JPS6033377Y2 - Light receiving device that can change the angle of incidence - Google Patents

Light receiving device that can change the angle of incidence

Info

Publication number
JPS6033377Y2
JPS6033377Y2 JP1978096271U JP9627178U JPS6033377Y2 JP S6033377 Y2 JPS6033377 Y2 JP S6033377Y2 JP 1978096271 U JP1978096271 U JP 1978096271U JP 9627178 U JP9627178 U JP 9627178U JP S6033377 Y2 JPS6033377 Y2 JP S6033377Y2
Authority
JP
Japan
Prior art keywords
light receiving
lens
angle
receiving element
light
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
Application number
JP1978096271U
Other languages
Japanese (ja)
Other versions
JPS5516408U (en
Inventor
秀一 三原
幸夫 尾高
Original Assignee
株式会社サンパツク
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 株式会社サンパツク filed Critical 株式会社サンパツク
Priority to JP1978096271U priority Critical patent/JPS6033377Y2/en
Publication of JPS5516408U publication Critical patent/JPS5516408U/ja
Application granted granted Critical
Publication of JPS6033377Y2 publication Critical patent/JPS6033377Y2/en
Expired legal-status Critical Current

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  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)
  • Exposure Control For Cameras (AREA)
  • Stroboscope Apparatuses (AREA)

Description

【考案の詳細な説明】 本考案は、オートストロボに使用する受光装置に関する
[Detailed Description of the Invention] The present invention relates to a light receiving device used in an auto strobe.

周知のように、オートストロボは、入射光を電気信号に
変える受光素子を用いた測光回路を有しており、この測
光回路によって被写体の明るさを測光し、オートストロ
ボからの光で被写体の明るさが予定光量に達したときに
、オートストロボの発光を停止させるようになっている
As is well known, an auto strobe has a photometric circuit that uses a light receiving element that converts incident light into an electrical signal.This photometric circuit measures the brightness of the subject, and the light from the auto strobe measures the brightness of the subject. The auto strobe stops firing when the light intensity reaches the scheduled light level.

このオートストロボにおける受光素子への入射角は、通
常一定に定められている。
The angle of incidence on the light receiving element in this autostrobe is usually fixed.

しかし使用の実際上は、このオートストロボからの光の
照射角によって、又はこのオートストロボを使用してい
るカメラのレンズの画角に応じて入射角を変えるように
することが望ましい。
However, in practical use, it is desirable to change the incident angle depending on the angle of illumination of the light from the autostrobe or depending on the angle of view of the lens of the camera using the autostrobe.

すなわち、広角レンズを用いオートストロボからの照射
角を大きくしたときは受光素子へ広い範囲から光が入射
するように入射角を大きくし、反対に望遠レンズを用い
てストロボの照射角を小としたときには入射角を小さく
することが望ましい。
In other words, when using a wide-angle lens to increase the angle of irradiation from an auto strobe, the angle of incidence is increased so that light enters the photodetector from a wider range, and conversely, when using a telephoto lens, the angle of irradiation from the strobe is reduced. Sometimes it is desirable to reduce the angle of incidence.

単純に受光素子への入射角を変えることは容易である。It is easy to simply change the angle of incidence on the light receiving element.

しかし、それに応じて入射光量が異なったのでは正確な
測光が行えない。
However, if the amount of incident light varies accordingly, accurate photometry cannot be performed.

すなわち、一定の明るさの被写体による受光素子表面の
明るさは、受光素子への入射角を変えても一定でなけれ
ばならない。
That is, the brightness on the surface of the light receiving element due to a subject having a constant brightness must remain constant even if the angle of incidence on the light receiving element is changed.

これを実現するための一手段として例えば特開昭53−
78872号公報に示されるように受光素子の前にズー
ムレンズを配置するものが知られている。
As a means to achieve this, for example,
As shown in Japanese Patent No. 78872, a zoom lens is known in which a zoom lens is placed in front of a light receiving element.

しかしながら周知のようにズームレンズは極めて高価な
もので、ストロボ全体の値段より高くなることもありス
トロボの受光装置としては使用することはできない。
However, as is well known, zoom lenses are extremely expensive, sometimes costing more than the entire strobe, and cannot be used as a light receiving device for a strobe.

従って、本考案の目的は簡単な構造で受光素子への入射
角を変えても同一の明るさの被写体に対しては受光素子
への入射光量を一定とすることができる受光装置を提供
することを目的とするものである。
Therefore, an object of the present invention is to provide a light receiving device that has a simple structure and can keep the amount of light incident on the light receiving element constant for an object of the same brightness even if the angle of incidence on the light receiving element is changed. The purpose is to

そのため、本考案は受光素子の前に受光素子との間の距
離を変えることができるように設置するレンズにそのレ
ンズの焦点距離と等しい長さのフードを設けたことを特
徴とするものである。
Therefore, the present invention is characterized in that a hood with a length equal to the focal length of the lens is provided on the lens installed in front of the light receiving element so that the distance between the lens and the light receiving element can be changed. .

受光素子の表面の明るさとは、レンズによる像の照度で
ある。
The brightness of the surface of the light receiving element is the illuminance of the image formed by the lens.

レンズ系による像の照度Eは、第2図に示すように物体
の輝度をLとし、像点Pからレンズ系の射出瞳を見る角
度の半分をθとすると、 E = r ?rLsinθ で表される。
The illuminance E of the image produced by the lens system is determined by E = r?, where L is the brightness of the object and θ is half the angle at which the exit pupil of the lens system is viewed from the image point P, as shown in Fig. 2. It is expressed as rLsinθ.

丁はレンズ系の透過率である。従って、θが同ブであれ
ば物体の輝度りが同一である限り照度E1すなわち受光
素子の表面の明るさは一定である。
D is the transmittance of the lens system. Therefore, if θ is the same, as long as the brightness of the object is the same, the illuminance E1, that is, the brightness of the surface of the light receiving element is constant.

レンズと受光素子の距離を変えればθも変化し受光素子
の表面の照度も変化する。
If the distance between the lens and the light receiving element is changed, θ will also change, and the illuminance on the surface of the light receiving element will also change.

従って、単に受光素子の前にレンズを配置し受光素子と
の距離を変えるようにしただけでは、受光素子への入射
角を変えることはできるが、それにより受光素子表面の
照度も変化するので正しく測光することはできない。
Therefore, simply placing a lens in front of the light receiving element and changing the distance from the light receiving element can change the angle of incidence on the light receiving element, but this will also change the illuminance on the surface of the light receiving element, so it is not possible to It cannot be photometered.

次に第1図の実施例に示すようにフード1をレンズ2に
設置した場合について説明する。
Next, a case where the hood 1 is installed on the lens 2 as shown in the embodiment shown in FIG. 1 will be described.

受光素子(図示せず)はP点に置くものとする。It is assumed that a light receiving element (not shown) is placed at point P.

今、フード1の長さを1、レンズ2とP点との距離を8
ルンズの光軸からフード1までの高さをh、入射角をα
、レンズ2の焦点距離をfとし、角αでレンズ2に入射
した光線がレンズで屈折して角α′で進み焦点面Fに達
するものとする。
Now, the length of hood 1 is 1, and the distance between lens 2 and point P is 8.
The height from the optical axis of the lens to hood 1 is h, and the angle of incidence is α
, the focal length of the lens 2 is f, and a ray of light incident on the lens 2 at an angle α is refracted by the lens, advances at an angle α', and reaches the focal plane F.

このときのフード1の最先端を通ってレンズ2へ入射す
る光線のレンズ2と交わる位置のレンズの光軸からの距
離をdとし、焦点面F上でその中央からその光線がその
面と交わる点までの距離をDとすると以下の式が成立す
る。
At this time, the distance from the optical axis of the lens at the position where the ray of light that passes through the leading edge of the hood 1 and enters the lens 2 intersects with the lens 2 is d, and the ray of light intersects with that surface from the center on the focal plane F. Letting the distance to the point be D, the following equation holds true.

tana = (h d) / 1 =D/ f
””(1)tana =d/ s=D/ (f−
s) =(2)従って、 d=fsh/ (fl−sl+sf) となるのでこれを(1)式に代入すると tana=h(f−s)/(fl−sl+sf)
・・・・・(3)a =tan−” (h (f s
) / (fl−sl+5f))・・・・・・(4) となる。
tana = (h d) / 1 = D/ f
"" (1) tana = d/ s = D/ (f-
s) = (2) Therefore, d = fsh/ (fl-sl + sf), so by substituting this into equation (1), tana = h (f-s) / (fl-sl + sf)
...(3) a = tan-" (h (f s
) / (fl-sl+5f)) (4).

一方(2)式は tana’=fh/ (S (f l) +fl)
””(5)となる。
On the other hand, equation (2) is tana'=fh/ (S (f l) + fl)
”” (5).

(3)及び(5)式からSを変えればα及びα′が変化
することがわかる。
It can be seen from equations (3) and (5) that if S is changed, α and α' will change.

ここでf=1、すなわち、フードの長さをレンズ2の焦
点距離に等しくする。
Here, f=1, that is, the length of the hood is equal to the focal length of lens 2.

すると(5)式は tan a ’ =fh/f2= h / f
””(6)となる。
Then, equation (5) becomes tan a' = fh/f2= h/f
” (6).

h及びfは一定である。従って、α′は不変となる。h and f are constant. Therefore, α' remains unchanged.

一方(3)式は tan a = h (f s ) /F
””(7)となる。
On the other hand, equation (3) is tan a = h (f s ) /F
””(7).

従って、tanaはSlすなわちレンズと受光素子との
距離によって変化する。
Therefore, tana changes depending on Sl, that is, the distance between the lens and the light receiving element.

このように、本考案によれば、フード1の長さをレンズ
2の焦点距離と等しくすれば、レンズと受光素子との距
離を変えることによって、被写体からの入射角を変える
ことができ、しかも、入射角の変化にかかわらず、受光
素子へ入射光量を等しくすることができる。
As described above, according to the present invention, if the length of the hood 1 is made equal to the focal length of the lens 2, the angle of incidence from the subject can be changed by changing the distance between the lens and the light receiving element. , the amount of light incident on the light receiving element can be made equal regardless of changes in the incident angle.

しかも、本考案はレンズに単にその焦点距離と等しい長
さのフードを設置するだけであるので極めて簡単な構造
とすることができ、従って、安価とすることができる。
Moreover, since the present invention simply requires installing a hood with a length equal to the focal length of the lens, the structure can be extremely simple, and the cost can therefore be reduced.

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

第1図は、本考案実施例に関するもので、光線の進光を
示す概略図、第2図は一般のレンズ系の光線説明図であ
る。 1:フード、2:レンズ。
FIG. 1 relates to an embodiment of the present invention, and is a schematic diagram showing the propagation of light rays, and FIG. 2 is an explanatory diagram of light rays in a general lens system. 1: Hood, 2: Lens.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 受光素子と、該受光素子の前に設けたレンズとからなり
、受光素子とレンズとの距離を変えることにより、受光
素子への入射角を可変とした受光装置において、レンズ
に、レンズの焦点距離を等しい長さを有するフードを設
けたことを特徴とする受光装置。
In a light-receiving device that consists of a light-receiving element and a lens provided in front of the light-receiving element, the angle of incidence on the light-receiving element is variable by changing the distance between the light-receiving element and the lens. A light receiving device characterized in that a hood having equal lengths is provided.
JP1978096271U 1978-07-14 1978-07-14 Light receiving device that can change the angle of incidence Expired JPS6033377Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1978096271U JPS6033377Y2 (en) 1978-07-14 1978-07-14 Light receiving device that can change the angle of incidence

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1978096271U JPS6033377Y2 (en) 1978-07-14 1978-07-14 Light receiving device that can change the angle of incidence

Publications (2)

Publication Number Publication Date
JPS5516408U JPS5516408U (en) 1980-02-01
JPS6033377Y2 true JPS6033377Y2 (en) 1985-10-04

Family

ID=29030005

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1978096271U Expired JPS6033377Y2 (en) 1978-07-14 1978-07-14 Light receiving device that can change the angle of incidence

Country Status (1)

Country Link
JP (1) JPS6033377Y2 (en)

Also Published As

Publication number Publication date
JPS5516408U (en) 1980-02-01

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