JPH0760611B2 - Rainbow projection device - Google Patents

Rainbow projection device

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Publication number
JPH0760611B2
JPH0760611B2 JP61054511A JP5451186A JPH0760611B2 JP H0760611 B2 JPH0760611 B2 JP H0760611B2 JP 61054511 A JP61054511 A JP 61054511A JP 5451186 A JP5451186 A JP 5451186A JP H0760611 B2 JPH0760611 B2 JP H0760611B2
Authority
JP
Japan
Prior art keywords
light
condenser lens
light source
prism
rainbow
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.)
Expired - Lifetime
Application number
JP61054511A
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Japanese (ja)
Other versions
JPS62211802A (en
Inventor
昌 荒井
Original Assignee
昌 荒井
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 昌 荒井 filed Critical 昌 荒井
Priority to JP61054511A priority Critical patent/JPH0760611B2/en
Publication of JPS62211802A publication Critical patent/JPS62211802A/en
Publication of JPH0760611B2 publication Critical patent/JPH0760611B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 産業上の利用分野 本発明は、一般家庭、店舗、或いは舞台装置などの大型
装置として、或いは玩具、置物、縫包などの小型装置と
して、広い分野で光学的装飾効果を奏し得る虹投影装置
に関する。
Description: TECHNICAL FIELD The present invention has a wide range of optical decoration effects as a large device such as a general household, a store, or a stage device, or a small device such as a toy, a figurine, or a sewing bag. The present invention relates to a rainbow projection device.

従来の技術 従来の技術としては、発明者が既に実開昭60−26084号
公報で開示したように、光源の長さを大きくして光束を
増大し得る線状の白色光源と、これと平行に配置した平
板的な円筒コンデンサレンズと、プリズムとからなる虹
投影装置を挙げることができる。
2. Description of the Related Art As the prior art, as disclosed by the inventor in Japanese Utility Model Laid-Open No. 60-26084, a linear white light source capable of increasing the light flux by increasing the length of the light source, and a parallel white light source An example of the rainbow projection device includes a flat cylindrical condenser lens disposed in the above and a prism.

発明が解決しようとする問題点 従来の装置は、店舗照明や舞台照明を主とする大型で鮮
明な虹像を得る目的で、管状のハロゲンランプのように
輝度が高く且つ光源の長さを大きく採って光束を増大さ
せることができる線状光源を用い、これより発する光を
これと平行する円筒コンデンサレンズで平行光とし、こ
れをプリズムで分光して虹像を投影するものであった
が、光源が横長で且つコンデンサレンズが平板であるた
め、虹像の中央付近は鮮明に投影することができても、
両端に行くに従いコンデンサレンズから出る光は平行光
から次第に収斂光となり、プリズムによって分光された
色光が混合する結果、鮮明な虹像が得られない問題があ
った。
DISCLOSURE OF THE INVENTION Problems to be Solved by the Invention The conventional device has a high brightness and a long light source like a tubular halogen lamp for the purpose of obtaining a large and clear rainbow image mainly for store lighting and stage lighting. Using a linear light source that can increase the luminous flux, the light emitted from this is collimated by a cylindrical condenser lens parallel to this, and this is split by a prism to project a rainbow image. Since the light source is horizontally long and the condenser lens is a flat plate, it is possible to project clearly near the center of the rainbow image,
The light emitted from the condenser lens gradually converges from parallel light toward both ends, and as a result of mixing the colored light dispersed by the prism, a clear rainbow image cannot be obtained.

即ち、コンデンサレンズが平板であると、第6a図に示す
如く、光源0からコンデンサレンズ13に直交して入射す
る紙面に鉛直な0A断面に沿った光線は、第6b図のよう
に、平行光線となってプリズムに入射するが、光源0か
らコンデンサレンズ13に傾斜して入射する0B、0B′断面
に沿った光線は、第6c図のように、距離がD1だけ遠くな
るぶんだけ曲げられ、更に傾斜してコンデンサレンズ13
に入射する0C、0C′断面に沿った光線は、第6d図に示す
ように、距離がD2のように更に遠くなるぶんだけ強く曲
げられて収斂するため、これをプリズムで分光した虹像
は、第6e図に示す如く、中央Aから外側にB,B′、C,C′
のように遠ざかる程、曲率が増大して色光が混合し、鮮
明な虹像が得られないこととなり、光源0が横長管状の
場合には、光源とコンデンサレンズ13との距離は更に増
大することとなるから、色光の混合は更に大きくなり、
舞台照明や店舗照明を十分に満足する鮮明な虹像が得ら
れなかったのである。
That is, if the condenser lens is a flat plate, as shown in FIG. 6a, the light rays incident from the light source 0 orthogonally to the condenser lens 13 along the 0A cross section perpendicular to the paper surface are parallel rays as shown in FIG. 6b. The light rays along the 0B and 0B ′ cross sections which are incident on the prism from the light source 0 while being inclined to the condenser lens 13 are bent by the distance D1 as shown in FIG. 6c. Incline further and condenser lens 13
As shown in Fig. 6d, the rays incident on the 0C and 0C 'cross sections are strongly bent and converged as the distance becomes further D2, so that the rainbow image separated by the prism is , B, B ′, C, C ′ from the center A to the outside as shown in FIG. 6e.
As the distance from the light source increases, the curvature increases and the color lights are mixed, so that a clear rainbow image cannot be obtained. When the light source 0 is a horizontally long tube, the distance between the light source and the condenser lens 13 further increases. Therefore, the mixture of colored light becomes larger,
It was not possible to obtain a clear rainbow image that fully satisfied the stage lighting and store lighting.

また、この場合、平板状の円筒コンデンサレンズを使う
ため、光源を短くし点光源に近くして、中央付近の虹像
のみを使用しようとしても、光束が減少するばかりで、
光量不足となり、鮮明な虹像を得ることができない等の
問題があった。
Also, in this case, since a flat-plate cylindrical condenser lens is used, even if the light source is shortened to be close to the point light source and only the rainbow image near the center is used, the luminous flux is only reduced,
There was a problem that the amount of light became insufficient and a clear rainbow image could not be obtained.

問題点を解決するための手段 そこで本発明は、集光系の大きさに比較して点光源に近
い極く短い線状の白色光源と、該光源の発散光が中心に
向かう場合と左右両端に向かう場合で距離が殆ど同じ
で、屈折後に広い幅をもった扇状に拡がる平行光となる
ように、該光源を中心として円弧状に彎曲して設けた円
筒コンデンサレンズと、該コンデンサレンズで得られた
扇状の平行光を第一屈折面に入射するように設けた洗濯
板状のプリズムとからなる虹投影装置を提供しようとす
るものである。
Means for Solving the Problems Therefore, according to the present invention, an extremely short linear white light source that is closer to a point light source compared to the size of a light condensing system, and a case where divergent light of the light source goes to the center and both left and right ends The distance is almost the same when heading to, and a cylindrical condenser lens provided by bending the light source in an arc shape so as to obtain parallel light that spreads in a fan shape having a wide width after refraction and the condenser lens. It is intended to provide a rainbow projection device including a washing plate-shaped prism that is provided so that the fan-shaped parallel light is incident on the first refracting surface.

作用 本発明装置によれば、集光コンデンサレンズ等の集光系
の大きさに比較して点光源に近い極く短い線状の白色光
源と、該光源の発散光が中心に向かう場合と左右両端に
向かう場合で距離が殆ど同じで、屈折後に広い幅をもっ
た扇状に拡がる平行光となるように、該光源を中心とし
て円弧状に彎曲して設けた円筒コンデンサレンズとから
なる構成を有するから、第5a図に示す如く、光源0から
円弧状コンデンサレンズ3に至る距離は、コンデンサレ
ンズの中央に向かう場合0Aと、コンデンサレンズの左右
両端に向かう場合0B,0B′、OC,0C′とで殆ど同じであ
り、屈折後に収斂光または発散光となる比率は極めて小
さく、従って、コンデンサレンズから扇状に広がって出
る光は、第5b図に示す如く、全体にわたって略完全な平
行光であるから、プリズムによる分光後は、第5c図に示
すごとく、中央Aから両端部B,B′、C,C′に至るまで、
極めて鮮やかな色光が得られ、全体にわたり形の整った
美しい虹像が得られることとなり、玩具や置物に本発明
虹投影装置を内蔵することによって、新しい照明玩具や
室内装飾照明を創作することができる。
Effect According to the device of the present invention, an extremely short linear white light source that is closer to a point light source compared to the size of a light condensing system such as a condenser lens, and a case where divergent light of the light source goes to the center It has a configuration including a cylindrical condenser lens curved in an arc shape with the light source as a center so as to be parallel light that spreads in a fan shape having a wide width after refraction and has almost the same distance toward both ends. Therefore, as shown in FIG. 5a, the distance from the light source 0 to the arc-shaped condenser lens 3 is 0A when going to the center of the condenser lens, and 0B, 0B ′, OC, 0C ′ when going to the left and right ends of the condenser lens. The ratio of convergent light or divergent light after refraction is extremely small, and therefore, the light that spreads out in a fan shape from the condenser lens is almost perfectly parallel light as shown in FIG. 5b. , After spectroscopy with prism is, as shown in 5c view, both end portions B from the center A, B ', C, C' until the,
A very bright colored light can be obtained and a beautiful rainbow image with a well-shaped shape can be obtained over the whole. By incorporating the rainbow projection device of the present invention into a toy or a figurine, a new lighting toy or interior decoration lighting can be created. it can.

また、コンデンサレンズで得られた扇状の平行光を第一
屈折面に入射するように設けた洗濯板状のプリズムは、
第一屈折面の平面に対して多数の第二屈折面を構成する
面が洗濯板状に相対して、全体としては、第一屈折面に
沿った板状面がコンデンサレンズで得られた平行光の幅
の扇状の拡がり方向に沿って平板的に拡がることとなる
から、装置全体を虹の拡がりの扇の要の位置として平板
的に構成することができる作用がある。
Further, the washing plate prism provided so that the fan-shaped parallel light obtained by the condenser lens is incident on the first refracting surface,
The surfaces constituting the second refracting surfaces are opposed to the plane of the first refracting surface in a washing plate shape, and as a whole, the plate-like surface along the first refracting surface is parallel to that obtained by the condenser lens. Since it spreads in a flat plate shape along the fan-shaped spread direction of the light width, there is an effect that the entire device can be configured in a flat plate shape as a main position of the fan of the rainbow spread.

また、点光源に近い線状白色光源を中心として円弧状に
彎曲してコンデンサレンズを設けた構成であるから、投
影距離が大きくなれば、扇状に投影された虹像の幅も大
きくなり、分光後の各色は夫々色ごとに重なって純粋な
色光を示し、より鮮明になる効果があると共に、投影距
離が近いために起こる色光の混合を防ぐためには、コン
デンサレンズの円弧の中心に対して点光源の位置を調整
して、コンデンサレンズから出る光が虹投影位置で虹像
を結ぶように設置すれば、近距離でも鮮明な虹像を得る
ことができる。
In addition, since the condenser lens is provided by curving in an arc shape with a linear white light source close to a point light source as the center, the width of the fan-shaped projected rainbow image increases as the projection distance increases, and the spectral distribution increases. Each of the latter colors overlaps each other to show pure colored light, which has the effect of making it clearer, and in order to prevent the mixing of colored light that occurs due to the close projection distance, a point is set to the center of the arc of the condenser lens. If the position of the light source is adjusted so that the light emitted from the condenser lens forms a rainbow image at the rainbow projection position, a clear rainbow image can be obtained even at a short distance.

実施例 第1図及び第2図に示す本発明装置の原理図において、
1は白色電球で、2はその光源となる点光源に近いフィ
ラメントである。3はフィラメント2の中点を中心とし
て円弧状に彎曲する円筒コンデンサレンズで、4は円筒
コンデンサレンズ3の集光した光源を中心に扇状に広が
る平行光を第一屈折面に受けるプリズムである。
Example In the principle diagram of the device of the present invention shown in FIGS. 1 and 2,
Reference numeral 1 is a white light bulb, and 2 is a filament close to a point light source which is the light source. Reference numeral 3 is a cylindrical condenser lens which is curved in an arc shape with the midpoint of the filament 2 as the center, and 4 is a prism which receives parallel light spreading in a fan shape around the light source condensed by the cylindrical condenser lens 3 on the first refracting surface.

フィラメント2より発する光は、円筒コンデンサレンズ
3によって、第2図示の如く、紙面に平行となり、プリ
ズム4の稜線に垂直な面に沿った光線0Aを中心にして、
コンデンサレンズ3の円弧に向って光線0B、0Cのように
扇状に広がってプリズム4に入射する。
The light emitted from the filament 2 is made parallel to the paper surface by the cylindrical condenser lens 3 as shown in the second drawing, and the light ray 0A along the plane perpendicular to the ridgeline of the prism 4 is centered,
Light rays 0B and 0C spread in a fan shape toward the circular arc of the condenser lens 3 and enter the prism 4.

即ち、第5a図に示す如く、光源0から円弧状コンデンサ
レンズ3に至る距離は、コンデンサレンズの中央に向か
う場合0Aと、コンデンサレンズの左右両端に向かう場合
0B,0B′、OC,0C′とで殆ど同じであり、屈折後に収斂光
又は発散光となる比率は極めて小さく、従って、コンデ
ンサレンズから扇状に広がって出る光は、第5b図に示す
如く、全体にわたって略完全な平行光となる。
That is, as shown in FIG. 5a, the distance from the light source 0 to the arc-shaped condenser lens 3 is 0A when it is toward the center of the condenser lens and when it is toward both left and right ends of the condenser lens.
0B, 0B ', OC, 0C' are almost the same, and the ratio of convergent light or divergent light after refraction is extremely small.Therefore, the light emitted in a fan shape from the condenser lens is as shown in FIG. 5b. It becomes almost perfect parallel light throughout.

プリズム4に入射した光は、プリズムの第一、第二の屈
折面で屈折して、紙面の斜め下方にほぼ円錐状に拡がっ
て進み、且つ夫々の光はプリズムの分光作用により赤色
から紫色に分光され、第5c図に示すごとく、中央Aから
両端部B,B′、C,C′に至るまで、紙面に平行な投影面上
に円弧状の虹となって投影される。
The light incident on the prism 4 is refracted by the first and second refracting surfaces of the prism and spreads in a substantially conical shape obliquely below the paper surface, and each light changes from red to purple due to the spectral action of the prism. As shown in FIG. 5c, the light is dispersed and projected as an arc-shaped rainbow on the projection plane parallel to the paper from the center A to both ends B, B ', C, C'.

また、プリズム4から射出された夫々の色光は、第2図
でA,A1,A2に示すように、プリズム4に入射する角度条
件が同じ光は全て同じ角度に平行に屈折され、従って同
一色光は重なって、全体として虹の七色に分光された虹
像となる。
Also, as shown by A, A1, and A2 in FIG. 2, the respective colored lights emitted from the prism 4 are all refracted in the same angle at the same angle condition to be incident on the prism 4, so that the same colored light is emitted. Overlap to form a rainbow image that is spectrally divided into the seven colors of the rainbow.

また、この場合、投影距離が大きくなれば、投影された
虹像の幅も大きくなり、分光の各色は夫々色ごとに重な
って純粋な色光を示すようになる。投影距離が近いため
に起こる色光の混合を防ぐためには、円筒コンデンサレ
ンズ3による屈折後の光を完全な平行光とせず、投影距
離で焦点を結ぶような関係に構成すれば、近距離でも鮮
明な虹像を得ることができる。
Further, in this case, as the projection distance increases, the width of the projected rainbow image also increases, and the respective colors of the spectrum overlap with each other to show pure colored light. In order to prevent mixing of colored light caused by the short projection distance, if the light after refraction by the cylindrical condenser lens 3 is not made to be a perfect parallel light but is configured so as to focus at the projection distance, it is clear even at a short distance. You can get a nice rainbow image.

他方、第3図示の如く、プリズム3を一個の三角柱プリ
ズムではなく、小さな三角柱プリズムを多数平行に並べ
たものでも、同じプリズム分光効果を挙げることができ
るから、洗濯板状のプリズム4を代わりに使用すること
ができる。一般に、色分解には比較的高価な光学ガラス
を材料とするため、これを洗濯板状にすれば、材料の節
減となり、更にまた、光学ガラスに代わって加工が容易
で軽量且つ安価な透明プラスチックの材料で成形するこ
とも可能となる。
On the other hand, as shown in FIG. 3, the prism 3 is not a single triangular prism but a plurality of small triangular prisms are arranged in parallel to obtain the same prism spectral effect. Therefore, the washing plate prism 4 is used instead. Can be used. In general, a relatively expensive optical glass is used for color separation, so if it is made into a washing plate, the material will be saved. Furthermore, instead of the optical glass, a transparent plastic that is easy to process, lightweight and inexpensive. It is also possible to mold the material.

第4図は洗濯板状のプリズムを使用した本発明装置の実
施例を示すもので、装置全体のコストダウン、小型化及
び重量軽減が達成されている。
FIG. 4 shows an embodiment of the device of the present invention using a washing plate-shaped prism, and cost reduction, size reduction and weight reduction of the entire device are achieved.

即ち、図において、10は内側ケースで、図には示さない
外ケースでプリズム4部分を除いて周囲を光学的に被覆
してある。1は白色光源となる電球、2はそのフィラメ
ント、3は電球1を中心に円弧状をなす円筒コンデンサ
レンズ、4は洗濯板状のプリズムである。その他、11は
電球1に供電する導電線である。
That is, in the figure, 10 is an inner case, and the outer case (not shown) is optically coated around the periphery except for the prism 4. Reference numeral 1 is a light bulb serving as a white light source, 2 is a filament thereof, 3 is a cylindrical condenser lens having an arc shape around the light bulb 1, and 4 is a washing plate prism. In addition, 11 is a conductive wire that supplies electricity to the light bulb 1.

この場合、洗濯板状のプリズム4は、第3図からも明ら
かな如く、円筒コンデンサレンズ3による平行光を第一
屈折面の全体で斜めに受けるスペースで形成されていれ
ば良く、且つ、第二屈折面は第一屈折面に対して極めて
狭い間隔で平行に並ぶ多数の面の連なりからなり、全体
としては第一屈曲面に平行な稜線を連ねて連続する第二
屈曲面が構成されていることとなるから、洗濯板状のプ
リズム4の大きさは、コンデンサレンズで得られた平行
光の幅の扇状の拡がり方向に沿って平板的に拡がること
となるから、装置全体を虹の拡がりの扇の要の位置とし
て小型で薄い平板的な構成することができる。
In this case, as is clear from FIG. 3, the washing plate-shaped prism 4 may be formed in a space in which parallel light from the cylindrical condenser lens 3 is obliquely received by the entire first refraction surface, and The birefringent surface is composed of a series of many surfaces arranged in parallel with each other at an extremely narrow interval with respect to the first refracting surface, and as a whole, a continuous second bending surface is formed by connecting ridge lines parallel to the first bending surface. Since the size of the washing plate-shaped prism 4 spreads flatly along the fan-shaped spreading direction of the parallel light width obtained by the condenser lens, the entire device spreads a rainbow. It can be configured as a small and thin flat plate as a main position of the fan.

これら構成の小型照明玩具等に適した具体例を示すと、
フィラメント2の太さ約0.2mm、長さ約1.5mm、コンデン
サレンズ3の焦点距離約14mm、コンデンサレンズ3の円
弧の半径(光源の中心からコンデンサレンズの主点まで
の曲率半径)約14mm、コンデンサレンズ3の幅約10mm、
円弧の中心角約90°、豆電球の出力4.4W、光束85Lumen
である。また、強力な虹投影機を構成する場合は、メタ
ルハライドランプ等の輝度の高い放電灯を光源として、
前記各部の寸法を比例的に大きくすれば、比較的小型な
もので強力な投影装置が得られることとなる。
A specific example suitable for a compact lighting toy or the like having these configurations is as follows.
The thickness of the filament 2 is about 0.2 mm, the length is about 1.5 mm, the focal length of the condenser lens 3 is about 14 mm, the radius of the arc of the condenser lens 3 (the radius of curvature from the center of the light source to the main point of the condenser lens) about 14 mm, the condenser The width of the lens 3 is about 10 mm,
Center angle of arc about 90 °, miniature bulb output 4.4W, luminous flux 85Lumen
Is. Also, when constructing a powerful rainbow projector, a high-luminance discharge lamp such as a metal halide lamp is used as the light source.
If the dimensions of the respective parts are proportionally increased, a relatively compact and powerful projection device can be obtained.

効果 以上の通り、本発明装置によれば、集光系の大きさに比
較して点光源に近い極く短い線状の白色光源と、該光源
の発散光が中心に向かう場合と左右両端に向かう場合で
距離が殆ど同じで、屈折後に広い幅をもった扇状に拡が
る平行光となるように該光源を中心として、円弧状に彎
曲して設けた円筒コンデンサレンズと、該コンデンサレ
ンズで得られた扇状の平行光を第一屈折面に入射するよ
うに設けた洗濯板状のプリズムとからなる構成を有する
から、光源から円弧状コンデンサレンズに至る距離は、
コンデンサレンズの中央に向かう場合とコンデンサレン
ズの左右両端に向かう場合とで殆ど同じであり、屈折後
に収斂光又は発散光となる比率は極めて小さく、従っ
て、コンデンサレンズから扇状に広がって出る光は全体
にわたって略完全な平行光であるから、分光後は極めて
鮮やかな色光が得られ、全体にわたり形の整った美しい
虹像が得られる効果があり、且つ、本発明装置のコンデ
ンサレンズで得られた扇状の平行光を第一屈折面に入射
するように設けた洗濯板状のプリズムは、円筒コンデン
サレンズの幅と略一致する平行光を第一屈折面の全体で
斜めに受けると共に、第二屈折面は第一屈折面に対して
極めて狭い間隔で平行に並ぶ多数の面の連なりからな
り、全体としては第一屈折面に平行な稜線を連ねて連続
する第二屈折面の構成となるから、洗濯板状のプリズム
の大きさは、コンデンサレンズで得られた平行光の幅の
扇状の拡がり方向に沿って平板的に拡がることとなるか
ら、装置全体を虹の拡がりの扇の要の位置として小型で
薄い平板的な構成することができ、これを玩具や置物に
内蔵することによって、新しい照明玩具や室内装飾照明
を創作することができる効果がある。
Effects As described above, according to the device of the present invention, an extremely short linear white light source that is closer to a point light source compared to the size of the condensing system, and a case where the divergent light of the light source goes to the center and both left and right ends are provided. A cylindrical condenser lens curved in an arc shape with the light source as the center so as to become parallel light that spreads in a fan shape having a wide width after refraction and has almost the same distance when heading, and is obtained by the condenser lens. Since the fan-shaped parallel light is incident on the first refracting surface and the washing plate-shaped prism is provided, the distance from the light source to the arc-shaped condenser lens is
Almost the same when going to the center of the condenser lens and when going to the left and right ends of the condenser lens, the ratio of convergent light or divergent light after refraction is extremely small. Therefore, the light that spreads out in a fan shape from the condenser lens is the whole. Since it is a nearly perfect parallel light over the entire range, it has an effect that extremely bright colored light is obtained after the spectrum and a beautiful rainbow image with a regular shape is obtained over the whole area, and the fan shape obtained by the condenser lens of the device of the present invention. The washing plate-shaped prism provided so that the parallel light of the first refracting surface is incident on the first refracting surface as a whole while the parallel light substantially matching the width of the cylindrical condenser lens is obliquely received. Is a series of a number of surfaces arranged in parallel to the first refracting surface at extremely narrow intervals, and as a whole, a structure of a second refracting surface that is continuous with ridge lines parallel to the first refracting surface. Therefore, the size of the washing plate-shaped prism spreads flatly along the fan-shaped spreading direction of the width of the parallel light obtained by the condenser lens. The position can be made small and thin like a flat plate, and by incorporating this into a toy or a figurine, there is an effect that a new lighting toy or interior decoration lighting can be created.

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

第1図は本発明装置の光学系の原理を示す正面図、第2
図はそのII−II線で縦断して示す縦断側面図、第3図は
本発明装置の一実施例の光学系の原理を第2図と同様に
示す縦断側面図、第4図は第3図の光学系による実施例
の要部を一部切欠して示す斜面図、第5a図乃至第5c図は
本発明装置の要部の作用を説明する説明図であり、第6a
c図乃至第6e図はそれぞれ従来装置の要部の作用態様を
説明する説明図である。 1……白色電球 2……フィラメント 3……円弧状の円筒コンデンサレンズ 4……プリズム
FIG. 1 is a front view showing the principle of the optical system of the device of the present invention, and FIG.
FIG. 3 is a vertical sectional side view taken along the line II-II, FIG. 3 is a vertical sectional side view showing the principle of an optical system of an embodiment of the device of the present invention in the same manner as FIG. 2, and FIG. FIG. 6a is a perspective view showing a partial cutaway view of a main part of an embodiment of the optical system in the figure, and FIGS. 5a to 5c are explanatory views for explaining the operation of the main part of the device of the present invention.
FIGS. 6C to 6E are explanatory views for explaining the mode of action of the main part of the conventional device. 1 ... White light bulb 2 ... Filament 3 ... Arc-shaped cylindrical condenser lens 4 ... Prism

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】集光系の大きさに比較して点光源に近い極
く短い線状の白色光源と、該光源の発散光が中心に向か
う場合と左右両端に向かう場合で距離が殆ど同じで、屈
折後に広い幅をもった扇状に拡がる平行光となるよう
に、該光源を中心として円弧状に彎曲して設けた円筒コ
ンデンサレンズと、該コンデンサレンズで得られた扇状
の平行光を第一屈折面に入射するように設けた洗濯板状
のプリズムとからなる虹投影装置
1. A very short linear white light source that is closer to a point light source compared to the size of a condensing system, and the distances when the divergent light of the light source goes to the center and to the left and right ends are almost the same. In order to obtain parallel light that spreads in a fan shape with a wide width after refraction, the cylindrical condenser lens provided by bending the light source in an arc shape and the fan-shaped parallel light obtained by the condenser lens are Rainbow projection device including a washing plate-shaped prism provided so as to enter one refracting surface
JP61054511A 1986-03-12 1986-03-12 Rainbow projection device Expired - Lifetime JPH0760611B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61054511A JPH0760611B2 (en) 1986-03-12 1986-03-12 Rainbow projection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61054511A JPH0760611B2 (en) 1986-03-12 1986-03-12 Rainbow projection device

Publications (2)

Publication Number Publication Date
JPS62211802A JPS62211802A (en) 1987-09-17
JPH0760611B2 true JPH0760611B2 (en) 1995-06-28

Family

ID=12972666

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61054511A Expired - Lifetime JPH0760611B2 (en) 1986-03-12 1986-03-12 Rainbow projection device

Country Status (1)

Country Link
JP (1) JPH0760611B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113823160B (en) * 2021-11-08 2022-10-18 中国石油大学(北京) Rainbow presenting, measuring and controlling device

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS482082U (en) * 1971-05-26 1973-01-11
JPS538469Y2 (en) * 1974-08-07 1978-03-04
JPS6026084U (en) * 1983-07-29 1985-02-22 日本応用光学株式会社 rainbow projection device

Also Published As

Publication number Publication date
JPS62211802A (en) 1987-09-17

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