JPS61213638A - Measuring instrument for visual sensitivity - Google Patents

Measuring instrument for visual sensitivity

Info

Publication number
JPS61213638A
JPS61213638A JP5492285A JP5492285A JPS61213638A JP S61213638 A JPS61213638 A JP S61213638A JP 5492285 A JP5492285 A JP 5492285A JP 5492285 A JP5492285 A JP 5492285A JP S61213638 A JPS61213638 A JP S61213638A
Authority
JP
Japan
Prior art keywords
light
lev
mask
luminance
parallel 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.)
Granted
Application number
JP5492285A
Other languages
Japanese (ja)
Other versions
JPH0453366B2 (en
Inventor
Teruaki Shigeta
照明 重田
Shigeru Horii
滋 堀井
Hideo Nishiyama
西山 英夫
Yoshiharu Osaki
吉晴 大崎
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP5492285A priority Critical patent/JPS61213638A/en
Publication of JPS61213638A publication Critical patent/JPS61213638A/en
Publication of JPH0453366B2 publication Critical patent/JPH0453366B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • G01J1/0407Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings
    • G01J1/0437Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings using masks, aperture plates, spatial light modulators, spatial filters, e.g. reflective filters
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • G01J1/0407Optical elements not provided otherwise, e.g. manifolds, windows, holograms, gratings
    • G01J1/0474Diffusers
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/02Details
    • G01J1/04Optical or mechanical part supplementary adjustable parts
    • G01J2001/0485Cosinus correcting or purposely modifying the angular response of a light sensor

Abstract

PURPOSE:To obtain a measuring instrument which facilitates corrections of angular characteristics of equivalent light curtain brightness by providing a photodetection window which has diffuse transmission characteristics, a light shielding plate, a condenser lens, a mask for parallel light, a photodetector, etc. CONSTITUTION:Equivalent light curtain brightness (Lev) information from a measure ment visual field of max. 180 deg. is incident on the photodetection window 37. In considera tion of characteristics of Lev, the information is passed through aperture parts of light shield plates 38 and 39, converged by the condenser lens 40, and then made entered into the photodetector 43 for Lev through the mask 41 for parallel light and a diffusing plate 42 so as to extract only a parallel light component from the incident light. Further, the photodetection window 37 has diffuse transmission characteristics and is increased in diffuse transmissivity at a part (a) of the optical axis center part of the window 37 and made lower in diffuse transmissivity at a part (b) of the periph eral part than at the optical axis center part to equalize angular characteristics of Lev to a logical value. Then, an Lev measurement system is not an image formation system, so the influence of variances in cosine biquadratic rule characteristics and aperture efficiency characteristics is hard to exert.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、視対象物の税率輝度(ブライトネス)を導く
計測装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a measuring device for determining the brightness of a visual object.

従来の技術 一般の複雑な輝度分布を有する視環境内に存在する視対
象物の“明るさ”(以後、祝意輝度Bと呼ぶ)は、その
視対象物輝度Lo (以後、  Loと呼ぶ)とそれを
見る観測者の目の順応輝度に対応する輝度差別いきΔL
min  (以後ΔL minと呼ぶ)の関数として定
量的に求められる。たとえば、祝意輝度Bは。
Conventional technology The "brightness" of a visual object (hereinafter referred to as congratulatory brightness B) existing in a visual environment with a complex brightness distribution in general is expressed as the brightness of the visual object Lo (hereinafter referred to as Lo). Luminance discrimination ΔL corresponding to the adapted luminance of the eye of the observer who sees it
It is quantitatively determined as a function of min (hereinafter referred to as ΔL min). For example, congratulatory brightness B is.

” =”gl”” (l Lmin )”’ ”’ ”
’(1)と表わすことができる。
"="gl"" (l Lmin)"'"'"
'(1).

ここで、ΔL winは、特開昭65−46185号公
報に示すように、観測者の中心窩順応輝度Lf’(以後
、Lfと呼ぶ)と等価光幕輝度Leマ(以後。
Here, as shown in Japanese Unexamined Patent Publication No. 65-46185, ΔL win is the foveal adaptation luminance Lf' (hereinafter referred to as Lf) of the observer and the equivalent light curtain luminance Lema (hereinafter referred to as Lf).

Loマと呼ぶ)とから求められる。(called Loma).

したがって、祝意輝度Bは、Lf、Loマ、Loの3種
類の輝度計測値から第4図のような手順で求めることが
できる。
Therefore, the congratulatory brightness B can be determined from the three types of brightness measurement values Lf, Loma, and Lo using the procedure shown in FIG. 4.

第4図において、&では中心窩順応輝度Lfを計測する
。bでは等価光幕輝度Levを計測する。
In FIG. 4, the foveal adaptation brightness Lf is measured at &. In b, the equivalent light curtain luminance Lev is measured.

Cでは視対象物輝度LOを計測する。dでは中心窩順応
輝度に関係する輝度差弁別いきΔLfを求める。eでは
等価光幕輝度に関係する輝度差弁別いきΔLeマを求め
る。fでは輝度差弁別いきΔLを求める。Cでは祝意輝
度Bを求める。
At C, the visual object brightness LO is measured. In d, the luminance difference discrimination ΔLf related to the foveal adaptation luminance is determined. In e, a luminance difference discrimination ΔLe matrix related to the equivalent light screen luminance is determined. At f, ΔL is determined by brightness difference discrimination. At C, congratulatory brightness B is determined.

このような計測原理をもとに、具体的な計測装置として
第6図に示すようなLf’計測系、 Lav計測系、 
Lo計測系およびファインダ系を同一の光学系で構成し
た祝意輝度計測装置が考えられている。
Based on such measurement principles, specific measurement devices include Lf' measurement system, Lav measurement system, as shown in Fig. 6.
A congratulatory luminance measurement device is being considered in which the Lo measurement system and the finder system are configured with the same optical system.

以下に、上記従来の祝意輝度計測装置について説明する
The conventional congratulatory luminance measuring device described above will be explained below.

第5図は祝意輝度計測装置の光学系の構成を示すもので
あり、1は視野内の視対象物である。2は前記視対象物
1の輝度情報を含んだ像を、後述の受光器やファインダ
に導くための対物レンズ、3.4,6.6は対物レンズ
2からの像を、受光器やファインダに分離させるハーフ
プリズム、7はLOの計測視野角を限定するマスク、8
はマスク7を通過した光束(輝度)を拡散させる拡散板
、9はLoを受光するための受光器、10はLfの計測
視野角を限定するマスク、11はマスク10を通過した
光束(輝度)を拡散させる拡散板、12はLfを受光す
るための受光器、13はLevの角度特性(1/θ2特
性)を補正する補正フィルタ、14は補正フィルタ13
を通過した光束(輝度)を拡散させる拡散板、15はL
evを受光するための受光器、16はLOとLfの計測
範囲を表示したレチクル、17はLoとLfの計測範囲
を確認するためのファインダ、18,19,20,21
.22は対物レンズ2からの像を、受光器9、受光器1
5゜ファインダ1Tにそれぞれ導くリレーレンズである
FIG. 5 shows the configuration of the optical system of the congratulatory luminance measuring device, and 1 is a visual object within the field of view. 2 is an objective lens for guiding an image containing luminance information of the viewing object 1 to a light receiver or finder, which will be described later; 3.4 and 6.6 are for guiding an image from the objective lens 2 to a light receiver or finder. A half prism to be separated, 7 is a mask that limits the LO measurement viewing angle, 8
1 is a diffuser plate that diffuses the light flux (brightness) that has passed through the mask 7; 9 is a light receiver that receives Lo; 10 is a mask that limits the Lf measurement viewing angle; 11 is a light flux (brightness) that has passed through the mask 10 12 is a light receiver for receiving Lf; 13 is a correction filter that corrects the angular characteristic (1/θ2 characteristic) of Lev; 14 is a correction filter 13
A diffuser plate that diffuses the luminous flux (luminance) that has passed through the
16 is a reticle displaying the measurement range of LO and Lf; 17 is a finder for confirming the measurement range of Lo and Lf; 18, 19, 20, 21
.. 22, the image from the objective lens 2 is transmitted to the light receiver 9 and the light receiver 1.
These are relay lenses that each lead to the 5° finder 1T.

以上のように構成された従来の祝意輝度計測装置の動作
を説明すると、まず視野内の視対象物1は対物レンズ2
により、Xの位置に空間像として結像される。この場合
、対物レンズ2の視野角(画角)は、Levの特性から
1112LX、180’が要求されるため、超広角レン
ズが用いられている。
To explain the operation of the conventional congratulatory luminance measuring device configured as described above, first, the visual object 1 in the field of view is detected by the objective lens 2.
As a result, an image is formed at the X position as an aerial image. In this case, the viewing angle (angle of view) of the objective lens 2 is required to be 1112LX, 180' due to the characteristics of Lev, so an ultra-wide-angle lens is used.

Xに結像された像は、リレーレンズ18を通ったのち、
ハーフプリズム4→ハーフプリズム3→リレーレンズ1
9→マスク7→拡散板8→受光器9へ導かれる( Lo
の計測)とともに、ノ・−フグリズム4→リレーレンズ
20→マスク1o→拡散板11→受光器12(Lfの計
測)へ、さらにハーフプリズム4→ハーフプリズム6→
リレーレンズ21→レチクル16→フアインダ17(フ
ァインダによる計測範囲の確認)へと導かれ、最終。
After the image formed on X passes through the relay lens 18,
Half prism 4 → Half prism 3 → Relay lens 1
9 → mask 7 → diffuser plate 8 → guided to light receiver 9 (Lo
(Measurement of Lf), along with No. 4 -> relay lens 20 -> mask 1o -> diffuser plate 11 -> light receiver 12 (measurement of Lf), and then half prism 4 -> half prism 6 ->
Relay lens 21 → reticle 16 → guide to finder 17 (confirmation of measurement range with finder), and finally.

ハーフプリズム4→ハーフプリズム5→ハーフプリズム
6→リレーレンズ22→補正フイルタ13→拡散板14
→受光器15(Levの計測)へそれ。
Half prism 4 → Half prism 5 → Half prism 6 → Relay lens 22 → Correction filter 13 → Diffusion plate 14
→It goes to the light receiver 15 (Lev measurement).

ぞれ導かれる。Each will be guided.

このようにして、3種類の輝度計測を行ない、それらの
計測値を演算処理することにより、祝意輝度Bを計測す
る。
In this way, three types of brightness measurements are performed, and the congratulatory brightness B is measured by performing arithmetic processing on these measured values.

以上のように、従来の祝意輝度計測装置の動作では、L
O計測系、Lf計測系、 Lev計測系およびファイン
ダ系が同一の光軸を有しており、同時計測ができること
から、ひとつの計測装置で同一場所における祝意輝度計
測を行なわせようとしたものである。
As described above, in the operation of the conventional congratulatory luminance measurement device, L
Since the O measurement system, Lf measurement system, Lev measurement system, and finder system have the same optical axis and can perform simultaneous measurements, we attempted to measure the congratulatory luminance at the same location using one measurement device. be.

このような構成において、前記補正フィルタ13は、光
軸中心とθの角度で入射する光の透過率Lf’を第6図
に示すようにK cosθ/θ2(Kは定数)で減衰す
る特性となるようにしたものである。
In such a configuration, the correction filter 13 has a characteristic that the transmittance Lf' of light incident at an angle θ with respect to the center of the optical axis is attenuated by K cos θ/θ2 (K is a constant) as shown in FIG. It was made so that it would become so.

この特性は対物レンズ2のもつ、余弦四乗側特性と開口
効率特性がばらつくことから、これらの補正も合わせて
行なう必要があり、角度特性(透過率特性)の精度が要
求される。
Since this characteristic varies in the cosine-fourth power side characteristic and the aperture efficiency characteristic of the objective lens 2, it is necessary to also correct these characteristics, and accuracy of the angular characteristic (transmittance characteristic) is required.

通常、このような特性を得るものとしては、ガラスや石
英の基板上に濃度勾配をもつ蒸着薄膜層を設けた。いわ
ゆるニュートラルデンシティフィルタなどが知られてい
る。しかし、これらのフィルタを製作する場合、上記の
ように透過率が10−4%程度になると、製作上、透過
率のコントロールがむずかしくなり、希望通りの特性が
得られないのが実情である。
Typically, such properties are obtained by depositing a thin film layer with a concentration gradient on a glass or quartz substrate. So-called neutral density filters are known. However, when manufacturing these filters, when the transmittance reaches about 10-4% as mentioned above, it becomes difficult to control the transmittance during manufacturing, and the actual situation is that desired characteristics cannot be obtained.

発明が解決しようとする問題点 このような従来の構成では、前記対物レンズ2の余弦四
乗側特性と開口効率特性をあらかじめ求めておき、個々
の対物レンズの特性に合わせた補正フィルタを、その都
度、製作するという問題を有していた。
Problems to be Solved by the Invention In such a conventional configuration, the cosine fourth power side characteristics and the aperture efficiency characteristics of the objective lens 2 are determined in advance, and a correction filter that matches the characteristics of each objective lens is created. There was the problem of having to manufacture the product each time.

本発明は上記従来の問題点を解消するもので。The present invention solves the above-mentioned conventional problems.

等価光幕輝度Levの角度特性の補正を容易にした祝意
輝度計測装置を提供することを目的とする。
It is an object of the present invention to provide a congratulatory brightness measuring device that facilitates correction of the angular characteristics of the equivalent light curtain brightness Lev.

問題点を解決するための手段 本発明は等価光幕輝度Leマの計測系において。Means to solve problems The present invention relates to a measurement system for equivalent light screen luminance Le.

拡散透過特性を有する受光窓と、この受光窓からの平行
光成分のみを取り出す開口部をもつ遮光板と、前記遮光
板を通過した平行光を後述の受光器に入射させるコンデ
ンサレンズと、コンデンサレンズからの平行光成分を通
過させるマスクと、平行光用マスクからのLevを受光
する受光器を備えた祝意輝度計測装置であり、均等な厚
さをもつ前記受光窓の光軸中心部の拡散透過率を高くし
、周辺部の拡散透過率を光軸中心部より低くすることに
より、Levの角度特性を理論値に合致させることがで
きるものである。
A light-receiving window having diffuse transmission characteristics, a light-shielding plate having an opening that takes out only the parallel light component from the light-receiving window, a condenser lens that allows the parallel light that has passed through the light-shielding plate to enter a light receiver to be described later, and a condenser lens. This is a congratulatory luminance measurement device equipped with a mask that allows parallel light components to pass through, and a light receiver that receives Lev from the parallel light mask, and the diffused transmission at the center of the optical axis of the light receiving window that has a uniform thickness. The angular characteristic of Lev can be made to match the theoretical value by increasing the transmittance and making the diffuse transmittance in the peripheral area lower than that in the center of the optical axis.

作用 この技術的手段による作用は次のようになる。action The effect of this technical means is as follows.

すなわち、本発明は拡散透過特性が既知の材料を、受光
窓に使用することができ、それらを組み合わせることに
よって所期の特性が容易に得られる。また、 Lev計
測系が従来例のような結像系でないため、余弦四乗側特
性・開口効率特性のばらつきによる影響を受けにくい。
That is, in the present invention, materials with known diffuse transmission characteristics can be used for the light receiving window, and desired characteristics can be easily obtained by combining them. Furthermore, since the Lev measurement system is not an imaging system like the conventional example, it is less susceptible to variations in cosine-fourth power side characteristics and aperture efficiency characteristics.

実施例 以下、本発明の一実施例を添付図面にもとづいて説明す
る。
Embodiment Hereinafter, one embodiment of the present invention will be described based on the accompanying drawings.

第1図は祝意輝度計測装置の光学系の構成図を示したも
のである。第1図において、23は視野内の視対象物で
ある。24は前記視対象物23の輝度情報を含んだ光学
像を、後述の受光器やファインダに導くための対物レン
ズ、26は対物レンズ24からの光学像を後述の中心窩
順応輝度用受光器やファインダに導くとともに、視対象
物輝度LOの計測視野角(1°〜2°)を限定するため
の穴あきミラー、26は穴あきミラー25の穴部分を通
過した光束(輝度)を拡散させる拡散板、27はり、を
受光するだめの受光器(視感度補正済み)、28は中心
窩順応輝度計測系とファインダ系とを分離させるハーフ
プリズム、29は中心窩順応輝度Lfの計測視野角(1
00〜20’)を限定するマスク、30はマスク29を
通過した光束(輝度)を拡散させる拡散板、31はLf
を受光するための受光器(視感度補正済み)、32は穴
あきミラー25の位置に結像された視対象物23の光学
像を、Lf 用マスク29と後述のレチクルの位置に再
度結像させる中間レンズ、33および34はハーフプリ
ズム28で一部反射された光学像をファインダ系に導く
ためのリレーレンズ、36はLOとLfの計測範囲を表
示したレチクル。
FIG. 1 shows a configuration diagram of the optical system of the congratulatory luminance measuring device. In FIG. 1, 23 is a visual object within the visual field. Reference numeral 24 denotes an objective lens for guiding an optical image containing luminance information of the viewing object 23 to a light receiver or finder, which will be described later. Reference numeral 26 indicates an objective lens for guiding an optical image containing luminance information of the viewing object 23 to a light receiver or a finder, which will be described later. A perforated mirror for guiding the light to the finder and limiting the viewing angle (1° to 2°) for measuring the luminance LO of the visible object; 26 is a diffuser for diffusing the luminous flux (brightness) that has passed through the hole of the perforated mirror 25; 28 is a half prism that separates the foveal adaptation brightness measurement system from the finder system; 29 is a measurement viewing angle (1
00 to 20'), 30 is a diffusion plate that diffuses the luminous flux (luminance) that has passed through the mask 29, and 31 is Lf.
A light receiver (with visibility correction) 32 is for re-imaging the optical image of the visual object 23 formed at the position of the perforated mirror 25 at the position of the Lf mask 29 and the reticle, which will be described later. 33 and 34 are relay lenses for guiding the optical image partially reflected by the half prism 28 to the finder system, and 36 is a reticle displaying the LO and Lf measurement ranges.

36はり、とI、fの計測範囲を確認するためのファイ
ンダ(視野角30’)、37は等価光幕輝度Lavを視
野角16oO〜18o0で計測するための受光窓(拡散
透過特性を有したもの)、38および39は受光窓37
に入射するL6マ輝度情報のうち、平行光成分のみを取
り出すだめの開口部(円形)をもつ遮光板、40は遮光
板38.39を通過した平行光を集光し、後述の受光器
に入射させるコンデンサレンズ、41はコンデンサレン
ズ4oからの平行光成分を通過させるマスク、42は平
行光用マスク41からの光束(輝度)を拡散させる拡散
板、43はLevを受光するための受光器(視感度補正
済み)である。
36 beams, and a finder (viewing angle 30') for checking the measurement range of I and f; 37 a light receiving window (with diffuse transmission characteristics) for measuring the equivalent light screen brightness Lav at a viewing angle of 16oO to 18o0; ), 38 and 39 are light receiving windows 37
A light shielding plate 40 has an aperture (circular) for extracting only the parallel light component out of the L6 luminance information incident on the light shielding plate 38, 39. The light shielding plate 40 collects the parallel light that has passed through the light shielding plate 38 and 39, and sends it to the light receiver described later. 41 is a mask that allows the parallel light component from the condenser lens 4o to pass through; 42 is a diffuser plate that diffuses the luminous flux (luminance) from the parallel light mask 41; 43 is a light receiver (for receiving Lev); (visual sensitivity corrected).

以上のように構成された本発明の実施例の祝意輝度計測
装置について、以下その動作を説明する。
The operation of the congratulatory luminance measuring device according to the embodiment of the present invention configured as described above will be described below.

第1図において、視対象物23の光学像は対物レンズ2
4を介したのち、一部穴あきミラー25の穴部分を通過
後、拡散板26を経てLO用受光器27に到達する。前
記穴あきミラー26にはり。
In FIG. 1, an optical image of a visual object 23 is formed by an objective lens 2
4, passes through a hole in a partially perforated mirror 25, passes through a diffuser plate 26, and reaches an LO light receiver 27. Glue to the perforated mirror 26.

の計測視野角(10〜2°)を限定する大きさの開口部
(円形の穴部分)が設けられている。以上がLOの計測
動作である。
An opening (circular hole) is provided with a size that limits the measurement viewing angle (10 to 2 degrees). The above is the LO measurement operation.

一方、穴あきミラー25のミラ一部分で反射された光学
像は、中間レンズ32を通過したのち、ハーフプリズム
28により、Lf計測系とファインダ系とに分離された
のち、透過光(光学像)はマスク29の位置に結像され
る。マスク29にはLfの計測視野角(10°〜2o0
)を限定する大きさの開口部(円形)が設けられており
、Lf輝度情報はマスク29を通過後、拡散板3oを経
てLf用受光器31に到達する。以上がLfの計測動作
である。
On the other hand, the optical image reflected by a portion of the perforated mirror 25 passes through the intermediate lens 32 and is separated into the Lf measurement system and the finder system by the half prism 28, and then the transmitted light (optical image) is An image is formed at the position of the mask 29. The mask 29 has a measurement viewing angle of Lf (10° to 2o0
), and after passing through the mask 29, the Lf luminance information reaches the Lf light receiver 31 via the diffuser plate 3o. The above is the Lf measurement operation.

また、ハーフプリズム28からの反射光(光学像)はリ
レーレンズ33および34を介したのち、レチクル35
の位置に結像される。レチクル35はLOとLfの計測
範囲がわかるように1°〜2゜および100〜2o0の
円形が表示されている。そして、ファインダ36により
計測者はLo、Lfの計測範囲を確認することができる
Further, the reflected light (optical image) from the half prism 28 passes through relay lenses 33 and 34, and then passes through the reticle 35.
The image is formed at the position of The reticle 35 displays circles of 1° to 2° and 100 to 2o0 so that the measurement ranges of LO and Lf can be seen. The finder 36 allows the measurer to check the measurement ranges of Lo and Lf.

以上はLO計測系、Lf計測系、ファインダ系の動作に
ついて説明したもので、次にL6マ計測系の動作を説明
する。
The operations of the LO measurement system, Lf measurement system, and finder system have been explained above, and next, the operation of the L6 measurement system will be explained.

第1図において、受光窓37はm&X。18o0の計測
視野内からのLat輝度情報が入射する。そしてLOマ
の特性上、これらの入射光のうち、平行光成分のみを取
り出すため、遮光板38および39の開口部を通過させ
、コンデンサレンズ40で集光したのち、平行光用マス
ク41.拡散板42を経てLaマ用受光器43に到達す
る。
In FIG. 1, the light receiving window 37 is m&X. Lat luminance information from within the measurement field of view of 18o0 is incident. Due to the characteristics of the LO beam, in order to extract only the parallel light component of these incident lights, the light is passed through the openings of the light shielding plates 38 and 39, condensed by the condenser lens 40, and then passed through the parallel light mask 41. The light passes through the diffuser plate 42 and reaches the La light receiver 43.

受光窓3γは拡散透過特性を有しておシ、本発明では受
光窓37の光軸中心部(対物レンズ24の周囲、図中の
aの部分)の拡散透過率を高くシ。
The light-receiving window 3γ has a diffuse transmission characteristic, and in the present invention, the diffuse transmittance of the optical axis center portion of the light-receiving window 37 (around the objective lens 24, the part a in the figure) is made high.

周辺部(図中のbの部分)の拡散透過率を光軸中心部よ
り低くしている。ここで、受光窓37は均等な厚さをも
つ光学ガラスを使用しており、上記aおよびbの拡散透
過特性は第2図のようになっている。
The diffused transmittance of the peripheral portion (portion b in the figure) is lower than that of the central portion of the optical axis. Here, the light-receiving window 37 is made of optical glass having a uniform thickness, and the diffuse transmission characteristics of a and b mentioned above are as shown in FIG.

なお、受光窓37の拡散透過特性を実現する方法として
は、光学ガラスの場合、機械的に拡散透過特性を得る方
法、たとえば、砂かけや研摩、ダイレクトプレスなどに
より、ガラス面をあらす方法および化学的に拡散透過特
性を得る方法、たとえば、ふっ化水素などにより、ガラ
ス面をあらす方法などが考えられる。
In the case of optical glass, methods for achieving the diffuse transmission characteristics of the light receiving window 37 include methods for mechanically obtaining the diffuse transmission characteristics, such as roughening the glass surface by sanding, polishing, direct pressing, etc., and chemical methods. One possible method is to obtain diffuse transmission characteristics, for example, by roughening the glass surface with hydrogen fluoride or the like.

ここで−例として、受光窓37(直径φ703111)
を機械加工、すなわち砂かけ・研摩してaの部分(φ2
o〜φ4o1nIl)とbの部分(φ40〜φ7oso
g)とを、それぞれ異なる拡散透過特性にしたのち、L
6マ計測系の角度特性を求めると第3図のような結果を
得た。第3図の結果から、上記方法により所期の角度特
性が得られることがわかる。
Here, as an example, the light receiving window 37 (diameter φ703111)
is machined, that is, sanded and polished to form part a (φ2
o~φ4o1nIl) and part b (φ40~φ7oso
g) and have different diffuse transmission characteristics, and then L
When the angular characteristics of the 6-ma measurement system were determined, the results shown in Figure 3 were obtained. From the results shown in FIG. 3, it can be seen that the desired angular characteristics can be obtained by the above method.

本実施例において、受光窓37には光学ガラスを使用し
ているが、光学ガラスの代わりに拡散透過特性の異なる
樹脂(たとえば、三菱アクリライト、住友スミペックス
:いずれも商品名)の組み合わせ、樹脂の成形(片面に
拡散面を設ける)、拡散透過特性を有するフィルム・シ
ートなどの貼り付けなどKよっても、上記光学ガラスの
場合と同様の特性が得られることはいうまでもない。
In this embodiment, optical glass is used for the light receiving window 37, but instead of optical glass, a combination of resins with different diffuse transmission characteristics (for example, Mitsubishi Acrylite, Sumitomo Sumipex: both trade names), It goes without saying that properties similar to those of the above-mentioned optical glass can also be obtained by molding (providing a diffusing surface on one side), attaching a film or sheet having diffuse transmission properties, etc.

以上のように本実施例によれば1等価光幕輝度計測系に
おいて、視野角1800からの等価光幕輝度情報を受光
する受光窓を、2種類以上の拡散透過特性を有した材料
で構成し、受光窓の光軸中心部の拡散透過率を高くする
とともに、周辺部の拡散透過率を光軸中心部より低くす
ることにより、LOマの角度特性を容易に理論値に合致
させることができる。
As described above, according to this embodiment, in the one-equivalent light curtain luminance measurement system, the light receiving window that receives the equivalent light curtain luminance information from the viewing angle of 1800 is made of two or more types of materials having diffuse transmission characteristics. By increasing the diffuse transmittance at the center of the optical axis of the light receiving window and lowering the diffuse transmittance at the periphery than at the center of the optical axis, the angular characteristics of the LO beam can be easily matched to the theoretical values. .

発明の効果 以上の実施例の説明より明らかなように1本発明の祝意
輝度計測装置は、等価光幕薄度Levの計測系において
、拡散透過特性を有する受光窓と、この受光窓からの平
行光成分のみを取り出す開口部をもつ遮光板と、前記遮
光板を通過した平行光を受光器に入射させるコンデンサ
レンズと、コンデンサレンズからの平行光成分を通過さ
せる平行光用マスクと平行光用マスクからのLOマを受
光する受光器を設け、前記受光窓を2種類以上の拡散透
過特性を有する材料で構成し、受光窓の光軸中心部の拡
散透過率を高くするとともに、周辺部の拡散透過率を光
軸中心部より低くするような組合わせを決めることによ
り、LOマの角度特性を理論値に合致させることができ
る。
Effects of the Invention As is clear from the above description of the embodiments, the congratulatory luminance measuring device of the present invention has a light receiving window having a diffuse transmission characteristic and a parallel A light shielding plate having an opening that takes out only light components, a condenser lens that allows the parallel light that has passed through the light shielding plate to enter a light receiver, a parallel light mask that allows the parallel light component from the condenser lens to pass, and a parallel light mask. A light receiver is provided for receiving LO beams from By determining a combination that makes the transmittance lower than the center of the optical axis, the angular characteristics of the LO beam can be made to match the theoretical values.

さらには1本実施例でのLeマ計測系が、従来例のよう
な結像系でないため、余弦四乗側特性・開口効率特性の
ばらつきによる影響を受けにくいなどの効果がある。
Furthermore, since the Lema measurement system in this embodiment is not an imaging system like the conventional example, it has the advantage of being less susceptible to variations in the cosine fourth power side characteristics and the aperture efficiency characteristics.

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

第1図は本発明の一実施例の祝意輝度計測装置における
光学系の構成図、第2図は実施例における受光窓の拡散
透過特性を示す図、第3図は実施例における等価光幕輝
度計測系の角度特性を示す図、第4図は祝意輝度計測の
原理を示す図、第6図は従来例における祝意輝度計測装
置の光学系の構成図、第6図は等価光幕輝度の角度特性
の理論特性図である。 23・・・・・・視対象物、24・・・・・・対物レン
ズ、26・・・・・・穴あきミラー、26,3o、42
・・・・・・拡散板。 27.31,43・・・・・・受光器、28・・・・・
・ハーフプリズム、29・・・・・・マスク、32・・
・・・・中間レンズ、33.34・・・・・・リレーレ
ンズ、36・・・…レチクル、36・・・・・・ファイ
ンダ、37・・・・・・受光窓、38゜39・・・・・
・遮光板、40・・・・・・コンデンサレンズ。 41・・・・・・平行光用マスク。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第2
図 ※At O(de3)で−qth’!−14H(%)+
擾hir=H%第3図 θ(dす]
Fig. 1 is a configuration diagram of an optical system in a congratulatory luminance measuring device according to an embodiment of the present invention, Fig. 2 is a diagram showing the diffuse transmission characteristics of the light receiving window in the embodiment, and Fig. 3 is an equivalent light curtain luminance in the embodiment. Figure 4 is a diagram showing the angular characteristics of the measurement system, Figure 4 is a diagram showing the principle of congratulatory luminance measurement, Figure 6 is a configuration diagram of the optical system of a conventional congratulatory luminance measurement device, and Figure 6 is the angle of equivalent light curtain luminance. It is a theoretical characteristic diagram of characteristics. 23... Visual object, 24... Objective lens, 26... Hole mirror, 26, 3o, 42
...Diffusion board. 27.31,43...Receiver, 28...
・Half prism, 29...Mask, 32...
...Intermediate lens, 33.34...Relay lens, 36...Reticle, 36...Finder, 37...Light receiving window, 38°39... ...
- Light shielding plate, 40... Condenser lens. 41...Mask for parallel light. Name of agent: Patent attorney Toshio Nakao and 1 other person 2nd
Figure *At O(de3) -qth'! -14H (%)+
擾hir=H% Figure 3 θ(ds)

Claims (1)

【特許請求の範囲】[Claims] 均等な厚さをもち、2種類以上の拡散透過特性を有する
材料で構成し、光軸中心部の拡散透過率を高くするとと
もに、周辺部の拡散透過率を光軸中心部より低くした等
価光幕輝度用受光窓と、この受光窓からの平行光成分の
みを取り出す開口部をもつ遮光板と、前記遮光板を通過
した平行光を受光器に入射させるコンデンサレンズと、
このコンデンサレンズからの平行光成分を通過させるマ
スクと、前記平行光用マスクからの等価光幕輝度情報を
受光する受光器とからなる等価光幕輝度計測系と、結像
系からなる視対象物輝度計測系・中心窩順応輝度計測系
およびファインダ系とを備えた視感輝度計測装置。
Equivalent light that has a uniform thickness and is made of materials with two or more types of diffuse transmission characteristics, and has a high diffuse transmittance at the center of the optical axis and a lower diffuse transmittance at the periphery than at the center of the optical axis. a light-receiving window for curtain luminance, a light-shielding plate having an opening that takes out only the parallel light component from the light-receiving window, and a condenser lens that causes the parallel light that has passed through the light-shielding plate to enter the light receiver;
An equivalent light curtain brightness measurement system consisting of a mask that allows the parallel light component from the condenser lens to pass through, and a light receiver that receives equivalent light curtain brightness information from the parallel light mask, and a visual object that includes an imaging system. A visual luminance measurement device equipped with a luminance measurement system, a foveal adaptation luminance measurement system, and a finder system.
JP5492285A 1985-03-19 1985-03-19 Measuring instrument for visual sensitivity Granted JPS61213638A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5492285A JPS61213638A (en) 1985-03-19 1985-03-19 Measuring instrument for visual sensitivity

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5492285A JPS61213638A (en) 1985-03-19 1985-03-19 Measuring instrument for visual sensitivity

Publications (2)

Publication Number Publication Date
JPS61213638A true JPS61213638A (en) 1986-09-22
JPH0453366B2 JPH0453366B2 (en) 1992-08-26

Family

ID=12984108

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5492285A Granted JPS61213638A (en) 1985-03-19 1985-03-19 Measuring instrument for visual sensitivity

Country Status (1)

Country Link
JP (1) JPS61213638A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2010003362A1 (en) * 2008-07-07 2010-01-14 Mou Tongsheng Brighness measurement device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2010003362A1 (en) * 2008-07-07 2010-01-14 Mou Tongsheng Brighness measurement device

Also Published As

Publication number Publication date
JPH0453366B2 (en) 1992-08-26

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