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JP2018174050A - Film for lighting apparatus, film laminate for lighting apparatus, and lighting apparatus - Google Patents

Film for lighting apparatus, film laminate for lighting apparatus, and lighting apparatus Download PDF

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Publication number
JP2018174050A
JP2018174050A JP2017070328A JP2017070328A JP2018174050A JP 2018174050 A JP2018174050 A JP 2018174050A JP 2017070328 A JP2017070328 A JP 2017070328A JP 2017070328 A JP2017070328 A JP 2017070328A JP 2018174050 A JP2018174050 A JP 2018174050A
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light
film
lighting
degrees
lighting fixture
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勝朗 久世
Katsuro Kuze
勝朗 久世
正夫 高地
Masao Takachi
正夫 高地
池田 篤志
Atsushi Ikeda
篤志 池田
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Nakashima Kogyo Corp
Excel KK
Belle Green Wise Co Ltd
Cargill Meat Solutions Corp
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Nakashima Kogyo Corp
Excel KK
Belle Green Wise Co Ltd
Excel Corp
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Abstract

【課題】発光ダイオード素子を用いた照明器具の明るくなる範囲が狭いという欠点を低コストで改善できる照明器具用フィルム、照明器具用フィルム積層体及びこれらを組み込んだ照明器具を提供する。【解決手段】照明器具用フィルムは、異方性光拡散フィルムから構成され、照明器具の光源ユニットの出光面側に配置して用いられる照明器具用フィルムであって、照明器具用フィルムは、照明器具用フィルムにほぼ垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に、該レーザーポインターの出光方向を傾け、フィルムに入光する光の角度がフィルム面に対して斜めになるように変化させた場合に、フィルムを出光する光の投影像が入光方向の延長方向のみでなく、延長方向と対角にも現れ、少なくとも2方向にスプリットして出光する機能を有する。【選択図】図1Provided are a film for a lighting fixture, a film laminate for a lighting fixture, and a lighting fixture incorporating the same, which can improve at a low cost the disadvantage that the lighting range using a light-emitting diode element is narrow. A film for a lighting fixture is a film for a lighting fixture that is made of an anisotropic light diffusing film and is used by being disposed on a light exit surface side of a light source unit of the lighting fixture. Tilt the light output direction of the laser pointer to the main diffusion direction of light that can be confirmed by irradiating the light of the laser pointer almost perpendicularly to the film, so that the angle of the light entering the film is oblique to the film surface When changed, the projection image of the light emitted from the film appears not only in the extension direction of the incident light direction but also in the diagonal direction with respect to the extension direction, and has a function of splitting the light in at least two directions and outputting the light. [Selection] Figure 1

Description

本発明は、照明器具用フィルム、照明器具用フィルム積層体及び照明器具に関する。   The present invention relates to a film for a lighting fixture, a film laminate for a lighting fixture, and a lighting fixture.

近年エコロジーの観点から、照明用の光源として、消費電力が低く、振動に強く、超高輝度で長時間安定して発光可能な発光ダイオード(以下、LEDという)を用いたLED電球や蛍光管形状のLED管などのLED照明装置が使用されるようになってきている。LEDは上記の長所を有する一方、点光源であるため、光の指向性が高いという特性があるために、白熱電球や蛍光灯に比べて明るくなる範囲が狭いという課題があり、その改善が強く望まれている。   In recent years, from the viewpoint of ecology, LED light bulbs and fluorescent tube shapes that use light-emitting diodes (hereinafter referred to as LEDs) that have low power consumption, vibration resistance, ultra-brightness, and stable light emission for a long period of time as light sources for lighting LED lighting devices such as LED tubes have come to be used. While LED has the above-mentioned advantages, it is a point light source, so it has the characteristic that the directivity of light is high. It is desired.

また、発光ダイオード素子を用いた照明器具は、発光ダイオード素子は発光面積が小さいために発光面の明るさが極めて高いので、照明器具を直視した時の眩しさ、いわゆるグレア性が著しく劣るという課題を有する。そこで、これらの課題を解決する方法として、照明器具の出光面に光を拡散する拡散部材(以下、単に拡散部材と称する)を設置する方法が広く用いられている。例えば、特許文献1の比較例2において、全光線透過率が68.5%で、かつヘーズが99.1%という非常に拡散度の高い拡散板を用いた例が開示されている。しかし、広く用いられている通常の拡散板を用いた場合は、このような拡散度が高い拡散板を用いても1/2ビーム角は104度にしかならない事が記載されている。すなわち、通常の拡散部材を用いた場合は、拡散度の高い拡散部材を用いても、該拡散部材を出光する光の配光分布は、極座標表示の配光分布が円形となるランバシアン分布に近づける事ができるのみで、それ以上の高配光角を達成する事は困難である。というのは、光学部材として通常の拡散板を用いた場合は、光源の法線方向に強く放出された光を、該法線方向となす角度をθとした時、cosθに比例して光度が減衰する指向性を有しているためである。   In addition, the lighting fixture using the light emitting diode element has a problem that the glare when the lighting fixture is directly viewed, that is, the so-called glare property, is extremely inferior because the light emitting diode has a small light emitting area and the brightness of the light emitting surface is extremely high. Have Therefore, as a method for solving these problems, a method of installing a diffusing member that diffuses light (hereinafter simply referred to as a diffusing member) on a light exit surface of a lighting fixture is widely used. For example, in Comparative Example 2 of Patent Document 1, an example using a diffusion plate having a very high diffusivity having a total light transmittance of 68.5% and a haze of 99.1% is disclosed. However, it is described that when an ordinary diffuser plate that is widely used is used, even if such a diffuser plate having a high diffusivity is used, the 1/2 beam angle is only 104 degrees. That is, when a normal diffusing member is used, even if a diffusing member having a high diffusivity is used, the light distribution of the light emitted from the diffusing member is close to the Lambertian distribution in which the light distribution in the polar coordinate display is circular. It is difficult to achieve a high light distribution angle beyond that. This is because when a normal diffuser plate is used as an optical member, the light intensity is proportional to cos θ, where θ is the angle between the light emitted strongly in the normal direction of the light source and the normal direction. This is because it has a directivity to attenuate.

そのために、上記課題を解決する方法として、発光ダイオード素子の出光面に光学レンズを設置し、該光学レンズで発光ダイオード素子を出光する光を広げる方法が広く用いられている。例えば、特許文献2において、該光学レンズを設置する方法が開示されている。また、特許文献3において、光学レンズを設置する方法と照明器具の出光面にレンズ構造を有した透光部材を設置する方法を組み合わせた方法が開示されている。   Therefore, as a method for solving the above-described problem, a method in which an optical lens is installed on a light emitting surface of a light emitting diode element and the light emitted from the light emitting diode element is spread by the optical lens is widely used. For example, Patent Document 2 discloses a method of installing the optical lens. Further, Patent Document 3 discloses a method that combines a method of installing an optical lens and a method of installing a translucent member having a lens structure on a light exit surface of a lighting fixture.

確かに、これらの特許文献2及び特許文献3において開示されている方法により、照明器具を出光する光の配光角を広げる事ができる。しかし、これらの方法は、個々の光源に光学レンズを設置する必要があるのでコストが高くなるという課題を有している。   Certainly, the light distribution angle of the light emitted from the luminaire can be widened by the methods disclosed in Patent Document 2 and Patent Document 3. However, these methods have a problem that the cost increases because it is necessary to install an optical lens in each light source.

特開2010−218723号公報JP 2010-218723 A 特開2012−160666号公報JP 2012-160666 A 特開2016−58284号公報Japanese Patent Laid-Open No. 2006-58284

本発明の目的は、上記の問題点を解決するものであり、発光ダイオード素子を用いた照明器具の明るくなる範囲が狭いという欠点を低コストで改善できる照明器具用フィルム、照明器具用フィルム積層体及びこれらを組み込んだ照明器具を提供することにある。   SUMMARY OF THE INVENTION An object of the present invention is to solve the above-mentioned problems, and a lighting device film and a lighting device film laminate that can improve at low cost the disadvantage that the lightening range using a light emitting diode element is narrow. And it is providing the lighting fixture incorporating these.

本発明の第1の観点に係る照明器具用フィルムは、
異方性光拡散フィルムから構成され、照明器具の光源ユニットの出光面側に配置して用いられる照明器具用フィルムであって、
前記照明器具用フィルムは、前記照明器具用フィルムにほぼ垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に、該レーザーポインターの出光方向を傾け、フィルムに入光する光の角度がフィルム面に対して斜めになるように変化させた場合に、フィルムを出光する光の投影像が入光方向の延長方向のみでなく、延長方向と対角にも現れ、少なくとも2方向にスプリットして出光する機能を有する、
ことを特徴とする。
The film for lighting equipment according to the first aspect of the present invention is
It is composed of an anisotropic light diffusing film, and is a film for a lighting fixture that is used by being disposed on the light exit surface side of a light source unit of a lighting fixture,
The lighting device film has an angle of light incident on the film by tilting the light emitting direction of the laser pointer to the main diffusion direction of light that can be confirmed by irradiating the light of the laser pointer almost perpendicularly to the lighting device film. When the projection is changed so as to be inclined with respect to the film surface, the projected image of the light emitted from the film appears not only in the extension direction of the incident light direction but also in the diagonal direction with respect to the extension direction, and is split in at least two directions. And has the function of emitting light,
It is characterized by that.

また、前記照明器具用フィルムは、
変角色差計を用いて測定される、−45度の入射角度で入射されて−45度の透過角度で出光する光の相対光透過度が0.25以上であることが好ましい。
Moreover, the film for a lighting fixture is:
The relative light transmittance of light incident at an incident angle of −45 degrees and emitted at a transmission angle of −45 degrees, measured using a variable angle color difference meter, is preferably 0.25 or more.

また、前記照明器具用フィルムは、
変角色差計を用いた方法で測定される、−45度の入射角度で入射され、−45度の透過角度で出光する光の相対光透過度が、+45度の透過角度で出光する光の相対光透過度に対して0.7以上であることが好ましい。
Moreover, the film for a lighting fixture is:
The relative light transmittance of light incident at −45 degrees and emitted at a transmission angle of −45 degrees is measured by a method using a variable angle color difference meter, and the light emitted at a transmission angle of +45 degrees is The relative light transmittance is preferably 0.7 or more.

また、前記照明器具用フィルムは、
主構成成分と屈折率の異なる部分が前記照明器具用フィルムの厚み方向に延びた形で存在することが好ましい。
Moreover, the film for a lighting fixture is:
It is preferable that a portion having a refractive index different from that of the main constituent component exists in a form extending in the thickness direction of the film for lighting equipment.

また、前記異方性光拡散フィルムは、内部に前記異方性光拡散フィルムの厚み方向に延びたクレーズを有するクレーズフィルムであることが好ましい。   Moreover, it is preferable that the said anisotropic light-diffusion film is a craze film which has the craze extended in the thickness direction of the said anisotropic light-diffusion film inside.

本発明の第2の観点に係る照明器具用フィルム積層体は、
本発明の第1の観点に係る照明器具用フィルムと厚みが0.1〜10mmである透光性の支持体とが複合している、
ことを特徴とする。
The film laminate for lighting equipment according to the second aspect of the present invention,
The film for lighting equipment according to the first aspect of the present invention and a translucent support having a thickness of 0.1 to 10 mm are combined,
It is characterized by that.

また、前記照明器具用フィルム積層体は、変角色差計を用いて測定される、前記照明器具用フィルム積層体に垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に傾斜して−45度の入射角度で入射され、−45度の透過角度で出光する光の相対光透過度が0.25以上であることが好ましい。   The lighting device film laminate is inclined in a main diffusion direction of light, which is measured by applying a laser pointer light perpendicularly to the lighting device film laminate, which is measured using a goniochromimeter. The relative light transmittance of light incident at an incident angle of −45 degrees and exiting at a transmission angle of −45 degrees is preferably 0.25 or more.

また、前記照明器具用フィルム積層体は、変角色差計を用いて測定される、前記照明器具用フィルム積層体に垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に傾斜して−45度の入射角度で入射され、−45度の透過角度で出光する光の相対光透過度が、+45度の透過角度で出光する光の相対光透過度に対して0.7以上であることが好ましい。   The lighting device film laminate is inclined in a main diffusion direction of light, which is measured by applying a laser pointer light perpendicularly to the lighting device film laminate, which is measured using a goniochromimeter. The relative light transmittance of light incident at an incident angle of −45 degrees and emitted at a transmission angle of −45 degrees is 0.7 or more than the relative light transmittance of light emitted at a transmission angle of +45 degrees. Preferably there is.

本発明の第3の観点に係る照明器具は、
発光ダイオード素子の出光面側に本発明の第1の観点に係る照明器具用フィルム又は本発明の第2の観点に係る照明器具用フィルム積層体が設置された照明器具であって、
前記照明器具用フィルム又は前記照明器具用フィルム積層体の少なくともその一部の面が、発光ダイオード素子より出光する出射光の最大の出射光強度の方向に対して斜めになるように設置されてなる、
ことを特徴とする。
A lighting fixture according to a third aspect of the present invention is:
A lighting fixture in which the film for a lighting fixture according to the first aspect of the present invention or the film laminate for a lighting fixture according to the second aspect of the present invention is installed on the light-emitting surface side of the light-emitting diode element,
At least a part of the surface of the film for lighting fixture or the film stack for lighting fixture is installed so as to be inclined with respect to the direction of the maximum outgoing light intensity of outgoing light emitted from the light emitting diode element. ,
It is characterized by that.

本発明に係る照明器具用フィルムは、照明器具を出光する光の配光角を広げることができるので、発光ダイオード素子を用いた照明器具の課題である白熱電球や蛍光灯に比べて明るくなる範囲が狭くなるという欠点が改善できる。   Since the film for lighting fixtures according to the present invention can widen the light distribution angle of light emitted from the lighting fixtures, it is brighter than incandescent bulbs and fluorescent lamps, which are problems of lighting fixtures using light-emitting diode elements. The drawback of narrowing can be improved.

照明器具用フィルムや照明器具用フィルム積層体の光の拡散方向を確認する方法の概略図である。It is the schematic of the method of confirming the diffusion direction of the light of the film for lighting fixtures, or the film laminated body for lighting fixtures. 照明器具用フィルムや照明器具用フィルム積層体の光のスプリット効果を確認する方法の概略図である。It is the schematic of the method of confirming the split effect of the light of the film for lighting fixtures, or the film laminated body for lighting fixtures. 実施例における照明器具としての照度や輝度等の特性評価に用いた光源モジュールの写真である。It is the photograph of the light source module used for characteristic evaluation, such as illumination intensity and a brightness | luminance as a lighting fixture in an Example. 実施例における照明器具用フィルム積層体の性能評価の一例として用いた図3に示した光源モジュールに照明器具用フィルム積層体を傾斜して設置した照明器具モデル器具の写真である。It is the photograph of the lighting fixture model fixture which inclined and installed the lighting device film laminated body in the light source module shown in FIG. 3 used as an example of the performance evaluation of the lighting fixture film laminated body in an Example. 実施例における照明器具用フィルム積層体の性能評価の一例として用いた図3に示した光源モジュールに照明器具用フィルム積層体を湾曲形状に成型して設置した照明器具モデル器具の写真である。It is the photograph of the lighting fixture model instrument which shape | molded and installed the film stack for lighting fixtures in the curved shape in the light source module shown in FIG. 3 used as an example of the performance evaluation of the film laminate for lighting fixtures in an Example. 実施例における天井面及び壁面の輝度特性を評価するモデル評価方法の状況の写真である。It is a photograph of the situation of the model evaluation method which evaluates the brightness | luminance characteristic of the ceiling surface and wall surface in an Example. 実施例2と比較例2との床面照度の配光分布の比較を示したグラフである。It is the graph which showed the comparison of the light distribution of the floor surface illumination intensity of Example 2 and Comparative Example 2. FIG. 実施例1〜8及び比較例4〜7における−45度相対光線透過度と配光角70度の床面照度の関係を示したグラフである。It is the graph which showed the relationship between -45 degree relative light transmittance in Examples 1-8 and Comparative Examples 4-7, and the floor surface illumination intensity of the light distribution angle of 70 degree | times. 実施例1〜8及び比較例4〜7におけるスプリット効果と高配光化係数の関係を示したグラフである。It is the graph which showed the relationship between the split effect in Examples 1-8 and Comparative Examples 4-7, and a high light distribution coefficient. 実施例3及び比較例2における壁面モデルの輝度配光分布を示すグラフである。It is a graph which shows the luminance light distribution of the wall surface model in Example 3 and Comparative Example 2. 実施例1〜8及び比較例4〜7における−45度相対光線透過度と天井面と接する壁面位置である0m位置の壁面輝度の関係を示したグラフである。It is the graph which showed the relationship of -45 degree relative light transmittance in Examples 1-8 and Comparative Examples 4-7, and the wall surface brightness | luminance of 0 m position which is a wall surface position which touches a ceiling surface. 図12(A)及び(B)は、床面照度測定時の実施例3及び比較例2の場合の暗室の明るさの違いを示した写真である。FIGS. 12A and 12B are photographs showing the difference in the brightness of the dark room in Example 3 and Comparative Example 2 when measuring the floor illuminance.

(照明器具用フィルム)
本発明の照明器具用フィルムは、一方向に光が拡散する異方性光拡散フィルムから構成され、照明器具の光源ユニットの出光面側に配置されて用いられる。
上記照明器具用フィルムは、上記照明器具用フィルムにほぼ垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に、該レーザーポインターの出光方向を傾け、フィルムに入光する光の角度がフィルム面に対して斜めになるように変化させた場合に、フィルムを出光する光の投影像が該入光方向の延長方向のみでなく、該延長方向と対角側にも投影像が現れ、照明器具用フィルムから出稿する光が少なくとも2方向にスプリットする機能を有する事が重要である。
例えば、広く用いられている拡散フィルムや拡散板等の汎用の拡散部材の場合は、上記評価をしても、入光した角度の延長線方向のみに光が出光するのみでありスプリット効果は発現しない。
(Lighting film)
The film for lighting fixtures of this invention is comprised from the anisotropic light-diffusion film which light diffuses to one direction, and is arrange | positioned and used for the light-emitting surface side of the light source unit of a lighting fixture.
The lighting device film has an angle of light incident on the film by tilting the light emitting direction of the laser pointer to the main diffusion direction of light that can be confirmed by irradiating the light of the laser pointer almost perpendicularly to the film for the lighting device. When the projection is changed so as to be inclined with respect to the film surface, the projected image of the light emitted from the film appears not only in the extension direction of the light incident direction but also in the diagonal direction with respect to the extension direction. It is important to have a function of splitting light emitted from the film for lighting equipment in at least two directions.
For example, in the case of a general-purpose diffusion member such as a widely used diffusion film or diffusion plate, the light is emitted only in the extension line direction of the incident angle even if the above evaluation is performed, and the split effect is manifested. do not do.

(異方性及び拡散方向の確認方法)
照明器具用フィルムの要件である異方性の確認方法の概略図を図1に示す。白色系の壁面に照明器具用フィルムを壁とほぼ平行になるように垂直に配置して、照明器具用フィルムの壁面と反対面からレーザーポインターの光を照明器具用フィルムの面に対してほぼ垂直に照射する。照明器具用フィルムに入射された光が拡散、透過して、図1に示すように、壁面に光の投影像4が現れる。壁面に投影される光の投影像の長径方向の幅が短径方向の幅に対して1.2以上であれば異方性を有すると定義する。なお、本発明においては、上記方法で求めた投影像の長径方向を主拡散方向と定義する。
(Method for confirming anisotropy and diffusion direction)
FIG. 1 shows a schematic diagram of a method for confirming anisotropy, which is a requirement for a film for lighting equipment. Place the lighting fixture film vertically on the white wall so that it is almost parallel to the wall, and the laser pointer light from the opposite side of the lighting fixture film wall is almost perpendicular to the surface of the lighting fixture film. Irradiate. The light incident on the film for a lighting fixture is diffused and transmitted, and a projected image 4 of the light appears on the wall surface as shown in FIG. If the width in the major axis direction of the projected image of the light projected on the wall surface is 1.2 or more with respect to the width in the minor axis direction, it is defined as having anisotropy. In the present invention, the major axis direction of the projected image obtained by the above method is defined as the main diffusion direction.

(スプリット効果の確認方法)
照明器具用フィルムの要件であるスプリット性の確認方法の概略図を図2に示す。
上記図1を参照して説明した方法で確認された投影像の主拡散方向に、図2に示すようにレーザー光の入光角度を傾ける。例えば図2に示すように角度θで入光した場合にその延長線方向に出光する光の投影像4のみでなく、該延長方向と対角側に出光する光の投影像4’が現れる場合、スプリット性があると定義する。なお、2つの投影像である4及び4’の明るさの差は問わない。
光のスポット4’の明るさが高いほど、照明器具に照明器具用フィルムを組み込んだ場合に、照明器具から出光する光の配光角を広げる効果を大きくできる。
本発明においては、上記の2つの投影像のほかにも投影像が現れる、いわゆるマルチスプリット効果を発揮する照明器具用フィルムであってもよい。
(How to check the split effect)
FIG. 2 shows a schematic diagram of a method for confirming the split property, which is a requirement for a film for lighting equipment.
The incident angle of the laser beam is inclined as shown in FIG. 2 in the main diffusion direction of the projected image confirmed by the method described with reference to FIG. For example, as shown in FIG. 2, when light is incident at an angle θ, not only the projected image 4 of the light emitted in the extension direction but also the projected image 4 ′ of the light emitted diagonally to the extension direction appears. , Defined as split. Note that the difference in brightness between the four projected images 4 and 4 'does not matter.
The higher the brightness of the light spot 4 ', the greater the effect of widening the light distribution angle of the light emitted from the lighting fixture when the lighting fixture film is incorporated into the lighting fixture.
In the present invention, a film for a lighting fixture that exhibits a so-called multi-split effect in which a projected image appears in addition to the two projected images may be used.

(照明器具用フィルム及び照明器具用フィルム積層体のスプリット効果の定量化)
本発明の照明器具用フィルムは、変角色差計を用いた方法で測定される相対光透過度、具体的には、照明器具用フィルムの垂線方向に対して光の主拡散方向に傾斜して−45度の入射角度で光が入光したときに、−45度の透過角度に出光する光の相対光透過度(以下、これを−45度相対光透過度と記す)が0.25以上であることが好ましい。
−45度相対光透過度が0.25未満ではスプリット効果が不足し、高配光化の向上効果が小さくなる。また、−45度相対光透過度は0.6以上がより好ましい。理由は定かでないが、実施例において詳細する如く、−45度相対光透過度と高配光化効果の関係には極大値が存在する。従って、0.6以上で4未満が更に好ましい。
なお、上記の測定方法の詳細は実施例において詳細する。該測定方法で測定される相対光透過度は、後述の如く、標準拡散板を用いて校正された値である。したがって、広く使用されている変角光度計による測定値と異なり、準定量値であるという特徴を有する。このため、照明器具用フィルムを出光する光量に対応した値になる。一方、広く用いられている変角光度計の場合は、特定測定条件での相対値評価になるので、出光する光量が大きく変わる場合は、測定条件を変更して測定する必要があるので定量化はできない。
上記の−45度相対光透過度は、照明器具用フィルム及び照明器具用フィルム積層体の前記したスプリット効果の尺度になる。従って、該−45度相対光透過度は、出来る限り大きいことが好ましい。
(Quantification of split effect of film for lighting equipment and laminated film for lighting equipment)
The film for lighting fixtures of the present invention has a relative light transmittance measured by a method using a goniochromimeter, specifically, tilted in the main diffusion direction of light with respect to the normal direction of the lighting fixture film. When light is incident at an incident angle of −45 degrees, the relative light transmittance of light emitted at a transmission angle of −45 degrees (hereinafter referred to as “−45 degrees relative light transmittance”) is 0.25 or more. It is preferable that
When the -45 degree relative light transmittance is less than 0.25, the split effect is insufficient, and the effect of improving the light distribution is reduced. Further, the -45 degree relative light transmittance is more preferably 0.6 or more. The reason is not clear, but there is a maximum value in the relationship between the -45 degree relative light transmittance and the high light distribution effect as described in detail in the examples. Therefore, 0.6 or more and less than 4 is more preferable.
The details of the above measurement method will be described in detail in Examples. The relative light transmittance measured by this measuring method is a value calibrated using a standard diffusion plate as described later. Therefore, it has a feature that it is a quasi-quantitative value, unlike a measurement value by a widely used goniophotometer. For this reason, it becomes a value corresponding to the amount of light emitted from the film for lighting equipment. On the other hand, in the case of a widely used goniophotometer, the relative value is evaluated under specific measurement conditions, so if the amount of emitted light changes significantly, it is necessary to change the measurement conditions for quantification. I can't.
The above-mentioned -45 degree relative light transmittance is a measure of the above-mentioned split effect of the film for lighting fixtures and the film laminate for lighting fixtures. Therefore, the -45 degree relative light transmittance is preferably as large as possible.

また、照明器具用フィルムは、−45度の入射角度で光が入射された時に、−45度透過相対光透過度と+45度の透過角度に出光する光の相対光透過度(+45度相対光透過度)の比(−45度透過相対光透過度/+45度相対光透過度)が0.7以上であることが好ましく、0.8以上であることがより好ましい。
上記の比が0.7未満ではスプリット効果が低下して高配光化の効果が低下するためである。また、上記の比の上限は限定されないが、技術的困難さより1.5以下が好ましい。
上記の−45度相対光透過度と+45度相対光透過度の比は、上記の−45度相対光透過度の測定方法に準じて測定され、その測定方法の詳細は実施例において詳細する。
In addition, the film for lighting fixtures has a relative light transmittance of +45 degrees relative light (+45 degrees relative light) that is emitted at a transmission angle of −45 degrees and a transmission angle of +45 degrees when light is incident at an angle of −45 degrees. The ratio of (transmittance) (−45 degrees transmitted relative light transmittance / + 45 degrees relative light transmittance) is preferably 0.7 or more, and more preferably 0.8 or more.
This is because if the ratio is less than 0.7, the split effect is lowered and the effect of increasing the light distribution is lowered. Moreover, although the upper limit of said ratio is not limited, 1.5 or less is preferable from technical difficulty.
The ratio between the −45 degree relative light transmittance and the +45 degree relative light transmittance is measured in accordance with the measurement method of the −45 degree relative light transmittance, and details of the measurement method will be described in detail in Examples.

(スプリット効果を付与する方法)
照明器具用フィルムがスプリット効果を発揮する構造として、例えば、フィルムの構成成分と屈折率の異なる微細な部分がフィルムの厚み方向に延びた形で存在する形態が挙げられる。このような構成において、屈折率の異なる微細部分に入射角度θiが−x度で入光した光が到達したときに、微細構造を透過して進む透過角度θtがx度の透過光と、微細構造の界面で反射されて透過角度θtが−x度の出光する反射透過光に分割されることにより、スプリット効果が発現する。なお、照明器具用フィルムはスプリット効果を発揮し得る限り、上記の構成に限定されない。
(How to give a split effect)
As a structure in which the film for lighting equipment exhibits the split effect, for example, there is a form in which fine portions having different refractive indexes from the constituent components of the film are present in a form extending in the thickness direction of the film. In such a configuration, when light incident at an incident angle θi of −x degrees arrives at a fine portion having a different refractive index, the transmitted angle θt that travels through the microstructure is x degrees and the transmitted light is fine. By being divided into reflected and transmitted light that is reflected at the interface of the structure and emits light having a transmission angle θt of −x degrees, a split effect appears. In addition, as long as the film for lighting fixtures can exhibit the split effect, it is not limited to said structure.

(スプリット効果を有するフィルムの製造方法)
上記構造を形成する方法も限定されないが、フィルム内部にフィルムの厚み方向に延びた微細なクレーズが形成されているクレーズフィルムであることが好ましい。上記クレーズフィルムとしては、例えば、特開平07−241917号公報において開示されるものが挙げられる。
(Method for producing film having split effect)
The method for forming the structure is not limited, but is preferably a craze film in which a fine craze extending in the thickness direction of the film is formed inside the film. Examples of the crazing film include those disclosed in Japanese Patent Application Laid-Open No. 07-241917.

また、クレーズフィルムの製造方法の一例として、以下の方法が挙げられる。緊張状態に保持された透明性あるいは半透明性の高分子樹脂フィルム面に、先端部が鋭角の支持体を押し付けて、高分子樹脂フィルムをその分子配向方向と略平行に折り曲げ、そこに局部的な折り曲げ部を形成する。その後、高分子樹脂フィルムを支持体の先端部に接触させつつ、折り曲げ部における折り曲げ線に対して直交する方向に引っ張る。これにより、高分子樹脂フィルムの分子配向方向と略平行に連続的な縞状のクレーズ領域を形成することができる。   Moreover, the following method is mentioned as an example of the manufacturing method of a craze film. A support having an acute angle is pressed against a transparent or translucent polymer resin film surface held in a tension state, the polymer resin film is bent substantially parallel to the molecular orientation direction, and locally there. A bent portion is formed. Thereafter, the polymer resin film is pulled in a direction perpendicular to the folding line at the bent portion while contacting the tip of the support. Thereby, a continuous striped craze region can be formed substantially parallel to the molecular orientation direction of the polymer resin film.

ここでいうクレーズ領域とは、高分子樹脂フィルムの表面に現れる表面クレーズとその内部に発生する内部クレーズの両方を含むものであって、細かなひび状の模様を有する領域をいう。そしてこのクレーズは、分子束(フィブリル)とボイドから構成されており、全体としてスポンジの構造に似たものとなっている。   The craze area | region here contains both the surface craze which appears on the surface of a polymer resin film, and the internal craze generate | occur | produced in the inside, Comprising: The area | region which has a fine crack-like pattern is said. This craze is composed of molecular bundles (fibrils) and voids, and has a structure similar to that of a sponge as a whole.

(透明性あるいは半透明性高分子樹脂フィルムの種類)
上記のクレーズフィルムの製造に用いられる透明性あるいは半透明性の高分子樹脂フィルムの種類は、上記方法でクレーズが発現できるフィルムであれば限定されない。例えば、ポリオレフィン系樹脂、ポリエステル系樹脂、ポリスチレン系樹脂及びポリカーボネート系樹脂を用いたフィルムが挙げられる。これらの樹脂で、結晶性の低い樹脂を用いるのが好ましい。
(Types of transparent or translucent polymer resin film)
The kind of the transparent or translucent polymer resin film used in the production of the above craze film is not limited as long as the film can exhibit crazing by the above method. For example, a film using a polyolefin resin, a polyester resin, a polystyrene resin, and a polycarbonate resin can be given. Of these resins, a resin having low crystallinity is preferably used.

(クレーズフィルムの構造)
本発明のクレーズフィルムを製造するための透明性あるいは半透明性のフィルムは、単層構造でも多層構造であっても構わない。多層構造において、各層の厚み比や樹脂種の変更等で、照明器具用フィルムのスプリット効果特性等を制御することができるほか、その他の特性等の制御等の多様性を広げる意味で多層構造が好ましい。
(Craze film structure)
The transparent or translucent film for producing the craze film of the present invention may have a single layer structure or a multilayer structure. In the multilayer structure, it is possible to control the split effect characteristics etc. of the film for lighting equipment by changing the thickness ratio of each layer and the resin type, etc. In addition, the multilayer structure is intended to expand the variety of control of other characteristics etc. preferable.

(クレーズフィルムのスプリット効果の制御方法)
クレーズフィルムのスプリット効果の制御方法は限定されない。例えば、クレーズ形成工程において、張力や処理速度を変化させる事等によって制御しても良いし、クレーズ形成処理をするフィルムの樹脂種や、多層構造の層構成比等を変えることによって行ってもよい。特に、後者の方法が有効であるので、好ましい実施態様である。
(Control method of split effect of craze film)
The method for controlling the split effect of the craze film is not limited. For example, in the craze formation step, it may be controlled by changing the tension or the processing speed, or may be performed by changing the resin type of the film to be craze-formed, the layer constitution ratio of the multilayer structure, or the like. . In particular, since the latter method is effective, it is a preferred embodiment.

(照明器具用フィルムの厚み)
照明器具用フィルムの厚みは限定されない。上記クレーズフィルムで展開をする場合は、クレーズを形成するクレーズ加工の加工性等より0.03〜0.5mm程度で有ることが好ましい。
(Thickness of film for lighting equipment)
The thickness of the film for lighting equipment is not limited. When unfolding with the above crazed film, it is preferably about 0.03 to 0.5 mm in view of the workability of the crazing process for forming the craze.

(照明器具用フィルム積層体)
続いて、照明器具用フィルム積層体について説明する。照明器具用フィルム積層体は、上述した照明器具用フィルムと透光性の支持体が積層された構造をしている。上述した照明器具用フィルムは、フィルムを構成する樹脂の種類等により柔らく自己支持性が劣る場合がある。柔らかい照明器具用フィルムを照明器具に組み込む場合、自己支持性が劣ることから、照明器具用フィルムの形状を保持するのに、照明器具用フィルムを緊張状態で固定する等の固定方法の工夫が必要になる。それ故、本発明においては、照明器具用フィルムを透光性の支持体に積層した照明器具用フィルム積層体を用いるのが好ましい。
支持体の厚みは0.3〜10mmであることが好ましい。厚みが0.3mm未満では照明器具用フィルムの自己保持性が低下するため、逆に、支持体の厚みが10mmを越すとコストが高くなるためである。
(Film laminate for lighting equipment)
Then, the film laminated body for lighting fixtures is demonstrated. The film laminate for a lighting fixture has a structure in which the above-described film for a lighting fixture and a translucent support are laminated. The above-mentioned film for lighting equipment may be soft and inferior in self-support depending on the type of resin constituting the film. When a soft lighting fixture film is incorporated into a lighting fixture, self-supporting is inferior. Therefore, in order to maintain the shape of the lighting fixture film, it is necessary to devise a fixing method such as fixing the lighting fixture film in a tensioned state. become. Therefore, in this invention, it is preferable to use the film laminated body for lighting fixtures which laminated | stacked the film for lighting fixtures on the translucent support body.
The thickness of the support is preferably 0.3 to 10 mm. This is because, if the thickness is less than 0.3 mm, the self-holding property of the film for lighting equipment is lowered, and conversely, if the thickness of the support exceeds 10 mm, the cost increases.

(支持体の特性)
支持体は、透光性であればその特性は限定されない。例えば、全光線透過率が60%以上である透明板や拡散板を用いる事ができる。
(Characteristics of support)
The characteristics of the support are not limited as long as it is translucent. For example, a transparent plate or a diffusion plate having a total light transmittance of 60% or more can be used.

(支持体の材質)
上記支持体の材質は、上記特性を有しておれば、適宜選択できる。例えば、プラスチックス、ガラス及びセラミックス等が挙げられる。
(Support material)
The material of the support can be appropriately selected as long as it has the above characteristics. For example, plastics, glass, ceramics, etc. are mentioned.

(照明器具用フィルム用積層体の製造方法)
照明器具用フィルム積層体の製造方法は限定されない。例えば、上記した照明器具用フィルムと支持体とを透光性の粘着剤や接着剤で貼着して製造する方法が上げられる。
(Manufacturing method of film laminate for lighting equipment)
The manufacturing method of the film laminated body for lighting fixtures is not limited. For example, there can be mentioned a method for producing a film for lighting equipment and a support by sticking them with a translucent adhesive or adhesive.

(照明器具)
本発明の照明器具は、発光ダイオード素子の出光面側に前記の照明器具用フィルムあるいは照明器具用フィルム積層体が設置された照明器具である。照明器具は、上記照明器具用フィルムあるいは照明器具用フィルム積層体の少なくともその一部の面が、発光ダイオード素子より出光する出射光の最大の出射光強度の方向に対して斜めになるように設置されている(以下、単に斜め入光設置法と称する事もある)。
発光ダイオード素子の出光面側に拡散部材等の透光性の光学部材を設置して、発光ダイオード素子による直視した時のグレア性を改善したり、あるいは明るくなる範囲を広げる等の機能を付与する事は広く実施されている。
一方、本発明の照明器具に用いられる照明器具用フィルムまたは照明器具用フィルム積層体は、本発明の効果である高配光化効果を発現するために必要なスプリット効果は、前記したごとく、斜め入光設置法が必須である。該斜め入光設置法も汎用の拡散部材を用いた方法は広く実施されている。従って、本発明は、照明器具用フィルムまたは照明器具用フィルム積層体を用い、かつ斜め入光設置法と組み合わせる事が新規技術になる。
(lighting equipment)
The lighting fixture of this invention is a lighting fixture in which the said film for lighting fixtures or the film laminated body for lighting fixtures was installed in the light emission surface side of the light emitting diode element. The luminaire is installed such that at least a part of the surface of the luminaire film or the luminaire film laminate is inclined with respect to the direction of the maximum outgoing light intensity of the outgoing light emitted from the light emitting diode element. (Hereinafter, it may be simply referred to as an oblique incident light installation method).
A light-transmitting optical member such as a diffusing member is installed on the light-emitting surface side of the light-emitting diode element to provide functions such as improving the glare when directly viewed by the light-emitting diode element or expanding the brightening range. Things are widely implemented.
On the other hand, as described above, the lighting effect film or the lighting device film laminate used in the lighting device of the present invention has the split effect necessary to exhibit the high light distribution effect, which is the effect of the present invention, as described above. The light installation method is essential. As the oblique incident light installation method, a method using a general-purpose diffusing member is widely practiced. Therefore, the present invention is a novel technique that uses a film for lighting fixtures or a film laminate for lighting fixtures and is combined with an oblique light incident installation method.

(照明器具の構成)
本発明の照明器具は上記要件を満たせば限定されないが、少なくとも発光ダイオード素子よりなる光源ユニット及び該光源ユニットを収納する筐体から構成される光源モジュールと、光源ユニットの出光面側に設置された照明器具用フィルムあるいは照明器具用フィルム積層体から構成される配光角制御部材(以下、単に配光角制御部材と称する事もある)を最小構成部材とすることが好ましい。
(Structure of lighting equipment)
The lighting fixture of the present invention is not limited as long as it satisfies the above requirements, and is installed on the light-emitting surface side of the light source module including at least a light source unit composed of a light-emitting diode element and a housing for housing the light source unit. It is preferable that a light distribution angle control member (hereinafter, also simply referred to as a light distribution angle control member) composed of a film for lighting fixtures or a film laminate for lighting fixtures be a minimum constituent member.

(光源ユニット)
本発明においては、光源ユニットの構成や構造も限定されないが、例えば、少なくとも基板の表面に実装された単数又は複数の発光ダイオード素子を有する実装基板を用いる事ができる。該実装基板の発光ダイオード素子の設置面の反対面に放熱部材を積層する事や、放熱フィンを組み込む等により、放熱対策を施す等の態様も排除されない。
(Light source unit)
In the present invention, the configuration and structure of the light source unit are not limited. For example, a mounting substrate having at least one light emitting diode element mounted on the surface of the substrate can be used. It is not excluded that a heat dissipation measure is taken by laminating a heat dissipating member on the surface of the mounting substrate opposite to the light emitting diode element installation surface or by incorporating a heat dissipating fin.

(光源モジュール)
本発明における光源モジュールの構成や構造も限定されないが、例えば、照明器具用の筐体の底面あるいは底面付近に上記光源ユニットを組み込んだ構造を挙げる事ができる。
更に、該光源モジュールの実装基板の出光面や筐体の内面に反射塗料で塗装したり、あるいは、反射部材を組み込む等により、筐体の内面の光の反射度を向上させる事が好ましい実施態様である。該実施態様により、照明器具から出光する照度を増加させる事ができ、直下照度の向上に繋げる事ができる。
(Light source module)
The configuration and structure of the light source module in the present invention are not limited, and examples thereof include a structure in which the light source unit is incorporated in the bottom surface or the vicinity of the bottom surface of a housing for a lighting fixture.
Furthermore, it is preferable to improve the light reflectivity of the inner surface of the casing by coating the light exit surface of the mounting substrate of the light source module or the inner surface of the casing with a reflective paint or incorporating a reflecting member. It is. According to this embodiment, the illuminance emitted from the lighting fixture can be increased, and the illuminance directly below can be improved.

(発光ダイオード素子)
本実施の形態における上記の発光ダイオード素子は、LED光源やレーザ光源等の点状の発光素子よりなる発光ダイオード素子が挙げられる。該発光ダイオード素子の種類は限定されないが、広く普及が進んでいるLED光源が好ましい。
LED光源の種類も限定されない。例えば、広く使用されている砲弾型LED、表面実装型(SMD)及びチップオンボード(COB)等が挙げられる。特に、表面実装型(SMD)及びチップオンボード(COB)の使用が好ましい。
(Light-emitting diode element)
Examples of the light emitting diode element in the present embodiment include a light emitting diode element made of a point light emitting element such as an LED light source or a laser light source. The type of the light-emitting diode element is not limited, but an LED light source that is widely spread is preferable.
The kind of LED light source is not limited. For example, a bullet type LED, a surface mount type (SMD), a chip on board (COB) and the like that are widely used can be cited. In particular, the use of surface mount type (SMD) and chip on board (COB) is preferable.

(発光ダイオード素子の設置場所及び個数)
上記の実施の形態においては、上記発光ダイオード素子は、光源ユニットの実装基板の出光面に単数又は複数個が設置されてなることが好ましい。特に、発光ダイオード素子が複数個設置されたタイプが好ましい。複数個のLEDを設置する場合の個数や配列状態は限定されない。
(Installation location and number of light emitting diode elements)
In said embodiment, it is preferable that the said light emitting diode element is installed in the light emission surface of the mounting substrate of a light source unit by one or more. In particular, a type in which a plurality of light emitting diode elements are installed is preferable. The number and arrangement state in the case of installing a plurality of LEDs are not limited.

(斜め入光設置法)
本発明における斜め入光設置法の形態は、上記配光角制御部材の少なくともその一部の面が、発光ダイオード素子より出光する出射光の最大の出射光強度の方向に対して斜めになるように設置されておれば限定されない。
該形態は、発光ダイオード素子より出光する出射光の最大の出射光強度の方向(以下、単に出光方向と称する事もある)が、発光ダイオード素子の出光面から垂直方向に出光する発光ダイオード素子の出光方向に対し、斜めになるように配光角制御部材が設置された形態、逆に、配光角制御部材を水平に設置して、配光角制御部材に対して発光ダイオード素子の出光面が斜めになるように上記発光ダイオード素子が設置された形態、及び、発光ダイオード素子の出光面に光源用のレンズ部材を設置して、発光ダイオード素子の出光方向が斜めになるような発光ダイオード素子を用いて、発光ダイオード素子の出光面及び照明器具用フィルムあるいは配光角制御部材が平行に設置された形態の3形態に大別される。本発明においては、いずれの形態でも良い。また、これらの形態を組み合わせた形態で実施しても良い。
(Diagonal light installation method)
In the aspect of the oblique light incident installation method according to the present invention, at least a part of the surface of the light distribution angle control member is inclined with respect to the direction of the maximum emitted light intensity of the emitted light emitted from the light emitting diode element. If it is installed in, it will not be limited.
In this embodiment, the direction of the maximum outgoing light intensity of the outgoing light emitted from the light emitting diode element (hereinafter sometimes simply referred to as the outgoing direction) is emitted from the light emitting diode element in the vertical direction. A configuration in which the light distribution angle control member is installed so as to be inclined with respect to the light emission direction, conversely, the light distribution angle control member is installed horizontally, and the light emission surface of the light emitting diode element with respect to the light distribution angle control member The light emitting diode element in which the light emitting diode element is installed so that the light emitting diode element is inclined, and the light emitting lens element is installed on the light emitting surface of the light emitting diode element so that the light emitting direction of the light emitting diode element is inclined Are roughly divided into three forms, in which the light-emitting surface of the light-emitting diode element and the film for lighting equipment or the light distribution angle control member are installed in parallel. Any form may be used in the present invention. Moreover, you may implement with the form which combined these forms.

上記の第一の形態の場合は、配光角制御部材が湾曲化した形態でも良い。該湾曲化して設置する方法は、通常の拡散板を用いた光学部材の設置方法として、直管型照明器具や一体型ベースライトで広く採用されている。該製品の拡散板を本発明の配光角制御部材に変更する事によっても本発明の効果を発現する事ができるので、好ましい実施態様の一つである。
本発明の実施例においては、2種の形態のみの結果を示しているが、上記要件を満たせば斜め入光設置法の形態はこれらに限定されない。
In the case of the first form, the light distribution angle control member may be curved. The curved installation method is widely used in straight tube lighting fixtures and integrated base lights as a method for installing an optical member using a normal diffusion plate. Since the effect of the present invention can be expressed also by changing the diffusion plate of the product to the light distribution angle control member of the present invention, it is one of the preferred embodiments.
In the embodiment of the present invention, the results of only two forms are shown, but the form of the oblique light incident installation method is not limited to these as long as the above requirements are satisfied.

(照明器具の形状)
本発明の配光角制御部材は、異方拡散性を有しており、かつ主配光方向にスプリット効果が発現する。従って、照明器具の形状も異方形状である事が好ましい。例えば、長方形や楕円形が好ましい。スプリット効果が出る方向は限定されず、照明器具の短径方向であっても長径方向であってもよいが、斜め入光設置法にて、入光角度を大きくできることから、短径方向にスプリット効果が出るような方向で設置するのが好ましい。
(Lighting fixture shape)
The light distribution angle control member of the present invention has anisotropic diffusibility and exhibits a split effect in the main light distribution direction. Therefore, it is preferable that the shape of the lighting fixture is also anisotropic. For example, a rectangle or an ellipse is preferable. The direction in which the split effect is produced is not limited, and it may be the minor axis direction or the major axis direction of the lighting fixture. However, since the incident angle can be increased by the oblique incident light installation method, the split is performed in the minor axis direction. It is preferable to install it in such a direction as to produce an effect.

(光源ユニットと配光角制御部材との位置関係)
本発明における光源ユニットと配光角制御部材との位置関係は、光源ユニットの出光面側に配光角制御部材が位置すれば、例えば、光源ユニットと配光角制御部材との間隔は限定されない。該両者の間隔は、最接近位置で2mmから最遠距離部分で200mmが好ましい。該間隔を大きくする事で、照度の低下をした形で照明器具を直視した場合のグレア性を大幅に改善する事ができるので、出来るだけ離した方が好ましいが、間隔を広げると照明器具の厚みが厚くなるので、200mm以下が好ましく、100mm以下がより好ましい。
配光角制御部材は、光源モジュールの筐体の出光面に設置されても良いし、筐体の内部に設置されても良い。高配光化効果の向上効果や照明器具を直視した時の眩しさ、即ち、グレア性を低減する効果が大きくなるので出光面に配置されていることが好ましい。
(Positional relationship between light source unit and light distribution angle control member)
The positional relationship between the light source unit and the light distribution angle control member in the present invention is not limited, for example, if the light distribution angle control member is positioned on the light exit surface side of the light source unit. . The distance between the two is preferably 2 mm at the closest position to 200 mm at the farthest distance portion. Increasing the distance can greatly improve the glare when the illuminator is viewed directly in the form of reduced illuminance, so it is preferable to keep it as far apart as possible. Since thickness becomes thick, 200 mm or less is preferable and 100 mm or less is more preferable.
The light distribution angle control member may be installed on the light exit surface of the casing of the light source module, or may be installed inside the casing. Since the effect of improving the high light distribution effect and the glare when the lighting apparatus is directly viewed, that is, the effect of reducing the glare, is increased, it is preferably disposed on the light exit surface.

(照明器具の明るさの特性)
照明器具の特性としては、床面の配光角70度における照度、天井面の照明器具より0.02m離れた位置の輝度及び壁面の天井面位置である0m位置の輝度が、それぞれ光源モジュールの出光面に光学部材が配置されていない場合の特性値(光源モジュールのみの特性値)に対し、表1に示す倍率以上の明るさを示す事が好ましい。
(Brightness characteristics of lighting equipment)
As the characteristics of the lighting fixture, the illuminance at a light distribution angle of 70 degrees on the floor surface, the luminance at a position 0.02 m away from the lighting fixture on the ceiling surface, and the luminance at the 0 m position, which is the ceiling surface position of the wall surface, respectively. It is preferable to show a brightness higher than the magnification shown in Table 1 with respect to the characteristic value (characteristic value of only the light source module) when no optical member is arranged on the light exit surface.

以下、本発明の実施例について説明するが、本発明はこれらの実施例に何ら限定されるものではない。各実施例、比較例で得られた試料についての物性測定方法は以下の通りである。   Examples of the present invention will be described below, but the present invention is not limited to these examples. The physical property measurement methods for the samples obtained in each Example and Comparative Example are as follows.

(評価方法)
(1)異方性及び拡散方向の確認方法
上述した手法に基づいて異方性及び拡散方向を確認した。
(Evaluation method)
(1) Confirmation method of anisotropy and diffusion direction The anisotropy and diffusion direction were confirmed based on the method mentioned above.

(2)スプリット効果の確認方法
上述した手法に基づいてスプリット効果を確認した。
(2) Confirmation method of split effect The split effect was confirmed based on the method mentioned above.

(3)スプリット効果の定量方法
変角分光測色システムGCMS−4型(株式会社村上色彩技術研究所製、変角分光光度計GPS−2型)を用いて透過光強度の測定を行った。
まず、上記GCMS−4型用の透過光拡散標準板(オパールガラス)を用いて装置の校正を行い、該透過光拡散標準板の受光角度0度における透過光強度Tを基準(1.000)とした。なお、上記透過拡散標準板は、積分球式分光計測で空気層を1.000とした時の波長550nmの透過率が0.3535であった。
次に、透過測定のrモード(試料に対して所定の入射角で光を入光した時の透過光強度の角度依存性を測定)で測定した。測定条件は以下とした。
光線入射角:―45度、受光角度:−80度から80度までを5度ピッチ(フィルム法線からの極角方位角は水平)、光源:D65、視野:2度の条件で、試料(照明器具用フィルムあるいは照明器具用フィルム積層体)の主光拡散方向が水平方向になるように試料台に固定(試料台の軸と主光拡散方向の軸とのずれは20度程度までは許容される。主拡散方向は、上記方法で判定した。)し、各受光角度における透過光強度を測定した。あおり角は0度とした。照明器具用フィルム積層体の場合は、照明器具に組み込んだ場合の入光面と同じ側より光を入光して測定した。本実施例においては、照明器具用フィルム側より入光する方法で評価した。
上記方法で、測定される−45度相対光線透過度及び+45度相対光線透過度を求めた。−45度相対光線透過度及び+45度の相対光線透過度は、共に、波長550nmの値で表示した。波長550nmの値で表示したのは、波長550nmの値が視感強度との相関性が高いとされているためである。
スプリット効果は、−45度相対光線透過度/+45度相対光線透過度の値で表示した。該値が大きい程スプリット効果が大きい。
(3) Quantitative method of split effect The transmitted light intensity was measured using a variable angle spectrophotometric system GCMS-4 type (manufactured by Murakami Color Research Laboratory Co., Ltd., variable angle spectrophotometer GPS-2 type).
First, the GCMS-4 type transmitted light diffusion standard plate (opal glass) is calibrated, and the transmitted light intensity T of the transmitted light diffusion standard plate at a light receiving angle of 0 degree is used as a reference (1.000). It was. The transmission diffusion standard plate had a transmittance of 0.3535 at a wavelength of 550 nm when the air layer was set to 1.000 by integrating sphere spectroscopic measurement.
Next, the measurement was performed in the r mode of transmission measurement (measurement of the angle dependency of transmitted light intensity when light was incident on the sample at a predetermined incident angle). The measurement conditions were as follows.
Light incident angle: -45 degrees, light receiving angle: -80 degrees to 80 degrees, 5 degree pitch (polar angle azimuth from film normal is horizontal), light source: D65, field of view: 2 degrees Fixed to the sample stage so that the main light diffusing direction of the lighting fixture film or lighting fixture film laminate is horizontal (the deviation between the axis of the sample stand and the axis of the main light diffusing direction is allowed up to about 20 degrees) The main diffusion direction was determined by the above method), and the transmitted light intensity at each light receiving angle was measured. The tilt angle was 0 degree. In the case of the film laminated body for lighting fixtures, it measured by entering light from the same side as the light-incidence surface at the time of incorporating in a lighting fixture. In the present Example, it evaluated by the method of entering light from the film side for lighting fixtures.
The -45 degree relative light transmittance and +45 degree relative light transmittance measured by the above method were determined. Both the −45 degree relative light transmittance and the +45 degree relative light transmittance are indicated by values at a wavelength of 550 nm. The reason why the wavelength 550 nm is displayed is that the value of the wavelength 550 nm is highly correlated with the luminous intensity.
The split effect was expressed as a value of −45 degrees relative light transmittance / + 45 degrees relative light transmittance. The larger the value, the greater the split effect.

(4)照明器具の特性評価
(4−1)光源モジュール
コイズミ照明(株)LEDライン照明(AL37225L)の出光面に組み込まれている拡散板を取り外して用いた。該光源モジュールの写真を図3に示す。
(4) Characteristic evaluation of lighting fixture (4-1) Light source module Koizumi Lighting Co., Ltd. LED line illumination (AL37225L) The diffuser plate incorporated in the light emission surface was removed and used. A photograph of the light source module is shown in FIG.

(4−2)配光角制御部材の性能評価用モデル照明器具
(4−2−1)傾斜設置法
図4の写真で示したように、上記光源モジュールの出光面に配光角制御部材を光源モジュールの短径方向の中心位置より両側に45度の傾斜角で設置して評価をした。配光角制御部材は2枚の平板を透明テープで繋ぎ合わせて写真のように、断面が正三角形になるように、光源モジュールの出光面に透明テープで固定して評価した。配光角制御部材は、各種支持体の片面に照明器具用フィルムを水で貼着して評価した。該貼着の光源モジュールへの設置は、照明器具用フィルムが入光面側になるように設置した。また、照明器具用フィルムは、主拡散方向が短手方向になるように貼着した。
本評価においては、配光角制御部材は照明器具用フィルムのサンプル長が190mmであったので、光源モジュールの中心部より±95mmを開口部として、両端を黒色の遮光紙で遮光し、該開口部に上記配光角制御部材を設置して評価した。
(4-2) Model lighting fixture for performance evaluation of light distribution angle control member (4-2-1) Inclined installation method As shown in the photograph of FIG. 4, a light distribution angle control member is provided on the light output surface of the light source module. Evaluation was performed by installing the light source module at an inclination angle of 45 degrees on both sides from the center position in the minor axis direction. The light distribution angle control member was evaluated by fixing two flat plates with a transparent tape and fixing them with a transparent tape on the light emitting surface of the light source module so that the cross section becomes a regular triangle as shown in the photograph. The light distribution angle control member was evaluated by sticking a film for a lighting fixture with water on one side of various supports. The attachment to the light source module was performed so that the film for lighting equipment was on the light incident surface side. Moreover, the film for lighting fixtures was stuck so that the main spreading | diffusion direction might become a transversal direction.
In this evaluation, since the sample length of the light distribution film was 190 mm, the light distribution angle control member was shielded with black shading paper at both ends with ± 95 mm as the opening from the center of the light source module. The light distribution angle control member was installed in the part and evaluated.

(4−2−2)湾曲設置法
上記の傾斜設置法に準じて、図5の写真に示したように配光角制御部材を出光側が凸状に湾曲した形状の成型体に変更する以外は、傾斜設置法と同様にして評価した。なお、配光角制御部材の頭頂上面と光源モジュールの出光面との距離は45mmとした。照明器具用フィルムは、傾斜設置法と同様に内面側に水で貼着して評価した。
(4-2-2) Curved Installation Method According to the above-described inclined installation method, except that the light distribution angle control member is changed to a molded body having a curved shape on the light output side as shown in the photograph of FIG. The evaluation was performed in the same manner as the inclined installation method. The distance between the top surface of the light distribution angle control member and the light exit surface of the light source module was 45 mm. The film for lighting fixtures was evaluated by sticking to the inner surface side with water in the same manner as the inclined installation method.

(4−3)床面照度測定
変角照度計((有)ハイランド社製「ZERO−ONE」)を用いて、照明装置を駆動方式の試料台上に、光源モジュールの中心点と試料台の中心点が一致するように設置し、照明装置出光面と照度計受光面との距離:1000mm、変角範囲:−90度から+90度までを5度ピッチの条件で、光源モジュールの短径方向の照度の配光分布を測定した。
照度の測定は暗室下で行い、照明装置を点灯後30分経過後より測定を開始した。評価結果は70度照度及び0度の照度で表示した。70度照度は−70度の照度と+70度の照度の平均値で表示した。70度照度が高い程、高配光化効果が大きい。
また、70度照度と0度照度の比(70度照度/0度照度)を求めて、高配光化係数とした。
70度照度が高く、かつ高配光化係数が高い程、高配光化効果が大きい。
(4-3) Floor surface illuminance measurement Using a variable angle illuminometer ("ZERO-ONE" manufactured by Highland), the illuminator is placed on the drive-type sample table, the center point of the light source module and the sample table The center point of the light source module is set so that the distance between the light emitting surface and the light receiving surface of the illuminating device is 1000 mm, and the angle-of-change range is -90 degrees to +90 degrees with a 5 degree pitch condition. The light distribution of illuminance in the direction was measured.
The illuminance was measured in a dark room, and the measurement was started 30 minutes after the lighting device was turned on. The evaluation results were displayed at 70 degrees illuminance and 0 degrees illuminance. The 70 degree illuminance was displayed as an average value of −70 degree illuminance and +70 degree illuminance. The higher the illuminance at 70 degrees, the greater the light distribution effect.
Further, the ratio of the 70 ° illuminance to the 0 ° illuminance (70 ° illuminance / 0 ° illuminance) was determined and used as a high light distribution coefficient.
The higher the 70 degree illuminance and the higher the light distribution coefficient, the greater the light distribution effect.

(4−4)天井面輝度及び壁面輝度
天井面の照度は測定できない。そこで、輝度で評価した。該評価では壁面の輝度も合わせて測定できる方法で評価した。図6の写真で示したモデル評価方法で評価した。
即ち、暗室の出入り口にテーブル机を垂直に立てて、該暗室の床面及び垂直に立てたテーブル机面にエプソン(株)のPXマット紙(拡散反射度の高い白色反射紙)をボードに貼り付け白色反射ボードを設置して、床面の白色反射ボードの暗室の奥側の端部に光源モジュールを、光源モジュールの長径方向が壁面と平行で、かつ出光面が暗室の天井面になるように設置して、該光源モジュールを点灯し、床面及び床面の垂直の白色反射ボード面の輝度を(有)ハイランド社製の二次元輝度計(ACE−100)を用いて、床面及び垂直面の白色反射ボード面全面の輝度を測定し、該白色反射ボードの中心部の輝度をライン解析した計測値で解析をした。壁面のモデル面は机の端面よりさらに上部位置の明るさが大きく変化するケースがある事が判ったので、白色反射ボードを暗室の天井面までに延長をして評価した。
暗室の床面の白色反射ボードが天井面の、該床面の白色反射ボードに対して垂直に設置された白色反射ボードが壁面の明るさに対応している。天井面の光源より壁面までの距離は2mとした。壁面モデルの高さは4.24mであった。
天井面モデル面の輝度は、光源モジュールより0.02m、1m及び2m離れた位置の値で表示した。当然であるが2m位置は壁面モデル面との接点の位置である。
壁面モデル面の輝度は天井面位置より0m、1m、2m及び4mの位置の値で表示した。
(4-4) Ceiling surface luminance and wall surface luminance The illuminance on the ceiling surface cannot be measured. Therefore, the brightness was evaluated. In this evaluation, evaluation was performed by a method that can also measure the luminance of the wall surface. Evaluation was performed by the model evaluation method shown in the photograph of FIG.
In other words, a table desk is set up vertically at the entrance and exit of the dark room, and Epson PX matte paper (white reflective paper with high diffuse reflectance) is pasted on the board on the floor surface of the dark room and the table desk set up vertically. Install a white reflective board, place the light source module at the end of the dark room of the white reflective board on the floor, make the major axis direction of the light source module parallel to the wall surface, and the light exit surface to the ceiling surface of the dark room The light source module is turned on, and the luminance of the floor surface and the white reflective board surface perpendicular to the floor surface is measured using a two-dimensional luminance meter (ACE-100) manufactured by Highland Corporation. And the brightness | luminance of the white reflective board surface whole surface of a perpendicular | vertical surface was measured, and it analyzed by the measured value which carried out the line analysis of the brightness | luminance of the center part of this white reflective board. The model surface of the wall surface was found to have a case where the brightness at the upper position greatly changed from the end surface of the desk. Therefore, the white reflection board was extended to the ceiling surface of the dark room and evaluated.
The white reflective board on the floor surface of the dark room is on the ceiling surface, and the white reflective board installed perpendicular to the white reflective board on the floor surface corresponds to the brightness of the wall surface. The distance from the light source on the ceiling surface to the wall surface was 2 m. The height of the wall model was 4.24 m.
The brightness of the ceiling model surface was displayed as values at positions 0.02 m, 1 m, and 2 m away from the light source module. Naturally, the 2m position is the position of the contact point with the wall surface model surface.
The brightness of the wall model surface was displayed as values of 0 m, 1 m, 2 m, and 4 m from the ceiling surface position.

(照明器具用フィルムAの製造方法)
(5)フィルムの製膜
3台の溶融押し出し機を用い、第1の押し出し機にて、ホモポリプロピレン樹脂(日本ポリプロ株式会社製 MA3U メルトフローレート:15(230℃))100重量部を表面層となるように押し出し、第2の押し出し機にて、ホモポリプロピレン樹脂(日本ポリプロ株式会社製 MA3U メルトフローレート:15(230℃))20重量部とエチレンとブテンが共重合された共重合ポリプロピレン樹脂(住友化学株式会社製 WF345S メルトフローレート:10(230℃))80重量部を中間層となるように押し出し、さらに第3の押し出し機にて、エチレンが共重合された共重合ポリプロピレン樹脂(日本ポリプロ株式会社製 WINTEC WFX4 メルトフローレート:10(230℃))100重量部を第1の押し出し機より押し出した層とは反対面となる表層になるように溶融押し出しをして、Tダイの中で3種3層構成となる様に積層後、第1の押し出し機より押し出した層が、冷却ロールに接触巻き取る様にして、総厚み40μmのフィルムを得た。層厚み構成は第1の押し出し機より押し出した層側から、12/25/3(μm)であった。
(Manufacturing method of film A for lighting equipment)
(5) Film formation Using three melt extruders, in the first extruder, 100 parts by weight of a homopolypropylene resin (MA3U melt flow rate: 15 (230 ° C.) manufactured by Nippon Polypro Co., Ltd.) is a surface layer. In a second extruder, a copolymer polypropylene resin obtained by copolymerizing 20 parts by weight of homopolypropylene resin (MA3U melt flow rate: 15 (230 ° C.) manufactured by Nippon Polypro Co., Ltd.) with ethylene and butene. (Sumitomo Chemical Co., Ltd. WF345S Melt flow rate: 10 (230 ° C.)) Extruded 80 parts by weight to be an intermediate layer, and further copolymerized polypropylene resin obtained by copolymerizing ethylene with a third extruder (Japan) Polytech Co., Ltd. WINTEC WFX4 Melt flow rate: 10 (230 ° C)) 100 weight The first extruder after melt-extruding so that the surface becomes the surface layer opposite to the layer extruded from the first extruder and laminating to form a three-layer three-layer structure in the T-die A film having a total thickness of 40 μm was obtained in such a manner that the further extruded layer was wound around the cooling roll. The layer thickness constitution was 12/25/3 (μm) from the layer side extruded from the first extruder.

(6)クレーズの形成
上記の様にして得られたフィルムに、第1の押し出し機より押し出した層側からクレーズ加工を以下の様にして実施した。スプリングとネジにより上下動して高分子樹脂フィルムの張力を調整する補助具と、先端部が鋭角の支持体とを備えたクレージング装置を使用する。まず、緊張状態に保持した上記フィルム面に、支持体の先端部を押し付けてこれを折り曲げると共に、この高分子樹脂フィルムに補助具により一定の張力を与え、そして高分子樹脂フィルムを支持体に接触させつつ引っ張る。これにより、高分子樹脂フィルムの分子配向方向と略平行に連続的なクレーズ領域を有する照明器具用フィルムAを得た。
得られた照明器具用フィルムAの−45度の相対光線透過度、+45度相対光線透過度及びスプリット効果(−45度相対光線透過度/+45度相対光線透過度)はそれぞれ、7.80、7.22及び1.08であった。
(6) Formation of craze The film obtained as described above was subjected to craze processing from the layer side extruded from the first extruder as follows. A crazing device including an auxiliary tool that moves up and down by a spring and a screw to adjust the tension of the polymer resin film and a support having an acute-angle tip is used. First, the tip of the support is pressed against the film surface held in tension and bent, and a constant tension is applied to the polymer resin film by an auxiliary tool, and the polymer resin film is brought into contact with the support. Pull while letting. Thereby, the film A for lighting fixtures which has a continuous craze area | region substantially parallel to the molecular orientation direction of a polymer resin film was obtained.
-45 degree relative light transmittance, +45 degree relative light transmittance and split effect (-45 degree relative light transmittance / + 45 degree relative light transmittance) of the obtained film A for lighting equipment were 7.80, It was 7.22 and 1.08.

(支持体)
実施例及び比較例において用いた支持体の種類及び特性を表2に示す。
(Support)
Table 2 shows the types and characteristics of the supports used in the examples and comparative examples.

なお、照明器具に設置されていたアクリル系拡散板の相対光線透過度及び配光角は、それぞれ0.8及び130度で支持体Eと同じ特性であった。   In addition, the relative light transmittance and light distribution angle of the acrylic diffusion plate installed in the lighting fixture were 0.8 and 130 degrees, respectively, which were the same characteristics as the support E.

(実施例1〜実施例8)
図3に示した光源モジュールに照明器具用フィルム積層体を傾斜して設置した照明器具モデル器具(図4)を用いて、照明器具用フィルムAと各種支持体との積層体について、床面照度の結果を表3に示す。
底面照度特性としては、高配光化効果の尺度である配光角70度の照度、直下照度に相当する0度照度、照度の均一性の尺度である高配光化係数及び高配光化効果の度合いである光源モジュール及び該光源モジュールを用いた照明器具仕様である該照明器具に組み込まれていたアクリル系拡散板を組み込んだ場合のそれぞれの照度を基準とした相対値である70度照度比も記載した。
照明器具用フィルム積層体は、照明器具用フィルムと支持体を水で貼着して、照明器具用フィルムが入光面側になるように光源モジュールに組み込んで評価した。
配光角70度の床面照度及び高配光化係数が大幅に向上し、床面の明るくなる範囲が広くなる。また、床面の明るさの均質性が向上する。光源モジュールの照度に対して10倍を超す明るさが出る場合がある。
ただし、直下照度が、光源モジュールのみ(比較例1)や該光源モジュールを用いた製品(比較例2)に比べると低下する。しかし、後述の如くこれらの実施例においては、天井面や壁面の明るさが該比較例1や比較例2に比べると大幅に向上する。人の目線は、天井面や壁面に向くので、天井面や壁面が明るいと床面の明るさが半分になっても同じ明るさ感を感じると言われているので、直下照度が低くなる事は許容される。むしろ部屋全体の明るさが明るくなる方が優位である。
(Example 1 to Example 8)
Using the lighting fixture model fixture (FIG. 4) in which the lighting fixture film laminate is installed on the light source module shown in FIG. Table 3 shows the results.
As the bottom surface illuminance characteristics, the illuminance with a light distribution angle of 70 degrees, which is a measure of the high light distribution effect, the 0 degree illuminance corresponding to the illuminance directly below, the high light distribution coefficient which is a measure of illuminance uniformity, and the degree of the high light distribution effect 70 degree illuminance ratio, which is a relative value based on each illuminance when the acrylic diffusion plate incorporated in the illuminator that is a specification of the illuminator using the light source module and the illuminator specification using the light source module is also described did.
The lighting device film laminate was evaluated by incorporating the lighting device film and the support with water and incorporating the lighting device film into the light source module so that the lighting device film was on the light incident surface side.
The floor surface illuminance and the high light distribution coefficient at a light distribution angle of 70 degrees are greatly improved, and the range in which the floor surface is brightened is widened. Moreover, the uniformity of the brightness of the floor surface is improved. There may be a brightness exceeding 10 times the illuminance of the light source module.
However, the illuminance immediately below is lower than that of the light source module alone (Comparative Example 1) or a product using the light source module (Comparative Example 2). However, as will be described later, in these examples, the brightness of the ceiling surface and the wall surface is significantly improved as compared with Comparative Example 1 and Comparative Example 2. Since human eyes are directed to the ceiling and walls, it is said that if the ceiling and walls are bright, the same brightness will be felt even if the brightness of the floor is halved. Is acceptable. Rather, it is more advantageous that the brightness of the whole room becomes brighter.

(比較例1及び比較例2)
光源モジュールのみ場合及び該光源モジュールの出光面にアクリル系拡散板が組み込まれた本光源モジュールを用いた照明器具の床面の照度結果を表3に示す。直下照度(0度照度)は実施例1〜8より高いが配光角70度照度が低く床面の明るさの広がりが狭くなる。
(Comparative Example 1 and Comparative Example 2)
Table 3 shows the results of illuminance on the floor surface of a lighting fixture using the light source module in which only the light source module is used and the light source module in which an acrylic diffusion plate is incorporated on the light exit surface of the light source module. The illuminance directly below (0 degree illuminance) is higher than those in Examples 1 to 8, but the illuminance is 70 degrees and the brightness spread on the floor surface is narrow.

(実施例3と比較例2との床面照度の配光分布の比較)
実施例2と比較例2との床面照度の配光分布の比較を図7に示す。比較例2はほぼランバーシアン配光分布であるのに対して、実施例2は−90度から90度までほぼ均一な明るさになり、本発明の効果が顕著である事が判る。
(Comparison of light distribution of floor illuminance between Example 3 and Comparative Example 2)
FIG. 7 shows a comparison of light distribution of floor illuminance between Example 2 and Comparative Example 2. While Comparative Example 2 has a substantially Lambertian light distribution, Example 2 has a substantially uniform brightness from -90 degrees to 90 degrees, indicating that the effect of the present invention is remarkable.

(比較例3)
上記照明器具用フィルムと支持体Cとの積層体を光源モジュールの出光面に水平に設置した場合の結果を表3に示す。実施例3で発現した高配光化の効果が出ない。配光角制御部材に対して斜めに入光する光の量が低くなると前述したスプリット効果が出ない事を示している。
(Comparative Example 3)
Table 3 shows the results when the laminate of the lighting fixture film and the support C is horizontally installed on the light exit surface of the light source module. The effect of increasing the light distribution expressed in Example 3 is not achieved. It shows that the above-described split effect does not occur when the amount of light incident obliquely with respect to the light distribution angle control member decreases.

(比較例4〜比較例7)
支持体のみを傾斜して設置した照明器具モデル器具の結果を表3に示す。配光角70度の照度や高配光化効果が小さい。本発明の効果を出すには照明器具用フィルムの積層が必須である事を示している。
(Comparative Example 4 to Comparative Example 7)
Table 3 shows the results of the luminaire model apparatus in which only the support is inclined. Illuminance with a light distribution angle of 70 degrees and high light distribution effect are small. In order to obtain the effect of the present invention, it is shown that lamination of a film for a lighting fixture is essential.

(−45度相対光線透過度と配光角70度の床面照度との関係)
実施例1〜8及び比較例4〜7における−45度相対光線透過度と配光角70度の床面照度の関係を図8に示す。実施例においてのみ本発明の効果である高配光化の効果が発現し、本発明の効果が臨界的である事が示されている。また、前記したより好ましい範囲を満たすことで、高配光化効果がより高くなる事を示している。なお、上記関係において極大値がでる事の原因は定かでない。
(Relationship between -45 degree relative light transmittance and floor surface illumination with light distribution angle of 70 degree)
FIG. 8 shows the relationship between the −45 degree relative light transmittance and the floor illuminance at a light distribution angle of 70 degrees in Examples 1 to 8 and Comparative Examples 4 to 7. Only in the examples, the effect of increasing the light distribution, which is the effect of the present invention, is expressed, and it is shown that the effect of the present invention is critical. Moreover, it has shown that the high light distribution effect becomes higher by satisfy | filling the more preferable range mentioned above. Note that the cause of the maximum value in the above relationship is not clear.

(スプリット効果と高配光化係数との関係)
実施例1〜8及び比較例4〜7におけるスプリット効果と高配光化係数の関係を図9に示す。該図9においても、実施例においてのみ本発明の効果である高配光化の効果が発現し、本発明の効果が臨界的である事が示されている。
また、本発明の効果が配光角制御部材のスプリット効果により引き起こされている事を示している。
(Relationship between split effect and high light distribution coefficient)
FIG. 9 shows the relationship between the split effect and the high light distribution coefficient in Examples 1 to 8 and Comparative Examples 4 to 7. FIG. 9 also shows that the effect of increasing the light distribution, which is the effect of the present invention, is manifested only in the embodiment, and the effect of the present invention is critical.
It also shows that the effect of the present invention is caused by the split effect of the light distribution angle control member.

(天井面輝度)
実施例1〜実施例8及び比較例1〜比較例7における天井面モデルの輝度評価結果を表4に示す。
(Ceiling brightness)
Table 4 shows the luminance evaluation results of the ceiling surface models in Examples 1 to 8 and Comparative Examples 1 to 7.

輝度特性としては、照明器具用近辺の明るさ(照明器具用との距離:0.02m)、照明器具との距離:2m、即ち、壁面位置の明るさで表示した。また、0.2m位置の輝度に対する2mの輝度の維持率の結果を示した。
床面照度と同様に、実施例の結果は比較例1〜比較例3とは顕著な差はあるが、傾斜設置法における照明器具用フィルム積層をしていない比較例4〜比較例7との差異は小さい結果になった。即ち、天井面輝度に関しては、光学部材に斜めに光が入光する効果の寄与が大きく、照明器具用フィルムのスプリット効果の寄与は小さいと言える。
ただし、明るさの距離による減衰率に相当する輝度の維持率は照明器具用フィルム積層により向上する。該維持率が高い事は天井面の明るさの距離による影響が小さい事であるので照明器具用フィルム積層は好ましい効果を発現していると言える。
As the luminance characteristics, the brightness in the vicinity of the lighting fixture (distance to the lighting fixture: 0.02 m) and the distance to the lighting fixture: 2 m, that is, the brightness of the wall surface position are displayed. Moreover, the result of the maintenance factor of the brightness | luminance of 2 m with respect to the brightness | luminance of a 0.2-m position was shown.
Similar to the floor illuminance, the results of the examples are significantly different from those of Comparative Examples 1 to 3, but with Comparative Examples 4 to 7 in which the film for lighting equipment is not laminated in the inclined installation method. The difference was small. That is, regarding the ceiling surface luminance, it can be said that the contribution of the effect that light enters the optical member obliquely is large, and the contribution of the split effect of the film for lighting equipment is small.
However, the maintenance rate of the luminance corresponding to the attenuation rate due to the distance of the brightness is improved by the lamination of the lighting fixture film. Since the high maintenance factor means that the influence of the brightness of the ceiling surface is small, it can be said that the film lamination for lighting fixtures exhibits a favorable effect.

(壁面の輝度分布)
前記した方法にて測定した壁面モデルの輝度配光分布の代表例として、実施例3及び比較例2の評価結果を図10に示す。図10の縦軸は壁面モデルの輝度、即ち、壁面の明るさの度合いを示している。一方、横軸は天井面モデルよりの距離を示している。
壁面輝度の配光分布は、実施例3と比較例2とで大きく異なる。比較例2は、天井面より約2.5m離れた位置の明るさが最も明るくなり、天井面と接する0m位置の明るさは暗い。これに対して実施例2の場合は、天井面近辺が最も明るく天井面からの距離が大きくなるに従い漸次明るさが低下する理想的な明るさ分布になり、本発明の効果が顕著である事を示している。
(Wall brightness distribution)
FIG. 10 shows the evaluation results of Example 3 and Comparative Example 2 as a representative example of the luminance distribution of the wall surface model measured by the method described above. The vertical axis in FIG. 10 indicates the brightness of the wall surface model, that is, the degree of brightness of the wall surface. On the other hand, the horizontal axis indicates the distance from the ceiling model.
The light distribution of the wall luminance is greatly different between Example 3 and Comparative Example 2. In Comparative Example 2, the brightness at a position about 2.5 m away from the ceiling surface is the brightest, and the brightness at the 0 m position in contact with the ceiling surface is dark. On the other hand, in the case of Example 2, the ideal brightness distribution in which the brightness near the ceiling surface is brightest and the brightness gradually decreases as the distance from the ceiling surface increases, and the effect of the present invention is remarkable. Is shown.

(壁面の輝度特性)
実施例1〜実施例8及び比較例1〜比較例7における壁面モデルの輝度評価結果を表5に示す。
輝度特性としては、天井面からの距離0m、1m、2m及び4mの輝度を記載した。これらの輝度値は、図10にその代表例を示した壁面モデルの輝度の配光分布の測定結果より求めた。
また、0m位置の光源モジュールの輝度である比較例1に対する相対値を記載した。該相対値は、本発明の効果の度合いの尺度になる。この値が大きい方が本発明の効果である高配光化の効果が大きいと言える。
床面照度と同様に、この天井面近辺の明るさが比較例1の12倍以上になり、本発明の効果が極めて顕著である事が判る。
(Brightness characteristics of wall surface)
Table 5 shows the luminance evaluation results of the wall surface models in Examples 1 to 8 and Comparative Examples 1 to 7.
As the luminance characteristics, the luminances at distances of 0 m, 1 m, 2 m, and 4 m from the ceiling surface are described. These luminance values were obtained from the measurement result of the luminance distribution of the wall model whose typical example is shown in FIG.
Moreover, the relative value with respect to the comparative example 1 which is the brightness | luminance of the light source module of 0 m position was described. The relative value is a measure of the degree of the effect of the present invention. It can be said that the larger this value is, the greater the light distribution effect, which is the effect of the present invention.
Similar to the floor surface illuminance, the brightness in the vicinity of the ceiling surface is 12 times or more that of Comparative Example 1, and it can be seen that the effect of the present invention is extremely remarkable.

輝度特性としては、天井面からの距離0m、1m、2m及び4mの輝度を記載した。また、0m位置の光源モジュールの輝度である比較例1に対する相対値を記載した。該相対値は、本発明の効果の度合いの尺度になる。
光源モジュールや光学部材を出光面に水平に設置した場合は、天井面より約2.5m離れた位置の明るさが最も明るくなり、天井面と接する0m位置の明るさは暗い。これに対して実施例の場合は、天井面近辺が最も明るく天井面からの距離が大きくなるに従い漸次明るさが低下する理想的な明るさ分布になる。しかも、床面照度と同様に、この天井面近辺の明るさが光源モジュールの10倍以上になる場合もあり、本発明の効果が極めて顕著である事が判る。
As the luminance characteristics, the luminances at distances of 0 m, 1 m, 2 m, and 4 m from the ceiling surface are described. Moreover, the relative value with respect to the comparative example 1 which is the brightness | luminance of the light source module of 0 m position was described. The relative value is a measure of the degree of the effect of the present invention.
When the light source module or the optical member is installed horizontally on the light exit surface, the brightness at the position about 2.5 m away from the ceiling surface is the brightest, and the brightness at the 0 m position in contact with the ceiling surface is dark. On the other hand, in the case of the embodiment, an ideal brightness distribution in which the vicinity of the ceiling surface is brightest and the brightness gradually decreases as the distance from the ceiling surface increases. In addition, as in the case of the floor surface illuminance, the brightness in the vicinity of the ceiling surface may be 10 times or more that of the light source module, and it can be seen that the effect of the present invention is extremely remarkable.

(−45度相対光線透過度と壁面輝度との関係)
実施例1〜8及び比較例4〜7における−45度相対光線透過度と天井面と接する壁面位置である0m位置の壁面輝度の関係を図11に示す。
実施例においてのみ本発明の効果である高配光化の効果が発現し、本発明の効果が臨界的である事が示されている。
また、前記したより好ましい範囲を満たすことで、高配光化効果がより高くなる事を示している。
なお、上記関連において極大値がでる事の原因は定かでない。
(Relationship between -45 degree relative light transmittance and wall brightness)
FIG. 11 shows the relationship between the −45 degree relative light transmittance and the wall surface luminance at the 0 m position that is the wall surface position in contact with the ceiling surface in Examples 1 to 8 and Comparative Examples 4 to 7.
Only in the examples, the effect of increasing the light distribution, which is the effect of the present invention, is expressed, and it is shown that the effect of the present invention is critical.
Moreover, it has shown that the high light distribution effect becomes higher by satisfy | filling the more preferable range mentioned above.
In addition, the cause of the maximum value in the above relation is not clear.

(暗室の明るさ)
床面照度測定時の実施例3及び比較例2の場合の暗室の明るさの違いを示した写真を図12(A)、(B)に示す。
照明器具は各写真の左側下部に出光面が上側になるように設置されている。従って、暗室の天井面が床面に相当する。
実施例1の場合は暗室全体がほぼ均一な明るさになるのに対して、比較例2の場合は床面が明るくなっているのみであり、本発明の効果が極めて大きい事が明らかである。
(Dark room brightness)
FIGS. 12A and 12B show photographs showing the difference in brightness of the dark room in the case of Example 3 and Comparative Example 2 when measuring the floor illuminance.
The luminaire is installed in the lower left part of each photo so that the light exit surface is on the upper side. Therefore, the ceiling surface of the dark room corresponds to the floor surface.
In the case of Example 1, the entire dark room has almost uniform brightness, whereas in the case of Comparative Example 2, only the floor surface is bright, and it is clear that the effect of the present invention is extremely large. .

(実施例9及び実施例10)
図3に示した光源モジュールに照明器具用フィルム積層体を図5の写真に示した如く出光面側が凸になるように湾曲化した形で設置して評価した結果を表6に示す。照明器具用フィルム積層体の内面に照明器具用フィルムAを水で貼着して評価した。
実施例2及び実施例3に比べると高配光化効果は少し低くなるが本発明の効果が発現できるが判る。
(Example 9 and Example 10)
Table 6 shows the results of evaluation by installing the film laminate for a lighting fixture on the light source module shown in FIG. 3 in a curved shape so that the light exit surface side is convex as shown in the photograph of FIG. The film A for lighting fixtures was stuck with water on the inner surface of the film laminate for lighting fixtures and evaluated.
Compared to Example 2 and Example 3, the effect of the present invention can be realized although the effect of increasing the light distribution is slightly lower.

(照明器具用フィルムB及び照明器具用フィルムC)
環状ポリオレフィン系樹脂及び共重合ポリエステル樹脂を用いて、照明器具用フィルムAの製造方法に準じてそれぞれ照明器具用フィルムB及び照明器具用フィルムCを製造した。得られた照明器具用フィルムの特性を表7に示す。
(Lighting device film B and Lighting device film C)
Using a cyclic polyolefin resin and a copolymerized polyester resin, a lighting device film B and a lighting device film C were manufactured according to the manufacturing method of the lighting device film A, respectively. Table 7 shows the characteristics of the obtained film for lighting equipment.

(実施例11及び実施例12)
それぞれ照明器具用フィルムBあるいは照明器具用フィルムCと支持体Cとの積層体を用いて、実施例3と同様の方法で床面照度、天井面モデル輝度及び壁面モデル輝度を評価した。どちらも実施例3と同等の高配光化効果が得られた。
(Example 11 and Example 12)
The floor surface illuminance, the ceiling surface model luminance, and the wall surface model luminance were evaluated in the same manner as in Example 3 using the lighting device film B or a laminate of the lighting device film C and the support C, respectively. In both cases, an effect of increasing light distribution equivalent to that in Example 3 was obtained.

本発明の照明器具用フィルムあるいは照明器具用フィルム積層体は、該照明器具用フィルムあるいは照明器具用フィルム積層体に対して光を斜めに入光した場合に、該入光した角度の延長線方向に出光するのみでなく、該延長線方向とほぼ対角方向にも入光した光がスプリットされた形で出光するという特異特性を有するので、発光ダイオード素子を用いた照明器具の出光面側に該照明器具用フィルムあるいは照明器具用フィルム積層体を上記のスプリット効果が発現できるような形で組み込む事により、照明器具を出光する光の配光角を従来公知の光拡散部材部材を用いた場合よりも著しく広げる事ができるので、発光ダイオード素子を用いた照明器具の課題である白熱電球や蛍光灯に比べて明るくなる範囲が狭くなるという欠点が改善できる。従って、住宅用、施設用及び屋外用等の幅広い用途の照明器具として広く好適に用いる事ができる。   The lighting device film or the lighting device film laminate of the present invention has a direction of an extended line of the incident angle when light is obliquely incident on the lighting device film or the lighting device film laminate. In addition to the light emitted from the light source, it has a unique characteristic that light incident in a direction substantially diagonal to the extension line direction is emitted in a split form, so that it is on the light exit surface side of a lighting fixture using a light emitting diode element. When a conventionally known light diffusing member is used for the light distribution angle of light emitted from the lighting fixture by incorporating the lighting fixture film or the lighting fixture film laminate in such a form that the above-mentioned split effect can be exhibited. As a result, the lightening range is narrower compared to incandescent bulbs and fluorescent lamps, which is a problem with lighting equipment using light-emitting diode elements. That. Therefore, it can be used widely and suitably as a lighting device for a wide range of uses such as residential use, facility use and outdoor use.

Claims (9)

異方性光拡散フィルムから構成され、照明器具の光源ユニットの出光面側に配置して用いられる照明器具用フィルムであって、
前記照明器具用フィルムは、前記照明器具用フィルムにほぼ垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に、該レーザーポインターの出光方向を傾け、フィルムに入光する光の角度がフィルム面に対して斜めになるように変化させた場合に、フィルムを出光する光の投影像が入光方向の延長方向のみでなく、延長方向と対角にも現れ、少なくとも2方向にスプリットして出光する機能を有する、
ことを特徴とする照明器具用フィルム。
It is composed of an anisotropic light diffusing film, and is a film for a lighting fixture that is used by being disposed on the light exit surface side of a light source unit of a lighting fixture,
The lighting device film has an angle of light incident on the film by tilting the light emitting direction of the laser pointer to the main diffusion direction of light that can be confirmed by irradiating the light of the laser pointer almost perpendicularly to the lighting device film. When the projection is changed so as to be inclined with respect to the film surface, the projected image of the light emitted from the film appears not only in the extension direction of the incident light direction but also in the diagonal direction with respect to the extension direction, and is split in at least two directions. And has the function of emitting light,
A film for lighting equipment characterized by the above.
前記照明器具用フィルムは、
変角色差計を用いて測定される、−45度の入射角度で入射されて−45度の透過角度で出光する光の相対光透過度が0.25以上である、
ことを特徴とする請求項1に記載の照明器具用フィルム。
The film for lighting equipment is:
The relative light transmittance of light incident at an incident angle of −45 degrees and emitted at a transmission angle of −45 degrees, measured using a variable angle color difference meter, is 0.25 or more.
The film for lighting equipment according to claim 1.
前記照明器具用フィルムは、
変角色差計を用いた方法で測定される、−45度の入射角度で入射され、−45度の透過角度で出光する光の相対光透過度が、+45度の透過角度で出光する光の相対光透過度に対して0.7以上である、
ことを特徴とする請求項1又は2に記載の照明器具用フィルム。
The film for lighting equipment is:
The relative light transmittance of light incident at −45 degrees and emitted at a transmission angle of −45 degrees is measured by a method using a variable angle color difference meter, and the light emitted at a transmission angle of +45 degrees is 0.7 or more relative light transmittance,
The film for lighting equipment according to claim 1 or 2, wherein
前記照明器具用フィルムは、
主構成成分と屈折率の異なる部分が前記照明器具用フィルムの厚み方向に延びた形で存在する、
ことを特徴とする請求項1〜3のいずれか一項に記載の照明器具用フィルム。
The film for lighting equipment is:
A portion having a refractive index different from that of the main constituent component exists in a form extending in the thickness direction of the film for lighting equipment,
The film for lighting fixtures as described in any one of Claims 1-3 characterized by the above-mentioned.
前記異方性光拡散フィルムは、内部に前記異方性光拡散フィルムの厚み方向に延びたクレーズを有するクレーズフィルムである、
ことを特徴とする請求項4に記載の照明器具用フィルム。
The anisotropic light diffusion film is a craze film having a craze extending in the thickness direction of the anisotropic light diffusion film inside.
The film for lighting equipment according to claim 4, wherein
請求項1〜5のいずれか一項に記載の照明器具用フィルムと厚みが0.1〜10mmである透光性の支持体とが複合している、
ことを特徴とする照明器具用フィルム積層体。
The film for lighting equipment according to any one of claims 1 to 5 and a translucent support having a thickness of 0.1 to 10 mm are combined.
The film laminated body for lighting fixtures characterized by the above-mentioned.
変角色差計を用いて測定される、前記照明器具用フィルム積層体に垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に傾斜して−45度の入射角度で入射され、−45度の透過角度で出光する光の相対光透過度が0.25以上である、
ことを特徴とする請求項6に記載の照明器具用フィルム積層体。
Inclined in the main diffusion direction of light that can be confirmed by applying light from a laser pointer perpendicularly to the film laminate for lighting equipment, measured using a variable angle color difference meter, and incident at an incident angle of −45 degrees, The relative light transmittance of light emitted at a transmission angle of −45 degrees is 0.25 or more,
The film laminated body for lighting fixtures of Claim 6 characterized by the above-mentioned.
変角色差計を用いて測定される、前記照明器具用フィルム積層体に垂直にレーザーポインターの光を当てる事により確認できる光の主拡散方向に傾斜して−45度の入射角度で入射され、−45度の透過角度で出光する光の相対光透過度が、+45度の透過角度で出光する光の相対光透過度に対して0.7以上である、
ことを特徴とする請求項6又は7に記載の照明器具用フィルム積層体。
Inclined in the main diffusion direction of light that can be confirmed by applying light from a laser pointer perpendicularly to the film laminate for lighting equipment, measured using a variable angle color difference meter, and incident at an incident angle of −45 degrees, The relative light transmittance of light emitted at a transmission angle of −45 degrees is 0.7 or more relative to the relative light transmittance of light emitted at a transmission angle of +45 degrees.
The film laminated body for lighting fixtures of Claim 6 or 7 characterized by the above-mentioned.
発光ダイオード素子の出光面側に請求項1〜5のいずれか一項に記載の照明器具用フィルム又は請求項6〜8のいずれか一項に記載の照明器具用フィルム積層体が設置された照明器具であって、
前記照明器具用フィルム又は前記照明器具用フィルム積層体の少なくともその一部の面が、発光ダイオード素子より出光する出射光の最大の出射光強度の方向に対して斜めになるように設置されてなる、
ことを特徴とする照明器具。
The lighting device film according to any one of claims 1 to 5 or the lighting device film laminate according to any one of claims 6 to 8 installed on a light-emitting surface side of the light emitting diode element. An instrument,
At least a part of the surface of the film for lighting fixture or the film stack for lighting fixture is installed so as to be inclined with respect to the direction of the maximum outgoing light intensity of outgoing light emitted from the light emitting diode element. ,
A lighting apparatus characterized by that.
JP2017070328A 2017-03-31 2017-03-31 Film for lighting apparatus, film laminate for lighting apparatus, and lighting apparatus Pending JP2018174050A (en)

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