JPS61273503A - Luminous radiation body - Google Patents

Luminous radiation body

Info

Publication number
JPS61273503A
JPS61273503A JP60116147A JP11614785A JPS61273503A JP S61273503 A JPS61273503 A JP S61273503A JP 60116147 A JP60116147 A JP 60116147A JP 11614785 A JP11614785 A JP 11614785A JP S61273503 A JPS61273503 A JP S61273503A
Authority
JP
Japan
Prior art keywords
refractive index
core
light
substance
cladding layer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP60116147A
Other languages
Japanese (ja)
Inventor
Hideaki Ito
英昭 伊藤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Rayon Co Ltd
Original Assignee
Mitsubishi Rayon Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Rayon Co Ltd filed Critical Mitsubishi Rayon Co Ltd
Priority to JP60116147A priority Critical patent/JPS61273503A/en
Publication of JPS61273503A publication Critical patent/JPS61273503A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To inexpensively produce the titled body having the excellent visual property of an outgoing light by constituting at least a part of the clad layer with a material having a higher refractive index than that of the core material. CONSTITUTION:The titled body consists of a core 1 made of a transparent high polymer substance, a substance layer 2 having a lower refractive index than that of the core 1, and a substance layer 3 having a higher refractive index than that of the core 1. When the light propagated from the titled body having the clad material composed of the substance having the lower refractive index than that of the core material 1 is reached a part having a large refractive index of the clad layer, as the propagated light is radiated from the prescribed part, the titled body having the clad alternately constituted from the material 2 having the low refractive index and the material 3 having the high refractive index as shown in the figure has the excellent visual property of the outgoing light. The transparent high polymer constituting the core 1 is polymethylmethacrylate. The material 2 having the low refractive index of the clad layer is 2,2,2 trifluoroethylmethacrylate, and the material 3 having the high refractive index is polycarbonate. The titled body is produced from the prescribed materials by a melt-spinning method.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、照明、装飾、ディスプレーなど伝送光を視覚
的に利用するための光放射体の構造(:関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to the structure of a light emitter for visually utilizing transmitted light such as illumination, decoration, and display.

〔従来の技術〕[Conventional technology]

従来、光ファイバーを照明、装飾、ディスプレーなどに
利用する場合、光源から、光ファイバーで伝送された光
を光ファイバーの他端から出射させるかあるいは光ファ
イバーのクラッド層の一部を除去して光フアイバー側面
から伝送光を漏光させる方法が採用されており、特に透
明高分子物質をコア材料とする光ファイバーは大口径の
ものが安価C:得られ、また低屈折率物質からなるクラ
ッド層も薄いものが簡単(二得られるため、この分野に
は広く用いられている。
Conventionally, when using optical fibers for lighting, decoration, displays, etc., the light transmitted by the optical fiber is emitted from the other end of the optical fiber, or a part of the cladding layer of the optical fiber is removed and the light is transmitted from the side of the optical fiber. A method of leaking light is adopted, and in particular optical fibers with large diameters made of transparent polymeric materials are inexpensive, and thin cladding layers made of low refractive index materials are easy to obtain. Therefore, it is widely used in this field.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

この様な光ファイバーの利用において、光ファイバーの
端面からの出射光は、光ファイバーの開口数監=より決
まる出射光強度分布の角度特性をもっており、広い範囲
からの視認性にも劣り、また照明光として利用する場合
には、スポット状の照明になるなどの欠点を有している
When using such an optical fiber, the light emitted from the end face of the optical fiber has an angular characteristic of the output light intensity distribution determined by the numerical aperture of the optical fiber, and its visibility from a wide range is poor, and it is difficult to use it as illumination light. In this case, there are drawbacks such as spot-like illumination.

一方、クラッド層の一部を除去した光ファイバーは、ク
ラッド層を除去するための手数を要するほか、クラッド
層の除去作業中、コア層にもキズなつけ、そのため光の
利用効率が劣る欠点を有している。
On the other hand, optical fibers with a portion of the cladding layer removed require a lot of effort to remove the cladding layer, and the core layer is also scratched during the cladding layer removal process, resulting in poor light utilization efficiency. are doing.

本発明は、照明、装飾、ディスプレーなど視覚用に供さ
れるこの様な元ファイバーの欠点を解消しようとするも
のであり、安価にして簡単に、優れた出射光の視覚特性
を有する光伝送体を提供せんとするものである。
The present invention aims to eliminate the drawbacks of such original fibers used for visual purposes such as illumination, decoration, and displays, and provides an inexpensive and simple optical transmission body with excellent visual characteristics of emitted light. We aim to provide the following.

〔問題点を解決するための手段〕[Means for solving problems]

光ファイバーなどの光伝送体は、透明なコア材料(A)
を用い、コアより低屈折率の物質で被覆したクラッド層
(B)(二より構成されるが、本発明は、この様な光伝
送体においてクラッド層の一部をコアよ1]高屈折率の
物質(C)で置きかえることにより、置きかえた部分か
ら光を放射させるようになしたものである。
Optical transmission bodies such as optical fibers are made of transparent core material (A)
The cladding layer (B) is coated with a material having a lower refractive index than the core. By replacing the material with substance (C), light is emitted from the replaced part.

ここで用いられるコア材料(A)は、ポリメチルメタア
クリレートなどの透明高分子物質であり、低屈折率のク
ラッド材料は上記コア材料ポリマーの部分弗素化合物や
シリコン樹脂などを用いる。また、高屈折率のクラッド
材料は、ポリスチレンやポリカーボネート樹脂、ポリエ
ステル樹脂のようなポリマーが用いられる。
The core material (A) used here is a transparent polymeric substance such as polymethyl methacrylate, and the low refractive index cladding material is a partially fluorinated compound of the core material polymer, silicone resin, or the like. Further, as the cladding material having a high refractive index, a polymer such as polystyrene, polycarbonate resin, or polyester resin is used.

本発明の詳細を図面に基き実施例で説明する。The details of the present invention will be explained by examples based on the drawings.

図面は、本発明による光放射体の一つの実施例を示すも
のであり、光放射体の構造のすべてを示すものではない
The drawings show one embodiment of the light emitter according to the present invention, and do not show the entire structure of the light emitter.

第1図、第2図は本発明による光放射体の斜視図の例で
あり、第3図、第4図は本発明:二よる別の例の断面図
である。図中(1)は透明高分子物質からなるコア、(
2)はコアより低屈折率の物質、(3)はコアより高屈
折率の物質からなる層を示す。
1 and 2 are perspective views of a light emitter according to the present invention, and FIGS. 3 and 4 are cross-sectional views of another example according to the present invention. In the figure (1) is a core made of a transparent polymer material, (
2) shows a layer made of a material with a lower refractive index than the core, and (3) shows a layer made of a material with a higher refractive index than the core.

一般C二、コア材料より低屈折率の物質をクラッド材料
とする光伝送体により伝送される光は、その比屈折率差
(Δ)に応じた全反射角(θC)を有し、これは次の式
で表わされる。
General C2: Light transmitted by an optical transmission body whose cladding material is a substance with a lower refractive index than the core material has a total reflection angle (θC) according to the relative refractive index difference (Δ), which is It is expressed by the following formula.

θC=血−1〜rrad〕 ここでΔはコアの屈折率をη1.クラッドの屈折率をη
2とすると Δ=(η7−訃)/2η: である。
θC=Blood−1~rrad] Here, Δ is the refractive index of the core and η1. The refractive index of the cladding is η
2, Δ=(η7−訃)/2η:

従って、η、がη1より小さいときは全反射角が存在す
るが、η、がη、より大きいときにはΔは負となり、全
反射角は存在しない。そのため、コア材料より低屈折率
の物質をクラッド材料とする光伝送体により伝送された
光は、クラッド層の屈折率が大きい部分に達すると、こ
の部分から光が放射される。
Therefore, when η is smaller than η1, a total reflection angle exists, but when η is larger than η, Δ becomes negative and no total reflection angle exists. Therefore, when light transmitted by an optical transmission body whose cladding material is a substance with a lower refractive index than the core material reaches a portion of the cladding layer with a higher refractive index, the light is emitted from this portion.

本発明の光放射体は、この様な原理に基くものであり、
第1図はクラッドとして低屈折率の物質と高屈折率の物
質が交互に形成された放射体の例であり、第2図は光フ
アイバー先端部のクラッド層が、高屈折率の物質で構成
され、この先端部2二至る光伝送部は、従来の光ファイ
バーと同様低屈折率のクラッド層で構成されている例で
ある。
The light emitter of the present invention is based on such a principle,
Figure 1 shows an example of a radiator in which a material with a low refractive index and a material with a high refractive index are alternately formed as the cladding, and in Figure 2, the cladding layer at the tip of the optical fiber is made of a material with a high refractive index. The optical transmission section leading to the tip end 22 is an example of a cladding layer having a low refractive index, similar to conventional optical fibers.

第3図、第4図は光ファイバーの断面方向C二おいてク
ラッド層の一部が高屈折率物質、他の部分が低屈折率物
質で構成されている例である。
3 and 4 are examples in which a part of the cladding layer is made of a high refractive index material and the other part is made of a low refractive index material in the cross-sectional direction C2 of the optical fiber.

〔実施例〕〔Example〕

この様な構造を有する光放射体は、コアとなる透明高分
子物質として、ポリメチルメタアクリレートを用い、ク
ラッド層低屈折率物質としてボ!j2.2.隼)リフル
オロエチルメタクリレート、高屈折率物質としてポリカ
ーボネートを用い、熔融紡糸法(二より2層ファイバー
製造ノズルに供給するクラッド物質を交互!:切替なが
ら紡糸すると、コア径980μ、クラッド厚さ10μの
光放射体が得られ、これは高屈折率のクラッド層を有す
る部分から伝送光の漏光が確認された。
A light emitting body having such a structure uses polymethyl methacrylate as the transparent polymer material serving as the core, and Bo! as the low refractive index material for the cladding layer. j2.2. Hayabusa) Using polycarbonate as the high refractive index material and polyfluoroethyl methacrylate, the melt spinning method (the cladding material supplied to the two-layer fiber production nozzle is alternated!: When spinning while switching, the core diameter is 980μ and the cladding thickness is 10μ). A light emitter was obtained, and leakage of transmitted light was confirmed from a portion having a cladding layer with a high refractive index.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、出射光の視覚特性が優れた光伝送体を
安価に、しかも簡単に製造す′ることができる。
According to the present invention, it is possible to inexpensively and easily manufacture a light transmission body with excellent visual characteristics of emitted light.

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

第1図および第2図は、本発明の実施例を示すそれぞれ
の光放射体の拡大斜視図である。 第3図および第4図は、本発明の他の実施例を示すそれ
ぞれの光放射体の拡大横断面図である。 図中の符号(1)は透明高分子コア、(2)は低屈折率
物質、(3)は高屈折率物質である。 青 l 図 膏 2 目 青4日
1 and 2 are enlarged perspective views of respective light emitters showing embodiments of the present invention. 3 and 4 are enlarged cross-sectional views of respective light emitters showing other embodiments of the present invention. In the figure, reference numeral (1) is a transparent polymer core, (2) is a low refractive index material, and (3) is a high refractive index material. Blue l plaster 2 eye blue 4th

Claims (3)

【特許請求の範囲】[Claims] (1)透明高分子物質からなるコア(A)と該コアを被
覆し、コアより低い屈折率の物質からなるクラッド層(
B)を有する光伝送体において、クラッド層(B)の少
なくとも一部が、前記のコアより高い屈折率を有する物
質(C)によつて形成していることを特徴とする光放射
体。
(1) A core (A) made of a transparent polymeric material and a cladding layer (A) covering the core and made of a material having a lower refractive index than the core.
1. A light transmitting body having a structure B), wherein at least a part of the cladding layer (B) is formed of a substance (C) having a higher refractive index than the core.
(2)コアより高い屈折率を有する物質(C)からなる
クラッド層が、光伝送体の片端部またはその付近に形成
されている特許請求の範囲第1項記載の光放射体。
(2) The light emitting body according to claim 1, wherein a cladding layer made of a substance (C) having a higher refractive index than the core is formed at or near one end of the light transmitting body.
(3)光伝送体の長さ方向に対して、クラッド層が、コ
アより低い屈折率を有する物質(B)とコアより高い屈
折率を有する物質(C)が交互に形成されている特許請
求の範囲第1項記載の光放射体。
(3) A patent claim in which the cladding layer is formed alternately of a material (B) having a refractive index lower than that of the core and a material (C) having a higher refractive index than the core in the longitudinal direction of the optical transmission body. The light emitter according to item 1.
JP60116147A 1985-05-29 1985-05-29 Luminous radiation body Pending JPS61273503A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60116147A JPS61273503A (en) 1985-05-29 1985-05-29 Luminous radiation body

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60116147A JPS61273503A (en) 1985-05-29 1985-05-29 Luminous radiation body

Publications (1)

Publication Number Publication Date
JPS61273503A true JPS61273503A (en) 1986-12-03

Family

ID=14679909

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60116147A Pending JPS61273503A (en) 1985-05-29 1985-05-29 Luminous radiation body

Country Status (1)

Country Link
JP (1) JPS61273503A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008215926A (en) * 2007-03-01 2008-09-18 Hitachi High-Technologies Corp Electrolyte measuring instrument and biochemical autoanalyzer
WO2010001589A1 (en) * 2008-07-02 2010-01-07 パナソニック株式会社 Guiding device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008215926A (en) * 2007-03-01 2008-09-18 Hitachi High-Technologies Corp Electrolyte measuring instrument and biochemical autoanalyzer
WO2010001589A1 (en) * 2008-07-02 2010-01-07 パナソニック株式会社 Guiding device
CN102067194A (en) * 2008-07-02 2011-05-18 松下电器产业株式会社 Guiding device
JPWO2010001589A1 (en) * 2008-07-02 2011-12-15 パナソニック株式会社 Guide device
JP5291101B2 (en) * 2008-07-02 2013-09-18 パナソニック株式会社 Guide device

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