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JPS5944703A - Illuminator - Google Patents

Illuminator

Info

Publication number
JPS5944703A
JPS5944703A JP15628082A JP15628082A JPS5944703A JP S5944703 A JPS5944703 A JP S5944703A JP 15628082 A JP15628082 A JP 15628082A JP 15628082 A JP15628082 A JP 15628082A JP S5944703 A JPS5944703 A JP S5944703A
Authority
JP
Japan
Prior art keywords
lens
optical axis
lamp
light
point
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
JP15628082A
Other languages
Japanese (ja)
Inventor
堀 恒夫
茂 岡田
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.)
Toshiba Electric Equipment Corp
Toshiba Denzai KK
Original Assignee
Toshiba Electric Equipment Corp
Toshiba Denzai KK
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 Toshiba Electric Equipment Corp, Toshiba Denzai KK filed Critical Toshiba Electric Equipment Corp
Priority to JP15628082A priority Critical patent/JPS5944703A/en
Publication of JPS5944703A publication Critical patent/JPS5944703A/en
Pending legal-status Critical Current

Links

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】[Detailed description of the invention]

〔発明の技術外野〕 本発明は釘台やスタジオなどで使用するスポットライト
に好適な照明装置に関する。 〔発明の技術的背景〕 この種照明装置はgl1図に示すように、球面状の平凸
レンズまたはフレネルレンズなどのレンズlを光源2の
前面に配設し、光源2とレンズlとの距離をかえること
によってスポットの開き角全変更させるのが一般的に行
なわれCいる。そうして、この場合、第2図に示すよう
な配光特性となる。すなわち、光源2をレンズ1の光軸
Aのa点に設置したときは曲線Bとなf&)、光源2を
光軸Aのb点に設(へ1したときは曲線Oどなり、いず
れの場合も配光特性は裾が長くなる。すなわら、スポラ
トノ照射ハターンの輪郭がほけてシャープなスポットが
形成できない傾向にある。その原因Qユ・63図に示す
ように、レンズlを透過して照射される光の光軸Aとの
なす各点の角度の最大値θhθ2θ3が01〉θ2〉θ
3 となって異なってしまうので、止むを得ないとされ
tいた。 〔発明の目的〕 本発明tユ上Jの事情を考慮1.てンよされたもので、
ランプ位置を変化さL−Cスポットの大きさを変え°C
も常にスポットの照射パタ゛−ンの輪郭にほけが生ずこ
とがなく明確なスポットが形成できる照明装置百:提供
することを目的とする。 〔発明の概要〕 本発明はランプに対設される集光レンズを光軸をとおる
断?■形状が光軸から変位した点を円中心とした円の一
部で形成したこと全特徴とする。 〔発明の実施例〕 本発明の一実施例を第4図および第5図を参照して説明
する。11はランプ、C12は集光レンズである。 +1.レンズ12の中心部
[Technical Field of the Invention] The present invention relates to a lighting device suitable for spotlights used in nail stands, studios, and the like. [Technical Background of the Invention] As shown in Figure GL1, this type of illumination device has a lens l such as a spherical plano-convex lens or a Fresnel lens arranged in front of a light source 2, and the distance between the light source 2 and the lens l is It is common practice to completely change the spot opening angle by changing the spot. In this case, the light distribution characteristics as shown in FIG. 2 are obtained. In other words, when the light source 2 is installed at point a of the optical axis A of the lens 1, the curve B becomes f &), and when the light source 2 is installed at the point b of the optical axis A (f &), the curve becomes In other words, the light distribution characteristics have a longer tail.In other words, the outline of the irradiation pattern becomes blurred, making it difficult to form a sharp spot.The reason for this is that as shown in Figure 63, light passes through the lens L. The maximum value θhθ2θ3 of the angle of each point with the optical axis A of the irradiated light is 01>θ2>θ
3 and would be different, so it was deemed unavoidable. [Object of the Invention] The present invention was made in consideration of the circumstances mentioned above.1. I was so excited,
Change the lamp position and change the size of the L-C spot °C
An object of the present invention is to provide an illumination device which can always form a clear spot without blurring the outline of the spot irradiation pattern. [Summary of the Invention] The present invention provides a method for cutting a condensing lens placed opposite a lamp through an optical axis. ■The entire feature is that the shape is formed by a part of a circle whose center is a point displaced from the optical axis. [Embodiment of the Invention] An embodiment of the present invention will be described with reference to FIGS. 4 and 5. 11 is a lamp, and C12 is a condenser lens. +1. Center of lens 12

【3とランプllの発光部1
4とがほぼ光軸X上にあるように配設されている。 」二記集光レンズJ2は光軸Kff:とおる断面形状が
光軸Xかし変位した点を円中心とした円の一部で形成さ
れている。すなわぢ、レンズ12は第5図で示すように
、光軸Xの両側に光軸Xから変位したC2d点をそれず
れ円中心とした2個の円の一部で形成され、円中心とし
ての点、c、dはそれぞれランプ】1よりレンズ12側
にあるようにしている。なお、第4図および第5図にお
いて集光レンズ12の中央部で凹状に表わしているが、
この部分Q」、点線で示すように連続した曲面に形成(
7てもよい。 つぎに作用VCついて説明する。ランプ11の発光部1
4から放射した光は集光レンズ12ケとおし′C前方に
照射される。そして、集光レンズ12は円中心c、d点
を光軸Xから変位させた円の一部で形感されているので
、第5図に示すようにレンズ12の中央部、端部および
これらの中間部を透過して照射される光の光軸Xとのな
す各点の内置の最大値ψ8.ψ2.ψ3がψ1−Fψ2
キψ3となりて、レンズ各部を通過する光出力が光[1
Ill]Xとなず角の最大値の差を従来のレンズの場合
よ如小さくすることができる。そして、この場合の配光
が第6図に示すように、裾が長くなることがなく、明確
な照射パターンケなシシャープなスボ°ットが形成でき
る。また、ランプ11ヲ光輔XK沿って移動し、スポッ
トの開き角を変更させて照射パターンの径?変化させて
も上述と同様の傾向を示すことが確認された。すなわち
、第7図に点線で示す従来の平凸レン、ズと実線で示す
本発明・のレンズとをレンズの各部の光出力角とレンズ
中央部からの距離との関係でみると、本発明の実施例の
装置では最大開き角を示す範囲が従来のレンズを用いた
装ト↓シ広くなる。 すなわち、配光のきれ目が明確となυ第6図に示す配光
が得られ、ランプとレンズとの位置を変イヒさせてスポ
ットの開き角を変えても常にシャープな照射パターンが
得られる。 本発明を以上図示実施例に基づいて詳述したが、本発明
tよ種々の実施態様全許容すl。たとえば、ランプの背
部に反射板を設けたものであってもよい0 〔発明の効果〕 以上詳述したように、本発明はランプに対設される集光
レンズを光軸をとおる1面形状が光軸から変位した点を
円中心とした円の一部で形成したものであるから、kン
ズ各部を透過する光が光軸となす角度の最大値の差を小
さくすることができ、照射パターンの輪郭が明確化され
、シャープなスポット照明ができる。
[3 and light emitting part 1 of lamp ll
4 are arranged so that they are substantially on the optical axis X. 2. The condensing lens J2 is formed by a part of a circle whose cross-sectional shape passing through the optical axis Kff is centered at a point displaced from the optical axis X. In other words, as shown in FIG. 5, the lens 12 is formed by parts of two circles on both sides of the optical axis X, each having a point C2d displaced from the optical axis X as the center of the circle. Points c and d are located closer to the lens 12 than the lamp 1, respectively. Although the condensing lens 12 is shown in a concave shape at the center in FIGS. 4 and 5,
This part Q'' is formed into a continuous curved surface as shown by the dotted line (
7 is fine. Next, the effect VC will be explained. Light emitting part 1 of lamp 11
The light emitted from 4 is irradiated in front of 1'C through 12 condensing lenses. Since the condensing lens 12 is formed by a part of a circle whose centers c and d are displaced from the optical axis X, as shown in FIG. Maximum value ψ8. ψ2. ψ3 is ψ1−Fψ2
key ψ3, and the light output passing through each part of the lens is light [1
The difference between the maximum value of Ill]X and the bevel angle can be made smaller than in the case of conventional lenses. In this case, as shown in FIG. 6, the light distribution does not become long, and a sharp spot with a clear irradiation pattern can be formed. Also, move the lamp 11 along the XK and change the spot opening angle to determine the diameter of the irradiation pattern. It was confirmed that the same tendency as described above was exhibited even when the temperature was changed. That is, if we look at the relationship between the light output angle of each part of the lens and the distance from the center of the lens, we can see that the conventional plano-convex lens shown by the dotted line in FIG. 7 and the lens of the present invention shown by the solid line in FIG. In the device of this embodiment, the range showing the maximum aperture angle is wider than when mounting with a conventional lens. In other words, the light distribution shown in Figure 6 with clear breaks in the light distribution can be obtained, and even if the position of the lamp and lens is changed and the spot opening angle is changed, a sharp irradiation pattern can always be obtained. . Although the present invention has been described above in detail based on the illustrated embodiments, it is possible to implement the present invention in various ways. For example, a reflector may be provided on the back of the lamp. [Effects of the Invention] As described in detail above, the present invention provides a condenser lens disposed opposite to the lamp in a one-sided shape that passes through the optical axis. Since it is formed by a part of a circle centered on a point displaced from the optical axis, it is possible to reduce the difference in the maximum value of the angle that the light passing through each part of the lens makes with the optical axis. The outline of the pattern becomes clear and sharp spot lighting is possible.

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

第1〜第3図は従来例全示し、第1図は照明装置の概略
図、第2図tよ配光図、第3図はレンズ各点における光
出力範囲fの説明図、第4図〜6図は本発明の一実施例
を示し、絹4図は照ψJ装置の概略図、第5図はレンズ
各点における光出力範囲の説明図、第6図は配光図、第
7図はレンズ各点における光出力範囲を比較して示す図
。 11・・・う/ブ    12・・レンズ%許出願人 
東芝電徊株式会社 代理人 弁理士 小’+rf []:l芳弘f 1 図 才  2  悶 牙 3  邑 + 5 口 計 6  ロ 一6&−
Figures 1 to 3 show all conventional examples, Figure 1 is a schematic diagram of the illumination device, Figure 2 is a light distribution diagram, Figure 3 is an explanatory diagram of the light output range f at each point of the lens, and Figure 4 Figures 6 to 6 show an embodiment of the present invention, Figure 4 is a schematic diagram of the illumination ψJ device, Figure 5 is an explanatory diagram of the light output range at each point of the lens, Figure 6 is a light distribution diagram, and Figure 7 is a diagram showing a comparison of the light output range at each point of the lens. 11...U/B 12...Lens% Applicant
Toshiba Electric Co., Ltd. Agent Patent Attorney Ko' + rf []:l Yoshihiro f 1 Illustration 2 Agony 3 O + 5 Account 6 Loichi 6 &-

Claims (3)

【特許請求の範囲】[Claims] (1)  ランプと、 このランプに対設された集光レンズと、を具備し、上記
集光レンズは光軸をとおる断面形状が光軸から変位した
点を円中心とした円の一部で形成されていることを特徴
とする照明装置。
(1) It comprises a lamp and a condensing lens installed opposite to the lamp, and the condensing lens has a cross-sectional shape passing through the optical axis that is part of a circle centered at a point displaced from the optical axis. A lighting device characterized in that:
(2)  前記レン′ズは光軸の両側に光軸から変位し
た点を円中心とした2個の円の一部で形成したこと全特
徴とする特許請求の範囲(1)記載の照明装置。
(2) The illumination device according to claim (1), characterized in that the lenses are formed by parts of two circles on both sides of the optical axis, the centers of which are points displaced from the optical axis. .
(3)前記レンズの円中心はランプよりレンズ側に設け
ていることを特徴とする特許請求の範囲(1)または(
2)記載の照明装置。
(3) Claim (1) or (3) characterized in that the center of the circle of the lens is located closer to the lens than the lamp.
2) The lighting device described.
JP15628082A 1982-09-08 1982-09-08 Illuminator Pending JPS5944703A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15628082A JPS5944703A (en) 1982-09-08 1982-09-08 Illuminator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15628082A JPS5944703A (en) 1982-09-08 1982-09-08 Illuminator

Publications (1)

Publication Number Publication Date
JPS5944703A true JPS5944703A (en) 1984-03-13

Family

ID=15624365

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15628082A Pending JPS5944703A (en) 1982-09-08 1982-09-08 Illuminator

Country Status (1)

Country Link
JP (1) JPS5944703A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006286608A (en) * 2005-03-07 2006-10-19 Nichia Chem Ind Ltd Planar illumination light source and planar illumination device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006286608A (en) * 2005-03-07 2006-10-19 Nichia Chem Ind Ltd Planar illumination light source and planar illumination device

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