JPH01267601A - Condenser lens - Google Patents

Condenser lens

Info

Publication number
JPH01267601A
JPH01267601A JP9576288A JP9576288A JPH01267601A JP H01267601 A JPH01267601 A JP H01267601A JP 9576288 A JP9576288 A JP 9576288A JP 9576288 A JP9576288 A JP 9576288A JP H01267601 A JPH01267601 A JP H01267601A
Authority
JP
Japan
Prior art keywords
light
reflecting surface
incident
discharge tube
photographing range
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
JP9576288A
Other languages
Japanese (ja)
Inventor
Satoru Ishizaka
哲 石坂
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.)
Konica Minolta Inc
Original Assignee
Konica Minolta Inc
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 Konica Minolta Inc filed Critical Konica Minolta Inc
Priority to JP9576288A priority Critical patent/JPH01267601A/en
Publication of JPH01267601A publication Critical patent/JPH01267601A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve the light condensing efficiency of an electronic flash device, etc., by forming a reflecting surface which totally reflects the light from a light source in a photographing range to the edge of the lens and forming an incident face which guides the light from the light source to the reflecting surface in the position adjacent to said reflecting surface. CONSTITUTION:The reflecting surface S2 which totally reflects the light form an electric discharge tube 1 to the inside of the photographing range is provided to the edge of the condenser lens and the incident surface S1 for guiding the light from the discharge tube to the reflecting surface S2 is provided in the position adjacent to the reflecting surface S2. The incident surface S1 has the inclination reverse from the refracting face (Fresnel face) of the condenser lens 4 and projects the light from the discharge tube 1 to the reflecting surface S2 at such an angle at which the light reflects totally on the reflecting surface S2. Namely, the ray emitted from near the center of the discharge tube 1 and enters the incident surface S1 is so refracted as to be reflected at a suitable incident angle by the reflecting surface S2 and is directed to the photographing range after the light is reflected by the reflecting surface S2. The light which is heretofore reflected by a reflecting shade near the edge of the condenser lens 4 and escapes to the outside of the photographing range can be directed to the inside of the photographing range and, therefore, the condensing efficiency of the electronic flash device, etc., is improved.

Description

【発明の詳細な説明】 (産業上の利用分野) 、(発明はカメラのストロボ装置などに用いられる集光
レンズに関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Field of Application) The present invention relates to a condenser lens used in a strobe device of a camera, etc.

(従来技術) 小型カメラのストロボ装置は、一般に円筒状の放電管と
、その放電管を照射口を残して取り囲む反射傘とから構
成され、放電管からの光は直接。
(Prior Art) A strobe device for a small camera generally consists of a cylindrical discharge tube and a reflector that surrounds the discharge tube leaving an irradiation opening, and the light from the discharge tube is directly transmitted.

または反射傘に反射した後照射口から被写体に向けて照
射される。照射口は長方形状てあり、その短辺方向には
1反射傘だけでもある程度の集光作用かあるか、長辺方
向に関しては1反射傘のみにより集光は困難であるため
、照射[1にレンズを配にして集光を行うのか普通であ
る。集光レンズとしてはフレネルレンズかしばしば用い
られ、フレネルレンズの溝形状は直線状てあったり1輪
帯状であったりする。
Alternatively, after being reflected by a reflective umbrella, the light is irradiated from the irradiation port toward the subject. The irradiation port has a rectangular shape, and in the direction of the short side, one reflective umbrella has a certain amount of light focusing effect, and in the long side direction, it is difficult to collect light with only one reflective umbrella, so the irradiation [1] It is normal to use lenses to collect light. A Fresnel lens is often used as a condensing lens, and the groove shape of the Fresnel lens may be linear or ring-shaped.

ところか、このような集光レンズにおいては。However, with a condensing lens like this.

発光部(放電管)からレンズの屈折面までの距層か長辺
方向の寸法に比べて短いため、フレネル面を用いて屈折
力を強くしても、発散する光を画角内へ集めることので
きる範囲には限界かあった。
The distance layer from the light emitting part (discharge tube) to the refractive surface of the lens is short compared to the long side dimension, so even if you use a Fresnel surface to strengthen the refractive power, the diverging light cannot be focused within the angle of view. There were limits to what he could do.

すなわち、第4図に示すように、放′it管lの中心付
近から発する光線R1〜R5を考えた場合、山内へ向か
うのはR1,R2の2本のみである。
That is, as shown in FIG. 4, when considering the light rays R1 to R5 emitted from the vicinity of the center of the radiation tube 1, only two, R1 and R2, head toward the interior of the mountain.

R3は集光レンズ2のフレネル面の屈折力が不足してい
るために画角外へ向かい、R4は屈折作用面ではなく、
壁2aにあたって拡散してしまう。
R3 goes outside the angle of view because the Fresnel surface of the condensing lens 2 lacks refractive power, and R4 is not a refractive surface.
It hits the wall 2a and spreads.

また、反射傘3の側面で反射した光線R,は、フレネル
面2bか逆に発散作用を持つ方向に向いているため、や
はり画伯外へ向かう、ここで、フレネル面の屈折力を強
く1れば、光線Rコを画角内へ向けることもてきるか、
rうする゛と光線かフレネル作用面より壁の部分に入射
する割合か多くなり、効果は期待てきない。
In addition, since the light ray R reflected on the side surface of the reflective umbrella 3 is directed toward the Fresnel surface 2b or in a direction that has a diverging effect, it also goes outside the artist, where the refractive power of the Fresnel surface is strongly increased. For example, is it possible to direct the light ray R into the angle of view?
If you do so, more of the rays will be incident on the wall than on the Fresnel action surface, and the effect will not be as expected.

(発1!1の目的および構成) 、(発fjJは1.記の点にかんがみてなされたもので
、ストロボ装置などの集光効−4にを向−[、させるこ
とを目的とし、かかる目的を連1&するため、集光レン
ズの縁部に光源からの光な画角内へ全反射させる反射面
を形成するとともに、この反射面と隣合う位置に、光源
からの光を反射面へ導く入射面を形成するように構成し
た。
(Purpose and configuration of 1!1) , (The purpose of 1.1 is that fjJ was created in view of the points mentioned in 1., and its purpose is to improve the light condensing effect of strobe devices, etc.). In order to achieve this goal, a reflective surface is formed at the edge of the condensing lens that completely reflects the light from the light source within the angle of view, and a reflective surface is placed adjacent to this reflective surface to direct the light from the light source to the reflective surface. It was configured to form an incident surface that guides the light.

(−を二、ら−色例) 以ド未発+!1を図面に基づいて説IJiする。(-2, ra-color example) More unreleased +! 1 will be explained based on the drawings.

第1L!Jは未発IJIによる集光レンズ′の−・実施
例の断面1i1であり、図中、第4 [Aと回し構成部
分には回し参照番号を付して示しである。
1st L! J is a cross section 1i1 of the condensing lens '--Example due to unreleased IJI.

IAにおいて、4はフレネルしンズを用いた集光レンズ
であり、集光レンズ4の中心付近には従来と同様(第4
14参り)の長辺方向に屈折力をi−、) −1)直線
状フレネル面か形成されている。しかlノ、集光レンズ
4の縁部には放電管lからの光を画角内へ全反射させる
反射面S2と、この反射面S2と隣合う位置に放′屯管
からの光を反射面S2に導くための入射面Slか形成さ
れている。入射面S。
In the IA, reference numeral 4 is a condenser lens using Fresnel lenses, and near the center of the condenser lens 4 there is a condenser lens (the fourth
14) The refractive power is i- in the long side direction,) -1) A straight Fresnel surface is formed. However, at the edge of the condensing lens 4, there is a reflecting surface S2 that totally reflects the light from the discharge tube l into the angle of view, and at a position adjacent to this reflecting surface S2, the light from the discharge tube is reflected. An incident surface Sl is formed for guiding the light to the surface S2. Incidence surface S.

は集光レンズ4の屈折面(フレネル面)と逆の傾きを4
シし、光か反射面S2て全反射するような角で、放’i
lr、管lからの光を反射面S2 ”\に射さt1′る
is the inclination opposite to the refractive surface (Fresnel surface) of the condenser lens 4.
The light is emitted at a corner where the light is totally reflected by the reflective surface S2.
lr, the light from the tube l is emitted onto the reflecting surface S2''\t1'.

さ”C1以]二のように構成すれば1、尤m、R,−R
4は第4図と同様の経路を通り、光線R、およびR2の
みか画角内へ向かう、しか)ノ、本発明では集光レンズ
4の縁部に形成された反射rniS2”rの全反射を利
用するため、光1IaR,,は画角内・\向かう。すな
わち、放電IrFlの中心村山−から発1ッて入射面S
1に入射した光線は反射面S2でi+! 当な入射角で
反射されるように屈折され、反射面S2て全反射された
後画角内へ向かう。ここては、発光源を放電管1の中心
に仮定1ノだか、中心からすれた場合ても、光線R6と
同様の角度で入射面S1に入射するものは、画角内に向
かうことかてきる。さらに、光線R6のように、1度後
方で反射した光線も利用できることも考えれば1本発明
による効果は大きい。
If configured as shown in 2, 1, likely m, R, -R
4 passes through the same path as in FIG. In order to utilize
The light beam incident on 1 becomes i+! on the reflecting surface S2. It is refracted so as to be reflected at a proper incident angle, and after being totally reflected by the reflecting surface S2, it heads into the field of view. Here, assuming that the light source is located at the center of the discharge tube 1, even if the light source deviates from the center by one angle, the light that is incident on the incident surface S1 at the same angle as the light ray R6 will be directed within the angle of view. Ru. Furthermore, considering that a light beam reflected once backward, such as the light beam R6, can also be used, the effects of the present invention are significant.

7fS2[Jは集光レンズ4の右縁部の部分拡大図であ
り、入射面S1と反射面S2のなす角をθとすると、角
θは次の条件を:島だすのか好ましい。
7fS2[J is a partial enlarged view of the right edge of the condensing lens 4. If the angle between the incident surface S1 and the reflective surface S2 is θ, the angle θ satisfies the following conditions: It is preferable to make an island.

0<50’ この条件をこえてθか小さくなると放電管lからの光は
ほぼ争直に入射面S、に入射し反射面S2への入射角か
小さくなる。そのため全反射後の光はi 3 fMに示
すように画角外へ向ってしまう9(発明の効果) 以り説明したように、本発明によれば、集光レンズの縁
部に光源からの光を画角内へ全反射させる反射面を形成
するとともに、この反射面と隣合う位置に、光源からの
光を反射面へ導く入射面を形;表するようにatJtシ
たことにより、従来は集光レンズの縁部付近の反射傘に
反射して画角外へ逃げCいた光を、画角内へ向けること
ができるのて、ストロボ装置なとの集光効率を向トさせ
ろことかできる。
0<50' When θ becomes smaller beyond this condition, the light from the discharge tube I enters the incident surface S almost directly, and the angle of incidence on the reflecting surface S2 becomes smaller. Therefore, the light after total reflection goes outside the angle of view as shown by i 3 fM 9 (Effects of the Invention) As explained above, according to the present invention, the light from the light source is attached to the edge of the condenser lens. By forming a reflective surface that totally reflects the light within the angle of view, and by forming an incident surface adjacent to this reflective surface that guides the light from the light source to the reflective surface, it is possible to The light that was reflected by the reflector near the edge of the condensing lens and escaped outside the field of view can be directed into the field of view, improving the light collection efficiency of a strobe device. can.

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

第1図は本発明による集光レンズの一実施例を示す断面
図、第211はレンズの右縁部の部分拡大(A、第3図
は集光レンズの他の例を示す断面図、第4図は従来の集
光レンズを示す断面図である。 l・・・放電管、2.4・・・集光レンズ、3・・・反
射傘、SI・−・入射面、S2・・・反射面
FIG. 1 is a cross-sectional view showing one embodiment of the condensing lens according to the present invention, FIG. 211 is a partial enlargement of the right edge of the lens (A), FIG. Fig. 4 is a sectional view showing a conventional condensing lens. 1...Discharge tube, 2.4...Condensing lens, 3...Reflector, SI...Incidence surface, S2... reflective surface

Claims (1)

【特許請求の範囲】[Claims] 光源からの光を画角内へ集光するための屈折面を有する
集光レンズにおいて、レンズの縁部に光源からの光を画
角内へ全反射させる反射面を形成するとともに、この反
射面と隣合う位置に、光源からの光を前記反射面へ導く
入射面を形成したことを特徴とする集光レンズ。
In a condensing lens having a refractive surface for condensing light from a light source into an angle of view, a reflective surface is formed at the edge of the lens to totally reflect light from a light source into an angle of view, and this reflective surface A condensing lens characterized in that an incident surface for guiding light from a light source to the reflecting surface is formed at a position adjacent to the condensing lens.
JP9576288A 1988-04-20 1988-04-20 Condenser lens Pending JPH01267601A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9576288A JPH01267601A (en) 1988-04-20 1988-04-20 Condenser lens

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9576288A JPH01267601A (en) 1988-04-20 1988-04-20 Condenser lens

Publications (1)

Publication Number Publication Date
JPH01267601A true JPH01267601A (en) 1989-10-25

Family

ID=14146500

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9576288A Pending JPH01267601A (en) 1988-04-20 1988-04-20 Condenser lens

Country Status (1)

Country Link
JP (1) JPH01267601A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015088349A (en) * 2013-10-31 2015-05-07 パナソニックIpマネジメント株式会社 Lighting device
JP2015090782A (en) * 2013-11-05 2015-05-11 パナソニックIpマネジメント株式会社 Lighting fixture

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015088349A (en) * 2013-10-31 2015-05-07 パナソニックIpマネジメント株式会社 Lighting device
JP2015090782A (en) * 2013-11-05 2015-05-11 パナソニックIpマネジメント株式会社 Lighting fixture

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