JP2003297641A - Electronic component for communications equipment superior in thdf characteristic, and its thdf reducing method - Google Patents

Electronic component for communications equipment superior in thdf characteristic, and its thdf reducing method

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Publication number
JP2003297641A
JP2003297641A JP2002102652A JP2002102652A JP2003297641A JP 2003297641 A JP2003297641 A JP 2003297641A JP 2002102652 A JP2002102652 A JP 2002102652A JP 2002102652 A JP2002102652 A JP 2002102652A JP 2003297641 A JP2003297641 A JP 2003297641A
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JP
Japan
Prior art keywords
magnetic core
thd
characteristic
electronic component
thdf
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
JP2002102652A
Other languages
Japanese (ja)
Other versions
JP2003297641A5 (en
Inventor
Katsuyuki Kiguchi
勝之 城口
Keiji Otani
圭治 大谷
Tokukazu Koyuhara
徳和 小湯原
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.)
Proterial Ltd
Original Assignee
Hitachi Metals 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
Application filed by Hitachi Metals Ltd filed Critical Hitachi Metals Ltd
Priority to JP2002102652A priority Critical patent/JP2003297641A/en
Publication of JP2003297641A publication Critical patent/JP2003297641A/en
Publication of JP2003297641A5 publication Critical patent/JP2003297641A5/ja
Pending legal-status Critical Current

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Abstract

<P>PROBLEM TO BE SOLVED: To provide an electronic component for communications equipment which is superior in a THDF characteristic by making a distortion of output waveform to an input wave small, and to provide a method for easily reducing the THDF characteristic. <P>SOLUTION: The electronic component is provided with a magnetic core with leg, forming an external leg and an internal leg, a magnetic core matched with the magnetic core with the leg, and a winding arranged in the internal leg. Center line average roughness Ra of the matched face of the magnetic core with the leg and the magnetic core is 1.2 μm or smaller. <P>COPYRIGHT: (C)2004,JPO

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、xDSL用通信機
器の伝送トランス、フィルタに使用される通信機器用電
子部品であって、特に信号が磁心を通過する際に発生す
る波形歪の少ない、THD特性に優れた通信機器用電
子部品およびそのTHD特性低減方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a communication device electronic component used for a transmission transformer and a filter of a communication device for xDSL, and particularly, a THD having a small waveform distortion generated when a signal passes through a magnetic core. The present invention relates to an electronic component for communication equipment having excellent F characteristics and a THD F characteristic reducing method thereof.

【0002】[0002]

【従来の技術】従来高透磁率を有するMn−Zn系フェ
ライトは各種トランス、フィルタ、xDSLモデム等の
通信機器用電子部品に使用されているが、通信機器用電
子部品の磁心として用いられるフェライトには高透磁率
であることに加えて、通信信号が通信機器用電子部品を
通過する際に発生する波形歪が少ないことが要求され
る。
2. Description of the Related Art Conventionally, Mn-Zn type ferrite having a high magnetic permeability has been used for electronic components for communication equipment such as various transformers, filters and xDSL modems. Is required to have a high magnetic permeability and to have a small waveform distortion when a communication signal passes through an electronic component for communication equipment.

【0003】[0003]

【発明が解決しようとする課題】特に高速・大容量の通
信に対応したADSL(Asymmetric Dig
ital Subscriber Line)に代表さ
れるxDSL用通信機器に使用される磁心においては、
信号が通過する際に発生する信号波形の歪が、情報伝送
の際にエラーレートの増加を招くため、信号が出力する
際の波形歪のよりいっそうの低減が要求され、その主要
部材であるフェライト磁心の特性の改善が求められてい
る。
SUMMARY OF THE INVENTION ADSL (Asymmetric Metric Dig) especially for high-speed and large-capacity communication
In the magnetic core used in the communication device for xDSL represented by ital Subscriber Line),
Since the distortion of the signal waveform that occurs when the signal passes causes an increase in the error rate during information transmission, it is necessary to further reduce the waveform distortion when the signal is output. Improvements in magnetic core characteristics are required.

【0004】例えば、信号が磁心を通過する際に発生す
る出力波形の歪は、入力する基本波に対する三次高調波
を中心とした高調波成分が出力基本波に含まれることに
より生じる。それは磁界Hと磁束密度Bの非線形性・ヒ
ステリシスカーブ特性に起因すると考えられる。実用的
には、かかる出力波形の歪に対して磁心にギャップを設
けて、実効透磁率を下げることにより線形性を改善し、
通信用トランスなどとして用いているのが現状である。
しかし、かかる方法では保磁力低減等のBHループの線
形性の本質的な改善には至っておらず、また必要なイン
ダクタンスを得るためには巻線数の増加という負荷を伴
うといった問題があった。そのためxDSL用通信機器
に使用されるフェライト磁心そのものの改善によるさら
なる低歪化が必要とされていた。
For example, the distortion of the output waveform that occurs when a signal passes through the magnetic core is caused by the fact that the output fundamental wave contains a harmonic component centered on the third harmonic of the input fundamental wave. It is considered that this is due to the non-linearity / hysteresis curve characteristics of the magnetic field H and the magnetic flux density B. Practically, the linearity is improved by providing a gap in the magnetic core for the distortion of the output waveform and reducing the effective magnetic permeability.
It is currently used as a communication transformer.
However, such a method has not been able to substantially improve the linearity of the BH loop such as reduction of coercive force, and has a problem that a load of increasing the number of windings is required to obtain a required inductance. Therefore, it has been necessary to further reduce the distortion by improving the ferrite core itself used in the communication device for xDSL.

【0005】本発明は上記問題を解決するために鋭意検
討した結果見いだされたものであり、入力波に対する出
力波形の歪の小さい、THD特性に優れた通信機器用
電子部品と、容易にTHD特性を低減する方法を提供
することを目的とする。
The present invention has been discovered as a result of intensive studies for solving the above problems, and it is an electronic component for communication equipment which has a small distortion of an output waveform with respect to an input wave and is excellent in THD F characteristics, and THD easily. An object is to provide a method of reducing the F characteristic.

【0006】[0006]

【課題を解決するための手段】第1の発明は、外脚と内
脚とを形成した脚付磁心と、当該脚付磁心と突き合わせ
る磁心と、前記内脚に配置される巻線を備え、前記脚付
磁心と前記磁心の突き合わせ面の中心線平均あらさRa
が1.2μm以下であるTHD特性に優れた通信機器
用電子部品である。本発明において、THD特性が印
加磁束密度50mT、周波数10kHz、温度25℃に
おいて−100dB以下であることが好ましい。そし
て、前記脚付磁心及び前記磁心の温度25℃における初
透磁率μiが3,000以上のフェライト材料を用いるこ
とがより好ましい。初透磁率が3,000未満であると
巻線数増加に起因する損失が増加するので好ましくな
い。第2の発明は、外脚と内脚とを形成した脚付磁心
と、当該脚付磁心と突き合わせる磁心と、前記内脚に配
置される巻線を備えた通信用電子部品において、前記脚
付磁心と前記磁心の突き合わせ面の中心線平均あらさR
aを1.2μm以下とする通信機器用電子部品のTHD
特性低減方法である。
According to a first aspect of the present invention, there is provided a legged magnetic core having an outer leg and an inner leg, a magnetic core abutting the legged magnetic core, and a winding disposed on the inner leg. , The center line average roughness Ra of the abutting surface of the magnetic core with legs and the magnetic core
Is 1.2 μm or less, which is an electronic component for communication equipment excellent in THD F characteristics. In the present invention, it is preferable that the THD F characteristic is −100 dB or less at an applied magnetic flux density of 50 mT, a frequency of 10 kHz and a temperature of 25 ° C. It is more preferable to use the legged magnetic core and a ferrite material having an initial magnetic permeability μi of 3,000 or more at a temperature of 25 ° C. of the magnetic core. If the initial magnetic permeability is less than 3,000, the loss due to the increase in the number of windings increases, which is not preferable. A second aspect of the present invention is a communication electronic component including a legged magnetic core having an outer leg and an inner leg, a magnetic core that abuts the legged magnetic core, and a winding disposed on the inner leg, wherein the leg is provided. Centerline average roughness R of the magnetic core and the abutting surface of the magnetic core
THD of electronic parts for communication equipment with a of 1.2 μm or less
This is an F characteristic reduction method.

【0007】[0007]

【発明の実施の形態】以下本発明を実施例によって具体
的に説明するが、本発明はこれらの実施例によって限定
されるものではない。
BEST MODE FOR CARRYING OUT THE INVENTION The present invention will be specifically described below with reference to examples, but the present invention is not limited to these examples.

【0008】本発明において出力波形の歪量を示す指標
として用いているTHD特性について説明する。TH
D(Total Harmonic Distorti
on総高調波歪)は基本波Vb(V)に対する高調波成
分Vh(V)の比であり、次式で与えられる。 THD=20×LOG10(Vh/Vb) [dB] ここで前記μaは振幅透磁率である。高調波成分の割合
を振幅透磁率μaで除した値THD/μaは次式により
得る。 THD/μa=20×LOG10((Vh/Vb)/μ
a) [dB] THD値をμaで除した値としているのは、例えばPr
oceedingsof The Eighth Int
ernational Conference on
Ferrite、509、2000にあるように、ギャ
ップ形成等によるμa変化がTHDへ与える影響を除い
て材料固有の評価をするためである。本発明では、さら
に巻線数、回路抵抗、インダクタンスなどのファクター
の影響を除くように、以下に示すDistortion
of Transformer Coefficie
nt(DTC)を用いた。
The THD F characteristic used as an index indicating the distortion amount of the output waveform in the present invention will be described. TH
D (Total Harmonic Distorti
on total harmonic distortion) is the ratio of the harmonic component Vh (V) to the fundamental wave Vb (V) and is given by the following equation. THD = 20 × LOG 10 (Vh / Vb) [dB] where μa is the amplitude permeability. A value THD / μa obtained by dividing the ratio of harmonic components by the amplitude permeability μa is obtained by the following equation. THD / μa = 20 × LOG 10 ((Vh / Vb) / μ
a) [dB] The value obtained by dividing the THD value by μa is, for example, Pr.
ocedingsof The Eight Int
international Conference on
This is because, as described in Ferrite, 509, 2000, the evaluation peculiar to the material is performed by excluding the influence of the μa change due to the gap formation or the like on THD. In the present invention, in order to further eliminate the influence of factors such as the number of windings, circuit resistance, and inductance, the following Distortion
of Transformer Coeffie
nt (DTC) was used.

【0009】[0009]

【数1】 [Equation 1]

【0010】そして、前記DTCとTHD/μaとで得
られ、次式で求められるTHD特性を磁心特性の指標
とした。これにより、実製品の形状・仕様の影響を極力
排除して磁心特性の評価を行うことが出来る。 THD=THD/μa+20×LOG10(1/DT
C) [dB] ここで、かかるTHD特性は小さいほど出力波形の歪
量が少ないことを示す。なおADSLの使用周波数は2
0kHz〜1.1MHzであるが、前記THDの測定に
使用するオーディオアナライザーはその周波数範囲の低
周波数側の一部しかカバーしていないうえ、かかる範囲
でも十分な精度が得られない場合があるため、本発明に
おいては前記THDの測定の周波数を便宜上10kHz
として評価した。
The THD F characteristic obtained by the above DTC and THD / μa and obtained by the following equation was used as an index of the magnetic core characteristic. This makes it possible to evaluate the magnetic core characteristics while eliminating the influence of the shape and specifications of the actual product as much as possible. THD F = THD / μa + 20 × LOG 10 (1 / DT
C) [dB] Here, it is shown that the smaller the THD F characteristic, the smaller the distortion amount of the output waveform. The frequency used by ADSL is 2
Although it is 0 kHz to 1.1 MHz, the audio analyzer used for the measurement of the THD covers only a part of the low frequency side of the frequency range, and sufficient accuracy may not be obtained even in this range. In the present invention, the THD measurement frequency is conveniently set to 10 kHz.
Evaluated as.

【0011】また、THD特性の値は印加磁束密度が
増加するにつれて大きくなるが、実用される際の水準か
ら本発明では50mTとした。すなわち、THD特性
の値は測定周波数、磁束密度によって異なり一義的でな
いため、本発明におけるTHD特性は上記測定条件に
おける値を用い、磁心評価の基準とした。
Although the value of the THD F characteristic increases as the applied magnetic flux density increases, it is set to 50 mT in the present invention from the level of practical use. That is, since the value of the THD F characteristic differs depending on the measurement frequency and the magnetic flux density and is not unique, the THD F characteristic in the present invention uses the value under the above-mentioned measurement conditions and is used as a reference for magnetic core evaluation.

【0012】また、本発明におけるTHD特性の評価
は室温状態(25℃)で行った。周波数10kHz、印
加磁束密度50mTの測定条件で、THD特性が−1
00dB以下であれば、実機での情報伝送のエラーレー
トが改善され実用上十分な水準とすることができること
を本発明者らは研究の中で見出しており、これをTHD
特性の良否判断のしきい値とした。
The THD F characteristics of the present invention were evaluated at room temperature (25 ° C.). THD F characteristic is -1 under the measurement conditions of frequency 10 kHz and applied magnetic flux density 50 mT.
The inventors have found in research that the error rate of information transmission in an actual device can be improved to a practically sufficient level if it is at most 00 dB, and this has been found in THD.
The threshold value was used as a threshold for judging the quality of the F characteristic.

【0013】本発明の通信機機器用電子部品の磁心材料
は、μi3,000以上であれば特に限定するものでは
ないが、当然それ自身もTHD特性が小さな材料であ
ることが望まれる。その磁心材料として、例えば、透磁
率8,000〜15,000程度のフェライト材料にお
いて、その主成分組成を、Fe換算で52.0〜
54.0モル%、より好ましくは52.0〜53.0モ
ル%、ZnO換算で22.0〜25.0モル%、残部酸
化マンガンとするMn−Zn系フェライトとするのが好
ましい。上記のように主成分範囲を限定したのは以下の
理由による。主成分であるFe、ZnOおよび酸
化マンガンの比を変化させることによってキュリー温度
(Tc)および初透磁率μiが極大を示すいわゆるセカ
ンダリーピーク温度(Ts)を制御することができる
が、本発明において波形歪の指標としているTHD
性も上記主成分比によってその温度変化を制御すること
ができる。すなわちTHD特性の温度変化はμiの温
度変化と連動し、μiのセカンダリーピーク温度(T
s)で極小となる。THD特性はセカンダリーピーク
温度を超えると温度上昇に伴って増加した後、キュリー
温度(Tc)に向かって再び減少する。このTsとTc
の温度差が大きくなればなるほど、TsとTc間でのT
HDの増加が大きくなる。例えば透磁率8,000〜
15,000程度のフェライト材料において、0℃〜8
5℃という実用的な温度範囲で安定したTHD特性を
得るには、これらTsおよびTcを一定の範囲に制御す
る必要があり、好ましくはTsは−20℃〜50℃かつ
Tcは90〜140℃、より好ましくはTsは0℃〜4
0℃かつTcは100℃〜130℃とするのが好まし
い。Feが52.0モル%未満であるとTsが高
温側にシフトする結果、低温でのTHD特性の増加が
顕著となり、54.0モル%を超えるとTsが低温側に
シフトする結果、TsおよびTc間でのTHD特性の
増加が大きくなるからである。より好ましくは52.0
〜53.0モル%とすることで0℃〜85℃の常用温度
域でより小さいTHD特性を得ることができる。
The magnetic core material of the electronic component for communication equipment of the present invention is not particularly limited as long as it has a μi of 3,000 or more, but it is naturally desired that the magnetic core material itself has a small THD F characteristic. As the magnetic core material, for example, in a ferrite material having a magnetic permeability of about 8,000 to 15,000, its main component composition is 52.0 to 5 in terms of Fe 2 O 3.
54.0 mol%, more preferably 52.0 to 53.0 mol%, 22.0 to 25.0 mol% in terms of ZnO, and the balance is preferably manganese oxide. The reason for limiting the main component range as described above is as follows. By changing the ratio of the main components Fe 2 O 3 , ZnO and manganese oxide, the Curie temperature (Tc) and the so-called secondary peak temperature (Ts) at which the initial permeability μi exhibits a maximum can be controlled. In the invention, the THD F characteristic, which is used as an index of waveform distortion, can also be controlled in temperature change by the above principal component ratio. That is, the temperature change of the THD F characteristic is linked with the temperature change of μi, and the secondary peak temperature (T
It becomes a minimum in s). When the THD F characteristic exceeds the secondary peak temperature, the THD F characteristic increases as the temperature rises, and then decreases again toward the Curie temperature (Tc). This Ts and Tc
The greater the temperature difference between Ts and Tc, the more T
The increase in HD F is large. For example, magnetic permeability 8,000-
For ferrite materials of about 15,000, 0 ° C-8
In order to obtain stable THD F characteristics in a practical temperature range of 5 ° C, it is necessary to control Ts and Tc within a certain range, preferably Ts is -20 ° C to 50 ° C and Tc is 90 to 140. ℃, more preferably Ts is 0 ℃ ~ 4
It is preferable that 0 ° C. and Tc are 100 ° C. to 130 ° C. When Fe 2 O 3 is less than 52.0 mol%, Ts shifts to the high temperature side, and as a result, the THD F characteristic at a low temperature increases remarkably, and when it exceeds 54.0 mol%, Ts shifts to the low temperature side. As a result, the increase of the THD F characteristic between Ts and Tc becomes large. More preferably 52.0
It is possible to obtain smaller THD F characteristics in a conventional temperature range of 0 ° C. to 85 ° C. by a ~53.0 mol%.

【0014】また、ZnOを上記範囲に限定したのは、
ZnOが22.0モル%未満であるとTcが高温側にシ
フトする結果TsおよびTc間でのTHD特性の増加
が大きくなるからであり、25.0モル%を超えるとT
cが低温側にシフトし実用温度の上限以下となり、実用
に耐えないからである。
Further, ZnO is limited to the above range because
When ZnO is less than 22.0 mol%, Tc shifts to the high temperature side, resulting in a large increase in THD F characteristic between Ts and Tc.
This is because c shifts to the low temperature side and becomes equal to or lower than the upper limit of the practical temperature, and it cannot be practically used.

【0015】また、本発明に用いるMn−Zn系フェラ
イトは副成分としてCaO換算で0〜0.3wt%のC
aを含有するのが好ましい。なお、CaOは一般にはそ
の添加によって粒界の電気抵抗を上げ、損失を低減する
効果を有する。一方、十分な磁界を印加して測定したメ
ジャ−ル−プでの保磁力は増加し、かかる保磁力の増加
はBHル−プの線形性の低下、ヒステリシス損の増加を
招くことになる。しかし、xDSL用通信機器、例えば
ADSL用モデムでは、印加磁界の小さいいわゆるレ−
リ−範囲で使用されるが、かかるマイナ−ル−プの範囲
であると考えられる50mTではCaOの添加によって
逆にHcは減少し、BHル−プの線形性が向上すること
が見出されたのである。CaOを上記範囲に限定したの
は、CaOを添加することによってTHD特性が低下
し、波形の歪を低減することができるが、CaOの含有
量が多くなるにしたがい、CaOの効果が徐々に飽和
し、特に0.3wt%を超えると焼結体の組織が不均一
になり、初透磁率の低下が大きくなるとともに、THD
特性の値も劣化するからである。したがってCaOは
0〜0.3wt%が好ましく、さらに好ましくは0.0
05wt%〜0.15wt%である。
The Mn-Zn ferrite used in the present invention contains 0 to 0.3 wt% of C, calculated as CaO, as a subcomponent.
It is preferable to contain a. Note that CaO generally has the effect of increasing the electrical resistance of the grain boundaries and reducing the loss by adding it. On the other hand, the coercive force in the measure loop measured by applying a sufficient magnetic field increases, and the increase in the coercive force causes a decrease in the linearity of the BH loop and an increase in hysteresis loss. However, in a communication device for xDSL, for example, a modem for ADSL, a so-called laser with a small applied magnetic field is used.
It has been found that Hc is decreased by addition of CaO at 50 mT, which is used in the low range and is considered to be in the range of the minor loop, and the linearity of the BH loop is improved. It was. The reason why CaO is limited to the above range is that the THD F characteristic is lowered by adding CaO and the distortion of the waveform can be reduced, but the effect of CaO gradually increases as the content of CaO increases. When it is saturated, especially when it exceeds 0.3 wt%, the structure of the sintered body becomes non-uniform, the initial permeability decreases greatly, and THD
This is because the value of the F characteristic also deteriorates. Therefore, CaO is preferably 0 to 0.3 wt%, and more preferably 0.0
It is from 05 wt% to 0.15 wt%.

【0016】また、本発明に用いるMn−Zn系フェラ
イトには初透磁率の向上、磁心損失の低減の観点からB
換算で0〜0.03wt%、SiO換算で0
〜0.02wt%、Nb換算で0〜0.05wt
%のBi、Si、Nbを含有することが好ましい。Bi
をかかる範囲に限定したのは、Biは粒成
長を促進し、初透磁率の向上に寄与するが、0.05w
t%を超えると粒成長が著しくなり、THD特性の値
が大きくなるためである。したがってBi は0〜
0.05wt%とするのが好ましく、より好ましくは0
〜0.035wt%である。
Further, the Mn-Zn-based blower used in the present invention
It has a B value from the viewpoint of improving the initial permeability and reducing core loss.
iTwoOThree0 to 0.03 wt% in conversion, SiOTwoConverted to 0
~ 0.02wt%, NbTwoO50 to 0.05 wt in conversion
% Bi, Si, Nb is preferably contained. Bi
TwoOThreeIs limited to this range by BiTwoOThreeIs grainy
Promotes length and contributes to improvement of initial permeability, but 0.05w
If t% is exceeded, grain growth will be remarkable and THDFValue of characteristic
Because it becomes larger. Therefore BiTwoO ThreeIs 0
It is preferably 0.05 wt%, more preferably 0
Is about 0.035 wt%.

【0017】また、SiOを上記範囲に限定したの
は、SiOは粒界の電気抵抗を上げ損失低減・相対損
失係数tanδ/μiの改善に寄与するが、添加量が
0.02wt%を超えると焼結時に異常粒成長が生じT
HDが大きくなるからである。したがってSiO
0〜0.02wt%が好ましく、より好ましくは0〜
0.01wt%である。
Further, SiO 2 is limited to the above range because SiO 2 contributes to increase the electrical resistance of the grain boundary to reduce loss and improve the relative loss coefficient tan δ / μi, but the addition amount is 0.02 wt%. If it exceeds, abnormal grain growth occurs during sintering and T
This is because the HD F becomes large. Therefore, SiO 2 is preferably 0 to 0.02 wt%, more preferably 0 to
It is 0.01 wt%.

【0018】また、Nbを上記範囲に限定したの
は、Nbは焼結性向上・相対損失係数tanδ/
μi改善の効果を有するが0.05wt%を超えると異
常粒成長し、その結果THD特性が著しく大きくなる
ためである。したがってNb は0〜0.05wt
%が好ましく、より好ましくは0〜0.03wt%であ
る。上述のとおり、本発明の通信機機器用電子部品に用
いる磁心材料における上記の副成分は、主にTHD
性、初透磁率μi、相対損失係数等の特性値の絶対値を
向上する目的でその含有量を制御するのが好ましい。な
お、本発明においては上記主成分、副成分以外の成分の
含有を否定するものではなく、必要に応じて上記主成
分、副成分以外の成分も含むことができる。
Also, NbTwoO5Was limited to the above range
Is NbTwoO5Is the sinterability improvement / relative loss coefficient tan δ /
It has the effect of improving μi, but is different when it exceeds 0.05 wt%.
Constant grain growth resulting in THDFCharacteristic becomes significantly large
This is because. Therefore Nb TwoO5Is 0 to 0.05 wt
%, More preferably 0 to 0.03 wt%.
It As described above, for electronic parts for communication equipment of the present invention
The above-mentioned subcomponents in magnetic core materials are mainly THDFSpecial
Property, initial magnetic permeability μi, relative loss coefficient, etc.
It is preferable to control the content for the purpose of improving. Na
In the present invention, components other than the above main component and subcomponents
It does not mean that the content is not denied, but the above main elements are
In addition, components other than the minor components can be included.

【0019】以下本発明の一実施例に係る通信機器用電
子部品について具体的に説明する。通信機器用電子部品
を構成する磁心材料として、Fe、ZnO、Mn
Oがそれぞれ、Fe 52.3mol%、ZnO
23.0mol%、MnO 24.7mol%としな
るように計量・混合しこれを850℃で2時間仮焼成し
た。これに、Biを0.035wt%、SiO
を0.002wt%、Nbを0.01wt%、C
aCOを0.01wt%含有させ、湿式ボールミルに
て5時間粉砕した。これらにバインダーを添加し、スプ
レイドライヤーで造粒後して圧縮成形し、1300℃に
て5時間、酸素濃度を制御した窒素雰囲気中で焼結し
て、図2に示すE形磁心1、及び図4に示すEP形磁心
1とした。そして、前記磁心の突き合わせ面aを、異な
る粒度を有する砥石を用いて研削し、突き合わせ面の中
心線平均あらさRaが0.4μm〜1.2μmとなるよ
うに加工した。更に、内脚2には実用上ギャップを施し
インダクタンスを調整する関係上、本発明の実施例にお
いても図2に示すE形磁心1の一方には0.35mm、
及び図4に示すEP形磁心1の一方には0.05mmの
ギャップを施した。なお、本発明においてギャップの有
無については特に限定するものではなく、またギャップ
によりTHDの絶対値が変動することもない。次に、
E形磁心の内脚2に、巻線を巻装したコイルボビン5を
組み込み、さらに前記E形磁心に突き合わせるように、
同様に形成された他のE形磁心を組み込み、ケース20
0に配置固定して、図6に示す等価回路を備え、図3の
斜視図に示す外観の通信機機器用トランスとした。また
同様にしてEP形磁心を用いて図5に斜視図として示す
通信機機器用トランスとした。これらの通信機機器用ト
ランスは、例えばxDSL用モデムに使用され、このモ
デムはデータ伝送線路において、音声信号とデジタル信
号とを分離するスプリッタとコンピュータとの間に配置
されるものであり、前記通信機機器用トランスはデジタ
ル変復調や制御回路を含むLSIと電話線との間のライ
ンカップリングなどの使用される。
An electronic component for communication equipment according to an embodiment of the present invention will be specifically described below. As core material constituting the electronic component communication equipment, Fe 2 O 3, ZnO, Mn
O is Fe 2 O 3 52.3 mol% and ZnO, respectively.
The mixture was weighed and mixed so as to be 23.0 mol% and 24.7 mol% MnO, and this was calcinated at 850 ° C. for 2 hours. To this, 0.035 wt% of Bi 2 O 3 and SiO 2
0.002 wt%, Nb 2 O 5 0.01 wt%, C
0.01 wt% of aCO 3 was contained and pulverized with a wet ball mill for 5 hours. A binder is added to these, the mixture is granulated with a spray dryer, compression molded, and sintered at 1300 ° C. for 5 hours in a nitrogen atmosphere in which the oxygen concentration is controlled to obtain the E-shaped magnetic core 1 shown in FIG. The EP magnetic core 1 shown in FIG. 4 was used. Then, the abutting surface a of the magnetic core was ground using grindstones having different grain sizes, and processed so that the centerline average roughness Ra of the abutting surface was 0.4 μm to 1.2 μm. Further, in order to adjust the inductance by practically providing a gap to the inner leg 2, one side of the E-shaped magnetic core 1 shown in FIG.
A gap of 0.05 mm is formed on one side of the EP magnetic core 1 shown in FIG. In the present invention, the presence / absence of a gap is not particularly limited, and the absolute value of THD F does not change due to the gap. next,
A coil bobbin 5 having a winding wound therein is incorporated into the inner leg 2 of the E-shaped magnetic core, and further, the coil bobbin 5 is butted against the E-shaped magnetic core.
Incorporating another E-shaped magnetic core formed in the same manner, the case 20
It was arranged and fixed at 0, and was provided with the equivalent circuit shown in FIG. 6 to provide a transformer for communication equipment having the appearance shown in the perspective view of FIG. Similarly, an EP type magnetic core was used to form a transformer for communication equipment as shown in a perspective view in FIG. These transformers for communication equipment are used, for example, in a xDSL modem, which is arranged between a computer and a splitter for separating a voice signal and a digital signal in a data transmission line. The machine transformer is used for line modulation between an LSI including a digital modulation / demodulation or control circuit and a telephone line.

【0020】得られた通信機機器用トランスの25℃に
おけるTHD特性を測定した。測定回路を図7に示
す。巻線数は、一次側(入力側)をN1、二次側(出力
側)N2とし、THDの測定はオーディオプレシジョン
社製オーディオアナライザー(System Two)
を使用して、測定周波数10kHz、測定磁束密度50
mTの評価条件とした。また磁心の突き合わせ面aの面
粗さを株式会社東京精密製サーフコム550ADを用
い、カットオフ値を0.8mmとして、中心線平均粗さ
Raを評価した。評価結果を図1および表1に、THD
測定条件を表2に示す。
The THD F characteristics at 25 ° C. of the obtained transformer for communication equipment were measured. The measurement circuit is shown in FIG. The number of windings is N1 on the primary side (input side) and N2 on the secondary side (output side), and THD is measured by an audio analyzer manufactured by Audio Precision (System Two).
Using a measuring frequency of 10 kHz, measuring magnetic flux density of 50
The evaluation condition was mT. The center line average roughness Ra was evaluated using the Surfcom 550AD manufactured by Tokyo Seimitsu Co., Ltd. for the surface roughness of the abutting surface a of the magnetic core, with the cutoff value set to 0.8 mm. The evaluation results are shown in FIG.
Table 2 shows the measurement conditions.

【0021】[0021]

【表1】 [Table 1]

【0022】[0022]

【表2】 [Table 2]

【0023】図1から明らかなように、突き合わせ面の
中心線平均あらさが小さくなるほどTHD特性が減少
し、Raが1.25μm以下であれば、−100dB以
下の優れたTHD特性が得られた。
As is clear from FIG. 1, the THD F characteristic decreases as the center line average roughness of the abutting surfaces decreases, and when Ra is 1.25 μm or less, an excellent THD F characteristic of -100 dB or less can be obtained. It was

【0024】[0024]

【発明の効果】本発明によれば、磁心を構成する磁心材
料に因らず、磁心の突き合わせ面の面精度の制御によっ
て容易にTHD特性を改善することが出来た。その結
果、入力波に対する出力波形の歪の小さい、THD
性に優れた通信機器用電子部品と、容易にTHD特性
を低減する方法を提供することが出来た。本実施例にお
いては、その磁心材料自体がTHD特性に優れたもの
であったが、THD特性に優位性を示さない他の磁心
材料であっても本発明の効果に変わりなく、換言すれば
多少THD特性の悪い磁心材料でも、磁心の突き合わ
せ面の面精度の制御によって容易にTHD特性を改善
することが出来る。
According to the present invention, the THD F characteristic can be easily improved by controlling the surface accuracy of the abutting surfaces of the magnetic cores, regardless of the magnetic core material forming the magnetic cores. As a result, a small distortion of the output waveform relative to the input wave, and electronic parts for communication equipment with excellent THD F characteristics, it was possible to provide a method for easily reducing the THD F characteristics. In this embodiment, the magnetic core material itself was excellent in THD F characteristics, be other magnetic core materials that do not exhibit superiority in THD F characteristics without changes to the effects of the present invention, in other words if even a bad core material somewhat THD F characteristics can be easily improved THD F characteristic by controlling the surface accuracy of the abutting surfaces of the magnetic core.

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

【図1】 本発明の実施例に係る磁心の中心線平均あら
さとTHDとの関係を示す図である。
FIG. 1 is a diagram showing a relationship between a center line average roughness and THD F of a magnetic core according to an example of the present invention.

【図2】 本発明に用いる磁心の一形状例を示す斜視図
である。
FIG. 2 is a perspective view showing a shape example of a magnetic core used in the present invention.

【図3】 本発明の一実施例に係るに係る通信機器用電
子部品の斜視図である。
FIG. 3 is a perspective view of an electronic component for communication equipment according to an embodiment of the present invention.

【図4】 本発明に用いる磁心の他の形状例を示す斜視
図である。
FIG. 4 is a perspective view showing another example of the shape of the magnetic core used in the present invention.

【図5】 本発明の一実施例に係るに係る他の通信機器
用電子部品の斜視図である。
FIG. 5 is a perspective view of another electronic component for communication device according to an embodiment of the present invention.

【図6】 本発明の一実施例に係るに係る通信機器用電
子部品の等価回路である。
FIG. 6 is an equivalent circuit of an electronic component for communication device according to an embodiment of the present invention.

【図7】 THDの測定評価回路図である。FIG. 7 is a THD measurement and evaluation circuit diagram.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 外脚と内脚とを形成した脚付磁心と、当
該脚付磁心と突き合わせる磁心と、前記内脚に配置され
る巻線を備え、前記脚付磁心と前記磁心の突き合わせ面
の中心線平均あらさRaが1.2μm以下であることを
特徴とするTHD特性に優れた通信機器用電子部品。
1. A legged magnetic core formed with an outer leg and an inner leg, a magnetic core that abuts on the legged magnetic core, and a winding disposed on the inner leg, and the abutment of the legged magnetic core and the magnetic core. A centerline average roughness Ra of the surface is 1.2 μm or less, which is an electronic component for communication equipment excellent in THD F characteristics.
【請求項2】 THD特性が、印加磁束密度50m
T、周波数10kHz、温度25℃において−100d
B以下であることを特徴とする請求項1に記載のTHD
特性に優れた通信機器用電子部品。
2. The THD F characteristic has an applied magnetic flux density of 50 m.
-100d at T, frequency 10 kHz, temperature 25 ° C
It is B or less, The THD of Claim 1 characterized by the above-mentioned.
Electronic components for communication equipment with excellent F characteristics.
【請求項3】 前記脚付磁心及び前記磁心の温度25℃
における初透磁率μiが3,000以上のフェライト磁性
材料を用いることを特徴とする請求項1又は2に記載の
THD特性に優れた通信機器用電子部品。
3. A temperature of the magnetic core with legs and the magnetic core of 25 ° C.
3. An electronic component for communication equipment having excellent THD F characteristics according to claim 1 or 2, characterized in that a ferrite magnetic material having an initial permeability μi of 3,000 or more is used.
【請求項4】 外脚と内脚とを形成した脚付磁心と、当
該脚付磁心と突き合わせる磁心と、前記内脚に配置され
る巻線を備えた通信用電子部品において、前記脚付磁心
と前記磁心の突き合わせ面の中心線平均あらさRaを
1.2μm以下とすることを特徴とする通信機器用電子
部品のTHD特性低減方法。
4. A communication electronic component comprising a legged magnetic core having outer and inner legs formed therein, a magnetic core abutting against the legged magnetic core, and a winding disposed on the inner leg, wherein the legged magnetic core is provided. A method for reducing THD F characteristics of an electronic component for a communication device, characterized in that a centerline average roughness Ra of a magnetic core and a surface where the magnetic core is abutted with each other is 1.2 μm or less.
JP2002102652A 2002-04-04 2002-04-04 Electronic component for communications equipment superior in thdf characteristic, and its thdf reducing method Pending JP2003297641A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
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Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2002102652A JP2003297641A (en) 2002-04-04 2002-04-04 Electronic component for communications equipment superior in thdf characteristic, and its thdf reducing method

Publications (2)

Publication Number Publication Date
JP2003297641A true JP2003297641A (en) 2003-10-17
JP2003297641A5 JP2003297641A5 (en) 2005-06-23

Family

ID=29389001

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Country Status (1)

Country Link
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006074006A (en) * 2004-08-05 2006-03-16 Sumida Corporation Magnetic element
JP2007513513A (en) * 2003-12-03 2007-05-24 サウス バンク ユニバーシティー エンタープライジズ リミテッド DSL modem and transformer

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007513513A (en) * 2003-12-03 2007-05-24 サウス バンク ユニバーシティー エンタープライジズ リミテッド DSL modem and transformer
JP2006074006A (en) * 2004-08-05 2006-03-16 Sumida Corporation Magnetic element

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