JPH04166705A - Minute-interval measuring method - Google Patents

Minute-interval measuring method

Info

Publication number
JPH04166705A
JPH04166705A JP29268690A JP29268690A JPH04166705A JP H04166705 A JPH04166705 A JP H04166705A JP 29268690 A JP29268690 A JP 29268690A JP 29268690 A JP29268690 A JP 29268690A JP H04166705 A JPH04166705 A JP H04166705A
Authority
JP
Japan
Prior art keywords
light
distance
lens
image
mirror
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.)
Granted
Application number
JP29268690A
Other languages
Japanese (ja)
Other versions
JP2821517B2 (en
Inventor
Kiyoshi Matsui
清 松井
Yoshimasa Kusano
吉雅 草野
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.)
Kyocera Corp
Original Assignee
Kyocera Corp
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 Kyocera Corp filed Critical Kyocera Corp
Priority to JP29268690A priority Critical patent/JP2821517B2/en
Publication of JPH04166705A publication Critical patent/JPH04166705A/en
Application granted granted Critical
Publication of JP2821517B2 publication Critical patent/JP2821517B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To measure a minute interval between objects simply by casting light on the light scattering surface of the object which is located at a position separated from a mirror surface by a minute distance, condensing the reflected light with a lens, and projecting the light on a detecting element. CONSTITUTION:An object 13 having the light scattering surface is located at a distance of a height (h) from a mirror surface 11. The object 13 has an irregularly reflecting surface 13a in a plane which is intersected with the mirror surface. When light is emitted from a light source 15, the light is irregularly reflected from the irregularly reflecting surface 13a. When the light is observed from the side of the light source 15 with respect to the reflecting surface 13a, the reflecting surface 13a and a mirror image 13a' are brightly observed, and the part between the surface 13a and the surface 13a' is darkly observed. The image is picked up with a lens 17 and projected and focused on a line sensor 19. Then, the image comprising a bright part EF, a dark part FG and a bright part GH is projected. Therefore, the length of the dark part FG can be obtained at the error of about one picture element by detecting the edge part of the output on the line sensor 19.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、磁気ヘッドの浮上量測定等に応用可能な微小
間隔の測定方法に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method for measuring minute intervals that can be applied to measuring the flying height of a magnetic head.

従速!口14 光磁気記録、特に磁界変調型の光磁気記録においては、
記録信号品質が磁界の強さなどに影  響を受けるため
、記録媒体から一定の高さに磁気ヘッドを維持して駆動
することが必要である。
Follow the speed! 14 In magneto-optical recording, especially magnetic field modulation type magneto-optical recording,
Since the recording signal quality is affected by the strength of the magnetic field, it is necessary to drive the magnetic head while maintaining it at a constant height above the recording medium.

しかしながら、光磁気ディスク駆動装置では、ディスク
上のゴミ等の異物、ディスク自体の反りや、コーディン
グされたディスクの傾きに基づく変位等があり、所定位
置に磁気ヘッドを維持しつづけたのでは、一定の磁気ヘ
ッド浮上量が得られない、特に光磁気ディスク駆動装置
では、ディスクのローディングおよび取出しが繰り返さ
れるため、ローディング毎に、ディスクの傾き等が変化
する。そこで、常に磁気ヘッドとディスクとの距離を測
定し、この距離が一定となるように磁気ヘッドを制御駆
動する必要がある。
However, in magneto-optical disk drives, there are foreign objects such as dust on the disk, warpage of the disk itself, displacement due to the tilt of the encoded disk, etc., and if the magnetic head is kept in a predetermined position, it will not be possible to maintain a constant position. Particularly in magneto-optical disk drives in which it is not possible to obtain a magnetic head flying height of 100.degree., loading and unloading of the disk is repeated, so the inclination of the disk changes each time it is loaded. Therefore, it is necessary to constantly measure the distance between the magnetic head and the disk, and control and drive the magnetic head so that this distance remains constant.

回転ディスク上に浮上するスライダ等の微小な浮上距離
を測定する方法としては、以下の方法が知られている。
The following method is known as a method for measuring the minute flying distance of a slider or the like floating above a rotating disk.

■ 多波長の光線を照射して干渉縞を測定する方法。■ A method of measuring interference fringes by irradiating light beams with multiple wavelengths.

■ スライダ等とディスク面との間の静電容量を測定す
る方法。
■ A method to measure the capacitance between a slider, etc. and the disk surface.

■ 発散光をディスク面に当て、反射してくる光をアパ
ーチャーを通して受光すると、距離によって受光強度が
異なるので、この受光強度から距離を測定する方法。
■ A method of measuring distance based on the intensity of the received light, which shines diverging light onto the disc surface and receives the reflected light through an aperture.The intensity of the received light varies depending on the distance.

しかし、上記■の方法は測定システムが非常に高価であ
り、また、干渉縞の動きが速い場合は測定に適さない。
However, the above method (2) requires a very expensive measurement system, and is not suitable for measurement when the interference fringes move quickly.

一方、上記■、■の方法は、基準値に対する精密な較正
が必要であり、簡単に測定するという訳にはいかず、実
装置における測定方法としては適さない。
On the other hand, the above methods (1) and (2) require precise calibration with respect to a reference value, and cannot be easily measured, so they are not suitable as measurement methods for actual equipment.

以上、光磁気記録における記録ディスクからの磁気ヘッ
ドの浮上量の測定を中心に説明したが、この他にも2つ
の物体の微小間隔距離を非接触で測定することが必要な
場合は多い。
The above description has focused on measuring the flying height of a magnetic head from a recording disk in magneto-optical recording, but there are many other cases in which it is necessary to measure a minute distance between two objects without contact.

日が  しようとする 本発明は、簡単なシステムで微小間隔距離を測定するこ
とを目的とする。
The purpose of the present invention is to measure minute distances with a simple system.

見匪勿豊履 本発明の微小間隔の測定方法は、鏡面から微小距離離れ
て位置する物体の光散乱面に光を照射し、この反射光を
、レンズで集光し検知素子に投影して、この投影像の、
光散乱面の像とその鏡像との間隔を検知することにより
、鏡面と該物体との距離を測定することを特徴とする。
The method of measuring minute intervals of the present invention involves irradiating light onto a light scattering surface of an object located a minute distance from a mirror surface, condensing this reflected light with a lens, and projecting it onto a sensing element. , of this projected image,
It is characterized by measuring the distance between the mirror surface and the object by detecting the distance between the image of the light scattering surface and its mirror image.

務−−−刑 光散乱面を有する物体に照射された光は、乱反射され、
直接あるいは鏡面で反射されたのちレンズにより集光さ
れて検知素子上に投影される。このとき、この投影像は
、物体の光散乱面とその鏡像との間に当たる部分が暗く
、光散乱面の像およびその鏡像部分が明るい”明−暗一
明”の像となる。よって、暗部の長さを検知することに
より、この長さとレンズ位置から、鏡面と物体間の距離
を算出する。
- Light irradiated onto an object with a light-scattering surface is diffusely reflected,
After being reflected directly or from a mirror surface, the light is focused by a lens and projected onto a detection element. At this time, this projected image becomes a "bright-dark-one-bright" image in which the portion between the light-scattering surface of the object and its mirror image is dark, and the image of the light-scattering surface and its mirror image are bright. Therefore, by detecting the length of the dark part, the distance between the mirror surface and the object is calculated from this length and the lens position.

スー」L−舅一 第1図は、本発明の測定方法の原理を示す説明図である
FIG. 1 is an explanatory diagram showing the principle of the measuring method of the present invention.

鏡面11から、高さhの距離を保って光散乱面を有する
物体13が位置している。この物体13は、鏡面11と
交差する面内に乱反射面13aを有する。
An object 13 having a light scattering surface is located at a distance of height h from the mirror surface 11. This object 13 has a diffused reflection surface 13a in a plane that intersects with the mirror surface 11.

第1図では乱反射面13aを含む面と鏡面11とが、は
ぼ直交している状態を示している。光源15から物体1
3に光照射すると、乱反射面13aで光が乱反射する。
FIG. 1 shows a state in which the surface including the diffused reflection surface 13a and the mirror surface 11 are substantially perpendicular to each other. From light source 15 to object 1
3, the light is diffusely reflected by the diffusely reflecting surface 13a.

これを光の反射方向、すなわち乱反射面13aに対して
光源15側から観察すると。
This is observed from the direction of light reflection, that is, from the light source 15 side with respect to the diffused reflection surface 13a.

乱反射面13aおよび乱反射面の鏡像13a’が明るく
、その間が暗く観察される。これを、レンズ17により
撮影し、ラインセンサ19上に結像、投影させると、明
部(訂)−暗部(岡)−明部(GH)からなる像が投影
されるので、ラインセンサ19上の出力のエツジ部を検
出することにより、1画素程度の誤差で暗部FGの長さ
を求めることができる。
The diffused reflection surface 13a and the mirror image 13a' of the diffused reflection surface are bright, and the area between them is observed to be dark. When this is photographed by the lens 17 and imaged and projected onto the line sensor 19, an image consisting of the bright area (revised) - dark area (Oka) - bright area (GH) is projected, so it is projected onto the line sensor 19. By detecting the edge portion of the output, the length of the dark portion FG can be determined with an error of about one pixel.

いま、第1図に示したように各長さおよび角度を設定す
る。
Now, set each length and angle as shown in FIG.

a:物体13とその鏡像13′との距離=2hb:レン
ズ17の光軸に垂直な面へのaの投影長(AB) θ:レンズ17の光軸と鏡面11とのなす角D1:レン
ズ17と線分ABとの距離 りよ:レンズ17とラインセンサ19との距離とすると
、 b=」二X面    ・・(1)7 Dよ となるので、ラインセンサ19によるFGの測定値から
長さしが求められる。
a: Distance between the object 13 and its mirror image 13' = 2hb: Projection length of a on the plane perpendicular to the optical axis of the lens 17 (AB) θ: Angle between the optical axis of the lens 17 and the mirror surface 11 D1: Lens Distance between 17 and line segment AB: If the distance is between lens 17 and line sensor 19, then b = 2 Sashi is required.

bは、鏡面11に対して角度θで測定したために生じた
aの投影長なので、b = a Xcosθであり、結
局、物体13と鏡面11との距離は、次式により求まる
Since b is the projected length of a caused by measurement at an angle θ with respect to the mirror surface 11, b = a

h=+a=+−x占=占×七×元・・・(2)上記(2
)式中、θ+pzは測定系によって決まり固定できるの
で、D工を固定可能な場合は。
h = + a = + - x divination = divination x 7 x yuan... (2) Above (2
) In the formula, θ+pz is determined by the measurement system and can be fixed, so if D can be fixed.

物体13と鏡面11との距離をラインセンサ19の出力
から容易に測定できる。
The distance between the object 13 and the mirror surface 11 can be easily measured from the output of the line sensor 19.

また、D□およびD2を一度固定して絶対値の較正を行
なえば、距離りの絶対値の測定を直接行なうことができ
る。D工に対してD2が大きいほど、距離りの正確な測
定が可能となる。
Furthermore, once D□ and D2 are fixed and the absolute values are calibrated, the absolute value of the distance can be directly measured. The larger D2 is with respect to D, the more accurate distance measurement becomes possible.

また、第1図で、鏡面11を記録媒体(光磁気ディスク
)面、物体13を磁気ヘッドないしは磁気ヘッドを搭載
する支持部材とすると、光磁気記録における磁気ヘッド
浮上量の測定、制御に応用できることが判る。
Furthermore, in FIG. 1, if the mirror surface 11 is a recording medium (magneto-optical disk) surface and the object 13 is a magnetic head or a support member on which a magnetic head is mounted, it can be applied to measurement and control of the flying height of a magnetic head in magneto-optical recording. I understand.

第2図は、光磁気記録装置における磁気ヘッドの浮上量
測定/制御方式に応用する実施例を示す説明図である。
FIG. 2 is an explanatory diagram showing an embodiment applied to a flying height measurement/control method of a magnetic head in a magneto-optical recording device.

磁気ヘッド(図示を省略)を搭載したスライダ21(磁
気ヘッド搭載部材)はアーム23により支持され、この
アーム23が支持部材25に固定されている。支持部材
25は、アクチュエータ(図示を省略)により制御駆動
され、光磁気ディスク41の径方向に磁気ヘッドをアク
セス駆動し、また、磁気ヘッドを搭載したスライダ21
を上下動させて、磁気ヘッドの浮上量を制御できる。ア
ーム23には、光源31、レンズ33および受光素子3
5が固定されている。
A slider 21 (magnetic head mounting member) on which a magnetic head (not shown) is mounted is supported by an arm 23, and this arm 23 is fixed to a support member 25. The support member 25 is controlled and driven by an actuator (not shown), drives the magnetic head in the radial direction of the magneto-optical disk 41, and also drives the slider 21 on which the magnetic head is mounted.
The flying height of the magnetic head can be controlled by moving up and down. The arm 23 includes a light source 31, a lens 33, and a light receiving element 3.
5 is fixed.

光磁気ディスク41が矢印A方向に回転し、光磁気記録
装置が駆動されると、アーム23に固定されたLED等
の光源31から、スライダ21の乱反射面21aに光照
射される。この状態を、レンズ33で撮影して、ライン
センサ等の受光素子35上に結像、投影する。これによ
り、スライダ21の浮上量h、すなわち磁気ヘッドの浮
上量を測定でき、これをサーボ信号としてアクチュエー
タに供給し、支持部材25を上下駆動することにより、
磁気ヘッドと光磁気ディスク41との距離を常に一定に
保つことができる。レンズ33とスライダ21は共に同
一のアーム23に固定されているので、レンズ33と乱
反射面21aとの距離(第1図のDl)が固定され、浮
上量りの測定制御が容易である。スライダ21の乱反射
面21aは、研磨面とするが、光散乱を起こす程度に研
磨する。
When the magneto-optical disk 41 rotates in the direction of arrow A and the magneto-optical recording device is driven, a light source 31 such as an LED fixed to the arm 23 irradiates the diffused reflection surface 21a of the slider 21 with light. This state is photographed with a lens 33, and an image is formed and projected onto a light receiving element 35 such as a line sensor. Thereby, the flying height h of the slider 21, that is, the flying height of the magnetic head can be measured, and by supplying this as a servo signal to the actuator and driving the support member 25 up and down,
The distance between the magnetic head and the magneto-optical disk 41 can always be kept constant. Since the lens 33 and the slider 21 are both fixed to the same arm 23, the distance (Dl in FIG. 1) between the lens 33 and the diffused reflection surface 21a is fixed, making it easy to control the measurement of the flying height. The diffused reflection surface 21a of the slider 21 is a polished surface, but it is polished to the extent that it causes light scattering.

なお5本実施例で磁気ヘッドの支持、搭載部材として用
いられているスライダ21は、ハードディスク装置など
で用いられているウィンチエスタ型の浮動ヘッドスライ
ダとは性質を異にする。この浮動ヘッドスライダは、デ
ィスクの回転による浮揚力を受けて、それ自体ディスク
との距離を一定に保とうとするものである。これに対し
て本実施例では、スライダ21とディスク41との距離
は、前述のように本発明方法により測定され、フィード
バック制御によりアクチュ  4エータ等を駆動して、
一定に保たれる。スライダ21は、大きな面積をもち、
スライダ21と光磁気ディスク41とが急激に異常接近
した際に、空気による浮上刃により2スライダ21(磁
気ヘッド)が光磁気ディスク41に衝突することを防止
するものである。
Note that the slider 21 used as a support and mounting member for the magnetic head in this embodiment has different properties from the winchiesta type floating head slider used in hard disk drives and the like. This floating head slider attempts to maintain a constant distance from the disk by receiving the buoyancy force caused by the rotation of the disk. On the other hand, in this embodiment, the distance between the slider 21 and the disk 41 is measured by the method of the present invention as described above, and the actuator 4 is driven by feedback control.
remains constant. The slider 21 has a large area,
This is to prevent the second slider 21 (magnetic head) from colliding with the magneto-optical disk 41 due to the air floating blade when the slider 21 and the magneto-optical disk 41 suddenly approach abnormally.

以上、光磁気ディスクにおける磁気ヘッド浮上量の測定
、制御を中心に説明したが、本発明の測定方法は、それ
ぞれ鏡面および光散乱面を有する種々の物体間の距離の
測定に応用できる。
Although the above description has focused on measuring and controlling the flying height of a magnetic head on a magneto-optical disk, the measuring method of the present invention can be applied to measuring distances between various objects having mirror surfaces and light scattering surfaces, respectively.

見吏立羞米 本発明によれば、鏡面から微小間隔で離れて位置する光
散乱面を有する物体に光照射し、この反射光をレンズで
投影して検知することにより、簡単な照明系と結像系の
組み合わせで、物体間の微小間隔を測定できる。この測
定系は構成が簡単で安価であるので、光磁気ディスク駆
動装置を始めとする種々の装置に組み込むことが可能で
ある。
According to the present invention, light is irradiated onto an object having a light scattering surface located a minute distance from a mirror surface, and the reflected light is projected and detected by a lens, thereby creating a simple illumination system. By combining imaging systems, it is possible to measure minute distances between objects. Since this measurement system has a simple configuration and is inexpensive, it can be incorporated into various devices including magneto-optical disk drives.

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

第1図は、本発明の原理を示す説明図である。 第2図は、光磁気記録装置における磁気ヘッドの浮上量
測定/制御方式に応用する実施例を示す説明図である。 11・・・鏡 面    13・物 体13′・・・物
体の鏡像  15・・・光 源エフ・・・レンズ   
  19  ラインセンサ21・・・スライダ    
23・・・アーム25・・・支持部材    31・・
・光 源33・・・レンズ     35・受光素子4
1・・・光磁気ディスク
FIG. 1 is an explanatory diagram showing the principle of the present invention. FIG. 2 is an explanatory diagram showing an embodiment applied to a flying height measurement/control method of a magnetic head in a magneto-optical recording device. 11...Mirror surface 13.Object 13'...Mirror image of object 15...Light source F...Lens
19 Line sensor 21...Slider
23...Arm 25...Supporting member 31...
・Light source 33...Lens 35・Light receiving element 4
1... Magneto-optical disk

Claims (1)

【特許請求の範囲】 1、鏡面から微小距離離れて位置する物体の光散乱面に
光を照射し、この反射光を、レンズで集光し検知素子に
投影して、この投影像の、光散乱面の像とその鏡像との
間隔を検知することにより、鏡面と該物体との距離を測
定することを特徴とする微小間隔の測定方法。 2、前記物体とレンズとの距離が固定されている請求項
1記載の測定方法。 3、前記鏡面が記録媒体であり、前記物体が磁気ヘッド
または磁気ヘッドの搭載部材である請求項1または2に
記載の測定方法。
[Claims] 1. Light is irradiated onto the light-scattering surface of an object located a minute distance from the mirror surface, and this reflected light is collected by a lens and projected onto a detection element, and the light of this projected image is A method for measuring minute distances, characterized in that the distance between the mirror surface and the object is measured by detecting the distance between the image of the scattering surface and its mirror image. 2. The measuring method according to claim 1, wherein the distance between the object and the lens is fixed. 3. The measuring method according to claim 1 or 2, wherein the mirror surface is a recording medium, and the object is a magnetic head or a mounting member for a magnetic head.
JP29268690A 1990-10-30 1990-10-30 How to measure minute intervals Expired - Fee Related JP2821517B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29268690A JP2821517B2 (en) 1990-10-30 1990-10-30 How to measure minute intervals

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29268690A JP2821517B2 (en) 1990-10-30 1990-10-30 How to measure minute intervals

Publications (2)

Publication Number Publication Date
JPH04166705A true JPH04166705A (en) 1992-06-12
JP2821517B2 JP2821517B2 (en) 1998-11-05

Family

ID=17784991

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29268690A Expired - Fee Related JP2821517B2 (en) 1990-10-30 1990-10-30 How to measure minute intervals

Country Status (1)

Country Link
JP (1) JP2821517B2 (en)

Also Published As

Publication number Publication date
JP2821517B2 (en) 1998-11-05

Similar Documents

Publication Publication Date Title
JP4669047B2 (en) Method and device for position detection in an imaging system
EP0599806B1 (en) Position detector
US4689480A (en) Arrangement for improved scanned 3-D measurement
JPH04166705A (en) Minute-interval measuring method
US4032158A (en) Method and apparatus for indicating angular displacement
EP1113243A2 (en) Optical interference apparatus and position detection apparatus
JPS6161070B2 (en)
JP2574230B2 (en) Displacement detector
US4592650A (en) Apparatus for projecting a pattern on a semiconductor substrate
JPH11132713A (en) Distance measuring device and automatic focus control and photographing device, and recessed and projecting part detector
JP2626611B2 (en) Object shape measurement method
US6404715B1 (en) Detecting system for detecting rotation angle of deflection mirror
JP2657868B2 (en) Interference wave calibration method in head flying height measurement
JPH0626842A (en) One-dimensional scanning type surface displacement meter
JPH04128605A (en) Orientation flat detecting apparatus
JP2000182251A (en) Reading/writing device for optical recording medium
JPH02272308A (en) Non-contact type shape measuring instrument
JPH08114431A (en) Method and device for evaluating magnetic disc
JP2815808B2 (en) Radiation thermometer
JP3298300B2 (en) Position coordinate measuring method and position coordinate measuring device
JPH01267403A (en) Measuring apparatus for warped shape of disc
RU2165069C2 (en) Optical device measuring small displacements
JPH0861917A (en) Position detecting device
JPS6118962B2 (en)
JPS63281284A (en) Disk for measuring floating quantity of floating type magnetic head

Legal Events

Date Code Title Description
FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20070904

Year of fee payment: 9

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20080904

Year of fee payment: 10

LAPS Cancellation because of no payment of annual fees