JPH09222580A - Converging reflector - Google Patents

Converging reflector

Info

Publication number
JPH09222580A
JPH09222580A JP8029105A JP2910596A JPH09222580A JP H09222580 A JPH09222580 A JP H09222580A JP 8029105 A JP8029105 A JP 8029105A JP 2910596 A JP2910596 A JP 2910596A JP H09222580 A JPH09222580 A JP H09222580A
Authority
JP
Japan
Prior art keywords
reflector
shape
light
condensing
illuminated
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
JP8029105A
Other languages
Japanese (ja)
Inventor
Keisuke Mitani
圭輔 三谷
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.)
Sharp Corp
Original Assignee
Sharp Corp
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 Sharp Corp filed Critical Sharp Corp
Priority to JP8029105A priority Critical patent/JPH09222580A/en
Publication of JPH09222580A publication Critical patent/JPH09222580A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To provide a converging reflector improved incolor evenness and luminance evenness and having high convergent efficiency of irradiation light. SOLUTION: A reflection surface consists of division surfaces 11 -14 ... in the rotational (peripheral) direction and the axial (concentric circular) direction. The reference shape of the reflector is in an elliptic surface shape, and respective reflection surfaces constituting the reflector are constituted having a certain tilt for the reference elliptic shape, and converging positions are set by the tilts of respective reflection surfaces. A converging range being a circle generally lighting on a surface to be irradiated is set in different points in convergent positions in the respective rotational direction, and a lighting range in the surface to be irradiated is able to be converged so as to approach no a square shape.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、集光リフレクタに
関し、より詳細には、液晶プロジェクタ等の各種光学系
に用いられ、投射特性を向上させる集光リフレクタに関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a condensing reflector, and more particularly to a condensing reflector used in various optical systems such as liquid crystal projectors to improve projection characteristics.

【0002】[0002]

【従来の技術】従来のこの種の集光リフレクタの例が図
7に示され、同図には、反射面形状を放物形状の回転面
とした集光リフレクタが示されている。図7において、
光源12から発せられた光は、集光リフレクタ11によ
り反射されて被照射面13に照射される。この時、被照
射面13での照度分布は、ランプの光源12の発光分布
及び集光リフレクタ11の形状等により、一般に、図7
の右側に示したように中央部が明るく、周辺部が暗い照
度分布の特性となる。また、集光リフレクタ11の反射
面形状が回転対称形状となっていることより、被照射面
での照明範囲の形状は、図8に示すように円形となる。
2. Description of the Related Art An example of a conventional light collecting reflector of this type is shown in FIG. 7, which shows a light collecting reflector having a paraboloidal rotating surface as a reflecting surface. In FIG.
The light emitted from the light source 12 is reflected by the condensing reflector 11 and applied to the illuminated surface 13. At this time, the illuminance distribution on the illuminated surface 13 is generally shown in FIG. 7 depending on the light emission distribution of the light source 12 of the lamp, the shape of the condenser reflector 11, and the like.
As shown on the right side of the figure, the illuminance distribution has a characteristic that the central part is bright and the peripheral part is dark. Further, since the reflecting surface of the condensing reflector 11 has a rotationally symmetrical shape, the shape of the illumination range on the illuminated surface is circular as shown in FIG.

【0003】また、従来の例として、図9に示されるよ
うに、回転放物面体の異なる部分に対応する複数の輪帯
形状の鏡面から成る集光リフレクタ(特開平2−259
713号公報)を挙げることができる。図9で、リフレ
クタは、n個の輪帯形状鏡面111〜11nから成る集光
装置で、各輪帯形状鏡面は、輪帯の中心軸を一致させた
構造を持つ。このリフレクタでは、鏡面111の焦点位
置F1に対して、鏡面112の焦点位置F2が内側へ、か
つ、鏡面112の焦点位置F2に対し、鏡面11nの焦点
位置Fnが内側にくるように、鏡面111,112,11n
を配置している。このことにより、多少は、被照射面で
の照度分布(中心の照度に対する周辺の照度)を改善す
ることは出来、また、光源の発光部の色むら及び照度む
らを低減する効果を有している。ただし、この例の場
合、反射鏡面111〜11nが輪帯状になっているため、
上記の照度分布及び色むらについても、同心円状に発生
する分布,むらについては改善できない為、完全に改善
することは出来ない。また、被照射面での照明範囲の形
状は、前記の例と同様に円形となり、この点における集
光効率の低下は改善できていない。
As a conventional example, as shown in FIG. 9, a condensing reflector composed of a plurality of ring-shaped mirror surfaces corresponding to different portions of a paraboloid of revolution (Japanese Patent Laid-Open No. 2-259).
No. 713). In FIG. 9, the reflector is a condensing device composed of n ring-shaped mirror surfaces 11 1 to 11 n , and each ring-shaped mirror surface has a structure in which the center axes of the ring zones are aligned. In this reflector, with respect to the focal position F 1 of the mirror 11 1, the focal position F 2 the mirror 11 2 are inward, and, with respect to the focal position F 2 the mirror 11 2, the focus position F n of the mirror surface 11 n Mirror surfaces 11 1 , 11 2 , 11 n to come inside
Has been arranged. As a result, the illuminance distribution on the surface to be illuminated (illuminance in the periphery with respect to the illuminance in the center) can be improved to some extent, and it also has the effect of reducing unevenness in color and unevenness in illuminance of the light emitting section of the light source. There is. However, in the case of this example, since the reflecting mirror surfaces 11 1 to 11 n are ring-shaped,
Concerning the above-mentioned illuminance distribution and color unevenness, it is not possible to completely improve the distribution and unevenness that occur in a concentric circle shape. Further, the shape of the illumination range on the illuminated surface is circular as in the above example, and the reduction of the light collection efficiency at this point cannot be improved.

【0004】[0004]

【発明が解決しようとする課題】上述したところの従来
のこの種の集光リフレクタの技術では、被照射面での照
度分布は、中央が明るく周辺が暗い特性となり、均一な
照度特性を得ることが出来ない。また、通常、光源の発
光部には、色むら及び輝度むらがある為、この色むら,
輝度むらが被照射面に現れてしまう。また、被照射面で
の照明範囲が円形である(図8、参照)ため、被照射面
が方形である場合が通常である画面において、照射光が
有効に利用されず(図8に示すように、照射範囲の円形
と被照射面の方形の形状の違いにより生じる斜線部
分)、集光効率を低下させる大きな要因となる。本発明
は、このような従来技術における問題点に鑑みてなされ
たもので、色むら及び輝度むらが改善され、照射光の集
光効率の高い集光リフレクタを提供することをその課題
とする。
SUMMARY OF THE INVENTION In the conventional technique of this kind of condensing reflector as described above, the illuminance distribution on the illuminated surface has a characteristic that the center is bright and the periphery is dark, and uniform illuminance characteristics are obtained. I can't. Further, since the light emitting portion of the light source usually has color unevenness and brightness unevenness, the color unevenness,
Brightness unevenness appears on the illuminated surface. In addition, since the illuminated area on the illuminated surface is circular (see FIG. 8), the illuminated light is not effectively used on the screen where the illuminated surface is usually rectangular (see FIG. 8). In addition, the shaded area caused by the difference between the circular shape of the irradiation range and the rectangular shape of the surface to be irradiated) is a major factor that reduces the light collection efficiency. The present invention has been made in view of the above problems in the prior art, and an object of the present invention is to provide a light condensing reflector with improved color non-uniformity and brightness non-uniformity and high irradiation light condensing efficiency.

【0005】[0005]

【課題を解決するための手段】請求項1の発明は、反射
面形状を楕円回転面とする集光リフレクタにおいて、基
準の一楕円回転面を複数個の面に分割して得た分割面に
ついて前記基準面に対する傾きを該分割面個々に変化さ
せ、変化後に形成される面により反射面を構成するよう
にし、分割面個々の集光位置を変えることにより、被照
射面での照度分布の形状を任意に設計可能とするもので
ある。
According to a first aspect of the present invention, in a condensing reflector having a reflecting surface shape as an elliptical rotation surface, a reference split surface obtained by dividing one elliptical rotation surface into a plurality of surfaces. By changing the inclination with respect to the reference plane for each of the divided surfaces so that the surface formed after the change constitutes a reflecting surface, and changing the condensing position of each of the divided surfaces, the shape of the illuminance distribution on the irradiated surface Can be arbitrarily designed.

【0006】請求項2の発明は、請求項1の発明におい
て、前記複数個の面の分割は、基準の一楕円回転面の回
転(周)方向に行うようにし、被照射面での照射分布形
状の設計をより容易にするものである。
According to a second aspect of the invention, in the first aspect of the invention, the plurality of surfaces are divided in the rotation (circumferential) direction of the reference elliptical rotation surface, and the irradiation distribution on the surface to be irradiated is determined. This makes it easier to design the shape.

【0007】請求項3の発明は、請求項1又は2の発明
において、前記複数個の面の分割は、基準の一楕円回転
面の軸(同心円)方向に行うようにし、被照射面での照
射分布形状の設計をより容易にするものである。
According to a third aspect of the present invention, in the first or second aspect of the present invention, the plurality of surfaces are divided in the direction of the axis (concentric circle) of the reference elliptical rotation surface, and the surface to be irradiated is This makes it easier to design the irradiation distribution shape.

【0008】請求項4の発明は、請求項1ないし3のい
ずれかの発明において、前記分割面の傾きを、被照射面
の所定の形状に対応して集光するように変化させるよう
にし、基準の楕円回転面によると、照明範囲が円形とな
るものを、通常の矩形の画面に対応するように照射分布
を変えて集光効率を上げることを可能とするものであ
る。
According to a fourth aspect of the present invention, in any one of the first to third aspects of the present invention, the inclination of the divided surface is changed so as to focus light in accordance with a predetermined shape of the illuminated surface, According to the reference elliptical rotation surface, it is possible to improve the light collection efficiency by changing the irradiation distribution so that the illumination range becomes circular and corresponds to a normal rectangular screen.

【0009】[0009]

【発明の実施の形態】図1は、本発明の集光リフレクタ
の実施形態を示す図である。この実施形態では、図1
(B)に示すように、集光リフレクタの反射面を回転
(周)方向及び軸(同心円)方向にカットしたそれぞれ
の面に分割している。なお、この分割方法については、
この他に、各分割面を同一形状で分割する方法、周方向
のみ分割、軸方向のみ分割する方法等が考えられる。そ
して、このリフレクタの基本形状は、回転楕円面形状を
している。それは、図1(A)の二点鎖線で示した曲線
が楕円面形状となるということで、リフレクタを構成す
る各反射面は、この基準の楕円形状よりある傾きを持っ
て構成されている。図2に、基準の回転楕円面形状リフ
レクタ1′での光の集光状態を示す。図2では、光源2
より出た光は、集光リフレクタ1′により反射され、被
照射面3の1点に集まる。本発明の例では、この基準の
回転楕円面形状リフレクタ面を分割し、その分割された
反射面にそれぞれ異なった傾きをつけることにより、被
照射面での光の集光位置を自由に設計することを特徴と
している。
1 is a diagram showing an embodiment of a light collecting reflector of the present invention. In this embodiment, FIG.
As shown in (B), the reflecting surface of the condenser reflector is divided into respective surfaces cut in the rotational (circumferential) direction and the axial (concentric) direction. In addition, about this division method,
Other than this, a method of dividing each divided surface with the same shape, a method of dividing only in the circumferential direction, a method of dividing only in the axial direction, and the like can be considered. The basic shape of this reflector is a spheroidal surface. That is, the curve indicated by the chain double-dashed line in FIG. 1 (A) has an elliptical shape, so that each reflecting surface forming the reflector is formed with a certain inclination from this reference elliptical shape. FIG. 2 shows a light collecting state of the reference spheroidal reflector 1 '. In FIG. 2, the light source 2
The emitted light is reflected by the condenser reflector 1 ′ and gathers at one point on the illuminated surface 3. In the example of the present invention, the reference spheroidal reflector surface is divided, and the divided reflecting surfaces are provided with different inclinations, whereby the light condensing position on the illuminated surface is freely designed. It is characterized by that.

【0010】このリフレクタの例を光軸を通る断面で見
た図を図3に示す。図2においては、光源2より出た光
は、リフレクタの各反射面で反射して被照射面3で各面
とも一点に集光するが、本発明の実施形態では、各反射
面の傾きを各々変えているため、その集光位置は、回転
楕円面リフレクタの場合と異なり、各反射面の傾きに応
じた点に集光することとなる。図3では、各反射面
1,12,13及び14で反射した光は、被照射面の各位
置,,,に集光することとなる。図4には、この
被照射面での集光位置を各点として表わして、その分布
が示されている。なお、図4中の,,及びは、図
3の同符号に対応し、それぞれ図1(B)及び図3の反
射面11,12,13及び14の各反射面からの集光位置を
示すものである。図4に示される集光位置は、各反射面
の傾きによって設定できる。従って、この集光位置を被
照射面の集光範囲の形状に従い(この例の場合は、方形
形状となっている)、各回転方向で集光位置を異なる点
とし、結果的に被照射面での照明範囲を方形形状に集光
するようにできる。また、各回転方向の集光位置は、被
照射面での照度分布の要望にあわせ、その位置間隔を設
計することにより、被照射面の照度分布を自由に設計す
ることが出来る。設計によって被照射面での照度分布を
均一にすることもできる。
FIG. 3 shows a view of an example of this reflector as seen in a cross section passing through the optical axis. In FIG. 2, the light emitted from the light source 2 is reflected by each reflection surface of the reflector and condensed on each surface of the irradiated surface 3 at one point, but in the embodiment of the present invention, the inclination of each reflection surface is changed. Since each is changed, the focusing position is different from the case of the spheroidal reflector, and the focusing position is to a point corresponding to the inclination of each reflecting surface. In FIG. 3, the light reflected by each of the reflecting surfaces 1 1 , 1 2 , 1 3 and 1 4 is condensed at each position of the illuminated surface. In FIG. 4, the light collection positions on the illuminated surface are represented as points and the distribution thereof is shown. Note that, and in FIG. 4 correspond to the same reference numerals in FIG. 3, and are collected from the reflecting surfaces 1 1 , 1 2 , 1 3 and 1 4 in FIGS. 1B and 3 respectively. It shows the light position. The condensing position shown in FIG. 4 can be set by the inclination of each reflecting surface. Therefore, according to the shape of the condensing range of the irradiated surface (in this example, the condensing position is rectangular), the condensing position is different in each rotation direction, and as a result, the irradiated surface is changed. It is possible to focus the illumination range at to a rectangular shape. Further, the condensing position in each rotation direction can be designed freely by designing the position interval according to the demand of the illuminance distribution on the illuminated surface. The illuminance distribution on the illuminated surface can be made uniform by design.

【0011】以上の説明は、基本的に光源は点光源であ
るとして説明したが、実際には、発光源は完全な点光源
ではなく、ある程度の大きさを持つ。図5は、ある程度
の大きさを持つ発光源により各反射面で反射した光が、
被照射面でどのように照射されるかを示す図である。な
お、図5中の,,及びは、図4の同符号に相当す
る。図5に示すように、実際には、被照射面では、各面
で反射した光が重なりながら照射されることとなるが、
この結果に示されるような被照射面分布も上記したとこ
ろの反射面の各傾きを変えることにより、均一化が行わ
れるように対応することが出来る。次に、各反射面の傾
きの付け方についての一例を示す。図6は、楕円面を焦
点(光源位置)を中心に回転させ、傾かせることを説明
する図である。図6において、焦点(光源位置)を中心
にして、実線で示す楕円回転面及び光線をθ回転させた
後の位置及び光線を破線で示す。また、その他の傾け方
としては、各反射面の中心部を回転軸として回転させる
方法を用いてもよい。
In the above description, the light source is basically a point light source, but in reality, the light emitting source is not a perfect point light source but has a certain size. In FIG. 5, the light reflected by each reflecting surface by the light emitting source having a certain size is
It is a figure which shows how it is irradiated by the to-be-irradiated surface. Note that ,, and in FIG. 5 correspond to the same symbols in FIG. As shown in FIG. 5, actually, on the illuminated surface, the light reflected by each surface is emitted while overlapping.
The distribution of the surface to be illuminated as shown in this result can also be dealt with so as to be uniform by changing the inclinations of the reflecting surface as described above. Next, an example of how to attach the inclination of each reflecting surface is shown. FIG. 6 is a diagram for explaining that the elliptical surface is rotated and tilted about a focus (light source position). In FIG. 6, the elliptical surface of rotation indicated by the solid line and the position and light ray after the light ray is rotated by θ around the focal point (light source position) are indicated by broken lines. Further, as another tilting method, a method of rotating the center of each reflecting surface as a rotation axis may be used.

【0012】[0012]

【発明の効果】請求項1の発明によると、楕円回転面を
分割して求めた個々の反射面の傾きを基準面から変化,
調整させて、従来の回転対称形状の反射面を持つ集光リ
フレクタにより、生じていた色むら及び輝度むらをなく
すことができ、被照射面における照明範囲についても、
従来の円形から任意の分布を得るように変えることがで
きる。
According to the invention of claim 1, the inclination of each reflecting surface obtained by dividing the elliptical surface of revolution is changed from the reference plane,
It is possible to eliminate the color unevenness and brightness unevenness that have been caused by the condensing reflector having the conventional rotationally symmetrical reflecting surface, and the illumination range on the illuminated surface can also be adjusted.
It can be changed to obtain any distribution from the conventional circle.

【0013】請求項2又は3の発明によると、上記請求
項1の効果に加えて、分割面を楕円回転面の幾何学的性
質に合わせて分割することにより、設計が容易で作りや
すい反射面をもつ当該リフレクタが提供される。
According to the invention of claim 2 or 3, in addition to the effect of claim 1, by dividing the dividing surface in accordance with the geometrical properties of the elliptical surface of revolution, the reflecting surface is easy to design and easy to make. The reflector with is provided.

【0014】請求項4の発明によると、上記請求項1な
いし3の効果に加えて、被照射面上の照明範囲として、
例えば、矩形といった所定の形状にすることが要求され
る場合にも、分割された楕円回転面とその傾きの調整に
より、容易にその要求に応えることが可能となる。
According to the invention of claim 4, in addition to the effects of claims 1 to 3, as an illumination range on the surface to be illuminated,
For example, even when a predetermined shape such as a rectangle is required, it is possible to easily meet the request by adjusting the divided elliptical rotation surface and its inclination.

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

【図1】本発明の回転楕円面形状の反射面を有する集光
リフレクタの実施形態における断面図(A)と正面図
(B)を示すものである。
FIG. 1 is a sectional view (A) and a front view (B) of an embodiment of a light collecting reflector having a spheroidal reflecting surface of the present invention.

【図2】基準の楕円面リフレクタでの集光状態を示す図
である。
FIG. 2 is a diagram showing a light collecting state at a reference ellipsoidal reflector.

【図3】本発明の集光リフレクタの一実施形態の断面図
を作用光とともに示す図である。
FIG. 3 is a diagram showing a cross-sectional view of an embodiment of a light collecting reflector of the present invention together with working light.

【図4】本発明の集光リフレクタの一実施形態による被
照射面の集光状態を概念的に示す図である。
FIG. 4 is a diagram conceptually showing a condensing state of a surface to be illuminated by an embodiment of a condensing reflector of the present invention.

【図5】本発明の集光リフレクタの一実施形態による被
照射面の集光状態を説明するための図である。
FIG. 5 is a diagram for explaining a light collecting state of an illuminated surface according to an embodiment of a light collecting reflector of the present invention.

【図6】本発明の集光リフレクタの一実施形態における
反射面の傾け方を説明するための図である。
FIG. 6 is a diagram for explaining how to incline a reflecting surface in an embodiment of a light collecting reflector of the present invention.

【図7】反射面形状を放物形状の回転面としたこの種の
集光リフレクタの従来例を示す図である。
FIG. 7 is a diagram showing a conventional example of a condensing reflector of this type in which a reflecting surface shape is a paraboloidal rotating surface.

【図8】従来の被照射面での照明範囲を示す図である。FIG. 8 is a diagram showing a conventional illumination range on a surface to be illuminated.

【図9】回転放物面体を反射面とする集光リフレクタの
従来例を示す図である。
FIG. 9 is a diagram showing a conventional example of a light collecting reflector having a rotating paraboloid as a reflecting surface.

【符号の説明】[Explanation of symbols]

1′…回転楕円面形状リフレクタ、11,12,13,14
…反射面、2…光源、3…被照射面、11…集光リフレ
クタ、111〜11n…輪帯形状鏡面、12…光源、13
…被照射面、F1〜Fn…焦点位置。
1 '... spheroidal reflector 1 1 , 1 2 , 1 3 , 1 4
... Reflecting surface, 2 ... Light source, 3 ... Irradiation surface, 11 ... Condensing reflector, 11 1 to 11 n ... Ring-shaped mirror surface, 12 ... Light source, 13
... illuminated surface, F 1 to F n ... focal position.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 反射面形状を楕円回転面とする集光リフ
レクタにおいて、基準の一楕円回転面を複数個の面に分
割して得た分割面について前記基準面に対する傾きを該
分割面個々に変化させ、変化後に形成される面により反
射面を構成するようにしたことを特徴とする集光リフレ
クタ。
1. A condensing reflector having a reflecting surface shape as an elliptical rotation surface, wherein a reference surface is tilted with respect to each of the division surfaces obtained by dividing a reference one elliptical rotation surface into a plurality of surfaces. A condensing reflector characterized in that a reflecting surface is constituted by a surface formed after the change.
【請求項2】 前記複数個の面の分割は、基準の一楕円
回転面の回転(周)方向に行うようにしたことを特徴と
する請求項1記載の集光リフレクタ。
2. The condensing reflector according to claim 1, wherein the plurality of surfaces are divided in a rotation (circumferential) direction of a reference one elliptical rotation surface.
【請求項3】 前記複数個の面の分割は、基準の一楕円
回転面の軸(同心円)方向に行うようにしたことを特徴
とする請求項1又は2記載の集光リフレクタ。
3. The condensing reflector according to claim 1, wherein the plurality of surfaces are divided in a direction of an axis (concentric circle) of a reference one elliptical rotation surface.
【請求項4】 前記分割面の傾きを、被照射面の所定の
形状に対応して集光するように変化させることを特徴と
する請求項1ないし3のいずれかに記載の集光リフレク
タ。
4. The condensing reflector according to claim 1, wherein the inclination of the divided surface is changed so as to condense light according to a predetermined shape of the irradiation surface.
JP8029105A 1996-02-16 1996-02-16 Converging reflector Pending JPH09222580A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8029105A JPH09222580A (en) 1996-02-16 1996-02-16 Converging reflector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8029105A JPH09222580A (en) 1996-02-16 1996-02-16 Converging reflector

Publications (1)

Publication Number Publication Date
JPH09222580A true JPH09222580A (en) 1997-08-26

Family

ID=12267067

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8029105A Pending JPH09222580A (en) 1996-02-16 1996-02-16 Converging reflector

Country Status (1)

Country Link
JP (1) JPH09222580A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7954963B2 (en) 2007-03-28 2011-06-07 Seiko Epson Corporation Light source and projector

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7954963B2 (en) 2007-03-28 2011-06-07 Seiko Epson Corporation Light source and projector

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