JPS5880601A - Generator for parallel luminous fluxes - Google Patents
Generator for parallel luminous fluxesInfo
- Publication number
- JPS5880601A JPS5880601A JP56179248A JP17924881A JPS5880601A JP S5880601 A JPS5880601 A JP S5880601A JP 56179248 A JP56179248 A JP 56179248A JP 17924881 A JP17924881 A JP 17924881A JP S5880601 A JPS5880601 A JP S5880601A
- Authority
- JP
- Japan
- Prior art keywords
- generator
- luminous fluxes
- parallel luminous
- paraboloid
- paraboloids
- 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
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/18—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical projection, e.g. combination of mirror and condenser and objective
- G02B27/20—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical projection, e.g. combination of mirror and condenser and objective for imaging minute objects, e.g. light-pointer
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B19/00—Condensers, e.g. light collectors or similar non-imaging optics
- G02B19/0004—Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed
- G02B19/0019—Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed having reflective surfaces only (e.g. louvre systems, systems with multiple planar reflectors)
- G02B19/0023—Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed having reflective surfaces only (e.g. louvre systems, systems with multiple planar reflectors) at least one surface having optical power
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B19/00—Condensers, e.g. light collectors or similar non-imaging optics
- G02B19/0033—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
- G02B19/0047—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with a light source
Abstract
Description
【発明の詳細な説明】
本発明は、収斂した平行光束を得ることのできる平行光
束発生器Kil!する。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a parallel light flux generator Kil! that can obtain a convergent parallel light flux. do.
従来、この種のものとし【゛第1図に示すようなものが
ある。図において、Ps、Pg、P>は放物面、Flは
放物面P1の焦点、F2は放物面Ps、Pmの共通焦点
な示す、焦点F1に点光源を置けば、図示の・ように平
行光束か得られる。しかし、従来の技術では3つの放物
@ Ps、Pg、Pgを別々に加工し、それを図のよう
な関係位置に保持しなければならなかった。Conventionally, there is a device of this kind [as shown in FIG. 1]. In the figure, Ps, Pg, P> are paraboloids, Fl is the focus of the paraboloid P1, and F2 is the common focus of the paraboloids Ps and Pm.If you place a point light source at the focus F1, it will look like the figure. A parallel beam of light is obtained. However, in the conventional technology, the three paraboloids @ Ps, Pg, and Pg had to be processed separately and held in the relative positions as shown in the figure.
%に、放鴫物′wiPもpmは距離及び光軸を正確にセ
ットする必要かあり、したかって製品として甚だ高価な
ものになっていた。%, it is also necessary to accurately set the distance and optical axis for the droplet release product 'wiP', making the product extremely expensive.
本肩明は、上記員作上の問題点を解機して、この種の6
異ないし装置な安価に量−しうるよ5にしたものである
。以下、Emkより本発明を異体的に説明する。In order to solve the above-mentioned problems in the work, this kind of 6
It is possible to reduce the amount by using different equipment or equipment at a low cost. Hereinafter, the present invention will be explained differently from Emk.
菖21Jは、本発明の基本構造を示す儒mgである。
1IIc#いて、(1)が本発明、による平行光束発生
器である。放物−Plは本発明と直接関係なく、放物面
Plの代わりに他の平行光線を発生するものを使用しう
る。重置1111にお′いては、放物面P8とF3をア
クリル樹脂等め透明#料で一体に成形し、反射面となる
AB 、 CD 、 EF部のみ表面に外側からアルR
11に着を施す、DWs(ロ)は、平行光束な通過させ
るための窓で光軸に直角な平面とする。放物1iPs側
の平行光線が入射する面も、同じく光軸に直角な平面と
する。よって、放物11 Ps、Ps t−蓋彫りした
成形用の金層を作ろておけば・、成形加工により安41
に大量に生産することが可能となる。Iris 21J is a Confucian mg showing the basic structure of the present invention.
1IIc#, (1) is a parallel light flux generator according to the present invention. The paraboloid Pl is not directly related to the present invention, and instead of the paraboloid Pl, another one that generates parallel rays may be used. In superposition 1111, the paraboloids P8 and F3 are integrally molded with a transparent material such as acrylic resin, and Al R is applied from the outside to only the AB, CD, and EF parts, which will be the reflective surfaces.
11, DWs (b) are windows for passing parallel light beams, and are planes perpendicular to the optical axis. The surface on which the parallel rays enter on the parabolic 1iPs side is also a plane perpendicular to the optical axis. Therefore, if you can make a gold layer for molding the paraboloid 11 Ps, Ps t-lid, it will be cheaper by molding process.
It becomes possible to produce in large quantities.
縞3及び纂4図は、ビーム状に収束するのに重置Mを適
用した場合の例を示す。第3図は1円筒状1(1)の一
端に重置9111Cよるビーム光束発生響(11)を嵌
合する!!I ml(3)を形成し、その1M1部(3
)の夷に放物面P1を形成したビーム光束−発生装置を
示す、放切面Plの焦点Ft K豆電球の如き点光源を
置けば、窓Wかも密度の大きいビーム状の光束が得られ
る。Figures 3 and 4 show examples in which superposition M is applied to converge into a beam. In Fig. 3, a beam light flux generating sounder (11) by an overlapping 9111C is fitted to one end of a cylindrical shape 1 (1)! ! 1 ml (3) and 1 part (3
), the focal point Ft of the truncated surface P1, which represents a beam generator having a paraboloid P1, is placed.If a point light source such as a miniature light bulb is placed, a beam-shaped light beam with high density can be obtained from the window W.
この場合、ビーム光束発生器(11)も短い8簡もしく
はドラム状とし、その放物面P宜、P3゛は回転放物面
とする。第4図は、その形状な示す斜視図である。In this case, the beam generator (11) is also shaped like a short octave or a drum, and its paraboloid P and P3' are paraboloids of revolution. FIG. 4 is a perspective view showing its shape.
11g5WAは、平面状に収束するのに本発明を適用し
た場合の何を示す。図において、(1g)は、第2図の
平行光束発生器(1)の放物間Pg、Ps 41−一定
方向。11g5WA shows what happens when the present invention is applied to converge into a plane. In the figure, (1g) is the parabolic interval Pg, Ps 41 of the parallel beam generator (1) of FIG. 2 - constant direction.
例えば横力肉Kjli長した平面光束発生器な示す。For example, a planar light beam generator with a long lateral force Kjli is shown.
この場合、光源としては螢光灯などの−長いものを用い
る。こうすると、平面に収束した光のフィルムが得られ
る。In this case, a long light source such as a fluorescent lamp is used as the light source. This results in a film of light converging onto a plane.
H6及び菖7図は、円柱又は角柱状に収束するのに本発
明な適用した場合の例な示す。第6gは、縞5図の横長
の千両光束発生i) (1m)をリング状にいて自己の
光軸に一層しない平行光軸を中心として1[’転させた
ものに@蟻する。この場合、光源としてリング状の螢光
灯を用いるか又は電球から平行光−を作って用いてもよ
い。そうすると、円柱状の光束を得ることができる。第
7sは、第5図の千両光束発生器(12)を額縁のよ5
に4角に曲げた角柱光束発生器(14)を示す。かかる
角柱光束発生−(14) Kより、角a状の光束を得る
ことができる。Figures H6 and Iris 7 are examples of the case where the present invention is applied to converge into a cylinder or a prism. In the 6th g, the horizontally elongated luminous flux i) (1 m) of the stripe diagram 5 is rotated by 1[' around the parallel optical axis that is not aligned with the own optical axis and is in a ring shape. In this case, a ring-shaped fluorescent lamp may be used as the light source, or parallel light may be generated from a light bulb. In this way, a cylindrical light beam can be obtained. The 7th s is the Senryo beam generator (12) shown in Fig. 5.
2 shows a prismatic beam generator (14) bent at four corners. By generating such a prismatic light beam -(14)K, a light beam having an angular a shape can be obtained.
第8及び籐9Eは、円錐又は角錐状に収束するのに装置
−を適用した場合の例な示す。纂8!Iは、菖6図の円
柱光束発生器(in)において小さい方の放物面P2の
光軸の方向を変えた円錨濤東発生器(1暴)を示す。こ
の場合、窓Wも光軸に直角の平面に変える。第11gA
はその状況を示す部分的側面図、第8gBは全体の斜視
図である。かかる円錐光束発生11 (is) Kより
1円錐状の光束か得られる。The eighth and rattan 9E are examples in which the device is applied to converge into a conical or pyramidal shape. Bottom line 8! I shows a circular anchor Taoto generator (1st row) in which the direction of the optical axis of the smaller paraboloid P2 is changed in the cylindrical beam generator (in) shown in Diagram 6. In this case, the window W is also changed to a plane perpendicular to the optical axis. 11th gA
8gB is a partial side view showing the situation, and No. 8gB is a perspective view of the whole. By generating such a conical light beam 11 (is) K, one conical light beam can be obtained.
篤9図は、篇1図の角柱光束発生器(14)において小
さい方の放物面Pgの光軸の方向を変えた角錐光束発m
1)(i@)を示す、かかる角錐光束**器(1−)に
より、角錐状の光束が得られる。Figure Atsushi 9 shows the pyramidal beam generator (14) in Figure 1, in which the direction of the optical axis of the smaller paraboloid Pg is changed.
1) A pyramidal light flux is obtained by such a pyramidal light flux **device (1-) which indicates (i@).
第10JiAは、嬉3図に示すビーム光束発生偏置の応
用飼を示す略図である。IIにおいて、(幼は菖3図に
示す8筒状体(2)に当たる把持体で、その先端K11
l示しないビーム光束発生II(11)が恢合固定され
ている。また、(5)はオーバーヘッド・プ資ジエクタ
、(6)は鏡、(7)はスクリーン、(8)はスクリー
ン(7)上に投jllされた画像を示す。円筒状の把持
体(2)K光源用スイッチ等を設けておけば、手頃なく
−ム発生器になるので、オーバーヘッド・プpジエタタ
(5)を使用した金−などで指示具として便利である。10th JiA is a schematic diagram showing an application of the beam generation eccentricity shown in Figure 3. In II, (young is a gripping body corresponding to the 8-cylindrical body (2) shown in Fig. 3 of the irises, and its tip K11
A beam generator II (11), not shown, is fixedly assembled. Further, (5) shows an overhead projector, (6) shows a mirror, (7) shows a screen, and (8) shows an image projected onto the screen (7). If a cylindrical grip (2) is equipped with a switch for the K light source, it becomes an inexpensive light source, so it is useful as an indicator when using an overhead printer (5). .
これは、普通の指示棒と違って離れた位置からでも容易
に指示しさる利点かある。This has the advantage that, unlike a normal pointing stick, it allows you to point easily even from a distance.
第11図は、諏S〜篇9図の各穏゛光東発生器(Ig)
〜(1・)の応用#1な示す略図である。lllは、1
例として第e#Aの円柱光束発生器(Is)、と第8図
の円錐光束発生器(1s)とを用いて立体相貫図を作っ
た場合を示す0図において、a74″は鍾箱である0図
示の円柱と円錐に@らず、角錐、角柱、平面などの光束
な用いて4に1mの立体相貫図を作番ことができるので
、立体幾何学の説明用模型ないし軟材として利用するこ
とができる。Figure 11 shows each modem Koto generator (Ig) in Figure 9 of Su S~.
This is a schematic diagram showing application #1 of ~(1.). lll is 1
As an example, in Figure 0, which shows the case where a three-dimensional interoperability diagram is created using the cylindrical beam generator (Is) of e#A and the conical beam generator (1s) of Figure 8, a74'' is a peg box. In addition to the cylinders and cones shown in the diagram, it is possible to create a 1m in 3-D stereoscopic diagram using light beams such as pyramids, prisms, planes, etc., so it can be used as a model for explaining 3D geometry or a soft material. It can be used as
上記用途のはか、縞3図のビーム光束発生器(li)
=を2段又はそれ以上組合わせて、晃学プレーヤ(D
AD)に用いられるレーザの代わりに使用することがで
きる。すなわち、ビーム光束発生1i(it)のビーム
を平行光線として入射させこれを更に収束する小部同形
のビーム光束発生器な作り、これらを組合わせると一層
高密度のビームが得られる。Beam light flux generator (li) with three stripes for the above applications
= by combining two or more stages, Kogaku player (D
It can be used in place of the laser used in AD). In other words, the beam generator 1i (it) is made to have a small portion that is identical in shape to the parallel beam that enters the beam and further converges the parallel beam. When these are combined, a beam with even higher density can be obtained.
なお、上記の各種の実施例は、いずれも金層を数値制御
加工などで臘彫りしこれを用いズ成拳加工することによ
り容易に製作することが可能である。In addition, all of the above-mentioned embodiments can be easily manufactured by carving a gold layer using numerical control processing or the like, and then using the gold layer to perform a zuseiken process.
以上説明したとおり、本発明によれば、2つの放物面P
g、Psを一体成廖することによりPg、Pg間の*m
及び光軸が正確に保持され光の集束効率を向上しうるの
みならず、金!IIKよる成形加工であるため円柱をは
じめ円錐、角錐などの複雑な光束発生器も容易に製作す
ることができ、且つ量i!に最適である。As explained above, according to the present invention, two paraboloids P
*m between Pg and Pg by integrally forming g and Ps
Not only can the optical axis be held accurately and the light focusing efficiency can be improved, but gold! Since it is a molding process using IIK, complex light flux generators such as cylinders, cones, and pyramids can be easily manufactured, and the quantity i! Ideal for
gmo簡単す1IIj!
菖11Elは従来例を示す略図、菖2図は本発明の基本
構造を示す儒画図、第3及び1114図はビーム状に収
束する本発明の実施1P1tl−示す断面図及び斜視図
、第S図は平面状に収束する本発明の実施例な示す斜視
図、第6図は円柱状に収束する本発明の実施例な示す斜
視図、第71iは角柱状に収束する本発明の実施例な示
す斜視図、嬉sWAは円錐状に収束する本発明の実施例
な示す斜視図、第9図は角錐状に1gL東する本発明の
実施例を示す斜視図、第10図はビーム光束発生器の応
用例−を示す略図、縞11gはビーム光束発生器を除く
各種の光束発、生器の応用例な示す略図である。gmo easy 1IIj! Iris 11El is a schematic diagram showing a conventional example, Iris 2 is a Confucian drawing showing the basic structure of the present invention, Figures 3 and 1114 are cross-sectional and perspective views showing the embodiment 1P1tl of the present invention converging into a beam shape, and Figure S 71i is a perspective view showing an embodiment of the present invention converging into a planar shape, FIG. 6 is a perspective view showing an embodiment of the present invention converging into a cylindrical shape, and FIG. A perspective view showing an embodiment of the present invention in which the light beam sWA converges in a conical shape, FIG. 9 is a perspective view showing an embodiment of the present invention in which the beam sWA converges in a pyramidal shape by 1 gL, and FIG. 10 shows a beam flux generator. The stripes 11g are schematic diagrams showing application examples of various light flux generators and generators other than the beam generator.
F3・・・・・共通焦点、Pz、Ps・・@O・対内反
射放物面。F3... Common focus, Pz, Ps... @O, internal reflection paraboloid.
Claims (1)
対向反射放物面を具えた平行光束発生器。A parallel light beam generator that is integrally molded from transparent resin and has two opposing reflecting paraboloids that have a common focal point.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56179248A JPS5880601A (en) | 1981-11-09 | 1981-11-09 | Generator for parallel luminous fluxes |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56179248A JPS5880601A (en) | 1981-11-09 | 1981-11-09 | Generator for parallel luminous fluxes |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5880601A true JPS5880601A (en) | 1983-05-14 |
Family
ID=16062521
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP56179248A Pending JPS5880601A (en) | 1981-11-09 | 1981-11-09 | Generator for parallel luminous fluxes |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5880601A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5013143A (en) * | 1986-03-19 | 1991-05-07 | Combined Optical Industries Limited | Lens |
-
1981
- 1981-11-09 JP JP56179248A patent/JPS5880601A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5013143A (en) * | 1986-03-19 | 1991-05-07 | Combined Optical Industries Limited | Lens |
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