JPS6398606A - Optical fiber line light - Google Patents
Optical fiber line lightInfo
- Publication number
- JPS6398606A JPS6398606A JP61246303A JP24630386A JPS6398606A JP S6398606 A JPS6398606 A JP S6398606A JP 61246303 A JP61246303 A JP 61246303A JP 24630386 A JP24630386 A JP 24630386A JP S6398606 A JPS6398606 A JP S6398606A
- Authority
- JP
- Japan
- Prior art keywords
- light
- line
- end surfaces
- projection
- optical fiber
- 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
Links
- 239000013307 optical fiber Substances 0.000 title claims abstract description 23
- 238000005498 polishing Methods 0.000 claims abstract description 8
- 238000009826 distribution Methods 0.000 abstract description 14
- 239000000835 fiber Substances 0.000 abstract description 11
- 238000005452 bending Methods 0.000 abstract description 9
- 238000000034 method Methods 0.000 abstract description 8
- 238000007788 roughening Methods 0.000 abstract description 3
- 238000000576 coating method Methods 0.000 abstract description 2
- 230000004807 localization Effects 0.000 abstract 1
- 230000003287 optical effect Effects 0.000 description 9
- 230000000694 effects Effects 0.000 description 4
- 238000000149 argon plasma sintering Methods 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 229910052736 halogen Inorganic materials 0.000 description 1
- 150000002367 halogens Chemical class 0.000 description 1
- 238000011835 investigation Methods 0.000 description 1
- 238000007517 polishing process Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔童業上の利用分野〕
本発明は光学事務機器特に複写機等のライン光源として
有効に利用しうるラインライト光学系に関するものであ
り、特に出射光量の均一化され次光ファイバーラインラ
イトに関する。[Detailed Description of the Invention] [Field of Industrial Use] The present invention relates to a line light optical system that can be effectively used as a line light source for optical office equipment, particularly copying machines, etc. Regarding the next fiber optic line light.
一般にライン状光源を得る方法としては蛍光灯や線状ハ
ロゲン灯などがあるが、長手方向の光量の均一度を維持
しつつ長尺ものにすることは、その構造上難しく、その
為長さにも自ずと限界がちつ友。しかし近年光ファイバ
ーの急速な実用化に伴ない、その一端を円筒状に束ね、
円筒端面より光を入射させ、他端を1本1本引tk揃え
てライン状に並べ、そのライン状端面よυ出射させるこ
とによりライン状の光源を得るラインライトが作られ、
7アイバ一本数を増せば容易に長尺ものが得られるよう
になった。Fluorescent lamps and linear halogen lamps are generally used to obtain linear light sources, but due to their structure, it is difficult to make them long while maintaining the uniformity of the light amount in the longitudinal direction. A friend who naturally has a limit. However, with the rapid commercialization of optical fibers in recent years, one end of the optical fibers has been bundled into a cylindrical shape.
A line light is made that obtains a line-shaped light source by inputting light from the end of a cylinder, aligning the other ends one by one in a line, and emitting light from the line-shaped end.
By increasing the number of 7-eye bars, it became possible to easily obtain long ones.
〔発明が解決しようとする問題点」
この光ファイバーを用いたラインライトは一般的な照明
に用いられる場合はライン状方向の光量斑は特に大きな
問題とはならなかったが、近年目覚しく発展する光学事
務機器等の高度な光学分野などでは、このようなライン
状方向の光量斑が重大な問題となった。[Problem to be solved by the invention] When this line light using optical fibers is used for general lighting, unevenness in the amount of light in the line direction does not pose a particular problem, but optical office work has developed rapidly in recent years. In the field of advanced optics such as equipment, such unevenness in the amount of light in a linear direction has become a serious problem.
この光量斑の原因となるものは種々あるが、本発明者ら
が検討した結果、光臨となるランプなどに起因する光源
斑以外に光ファイバーをラインライト光学系に形成する
上での各々の光ファイバーの曲げの違いに起因する出射
角度光量分布の斑も大きな要因であることが判明し友。There are various causes of this light intensity unevenness, but as a result of our investigation, we found that in addition to the light source unevenness caused by lamps, etc. It turned out that unevenness in the output angle light intensity distribution due to differences in bending was also a major factor.
即ち、本発明が解決しようとする問題点はラインライト
光学系の各々の光ファイバーの曲げの相違による出射角
度光量分布に生じる斑である。That is, the problem to be solved by the present invention is the unevenness that occurs in the light output angle distribution due to the difference in the bending of each optical fiber of the line light optical system.
解決手段として、原因となる光ファイバーの曲げを均一
にすることは極めて難しく、又曲げ全なくすことは光フ
ァイバーの持つ最大の特徴を利用出来ないことになジ、
現実的ではない。As a solution, it is extremely difficult to make the bending of the optical fiber uniform, and eliminating the bending entirely would mean not being able to utilize the greatest feature of the optical fiber.
It's not realistic.
そこでこのような各々の光ファイバーに曲げの相違が生
じても出射角度、光量分布に斑を生じない方法について
鋭意研冗し友結果、ラインライトを構成する光ファイバ
ー端面に散乱処理を施すことで曲げの影響を受けずに斑
を低下させることを見出し友。Therefore, we have been conducting extensive research to find a way to prevent unevenness in the output angle and light intensity distribution even if there are differences in the bending of each optical fiber.As a result, we have developed a method to prevent the bending from occurring by applying scattering treatment to the end face of the optical fibers that make up the line light. A friend who found that it lowers plaque without being affected.
即ち本発明は、多数の光ファイバーを引き揃え、その一
端上ライン状に並べ固定し、光の入射あるいは出射端と
し、他端はライン状に並べるか又は束状にし、光の出射
あるいは入射端として横取されるラインライトにおいて
、光の入出射端面であるところの光ファイバーの端面の
少なくとも−7に散乱処理を施したことを特徴とする斑
の少々いラインライトである。That is, the present invention arranges a large number of optical fibers and arranges and fixes them in a line on one end to serve as the light input or output end, and the other end is arranged in a line or in a bundle to serve as the light output or input end. In the line light that is intercepted, the line light is a slightly uneven line light characterized in that at least -7 of the end face of the optical fiber, which is the light input/output end face, is subjected to scattering treatment.
光ファイバー端面の散乱処理方法は光を分散させる方法
であt′Lは、一般的に限定はされないが、例えば光散
乱物質のコーティング伝、プラスト法、粗研磨による粗
面化法などがある。元ファイバ一端面の散乱処理は両端
面を行うことが作用効果が大きいが−7のみ行っても効
果は生ずる。The scattering treatment method for the optical fiber end face is a method of dispersing light, and t'L is generally not limited, but includes, for example, coating with a light scattering substance, a plasting method, and a surface roughening method by rough polishing. Although scattering treatment for one end face of the original fiber is effective when both end faces are performed, the effect is produced even if only -7 is performed.
ファイバ一端面に散乱処理を施すことによる作用は、入
射端面にあっては、入射光を高次モード化することによ
り、曲げによる角度光量の偏在化上域らし、又出射端面
にあっては、偏在化した角度光量を分散させることであ
る。ま交ファイバ一端面を高価な又は高度な光学研磨を
せずにサンドペーパー等で処理すれば良いことにもなる
ので加工コスト低減の点からも多大な効果がある。The effect of applying scattering treatment to one end face of the fiber is to convert the incident light into a higher-order mode at the input end face, resulting in uneven distribution of the angular light amount due to bending, and at the output end face, to This is to disperse the unevenly distributed angular light amount. Since one end face of the crossed fibers can be treated with sandpaper or the like without expensive or sophisticated optical polishing, there is a great effect in terms of reducing processing costs.
実施例1
1本の光ファイバーの端より光を入射し、途中にファイ
バーの曲げを規制する曲げ治具(曲率半径15 wai
、 ) f取付け、その曲げに沿わせてファイバーを9
0°の角度で曲げ、曲が9の終わった箇所から15鵬全
直線にして、その端面で出射角度光量分布を測定した。Example 1 A bending jig (with a radius of curvature of 15 wa
, ) Attach f and insert the fiber 9 along the bend.
It was bent at an angle of 0° and made into a full straight line 15 degrees from the point where the song 9 ended, and the output angle light amount distribution was measured at the end face.
サンドペーパー÷400で光ファイバーの両端面を粗研
磨し、その時のファイバーの角度0゜近傍における出射
光量の分布を図1に示し九。Both end faces of the optical fiber were roughly polished with sandpaper ÷ 400, and the distribution of the output light amount near the fiber angle of 0° at that time is shown in Figure 19.
一方図2には通常の光学研磨のみの端部を有するライン
ライトの同様の出射光量分布を示しである。両図を比較
すると明らか々如く端面を粗面化したラインライトは出
射光電分布が大巾に改善されている。On the other hand, FIG. 2 shows a similar output light amount distribution of a line light having an end portion only subjected to optical polishing. Comparing the two figures, it is clear that the line light with roughened end faces has a greatly improved output photoelectric distribution.
実施例2
ライン状約220m長さに直径[L75am(コア径E
l 73 m )の芯鞘構造の光ファイバーを300本
並べ、他端は束ねて直径15.6mのバンドル部をもつ
、図5に示す形状のラインライトに於て、光ファイバー
の入出射端にサンドペー パー +400で粗研磨処理
を施し、バンドル部よシ光を入射させライン状部より出
射される光量分布を測定した。結果全図4に示す。Example 2 Line shape with a length of about 220 m and a diameter [L75 am (core diameter E
In a line light with the shape shown in Figure 5, in which 300 optical fibers with a core-sheath structure of 73 m) are lined up and the other end is bundled to form a bundle part with a diameter of 15.6 m, sandpaper is placed at the input and output ends of the optical fibers. A rough polishing process was performed at +400, and light was incident on the bundle portion, and the distribution of the amount of light emitted from the linear portion was measured. The entire result is shown in Figure 4.
この結果から、図3に示す通常の光学研磨のみの端部を
有する光量斑分布に比べ端部の粗面化処理後は大巾に光
量斑が減少していることがわかる。From this result, it can be seen that the light intensity unevenness is greatly reduced after the edge roughening treatment compared to the light intensity uneven distribution with the edge portion only subjected to optical polishing as shown in FIG.
図1は実施例1に示した1本のファイバーの入出射端面
を粗研磨処理した時の光の出射角度の光量分布である。
図2は同じ〈実施例1に示し一7’c1本のファイバー
の入出射端面を通常の光学研磨した状態の出射角度の光
量分布である。
図3及び4は実施例2に示し次ラインライト光学系のラ
イン部から出射される光量斑分布である。
図5はラインライトの全体を表わす1例である。
1ニライン部ファイバ一端面
2ニライン部口金
6:元ファイバー
4:バンドル部口金
5:バンドル部フ了1バ一端面
光量
光量
未処理ラインライト
ライ>Jt (mrn)
うP 3 図
炸U軒原処理ラインライト
ライン長 を声m)
;1i=4 図
才 5 図FIG. 1 shows the light intensity distribution of the light output angle when the input and output end faces of one fiber shown in Example 1 were subjected to rough polishing. FIG. 2 shows the light intensity distribution at the output angle when the input and output end faces of one fiber shown in Example 1 were subjected to conventional optical polishing. 3 and 4 show uneven distributions of light intensity emitted from the line portion of the next line light optical system shown in Example 2. FIG. 5 is an example showing the entire line light. 1 Two-line part fiber one end face Two-line part cap 6: Original fiber 4: Bundle part cap 5: Bundle part completed 1 bar One end surface Light amount Light amount Unprocessed line Light lay>Jt (mrn) Line light line length voice m) ;1i=4 Figure 5 Figure
Claims (2)
ン状に並べ固定し、光の入射あるいは出射端とし、他端
はライン状に並べるか又は束状にし、光の出射あるいは
入射端として構成されるラインライトであつて、光の入
出射端面であるところの光ファイバーの端面の少なくと
も一方に散乱処理を施したことを特徴とする光ファイバ
ーラインライト。(1) A large number of optical fibers are aligned, one end of which is arranged in a line and fixed as a light input or output end, and the other end is arranged in a line or bundled and configured as a light output or input end. 1. An optical fiber line light characterized in that a scattering treatment is applied to at least one end face of an optical fiber, which is a light input/output end face.
されたものであることを特徴とする特許請求の範囲第1
項記載のラインライト。(2) Claim 1, characterized in that the scattering treatment on the end face of the optical fiber is performed by rough polishing.
Line light as described in section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61246303A JPS6398606A (en) | 1986-10-16 | 1986-10-16 | Optical fiber line light |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61246303A JPS6398606A (en) | 1986-10-16 | 1986-10-16 | Optical fiber line light |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6398606A true JPS6398606A (en) | 1988-04-30 |
Family
ID=17146552
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61246303A Pending JPS6398606A (en) | 1986-10-16 | 1986-10-16 | Optical fiber line light |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6398606A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0508272A1 (en) * | 1991-04-10 | 1992-10-14 | Allen-Bradley Company, Inc. | Encoder with fiber optic collimator/aperture |
JP2006108591A (en) * | 2004-10-08 | 2006-04-20 | Tdk Corp | Rare-earth sintered magnet and manufacturing method therefor |
-
1986
- 1986-10-16 JP JP61246303A patent/JPS6398606A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0508272A1 (en) * | 1991-04-10 | 1992-10-14 | Allen-Bradley Company, Inc. | Encoder with fiber optic collimator/aperture |
JP2006108591A (en) * | 2004-10-08 | 2006-04-20 | Tdk Corp | Rare-earth sintered magnet and manufacturing method therefor |
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