JPH0743848Y2 - Lighting equipment - Google Patents
Lighting equipmentInfo
- Publication number
- JPH0743848Y2 JPH0743848Y2 JP1989107960U JP10796089U JPH0743848Y2 JP H0743848 Y2 JPH0743848 Y2 JP H0743848Y2 JP 1989107960 U JP1989107960 U JP 1989107960U JP 10796089 U JP10796089 U JP 10796089U JP H0743848 Y2 JPH0743848 Y2 JP H0743848Y2
- Authority
- JP
- Japan
- Prior art keywords
- light
- bulb
- reflector
- reflecting member
- mirror
- 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
Links
- 230000003287 optical effect Effects 0.000 claims description 34
- 230000005540 biological transmission Effects 0.000 claims description 25
- 230000000694 effects Effects 0.000 claims description 5
- 238000007740 vapor deposition Methods 0.000 claims description 3
- 230000004907 flux Effects 0.000 description 10
- 238000007796 conventional method Methods 0.000 description 4
- 238000009826 distribution Methods 0.000 description 4
- 239000000835 fiber Substances 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 238000005452 bending Methods 0.000 description 3
- 238000009792 diffusion process Methods 0.000 description 3
- 239000000919 ceramic Substances 0.000 description 2
- 230000008859 change Effects 0.000 description 2
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000013307 optical fiber Substances 0.000 description 2
- 230000003595 spectral effect Effects 0.000 description 2
- 239000004925 Acrylic resin Substances 0.000 description 1
- 229920000178 Acrylic resin Polymers 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 230000009471 action Effects 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 239000004973 liquid crystal related substance Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 239000005304 optical glass Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 229920002050 silicone resin Polymers 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
Landscapes
- Light Guides In General And Applications Therefor (AREA)
- Optical Elements Other Than Lenses (AREA)
Description
【考案の詳細な説明】 〔産業上の利用分野〕 本考案は照明具に関し、特に、光伝送用ロッドあるいは
光伝送用ファイバーバンドル等の光伝送体の照明に用い
て好適な照明具に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to an illuminator, and more particularly to an illuminator suitable for illuminating an optical transmission body such as an optical transmission rod or an optical transmission fiber bundle.
光ファイバーバンドルの一端に光を入射させ、他端を線
状に配列して線状光線を出射する光ファイバーバンドル
照明用の照明具にあっては、スペースファクタ改善のた
めに、光源からの光を反射部材に反射させて、光路を途
中で折曲する方法が用いられる場合がある。(例えば、
特開平1−14803号公報参照)。In an illuminator for optical fiber bundle lighting, in which light is incident on one end of the optical fiber bundle and the other end is arranged in a line to emit a linear light beam, the light from the light source is reflected to improve the space factor. A method may be used in which the member is reflected and the optical path is bent halfway. (For example,
See Japanese Patent Laid-Open No. 1-14803).
従来の光路を折曲する方法にあっては、光路が直線状の
場合に比べると、光路を折曲するために反射部材を介在
させる必要がある。この反射部材の反射率が100%とは
なり得ないことにより、光路が直線状の場合の光量に比
べて、光路を折曲する場合の光量は、低下せざるを得な
かった。In the conventional method of bending the optical path, it is necessary to interpose a reflecting member to bend the optical path, as compared with the case where the optical path is linear. Since the reflectance of this reflecting member cannot be 100%, the amount of light when the optical path is bent must be reduced as compared with the amount of light when the optical path is linear.
特に、高光量用途のファイバー照明用及び特開昭62−14
2465号公報等に示されている石英ガラスロッド、光学ガ
ラスロッド、シリコーン樹脂ロッド、アクリル樹脂ロン
ド等よりなる光伝送用ロッドを用いた照明装置の照明用
として使用する場合には、従来のように、光源からの光
を何ら集光することなしに単に反射部材に反射させて光
路を折曲する方法では光量低下に対する改善が不十分で
あり、集光効率が悪かった。In particular, for fiber lighting for high light intensity applications and JP-A-62-14
When used for illumination of an illuminating device using an optical transmission rod made of a quartz glass rod, an optical glass rod, a silicone resin rod, an acrylic resin rod, etc. disclosed in Japanese Patent No. 2465, etc. However, the method of simply reflecting the light from the light source on the reflecting member and bending the optical path without collecting the light does not sufficiently improve the reduction of the light amount, and the light collecting efficiency is poor.
すなわち、線状光源用ファイバーバンドルあるいは液晶
ビデオプロジェクタ等において多用されている従来の光
路を折曲する方法は、いずれの場合においても、線状光
の分布を均一にするため、所定のエリアを均一に照射す
ることにのみ重点が置かれている。つまり光源からの光
は集光部材により集光されることなく、幅広い光束のま
まで反射部材に照射され、反射部材の反射により、幅広
い光束の光がファイバーバンドル等の入射端に入射され
ていた。従って、集光効率の面では、犠牲を強いられて
おり、満足のいく集光効率を達成することができないも
のであった。ところが光伝送用ロッドの場合には、線状
光の分布を均一にするための方法は、光伝送用ロッド自
体の加工により行えるため、集光効率の追求を主体とし
た設計が必要となっていた。That is, in any case, the conventional method of bending the optical path, which is often used in a fiber bundle for a linear light source, a liquid crystal video projector, or the like, makes a predetermined area uniform in order to make the distribution of the linear light uniform. The focus is only on irradiating. That is, the light from the light source is not condensed by the condensing member, and is irradiated to the reflecting member as a wide light flux, and the light of the wide light flux is incident on the incident end of the fiber bundle or the like by the reflection of the reflecting member. . Therefore, in terms of the light collection efficiency, there is a sacrifice, and a satisfactory light collection efficiency cannot be achieved. However, in the case of the optical transmission rod, the method for making the distribution of the linear light uniform can be performed by processing the optical transmission rod itself, so it is necessary to design mainly for the pursuit of light collection efficiency. It was
ところが、従来の方法において光量低下を補うために
は、光源の消費電力を増加させなければならないという
問題点があり、また装置全体としても比較的大型なもの
となっていて、小型化が図られていないという問題点が
あった。However, in the conventional method, there is a problem that the power consumption of the light source must be increased in order to compensate for the decrease in light amount, and the apparatus as a whole is relatively large, which leads to downsizing. There was a problem that not.
本考案は、従来の技術を有するこのような問題点に鑑み
てなされたものであり、その目的とするところは、集光
効率を向上させると共に反射部材の分光分布特性に一様
な変化を持たせて光量低下を招来することなく光路を折
曲することができ、反射部材を小型、低コストとし、さ
らに装置全体を小型軽量化した照明具を提供することを
目的とする。The present invention has been made in view of the above problems of the conventional technique, and an object of the present invention is to improve the light collection efficiency and to have a uniform change in the spectral distribution characteristics of the reflecting member. It is therefore an object of the present invention to provide an illuminator in which the optical path can be bent without causing a decrease in the amount of light, the reflecting member is small and low cost, and the entire device is small and lightweight.
上記目的を達成するために、本考案における照明具は、
光源たる反射鏡付電球の出射光を反射部材で90°折曲し
て光伝送体の入射端に入射するとともに、この反射鏡付
電球が出射端から反射部材までの光路を円錐形状として
光束の集光角に合わせ、光伝送体の入射端の結合ギャッ
プを極小化して集光効率を向上させ、さらに、反射鏡付
電球の閉口径と反射鏡付電球の出光部から集光点までの
集光距離(ワーキングディスタンス)が略等しいように
してなるものである。In order to achieve the above-mentioned object, the lighting device according to the present invention comprises:
The light emitted from the light bulb with a reflector, which is the light source, is bent 90 ° by the reflection member to enter the incident end of the light transmission body, and this light bulb with a reflector has a conical optical path from the emission end to the reflection member, and In accordance with the angle of collection, the coupling gap at the incident end of the optical transmission body is minimized to improve the efficiency of collection, and further, the closed diameter of the bulb with a reflector and the collection point from the light emitting part of the bulb with a reflector to the collection point. The optical distances (working distances) are made substantially equal.
反射鏡付電球の出射端から反射部材までの光路が円錐形
状で結合部の光モレ損失が少なく、反射鏡付電球の開口
径と反射鏡付電球のワーキングディスタンスが略等しい
ので、光伝送体への最大入射角が27°程度と入射端面で
のフレネル反射による影響を少なくし、全光路が短くな
り、かつ電球フィラメントの位置ずれあるいは反射鏡付
電球の反射鏡の曲率誤差等によって生じる集光部の光束
のビームウェストの広がりが少なくなり、光束のしぼり
込み効率が向上するため集光効率が向上する。また、反
射鏡付電球の出射端から反射部材までの光路を円錐形状
としたので、反射部材の形状が小型で済むとともに、光
路設計のコンパクト化に伴い集光部材の小型軽量化を促
進することができ、かつ製造コストも低減できる。Since the optical path from the emitting end of the light bulb with a reflector to the reflecting member is conical, there is little light leakage loss at the coupling part, and the aperture diameter of the light bulb with a reflector and the working distance of the light bulb with a reflector are approximately the same. The maximum incident angle of about 27 ° reduces the effect of Fresnel reflection on the incident end face, shortens the total optical path, and causes the light condensing part caused by the displacement of the bulb filament or the curvature error of the reflector of the bulb with a reflector. The spread of the beam waist of the light flux is reduced, and the efficiency of narrowing the light flux is improved, so that the light collection efficiency is improved. Further, since the optical path from the emission end of the light bulb with a reflecting mirror to the reflecting member has a conical shape, the shape of the reflecting member can be small, and the compactness and lightening of the light collecting member can be promoted as the optical path design becomes compact. And the manufacturing cost can be reduced.
以下、図面に基づいて本考案による照明具を詳細に説明
する。Hereinafter, a lighting device according to the present invention will be described in detail with reference to the drawings.
第1図乃至第4図は、本考案による一実施例を示し、こ
の照明具は、外周面に軸方向直線細縞状に高屈折率の微
粉体を塗付して形成した拡散縞1を有するロッド状の光
伝送体2と、この光伝送体2の両端部に嵌入される一対
の肉厚の薄い熱収縮性のあるフッ素樹脂よりなるチュー
ブ(FEP熱収縮チューブ)3と、光伝送体2の終端面2b
に位置する反射光拡散用セラミックシート4と、光伝送
体2を内部に位置させるとともに底面部が軸方向に延長
するスリット5aを切り欠かれた線状光出射スリット面5
とされた円筒鏡6と、円筒鏡6の終端部6bと係合するキ
ャップ7と、円筒鏡6の先端部6aと係合するシール部材
8と、シール部材8を介して円筒鏡6に取付けられた集
光部材9と、集光部材9に添設された反射部材10とを有
している。1 to 4 show an embodiment according to the present invention, in which the illuminating device has diffusion fringes 1 formed by applying fine powder having a high refractive index in the form of linear fine stripes in the axial direction on the outer peripheral surface. A rod-shaped optical transmission body 2 having the above, a pair of thin-walled tubes (FEP heat-shrinkable tubes) 3 made of heat-shrinkable fluororesin that are fitted into both ends of the optical transmission body 2, and the optical transmission body. 2 end face 2b
The ceramic sheet 4 for diffusing the reflected light located at the position, and the linear light emitting slit surface 5 in which the slits 5a extending in the axial direction are cut out while the optical transmission body 2 is positioned inside.
The cylindrical mirror 6, the cap 7 that engages with the end 6b of the cylindrical mirror 6, the seal member 8 that engages with the tip 6a of the cylindrical mirror 6, and the seal 6 attached to the cylindrical mirror 6 The light collecting member 9 and the reflecting member 10 attached to the light collecting member 9 are provided.
集光部材9は、略ピラミッド形状をしており、矩形状の
底面部9aは円形に開口していて、側面部9bのねじ穴9cに
ワッシャ9dを介してビス9eにより取り付けられた固形用
ばね9fによって、反射鏡付電球11の反射鏡11aが取り付
けられるようになっている。底面部9aの円形の開口の直
径は、反射鏡11aの開口の直径と略同一とされている。
集光部材9の内面は、底面部9aの円形の開口から連続す
るように円錐形状の集光面9gが形成されているととも
に、円錐の中心軸線Aと直交する軸線Bを中心軸とする
貫通孔9iが形成されている。この貫通孔9iは、円筒鏡6
を被覆した光伝送体2の中心軸が軸Bと重なるようにし
て密嵌されるように設定されている。The condensing member 9 has a substantially pyramid shape, a rectangular bottom portion 9a has a circular opening, and a solid spring attached to the screw hole 9c of the side surface portion 9b with a washer 9d by a screw 9e. The reflector 11a of the light bulb 11 with a reflector is attached by 9f. The diameter of the circular opening of the bottom surface portion 9a is substantially the same as the diameter of the opening of the reflecting mirror 11a.
A conical light-collecting surface 9g is formed on the inner surface of the light-collecting member 9 so as to be continuous from the circular opening of the bottom surface portion 9a, and penetrates with an axis B orthogonal to the central axis A of the cone as a central axis. The hole 9i is formed. This through hole 9i is used for the cylindrical mirror 6.
It is set so that the central axis of the optical transmission body 2 that covers is overlapped with the axis B and is closely fitted.
貫通孔9iと対向する斜面は切り欠かれており、楕円孔9j
が形成されている。この楕円孔9jは、集光器9の頂部に
形成されたねじ穴9kにワッシャ9lを介してビス9mにより
固定された係止部材9nと段部9oとの間で挟持された反射
部材10により遮蔽されている。The slope facing the through hole 9i is notched, and the elliptical hole 9j
Are formed. The elliptical hole 9j is formed by a reflecting member 10 sandwiched between a locking member 9n fixed to a screw hole 9k formed at the top of the condenser 9 with a screw 9m via a washer 9l and a step 9o. It is shielded.
反射部材10、軸線A、軸線B、円錐形の集光面9gとがな
す角度は、例えば第4図に示すように設定されている。
すなわち、軸線A及び軸線Bに対しては、45°の角度と
されている。また、貫通孔9i側の光線が、反射部材10に
より折曲されて光伝送体2の先端面2aの中心に向かう光
線となる際に、その光線と反射部材10とがなす角度は71
°である。さらにまた、貫通孔9iと対向する側の光線
が、反射部材10により折曲されて光伝送体2の先端面2a
の中心に向かう光線となる際に、その光線と反射部材10
とがなす角度は19°である。The angle formed by the reflecting member 10, the axis A, the axis B, and the conical light-collecting surface 9g is set as shown in FIG. 4, for example.
That is, the angle is 45 ° with respect to the axis A and the axis B. Further, when the light beam on the through hole 9i side is bent by the reflecting member 10 and becomes a light beam toward the center of the tip surface 2a of the light transmission body 2, the angle formed by the light beam and the reflecting member 10 is 71.
°. Furthermore, the light beam on the side facing the through hole 9i is bent by the reflecting member 10 to be the front end surface 2a of the optical transmission body 2.
When the light beam goes to the center of the
The angle formed by and is 19 °.
以上から明らかなように、本実施例においては、反射部
材10への入射角は19°〜71°となるように設定されてい
る。As is clear from the above, in this embodiment, the incident angle on the reflecting member 10 is set to be 19 ° to 71 °.
また、全光路(軸線A上の部位αと軸線B上の部位βと
の合計)を短くして、全体を小型化するため、反射鏡付
電球11の反射鏡11aの開口の直径と、この反射鏡付電球1
1の出光部から集光点までの集光距離(ワーキングディ
スタンス)が略等しくなるように設定されている。Further, in order to shorten the entire optical path (the total of the part α on the axis A and the part β on the axis B) to miniaturize the whole, the diameter of the opening of the reflecting mirror 11a of the light bulb with a reflecting mirror 11 and Bulb with reflector 1
The light collection distances (working distances) from the light emitting part of 1 to the light collection point are set to be substantially equal.
反射部材10は、集光面9g方向に反射面を有するようにさ
れており、この実施例にあっては、光線の熱線成分をカ
ットするためコールドミラーとされている。コールドミ
ラーは、熱線透過ミラーと呼ばれており、誘電体多層膜
によりコーティングが施こされている。The reflecting member 10 has a reflecting surface in the direction of the light collecting surface 9g, and in this embodiment, it is a cold mirror for cutting the heat ray component of the light beam. The cold mirror is called a heat ray transmitting mirror and is coated with a dielectric multilayer film.
誘電体多層膜の50%透過波長は、一般的に750nm付近に
設定されるが、入射角が本実施例のように約20°〜70°
の場合、入射角が大になるほど透過波長が短波長側へシ
フトするため、反射可視光の減少を招来する。このた
め、本実施例にあっては、蒸着により形成される誘電体
多層膜の蒸着膜各層の膜厚に一様な変化を持たせ、コー
ルドミラーに対する入射角の違いにより透過波長がシフ
トする影響を打ち消すことにより、あたかも平行光束が
入射して反射部材10のどの部位でも同一な透過波長特性
となる効果を得ている。膜厚に一様な変化を持たせるに
は、蒸着ターゲットに対し、被蒸着部材を一定角度傾斜
させるかまたは、濃淡のメッシュを有する金属網を介在
させる等の方法が用いられる。また通常の一定膜厚のコ
ールドミラーであっても、上記750nm付近の設定を800〜
850nmとすれば熱線成分の反射の影響を余り受けずに可
視反射光量を増大させることが出来る。(出願人によれ
ば、ほぼ約15〜20%の増大が見込める。)なお、符号20
は集光部材9に穿設されたねじ穴であり、ビス21をねじ
込むことにより、円筒鏡6を固定する。The 50% transmission wavelength of the dielectric multilayer film is generally set near 750 nm, but the incident angle is about 20 ° to 70 ° as in this embodiment.
In this case, the transmission wavelength shifts to the shorter wavelength side as the incident angle increases, which causes a decrease in reflected visible light. Therefore, in this embodiment, the thickness of each vapor-deposited film of the dielectric multilayer film formed by vapor deposition is uniformly changed, and the transmission wavelength shifts due to the difference in the incident angle to the cold mirror. By canceling, the effect that the parallel light flux is incident and the same transmission wavelength characteristic is obtained at any part of the reflecting member 10 is obtained. In order to make the film thickness have a uniform change, a method of inclining the member to be vapor-deposited by a certain angle with respect to the vapor deposition target or interposing a metal net having a light and shade mesh is used. Even with a normal cold mirror with a constant film thickness, the setting around 750 nm above 800
If it is set to 850 nm, the amount of visible reflected light can be increased without being significantly affected by the reflection of heat ray components. (According to the applicant, an increase of about 15 to 20% can be expected.) Note that reference numeral 20
Is a screw hole formed in the light collecting member 9, and the screw 21 is screwed in to fix the cylindrical mirror 6.
以上の構成において、反射鏡付電球11を点灯すると、光
が光伝送体2内に入射されて、スリット5aより線上の光
が放射されることになる。この際、反射鏡付電球11から
の出射光束は、集光部材9により円錐形状に集光され
て、反射部材10により反射されて90°折曲される。この
90°折曲された光束が、光伝送体2の先端面2aに入射さ
れることになる。In the above configuration, when the light bulb 11 with a reflecting mirror is turned on, the light is incident on the inside of the light transmission body 2, and the linear light is emitted from the slit 5a. At this time, the luminous flux emitted from the electric bulb 11 with a reflecting mirror is condensed into a conical shape by the condensing member 9, is reflected by the reflecting member 10, and is bent by 90 °. this
The light beam bent by 90 ° is incident on the tip surface 2a of the optical transmission body 2.
本考案は、以上説明したように構成されているので以下
に記載されるような効果を奏する。Since the present invention is configured as described above, it has the following effects.
反射鏡付電球の反射鏡の開口の直径とワーキングディス
タンスが略等しく設定されているので、集光部材を小型
軽量化出来る。Since the diameter of the opening of the reflector of the light bulb with a reflector is set to be substantially equal to the working distance, the light collecting member can be made smaller and lighter.
反射鏡付電球の反射鏡の開口の直径とワーキングディス
タンスが略等しく設定されているので、全光路が短くな
り、反射鏡付電球のフィラメントの位置ズレ及び反射鏡
付電球の反射鏡の曲率の誤差等によって生じる集光光束
のビームウェストの広がりが少なくなり、光束のしぼり
込み効率が向上し、また集光光束の入射角も損失を増大
させない範囲となる。Since the diameter of the aperture of the reflector of the bulb with a reflector and the working distance are set to be approximately equal, the total optical path is shortened, and the position deviation of the filament of the bulb with a reflector and the curvature of the reflector of the bulb with a reflector are inaccurate. The spread of the beam waist of the condensed light flux caused by the above is reduced, the efficiency of narrowing the light flux is improved, and the incident angle of the condensed light flux is in the range where the loss is not increased.
集光部材の集光面が円錐形状であるため、反射部材の形
状を小型化することができ、従って、この反射部材の製
造コストを低減できる。Since the condensing surface of the condensing member has a conical shape, the shape of the reflecting member can be downsized, and therefore the manufacturing cost of the reflecting member can be reduced.
反射部材をコールドミラーとし分光分布特性に一様な変
化を持たせるようにした場合、反射部材に対する光束入
射角の違いによる可視光線損失(反射部材後方への透過
割合)が減少するため利用光量が増大する。If the reflecting member is a cold mirror and the spectral distribution characteristics are changed uniformly, the visible light loss (transmission ratio to the rear of the reflecting member) due to the difference in the incident angle of the light flux on the reflecting member is reduced, so the amount of usable light is reduced. Increase.
図面は本考案の一実施例を示し、第1図は正面図、第2
図は第1図の側面図、第3図は分解斜視図、第4図は要
部概略説明図である。 符号の説明 1……拡散稿、2……光伝送体 3……チューブ 4……反射光拡散用セラミックシート 5……線状光出射スリット面 5a……スリット、6……円筒鏡 6a……先端部、6b……終端部 7……キャップ、8……シール部材 9……集光部材、9a……底面部 9b……側面部、9c……ねじ穴 9d……ワッシャ、9e……ビス 9f……固定用ばね、9g……集光面 9i……貫通孔、9j……楕円孔 9k……ねじ穴、9l……ワッシャ 9m……ビス、9n……係止部材 9o……段部、10……反射部材 11……反射鏡付電球、11a……反射鏡 20……ねじ穴、21……ビスThe drawings show one embodiment of the present invention, and FIG. 1 is a front view and a second view.
1 is a side view of FIG. 1, FIG. 3 is an exploded perspective view, and FIG. 4 is a schematic explanatory view of a main part. Explanation of symbols 1 ... Diffusion draft, 2 ... Optical transmission body 3 ... Tube 4 ... Reflected light diffusion ceramic sheet 5 ... Linear light emission slit surface 5a ... Slit, 6 ... Cylindrical mirror 6a. Tip part, 6b ... End part 7 ... Cap, 8 ... Seal member 9 ... Light collecting member, 9a ... Bottom part 9b ... Side part, 9c ... Screw hole 9d ... Washer, 9e .. 9f …… Fixing spring, 9g …… Focusing surface 9i …… Through hole, 9j …… Oval hole 9k …… Screw hole, 9l …… Washer 9m …… Screw, 9n …… Locking member 9o …… Step section , 10 …… Reflecting member 11 …… Reflecting light bulb, 11a …… Reflecting mirror 20 …… Screw hole, 21 …… Screw
Claims (2)
楕円面を形成する楕円の第1の焦点の位置に電球を配置
した反射鏡付電球と、 該反射鏡付電球の出射光を90°折曲する反射部材と、 前記回転楕円面からの光が前記反射部材により折曲され
て結ぶ集光点である第2の焦点の位置に配置した入射端
を有する光伝送体と、 前記反射鏡付電球の出射端から前記反射部材までの光路
を形成する円錐形状の集光部材と、からなり、 前記反射鏡付電球の開口の直径と前記反射鏡付電球の出
光部から集光点までの集光距離とを略等しくなるように
したことを特徴とする照明具。1. A reflector-equipped bulb in which a bulb is arranged at a first focal point of an ellipse forming the spheroid of a concave reflector having a spheroidal surface, and light emitted from the reflector-equipped bulb is set to 90. A reflecting member that bends; an optical transmission body that has an incident end that is disposed at a second focal point that is a converging point where the light from the spheroid is bent and connected by the reflecting member; A conical light-collecting member that forms an optical path from the emission end of the light bulb with a mirror to the reflecting member, and the diameter of the opening of the light bulb with a reflector and the light-emitting portion of the light bulb with a mirror to the light-collecting point. An illuminating device characterized in that the light collecting distances of the light emitting devices are made substantially equal to each other.
グを施して可視光のみを反射するコールドミラーとし、
蒸着膜各層の膜厚を各々連続的に変化させ、前記コール
ドミラーに対する入射角の違いにより透過波長がシフト
する影響を打ち消すようにしたことを特徴とする実用新
案登録請求の範囲第1項に記載の照明具。2. The reflection member is a cold mirror that is coated with a dielectric multilayer film and reflects only visible light.
Claim 1 of the utility model characterized in that the effect of shifting the transmission wavelength due to the difference in the incident angle with respect to the cold mirror is canceled out by continuously changing the film thickness of each layer of the vapor deposition film. Lighting equipment.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1989107960U JPH0743848Y2 (en) | 1989-09-14 | 1989-09-14 | Lighting equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1989107960U JPH0743848Y2 (en) | 1989-09-14 | 1989-09-14 | Lighting equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0346911U JPH0346911U (en) | 1991-04-30 |
| JPH0743848Y2 true JPH0743848Y2 (en) | 1995-10-09 |
Family
ID=31656625
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1989107960U Expired - Lifetime JPH0743848Y2 (en) | 1989-09-14 | 1989-09-14 | Lighting equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0743848Y2 (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2341815A1 (en) * | 1976-02-23 | 1977-09-16 | Nath Guenther | DEVICE EMITTING RADIATION IN THE SPECTRAL ULTRAVIOLET AREA |
| JPS58192606U (en) * | 1982-06-16 | 1983-12-21 | 株式会社メドス研究所 | Light introduction device for optical fiber bundle for lighting |
-
1989
- 1989-09-14 JP JP1989107960U patent/JPH0743848Y2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0346911U (en) | 1991-04-30 |
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| Date | Code | Title | Description |
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| EXPY | Cancellation because of completion of term |