn laminate, the number of turns is maintained at 5 as shown in FIG. The necessary Z (R) value has been cleared in the entire required frequency band, and as can be seen from the Z-f curve, there is little extra Z,
Since responsiveness rise and fall of the signal as described above is good, increase the number of turns is not as in the prior art, R DC and X L
Does not increase, and the signal loss is small.

【0022】[0022]

【実施例1】前記図1の(a)〜(d)は本実施例に用
いられた積層ノイズ除去部品の特性を示すZ−f曲線図
であって、これらを参照して以下説明する。
Embodiment 1 FIGS. 1 (a) to 1 (d) are Zf curve diagrams showing the characteristics of the laminated noise elimination component used in this embodiment, which will be described below with reference to these figures.

【0023】透磁率120のフェライト原料を有機バイ
ンダと混練して厚み50μmの第1のフェライトグリー
ンシートを、また透磁率800のフェライト原料を有機
バインダと混練して厚み50μmの第2のフェライトグ
リーンシートを形成した。
A ferrite raw material having a magnetic permeability of 120 is kneaded with an organic binder to form a first ferrite green sheet having a thickness of 50 μm, and a ferrite raw material having a magnetic permeability of 800 is kneaded with an organic binder to form a second ferrite green sheet having a thickness of 50 μm. Was formed.

【0024】第1のグリーンシートと第2のグリーンシ
ートとに積層してコイルを形成するコイル導体パターン
をスクリーン印刷し、第1グリーンシートを複数枚重
ね、その上に複数枚の第2グリーンシートを重ね、上下
にそれぞれカバーシートを重ねて圧着し、第1グリーン
シートで2ターン、第2グリーンシードで3ターンのコ
イルをスルーホール接続して5ターンのコイルを内設
し、コイル導体端末を素体端面に導出した積層体を得
た。
A coil conductor pattern for forming a coil by laminating the first green sheet and the second green sheet is screen-printed, a plurality of first green sheets are stacked, and a plurality of second green sheets are stacked thereon. The first green sheet has two turns, the second green seed has three turns, and the coil has three turns, and a five-turn coil is internally provided. A laminate led to the end face of the element was obtained.

【0025】これを焼成し、該積層体の端面に外部端子
電極を形成して前記コイル導体端末を該外部端子電極に
接続した。得られた積層ノイズ除去部品の透過斜視図を
図6に示す。
This was fired to form an external terminal electrode on the end face of the laminate, and the coil conductor terminal was connected to the external terminal electrode. FIG. 6 shows a transparent perspective view of the obtained laminated noise removing component.

【0026】低透磁率を有する材質1の積層体の上に高
透磁率を有する材質2の積層体が重ねられており、端面
に平行な断面図を図8に示す。同図の(a)は材質1と
2に内設されて周回する内部導体が近接している例であ
り、同図の(b)は同じく材質1と2の周回部分が離れ
ている例である。
FIG. 8 is a cross-sectional view of a laminate of a material 2 having a high magnetic permeability superposed on a laminate of a material 1 having a low magnetic permeability, and being parallel to the end face. (A) of the same figure is an example in which the inner conductors circulating around the materials 1 and 2 are close to each other, and (b) of the same figure is an example in which the circulating portions of the materials 1 and 2 are also separated. is there.

【0027】この積層ノイズ除去部品でノイズを除去す
ると、図1の(d)に示されているように、信号波形の
なまりもなく、リンギングの少ない波形が得られた。
When the noise was removed by the laminated noise removing component, a signal waveform was not rounded and a waveform with little ringing was obtained as shown in FIG. 1D.

【0028】[0028]

【実施例2】図5の(a)〜(e)は本実施例において
用いられた3種の異なる材質からなる積層ノイズ除去部
品の特性を示すZ−f曲線図であって、これらを参照し
て以下説明する。
Embodiment 2 FIGS. 5 (a) to 5 (e) are Zf curve diagrams showing characteristics of a laminated noise elimination component made of three different materials used in this embodiment. This will be described below.

【0029】前記実施例1においては2つの異なる透磁
率を有する磁性体を積層して積層ノイズ除去部品を形成
したが、本実施例では低い透磁率をもつ材質1の磁性体
と高い透磁率をもつ材質2の磁性体、およびその中間の
透磁率を持つ材質3の磁性体からなる3つの異なる透磁
率を有する磁性体をぞぞれ用意し、材質1の積層体中を
1ターン、材質3の積層体中を1ターン、および材質2
の積層体中を3ターンのコイル導体が周回するように各
積層体を下から1、3、2の順序に重ねて圧着した後、
実施例1の要領に従い積層ノイズ除去部品を得た。
In the first embodiment, a laminated noise elimination component is formed by laminating two magnetic materials having different magnetic permeability. In this embodiment, a magnetic material of material 1 having a low magnetic permeability and a high magnetic permeability are used. A magnetic material having a material 2 and a magnetic material having a material 3 having an intermediate magnetic permeability are prepared, and three magnetic materials having different magnetic permeability are prepared. One turn in the laminate and material 2
After laminating each laminate in the order of 1, 3, and 2 from the bottom so that the coil conductor of three turns goes around in the laminate of
According to the procedure of Example 1, a laminated noise removing component was obtained.

【0030】図7は得られた該部品の透過斜視図、図9
の(b)はその端面に平行な断面図である。なお図9の
(a)は材質1と2の間に磁性/非磁性材からなる材質
3が配置されている例、同図の(c)は材質が同じ磁性
体の間に違った材質のものをはさみ込んだ例、また同図
の(d)は3材質にわたって周回するコイル導体部分の
うち一部が近接しており、一部が離れている例である。
FIG. 7 is a transparent perspective view of the obtained part, and FIG.
(B) is a sectional view parallel to the end face. FIG. 9A shows an example in which a material 3 made of a magnetic / non-magnetic material is disposed between the materials 1 and 2, and FIG. (D) of the same figure is an example in which a part of a coil conductor portion circling over three materials is close to and partly apart.

【0031】実施例1において図1の(a)に示したノ
イズ減衰に要求される必要帯域よりもさらに広くした場
合に対する本実施例の適用について説明する。
The application of the present embodiment to the case where the required band required for noise attenuation shown in FIG. 1A is further widened in the first embodiment will be described.

【0032】すなわち、図5の(a)において白抜き矢
印の方向にふえた帯域7が加算される場合、積層ノイズ
除去部品を構成する各材質の部分のそれぞれのZ(R)
への寄与は材質2については図5の(b)に、材質3に
ついては図5の(c)に、および材質1については図5
の(d)に示す通りであって、各々Z曲線ではノイズを
取り切れない領域4が存在したが、これら材質1、2お
よび3を積層して形成された5ターンの積層体ではその
Z曲線は図5の(e)に見られるように、ふえた帯域を
も含めた必要な周波数帯域で必要なZ(R)値をカバー
し、かつZ曲線の形状も良好であるので、材質数を増や
すことによってさらに広い帯域のノイズを吸収できるこ
とを示している。
That is, when the band 7 added in the direction of the white arrow in FIG. 5A is added, each Z (R) of each material portion constituting the laminated noise removing component is added.
5 (b) for material 2, FIG. 5 (c) for material 3, and FIG.
(D), there was a region 4 in which noise could not be completely removed in each Z curve, but in a five-turn laminate formed by laminating these materials 1, 2 and 3, the Z curve As shown in FIG. 5 (e), the required Z (R) value is covered in the required frequency band including the overfilled band, and the shape of the Z curve is good. It shows that noise of a wider band can be absorbed by increasing the noise.

【0033】[0033]

【考案の効果】 以上、説明したように本考案は一磁性
体の材質で形成された積層ノイズ除去部品における問題
点を解決した。すなわち本考案は異なる透磁率を有する
複数の磁性体の組み合わせで一体化した積層体によって
コイル導体を覆うことを特徴とする。この結果、本考案
による積層ノイズ除去部品のZ−f曲線のピークがブロ
ードになると共にZ−f曲線の立ち上がりが急峻になる
ことになる。したがって本考案によると必要なノイズ除
去帯域をほぼ正確にカバーするロスの少ない積層ノイズ
除去部品が得られる。かくして本考案によるロスの少な
いノイズ除去部品は発熱が少ないため高密度実装が可能
になるなど小形化に貢献する効果は大きい。
[Effects of the Invention] As described above, the present invention has solved the problem of the laminated noise removing component formed of a single magnetic material. That is, the present invention is characterized in that the coil conductor is covered by a laminated body integrated by a combination of a plurality of magnetic materials having different magnetic permeability. As a result, the peak of the Zf curve of the laminated noise elimination component according to the present invention becomes broad and the rise of the Zf curve becomes steep. Therefore, according to the present invention, it is possible to obtain a low-loss laminated noise elimination component that covers the required noise elimination band almost accurately. Thus, the noise elimination component having a small loss according to the present invention has a large effect of contributing to miniaturization such as high density mounting is possible because of little heat generation.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本考案の一実施例に用いられた2種の異なる材
質からなる積層ノイズ除去部品の特性を示すZ−f線図
である。
FIG. 1 is a Zf diagram showing characteristics of a laminated noise elimination component made of two different materials used in an embodiment of the present invention.

【図2】同図の(a)〜(c)はノイズが重畳したとき
の信号波形の例である。
FIGS. 2A to 2C are examples of signal waveforms when noise is superimposed.

【図3】従来の比較的透磁率の高い単一磁性体で構成さ
れた積層ノイズ除去部品の特性を示すZ−f線図であ
る。
FIG. 3 is a Zf diagram showing characteristics of a conventional laminated noise elimination component composed of a single magnetic body having a relatively high magnetic permeability.

【図4】従来の比較的透磁率の低い単一磁性体で構成さ
れた積層ノイズ除去部品の特性を示すZ−f線図であ
る。
FIG. 4 is a Zf diagram showing the characteristics of a conventional laminated noise elimination component made of a single magnetic material having a relatively low magnetic permeability.

【図5】本考案の別の実施態様において用いられた3種
の異なる材質からなる積層ノイズ除去部品の特性を示す
Z−f線図である。
FIG. 5 is a Zf diagram showing characteristics of a laminated noise elimination component made of three different materials used in another embodiment of the present invention.

【図6】2種の異なる材質からなる本考案積層ノイズ除
去部品の透過斜視図である。
FIG. 6 is a transparent perspective view of the laminated noise elimination component of the present invention made of two different materials.

【図7】3種の異なる材質からなる本考案積層ノイズ除
去部品の透過斜視図である。
FIG. 7 is a transparent perspective view of the laminated noise elimination component of the present invention made of three different materials.

【図8】同図の(a)および(b)は図6に示した積層
ノイズ除去部品の端面に平行な断面図である。
8 (a) and 8 (b) are cross-sectional views parallel to the end faces of the laminated noise elimination component shown in FIG. 6;

【図9】同図の(a)〜(d)は図7に示した積層ノイ
ズ除去部品の端面に平行な断面図である。
9 (a) to 9 (d) are cross-sectional views parallel to the end faces of the laminated noise elimination component shown in FIG. 7;

【符号の説明】[Explanation of symbols]

1 材質1からなる積層体 2 材質2からなる積層体 3 材質3からなる積層体 4 とりきれない領域 5 内部導体パターン 6 外部端子電極 7 ふえた領域 REFERENCE SIGNS LIST 1 Laminated body made of material 1 2 Laminated body made of material 2 3 Laminated body made of material 3 4 Unremovable area 5 Internal conductor pattern 6 External terminal electrode 7 Overfilled area

Claims (1)

(57)【実用新案登録請求の範囲】(57) [Scope of request for utility model registration] 【請求項1】 セラミックの積層体内に導体をコイル状
に形成して当該導体の各端を前記積層体の表面に導出し
た積層ノイズ除去部品であって当該セラミック積層体が
少なくとも、 第1の透磁率ならびに第1の導体ターン数を有して周波
数変化による第1のインピーダンス・ピークを持つ第1
のセラミック積層部と、 第2の透磁率ならびに第2の導体ターン数を有して周波
数変化による第2のインピーダンス・ピークを持つ第2
のセラミック積層部と、 を備えていることを特徴とした積層ノイズ除去部品。
1. A laminated noise removing component in which a conductor is formed in a coil shape in a ceramic laminate and each end of the conductor is led out to the surface of the laminate, wherein the ceramic laminate has at least a first transparent member. A first having a first impedance peak due to frequency change having a magnetic susceptibility and a first number of conductor turns;
A second laminated body having a second permeability peak and a second impedance peak due to a frequency change having a second magnetic permeability and a second number of conductor turns.
A multilayer noise elimination component comprising: a ceramic laminated portion;
JP1993024392U 1993-03-10 1993-04-13 Multilayer noise removal components Expired - Lifetime JP2605565Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1993024392U JP2605565Y2 (en) 1993-03-10 1993-04-13 Multilayer noise removal components

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP5-16322 1993-02-03
JP1632293 1993-03-10
JP1993024392U JP2605565Y2 (en) 1993-03-10 1993-04-13 Multilayer noise removal components

Publications (2)

Publication Number Publication Date
JPH0682822U JPH0682822U (en) 1994-11-25
JP2605565Y2 true JP2605565Y2 (en) 2000-07-24

Family

ID=26352647

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1993024392U Expired - Lifetime JP2605565Y2 (en) 1993-03-10 1993-04-13 Multilayer noise removal components

Country Status (1)

Country Link
JP (1) JP2605565Y2 (en)

Also Published As

Publication number Publication date
JPH0682822U (en) 1994-11-25

Similar Documents

Publication Publication Date Title
JP3941508B2 (en) Multilayer impedance element
JP3039538B1 (en) Multilayer inductor
JP3058164B1 (en) Multilayer inductor
US6498553B1 (en) Laminated type inductor
US20020140539A1 (en) Laminated impedance device
JP2002246244A (en) Choke coil
JP2007027445A (en) Laminated common mode choke coil
JP3549286B2 (en) Multilayer noise suppression components
US10586647B2 (en) Electronic component
WO2002073641A1 (en) Inductor part, and method of producing the same
JP2011004324A (en) Laminated composite filter
JP2605565Y2 (en) Multilayer noise removal components
JP2009088329A (en) Coil component
JP2005012072A (en) Laminated common mode choke coil and its manufacturing method
JP4317179B2 (en) Multilayer filter
JP3204249B2 (en) Multilayer inductor
JP3089832B2 (en) Composite inductor components
JP2006041820A (en) Multilayer filter array
JP2002208515A (en) Laminated inductor
JPH11111541A (en) Unequally split inductor device
JPH07192925A (en) Bead inductor
JPH05326270A (en) Composite inductor part
JP2006140807A (en) Filter element
JP2004311830A (en) Stacked common mode choke coil and its manufacturing method
JPH0411709A (en) Common mode choke coil

Legal Events

Date Code Title Description
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20000425