JPH04151628A - Photometry device for electronic image pickup device - Google Patents

Photometry device for electronic image pickup device

Info

Publication number
JPH04151628A
JPH04151628A JP2275311A JP27531190A JPH04151628A JP H04151628 A JPH04151628 A JP H04151628A JP 2275311 A JP2275311 A JP 2275311A JP 27531190 A JP27531190 A JP 27531190A JP H04151628 A JPH04151628 A JP H04151628A
Authority
JP
Japan
Prior art keywords
light
photometry
lens
optical axis
pass filter
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
JP2275311A
Other languages
Japanese (ja)
Inventor
Takao Inoue
隆夫 井上
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.)
Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP2275311A priority Critical patent/JPH04151628A/en
Publication of JPH04151628A publication Critical patent/JPH04151628A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To reduce an effect of external diffusion and to minimize time delay from trigger-on regardless of the magnification or the sort of a lens by constituting a photometry device so that the photometry of light passed through the lens can be directly executed by the separation of polarized light. CONSTITUTION:An optical low-pass filter means 2 that double refraction for preventing the pseudo resolution of the light is utilized, a photoelectric conversion means which photoelectrically converts the light, a polarized light separation means and a photometry means are provided. That means, a photometry element 10 is arranged on an optical axis polarized by a polarizing beam splitter 11 so that the photometry of the light passed through the lens 1 can be directly executed. Thus, the effect of external diffusion is reduced and the time delay from the trigger-on is minimized regardless of the magnification or the sort of the lens.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は電子撮像装置の測光装置に関し、レンズを通っ
た光を直接測光できるようにしたものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a photometry device for an electronic image pickup device, and is capable of directly photometering light passing through a lens.

(従来の技術) 第2図は従来の電子撮像装置の測光装置の構成例を示し
、第3図はそのストロボ使用時の動作フローチャートを
示す。通常はレンズJを通った光は、光学的ローパスフ
ィルタ(LPF)2にて空間周波数の高い成分が除去さ
れ、電荷結合素子(CCDイメージセンサ−)3により
、予め仮露光される。このCCDの出力はプロセス部4
を経由としてマイクロコンピュータ(CPLJ)5に入
力され、仮露光で決定されたシャッタスピード(絞り)
にてシャッター駆動11FII6が制御され、レンズと
CCDとを結ぶ光軸上に配設されたシャッター7を本露
光させる。
(Prior Art) FIG. 2 shows a configuration example of a photometric device of a conventional electronic imaging device, and FIG. 3 shows an operation flowchart when using a strobe. Normally, the light passing through the lens J has high spatial frequency components removed by an optical low pass filter (LPF) 2, and is subjected to temporary exposure in advance by a charge coupled device (CCD image sensor) 3. The output of this CCD is the process section 4
The shutter speed (aperture) is input to the microcomputer (CPLJ) 5 via
The shutter drive 11FII6 is controlled at , and the shutter 7 disposed on the optical axis connecting the lens and the CCD is subjected to main exposure.

次にストロボ8を使用時には、シャッター7を固定(開
放)したまま(Sl)、ストロボ発光回路9からの信号
によりストロボ8を発光させ(S、)、レンズ外部の測
光素子IOで横比しくS6)、その横比信号にもとづき
CPU5が適正露光光量となったところで(S、のYE
S)、ストロボ発光回路9からの信号によりストロボ8
の発光を停止する(S、)。
Next, when using the strobe 8, with the shutter 7 fixed (open) (Sl), the strobe 8 is fired by a signal from the strobe light emitting circuit 9 (S,), and the photometric element IO outside the lens is used to set the horizontal ratio S6. ), and when the CPU 5 reaches the appropriate exposure light amount based on the horizontal ratio signal (YE of S)
S), the strobe 8 is activated by the signal from the strobe light emitting circuit 9.
stops emitting light (S,).

(発明が解決しようとするtlM) 上記従来の第2図に示す電子撮像装置の測光装置におい
ては、CCD3において測光する場合、トリガー(凹路
)を押してから仮露光するため、必ず時間遅れが発生す
る。また、CCD自体のラチチュードが狭いため極端に
高精度もしくは低輝度の被写体では、−度の仮露光では
正確な露出値を把握できない。
(tlM to be solved by the invention) In the conventional photometering device of the electronic image pickup device shown in FIG. 2, when measuring light using the CCD 3, a time delay always occurs because the trigger (concave path) is pressed and then provisional exposure is performed. do. Further, since the latitude of the CCD itself is narrow, in the case of an extremely high-precision or low-luminance subject, an accurate exposure value cannot be determined with -degree provisional exposure.

また、ストロボ使用時には、上記CCD露光が使えない
ため、外部素子にて測光することになるが、この場合、
次のような欠点がある。
Also, when using a strobe, the above CCD exposure cannot be used, so photometry must be done with an external element, but in this case,
It has the following drawbacks:

(a)レンズ外に測光素子があるため、レンズのズーム
倍率、変化により正確な露出値が得られない。
(a) Since there is a photometric element outside the lens, accurate exposure values cannot be obtained due to changes in the zoom magnification of the lens.

(b)レンズ変換に対応できない。(b) Cannot support lens conversion.

(c)被写体の正確な露出値ではない。(c) It is not an accurate exposure value of the subject.

(d)被写体の近くに高反射率の物体があると誤動作し
やすい。
(d) Malfunctions are likely to occur if there is a highly reflective object near the subject.

これらの欠点を解決する手段として、銀塩カメラで用い
られているTTLダイレクト測光方式がある。これは、
レンズを通してフィルム面に当った光の反射を測光素子
で測光する。このTTLダイレクト測光方式を電子撮像
装置に応用すれば、上記欠点は解消されるが、CODに
当った光の反射は、通常、省スペースのためCCD直前
に光学的ローパスフィルター(LPF)2を配置するた
め、測光素子を配置するのは難しいという問題があった
As a means to solve these drawbacks, there is a TTL direct photometry method used in silver halide cameras. this is,
A photometric element measures the reflection of the light that hits the film surface through the lens. If this TTL direct photometry method is applied to an electronic imaging device, the above-mentioned drawbacks will be solved, but in order to save space, an optical low-pass filter (LPF) 2 is usually placed just before the CCD to reduce the reflection of the light that hits the COD. Therefore, there was a problem in that it was difficult to arrange the photometric element.

本発明はこのような問題点を解決し、簡単な構成でCC
D面からの反射光を検出できる電子撮像装置の測光装置
を提供することを目的とする。
The present invention solves these problems and provides CC with a simple configuration.
It is an object of the present invention to provide a photometry device for an electronic imaging device that can detect reflected light from the D surface.

(課題を解決するための手段) 本発明は上記課題を解決し目的を達成するため、光の疑
解像を防止するための複屈折を利用した光学的ローパス
フィルター手段と、光を光電変換する光電変換手段と、
前記光学的ローパスフィルター手段と光電変換手段の光
軸上に配設された偏光光分離手段と、該偏光光分離手段
により光軸から分離された偏光光軸上に配設された前記
光電変換手段に入射した光量を直接に測光検出する測光
手段とを有することを特徴とする。
(Means for Solving the Problems) In order to solve the above problems and achieve the objects, the present invention provides optical low-pass filter means using birefringence to prevent false resolution of light, and photoelectric conversion of light. photoelectric conversion means;
Polarized light separation means disposed on the optical axis of the optical low-pass filter means and photoelectric conversion means; and the photoelectric conversion means disposed on the polarized optical axis separated from the optical axis by the polarized light separation means. and photometric means for directly photometrically detecting the amount of light incident on the device.

(作 用) 本発明はレンズを通った光を偏光分離によって直接測光
できるように構成したので、外乱による影響が少なく、
また、レンズの倍率、レンズの種類に左右されることな
く、トリガーオンからの時間遅れも最小に抑えられる。
(Function) The present invention is configured so that the light passing through the lens can be directly measured by polarization separation, so there is little influence from external disturbances.
Additionally, the time delay from trigger-on can be minimized, regardless of lens magnification or lens type.

(実施例) 第1図は本発明の一実施例の構成図を示し、2はCCD
3による疑解像を防止するための水晶ローパスフィルタ
ー(L P F)、11は該LPF2とCCD3の光軸
上に配設された光の偏光ビームスプリッタ−(PBS)
、■2は同じく光軸上に配設されたl/4波長板であり
、測光素子lOは前記PBSIIで偏光された光軸上に
配設され、レンズ1からCCD3を結ぶ光軸とは分離さ
れている。
(Embodiment) FIG. 1 shows a configuration diagram of an embodiment of the present invention, and 2 is a CCD
3 is a crystal low-pass filter (LPF) for preventing false resolution; 11 is a polarizing beam splitter (PBS) for light disposed on the optical axis of the LPF 2 and CCD 3;
, ■2 is a l/4 wavelength plate also placed on the optical axis, and the photometric element IO is placed on the optical axis polarized by the PBSII, and is separated from the optical axis connecting lens 1 to CCD 3. has been done.

次に上記構成の測光装置の動作について説明すると、レ
ンズ1を通った光は、CCD3による疑解像を防止する
ための水晶ローパスフィルター(LPF)2にて空間周
波数の高い成分が取除かれる。このLPF2を通過した
光は偏光ビームスプリッタ−(P B 5)11を通り
、174波長板12を介してCCD3に入射する。
Next, the operation of the photometric device having the above configuration will be described. The light passing through the lens 1 is filtered with high spatial frequency components by a crystal low-pass filter (LPF) 2 for preventing false resolution by the CCD 3. The light that has passed through the LPF 2 passes through the polarizing beam splitter (P B 5) 11 and enters the CCD 3 via the 174 wavelength plate 12 .

二のCCD3に入射した光の一部は、CCD板面上、も
しくはカバーガラスにて反射してPBSllに入射する
A part of the light incident on the second CCD 3 is reflected on the CCD plate surface or the cover glass and is incident on the PBSll.

さて、LPF2を出射した光は、このLPFが水晶の複
屈折を利用しているため直線偏光されている。この光は
、次に174波長板!2を2度通過するため反射して偏
光ビームスプリッタ−(P B 5)11に入射する光
は、L P j2の出射光に対して偏光方向の異なった
直線偏光光となる。即ち、PBSllの方向を適切な光
軸上に配置することで、損失なくCCD3からの反射光
を光軸外に取出せる。
Now, the light emitted from the LPF 2 is linearly polarized because this LPF utilizes the birefringence of crystal. This light is then a 174 wavelength plate! Since the light passes through L P j2 twice, the light that is reflected and enters the polarizing beam splitter (P B 5) 11 becomes linearly polarized light with a polarization direction different from that of the light emitted from L P j2. That is, by arranging the direction of PBSll on an appropriate optical axis, the reflected light from the CCD 3 can be taken out off the optical axis without loss.

この光軸外に取出した反射光を測光素子IOにて検出す
れば、CCD3の入射光量を正確にCPU5は知ること
が出来る。そして、該CPU5が測光素子10の検出値
にて露光量を決定し、シャッター駆動部6を制御する。
By detecting this reflected light taken out off the optical axis with the photometric element IO, the CPU 5 can accurately know the amount of light incident on the CCD 3. Then, the CPU 5 determines the exposure amount based on the detected value of the photometric element 10 and controls the shutter drive unit 6.

(発明の効果) 以上説明したように本発明は、偏光ビームスプリッタ−
により偏光した光軸上に測光素子を配置するようにした
ので5従来の問題点が解消された。
(Effects of the Invention) As explained above, the present invention provides a polarizing beam splitter.
Since the photometric element is arranged on the optical axis of the polarized light, the problems of the conventional method have been solved.

そして、レンズを通った光を直接測光できるので、外乱
による影響が少なく、また、レンズの倍率、レンズの種
類により左右されることなく、トリガーオンからの時間
遅れも最小に抑えることが出来る。
Since the light passing through the lens can be measured directly, there is little influence from external disturbances, and the time delay from trigger-on can be minimized without being influenced by the magnification of the lens or the type of lens.

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

第1図は本発明の一実施例の構成図、第2図は従来の電
子撮像装置の測光装置の構成例を示す図、第3図は第2
図でストロボ使用時の動作フローを示す図である。 l・・・レンズ、  2・・・ローパスフィルター(L
PF)、 3・・・電荷結合素子(COD)、4・・・
プロセス部、  5・・・マイクロコンピュータ(CP
 U)、  6・・・シャッター駆動部、  7・・・
シャッター  8・・・ストロボ、9・・・ストロボ発
光回路、 10・・・測光素子、11・・・偏光ビーム
スプリッタ−(P B S)、12・・・174波長板
。 特許呂願人 株式会社 リ コ 第 図 7ンマ、り 第 図 1し/ズ
FIG. 1 is a block diagram of an embodiment of the present invention, FIG. 2 is a diagram showing an example of the structure of a photometric device of a conventional electronic imaging device, and FIG.
FIG. 2 is a diagram illustrating an operation flow when using a strobe. l...Lens, 2...Low pass filter (L
PF), 3... Charge coupled device (COD), 4...
Process section, 5... microcomputer (CP
U), 6...Shutter drive unit, 7...
Shutter 8... Strobe, 9... Strobe light emitting circuit, 10... Photometric element, 11... Polarizing beam splitter (PBS), 12... 174 wavelength plate. Patent Roganjin Co., Ltd. Riko Figure 7, Figure 1/Z

Claims (1)

【特許請求の範囲】[Claims] 光の疑解像を防止するための複屈折を利用した光学的ロ
ーパスフィルター手段と、光を光電変換する光電変換手
段と、前記光学的ローパスフィルター手段と光電変換手
段の光軸上に配設された偏光光分離手段と、該偏光光分
離手段により光軸から分離された偏光光軸上に配設され
た前記光電変換手段に入射した光量を直接に測光検出す
る測光手段とを有することを特徴とする電子撮像装置の
測光装置。
an optical low-pass filter means using birefringence to prevent false resolution of light; a photoelectric conversion means for photoelectrically converting light; and an optical low-pass filter means disposed on the optical axis of the optical low-pass filter means and the photoelectric conversion means. a polarized light separating means; and a photometric means for directly photometrically detecting the amount of light incident on the photoelectric conversion means disposed on the polarized optical axis separated from the optical axis by the polarized light separating means. A photometric device for an electronic imaging device.
JP2275311A 1990-10-16 1990-10-16 Photometry device for electronic image pickup device Pending JPH04151628A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2275311A JPH04151628A (en) 1990-10-16 1990-10-16 Photometry device for electronic image pickup device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2275311A JPH04151628A (en) 1990-10-16 1990-10-16 Photometry device for electronic image pickup device

Publications (1)

Publication Number Publication Date
JPH04151628A true JPH04151628A (en) 1992-05-25

Family

ID=17553675

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2275311A Pending JPH04151628A (en) 1990-10-16 1990-10-16 Photometry device for electronic image pickup device

Country Status (1)

Country Link
JP (1) JPH04151628A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7616879B2 (en) 2004-10-06 2009-11-10 Canon Kabushiki Kaisha Optical apparatus and image-taking system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7616879B2 (en) 2004-10-06 2009-11-10 Canon Kabushiki Kaisha Optical apparatus and image-taking system

Similar Documents

Publication Publication Date Title
JPS6332370B2 (en)
US4626918A (en) Photometric optical system for single-lens reflex electronic photographic camera
JPH04151628A (en) Photometry device for electronic image pickup device
US4716284A (en) Photographic optical system having enhanced spectral transmittance characteristics
US4005441A (en) Photometric device of through the lens type exposure meter in a single-lens reflex camera
US5359364A (en) Electronic still camera having an optical system for TTL dimming
JP2579224B2 (en) Imaging device
US4470686A (en) Distance and light measuring device for single lens reflex camera
JPH0321937A (en) Solid-state image pickup camera
JPH01303410A (en) Af camera
SU1377811A1 (en) Device for automatic focusing of a reflex camera
JP2001188293A (en) Polarized light removing device and photographic system using it
US4364651A (en) Exposure ascertaining device for cameras
KR100323388B1 (en) device for measuring a distance and brightness of an object in digital still camera
JP2759270B2 (en) Photometer for electronic imaging camera
JPH05289144A (en) Photometry device for image pickup device
JPH01320876A (en) Ae device
JPH0862661A (en) Photometry device for camera
JPS614032A (en) Photometric device
JPH0281573A (en) Photometry device for electronic image pickup camera
JPS60123169A (en) Electronic camera
JPS6388536A (en) Photometry and range finding device
JPH07281083A (en) Distance measuring and photometric device
JPH01254925A (en) Camera
JPH01147438A (en) Light receiving device for camera