JPS61217716A - Apparatus for obtaining projection light using laser light - Google Patents
Apparatus for obtaining projection light using laser lightInfo
- Publication number
- JPS61217716A JPS61217716A JP5916785A JP5916785A JPS61217716A JP S61217716 A JPS61217716 A JP S61217716A JP 5916785 A JP5916785 A JP 5916785A JP 5916785 A JP5916785 A JP 5916785A JP S61217716 A JPS61217716 A JP S61217716A
- Authority
- JP
- Japan
- Prior art keywords
- light
- prism
- incident
- reflection surface
- cylindrical
- 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
Landscapes
- Lenses (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野〉
本発明はレーザ光を用いて遠方の壁面等に一条の合焦し
た投光線を得る装置に関し、水準儀等の測量機器、計測
機器、光エレクトロニス機器に利用しうるものである。Detailed Description of the Invention (Industrial Field of Application) The present invention relates to a device that uses a laser beam to obtain a focused beam of light on a distant wall, etc. It can be used for varnishing equipment.
〈発明が解決しようとする問題点〉
本発明者は、特願昭58−71746号(特開昭59−
196411号)等において、シリンドリカル反射面に
よってレーザビームを広範囲の角度に反射させて壁面等
に一条の投光線を得る発明を提案している。この発明は
、シリンドリカル反射面の曲面の設計次第で、投光線の
強度分布を任意に決定しうる利点がある反面、曲面の製
作が難カシく、また、左右の反射面によりレーザビーム
を拡散して左右の投光線を得ているため、左右の投光線
が完全に一直線になるようにするには反射面を高精度に
製作しなければならず製造コストが高くなるという欠点
があった。<Problems to be Solved by the Invention> The present inventor has proposed the following patent application in Japanese Patent Application No. 58-71746
No. 196,411), etc., propose an invention in which a laser beam is reflected at a wide range of angles by a cylindrical reflecting surface to obtain a single beam of light on a wall surface or the like. Although this invention has the advantage that the intensity distribution of the projected light beam can be determined arbitrarily depending on the design of the curved surface of the cylindrical reflecting surface, it is difficult to manufacture the curved surface, and the laser beam is diffused by the left and right reflecting surfaces. Since the left and right light beams are obtained by using the same method, the reflecting surface must be manufactured with high precision in order to ensure that the left and right light beams are perfectly aligned, which has the disadvantage of increasing manufacturing costs.
本発明の目的は、このような欠点を一挙に解決する、レ
ーザ光を用いて投光線を得る装置を提供することにある
。SUMMARY OF THE INVENTION An object of the present invention is to provide an apparatus for obtaining a projected light beam using a laser beam, which solves all of these drawbacks at once.
く問題点を解決するための手段〉
本発明の装置は、レーザ光の拡散ビーム発生装置と、上
記レーザ光を投光面に合焦させるための凸レンズと、そ
の凸レンズの通過光を所定方向に広角度拡散させるプリ
ズムを有し、そのプリズムが、入射レーザビームの光軸
に対し所定の角度をもつ第一の境界平面と、上記投光面
に対向し且つ上記光軸の方向と垂直な第二の境界平面と
、その第二の境界平面の後方に設けられたシリンドリカ
ル凸反射面と、上記第一の境界平面の入射光を上記シリ
ンドリカル凸反射面へ導く反射面を備えたものであるこ
とを特徴とする、レーザ光を用いて投光線を得る装置で
ある。Means for Solving Problems> The device of the present invention includes a diffused laser beam generator, a convex lens for focusing the laser beam on a projection surface, and a device for directing light passing through the convex lens in a predetermined direction. a prism for wide-angle diffusion, the prism having a first boundary plane having a predetermined angle with respect to the optical axis of the incident laser beam, and a second boundary plane facing the light projection surface and perpendicular to the direction of the optical axis; A second boundary plane, a cylindrical convex reflective surface provided behind the second boundary plane, and a reflective surface that guides the incident light of the first boundary plane to the cylindrical convex reflective surface. This is a device that uses laser light to obtain a projected light beam.
上記したレーザ光の拡散ビーム発生装置は、レーザ光源
自体の出力ビームが拡散している場合と、凹レンズ、凸
面鏡等により拡散させる場合とがある。In the above-described diffused laser beam generating device, the output beam of the laser light source itself is diffused, and the output beam is diffused by a concave lens, a convex mirror, or the like.
また、レーザ光を投映面に合焦させるための凸レンズに
対し、凹面鏡も均等手段である。Further, a concave mirror is also an equivalent means for a convex lens for focusing a laser beam on a projection surface.
〈実施例) 第1図に本発明実施例の全体構成図を示す。<Example) FIG. 1 shows an overall configuration diagram of an embodiment of the present invention.
レーザ光源1の光ビームは凹レンズ2によりやや拡散さ
れたのち、凸レンズ3により投光面に対し合焦させるよ
うに収束させ、プリズム4により一方向のみ広角度に拡
散させて扇状ビーム5を得、投光面6に一直線状の投光
線7を得ている。The light beam from the laser light source 1 is slightly diffused by a concave lens 2, then converged by a convex lens 3 so as to be focused on the projection surface, and diffused in only one direction at a wide angle by a prism 4 to obtain a fan-shaped beam 5. A linear projection line 7 is obtained on the projection surface 6.
第2図にプリズム4の斜視図を示す、全体形状は上下両
面が平坦な三角プリズムで、前部が方形、後部が三角形
をしており、入射レーザビームの光軸10に対し左右対
称形である。後部の境界平面11.12は光軸10に対
し角θの傾斜面をもちレーザビームの入射面となる。前
方部の左右の境界平面13.14は光軸10とほぼ平行
な平面であって入射光線の最初の全反射面となる。前面
の境界平面は光軸10と垂直な平面であってその左右両
端部に鏡面15.16が形成され、入射光線の2回目の
反射面となる。前面中央部17はレーザビームの外部へ
の放射面となる。この前面中央部17の後方にシリンド
リカル凸反射面18が形成されている。すなわち、放射
面17と平行な平面19と、光軸10と垂直な平面上に
あって且つ扇形ビーム5(第1図)と直交する線を軸と
するシリンドリカル面18より成る空間部20が形成さ
れており、シリンドリカル面18が鏡面になっている。Figure 2 shows a perspective view of the prism 4.The overall shape is a triangular prism with flat upper and lower surfaces, a square front part and a triangular rear part, and is symmetrical with respect to the optical axis 10 of the incident laser beam. be. The rear boundary plane 11,12 has an inclined surface at an angle .theta. to the optical axis 10 and serves as the entrance surface for the laser beam. The left and right boundary planes 13, 14 of the front part are planes substantially parallel to the optical axis 10 and serve as the initial total reflection surfaces of the incident light beam. The front boundary plane is a plane perpendicular to the optical axis 10, and mirror surfaces 15 and 16 are formed at both left and right ends thereof, and serve as a second reflection surface for the incident light beam. The front central portion 17 becomes a radiation surface for the laser beam to the outside. A cylindrical convex reflective surface 18 is formed behind this front center portion 17. That is, a space 20 is formed, which is composed of a plane 19 parallel to the radiation surface 17 and a cylindrical surface 18 whose axis is on a plane perpendicular to the optical axis 10 and perpendicular to the fan-shaped beam 5 (FIG. 1). The cylindrical surface 18 is a mirror surface.
第3図に、プリズム4の光路を示す。光軸10に沿って
入射するレーザビーム9のうち、左の入射面11に入射
した光は右方へ屈折し、右の側面14で全反射したのち
前面の反射面16で再び反射してシリンドリカル反射面
18の右半分に当り、ここで拡散反射され更に前面中央
の放射面17で屈折してプリズムの左前方へ放射される
。レーザビーム9のうち右の入射面12に入射した光は
、同様にして左の側面13.左の前面反射面15、シリ
ンドリカル反射面18.前面中央の放射面17を経て右
前方へ放射される。FIG. 3 shows the optical path of the prism 4. Of the laser beam 9 incident along the optical axis 10, the light incident on the left entrance surface 11 is refracted to the right, totally reflected on the right side surface 14, and then reflected again on the front reflection surface 16 to form a cylindrical beam. The light hits the right half of the reflection surface 18, is diffusely reflected there, is further refracted by the radiation surface 17 at the center of the front surface, and is radiated to the left front of the prism. The light incident on the right incident surface 12 of the laser beam 9 is similarly transmitted to the left side surface 13 . Left front reflective surface 15, cylindrical reflective surface 18. The light is emitted to the right front through the radiation surface 17 at the center of the front surface.
次に本発明により得られた投光線の強度特性について説
明する。Next, the intensity characteristics of the projected light beam obtained by the present invention will be explained.
第4図の曲線aに示す強度分布特性をもち、同図すに示
す円形の絞りを通過したレーザビームをプリズム4に入
射させ壁面6に投光する場合について、コンピュータに
よるシュミレーションを行った。第4図すに示すように
、光軸を通る鉛直面Cと平行で且つ等しい間隔で切断し
た板状部分CI+C2+ ’−−−・C1Bを考える。A computer simulation was performed for a case in which a laser beam having an intensity distribution characteristic shown by curve a in FIG. 4 and having passed through a circular aperture shown in FIG. 4 was incident on the prism 4 and projected onto the wall surface 6. As shown in FIG. 4, consider a plate-shaped portion CI+C2+'---.C1B cut parallel to a vertical plane C passing through the optical axis and at equal intervals.
この各部分による投光線は第5図に示すように、dl、
d2.・−・・dlBとなる。なお、レーザビームの径
すの左右両端部はプリズム内で有効に反射されず消失す
る。レーザビームの強度が最も大きい中央部c1が投光
線の最も遠方へ放射されてその投光線の長さが最も大き
くなり、これに反対に、レーザビームの強度が最も小さ
い端部CI8が投光線の中央へ放射されて投光線の長さ
が最も小さくなり、全体として投光線の強度分布がよく
均等化されていることが確認された。As shown in Fig. 5, the light beams projected by each part are dl,
d2. ...dlB. Note that the left and right ends of the laser beam are not effectively reflected within the prism and disappear. The center part c1, where the laser beam intensity is highest, is emitted to the farthest point of the light beam, and the length of the light beam is the largest.On the other hand, the end part CI8, where the laser beam intensity is the smallest, is the farthest part of the light beam. It was confirmed that the length of the projected light beam was the smallest when it was emitted toward the center, and that the intensity distribution of the projected light beam was well balanced as a whole.
第6図に本発明のプリズムの他の実施例を示す。FIG. 6 shows another embodiment of the prism of the present invention.
この実施例が第3図に示したものと相違している点は、
左右両側面の反射面13A、14Aが光軸10と平行で
ないことである。This embodiment differs from the one shown in FIG.
The reflective surfaces 13A and 14A on both the left and right sides are not parallel to the optical axis 10.
本発明のプリズム4は、上記実施例の形状に限定される
ものではなく、種々な変形により実施することができる
。入射面となる第一の境界平面が光軸に対しなす角θは
鋭角に限らず鈍角であってもよく、その場合はレーザビ
ームの左半分は左方へ、右半分は右方へ屈折入射する。The prism 4 of the present invention is not limited to the shape of the above-mentioned embodiments, but can be implemented with various modifications. The angle θ that the first boundary plane, which is the incident surface, makes with the optical axis is not limited to an acute angle, but may be an obtuse angle. In that case, the left half of the laser beam is refracted to the left, and the right half is refracted to the right. do.
また、反射面は実施例に示した2回反射に限らず、1回
反射又は3回以上の反射により実施することができる。Moreover, the reflective surface is not limited to the two-time reflection shown in the embodiment, but can be implemented by one-time reflection or three or more reflections.
更に、光軸に対し左右対象でなく、入射レーザビームの
すべてを一方向に屈折させるような形状でもよい。Furthermore, the shape may not be symmetrical with respect to the optical axis, but may be such that all of the incident laser beam is refracted in one direction.
く効果〉
本発明によれば、1 filのプリズムにより全長数十
メートルに及び、しかも線幅4.0 ms+以下の強く
てシャープな投光線が得られる。Effects> According to the present invention, a 1 fil prism can produce a strong and sharp projected light line with a total length of several tens of meters and a line width of 4.0 ms+ or less.
また、単一のシリンドリカル反射面により扇状拡散ビー
ムを得ているので左端から右端まで完全に直線な不連続
点のない一本の投光線が得られ、その光強度もほぼ均一
化されて強度むらが小さい。In addition, since a fan-shaped diffused beam is obtained using a single cylindrical reflecting surface, a single perfectly straight light beam with no discontinuities is obtained from the left end to the right end, and the light intensity is almost uniform, resulting in uneven intensity. is small.
第1図は本発明実施例の全体を示す斜視図、第2図は本
発明のプリズムの実施例を示す斜視図、第3図は第2図
に示すプリズムの平面図とその光路を併記した図、第4
図及び第5図は本発明の強度分布の説明図である。第6
図は本発明のプリズムの他の実施例の平面図とその光路
を併記した図である。
1−・−レーザ光源
2−凹レンズ
3−・・・凸レンズ
4・・・・プリズム
5−・・扇状ビーム
6−・−・投光面
7−・−投光線
lO・−・光軸
11.12・−・第一の境界平面(入射面)13.14
−・・反射面
15.16・・−反射面
17−第二の境界平面(放射面)
18・−・・シリンドリカル反射面
20−・・空間部
特許出願人 尾 崎 康 入
代 理 人 弁理士 西1) 新
第1図Fig. 1 is a perspective view showing the entire embodiment of the present invention, Fig. 2 is a perspective view showing an embodiment of the prism of the present invention, and Fig. 3 is a plan view of the prism shown in Fig. 2 and its optical path. Figure, 4th
FIG. 5 is an explanatory diagram of the intensity distribution of the present invention. 6th
The figure is a plan view of another embodiment of the prism of the present invention and its optical path. 1--Laser light source 2-Concave lens 3--Convex lens 4--Prism 5--Fan-shaped beam 6--Light projection surface 7--Light projection line lO--Optical axis 11.12・-・First boundary plane (incidence plane) 13.14
- Reflective surface 15, 16... - Reflective surface 17 - Second boundary plane (radiation surface) 18... Cylindrical reflective surface 20 - Spatial section Patent applicant Yasushi Ozaki Attorney Patent attorney West 1) New map 1
Claims (1)
面に合焦させるための凸レンズと、その凸レンズの通過
光を所定方向に広角度拡散させるプリズムを有し、その
プリズムが、入射レーザビームの光軸に対し所定の角度
をもつ第一の境界平面と、上記投光面に対向し且つ上記
光軸の方向と垂直な第二の境界平面と、その第二の境界
平面の後方に設けられたシリンドリカル凸反射面と、上
記第一の境界平面の入射光を上記シリンドリカル凸反射
面へ導く反射面を備えたものであることを特徴とする、
レーザ光を用いて投光線を得る装置。It has a diffused beam generator for laser light, a convex lens for focusing the laser light on a projection surface, and a prism for diffusing light passing through the convex lens over a wide angle in a predetermined direction, and the prism is configured to focus the laser beam on the incident laser beam. a first boundary plane having a predetermined angle with respect to the optical axis; a second boundary plane facing the light projection surface and perpendicular to the direction of the optical axis; and a second boundary plane provided behind the second boundary plane. a cylindrical convex reflective surface with a cylindrical convex reflective surface; and a reflective surface that guides incident light on the first boundary plane to the cylindrical convex reflective surface;
A device that uses laser light to obtain a projected light beam.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5916785A JPS61217716A (en) | 1985-03-22 | 1985-03-22 | Apparatus for obtaining projection light using laser light |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5916785A JPS61217716A (en) | 1985-03-22 | 1985-03-22 | Apparatus for obtaining projection light using laser light |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61217716A true JPS61217716A (en) | 1986-09-27 |
Family
ID=13105552
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5916785A Pending JPS61217716A (en) | 1985-03-22 | 1985-03-22 | Apparatus for obtaining projection light using laser light |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61217716A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6425008A (en) * | 1987-07-02 | 1989-01-27 | Spectra Physics | Transmitter |
WO2003052395A1 (en) * | 2001-12-18 | 2003-06-26 | Cognex Technology And Investment Corporation | Apparatus and method for slide illumination |
-
1985
- 1985-03-22 JP JP5916785A patent/JPS61217716A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6425008A (en) * | 1987-07-02 | 1989-01-27 | Spectra Physics | Transmitter |
WO2003052395A1 (en) * | 2001-12-18 | 2003-06-26 | Cognex Technology And Investment Corporation | Apparatus and method for slide illumination |
US6914679B2 (en) | 2001-12-18 | 2005-07-05 | Cognex Technology And Investment Corporation | Side light apparatus and method |
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