JPH05217753A - Method for trimming composite electronic component - Google Patents

Method for trimming composite electronic component

Info

Publication number
JPH05217753A
JPH05217753A JP4056231A JP5623192A JPH05217753A JP H05217753 A JPH05217753 A JP H05217753A JP 4056231 A JP4056231 A JP 4056231A JP 5623192 A JP5623192 A JP 5623192A JP H05217753 A JPH05217753 A JP H05217753A
Authority
JP
Japan
Prior art keywords
magnetic
electronic component
magnetic force
inductor
composite electronic
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.)
Withdrawn
Application number
JP4056231A
Other languages
Japanese (ja)
Inventor
Masanori Tomaru
渡丸昌典
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
Application filed by Taiyo Yuden Co Ltd filed Critical Taiyo Yuden Co Ltd
Priority to JP4056231A priority Critical patent/JPH05217753A/en
Publication of JPH05217753A publication Critical patent/JPH05217753A/en
Withdrawn legal-status Critical Current

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  • Coils Or Transformers For Communication (AREA)
  • Fixed Capacitors And Capacitor Manufacturing Machines (AREA)
  • Apparatuses And Processes For Manufacturing Resistors (AREA)

Abstract

PURPOSE:To develop a method in which a magnetic process is used for regener ating out-of-spec products that produced slight resonance frequency deviation occurring in the manufacturing process of a monolithic composite electronic component. CONSTITUTION:On a variable magnetic force electromagnet whose lines of magnetic force 5, can be controlled a composite electronic component 4 consisting of an inductor section 2 and a capacitor section 3 is placed, and the inductance value of the inductor section is adjusted by controlling the magnetic force, thereby to regulate and stabilize the resonance frequency.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は積層型複合電子部品にお
けるインダクタのトリミング方法に関し、さらに詳しく
はインダクタ部を構成する磁性体に磁力を印加してコイ
ル状導体のインダクタンス値を調整する事を特徴とする
該電子部品インダクタのトリミング方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method of trimming an inductor in a laminated composite electronic component, and more specifically, it applies a magnetic force to a magnetic material forming an inductor section to adjust the inductance value of a coiled conductor. And a trimming method for the electronic component inductor.

【0002】[0002]

【従来の技術】従来の積層型複合電子部品にはインダク
タンス値および容量値に僅かなバラツキがあるために、
適用回路を設定した装置における共振周波数が目標とす
る周波数よりずれる場合がしばしば発生する。これを矯
正するために該複合部品を構成する磁性体の一部を削り
取るなどしてインダクタンス値を調整するトリミング方
法が開発され(特許出願公告昭60−50046)、サ
ンドブラストトリミング装置、レーザートリミング装置
などを使用してインダクタンス値の調整が行われてい
る。しかしながら上述の装置を使用して磁性体の一部を
削り取り、穴を空ける場合には(1) トリミングのための
穴空け位置がむずかしく、磁性体のコイル導体パターン
に穴を空けてしまうことがしばしば発生して、インダク
タンス値がオープンになってしまう恐れがある、(2) 磁
性体を削り過ぎて、インダクタンス値が目標値よりはず
れた場合に再生は不可能である、(3) 複合部品チップの
裏面に穴が空いてしまうため、異物が侵入して故障を起
し易い、などの問題点が必然的に発生していた。
2. Description of the Related Art Conventional laminated composite electronic components have slight variations in inductance value and capacitance value.
It often happens that the resonance frequency in the device to which the application circuit is set deviates from the target frequency. In order to correct this, a trimming method has been developed in which the inductance value is adjusted by, for example, scraping off a part of the magnetic material forming the composite component (Patent Application Publication No. 60-50046), sandblast trimming device, laser trimming device, etc. Is used to adjust the inductance value. However, when a part of the magnetic material is scraped off using the above-mentioned device to make a hole, (1) it is difficult to make a hole for trimming, and a hole is often made in the coil conductor pattern of the magnetic material. There is a risk that the inductance value will be opened, (2) If the inductance value deviates from the target value by scraping the magnetic material too much, it is impossible to reproduce, (3) Since a hole is formed on the back surface, there are inevitably problems that foreign matter easily enters and causes a failure.

【0003】[0003]

【発明が解決しようとする課題】本発明の目的は上述の
問題点を解決するために、インダクタ部を構成する磁性
体の一部を削り取って穴を空けるということをしないで
インダクタタンス値を調整できる方法を開発して提供す
ることである。
SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, the object of the present invention is to adjust the inductor stance value without cutting a part of the magnetic material forming the inductor part to form a hole. It is to develop and provide a possible method.

【0004】[0004]

【課題を解決するための手段】本発明者はかゝかる課題
を解決するために、鋭意研究の結果、インダクタ部を構
成する磁性体に調整された強さの磁力を印加すれば、磁
力の強さに対応したインダクタンス値が該インダクタに
得られることを見出した。すなわち印加する磁力の強さ
を調整することによりインダクタンス値が選択できるた
め、磁性体を削り取るなどして磁性体に損傷を与えるこ
と無く、必要なインダクタンス値が得られ、該インダク
タの共振周波数を容易に目標とする周波数に合わせるこ
とができることを知り、本発明を達成することができ
た。
In order to solve such a problem, the present inventor has conducted earnest research and, as a result, applies a magnetic force of adjusted strength to a magnetic material forming an inductor section. It has been found that an inductance value corresponding to strength can be obtained in the inductor. That is, since the inductance value can be selected by adjusting the strength of the magnetic force applied, the required inductance value can be obtained without damaging the magnetic body by scraping off the magnetic body, and the resonance frequency of the inductor can be easily adjusted. The present invention has been accomplished by knowing that the target frequency can be tuned to.

【0005】磁力を印加する方法は次の2通りある。 (1) インダクタに埋設されたコイル状導体に直流電流を
印加する。 (2) 磁力線5を調節できる磁力可変型電磁石1上に図1
に示すようにインダクタ部2とコンデンサ部3とからな
る複合電子部品4を置く。 上記(1) の方法により磁性体に磁力を印加した場合にお
ける印加直流電流の強さ(mA)とインダクタのインダ
クタンス値 (μH)との関係を図2に示す。
There are the following two methods of applying a magnetic force. (1) Apply a direct current to the coil-shaped conductor embedded in the inductor. (2) Fig. 1 on the variable magnetic force type electromagnet 1 that can adjust the magnetic force lines 5.
The composite electronic component 4 including the inductor portion 2 and the capacitor portion 3 is placed as shown in FIG. FIG. 2 shows the relationship between the applied DC current strength (mA) and the inductance value (μH) of the inductor when a magnetic force is applied to the magnetic material by the method (1).

【0006】印加直流電流の強さが10 mA 以下ではイン
ダクタンス値は変化しないが、10mAをこえると徐々
に低下することがわかる。また該複合体部品のインダク
タンスをL、容量値をCで示せば共振周波数fo は
It can be seen that the inductance value does not change when the strength of the applied DC current is 10 mA or less, but gradually decreases when it exceeds 10 mA. If the inductance of the composite component is L and the capacitance value is C, the resonance frequency fo is

【0007】[0007]

【化1】 で表わされる。従って上式よりLが低下すればfo は上
昇することがわかる。
[Chemical 1] It is represented by. Therefore, it can be seen from the above equation that if L decreases, fo increases.

【0008】次に上記(2) の方法により磁性体に磁力を
印加した場合における磁界の強さ(Gauss) とインダクタ
ンス値 (μH)との関係を図3に示す。磁界の強さが3
0ガウスまではインダクタンスの低下は認められない
が、それ以上では徐々に低下することがわかる。
FIG. 3 shows the relationship between the magnetic field strength (Gauss) and the inductance value (μH) when a magnetic force is applied to the magnetic material by the method (2). Magnetic field strength is 3
It can be seen that the inductance does not decrease until 0 gauss, but it gradually decreases above 0 gauss.

【0009】[0009]

【作用】磁性体に磁力を印加すれば、これを囲むコイル
状導体のインダクタンスは直ちには低下せず、印加磁力
がある値を越えて初めて変化が表われ、それ以後は磁力
の強さを増加すると共に低下が大きくなる。この現象を
図4により説明する。磁界の磁力が微小である間は可逆
磁化範囲内にある。すなわちこの範囲内では磁界の磁力
が無くなれば(H=0)磁性体の残留磁気は無くなる
(W=0)。磁界の強さがこの値を越えた非可逆磁化範
囲に入れば磁界の磁力が無くなっても(H=0)磁性体
にはOBで示す残留磁気が残る(W>0)。この現象は
磁性体に磁力を印加することにより焼結体に磁気歪が残
留することに起因すると考えられるが、その結果、磁性
体を取り囲むコイル状導体のインダクタンスが低下し、
かつ磁界の強さが強い程その割合は大きい。
[Function] When a magnetic force is applied to a magnetic body, the inductance of the coil-shaped conductor surrounding it does not immediately decrease, but changes appear only when the applied magnetic force exceeds a certain value, after which the strength of the magnetic force increases. As it does, the drop increases. This phenomenon will be described with reference to FIG. It is in the reversible magnetization range while the magnetic force of the magnetic field is very small. That is, within this range, if the magnetic force of the magnetic field disappears (H = 0), the residual magnetism of the magnetic material disappears (W = 0). If the strength of the magnetic field falls within the irreversible magnetization range exceeding this value, even if the magnetic force of the magnetic field disappears (H = 0), the residual magnetism indicated by OB remains in the magnetic substance (W> 0). This phenomenon is considered to be due to the residual magnetostriction in the sintered body due to the application of magnetic force to the magnetic body, but as a result, the inductance of the coil-shaped conductor surrounding the magnetic body decreases,
Moreover, the higher the strength of the magnetic field, the larger the ratio.

【0010】なお磁性体に磁力を印加し過ぎた場合に
は、再び磁気変態温度(キュリー点)の直上の温度に加
熱すれば磁気歪が消滅するため、初期状態に戻すことが
できる。すなわちトリミングをし過ぎた場合にはこの方
法により再生することが可能であることも本発明による
方法の特徴である。
If too much magnetic force is applied to the magnetic substance, the magnetic strain disappears if the magnetic substance is heated again to a temperature just above the magnetic transformation temperature (Curie point), so that the initial state can be restored. That is, it is a feature of the method according to the present invention that reproduction can be performed by this method when trimming is excessively performed.

【0011】以下実施例により本発明をさらに詳細に説
明する。
The present invention will be described in more detail with reference to the following examples.

【0012】[0012]

【実施例1】ソフトフェライト粉末を使用して周知のシ
ート法により、コンデンサ部には誘電体をはさんで交互
に5層の電極を積層し、インダクタ部には磁性体シート
上に形成された導体パターンを用いて20ターン巻コイ
ルを作成した後、常法により圧縮、焼成、焼結してコン
デンサ1つ、インダクタ1つを有するLC積層複合部品
を製造した。得られた製品の中から格外品を取り出し、
本発明によるトリミング法を行った。
[Example 1] Using a known sheet method using soft ferrite powder, five layers of electrodes were alternately laminated with a dielectric material sandwiched in a capacitor portion, and an inductor portion was formed on a magnetic material sheet. A 20-turn winding coil was formed using the conductor pattern, and then compressed, fired, and sintered by an ordinary method to manufacture an LC laminated composite component having one capacitor and one inductor. Take out the extraordinary products from the obtained products,
The trimming method according to the present invention was performed.

【0013】本製品の共振回路を図5に示した。その規
格値は共振周波数 (fo)3.58MHz、コンデンサ容
量C:110pF、インダクタンス値:18μHであ
る。本発明の効果を確かめるために、製品の中からイン
ダクタンス値20μHを示す格外品を取り出して試料と
した。共振周波数は3.39MHzである。
The resonance circuit of this product is shown in FIG. The standard values are resonance frequency (fo) 3.58 MHz, capacitor capacity C: 110 pF, and inductance value: 18 μH. In order to confirm the effect of the present invention, an extraordinary product having an inductance value of 20 μH was taken out from the product and used as a sample. The resonance frequency is 3.39 MHz.

【0014】まず、コイル状導体に直流電流12mAを
通じて磁化した結果C:110pF、L:19μHとな
り共振周波数 (fo)3.48MHzとなり、3.58M
Hzには達しなかった。さらに直流電流20mAを通じ
た結果L:18μHとなり、共振周波数fo : 3.58
MHz(図6)に到達し本発明による効果が確認でき
た。
First, as a result of magnetizing a coil-shaped conductor through a direct current of 12 mA, C: 110 pF, L: 19 μH, and a resonance frequency (fo) of 3.48 MHz, 3.58 M
It did not reach Hz. Furthermore, as a result of passing a direct current of 20 mA, the L becomes 18 μH, and the resonance frequency fo: 3.58
It reached to MHz (Fig. 6) and the effect of the present invention was confirmed.

【0015】[0015]

【実施例2】供試試料は実施例1と同一である。すなわ
ちコンデンサ容量110pF、インダクタ値20μFで
共振周波数(fo) 3.39MHzである。
Example 2 The test sample is the same as in Example 1. That is, the resonance frequency (fo) is 3.39 MHz with a capacitor capacity of 110 pF and an inductor value of 20 μF.

【0016】これを本発明による方法により磁力可変型
電磁石上に置き500ガウスの磁界を加えた結果C:1
10pF、L:19μHとなり、fo : 3.48MHz
であった。さらに1000ガウスの磁界を加えた結果
C:110pF、L:18μH、fo : 3.58MHz
(図6)となり本実施例においても本発明の効果を確認
することができた。
This was placed on a variable magnetic force type electromagnet by the method according to the present invention, and a magnetic field of 500 gauss was applied, resulting in C: 1.
10pF, L: 19μH, fo: 3.48MHz
Met. As a result of applying a magnetic field of 1000 gauss, C: 110 pF, L: 18 μH, fo: 3.58 MHz
As shown in FIG. 6, the effect of the present invention could be confirmed also in this example.

【0017】なお上述実施例においては実施例1および
2とも積層型複合部品として並列共振回路を示したが、
直列共振回路を構成する複合部品あるいはその他の複合
部品にも本発明方法の適用は可能である。
In the above-described embodiments, the parallel resonant circuit is shown as the laminated composite component in both the first and second embodiments.
The method of the present invention can be applied to a composite component forming a series resonance circuit or other composite components.

【0018】[0018]

【発明の効果】本発明の開発により、積層型複合電子部
品のインダクタ部を構成するコイル状導体に直流電流を
通じるか、または該部品を磁界に保持するなどしてコイ
ル状導体に囲まれた磁性体に磁力を印加することにより
インダクタンスを調整することができるようになった。
従って、該部品を削り取りまたは穴空けなどのトリミン
グを行う必要は無く、万一トリミングし過ぎた場合には
磁気変態点(キュリー点)直上の温度に加熱するのみで
再生できるなどの利点がある。
As a result of the development of the present invention, a direct current is passed through the coil-shaped conductor that constitutes the inductor portion of the laminated composite electronic component, or the component is surrounded by the coil-shaped conductor by holding the component in a magnetic field. The inductance can be adjusted by applying a magnetic force to the magnetic body.
Therefore, there is no need to trim the part or trim the part, and if trimming is excessive, the part can be regenerated simply by heating to a temperature just above the magnetic transformation point (Curie point).

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

【図1】LC複合部品を磁石上に置いてインダクタ部磁
性体に磁力を印加する方法に関する説明図。
FIG. 1 is an explanatory diagram related to a method of placing an LC composite component on a magnet and applying a magnetic force to a magnetic body of an inductor.

【図2】インダクタ部を構成するコイル状導体に通ずる
電流の強さとインダクタンス値との関係を示す図。
FIG. 2 is a diagram showing the relationship between the strength of a current flowing through a coil-shaped conductor forming an inductor section and the inductance value.

【図3】図1に示す方法に置ける磁界の強さとインダク
タ値との関係を示す図。
3 is a diagram showing a relationship between a magnetic field strength and an inductor value in the method shown in FIG.

【図4】磁界の強さと残留磁気の関係を示すヒステリシ
スループ図であり、非可逆範囲の説明図。
FIG. 4 is a hysteresis loop diagram showing the relationship between magnetic field strength and residual magnetism, and is an explanatory diagram of an irreversible range.

【図5】LC複合部品の並列共振回路。FIG. 5 is a parallel resonant circuit of an LC composite component.

【図6】共振周波数の伝送特性を示す図。FIG. 6 is a diagram showing a transmission characteristic of a resonance frequency.

【符号の説明】[Explanation of symbols]

1‥‥‥磁力可変型電磁石 2‥‥‥インダクタ部 3‥‥‥コンデンサ部 4‥‥‥複合電子部品 5‥‥‥磁力線 1 ... variable magnetic force type electromagnet 2 ... inductor section 3 ... capacitor section 4 ... composite electronic component 5 ... magnetic field lines

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 インダクタ部とコンデンサ部との組合わ
せからなる積層型複合電子部品のインダクタ部を構成す
る磁性体に調整された強さの磁力を印加してコイル状導
体のインダクタンス値を調整することを特徴とする複合
電子部品のトリミング方法
1. An inductance value of a coiled conductor is adjusted by applying a magnetic force of adjusted strength to a magnetic material forming an inductor part of a laminated composite electronic component including a combination of an inductor part and a capacitor part. Trimming method of composite electronic component characterized by
【請求項2】 前記電子部品のインダクタ部に埋設され
たコイル状導体に直流電流を通じることにより該磁性体
に磁力を印加する請求項1記載の方法。
2. The method according to claim 1, wherein a magnetic force is applied to the magnetic material by passing a direct current through a coil-shaped conductor embedded in the inductor portion of the electronic component.
【請求項3】 前記電子部品を調節可能な磁界中に保持
することにより、該磁性体に磁力を印加する請求項1記
載の方法。
3. The method of claim 1, wherein a magnetic force is applied to the magnetic body by holding the electronic component in an adjustable magnetic field.
JP4056231A 1992-02-06 1992-02-06 Method for trimming composite electronic component Withdrawn JPH05217753A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4056231A JPH05217753A (en) 1992-02-06 1992-02-06 Method for trimming composite electronic component

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4056231A JPH05217753A (en) 1992-02-06 1992-02-06 Method for trimming composite electronic component

Publications (1)

Publication Number Publication Date
JPH05217753A true JPH05217753A (en) 1993-08-27

Family

ID=13021333

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4056231A Withdrawn JPH05217753A (en) 1992-02-06 1992-02-06 Method for trimming composite electronic component

Country Status (1)

Country Link
JP (1) JPH05217753A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2505672B (en) * 2012-09-06 2014-09-17 Siemens Plc Dry slag granulation system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2505672B (en) * 2012-09-06 2014-09-17 Siemens Plc Dry slag granulation system

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