JPH0463322B2 - - Google Patents

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Publication number
JPH0463322B2
JPH0463322B2 JP61187058A JP18705886A JPH0463322B2 JP H0463322 B2 JPH0463322 B2 JP H0463322B2 JP 61187058 A JP61187058 A JP 61187058A JP 18705886 A JP18705886 A JP 18705886A JP H0463322 B2 JPH0463322 B2 JP H0463322B2
Authority
JP
Japan
Prior art keywords
measured
reflected light
light image
image
reflective surface
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.)
Expired - Lifetime
Application number
JP61187058A
Other languages
Japanese (ja)
Other versions
JPS6342413A (en
Inventor
Koetsu Hibino
Hideaki Ueno
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.)
Toyota Motor Corp
Original Assignee
Toyota Motor 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 Toyota Motor Corp filed Critical Toyota Motor Corp
Priority to JP18705886A priority Critical patent/JPS6342413A/en
Publication of JPS6342413A publication Critical patent/JPS6342413A/en
Publication of JPH0463322B2 publication Critical patent/JPH0463322B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、主として透明もしくは半透明な板状
材料の反り量など、該材料の平坦度を測定する方
法及び装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a method and apparatus for measuring the flatness of a transparent or translucent plate-like material, such as the amount of warpage of the material.

本発明の方法及び装置は、ガラス板、液晶セ
ル、あるいは反射板などの平坦度を測定するのに
有用である。
The method and apparatus of the present invention are useful for measuring the flatness of glass plates, liquid crystal cells, reflectors, and the like.

[従来技術] 従来、ガラス基板などの、透明もしくは半透明
な板状材料の表面の平坦度、あるいは両面の平行
度などは、例えば、コヒーレント光を該板状材料
に照射し、表面及び裏面からの反射光の光路差に
よる干渉縞(ニユートンリング)を利用して測定
している。
[Prior Art] Conventionally, the flatness of the surface or the parallelism of both sides of a transparent or translucent plate-like material such as a glass substrate has been determined by, for example, irradiating the plate-like material with coherent light and measuring it from the front and back surfaces. It is measured using interference fringes (Newton rings) created by the optical path difference of the reflected light.

また、平坦度の測定方法としては、JIS−
R3202(JISハンドブツク、日本規格協会発行)に
規定された方法、あるいは、平坦な定盤上に被測
定物を載置し、〓間ゲージを用いて反り量を測定
する方法等が行われている。
In addition, as a method for measuring flatness, JIS-
The method specified in R3202 (JIS Handbook, published by the Japanese Standards Association) or the method of placing the object to be measured on a flat surface plate and measuring the amount of warpage using a distance gauge are used. .

[発明が解決しようとする問題点] しかし、上記した従来の方法は、簡便なもので
はなかつた。また、〓間ゲージを用いる方法は、
被測定物の平坦度を部分的にのみ測定する(周縁
部のみ測定する)ものでもあつた。
[Problems to be Solved by the Invention] However, the above-described conventional methods are not simple. Also, the method using the distance gauge is
In some cases, the flatness of the object to be measured was measured only partially (measuring only the periphery).

しかるに近年、車載のインナーミラー、メータ
デイスプレイ等、液晶セルを適用する装置の大型
化、大量生産化が進むにつれ、セル基板の反りを
無視できなくなつており、板状材料の反り量を簡
便に測定し得る方法及び装置が望まれている。
However, in recent years, as devices to which liquid crystal cells are applied, such as car interior mirrors and meter displays, have become larger and mass-produced, it has become impossible to ignore the warpage of cell substrates. A method and apparatus that can measure this is desired.

本発明はこのような問題点に鑑みてなされたも
のであり、上記要請を満たす方法及び装置を提供
するものである。
The present invention has been made in view of these problems, and it is an object of the present invention to provide a method and apparatus that meet the above requirements.

[問題点を解決するための手段] 本発明の第1の発明である平坦度測定方法は、
平坦な基準反射面を有する基準反射板の光入射側
に、透明又は半透明な板状の被測定物を重ねるよ
うにして配置し、格子状の基準パターンで遮光さ
れるとともにその照明領域に前記被測定物が包含
されるように設定された光線を、前記基準反射面
の法線に対して所定角度傾斜させて照射し、 前記被測定物の表面での反射による第1反射光
像、及び前記基準反射面での反射による第2反射
光像を、同一のスクリーンに投影させ、 前記第1反射光像と前記第2反射光像とのズレ
より、前記被測定物の反り量を求めることを特徴
とする。
[Means for solving the problem] The flatness measuring method which is the first invention of the present invention is as follows:
A transparent or semi-transparent plate-shaped object to be measured is placed on the light incident side of a reference reflection plate having a flat reference reflection surface, and is shielded from light by a grid-like reference pattern. A light beam set to include the object to be measured is irradiated at a predetermined angle with respect to the normal to the reference reflective surface, and a first reflected light image is formed by reflection on the surface of the object to be measured; projecting a second reflected light image resulting from reflection on the reference reflective surface onto the same screen, and determining the amount of warpage of the object to be measured from the deviation between the first reflected light image and the second reflected light image; It is characterized by

また、本発明の第2の発明である平坦度測定装
置は、平坦な基準反射面を有し、光入射側に重ね
るようにして透明又は半透明な板状の被測定物を
配置し得る基準反射板と、 前記基準反射面の法線に対して所定角度傾斜す
る方向から、その照明領域に前記被測定物が包含
されるように設定された光線を前記基準反射面に
照射する光源と、 該光源と前記基準反射面との間に位置し、前記
光源からの照射光を格子状の基準パターンで遮光
する遮光部と、 前記基準反射面及び前記被測定物からの反射光
像を投影するスクリーンとを有し、 該スクリーンに投影された、前記被測定物の表
面での反射による第1反射光像と、前記基準反射
面での反射による第2反射光像とのズレより前記
被測定物の反り量を求めるようにしたことを特徴
とする。
Further, the flatness measuring device, which is the second invention of the present invention, has a flat reference reflecting surface, and a reference surface on which a transparent or translucent plate-shaped object to be measured can be placed so as to be overlapped on the light incident side. a light source that irradiates the reference reflective surface with a light beam set such that the object to be measured is included in the illumination area from a direction inclined at a predetermined angle with respect to the normal to the reference reflective surface; a light shielding section located between the light source and the reference reflective surface, which blocks the irradiated light from the light source with a grid-like reference pattern; and projects an image of reflected light from the reference reflective surface and the object to be measured. and a screen, and due to a difference between a first reflected light image projected on the screen caused by reflection on the surface of the object to be measured and a second reflected light image caused by reflection at the reference reflective surface, the object to be measured is The feature is that the amount of warpage of an object is determined.

換言すれば本発明は、被測定物及び基準反射面
からのそれぞれの反射光線を同一スクリーン上に
投影し、そのズレより、反り量,つまり平坦度に
関する情報を得るものである。
In other words, the present invention projects the respective reflected light beams from the object to be measured and the reference reflecting surface onto the same screen, and obtains information regarding the amount of warpage, that is, the flatness, from the deviation thereof.

ここで平坦な基準反射面とは、凹凸及び反りが
なく、かつ曲率半径が無限大の反射面をいう。な
お、反射率は、被測定物表面の反射率との相対的
関係で決定される。要は、観測者が第1反射光像
と第2反射光像とを明確に識別できれば足りる。
Here, the flat reference reflective surface refers to a reflective surface that is free from unevenness and warpage and has an infinite radius of curvature. Note that the reflectance is determined in relation to the reflectance of the surface of the object to be measured. In short, it is sufficient that the observer can clearly distinguish between the first reflected light image and the second reflected light image.

また、被測定物としては、たとえば、薄膜作成
に用いられる各種ガラス基板、セラミツクス基
板、樹脂基板、これらの基板により製造された液
晶セル等の透明又は半透明な平板状部材を想定し
ている。
The object to be measured is assumed to be, for example, a transparent or translucent plate-like member such as various glass substrates, ceramic substrates, resin substrates, and liquid crystal cells manufactured using these substrates used for thin film production.

格子の基準パターンは、反射光像を与えるもの
である。
The grating reference pattern provides a reflected light image.

本発明において、基準反射面を照射する光線の
入射角は、該基準反射面の法線に対し、所定角度
傾斜させる。反射光像を、直接的にスクリーンに
投影させ得るようにするためである。ここで「直
接的に」とは、鏡、あるいは、レンズ等の光学機
器を介さないことをいう。なお傾斜角は、5度以
下とすると、入射光線が平行光線でないことによ
つて生ずる影響を無視できる。また、光線の照明
領域は被測定物の大きさに対応して設定される。
すなわち、基準反射板と被測定物の外縁部の間隔
(歪み量)が、同一スクリーンに投影した第1反
射光像と第2反射光像とのズレによつて求められ
るので、光線の照明領域は少なくとも被測定物を
包含するように設定される。これにより、被測定
物の内部から外縁部までの歪みが測定される。
In the present invention, the incident angle of the light beam that illuminates the reference reflective surface is inclined at a predetermined angle with respect to the normal to the reference reflective surface. This is to enable the reflected light image to be directly projected onto the screen. Here, "directly" means not via an optical device such as a mirror or lens. Note that when the inclination angle is set to 5 degrees or less, the influence caused by the fact that the incident light rays are not parallel rays can be ignored. Further, the illumination area of the light beam is set in accordance with the size of the object to be measured.
In other words, since the distance (distortion amount) between the reference reflector and the outer edge of the object to be measured is determined by the deviation between the first reflected light image and the second reflected light image projected on the same screen, the illumination area of the light beam is is set so as to include at least the object to be measured. Thereby, the strain from the inside of the object to be measured to the outer edge is measured.

スクリーンとしては、例えば、すりガラス、拡
散板、乳白色の樹脂板、薄い紙等を用いると、裏
面側から前記第1反射光像及び前記第2反射光像
を観測することができる。さらに、スクリーン上
にそれぞれの反射像のズレ距離を測定するための
目盛りを設けても良い。
For example, if frosted glass, a diffuser plate, a milky white resin plate, thin paper, or the like is used as the screen, the first reflected light image and the second reflected light image can be observed from the back side. Furthermore, a scale may be provided on the screen for measuring the shift distance of each reflected image.

[作用] 被測定物の反りが無く、平坦性が良好であり、
かつ平滑であれば第1反射光像と第2反射光像と
は重なり合い、スクリーンに結像された反射像は
鮮明に見える。
[Function] There is no warping of the object to be measured, and the flatness is good.
If the surface is smooth, the first reflected light image and the second reflected light image will overlap, and the reflected image formed on the screen will be clearly visible.

一方、被測定物の反りが有り、平坦性が悪い場
合は、被測定物表面と、基準反射面とが平行でな
いため、第1反射光像と第2反射光像とはそれぞ
れズレて投影される。
On the other hand, if the object to be measured is warped and has poor flatness, the surface of the object to be measured is not parallel to the reference reflective surface, so the first reflected light image and the second reflected light image are projected with deviations from each other. Ru.

該ズレ距離δを測定することにより被測定物の
反り量、つまり平坦度に関する情報を得る。
By measuring the deviation distance δ, information regarding the amount of warpage, that is, the flatness of the object to be measured is obtained.

[実施例] 以下、本発明を具体的実施例に基づいて説明す
る。
[Examples] The present invention will be described below based on specific examples.

(実施例 1) 第1図に本発明の実施例1に係わる平坦度測定
装置を示す。
(Example 1) FIG. 1 shows a flatness measuring device according to Example 1 of the present invention.

本装置は、光源と格子状パターンとを内蔵する
スライドプロジエクタ1と、その下方であつて、
スライドプロジエクタ1からの光線の光路に水平
に設けられ、上面に反りが無く平坦な基準反射面
21を有する基準反射板2と、該基準反射面21
上に載置された透明な被測定物4及び基準反射面
21からの2つの反射光像が投影されるスクリー
ン3とから構成されている。
This device includes a slide projector 1 having a built-in light source and a grid pattern, and below the slide projector 1,
A reference reflecting plate 2 is provided horizontally in the optical path of the light beam from the slide projector 1 and has a flat reference reflecting surface 21 with no warp on the upper surface; and the reference reflecting surface 21
It is composed of a transparent object to be measured 4 placed thereon and a screen 3 on which two reflected light images from a reference reflecting surface 21 are projected.

なお、スライドプロジエクタ1からの照射光の
中心部の光軸は、基準反射面21に立てた法線に
対して、3度傾斜している。また、被測定物の幅
2は300mmであり、上記照射光の照明領域は該
幅より大きく設定されている。
Note that the optical axis of the central part of the irradiated light from the slide projector 1 is inclined by 3 degrees with respect to the normal to the reference reflective surface 21. Further, the width 2 of the object to be measured is 300 mm, and the illumination area of the irradiation light is set to be larger than the width.

上記装置による測定原理を第3図に即して説明
する。
The principle of measurement by the above device will be explained with reference to FIG.

被測定物4の反射面の接線41と、基準反射面
21とが原点0(被測定物4の中心部:第1図参
照)から離れた部位において、θ[rad]の角
度を成すものとする。
The tangent 41 of the reflective surface of the object to be measured 4 and the reference reflective surface 21 form an angle of θ [rad] at a location away from the origin 0 (the center of the object to be measured 4: see Figure 1). do.

この場合、該部位における反り量dは、 d=θ……(1) で与えられる。 In this case, the amount of warpage d at the portion is d=θ……(1) is given by

いま、光源から、基準反射面21(図示のよう
に、該反射面21に平行な面21′で考えるとよ
い)の法線210に対して角度αを成す光線a1
入射すると、該光線a1は面21′で反射されて、
光線a2となる。
Now, when a light ray a 1 forming an angle α with respect to the normal 210 of the reference reflecting surface 21 (as shown in the figure, it is better to think of it as a plane 21' parallel to the reflecting surface 21) is incident from the light source, the light ray a 1 is reflected by surface 21',
The ray becomes a 2 .

同時に前記光線a1は、面41によつても反射さ
れて、光源a3となる。
At the same time, the light ray a 1 is also reflected by the surface 41 and becomes a light source a 3 .

しかるに、前記面21の法線210と、面41
に立てた法線410とは角度θ[rad]を成す。
故に、前記光線a2とa3とは角度2θ[rad]を成すこ
とになる。
However, the normal 210 of the surface 21 and the surface 41
It forms an angle θ [rad] with the normal line 410 erected at .
Therefore, the rays a 2 and a 3 form an angle 2θ [rad].

したがつて、前記反射点からスクリーン3に至
る距離をLとすると、スクリーン3上でのズレ距
離δは、 δ=2Lθ……(2) として与えられる。
Therefore, if the distance from the reflection point to the screen 3 is L, the deviation distance δ on the screen 3 is given as δ=2Lθ (2).

(1)式及び(2)式より δ=2Ld/……(3) を得る。 From equations (1) and (2), δ=2Ld/……(3) get.

即ち、ズレ距離δを測定することにより、反り
量dを求めることができる。
That is, by measuring the deviation distance δ, the amount of warpage d can be determined.

上記装置では、スライドプロジエクタ1−基準
反射面21間にコリメータを配せず、したがつて
照射光線も平行光線ではない。このため、若干の
誤差はま免れないが、たとえば、被測定物として
280×70×t1.9mmの板材を用い、 d>0.1mm(反り0.035%以上) のものを抽出する、はね出し検査を行つたとこ
ろ、抽出後の不良率を1%以下とすることができ
た。従来のスキマゲージによる不良率(不良品は
ね出し後の不良率)が30%以上であつたことに鑑
み、本装置は十分実用に耐えることが判明した。
In the above device, no collimator is disposed between the slide projector 1 and the reference reflecting surface 21, and therefore the irradiated light beam is not a parallel light beam. For this reason, some errors are inevitable, but for example,
Using a plate material of 280 x 70 x t1.9 mm, we conducted a pop-up inspection to extract those with d > 0.1 mm (warpage of 0.035% or more), and found that the defective rate after extraction could be kept below 1%. did it. In view of the fact that the defective rate (defective rate after defective products are pushed out) using conventional feeler gauges was over 30%, this device was found to be sufficiently durable for practical use.

なお、スライドプロジエクト1としては、キヤ
ビン工業製(f=75mm,1:2.5)のものを用い
た。
As the slide project 1, one manufactured by Cabin Kogyo (f=75 mm, 1:2.5) was used.

また、参考のために被測定物の反り量と投影時
のズレ距離との関係を第4図に示す。
Further, for reference, the relationship between the amount of warpage of the object to be measured and the displacement distance during projection is shown in FIG.

(実施例 2) 第2図に示すように、実施例1と同様のスライ
ドプロジエクタ1を平面に設置し、光線が基準反
射板の法線に対して5度の角度で照射されるよう
に、基準反射板2を傾斜させ、スライドプロジエ
クタ1との距離が70cm、スクリーン3との距離が
170cmになるように配置し、被測定物として長尺
板状のガラス基板4(280mm×70mm×1.9mm)を、
あらかじめストツパーを備付けた基準反射板2の
反射面21に載置した。また、ガラス基板4の反
射率は約4%であり、基準反射板21の表面には
反射膜を形成し反射率は約20%であつた。このよ
うにして測定されたガラス板4の反射光像のズレ
距離δは反り量が0.1mmのとき4mmであつた。
(Example 2) As shown in Fig. 2, a slide projector 1 similar to that of Example 1 was installed on a flat surface, and the light beam was irradiated at an angle of 5 degrees with respect to the normal to the reference reflector. , the reference reflector 2 is tilted, and the distance to the slide projector 1 is 70 cm, and the distance to the screen 3 is
170 cm, and a long plate-shaped glass substrate 4 (280 mm x 70 mm x 1.9 mm) as the object to be measured.
It was placed on the reflective surface 21 of the reference reflective plate 2, which was equipped with a stopper in advance. Further, the reflectance of the glass substrate 4 was about 4%, and a reflective film was formed on the surface of the reference reflecting plate 21, and the reflectance was about 20%. The shift distance δ of the reflected light image of the glass plate 4 measured in this manner was 4 mm when the amount of warpage was 0.1 mm.

[発明の効果] 以上のように、本発明によると容易な構成の装
置を用い、簡便に被測定物の反り量、つまり平坦
度を実用に耐える精度で測定することが可能とな
る。
[Effects of the Invention] As described above, according to the present invention, it is possible to easily measure the amount of warpage, that is, the flatness, of the object to be measured with an accuracy that can withstand practical use, using a device with a simple configuration.

また、コリメータ、半透鏡等の光学的手段を用
いない簡単な構成なので、光線の光量が低下しに
くいため、暗室内で検査する必要もなくなる。
In addition, since the configuration is simple and does not use optical means such as a collimator or a semi-transparent mirror, the amount of light is less likely to decrease, so there is no need to perform inspection in a dark room.

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

第1図は、本発明の実施例1に係る平坦度測定
装置の原理を示す図である。第2図は、本発明の
実施例2に係る平坦度測定装置を示す図である。
第3図は、本発明の測定原理を示す図である。第
4図は、被測定物の反り量と、投影時のズレ距離
との関係を示すグラフである。 1……スライドプロジエクタ、2……基準反射
板、3……スクリーン、4……被測定物。
FIG. 1 is a diagram showing the principle of a flatness measuring device according to Example 1 of the present invention. FIG. 2 is a diagram showing a flatness measuring device according to Example 2 of the present invention.
FIG. 3 is a diagram showing the measurement principle of the present invention. FIG. 4 is a graph showing the relationship between the amount of warpage of the object to be measured and the displacement distance during projection. 1...Slide projector, 2...Reference reflector, 3...Screen, 4...Measurement object.

Claims (1)

【特許請求の範囲】 1 平坦な基準反射面を有する基準反射板の光入
射側に、透明又は半透明な板状の被測定物を重ね
るようにして配置し、 格子状の基準パターンで遮光されるとともにそ
の照明領域に前記被測定物が包含されるように設
定された光線を、前記基準反射面の法線に対して
所定角度傾斜させて照射し、 前記被測定物の表面での反射による第1反射光
像、及び前記基準反射面での反射による第2反射
光像を、同一スクリーンに投影させ、 前記第1反射光像と前記第2反射光像とのズレ
より、前記被測定物の反り量を求めることを特徴
とする平坦度測定方法。 2 前記傾斜させる所定角度は、5度以下である
特許請求の範囲第1項記載の平坦度測定方法。 3 平坦な基準反射面を有し、光入射側に重ねる
ようにして透明又は半透明な板状の被測定物を配
置し得る基準反射板と、 前記基準反射面の法線に対して所定角度傾斜す
る方向から、その照明領域に前記被測定物が包含
されるように設定された光線を前記基準反射面に
照射する光源と、 該光源と前記基準反射面との間に位置し、前記
光源からの照射光を格子状の基準パターンで遮光
する遮光部と、 前記基準反射面及び前記被測定物からの反射光
像を投影するスクリーンとを有し、 該スクリーンに投影された、前記被測定物の表
面での反射による第1反射光像と、前記基準反射
面での反射による第2反射光像とのズレより前記
被測定物の反り量を求めるようにしたことを特徴
とする平坦度測定装置。 4 前記スクリーンは、裏面側から前記第1反射
光像及び前記第2反射光像を観測することができ
る乳白色の薄板状を呈する特許請求の範囲第3項
記載の平坦度測定装置。
[Claims] 1. Transparent or semi-transparent plate-shaped objects to be measured are arranged in an overlapping manner on the light incident side of a reference reflecting plate having a flat reference reflecting surface, and are shielded from light by a grid-like reference pattern. irradiating a light beam set so that the object to be measured is included in the illumination area at a predetermined angle with respect to the normal to the reference reflecting surface, A first reflected light image and a second reflected light image resulting from reflection on the reference reflective surface are projected on the same screen, and due to a deviation between the first reflected light image and the second reflected light image, the object to be measured is A flatness measurement method characterized by determining the amount of warpage. 2. The flatness measuring method according to claim 1, wherein the predetermined angle of inclination is 5 degrees or less. 3. A reference reflecting plate having a flat reference reflecting surface and on which a transparent or semi-transparent plate-shaped object to be measured can be arranged so as to overlap on the light incident side; and a predetermined angle with respect to the normal of the reference reflecting surface. a light source that irradiates the reference reflective surface with a light beam set such that the object to be measured is included in its illumination area from an inclined direction; and a light source that is located between the light source and the reference reflective surface; a light shielding part that blocks the irradiated light from the reference reflective surface using a grid-like reference pattern; and a screen that projects an image of the reflected light from the reference reflecting surface and the object to be measured, the image of the object to be measured projected onto the screen. Flatness characterized in that the amount of warpage of the object to be measured is determined from the difference between a first reflected light image due to reflection on the surface of the object and a second reflected light image due to reflection on the reference reflective surface. measuring device. 4. The flatness measuring device according to claim 3, wherein the screen has a milky white thin plate shape that allows the first reflected light image and the second reflected light image to be observed from the back side.
JP18705886A 1986-08-08 1986-08-08 Method and instrument for measuring flatness Granted JPS6342413A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18705886A JPS6342413A (en) 1986-08-08 1986-08-08 Method and instrument for measuring flatness

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18705886A JPS6342413A (en) 1986-08-08 1986-08-08 Method and instrument for measuring flatness

Publications (2)

Publication Number Publication Date
JPS6342413A JPS6342413A (en) 1988-02-23
JPH0463322B2 true JPH0463322B2 (en) 1992-10-09

Family

ID=16199427

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18705886A Granted JPS6342413A (en) 1986-08-08 1986-08-08 Method and instrument for measuring flatness

Country Status (1)

Country Link
JP (1) JPS6342413A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04102415U (en) * 1991-01-23 1992-09-03 旭光学工業株式会社 Film flatness measuring device
CN102692197B (en) * 2011-03-21 2014-10-08 上海茂霖高分子科技有限公司 Detector for flatness of semi-conductive rubber covered roller and detecting method thereof
FR3066816B1 (en) * 2017-05-24 2020-09-04 Centre Nat Rech Scient OPTICAL DEVICE FOR MEASURING THE CURVATURE OF A REFLECTIVE SURFACE
CN114263355B (en) * 2021-12-10 2023-08-25 中国一冶集团有限公司 Curtain wall installation adjusting device

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56122906A (en) * 1980-03-01 1981-09-26 Hitachi Maxell Ltd Measuring method for surface flatness of magnetic recording medium
JPS5862506A (en) * 1981-10-12 1983-04-14 Matsushita Electric Ind Co Ltd Inspecting device for micro-unevenness on surface

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56122906A (en) * 1980-03-01 1981-09-26 Hitachi Maxell Ltd Measuring method for surface flatness of magnetic recording medium
JPS5862506A (en) * 1981-10-12 1983-04-14 Matsushita Electric Ind Co Ltd Inspecting device for micro-unevenness on surface

Also Published As

Publication number Publication date
JPS6342413A (en) 1988-02-23

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