JPH05209723A - Method for measuring thickness of transparent sheet - Google Patents

Method for measuring thickness of transparent sheet

Info

Publication number
JPH05209723A
JPH05209723A JP4040692A JP4040692A JPH05209723A JP H05209723 A JPH05209723 A JP H05209723A JP 4040692 A JP4040692 A JP 4040692A JP 4040692 A JP4040692 A JP 4040692A JP H05209723 A JPH05209723 A JP H05209723A
Authority
JP
Japan
Prior art keywords
transparent sheet
distance
point
thickness
measured
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
JP4040692A
Other languages
Japanese (ja)
Inventor
Koichi Takahashi
浩一 高橋
Hideji Matsumura
松村  秀司
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.)
Mitsui Toatsu Chemicals Inc
Original Assignee
Mitsui Toatsu Chemicals Inc
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 Mitsui Toatsu Chemicals Inc filed Critical Mitsui Toatsu Chemicals Inc
Priority to JP4040692A priority Critical patent/JPH05209723A/en
Publication of JPH05209723A publication Critical patent/JPH05209723A/en
Pending legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)
  • Measurement Of Optical Distance (AREA)

Abstract

PURPOSE:To measure the thickness of a transparent sheet highly accurately by setting the path of laser light at a light path when the distance between preset two points is measured by triangulation, and using the difference between the distance values between two points, when the transparent sheet is not arranged yet and when the sheet is arranged, and a refractive index. CONSTITUTION:The path of laser light of a laser displacement gage 1 is set so that a distance D between a point A and a spot light source P is measured based on an angle 9 of the laser light, which is received by a light receiving part 3 at a point B, with the distance C between the point A and the point B that is a constant as a reference. In this light path, a transparent sheet 4 to be measured is arranged in parallel with a diffusing and reflecting surface so that the laser light is refracted one time and made to pass without reflection. When the light is refracted and made to pass through the sheet 4, the angle theta of the laser light, which is received by the light receiving part 3 at the point B, is changed to the same angle when the position of the spot light source P is located at a point Q. The distance D as the constant is measured as a distance (d) between the point A and the point Q, and deviation Z is generated. A refractive index (n) of the transparent sheet 4 to be measured is applied on the deviation Z. Thus, a thickness (t) is computed.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は透明シートの厚さ測定方
法に関し、詳しくはレーザー変位計のレーザー光を利用
した非接触型の測定方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a transparent sheet thickness measuring method, and more particularly to a non-contact type measuring method using a laser beam of a laser displacement meter.

【0002】[0002]

【発明の背景】従来、透明シートの厚さを測定するに
は、機械的接触による測定方法、即ち、マイクロメータ
等の測定器によって被測定物である透明シートを挾着し
て測定する単なる測定方法が簡易且つ安価でしかも高精
度な測定が可能であることから広く採用されている。し
かし、かかる測定方法では、透明シートがデリケートな
材質の物である場合、測定器によって透明シートを挾着
する際に表面に傷や汚れを付けてしまうことがあるの
で、測定することができない。
BACKGROUND OF THE INVENTION Conventionally, in order to measure the thickness of a transparent sheet, a measurement method by mechanical contact, that is, a mere measurement in which a transparent sheet which is an object to be measured is sandwiched by a measuring device such as a micrometer is used. It is widely used because the method is simple and inexpensive, and highly accurate measurement is possible. However, with such a measuring method, when the transparent sheet is made of a delicate material, the surface of the transparent sheet may be scratched or soiled when the transparent sheet is clamped by the measuring instrument, and therefore the measurement cannot be performed.

【0003】従って、上記のような接触型の測定方法に
よって測定できない材質の透明シートの場合には、透明
シートの厚さに応じて増減する赤外線吸収度の違いを利
用して厚さを測定する非接触型の赤外線吸収式厚さ測定
方法が行われている。
Therefore, in the case of a transparent sheet made of a material that cannot be measured by the contact type measuring method as described above, the thickness is measured by utilizing the difference in infrared absorption which increases or decreases depending on the thickness of the transparent sheet. A non-contact infrared absorption type thickness measuring method is used.

【0004】[0004]

【発明が解決しようとする課題】しかし、前記赤外線吸
収式厚さ測定方法では、測定物である透明シートの赤外
線吸収度を利用しているため、透明シートの色調や霞度
等により透明度が変化した場合に赤外線吸収度も変化す
るので誤差が生じ易い。また測定機構が複雑であるため
装置が高価となるという欠点を有している。
However, in the above infrared absorption type thickness measuring method, since the infrared absorption of the transparent sheet which is the object to be measured is utilized, the transparency changes depending on the color tone or the haze of the transparent sheet. In that case, the infrared absorption also changes, so an error is likely to occur. Further, it has a drawback that the device is expensive because the measuring mechanism is complicated.

【0005】尚、前記機械的接触による測定方法では、
長尺や幅広の透明シートの厚さ均一性を測定する場合に
は、手間がかかり煩雑であるという欠点を有している。
Incidentally, in the measuring method by the mechanical contact,
When measuring the thickness uniformity of a long or wide transparent sheet, there is a drawback that it is troublesome and complicated.

【0006】そこで本発明の目的は、透明シートの厚さ
を容易且つ高精度に測定することができる非接触型の測
定方法を提供することにある。
Therefore, an object of the present invention is to provide a non-contact type measuring method capable of easily and highly accurately measuring the thickness of a transparent sheet.

【0007】[0007]

【課題を解決するための手段】本発明者らは、上記目的
を達成するため、鋭意検討を重ねた結果、本発明に至っ
たものである。
The present inventors have achieved the present invention as a result of extensive studies to achieve the above object.

【0008】即ち、本発明に係る透明シートの厚さ測定
方法は、レーザー変位計のレーザー光の光路を、予め設
定された二点間の距離を三角測量により測定する際の光
路に設定し、該レーザー光の光路中に測定すべき透明シ
ートを前記レーザー光が全反射することなく少なくとも
1回屈折通過するように配置し、該透明シート屈折通過
により変化して得られる二点間距離値と本来の透明シー
ト未配置の場合の二点間距離値との差と、透明シートの
屈折率とから、透明シートの厚さを算出することを特徴
とする。
That is, in the method for measuring the thickness of a transparent sheet according to the present invention, the optical path of the laser beam of the laser displacement meter is set to the optical path for measuring the preset distance between two points by triangulation, A transparent sheet to be measured is arranged in the optical path of the laser beam so that the laser beam can be refracted and passed at least once without being totally reflected, and the distance between two points obtained by changing the refraction of the transparent sheet. It is characterized in that the thickness of the transparent sheet is calculated from the difference between the two-point distance value when the original transparent sheet is not arranged and the refractive index of the transparent sheet.

【0009】また本発明に係る透明シートの厚さ測定方
法の好ましい実施態様は、測定すべき透明シートの屈折
率が温度により変化する場合、温度補正値を加えて透明
シートの厚さを算出することである。
A preferred embodiment of the transparent sheet thickness measuring method according to the present invention calculates the thickness of the transparent sheet by adding a temperature correction value when the refractive index of the transparent sheet to be measured changes with temperature. That is.

【0010】尚、本明細書において、透明シートとは、
レーザー光を透過するシートをいうものであり、レーザ
ー光を透過するものであればその透明度、霞度及び色調
は特に限定されず、半透明シートも含むものである。
In the present specification, the transparent sheet means
The term “transparent sheet” refers to a sheet that transmits laser light, and the transparency, haze, and color tone are not particularly limited as long as the sheet transmits laser light, and includes a semitransparent sheet.

【0011】[0011]

【発明の作用】本発明によれば、公知のレーザー変位計
のレーザー光の光路を、予め設定された二点間の距離を
三角測量により測定する際の光路に設定し、該レーザー
光の光路中に測定すべき透明シートを前記レーザー光が
全反射することなく少なくとも1回屈折通過するように
配置することにより、レーザー光は透明シートを通過す
る際に屈折し光路変更が生じる。この光路変更により、
受光部の拡散光受光角が変わり、前記定まった二点間の
距離が見掛け上変化することになる。この変化の度合い
は、透明シートの屈折率一定下で厚さと対応する。従っ
て、本来の透明シート未配置の場合の定まった二点間距
離値に対する前記変化の度合いに、透明シートの屈折率
を加味することにより、透明シートの厚さを算出するこ
とができる。
According to the present invention, the optical path of the laser beam of the known laser displacement meter is set to the optical path for measuring the preset distance between two points by triangulation, and the optical path of the laser beam is set. By arranging the transparent sheet to be measured therein so that the laser light can be refracted and passed at least once without being totally reflected, the laser light is refracted when passing through the transparent sheet, and the optical path is changed. By changing this optical path,
The light receiving angle of the diffused light of the light receiving portion changes, and the distance between the two fixed points apparently changes. The degree of this change corresponds to the thickness of the transparent sheet under a constant refractive index. Therefore, the thickness of the transparent sheet can be calculated by adding the refractive index of the transparent sheet to the degree of the change with respect to the determined distance value between the two points when the original transparent sheet is not arranged.

【0012】ところで、レーザー変位計は非透明シート
の厚さを測定する際に用いられるものであり、その測定
方法は、シートの一方の面までの距離と他方の面までの
距離を夫々二台のレーザー変位計を用いて測定し、その
和から二台のレーザー変位計間の距離を差し引いて厚さ
を求めるものである。かかる測定方法では、シートの両
面においてレーザー光が反射することが絶対条件である
ため、レーザー光が反射することなく透過してしまう透
明シートの厚さを測定することができない。
A laser displacement meter is used to measure the thickness of a non-transparent sheet, and the measuring method is to measure the distance to one side of the sheet and the distance to the other side of the sheet, respectively. The thickness is obtained by subtracting the distance between the two laser displacement meters from the sum obtained by measuring using the laser displacement meter. In such a measuring method, since it is an absolute condition that the laser light is reflected on both surfaces of the sheet, it is impossible to measure the thickness of the transparent sheet through which the laser light is transmitted without being reflected.

【0013】[0013]

【実施例】以下、本発明の実施例について添付図面に基
づき説明する。
Embodiments of the present invention will be described below with reference to the accompanying drawings.

【0014】図1は本発明の測定方法の一例を示す概略
説明図、図2〜図5は他の例を示す概略説明図である。
FIG. 1 is a schematic explanatory view showing an example of the measuring method of the present invention, and FIGS. 2 to 5 are schematic explanatory views showing other examples.

【0015】図において、1はレーザー変位計、2はレ
ーザー光投光部、3はレーザー光受光部、4は測定すべ
き透明シート、5はレーザー変位計1の投光部2及び受
光部3と平行面である拡散反射面である。また、点Aは
レーザー光投光部2の位置(以下、単に点Aという)、
点Bはレーザー光受光部3の位置(以下、単に点Bとい
う)、Cは点Aから点Bまでの距離であって予め設定し
た定数(以下、単に距離Cという)、Dは点Aから拡散
反射面5までの距離であって予め設定した定数(以下、
単に距離Dという)、Pは投光部2から発したレーザー
光の拡散反射面5における点光源の位置(以下、点光源
Pという)、nは透明シート4の屈折率、tは透明シー
ト4の厚さ、θは点Bの受光部3に受光されるレーザー
光の角度であって被測定物である透明シート4の厚さt
と屈折率nによって変化する変数(以下、単に角度θと
いう)。さらに下記説明において、上記に記載の無い符
号については、その都度説明する。
In the figure, 1 is a laser displacement meter, 2 is a laser beam projecting section, 3 is a laser beam receiving section, 4 is a transparent sheet to be measured, and 5 is a projecting section 2 and a receiving section 3 of the laser displacement meter 1. It is a diffuse reflection surface that is parallel to. Further, the point A is the position of the laser light projecting unit 2 (hereinafter, simply referred to as the point A),
Point B is the position of the laser light receiving portion 3 (hereinafter simply referred to as point B), C is the distance from point A to point B and is a preset constant (hereinafter simply referred to as distance C), and D is from point A. The distance to the diffuse reflection surface 5 and a preset constant (hereinafter,
The distance is simply referred to as D), P is the position of the point light source on the diffuse reflection surface 5 of the laser light emitted from the light projecting portion 2 (hereinafter referred to as point light source P), n is the refractive index of the transparent sheet 4, and t is the transparent sheet 4. , Θ is the angle of the laser beam received by the light receiving portion 3 at the point B, and the thickness t of the transparent sheet 4 which is the object to be measured.
And a variable that changes depending on the refractive index n (hereinafter, simply referred to as an angle θ). Further, in the following description, reference numerals not mentioned above will be explained each time.

【0016】レーザー変位計1のレーザー光の光路は、
予め設定された二点間の距離を三角測量により測定する
際の光路、即ち、点Aから発したレーザー光は、拡散反
射面5の点Pを点光源として点Bの受光部3に受光され
るように設定する。即ち、点Aと点Bの距離であり定数
である距離Cを基準にして点Bの受光部3に受光される
レーザー光の角度θから、点Aと点光源Pとの距離Dを
測定するように設定する。本発明では、三角測量によっ
て測定される前記距離Dを予め設定した定数とする。
The optical path of the laser beam of the laser displacement meter 1 is
The optical path when the preset distance between two points is measured by triangulation, that is, the laser light emitted from the point A is received by the light receiving unit 3 at the point B using the point P of the diffuse reflection surface 5 as the point light source. To set. That is, the distance D between the point A and the point light source P is measured from the angle θ of the laser light received by the light receiving unit 3 at the point B with reference to the distance C which is the distance between the point A and the point B and is a constant. To set. In the present invention, the distance D measured by triangulation is set as a preset constant.

【0017】以上のように設定されたレーザー変移計1
のレーザー光の光路中に測定すべき透明シート4を拡散
反射面5と平行に、且つ前記レーザー光が全反射するこ
となく少なくとも1回屈折通過するように配置する。図
1の場合に透明シート4を屈折通過するのは、点光源P
において拡散反射し受光部3に受光されるレーザー光で
ある。
The laser displacement meter 1 set as described above
The transparent sheet 4 to be measured is arranged parallel to the diffuse reflection surface 5 in the optical path of the laser light, and the laser light is refracted at least once without being totally reflected. In the case of FIG. 1, it is point light source P that refracts and passes through the transparent sheet 4.
The laser light is diffusely reflected at and is received by the light receiving unit 3.

【0018】透明シート4を屈折通過することにより、
点Bの受光部3に受光されるレーザー光の角度θが、点
光源Pの位置が点線で示すように点Qに存在した場合と
同じ角度に変わる。従って、本来、定数である距離D
が、点Aと点Qの距離である距離dと測定されてしまう
ことになり、点Pと点Qの距離である偏差Zが生じる。
偏差Zは、透明シート4の屈折率n一定下で厚さtと対
応する。従って、この偏差Zに被測定物である透明シー
ト4の屈折率nを加味することにより、厚さtを算出す
ることができる。偏差Zと屈折率nとから厚さtを求め
る計算式[1]を下記に示す。
By refracting and passing through the transparent sheet 4,
The angle θ of the laser light received by the light receiving unit 3 at the point B changes to the same angle as when the position of the point light source P is at the point Q as shown by the dotted line. Therefore, the distance D which is originally a constant
Will be measured as the distance d that is the distance between the points A and Q, and the deviation Z that is the distance between the points P and Q will occur.
The deviation Z corresponds to the thickness t under a constant refractive index n of the transparent sheet 4. Therefore, the thickness t can be calculated by adding the refractive index n of the transparent sheet 4, which is the object to be measured, to this deviation Z. A calculation formula [1] for obtaining the thickness t from the deviation Z and the refractive index n is shown below.

【0019】[0019]

【式1】 [Formula 1]

【0020】尚、本発明において、測定すべき透明シー
ト4の屈折率nが温度により変化する場合には、温度補
正を行うこととする。また、定数である距離C及び距離
Dが測定環境等の条件により変動してしまう場合等、距
離C及び距離Dの精密管理が困難な場合には、距離C及
び距離Dを定数として厚さtと角度θの関係を計算して
検量線を作成してゼロ・スパン補正を行うこととする。
In the present invention, when the refractive index n of the transparent sheet 4 to be measured changes with temperature, temperature correction is performed. Further, when it is difficult to precisely manage the distance C and the distance D, such as when the distance C and the distance D, which are constants, change due to conditions such as a measurement environment, the thickness t is set to the constant t. And the angle θ are calculated and a calibration curve is created to perform zero / span correction.

【0021】尚また、本発明ではパソコン等を利用して
上記計算式[1]をソフト化し、さらに各種補正値を入
力可能とすることにより自動計測・算出可能に制御する
ことが好ましい。
Further, in the present invention, it is preferable to control the automatic calculation / calculation by using a personal computer or the like to make the above calculation formula [1] into software and further inputting various correction values.

【0022】以上、本発明に係る透明シートの厚さ測定
方法について説明したが、本発明では、測定すべき透明
シートの配置位置が図2〜図4に示すように変化した場
合でも測定することができる。
The method for measuring the thickness of the transparent sheet according to the present invention has been described above. However, in the present invention, it is possible to measure even when the arrangement position of the transparent sheet to be measured changes as shown in FIGS. You can

【0023】図2に示す態様は、透明シート4を拡散反
射面5に対して斜めに配置した場合、即ち、透明シート
4をレーザー光が2回屈折通過する場合である。
The embodiment shown in FIG. 2 is a case where the transparent sheet 4 is obliquely arranged with respect to the diffuse reflection surface 5, that is, the laser light is refracted and passes through the transparent sheet 4 twice.

【0024】この場合、拡散反射面5上の点光源の位置
はPではなくP′となり、点Bである受光部3への光路
は、P′〜X〜Y〜Bとなる。ここでBY//XP′。こ
のときの角度θはBY延長点と拡散反射面4との成す角
∠YP″Oに等しい。従って、見掛け上の距離は点Aと
点Qの距離である距離dとして測定されることになり、
点Pと点Qの距離である偏差Zが生じる。この偏差Zと
屈折率nとから前記計算式[1]により厚さtを求め
る。本態様の場合を下記に計算式[2]として示す。
In this case, the position of the point light source on the diffuse reflection surface 5 is not P but P ', and the optical path to the light receiving portion 3 at the point B is P'-X-Y-B. BY // XP 'here. The angle θ at this time is equal to the angle ∠YP ″ O formed by the BY extension point and the diffuse reflection surface 4. Therefore, the apparent distance is measured as the distance d which is the distance between the points A and Q. ,
A deviation Z, which is the distance between the points P and Q, occurs. From the deviation Z and the refractive index n, the thickness t is calculated by the above calculation formula [1]. The case of this embodiment is shown below as a calculation formula [2].

【0025】[0025]

【式2】 [Formula 2]

【0026】上記計算式[2]において、P′は透明シ
ート4によって屈折通過したレーザー光の拡散反射面5
における点光源の位置、P″は点Bより透明シート4越
しに見た時の点光源の位置、αは透明シート4が拡散反
射面5と成す角度、βは(90°−前記α)であり、そ
の他の記号は前述の通りである。即ち、レーザー光が透
明シート4を2回屈折通過する場合、透明シート4が拡
散反射面5と成す角度αが決まっていれば、その条件を
上記計算式[2]に当てはめることで厚さtが求まる。
In the above calculation formula [2], P'is a diffuse reflection surface 5 of the laser light refracted and passed by the transparent sheet 4.
Position of the point light source, P ″ is the position of the point light source when viewed from the point B through the transparent sheet 4, α is the angle that the transparent sheet 4 forms with the diffuse reflection surface 5, and β is (90 ° -α). The other symbols are as described above, that is, when the laser light refracts and passes through the transparent sheet 4 twice, if the angle α formed by the transparent sheet 4 and the diffuse reflection surface 5 is determined, the conditions are as described above. The thickness t can be obtained by applying the calculation formula [2].

【0027】上記のように斜めであって尚且つその角度
が45°の場合を、図3に基づき下記に計算式[3]と
して示す。
The case where the angle is 45 ° as described above and the angle is 45 ° is shown as a calculation formula [3] below based on FIG.

【0028】[0028]

【式3】 [Formula 3]

【0029】以上の図2及び図3の他、図4及び図5に
示すように透明シート4を配置して該透明シート4の端
部を利用しても測定することができる。即ち、図4は透
明シート4を拡散反射面5と平行に且つ投光部2からの
レーザー光が通過しないように配置し、点光源Pで拡散
反射したレーザー光のみを1回屈折通過させる態様であ
り、また図5は透明シート4を拡散反射面5に対して斜
めに配置し、レーザー光を1回屈折通過した後に拡散反
射面5において拡散反射させ、該拡散反射したレーザー
光が透明シート4を通過することなく受光部3に受光さ
れる態様である。
In addition to the above-mentioned FIGS. 2 and 3, as shown in FIGS. 4 and 5, the transparent sheet 4 may be arranged and the edge portion of the transparent sheet 4 may be used for the measurement. That is, in FIG. 4, the transparent sheet 4 is arranged in parallel with the diffuse reflection surface 5 so that the laser light from the light projecting unit 2 does not pass therethrough, and only the laser light diffusely reflected by the point light source P is refracted and passed once. Further, FIG. 5 shows that the transparent sheet 4 is obliquely arranged with respect to the diffuse reflection surface 5, the laser light is refracted and passed once and then diffused and reflected by the diffuse reflection surface 5, and the laser light diffusely reflected is a transparent sheet. This is a mode in which the light is received by the light receiving unit 3 without passing through 4.

【0030】以下、本発明の実験例について説明する。 実験例1 前記距離Cを20mm、距離Dを40mmと設定したレ
ーザー変位計によって、屈折率n=1.59のポリカー
ボネート(PC)製の透明シートを拡散反射面と平行に
配置して厚さを測定した。尚、透明シートは、公称厚1
mm、2mm、3mm、5mm、8mmの5種類とし、
マイクロメータ及び赤外吸収式による測定も同時に行っ
た。結果を下記表1に示す。尚、レーザー変位計として
は、市販のキーエンス社製LBシリーズを利用し、拡散
反射面は白紙とした。尚また、赤外線吸収式厚さ測定装
置としては、クラボウ社製赤外線厚さ計測装置を使用し
た。
Experimental examples of the present invention will be described below. Experimental Example 1 A transparent sheet made of polycarbonate (PC) having a refractive index n = 1.59 is arranged in parallel with the diffuse reflection surface by a laser displacement meter having the distance C set to 20 mm and the distance D set to 40 mm to adjust the thickness. It was measured. The transparent sheet has a nominal thickness of 1
mm, 2 mm, 3 mm, 5 mm, and 8 mm,
Measurements by a micrometer and infrared absorption method were also performed at the same time. The results are shown in Table 1 below. A commercially available LB series manufactured by Keyence Corporation was used as the laser displacement meter, and the diffuse reflection surface was a blank sheet. As the infrared absorption type thickness measuring device, an infrared thickness measuring device manufactured by Kurabo Industries, Ltd. was used.

【0031】[0031]

【表1】 [Table 1]

【0032】表1の結果から、本発明の測定方法によれ
ば、マイクロメータと同程度の精度での測定が可能であ
ることが判る。また、赤外線吸収式の場合、本発明の測
定方法と同程度の精度を得るためには装置の価格が10
倍程度となり、極めて高コストであるだけでなく、測定
に際しては、測定位置等の測定条件が厳密であるため測
定に手間がかかった。
From the results shown in Table 1, it can be seen that the measuring method of the present invention enables measurement with the same accuracy as a micrometer. In the case of the infrared absorption type, the price of the device is 10 in order to obtain the same accuracy as the measuring method of the present invention.
This is about double the cost and extremely high cost. In addition, it takes time and effort to perform the measurement because the measurement conditions such as the measurement position are strict.

【0033】実験例2 半透明シートに変えた以外は実験例1と同様にして実験
を行ったところ、本発明の測定方法では略同じ結果が得
られたのに対し、赤外線吸収式による測定では、かなり
の誤差が生じた。これは透明度の変化に応じて透明シー
トの赤外線吸収度が変化したためと思われる。
Experimental Example 2 An experiment was conducted in the same manner as in Experimental Example 1 except that a semi-transparent sheet was used. The measurement method of the present invention gave substantially the same results, while the infrared absorption measurement method , There was a considerable error. This is probably because the infrared absorption of the transparent sheet changed according to the change in transparency.

【0034】実験例1及び2から判る通り、本発明の測
定方法によれば、透明シートの厚さを、計器として比較
的簡易である公知のレーザー変位計のレーザー光を利用
して光の屈折を原理とすることで、極めて簡易且つ容易
に低コストで測定することができる。又、測定装置をコ
ンピュータと接続し、更に前記各計算式をソフト化して
おくことにより、計測・算出・表示が簡易に自動的に行
われるように構成することが好ましい。
As can be seen from Experimental Examples 1 and 2, according to the measuring method of the present invention, the thickness of the transparent sheet is refracted by using the laser light of a known laser displacement meter which is relatively simple as an instrument. Based on the principle, the measurement can be performed very easily and easily at low cost. Further, it is preferable that the measuring device is connected to a computer, and the calculation formulas described above are made into software so that measurement, calculation and display can be easily and automatically performed.

【0035】尚、レーザー変位計として、レーザー光の
受光量を同時に測定可能なものを用いれば、透明シート
通過後の吸収によって減衰したレーザー光の受光量から
該レーザー光の減衰量(又は吸収度)を算出し、該減衰
量と前記算出された透明シートの厚さとから単位厚さ当
りの光線透過率が判明するので、透明シートの透明度を
測定することが可能である。
If a laser displacement meter capable of simultaneously measuring the amount of received laser light is used, the amount of laser light attenuated (or the degree of absorption) of the laser light attenuated by absorption after passing through the transparent sheet. ) Is calculated, and the light transmittance per unit thickness is found from the attenuation amount and the calculated thickness of the transparent sheet, so that the transparency of the transparent sheet can be measured.

【0036】[0036]

【発明の効果】本発明によれば、レーザー光を透過する
ものであれば透明シートの色調、霞度等の透明度の変化
に影響されないので誤差が少ないという効果を有してい
る。
According to the present invention, as long as a laser beam can be transmitted, it is not affected by changes in transparency such as color tone and haze of a transparent sheet, so that it has an effect of reducing errors.

【0037】また、赤外線吸収式厚み測定方法に比し
て、測定範囲が広いだけでなく、用いる装置が計器とし
て比較的簡易且つ低価格で得られる公知のレーザー変位
計のレーザー光を利用するので、同程度の精度であれば
10分の1の価格、同程度の価格の装置であれば10倍
の精度となるので低コストであるという効果を有してい
る。
Further, in comparison with the infrared absorption type thickness measuring method, not only the measuring range is wide, but also the apparatus used uses a laser beam of a known laser displacement meter which is relatively simple and inexpensive as an instrument. However, if the accuracy is about the same, the cost is 1/10, and if the apparatus is about the same, the accuracy is 10 times, so that the cost is low.

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

【図1】本発明の測定方法の一例を示す概略説明図であ
る。
FIG. 1 is a schematic explanatory view showing an example of a measuring method of the present invention.

【図2】他の例を示す概略説明図である。FIG. 2 is a schematic explanatory view showing another example.

【図3】他の例を示す概略説明図である。FIG. 3 is a schematic explanatory view showing another example.

【図4】他の例を示す概略説明図である。FIG. 4 is a schematic explanatory view showing another example.

【図5】他の例を示す概略説明図である。FIG. 5 is a schematic explanatory view showing another example.

【符号の説明】[Explanation of symbols]

1 レーザー変位計 2 レーザー光投光部 3 レーザー光受光部 4 透明シート 5 拡散反射面 1 Laser displacement meter 2 Laser light projector 3 Laser light receiver 4 Transparent sheet 5 Diffuse reflection surface

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】レーザー変位計のレーザー光の光路を、予
め設定された二点間の距離を三角測量により測定する際
の光路に設定し、該レーザー光の光路中に測定すべき透
明シートを前記レーザー光が全反射することなく少なく
とも1回屈折通過するように配置し、該透明シート屈折
通過により変化して得られる二点間距離値と本来の透明
シート未配置の場合の二点間距離値との差と、透明シー
トの屈折率とから、透明シートの厚さを算出することを
特徴とする透明シートの厚さ測定方法。
1. An optical path of a laser beam of a laser displacement meter is set to an optical path for measuring a preset distance between two points by triangulation, and a transparent sheet to be measured is provided in the optical path of the laser beam. The distance between two points, which is arranged so that the laser light passes through refraction at least once without being totally reflected, and the distance between two points obtained by changing the transparent sheet through refraction and the distance between two points when the original transparent sheet is not arranged. A method for measuring the thickness of a transparent sheet, comprising calculating the thickness of the transparent sheet from the difference between the value and the refractive index of the transparent sheet.
【請求項2】測定すべき透明シートの屈折率が温度によ
り変化する場合、温度補正値を加えて透明シートの厚さ
を算出することを特徴とする請求項1記載の透明シート
の厚さ測定方法。
2. The thickness measurement of the transparent sheet according to claim 1, wherein when the refractive index of the transparent sheet to be measured changes with temperature, a temperature correction value is added to calculate the thickness of the transparent sheet. Method.
JP4040692A 1992-01-29 1992-01-29 Method for measuring thickness of transparent sheet Pending JPH05209723A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4040692A JPH05209723A (en) 1992-01-29 1992-01-29 Method for measuring thickness of transparent sheet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4040692A JPH05209723A (en) 1992-01-29 1992-01-29 Method for measuring thickness of transparent sheet

Publications (1)

Publication Number Publication Date
JPH05209723A true JPH05209723A (en) 1993-08-20

Family

ID=12579784

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4040692A Pending JPH05209723A (en) 1992-01-29 1992-01-29 Method for measuring thickness of transparent sheet

Country Status (1)

Country Link
JP (1) JPH05209723A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2503360A1 (en) * 2011-03-25 2012-09-26 Baumer Innotec AG Method for optically detecting at least partially transparent objects and use of a light source and an optical sensor
CN104858772A (en) * 2014-02-21 2015-08-26 株式会社迪思科 Grinding apparatus
JP2016209951A (en) * 2015-05-08 2016-12-15 株式会社ディスコ Dry type polishing device
CN109387488A (en) * 2018-11-29 2019-02-26 中国科学院光电技术研究所 A kind of method for fast measuring and instrument of optical glass refractive index

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2503360A1 (en) * 2011-03-25 2012-09-26 Baumer Innotec AG Method for optically detecting at least partially transparent objects and use of a light source and an optical sensor
EP2503360B1 (en) 2011-03-25 2020-08-19 Baumer Electric AG Method for optically detecting at least partially transparent objects
CN104858772A (en) * 2014-02-21 2015-08-26 株式会社迪思科 Grinding apparatus
JP2015155136A (en) * 2014-02-21 2015-08-27 株式会社ディスコ Polishing device
CN104858772B (en) * 2014-02-21 2019-09-06 株式会社迪思科 Grinding device
JP2016209951A (en) * 2015-05-08 2016-12-15 株式会社ディスコ Dry type polishing device
CN109387488A (en) * 2018-11-29 2019-02-26 中国科学院光电技术研究所 A kind of method for fast measuring and instrument of optical glass refractive index

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