JPH0246517A - Method for measuring gap width of magnetic head - Google Patents

Method for measuring gap width of magnetic head

Info

Publication number
JPH0246517A
JPH0246517A JP19817088A JP19817088A JPH0246517A JP H0246517 A JPH0246517 A JP H0246517A JP 19817088 A JP19817088 A JP 19817088A JP 19817088 A JP19817088 A JP 19817088A JP H0246517 A JPH0246517 A JP H0246517A
Authority
JP
Japan
Prior art keywords
gap width
bits
line sensor
analog signal
magnetic head
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
JP19817088A
Other languages
Japanese (ja)
Inventor
Hiromi Nagumo
南雲 浩美
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.)
Alps Alpine Co Ltd
Original Assignee
Alps Electric 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 Alps Electric Co Ltd filed Critical Alps Electric Co Ltd
Priority to JP19817088A priority Critical patent/JPH0246517A/en
Publication of JPH0246517A publication Critical patent/JPH0246517A/en
Pending legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To eliminate the impossibility of the judgement of a boundary part by a diffused light and to attain the high accurate measurement by measuring a gap width with the number of bits obtained by the A/D conversion of an analog signal voltage from a line sensor built in a microscope. CONSTITUTION:The gap width of a magnetic head composed of a material with a different reflecting ratio is detected as an analog signal voltage by a line sensor 9 built in the microscope, after the correction is executed up to the reference voltage set beforehand, the suitable slice level is applied by the circuit, the number of the bits of the horizontal signal at this time is obtained by the A/D conversion, and with the correction curve of the real value of the gap width and the number of the bits obtained beforehand, the number of the bits of the horizontal signal is corrected. Thus, the judgement imposibility of the boundary part to occur by the diffused light due to the material with a different reflecting ratio is eliminated and a high accurate gap measurement can be performed.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は、反射率の異なる3種類の材料からなる磁気ヘ
ッドのギャップ幅の測定方法に関する。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a method for measuring the gap width of a magnetic head made of three types of materials having different reflectances.

〈従来の技術〉 従来、第1図(a)に示すような磁気コア間にガラスな
どからなる非磁性材と、パーマロイ、FeAt  Si
合金(センダスト)、アモルファスなど磁性材を介在さ
せたメタルインギャップと称される磁気ヘッドのギャッ
プ幅の測定方法は、光学顕微鏡によシ目視(シアリング
法)で行っていた。
<Prior art> Conventionally, as shown in Fig. 1(a), a non-magnetic material made of glass or the like is used between the magnetic cores, and permalloy or FeAtSi is used.
The gap width of a magnetic head called metal-in-gap, which uses a magnetic material such as an alloy (sendust) or amorphous, has been measured visually using an optical microscope (shearing method).

〈発明が解決しようとする問題点〉 従来の目視による測定では、作業者が顕微鏡を用いギャ
ップ幅の寸法を判断してるが、メタルなどの反射率が高
く光が拡散するものと、ガラスのように比較的反射率が
低いものとを、組合せた場合には、前記ガラス部1cが
小さくなればなるほどガラス部1cと、メタル部1bの
境界が、目視で判断できなくなる。このため測定に誤差
が生じやすく、さらに作業者の個人差によって測定の精
度が異なる(バラツク)という問題点がある。
<Problems to be solved by the invention> In the conventional visual measurement, an operator uses a microscope to judge the gap width, but it is difficult to measure the width of the gap by using a microscope. When a material having a relatively low reflectance is combined with a material having a relatively low reflectance, the smaller the glass portion 1c becomes, the more difficult it becomes to visually determine the boundary between the glass portion 1c and the metal portion 1b. For this reason, there is a problem in that errors are likely to occur in measurement, and measurement accuracy varies (variation) due to individual differences among workers.

またシアリング法においては、メタル部1bのみ測定、
そののちガラス部1cを測定と独立して測定しなければ
いけないため、同時測定が原理上不可能でギャップ幅の
測定に時間を要すという問題があった。
In addition, in the shearing method, only the metal part 1b is measured;
After that, the glass portion 1c has to be measured independently from the previous measurement, so there is a problem that simultaneous measurements are impossible in principle and it takes time to measure the gap width.

〈問題が解決するための手段〉 顕微鏡に内蔵したラインセンサーからのアナログ信号電
圧を用いて反射率の異なる材料から形成される磁気ヘッ
ドのギャップ幅を測定する方法において、前記ラインセ
ンサーからのアナログ信号電圧の垂直信号の最大値をあ
らかじめ設定した基準電圧値まで補正し、この補正した
前記アナログ信号電圧波形に回路によシ所定のスライス
レベルをかけ、前記スライスレベルでのラインセンサー
の水平信号のビット数をA/D変換(アナログ−デジタ
ル変換)によってギャップ幅を求めるとともに、あらか
じめ顕微鏡によって求めたギャップ幅の真値と前記測定
で求めたビット数との相関々係を補正曲線にしておき、
前記A/D変換で求めたビット数を前記補正曲線で補正
して求めるギャップ幅を測定する磁気ヘッドのギャップ
幅測定方法である。
<Means for solving the problem> In a method for measuring the gap width of a magnetic head formed from materials with different reflectances using an analog signal voltage from a line sensor built into a microscope, an analog signal from the line sensor is used. The maximum value of the vertical voltage signal is corrected to a preset reference voltage value, the corrected analog signal voltage waveform is multiplied by a predetermined slice level in a circuit, and the bits of the horizontal signal of the line sensor at the slice level are The gap width is determined by A/D conversion (analog-to-digital conversion), and the correlation between the true value of the gap width determined in advance using a microscope and the number of bits determined by the measurement is made into a correction curve.
This is a method for measuring a gap width of a magnetic head, in which a gap width determined by correcting the number of bits determined by the A/D conversion using the correction curve is measured.

〈作用〉 」1記手段によれば、反射率の異々る材料の反射を、顕
微鏡に内蔵したラインセンサーでアナログ信号電圧とし
て検出し、前記アナログ信号電圧の最大値をあらかじめ
設定した基準電圧まで補正したのち、回路によシ所定の
スライスレベルをかけ、このときの水平信号のビット数
をA/D変換によって求めると共に、あらかじめ求めて
おいたギャップ幅の真値と前記ビット数との補正曲線を
用いて前記ビット数を補正することにより従来のように
拡散光による境界部の判断不能がなくなり、また、デジ
タル処理を行う事により、高精度な測定ができる。
<Operation> According to the means described in item 1, reflections of materials with different reflectances are detected as an analog signal voltage by a line sensor built into the microscope, and the maximum value of the analog signal voltage is increased to a preset reference voltage. After the correction, a predetermined slice level is applied to the circuit, the number of bits of the horizontal signal at this time is determined by A/D conversion, and a correction curve is created between the true value of the gap width determined in advance and the number of bits. By correcting the number of bits using , it is no longer impossible to determine the boundary due to diffused light as in the conventional method, and by performing digital processing, highly accurate measurement is possible.

〈実施例〉 以下、本発明の原理と一実施例を図面を参照しながら説
明する。
<Example> Hereinafter, the principle and one example of the present invention will be described with reference to the drawings.

第1図(a)〜(c)は、本発明の詳細な説明する図、
第2図は、信号の処理システムを示すブロック図、第3
図は、アナログ信号電圧波形の処理原理を示す波形図、
第4図は、本発明の測定方法で測定した測定値(ビット
数)と、光学顕微鏡で測定した実測値(真値)との相関
関係を示す補正曲線である。
FIGS. 1(a) to 1(c) are diagrams illustrating detailed explanations of the present invention,
Figure 2 is a block diagram showing the signal processing system; Figure 3 is a block diagram showing the signal processing system;
The figure is a waveform diagram showing the processing principle of analog signal voltage waveform.
FIG. 4 is a correction curve showing the correlation between the measured value (bit number) measured by the measuring method of the present invention and the actual measured value (true value) measured by an optical microscope.

第1図(a) 、 (b)において、lは、例えば磁気
ヘッドのギャップ部などの観察物で、この観察物1は、
説明を容易にするため例えば1aはFe −Si −A
t合金系磁性材のような反射率の高い物体1bはフェラ
イト磁性材のように反射率が中間の物体、1cはガラス
のように低い反射率の物体とし、3種類の材料が組合わ
されている磁気ヘッドのギャップとする。2は顕微鏡レ
ンズ、第1図(C)は例えば顕微鏡に内蔵(図示せず)
したラインセンサーからのアナログ信号電圧の出力波形
を示す。
In FIGS. 1(a) and 1(b), l is an object to be observed, such as a gap part of a magnetic head, and this object 1 is
For ease of explanation, for example, 1a is Fe-Si-A
The object 1b with a high reflectance such as a t-alloy magnetic material is an object with an intermediate reflectance such as a ferrite magnetic material, and the object 1c is an object with a low reflectance such as glass, and three types of materials are combined. Let it be the gap of the magnetic head. 2 is a microscope lens, and FIG. 1 (C) is, for example, a built-in microscope (not shown).
The figure shows the output waveform of the analog signal voltage from the line sensor.

上記顕微鏡のレンズ2から取りこまれた画像は、ライン
センサーを通りアナログ信号電圧4として出力される。
An image captured through the lens 2 of the microscope is output as an analog signal voltage 4 through a line sensor.

3は、あらかじめ設定した基準電圧、7は、電圧上昇方
向を示し、6は、水平信号の走査方向を示す。また実施
例においてラインセンサーは、%インチで512 Bi
tの分解能を有するものを使用したがこれに限定するも
のでない。
3 indicates a preset reference voltage, 7 indicates a voltage increasing direction, and 6 indicates a horizontal signal scanning direction. In addition, in the example, the line sensor is 512 Bi in % inch.
Although a resolution having a resolution of t was used, the present invention is not limited to this.

第2図は、信号処理システムのブロック図を示し、入力
された信号は、以下の様に処理されて行く。例えば、第
3図に示すように、前記アナログ信号電圧出力4の中に
各1ケの凹凸部があるとすると、凹部がガラスのような
低い反射率の物体1c部分(以下、ガラス部と称す)凸
部が前記磁性合金などの反射率の高い物体1a部分(以
下メタル部と称す)である。前記凹部の最低値の中心8
aと、前記凸部の最高値の中心8bは別々の物体と考え
処理をして行く。なお、第3図において、前記アナログ
信号電圧4が水平に表われているところは反射率が中間
の物体1bで、例えば磁気ヘッドの磁気回路を構成する
フェライト材である。
FIG. 2 shows a block diagram of the signal processing system, and input signals are processed as follows. For example, as shown in FIG. 3, if there is one concave and convex portion in the analog signal voltage output 4, the concave portion is a portion of an object 1c with a low reflectance such as glass (hereinafter referred to as the glass portion). ) The convex portion is the object 1a portion (hereinafter referred to as metal portion) having a high reflectance such as the magnetic alloy. Center 8 of the lowest value of the recess
a and the center 8b of the highest value of the convex portion are treated as separate objects. In FIG. 3, the analog signal voltage 4 appearing horizontally corresponds to an object 1b having an intermediate reflectance, such as a ferrite material constituting a magnetic circuit of a magnetic head.

(以下フェライト部と称す) 先ず、第2図に示す駆動回路10により前記ラインセン
サー9からのアナログ信号電圧を読みこみ、次に前記ア
ナログ信号電圧(以下入力信号と称す)をサンプルホー
ルド増幅回路11で基準電圧に達するよう補正した後そ
の値を保持する。第3図において、前記ガラス部1cで
あるが、4dがフェライト部からの距離であシ、図示の
ように、フェライト部1bとガラス部1c、およびフェ
ライト部1bとメタル部1a、メタル部1aとガラス部
1cとの境界はラインセンサー90分解能が反射率の変
化に追従できないため波形が曲線となる。従って正確に
ガラス部IC又はメタル部1aの真値4F、4Cは求め
られないので、前記波形の曲線の影響がないところにス
ライスレベルをかけてやシ、このときのガラス部IC水
平方向のBit数4fをもとめる。こと1での回路での
処理をサンプルホールド増幅回路で行う。同様にメタル
部1aの真値4Cを求めるとメタル部1aは、上記凹部
の最低値から凸部の最高値までの距離4aをもとめ、そ
れをガラス部ICと同様適宜のスライスレベルで処理し
た部分4Cを求め、この部分4Cが、メタル部1aのB
it数とな9、このBit数を、A/D回路12により
A/D (アナログ−デジタル)変換する事により、ガ
ラス部ICとメタル部1aの値が積算平均化回路13で
算出されメモリー回路14に記憶される。次に、あらか
じめ事前に求めておいた第4図に示す補正曲線と、前記
測定で求めたガラス部ICとメタル部1aの値をパソコ
ン(パーソナルコンピューター)15’r用いて演算し
各々のギャップ幅又は加算して累計のギャップ幅が測定
できる。上記で求めたギャップ幅をCRT (ブラウン
管)上に表示する。前記の方法での測定結果と顕微鏡で
の実測値との間にはりニアリテイがあるので正確な測定
がきる。(第4図)従って、本発明の測定方法は実用に
供することができる。
(hereinafter referred to as ferrite section) First, the analog signal voltage from the line sensor 9 is read by the drive circuit 10 shown in FIG. After correcting the voltage to reach the reference voltage, the value is held. In FIG. 3, 4d is the distance from the ferrite part of the glass part 1c, and as shown, the ferrite part 1b and the glass part 1c, the ferrite part 1b and the metal part 1a, and the metal part 1a. At the boundary with the glass portion 1c, the resolution of the line sensor 90 cannot follow changes in reflectance, so the waveform becomes a curve. Therefore, since the true values 4F and 4C of the glass part IC or the metal part 1a cannot be obtained accurately, a slice level is applied to a part where there is no influence from the curve of the waveform. Find the number 4f. The processing in the circuit in step 1 is performed by the sample and hold amplifier circuit. Similarly, when finding the true value 4C of the metal part 1a, the metal part 1a is a part obtained by finding the distance 4a from the lowest value of the concave part to the highest value of the convex part, and processing it at an appropriate slice level like the glass part IC. 4C is obtained, and this part 4C is B of the metal part 1a.
The number of bits is 9. By A/D (analog-digital) conversion of this bit number by the A/D circuit 12, the values of the glass part IC and the metal part 1a are calculated by the integrating and averaging circuit 13, and the memory circuit 14. Next, using a personal computer 15'r, the correction curve shown in FIG. Alternatively, the cumulative gap width can be measured by adding them. The gap width determined above is displayed on a CRT (cathode ray tube). Accurate measurements can be made because there is a high degree of linearity between the measurement results obtained by the method described above and the actual measurement values obtained using a microscope. (FIG. 4) Therefore, the measuring method of the present invention can be put to practical use.

尚本発明ではラインセンサーを用いたがCCDを用い映
像処理しても同様な測定ができること勿論である。また
、前記アナログ信号電圧4が補正しても規定電圧に達し
ない場合は回路処理によって測定不可であることを示す
表示をするようにしである。
In the present invention, a line sensor is used, but it goes without saying that similar measurements can be made by using a CCD and image processing. Further, if the analog signal voltage 4 does not reach a specified voltage even after correction, a display is displayed indicating that measurement is not possible through circuit processing.

〈効果〉 以上説明したように、本発明は反射率の異なる材料から
なる磁気ヘッドのギャップ幅を顕微鏡に内蔵したライン
センサーによシアナログ信号電圧として検出し、あらか
じめ設定した基準電圧まで補正したのち回路によシ適宜
のスライスレベルをかけ、このときの水平信号のビット
数をA/D変換により求めると共に、あらかじめ求めて
おいたギャップ幅の真値とビット数との補正曲線を用い
て上記水平信号のビット数を補正し磁気ヘッドのギャッ
プ幅を測定するので、従来のように反射率の異な材料に
よる拡散光によって生ずる境界部の判断不能がなくな)
且つ、デジタル処理を行う事により、高精度な、ギャッ
プ測定ができると言う顕著な効果を奏する。
<Effect> As explained above, the present invention detects the gap width of a magnetic head made of materials with different reflectances as an analog signal voltage using a line sensor built into a microscope, corrects it to a preset reference voltage, and then detects the gap width of a magnetic head made of materials with different reflectances. Apply an appropriate slice level to the circuit, find the number of bits of the horizontal signal at this time by A/D conversion, and use the correction curve of the true value of the gap width and the number of bits found in advance to Since the number of signal bits is corrected and the gap width of the magnetic head is measured, there is no longer an inability to judge boundaries caused by diffused light caused by materials with different reflectances, which was the case in the past.
Moreover, by performing digital processing, there is a remarkable effect that highly accurate gap measurement can be performed.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図(a)〜(C)は、本発明の詳細な説明する図で
、第1図(a)は磁気ヘッドのギャップ部の構成を示す
平面図、第1図(b)は同じく磁気ヘッドのギャップ部
の要部断面図、第1図(C)は磁気ヘッドのギャップ部
をラインセンサーで走査したときのアナログ信号電圧波
形を示す図。 第2図は、本発明の信号の処理システムの一実例を示す
ブロック。 第3図は、アナログ信号電圧波形の処理原理を示す波形
図。 第4図は、同本発明の測定方法で測定した測定値と実測
値との相関関係を示す補正曲線である。 1・・・磁気ヘッドのギャップ部、1a・・・メタル部
、1b・・・フェライト部、IC・・・ガラス部、2・
・・顕微鏡、3・・・基準電圧、4・・・アナログ信号
電圧波形、4F、4C・・・顕微鏡による実測値、4f
、4c・・・本発明の測定値、8a・・・アナログ信号
電圧の最低値、8b・・・アナログ信号電圧の最高値、
9・・・顕微鏡に内蔵したラインセンサ 1r 第 一1 第 図
1(a) to 1(C) are diagrams explaining the present invention in detail. FIG. 1(a) is a plan view showing the structure of the gap portion of the magnetic head, and FIG. FIG. 1C is a cross-sectional view of the main part of the gap portion of the head, and is a diagram showing an analog signal voltage waveform when the gap portion of the magnetic head is scanned by a line sensor. FIG. 2 is a block diagram showing an example of the signal processing system of the present invention. FIG. 3 is a waveform diagram showing the processing principle of analog signal voltage waveforms. FIG. 4 is a correction curve showing the correlation between measured values measured by the measuring method of the present invention and actual measured values. 1... Gap part of magnetic head, 1a... Metal part, 1b... Ferrite part, IC... Glass part, 2...
...Microscope, 3...Reference voltage, 4...Analog signal voltage waveform, 4F, 4C...Actual value measured by microscope, 4f
, 4c... Measured value of the present invention, 8a... Minimum value of analog signal voltage, 8b... Maximum value of analog signal voltage,
9...Line sensor 1r built into the microscope Figure 11

Claims (1)

【特許請求の範囲】 異なる反射率の材料から形成される磁気ヘッドのギャッ
プ幅の測定方法において、前記ギャップ幅を測定する。 顕微鏡にラインセンサーを取りつけ、ラインセンサーか
らのアナログ信号電圧を、あらかじめ設定しておいた基
準電圧まで補正したのち、所定のスライスレベルをかけ
このときの前記ラインセンサーからのアナログ信号電圧
波形の水平信号のビット数を求めるとともに、あらかじ
め求めておいた補正曲線により、上記ビット数を補正し
てギャップ幅を測定したことを特徴とする磁気ヘッドの
ギャップ幅測定方法。
Claims: In a method for measuring gap widths of magnetic heads formed from materials with different reflectances, the gap widths are measured. Attach a line sensor to the microscope, correct the analog signal voltage from the line sensor to a preset reference voltage, and then apply a predetermined slice level to the horizontal signal of the analog signal voltage waveform from the line sensor at this time. 1. A method for measuring a gap width of a magnetic head, characterized in that the number of bits is determined, and the gap width is measured by correcting the number of bits using a correction curve determined in advance.
JP19817088A 1988-08-09 1988-08-09 Method for measuring gap width of magnetic head Pending JPH0246517A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19817088A JPH0246517A (en) 1988-08-09 1988-08-09 Method for measuring gap width of magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19817088A JPH0246517A (en) 1988-08-09 1988-08-09 Method for measuring gap width of magnetic head

Publications (1)

Publication Number Publication Date
JPH0246517A true JPH0246517A (en) 1990-02-15

Family

ID=16386635

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19817088A Pending JPH0246517A (en) 1988-08-09 1988-08-09 Method for measuring gap width of magnetic head

Country Status (1)

Country Link
JP (1) JPH0246517A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6128805A (en) * 1984-07-20 1986-02-08 Toho Denshi Kogyo Kk Measuring method of minute width

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6128805A (en) * 1984-07-20 1986-02-08 Toho Denshi Kogyo Kk Measuring method of minute width

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