JPS60227105A - Measuring instrument for surface deflection - Google Patents

Measuring instrument for surface deflection

Info

Publication number
JPS60227105A
JPS60227105A JP7091085A JP7091085A JPS60227105A JP S60227105 A JPS60227105 A JP S60227105A JP 7091085 A JP7091085 A JP 7091085A JP 7091085 A JP7091085 A JP 7091085A JP S60227105 A JPS60227105 A JP S60227105A
Authority
JP
Japan
Prior art keywords
circuit
spot position
light spot
measured
disk
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
JP7091085A
Other languages
Japanese (ja)
Other versions
JPS6149604B2 (en
Inventor
Kazuo Shigematsu
和男 重松
Hirobumi Nakamura
博文 中村
Toshimasa Kamisada
利昌 神定
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Ltd filed Critical Hitachi Ltd
Priority to JP7091085A priority Critical patent/JPS60227105A/en
Publication of JPS60227105A publication Critical patent/JPS60227105A/en
Publication of JPS6149604B2 publication Critical patent/JPS6149604B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/30Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces
    • G01B11/306Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces for measuring evenness

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Optical Recording Or Reproduction (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、回転円板の面振れを光学的に測定する装置に
関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an apparatus for optically measuring surface runout of a rotating disk.

〔発明の背景〕[Background of the invention]

従来9回転円板の面振れの測定には、静電容量型の微小
変位計が一般に用いられているが、被測定面が導電材料
から成っている必要があり、ガラス円板にTeなどの非
導電材料が蒸着された回転円板などの面振れは測定する
ことができない。このような被測定面の材料に対する制
約を取り除くため本発明では、光を面振れ測定用のプロ
ーブに用いている。
Conventionally, capacitance-type micro-displacement meters have been generally used to measure the surface runout of nine-rotation disks, but the surface to be measured must be made of a conductive material, and the glass disk must be made of a material such as Te. It is not possible to measure the surface runout of a rotating disk or the like on which a non-conductive material is deposited. In order to remove such restrictions on the material of the surface to be measured, the present invention uses light as a probe for measuring surface runout.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、簡単な構成で、測定範囲や測定感度が
被測定面の面振れの大きさにあわせて容易に調整でき、
しかも信頼度の高い面振れ測定装置を提供することにあ
る。
An object of the present invention is to have a simple configuration, and to easily adjust the measurement range and measurement sensitivity according to the magnitude of surface runout of the surface to be measured.
Moreover, it is an object of the present invention to provide a highly reliable surface runout measuring device.

〔発明の概要〕[Summary of the invention]

まず、本発明の原理を第1図を用いて説明する。 First, the principle of the present invention will be explained using FIG.

第1図において、1は円板で3を中心に矢印の方向に回
転している。光ビーム100は、円板1の面にほぼ垂直
に入射し、点10で反射する。通常、反射した光束20
0は点10における面の方向によって入射光束100と
は異なった方向を向いている。今、点10を原点として
第1図のようにX。
In FIG. 1, 1 is a disk rotating around 3 in the direction of the arrow. A light beam 100 is incident approximately perpendicularly to the surface of the disk 1 and is reflected at a point 10. Normally, the reflected luminous flux 20
0 points in a different direction from the incident light beam 100 depending on the direction of the surface at point 10. Now, take point 10 as the origin and draw X as shown in Figure 1.

y、z軸をとる。すなわち、又は点10における回転方
向、yは半径の方向、2は円板1の回転軸の方向である
。点10における接面とX軸となす角をψとすると、点
10における円板1の2軸方向の振れ(上下振れと呼ぶ
)の大きさZとの間に、dz −= t a n ψ x なる関係がある。半径rの円板は、一定角速度ωで回転
しているとすれば dz 1 dz 一方、反射光束200のX軸方向の振れ角をθとすれば
、0=29であるから dz θ −= r ω “ tan − dt 2 である。ここで、充分小さな振れ角に対してはdz r
 ω θ dt 2 従って、上下槁れの大□きさZは で与えられる。又、上下振れの加速度αはで与えられる
Take the y and z axes. That is, or the direction of rotation at point 10, y is the direction of the radius, and 2 is the direction of the axis of rotation of the disk 1. If the angle between the tangent surface at point 10 and the There is a relationship called x. If the disk with radius r is rotating at a constant angular velocity ω, then dz 1 dz On the other hand, if the deflection angle in the X-axis direction of the reflected light beam 200 is θ, then 0=29, so dz θ −= r ω “ tan − dt 2 .Here, for a sufficiently small deflection angle, dz r
ω θ dt 2 Therefore, the magnitude Z of the vertical deviation is given by ω θ dt 2 . Further, the vertical vibration acceleration α is given by:

このように、反射光束200の角度θを測定すれば、そ
れから、上下振れの大きさ及び加速度を知ることができ
る。
In this way, by measuring the angle θ of the reflected light beam 200, it is possible to know the magnitude and acceleration of vertical vibration.

〔発明の実施例〕[Embodiments of the invention]

以下、実施例により本発明を説明する。第2図は、本発
明による測定装置の一実施例を示す構成図である。図に
於て1は回転円板で、2は被測定面である。3は回転中
心で、4は、円板1を回転させるためのモータである。
The present invention will be explained below with reference to Examples. FIG. 2 is a configuration diagram showing an embodiment of the measuring device according to the present invention. In the figure, 1 is a rotating disk, and 2 is a surface to be measured. 3 is a rotation center, and 4 is a motor for rotating the disc 1.

5は、はぼ平行な光束を出射する光源、例えばHe −
N eレーザあるいは半導体レーザである。光源5から
出た平行光束は、偏光プリズム6で反射し、円板1の面
2にほぼ垂直な方向に向けられてλ/4板7を通って、
面2の点10に入射する。点10における面の方向に従
ってわずかに向きをかえられた反射光束は、λ/4板7
、偏向プリズム6を通って光点位置検出器8に入射する
。光点位置検出器8は、反射光束200の位置9に応じ
て出力端子2OA、20Bに電流が流れ、抵抗Rによっ
て電圧が発生する。
5 is a light source that emits a substantially parallel light beam, for example, He −
It is a Ne laser or a semiconductor laser. The parallel light beam emitted from the light source 5 is reflected by the polarizing prism 6, directed in a direction substantially perpendicular to the surface 2 of the disk 1, and passes through the λ/4 plate 7.
It is incident on point 10 on surface 2. The reflected light beam whose direction is slightly changed according to the direction of the surface at the point 10 is reflected by the λ/4 plate 7.
, passes through the deflection prism 6 and enters the light spot position detector 8. In the light spot position detector 8, current flows through the output terminals 2OA and 20B depending on the position 9 of the reflected light beam 200, and a voltage is generated by the resistor R.

常、光点位置検器8の中心でX=O)、光点位置検出器
8の電流感度をαとすると となる。光ビーム200の変位量Xは、光ビーム200
のふれ角をθ (第1図の定義による)、測定点10か
ら光点位置検出器8までの距離を悲とすれば、Oが充分
小さい時は x=Q θ となる。
Normally, at the center of the light spot position detector 8, X=O), and if the current sensitivity of the light spot position detector 8 is α. The amount of displacement X of the light beam 200 is
If the deflection angle is θ (according to the definition in FIG. 1) and the distance from the measurement point 10 to the light spot position detector 8 is θ, then when O is sufficiently small, x=Q θ.

測定円板の回転数をω、測定点10の半径r′とすれば
、先に述べた原理によって、この円板の測定面2の上下
振れ量2の時間微分は dt、2 11Rα 流成分を持っており、単純に積分すると、時間と発生さ
せる原因は、入射ビーム100のわずかな傾むきゃ光点
位置検出器8の位置調整のわずかなずれなどによってお
り、完全に、直流成分をOKすることは、はとんど不可
能に近い。このようなのみを取り出すようにする必要が
ある。
If the rotational speed of the measuring disk is ω and the radius of the measuring point 10 is r', then according to the principle described above, the time differential of the vertical deflection amount 2 of the measuring surface 2 of this disk is dt, 2 11Rα The flow component is If we simply integrate it, we can see that the cause of the occurrence is a slight inclination of the incident beam 100, a slight deviation in the position adjustment of the light spot position detector 8, etc., and the DC component is completely OK. It's almost impossible. It is necessary to take out only such items.

第3図に、光点位置検出器8の出力から、上下振れ量、
および上下振れ加速度を検出する回路構成を示す。第3
図において21は差動増巾器で、先に述べたV を発生
させる回路である。22゜23は、コンデンサーと抵抗
で、直流成分をカットすることが目的であり、いわゆる
微分回路であるが、その時定数1/RCは、測定円板の
回転周期より充分大きく取る必要がある。この出力30
Aは、上下振れ量の速度変動を表わしている。
Fig. 3 shows the amount of vertical deflection,
and the circuit configuration for detecting vertical vibration acceleration. Third
In the figure, numeral 21 is a differential amplifier, which is a circuit that generates the voltage V mentioned above. 22 and 23 are a so-called differential circuit whose purpose is to cut the DC component using a capacitor and a resistor, but the time constant 1/RC must be set to be sufficiently larger than the rotation period of the measuring disk. This output 30
A represents the speed fluctuation of the amount of vertical runout.

24および25は、それぞれ積分回路、および微分回路
であり、30Bおよび30Cは、上下振れ量および上下
振れ加速度に比例した出力が得られる。それぞれの比例
定数は、r、ω、Q、R,α。
24 and 25 are an integrating circuit and a differentiating circuit, respectively, and 30B and 30C provide outputs proportional to the amount of vertical vibration and the vertical vibration acceleration. The respective proportionality constants are r, ω, Q, R, and α.

および回転定数など、全て既知の量からめりことかでき
る。すなわち9本実施例によれば、上下振れ量および上
下振れ加速度の絶対値の測定が容易に行なえる。
and rotation constant, all of which can be calculated from known quantities. That is, according to this embodiment, the absolute value of the amount of vertical vibration and the acceleration of vertical vibration can be easily measured.

さもに、測定面2の反射率のムラや光源5の強度の変動
などの影響をなくすために、第4図に示した回路を用い
る。すなわち、第4図は20A、20Bの出力電圧V、
2 o 、 V’2o (7)差VA 白 AB と和■1を、差動増巾器21と加算回路26によV+に
比例する出力Vを端子Duより取り出す回路であり、第
3図功差動増巾器21のかわりに用いる。■+は、光位
置検出器8の特性により、光ビーム200の光量に比例
しているから、反射率のむらや光源の強度変化などの影
響を全く受どけなくなる。また、このようにすると被測
定面2の蒸着膜の種類が異なるような円板の上下振れを
測定するような場合でも、反射率の違いによる測定値の
補正を行なう必要がなく、どのような円板であってもつ
ねに上下振れ量、および上下振れ加速度の絶対値を得る
ことができる。
In addition, in order to eliminate the effects of uneven reflectance on the measurement surface 2 and fluctuations in the intensity of the light source 5, the circuit shown in FIG. 4 is used. That is, in FIG. 4, the output voltage V of 20A and 20B,
2o, V'2o (7) This is a circuit that takes out the difference VA white AB and the sum ■1 from the terminal Du using the differential amplifier 21 and the adder circuit 26 to output V which is proportional to V+. It is used in place of the differential amplifier 21. (2) Since + is proportional to the amount of light beam 200 due to the characteristics of the optical position detector 8, it is completely unaffected by uneven reflectance and changes in the intensity of the light source. In addition, in this way, even when measuring the vertical runout of a disk with different types of vapor deposited films on the surface to be measured 2, there is no need to correct the measured value due to the difference in reflectance, and any Even in the case of a disc, the absolute value of the amount of vertical deflection and the vertical deflection acceleration can always be obtained.

〔発明の効果〕〔Effect of the invention〕

以上の如く本発明によれば、光を用いて回転円板の面振
れを測定するので被測定面の材料に対する制約が少なく
、しがも検出器出方の交流成分を用いるので、入射光速
の傾むきゃ光点位置検出器の位置ずれに強く、調整が容
易な装置で信頼度の高い面振れ測定を行なえる。
As described above, according to the present invention, since the surface runout of the rotating disk is measured using light, there are few restrictions on the material of the surface to be measured, and since the alternating current component from the detector output side is used, the speed of incident light is If the device is tilted, it is resistant to misalignment of the light spot position detector and can perform highly reliable surface runout measurements with an easily adjustable device.

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

第1図は、本発明の詳細な説明するための図、第2図は
、本発明の一実施例の構成図、第3図は、第2図に示し
た実施例の装置から、上下振れ:におよび上下振れ加速
度を算出する回路を示す構成図。 第4図は、被測定面の反射率のムラや光源の光量変化な
どの影響を取り除く回路を示す構成図である。 第 1 回
FIG. 1 is a diagram for explaining the present invention in detail, FIG. 2 is a configuration diagram of an embodiment of the present invention, and FIG. : A configuration diagram showing a circuit for calculating vertical vibration acceleration. FIG. 4 is a configuration diagram showing a circuit that eliminates the effects of uneven reflectance of the surface to be measured and changes in the amount of light from the light source. 1st

Claims (1)

【特許請求の範囲】[Claims] ■、はぼ平行な光束を出射する光源と、入射光束の照付
位置に応じた信号を出力する光点位置検出器と、該平行
光束を回転円板の被測定面にほぼ垂直に入射し、該被測
定面からの反射光束を上記光点位置検出器に導く光学系
と、上記光点位置の検出器の出力の交流成分を取り出す
回路と、該交流成分の積分値および/または微分値を取
り出す回路とを具備したことを特徴とする回転“円板の
面振れ測定装置。
■A light source that emits a nearly parallel beam; a light spot position detector that outputs a signal according to the illumination position of the incident beam; , an optical system that guides the reflected light flux from the surface to be measured to the light spot position detector, a circuit that extracts an alternating current component of the output of the detector at the light spot position, and an integral value and/or differential value of the alternating current component. A device for measuring surface runout of a rotating disk, characterized in that it is equipped with a circuit for taking out the information.
JP7091085A 1985-04-05 1985-04-05 Measuring instrument for surface deflection Granted JPS60227105A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7091085A JPS60227105A (en) 1985-04-05 1985-04-05 Measuring instrument for surface deflection

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7091085A JPS60227105A (en) 1985-04-05 1985-04-05 Measuring instrument for surface deflection

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP791086A Division JPS61228306A (en) 1986-01-20 1986-01-20 Surface deflection measuring device

Publications (2)

Publication Number Publication Date
JPS60227105A true JPS60227105A (en) 1985-11-12
JPS6149604B2 JPS6149604B2 (en) 1986-10-30

Family

ID=13445139

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7091085A Granted JPS60227105A (en) 1985-04-05 1985-04-05 Measuring instrument for surface deflection

Country Status (1)

Country Link
JP (1) JPS60227105A (en)

Also Published As

Publication number Publication date
JPS6149604B2 (en) 1986-10-30

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