JPS60231105A - Measurement of shift of absorbing axis - Google Patents
Measurement of shift of absorbing axisInfo
- Publication number
- JPS60231105A JPS60231105A JP8887784A JP8887784A JPS60231105A JP S60231105 A JPS60231105 A JP S60231105A JP 8887784 A JP8887784 A JP 8887784A JP 8887784 A JP8887784 A JP 8887784A JP S60231105 A JPS60231105 A JP S60231105A
- Authority
- JP
- Japan
- Prior art keywords
- measured
- axis
- optical system
- transmitted light
- angle
- 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
Links
Landscapes
- Length Measuring Devices By Optical Means (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は吸収軸ズレ測定方法、詳しくは各種偏光板等の
各位置における吸収軸のズレ角を測定する方法に関する
。DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a method for measuring absorption axis deviation, and more particularly to a method for measuring the absorption axis deviation angle at each position of various polarizing plates.
〈従来技術〉
各種偏光板は表示装置、特に液晶を用いた表示装置には
必要不可欠なものである。ところが、この用途の場合、
偏光板の吸収軸がずれていると可視光透過率が規格範囲
から外れる。またそのままセルとして組立てた場合には
色むらが生ずるなどの問題が起っていた。<Prior Art> Various polarizing plates are essential for display devices, especially display devices using liquid crystals. However, for this purpose,
If the absorption axis of the polarizing plate is misaligned, the visible light transmittance will deviate from the standard range. Further, when assembled as a cell as it is, problems such as uneven coloring occur.
〈発明が解決しようとする問題点〉
そこで、従来から各種偏光板の吸収軸のズレ角を測定し
ようと種々の方法が検討されてきているが、末だ確実な
方法が見出されていない。<Problems to be Solved by the Invention> Therefore, various methods have been studied to measure the deviation angle of the absorption axes of various polarizing plates, but no reliable method has yet been found.
本発明は各種偏光板等の各位置における吸収軸のズレ角
を測定できる方法の提供を目的とする。An object of the present invention is to provide a method that can measure the deviation angle of the absorption axis at each position of various polarizing plates.
く問題点を解決するための手段〉
本発明は光源、2つの偏光子、受光器を一軸方向に配列
した直交ニコル光学系により、前記2つの偏光子間に置
かれた被測定試料を前記直交ニコル光学系の軸の回りに
回転しつつその透過光強度を測定し、透過光強度が最低
となる回転位置までの回転角を測定することにより被測
定試料の吸収軸のズレを測定するようにしている。Means for Solving the Problems> The present invention uses an orthogonal Nicol optical system in which a light source, two polarizers, and a light receiver are arranged in a uniaxial direction, so that a sample to be measured placed between the two polarizers is While rotating around the axis of the Nikol optical system, the transmitted light intensity is measured, and the deviation of the absorption axis of the sample to be measured is measured by measuring the rotation angle to the rotational position where the transmitted light intensity is the lowest. ing.
〈実施例〉 図は本発明の方法を実施する装置の斜視図である。<Example> The figure is a perspective view of an apparatus for carrying out the method of the invention.
光源1と、互いに吸収軸が直交するように配設された2
個の偏光子3a、3bと、受光器4から直交ニコル光学
系が構成される。上記両側光子3a、3b間にチップ状
の被測定試料2をその面が前記直交ニコル光学系の軸X
と直交するように挿入し、軸Xの回りに回転させつつ、
各回転位置での透過光を受光器4でとらえ、透過光強度
を測定する。5は試料ホルダである。透過光強度はレコ
ーダ6でペン書きすることができる。この場合用紙6a
の移動速度は前記被測定試料2の回転角速度と予め対応
するようにしておく。A light source 1 and a light source 2 arranged so that their absorption axes are orthogonal to each other.
The polarizers 3a, 3b and the light receiver 4 constitute an orthogonal Nicol optical system. A chip-shaped sample to be measured 2 is placed between the photons 3a and 3b on both sides, with its surface facing the axis X of the orthogonal Nicol optical system.
Insert it so that it is perpendicular to the
The transmitted light at each rotational position is captured by the light receiver 4, and the transmitted light intensity is measured. 5 is a sample holder. The transmitted light intensity can be recorded with a pen on the recorder 6. In this case, paper 6a
The moving speed is made to correspond in advance to the rotational angular velocity of the sample to be measured 2.
被測定試料2の吸収軸のズレ角yの測定を説明する。The measurement of the deviation angle y of the absorption axis of the sample to be measured 2 will be explained.
いま被測定試料2を偏光子3a、偏光子3b間に挿入し
、光源1から平行光線を照射し、透過光を受光器4でさ
らえると、その透過光強度は、I ==A2ein2(
2、g) −Elin” (J / 2)但し δ=2
π・Δn−d/λ
A:定数
0:吸収軸ズレ角
Δn:屈折率差
d:被測定試料の厚さ
λ:光源の波長
で表わされる。Now, when the sample 2 to be measured is inserted between the polarizer 3a and the polarizer 3b, parallel light is irradiated from the light source 1, and the transmitted light is picked up by the receiver 4, the intensity of the transmitted light is I = = A2ein2 (
2, g) −Elin” (J / 2) where δ=2
π·Δn−d/λ A: Constant 0: Absorption axis deviation angle Δn: Refractive index difference d: Thickness of the sample to be measured λ: Represented by the wavelength of the light source.
ここでΔn、dおよびλは同一の装置で、同一の試料で
あれば変化せず、故に5in2(δ/2)の値は一定で
ある。したがって透過光強度工は吸収軸のズレ角yだけ
の関数となる。すなわち、エベ:5in2(20)
となる。Here, Δn, d, and λ do not change if the same device is used and the same sample is used, and therefore the value of 5in2 (δ/2) is constant. Therefore, the transmitted light intensity is a function only of the deviation angle y of the absorption axis. That is, Ebe: 5in2 (20).
したがって、理論的には透過光強度がゼロとなるまでの
回転角yがその被測定試料2の吸収軸のズレ角yになる
が、実際的にはノイズもあるので透過光強度が最低とな
る回転位置までの回転角〆をもって吸収軸のズレ角yと
決定することができる。レコーダ6を用いて透過光の強
度と回転角との関係を表示することにより、被測定試料
2の吸収軸ズレ角〆を即座に視認することができる。ま
た同一ロッドからの多数の被測定試料の吸収軸のズレ角
2を測定する場合は、1つの被測定試料について回転さ
せて、その透過光強度と吸収軸のズレ角yとの関係を予
め明らかにしておくことにより、他の被測定試料につい
ては回転させることなく、その位置での透過光強度を測
定するだけで、それに対応する吸収軸のズレ角グの値を
知ることができる。Therefore, theoretically, the rotation angle y until the transmitted light intensity becomes zero is the deviation angle y of the absorption axis of the sample 2 to be measured, but in reality, since there is noise, the transmitted light intensity is the lowest. The rotation angle up to the rotation position can be determined as the deviation angle y of the absorption axis. By displaying the relationship between the intensity of the transmitted light and the rotation angle using the recorder 6, the absorption axis deviation angle of the sample to be measured 2 can be visually confirmed immediately. In addition, when measuring the deviation angle 2 of the absorption axes of many samples to be measured from the same rod, rotate one sample to be measured and clarify the relationship between the transmitted light intensity and the deviation angle y of the absorption axis in advance. By setting the position to , it is possible to know the value of the corresponding deviation angle of the absorption axis by simply measuring the transmitted light intensity at that position without rotating other samples to be measured.
〈効果〉
本発明は以上の構成よりなり、被測定試料の吸収軸のズ
レ角を容易に、確実に知ることができる。<Effects> With the above configuration, the present invention allows the deviation angle of the absorption axis of the sample to be measured to be easily and reliably known.
測定も迅速におこなうことができるので、偏光板の品質
管理や、生産管理に適用できる。Since measurements can be performed quickly, it can be applied to quality control of polarizing plates and production control.
図は本発明の方法を実施する装置斜視図である。
1・・光源、2・・被測定試料、3a、3b・・偏光子
、4・・受光器、6・・レコーダ、X・・直交ニコル光
学系の軸。
特許出願人 日東電気工業株式会社
代 理 人 弁理士西1) 新The figure is a perspective view of a device implementing the method of the invention. 1. Light source, 2. Sample to be measured, 3a, 3b. Polarizer, 4. Light receiver, 6. Recorder, X. Axis of orthogonal Nicol optical system. Patent applicant: Nitto Electric Industry Co., Ltd. Agent: Patent Attorney Nishi 1) Shin
Claims (1)
ニコル光学系によシ、前記2つの偏光子間に置かれた被
測定試料を前記直交ニコル光学系の軸の回りに回転しつ
つその透過光強度を測定し、透過光強度が最低となる回
転位置までの回転角を測定することによシ被測定試料の
吸収軸のズレ角を測定することを特徴とする吸収軸ズレ
測定方法Using a crossed Nicol optical system in which a light source, two polarizers, and a light receiver are arranged in a uniaxial direction, a sample to be measured placed between the two polarizers is rotated around the axis of the crossed Nicol optical system. An absorption axis deviation measuring method characterized by measuring the deviation angle of the absorption axis of the sample to be measured by measuring the intensity of the transmitted light and measuring the rotation angle to the rotational position where the intensity of the transmitted light is the lowest.
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8887784A JPS60231105A (en) | 1984-05-01 | 1984-05-01 | Measurement of shift of absorbing axis |
US06/687,403 US4684256A (en) | 1983-12-30 | 1984-12-28 | Apparatus and method for continuously measuring polarizing property |
DE19843447878 DE3447878A1 (en) | 1983-12-30 | 1984-12-31 | DEVICE AND METHOD FOR CONTINUOUSLY MEASURING THE POLARIZATION PROPERTY |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8887784A JPS60231105A (en) | 1984-05-01 | 1984-05-01 | Measurement of shift of absorbing axis |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS60231105A true JPS60231105A (en) | 1985-11-16 |
JPH0444941B2 JPH0444941B2 (en) | 1992-07-23 |
Family
ID=13955228
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP8887784A Granted JPS60231105A (en) | 1983-12-30 | 1984-05-01 | Measurement of shift of absorbing axis |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60231105A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6435418A (en) * | 1987-07-30 | 1989-02-06 | Matsushita Electric Ind Co Ltd | Method for evaluating liquid crystal orientational capacity of oriented film |
-
1984
- 1984-05-01 JP JP8887784A patent/JPS60231105A/en active Granted
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6435418A (en) * | 1987-07-30 | 1989-02-06 | Matsushita Electric Ind Co Ltd | Method for evaluating liquid crystal orientational capacity of oriented film |
Also Published As
Publication number | Publication date |
---|---|
JPH0444941B2 (en) | 1992-07-23 |
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