JP2014055866A - Diffusion haze value measuring method and measuring device - Google Patents

Diffusion haze value measuring method and measuring device Download PDF

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JP2014055866A
JP2014055866A JP2012201139A JP2012201139A JP2014055866A JP 2014055866 A JP2014055866 A JP 2014055866A JP 2012201139 A JP2012201139 A JP 2012201139A JP 2012201139 A JP2012201139 A JP 2012201139A JP 2014055866 A JP2014055866 A JP 2014055866A
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haze value
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JP5882864B2 (en
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Shigeo Suga
茂雄 須賀
Manabu Muramatsu
学 村松
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Suga Test Instruments Co Ltd
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Abstract

PROBLEM TO BE SOLVED: To provide diffusion haze measuring method and measuring device in which a value representing a ratio of diffusion transmission light at an arbitrary angle in all light ray transmitted light is determined as a diffusion haze value, a diffusion haze value of a specimen can be measured, and a distribution of the diffusion transmission light for each angle can be examined.SOLUTION: Light beams from a light source are made into a parallel luminous flux to be radiated on a specimen, and an optical receiver is moved around an intersection of a radiation plane of the radiated luminous flux and an optical axis so that it takes an arbitrary angle with respect to the optical axis, whereby diffusion transmission light for each angle is measured.

Description

この発明は拡散ヘーズ値測定方法及び測定装置に係り、特に、透明物質の全光線透過光に対する任意の角度での拡散透過光の割合を求めることができる拡散ヘーズ値測定方法及び測定装置に関する。   The present invention relates to a diffusion haze value measuring method and measuring apparatus, and more particularly to a diffusion haze value measuring method and measuring apparatus capable of obtaining the ratio of diffuse transmitted light at an arbitrary angle with respect to the total light transmitted through a transparent substance.

透明プラスチックなど、透明物質の拡散透過光を測定する装置の一つが、JIS K 7 136や、JIS K 7361で規定されている。   One of the apparatuses for measuring diffused transmission light of transparent materials such as transparent plastics is defined by JIS K 7136 and JIS K 7361.

従来、透明物質のヘーズ値(曇価)を測定する方法には、積分球装置を用い、透明体の各波長毎の全光線透過率及び拡散透過率を測定し、「(拡散透過率/全光線透過率)×100」の式に基づいて、波長毎のヘーズ値を求める散乱光測定方法がある。(特許文献1)   Conventionally, as a method for measuring the haze value (cloudiness value) of a transparent substance, an integrating sphere device is used to measure the total light transmittance and diffuse transmittance for each wavelength of the transparent body, and “(diffuse transmittance / total There is a scattered light measurement method for obtaining a haze value for each wavelength based on the formula of “light transmittance” × 100 ”. (Patent Document 1)

また、測定過程中に、ヘーズ値及び全光線透過率の真値が値付けされたヘーズ標準板を測定し、全光線透過率と拡散透過率の補正係数を求め、試料測定の演算に用いるヘーズ値測定方法及び装置がある。(特許文献2)   In addition, during the measurement process, a haze standard plate to which the haze value and the true value of the total light transmittance are assigned is measured, a correction coefficient for the total light transmittance and the diffuse transmittance is obtained, and the haze used for the calculation of the sample measurement. There are value measuring methods and devices. (Patent Document 2)

特開2002−310902号公報JP 2002-310902 A 特許第3341212号公報Japanese Patent No. 3341212

従来、ヘーズ値の測定においては、拡散透過光を角度毎に直接測定して求めるものはなかった。またその測定において拡散透過光とは、試料を透過した全光線透過光のうち平行線透過光を除くことでもとめられていたものである。従来のヘーズ値とは、全光線透過光中の拡散透過光の割合を表したものである。   Conventionally, in the measurement of the haze value, there has been nothing to obtain by directly measuring diffuse transmitted light for each angle. Further, in the measurement, the diffuse transmission light is also obtained by removing the parallel light transmission light from the total light transmission light transmitted through the sample. The conventional haze value represents the ratio of diffusely transmitted light in the total light transmitted light.

ところで、近年、液晶ディスプレイのバックライト用拡散板などの拡散性や均等性の評価をする上で、試料透過後における光の指向性が重要なファクターの一つとなってきた。しかし上述の通り、従来は光の指向性に基づくヘーズ値の測定方法及び測定装置はなく、拡散透過光の角度特性の測定や、試料への光照射の角度依存性の測定は不可能であった。   Incidentally, in recent years, the directivity of light after passing through a sample has become one of the important factors in evaluating the diffusivity and uniformity of a backlight diffusion plate of a liquid crystal display. However, as described above, conventionally, there is no method and apparatus for measuring haze values based on the directivity of light, and it is impossible to measure the angular characteristics of diffusely transmitted light and to measure the angular dependence of light irradiation on a sample. It was.

この発明は、上記課題を解決するために、従来のヘーズ値が全光線透過光中の拡散透過光の割合を表した値であることに対して、全光線透過光中の任意の角度での拡散透過光の割合を表した値を拡散ヘーズ値とし、試料の拡散ヘーズ値を測定することができるとともに、試料の角度毎の拡散透過光の分布を調べることができる拡散ヘーズ値測定方法及び測定装置を実現することを目的とする。   In order to solve the above-mentioned problem, the present invention has a conventional haze value representing a ratio of diffusely transmitted light in all light transmitted light, but at an arbitrary angle in all light transmitted light. Diffusion haze value measurement method and measurement capable of measuring the diffusion haze value of a sample and determining the distribution of the diffuse transmitted light for each angle of the sample, with the value representing the ratio of diffuse transmitted light as the diffusion haze value The object is to realize the device.

上記目的を達成するために、本発明の拡散ヘーズ値測定方法は、光源からの光を平行光束にして試料に照射し、前記試料内を透過した光束が放射される光束放射面と光軸との交点を中心に、受光器を前記光軸に対して任意の角度を取るように移動させて角度毎の拡散透過光を測定することを特徴とする。これにより、試料の角度毎の拡散透過光の分布を調べることが可能である。   In order to achieve the above object, the diffusion haze value measuring method of the present invention irradiates a sample with light from a light source as a parallel light beam, and emits a light beam that has passed through the sample and an optical axis. The diffused transmitted light at each angle is measured by moving the light receiver so as to take an arbitrary angle with respect to the optical axis, centering on the intersection. Thereby, it is possible to investigate the distribution of diffuse transmitted light for each angle of the sample.

前記拡散ヘーズ値測定方法のさらなる実施形態においては、前記光軸を中心として前記試料を任意に回転させることを特徴とする。   In a further embodiment of the method for measuring the diffusion haze value, the sample is arbitrarily rotated about the optical axis.

前記拡散ヘーズ値測定方法のさらなる実施形態においては、リニア干渉フィルタを搭載した絞りを用いることを特徴とする。   In a further embodiment of the diffusion haze value measuring method, a diaphragm equipped with a linear interference filter is used.

前記拡散ヘーズ値測定方法のさらなる実施形態においては、波長選択フィルタを用いることを特徴とする。   In a further embodiment of the diffusion haze value measuring method, a wavelength selective filter is used.

前記拡散ヘーズ値測定方法のさらなる実施形態においては、前記受光器を前記交点に対して接離方向に任意に移動させることを特徴とする。   In a further embodiment of the diffusion haze value measuring method, the light receiver is arbitrarily moved in the contact / separation direction with respect to the intersection.

前記拡散ヘーズ値測定方法のさらなる実施形態においては、光束寸法可変手段と、受光面積可変手段とを用いることを特徴とする。   In a further embodiment of the diffusion haze value measuring method, a light beam size variable means and a light receiving area variable means are used.

前記拡散ヘーズ値測定方法のさらなる実施形態においては、前記試料を前記光軸に対して垂直または任意の角度に傾斜させることを特徴とする。   In a further embodiment of the method for measuring the diffusion haze value, the sample is inclined perpendicularly to the optical axis or at an arbitrary angle.

また、この発明の拡散ヘーズ値測定装置は、上述の拡散ヘーズ値測定方法により試料の拡散ヘーズ値を測定することを特徴とする。これにより、試料の角度毎の拡散透過光の分布を調べることが可能である。   The diffusion haze value measuring apparatus of the present invention is characterized in that the diffusion haze value of the sample is measured by the above-described diffusion haze value measurement method. Thereby, it is possible to investigate the distribution of diffuse transmitted light for each angle of the sample.

この発明の拡散ヘーズ値測定方法及び測定装置により、全光線透過光中の任意の角度での拡散透過光の割合を表した値を拡散ヘーズ値とし、試料の拡散ヘーズ値を測定するとともに、試料の角度毎の拡散透過光の分布を調べることができる。   With the diffusion haze value measuring method and measuring apparatus of the present invention, a value representing the ratio of diffuse transmitted light at an arbitrary angle in all light transmitted light is defined as a diffusion haze value, and the diffusion haze value of the sample is measured. The distribution of diffuse transmitted light for each angle can be examined.

また、リニア干渉フィルタを搭載した絞りを用いることで、拡散ヘーズ値の測定を波長毎に連続的に読み取ることを可能とし、任意の波長での拡散ヘーズ値を測定することで、波長によって拡散透過光の分布が異なる試料についてもその状況を測定できる。 Also, by using a diaphragm equipped with a linear interference filter, it is possible to continuously read the diffuse haze value for each wavelength, and by measuring the diffuse haze value at an arbitrary wavelength, diffuse transmission depending on the wavelength The situation can also be measured for samples with different light distributions.

あるいは任意の波長において前記リニア干渉フィルタの代わりに、波長選択フィルタを用いて、拡散ヘーズ値を求めることもできる。   Alternatively, the diffusion haze value can be obtained by using a wavelength selection filter instead of the linear interference filter at an arbitrary wavelength.

図1は実施例1の拡散ヘーズ値測定装置の平面構成図である。FIG. 1 is a plan configuration diagram of the diffusion haze value measuring apparatus according to the first embodiment. 図2は実施例2の拡散ヘーズ値測定装置の平面構成図である。FIG. 2 is a plan configuration diagram of the diffusion haze value measuring apparatus according to the second embodiment. 図3は実施例3においてリニア干渉フィルタを用いた拡散ヘーズ値測定装置の平面構成図である。FIG. 3 is a plan configuration diagram of a diffusion haze value measuring apparatus using a linear interference filter in the third embodiment. 図4は実施例3において波長選択フィルタを用いた拡散ヘーズ値測定装置の平面構成図である。FIG. 4 is a plan configuration diagram of a diffusion haze value measuring apparatus using a wavelength selection filter in the third embodiment. 図5は実施例3において450nmの光では均等拡散し、600nmの光では集光拡散する試料の拡散透過光の角度毎の分布を示す図である。 (A)は450nmの均等拡散透過光の角度毎の分布を示す図である。 (B)は600nmの集光拡散透過光の角度毎の分布を示す図である。FIG. 5 is a diagram showing the distribution of the diffused transmission light of the sample for each angle, which diffuses evenly with 450 nm light and collects and diffuses with 600 nm light in Example 3. (A) is a figure which shows distribution for every angle of 450-nm uniform diffused transmitted light. (B) is a figure which shows distribution for every angle of 600-nm condensing diffuse transmission light. 図6は実施例3において450nmと600nmの光で測定した試料の拡散透過光の角度毎の分布を合わせた図である。FIG. 6 is a diagram in which the distribution of the diffuse transmission light of the sample measured with light of 450 nm and 600 nm in Example 3 for each angle is combined. 図7は実施例3で拡散透過光の分布から標準ヘーズ値を算出する方法を示す図である。FIG. 7 is a diagram illustrating a method for calculating a standard haze value from the distribution of diffuse transmitted light in the third embodiment. 図8は実施例4の拡散ヘーズ値測定装置の平面構成図である。FIG. 8 is a plan configuration diagram of the diffusion haze value measuring apparatus according to the fourth embodiment. 図9は実施例5の拡散ヘーズ値測定装置の平面構成図である。FIG. 9 is a plan configuration diagram of the diffusion haze value measuring apparatus according to the fifth embodiment. 図10は実施例6の拡散ヘーズ値測定装置の平面構成図である。FIG. 10 is a plan configuration diagram of the diffusion haze value measuring apparatus according to the sixth embodiment.

以下、図面に基づいて、この発明の実施例を説明する。   Embodiments of the present invention will be described below with reference to the drawings.

図1は、この発明の実施例1を示すものである。図1において、1は本発明の拡散ヘーズ値測定方法を実現する拡散ヘーズ値測定装置である。拡散ヘーズ値測定装置1は、光源2と、集光レンズ3と、絞り4と、コリメータレンズ5と、虹彩絞り6と、受光部7とからなる。受光部7は受光器8と角度可変手段9とからなる。   FIG. 1 shows Embodiment 1 of the present invention. In FIG. 1, reference numeral 1 denotes a diffusion haze value measuring apparatus for realizing the diffusion haze value measuring method of the present invention. The diffuse haze value measuring apparatus 1 includes a light source 2, a condenser lens 3, a diaphragm 4, a collimator lens 5, an iris diaphragm 6, and a light receiving unit 7. The light receiving unit 7 includes a light receiver 8 and an angle variable means 9.

光源2からの光を集光レンズ3、絞り4、コリメータレンズ5によって平行光束とし、虹彩絞り6によって平行光束の断面が任意の径となるように絞る。虹彩絞り6によって絞られた光束Lは、試料11を透過して受光器8の受光素子10で受光される。本実施例では、透明物質で板状に形成した試料11を用いたが、試料11は板状のものに限定されるものではなく、未成型の試料や、セルを使用することで、液体や粒状の試料を測定することも可能である。   The light from the light source 2 is converted into a parallel light beam by the condenser lens 3, the diaphragm 4 and the collimator lens 5, and is narrowed by the iris diaphragm 6 so that the cross section of the parallel light beam has an arbitrary diameter. The light beam L focused by the iris diaphragm 6 passes through the sample 11 and is received by the light receiving element 10 of the light receiver 8. In this example, the sample 11 formed in a plate shape with a transparent material was used. However, the sample 11 is not limited to the plate shape, and an unmolded sample or a cell can be used to obtain liquid or It is also possible to measure a granular sample.

角度可変手段9は、光束Lが試料11内を透過し、光が放射される光束放射面12と光軸13との交点14を中心とし、受光器8を任意の角度θに移動可能としている。角度θは、交点14から受光素子10の受光面の中心までを結ぶ直線と光軸13とのなす角である。角度可変手段9は、交点14を中心として配置した半球面状の保持体15と、交点14から等距離となる保持体15の内周面16に保持されて内周面16上を移動可能な移動具17とにより構成される。すなわち受光器8の受光素子10が交点14に対して等距離rとなるように移動する。受光器8を移動具17により任意の角度θに移動させて試料11を透過した拡散透過光を三次元的に測定する。   The angle varying means 9 allows the light receiver 8 to move to an arbitrary angle θ around the intersection 14 between the light beam emitting surface 12 through which the light beam L passes through the sample 11 and the light is emitted and the optical axis 13. . The angle θ is an angle formed by a straight line connecting the intersection 14 to the center of the light receiving surface of the light receiving element 10 and the optical axis 13. The angle varying means 9 is movable on the inner peripheral surface 16 while being held by the hemispherical holding body 15 arranged around the intersection 14 and the inner peripheral surface 16 of the holding body 15 which is equidistant from the intersection 14. It is comprised with the moving tool 17. FIG. That is, the light receiving element 10 of the light receiver 8 moves so as to be equidistant r with respect to the intersection 14. The diffuser light transmitted through the sample 11 is measured three-dimensionally by moving the light receiver 8 to an arbitrary angle θ by the moving tool 17.

このように、拡散ヘーズ値測定装置1は、従来のヘーズ値が全光線透過光中の拡散透過光の割合を表した値であるのに対して、拡散ヘーズ値として全光線透過光中の任意の角度での拡散透過光の割合を表した値を求めることができる。それによって、拡散ヘーズ値測定装置1は、液晶ディスプレイのバックライト用拡散板のように方向依存性のある透明物質を、より詳細に評価することができる測定装置を実現することができる。   As described above, the diffuse haze value measuring apparatus 1 has a conventional haze value representing the ratio of diffuse transmitted light in the total light transmitted light, whereas the diffuse haze value is an arbitrary value in the total light transmitted light. A value representing the ratio of diffusely transmitted light at the angle can be obtained. Thereby, the diffusion haze value measuring apparatus 1 can realize a measuring apparatus capable of evaluating a transparent substance having direction dependency like a backlight diffusion plate of a liquid crystal display in more detail.

図2は、実施例2を示すものである。拡散ヘーズ値測定装置1の受光部7aは半円形の保持体15aと、交点14から等距離となる保持体15aの内周面16aに保持されて内周面16a上を移動可能な移動具17により構成される角度可変手段9aを備える。すなわち受光部7の受光素子10が交点14に対して等距離rとなるように移動する。受光部7aの角度可変手段9aにおいて、移動具17による受光器8の移動を半円上とし、試料11を、光軸を中心として任意に回転可能となるように試料回転手段18を備えることで、受光器8の移動と試料11の回転との組み合わせによって、試料11を透過した拡散透過光を三次元的に測定する。あるいは試料11を固定し、受光器8を0°〜90°または0°〜−90°と移動させることによって、試料11を透過した拡散透過光を二次元的に測定することも可能である。   FIG. 2 shows a second embodiment. The light receiving portion 7a of the diffusion haze value measuring apparatus 1 is held by a semicircular holding body 15a and an inner peripheral surface 16a of the holding body 15a that is equidistant from the intersection point 14, and is movable on the inner peripheral surface 16a. The angle variable means 9a comprised by these is provided. That is, the light receiving element 10 of the light receiving unit 7 moves so as to be equidistant r with respect to the intersection 14. In the angle variable means 9a of the light receiving portion 7a, the movement of the light receiver 8 by the moving tool 17 is set on a semicircle, and the sample rotating means 18 is provided so that the sample 11 can be arbitrarily rotated around the optical axis. The diffusely transmitted light transmitted through the sample 11 is measured three-dimensionally by a combination of the movement of the light receiver 8 and the rotation of the sample 11. Alternatively, it is also possible to measure the diffusely transmitted light transmitted through the sample 11 two-dimensionally by fixing the sample 11 and moving the light receiver 8 from 0 ° to 90 ° or from 0 ° to −90 °.

図3及び図4は、実施例3を示すものである。実施例1で示した拡散ヘーズ値測定装置1の絞り4に、リニア干渉フィルタ19を配置する(図3)、あるいは、拡散ヘーズ値測定装置1のコリメータレンズ5と虹彩絞り6との間に波長選択フィルタ20を配置する(図4)ことで、任意の波長の拡散ヘーズ値を測定可能とする。本実施例では、波長選択フィルタ20の位置を図4の位置としたが、この位置に限定されるものではなく光路上の任意の位置に設置することができる。図3に示すようにリニア干渉フィルタ19を配置した場合、リニア干渉フィルタ19により光源からの光の波長の透過率を変化させることで、連続したあるいは断続的な波長ごとの拡散ヘーズ値を測定することができる。また図4に示すように波長選択フィルタ20を配置することで、波長を選択的に測定することにより、例えば450nmの光は均等拡散するが(図5(A))、600nmの光は集光拡散する(図5(B))等の、拡散の角度特性が波長によって異なる試料11の拡散透過光の角度毎の分布(図6)を測定可能とする。これによって拡散の角度特性が波長によって異なる試料について、その状況を測定することができる。   3 and 4 show the third embodiment. A linear interference filter 19 is disposed on the diaphragm 4 of the diffuse haze value measuring apparatus 1 shown in the first embodiment (FIG. 3), or the wavelength between the collimator lens 5 and the iris diaphragm 6 of the diffuse haze value measuring apparatus 1 is set. By disposing the selection filter 20 (FIG. 4), it is possible to measure a diffusion haze value of an arbitrary wavelength. In the present embodiment, the position of the wavelength selection filter 20 is the position of FIG. 4, but is not limited to this position, and can be installed at an arbitrary position on the optical path. When the linear interference filter 19 is arranged as shown in FIG. 3, the diffusion haze value for each continuous or intermittent wavelength is measured by changing the transmittance of the wavelength of light from the light source by the linear interference filter 19. be able to. Further, by arranging the wavelength selection filter 20 as shown in FIG. 4, by selectively measuring the wavelength, for example, 450 nm light is evenly diffused (FIG. 5A), but 600 nm light is condensed. It is possible to measure the distribution (FIG. 6) of the diffusely transmitted light of each sample 11 having different diffusion angle characteristics depending on the wavelength, such as diffusion (FIG. 5B). As a result, it is possible to measure the situation of the sample whose diffusion angular characteristics are different depending on the wavelength.

なお、拡散ヘーズ値測定装置1は、波長選択フィルタ20として受光感度が視感度Vλ(Y)を満足するフィルタを使用し、図7に示すように、拡散透過光と平行透過光を測定することで、従来のヘーズ値を算出することができる。   Note that the diffusion haze value measuring apparatus 1 uses a filter whose light receiving sensitivity satisfies the visual sensitivity Vλ (Y) as the wavelength selection filter 20, and measures diffuse transmitted light and parallel transmitted light as shown in FIG. Thus, the conventional haze value can be calculated.

図8は、実施例4を示すものである。実施例4の拡散ヘーズ値測定装置1の受光部7bは、交点14に対して受光器8を接離方向に移動可能な距離可変手段21を備えている。距離可変手段21は、角度可変手段9の移動具17に設置した支持部22と、調節部23とから構成され、調節部23に受光器8を取り付け、調節部23により受光器8を交点14に対して接離方向に移動可能としている。拡散ヘーズ値測定装置1は、交点14に対して距離可変手段21により受光器8を接離方向に移動させて、試料11を透過した拡散透過光を受光器8により測定する。   FIG. 8 shows a fourth embodiment. The light receiving unit 7b of the diffusion haze value measuring apparatus 1 according to the fourth embodiment includes a distance variable unit 21 that can move the light receiver 8 in the contact / separation direction with respect to the intersection 14. The distance variable means 21 includes a support portion 22 installed on the moving tool 17 of the angle variable means 9 and an adjustment portion 23. The light receiver 8 is attached to the adjustment portion 23, and the light receiver 8 is connected to the intersection 14 by the adjustment portion 23. It is possible to move in the contact and separation direction. The diffuse haze value measuring apparatus 1 moves the light receiver 8 in the contact / separation direction by the distance varying means 21 with respect to the intersection point 14, and measures the diffusely transmitted light transmitted through the sample 11 by the light receiver 8.

試料11透過後の光が、受光器8での測定位置によっては弱くなる場合があり、受光する光量が少ないため精度が悪くなる不具合があった。そこで、実施例4の拡散ヘーズ値測定装置1は、距離可変手段21により受光器8を試料11に対して接離方向に移動可能としているので、より光量が多いところで測定するために、受光器8を試料11側に近付けることができ、測定精度を向上することができる。   The light after passing through the sample 11 may become weak depending on the measurement position at the light receiver 8, and there is a problem that accuracy is deteriorated because the amount of received light is small. Therefore, in the diffusion haze value measuring apparatus 1 according to the fourth embodiment, the light receiver 8 can be moved in the contact / separation direction with respect to the sample 11 by the distance varying means 21. 8 can be brought closer to the sample 11 side, and the measurement accuracy can be improved.

図9は、実施例5を示すものである。実施例5の拡散ヘーズ値測定装置1は、試料11に入射される光束の断面の寸法である光束径を任意の大きさに変更可能とする光束寸法可変手段24と、受光素子10の前面に、受光素子10に光が当たる領域を変更可能とする受光面積可変手段25とを備えている。光束寸法可変手段24は、試料11に光が入射する面26側に配置した枠状の開閉調節機構27と、開閉調節機構27に形成した開口部28を任意の大きさに開閉可能な開閉具29とから構成され、光束径を、開閉具29の開閉により開口部28の開口寸法を調節することで変更可能としている。さらに受光面積可変手段25は、受光素子10の前面に配置した調節機構30と、調節機構30に形成した開口部31を任意の大きさに開閉可能な開閉具32とから構成され、光束寸法可変手段24による光束径の変更に対応し、受光素子10に光が当たる面積を変更可能としている。拡散ヘーズ値測定装置1は、光束寸法可変手段24により試料11に入射する光束径を変更して、試料11を透過した拡散透過光を受光器8により測定する。   FIG. 9 shows the fifth embodiment. The diffusion haze value measuring apparatus 1 according to the fifth embodiment includes a light beam dimension varying unit 24 that can change a light beam diameter, which is a cross-sectional dimension of a light beam incident on the sample 11, to an arbitrary size, and a front surface of the light receiving element 10. , And a light receiving area variable means 25 that can change a region where the light receiving element 10 is irradiated with light. The light beam dimension changing means 24 is a frame-like opening / closing adjustment mechanism 27 arranged on the surface 26 side where light enters the sample 11 and an opening / closing tool capable of opening / closing the opening 28 formed in the opening / closing adjustment mechanism 27 to an arbitrary size. 29, and the beam diameter can be changed by adjusting the opening size of the opening 28 by opening / closing the opening / closing tool 29. Further, the light receiving area variable means 25 includes an adjusting mechanism 30 disposed on the front surface of the light receiving element 10 and an opening / closing tool 32 capable of opening and closing an opening 31 formed in the adjusting mechanism 30 to an arbitrary size. Corresponding to the change of the beam diameter by the means 24, the area where the light hits the light receiving element 10 can be changed. The diffusion haze value measuring apparatus 1 changes the diameter of the light beam incident on the sample 11 by the light beam size varying means 24 and measures the diffuse transmitted light that has passed through the sample 11 by the light receiver 8.

従来のヘーズ値測定では、積分球の開口径に対する光束径の寸法が規定されていた為、試料11に入射する光束径を変更するような自由度はなかった。実施例5の拡散ヘーズ値測定装置1は、試料11の大きさに合わせて光束径を変えて測定でき、小さい試料の測定も可能にしている。また、光束径を変更することで、試料透過後の平行線透過光の径も同時に変化するが、受光面積可変手段25によって受光素子10に光が当たる面積を変化させることで対応している。   In the conventional haze value measurement, since the size of the light beam diameter with respect to the opening diameter of the integrating sphere is defined, there is no degree of freedom to change the diameter of the light beam incident on the sample 11. The diffusion haze value measuring apparatus 1 according to the fifth embodiment can measure by changing the beam diameter according to the size of the sample 11 and can also measure a small sample. Further, by changing the beam diameter, the diameter of the parallel-line transmitted light after passing through the sample also changes at the same time, but this is dealt with by changing the area where the light receiving element 10 is irradiated by the light receiving area variable means 25.

図10は、実施例6を示すものである。実施例6の拡散ヘーズ値測定装置1は、光軸13に対して試料11を任意の角度φに変更可能な試料角度変更手段33を備えている。試料角度変更手段33は、試料11の外周を囲むように配置した一部球面円環状の枠体34と、枠体34の内周面35に保持されて光軸13を中心に内周面35上を移動可能な移動具36とにより構成され、試料11の外周を移動具36に取り付け、移動具36により試料11の角度φを任意に変更可能としている。拡散ヘーズ値測定装置1は、試料角度変更手段33により光軸13に対して試料11を角度φに傾斜させて、試料11を透過した拡散透過光を受光器8により測定する。   FIG. 10 shows a sixth embodiment. The diffusion haze value measuring apparatus 1 according to the sixth embodiment includes sample angle changing means 33 that can change the sample 11 to an arbitrary angle φ with respect to the optical axis 13. The sample angle changing means 33 includes a partially spherical annular frame 34 disposed so as to surround the outer periphery of the sample 11, and an inner peripheral surface 35 centered on the optical axis 13 held by the inner peripheral surface 35 of the frame 34. The movable tool 36 is movable on the top, the outer periphery of the sample 11 is attached to the movable tool 36, and the angle φ of the sample 11 can be arbitrarily changed by the movable tool 36. In the diffuse haze value measuring apparatus 1, the sample 11 is tilted at an angle φ with respect to the optical axis 13 by the sample angle changing means 33, and the diffuse transmitted light transmitted through the sample 11 is measured by the light receiver 8.

実施例6の拡散ヘーズ値測定装置1は、積分球を用いずに、受光器8が動いて拡散透過光を測定するため、既存の積分球方式のヘーズ測定方法では、不可能であった斜め入射によるヘーズ値を測定することができる。この拡散ヘーズ値測定装置1の測定方法では、光軸13に対して試料11を直交させて測定することも、試料11の配置を傾斜させて測定することも可能である。   Since the diffuser haze value measuring apparatus 1 of the sixth embodiment measures diffused transmitted light by moving the light receiver 8 without using an integrating sphere, it is not possible with the existing integrating sphere haze measuring method. The haze value due to incidence can be measured. In the measurement method of the diffusion haze value measuring apparatus 1, the measurement can be performed by making the sample 11 orthogonal to the optical axis 13 or by inclining the arrangement of the sample 11.

この発明の拡散ヘーズ値測定装置は、バックライト用拡散板のように放射光の方向依存性がある透明物質の評価に適用することができる。   The diffusion haze value measuring apparatus of the present invention can be applied to the evaluation of a transparent material having direction dependency of radiated light such as a backlight diffusion plate.

1 拡散ヘーズ値測定装置
2 光源
3 集光レンズ
4 絞り
5 コリメータレンズ
6 虹彩絞り
7、7a、7b 受光部
8 受光器
9、9a 角度可変手段
10 受光素子
11 試料
12 光束放射面
13 光軸
14 交点
15、15a 保持体
16、16a 内周面
17 移動具
18 試料回転手段
19 リニア干渉フィルタ
20 波長選択フィルタ
21 距離可変手段
22 支持部
23 調節部
24 光束寸法可変手段
25 受光面積可変手段
26 光が入射する面
27 開閉調節機構
28 開口部
29 開閉具
30 調節機構
31 開口部
32 開閉具
33 試料角度変更手段
34 枠体
35 内周面
36 移動具
DESCRIPTION OF SYMBOLS 1 Diffuse haze value measuring apparatus 2 Light source 3 Condensing lens 4 Aperture 5 Collimator lens 6 Iris diaphragm 7, 7a, 7b Light receiving part 8 Light receiver 9, 9a Angle variable means 10 Light receiving element 11 Sample 12 Light flux emitting surface 13 Optical axis 14 Intersection DESCRIPTION OF SYMBOLS 15, 15a Holding body 16, 16a Inner peripheral surface 17 Moving tool 18 Sample rotation means 19 Linear interference filter 20 Wavelength selection filter 21 Distance variable means 22 Support part 23 Adjustment part 24 Light beam dimension variable means 25 Light-receiving area variable means 26 Light incidence 27 Opening / closing adjustment mechanism 28 Opening portion 29 Opening / closing tool 30 Adjustment mechanism 31 Opening portion 32 Opening / closing tool 33 Sample angle changing means 34 Frame body 35 Inner peripheral surface 36 Moving tool

Claims (8)

光源からの光を平行光束にして試料に照射し、前記試料内を透過した光束が放射される光束放射面と光軸との交点を中心に、受光器を前記光軸に対して任意の角度を取るように移動させて角度毎の拡散透過光を測定することを特徴とする拡散ヘーズ値測定方法。   The sample is irradiated with light from a light source as a parallel light beam, and the light receiver is emitted at an arbitrary angle with respect to the optical axis around the intersection of the light beam emission surface from which the light beam transmitted through the sample is emitted and the optical axis. The diffuse haze value measuring method is characterized in that the diffused transmitted light at each angle is measured by moving the light beam so as to take an angle. 前記光軸を中心として前記試料を任意に回転させることを特徴とする請求項1に記載の拡散ヘーズ値測定方法。   2. The diffusion haze value measuring method according to claim 1, wherein the sample is arbitrarily rotated around the optical axis. リニア干渉フィルタを搭載した絞りを用いることを特徴とする請求項1あるいは請求項2に記載の拡散へーズ値測定方法。   The diffusion haze value measuring method according to claim 1 or 2, wherein a diaphragm equipped with a linear interference filter is used. 波長選択フィルタを用いることを特徴とする請求項1あるいは請求項2に記載の拡散ヘーズ値測定方法。   3. The diffusion haze value measuring method according to claim 1, wherein a wavelength selection filter is used. 前記受光器を前記交点に対して任意に接離方向に移動させることを特徴とする請求項1から請求項4のいずれか一項に記載の拡散ヘーズ値の測定方法。   The method for measuring a diffusion haze value according to any one of claims 1 to 4, wherein the light receiver is arbitrarily moved in a contact / separation direction with respect to the intersection. 光束寸法可変手段と、受光面積可変手段とを用いることを特徴とする請求項1から請求項5のいずれか一項に記載の拡散ヘーズ値測定方法。   6. The diffusion haze value measuring method according to any one of claims 1 to 5, wherein a light beam dimension varying unit and a light receiving area varying unit are used. 前記試料を前記光軸に対して垂直または任意の角度に傾斜させることを特徴とする請求項1から請求項6のいずれか一項に記載の拡散ヘーズ値測定方法。   The diffusion haze value measuring method according to any one of claims 1 to 6, wherein the sample is inclined perpendicularly to the optical axis or at an arbitrary angle. 請求項1から請求項7のいずれか一項に記載の拡散ヘーズ値測定方法を実現する拡散ヘーズ値測定装置。   A diffusion haze value measuring apparatus that realizes the diffusion haze value measuring method according to claim 1.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2020114467A (en) * 2016-10-25 2020-07-30 ラクテン メディカル インコーポレイテッド Light diffusion apparatus for use in photoimmunotherapy

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6117940A (en) * 1984-07-05 1986-01-25 Nippon Paint Co Ltd Method and instrument for measuring dispersion condition of particles in high-density suspension or the like
JPH03107745A (en) * 1989-09-20 1991-05-08 Mitsubishi Rayon Co Ltd Method and device for light scattering measurement
JPH09210848A (en) * 1996-01-31 1997-08-15 Kao Corp Method and apparatus for measurement of transmission and scattering capability
JP2003329570A (en) * 2002-05-10 2003-11-19 Horiba Ltd Apparatus for measuring distribution of particle size
JP2008070290A (en) * 2006-09-15 2008-03-27 Asahi Spectra Co Ltd Apparatus for measuring light distribution characteristics
JP2010071807A (en) * 2008-09-18 2010-04-02 Stanley Electric Co Ltd Photometric method for light source bulb for vehicle lighting fixture and light emitting property model generation method
JP2011033508A (en) * 2009-08-03 2011-02-17 Showa Denko Kk Device and method of measuring characteristic of measured object, program and light-emitting body
US20120081700A1 (en) * 2010-10-01 2012-04-05 Hung-Pin Kuo Optical measurement system

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6117940A (en) * 1984-07-05 1986-01-25 Nippon Paint Co Ltd Method and instrument for measuring dispersion condition of particles in high-density suspension or the like
JPH03107745A (en) * 1989-09-20 1991-05-08 Mitsubishi Rayon Co Ltd Method and device for light scattering measurement
JPH09210848A (en) * 1996-01-31 1997-08-15 Kao Corp Method and apparatus for measurement of transmission and scattering capability
JP2003329570A (en) * 2002-05-10 2003-11-19 Horiba Ltd Apparatus for measuring distribution of particle size
JP2008070290A (en) * 2006-09-15 2008-03-27 Asahi Spectra Co Ltd Apparatus for measuring light distribution characteristics
JP2010071807A (en) * 2008-09-18 2010-04-02 Stanley Electric Co Ltd Photometric method for light source bulb for vehicle lighting fixture and light emitting property model generation method
JP2011033508A (en) * 2009-08-03 2011-02-17 Showa Denko Kk Device and method of measuring characteristic of measured object, program and light-emitting body
US20120081700A1 (en) * 2010-10-01 2012-04-05 Hung-Pin Kuo Optical measurement system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2020114467A (en) * 2016-10-25 2020-07-30 ラクテン メディカル インコーポレイテッド Light diffusion apparatus for use in photoimmunotherapy

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