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JPH0617824B2 - Optical quantity distribution measuring method and optical quantity distribution measuring device - Google Patents
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JPH0617824B2 - Optical quantity distribution measuring method and optical quantity distribution measuring device - Google Patents

Optical quantity distribution measuring method and optical quantity distribution measuring device

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Publication number
JPH0617824B2
JPH0617824B2 JP18922488A JP18922488A JPH0617824B2 JP H0617824 B2 JPH0617824 B2 JP H0617824B2 JP 18922488 A JP18922488 A JP 18922488A JP 18922488 A JP18922488 A JP 18922488A JP H0617824 B2 JPH0617824 B2 JP H0617824B2
Authority
JP
Japan
Prior art keywords
optical quantity
image input
input means
aiming
conversion coefficient
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 - Lifetime
Application number
JP18922488A
Other languages
Japanese (ja)
Other versions
JPH0236323A (en
Inventor
敏彦 阪口
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 Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP18922488A priority Critical patent/JPH0617824B2/en
Publication of JPH0236323A publication Critical patent/JPH0236323A/en
Publication of JPH0617824B2 publication Critical patent/JPH0617824B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、いわゆるCCD(電荷結合素子)カメラな
どの高精細度で観測を行うことができる画像入力手段を
用いて、輝度などの光学量の分布を計測する光学量計測
方法および光学量計測装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial application] The present invention uses an image input means such as a so-called CCD (charge-coupled device) camera capable of observing with high definition to obtain an optical quantity such as brightness. The present invention relates to an optical amount measuring method and an optical amount measuring device for measuring the distribution of.

〔従来の技術〕[Conventional technology]

被照明領域等の計測対象の表面の輝度分布を計測する場
合、計測対象の全表面を連続的に測定することが理想で
あるが、実際にはそのような測定は困難である。そこ
で、被照明領域に所定間隔で点在する測定点を決め、各
測定点毎に測定を行うことが考えられる。
When measuring the luminance distribution of the surface of the measurement target such as the illuminated area, it is ideal to continuously measure the entire surface of the measurement target, but such measurement is difficult in practice. Therefore, it is conceivable to determine measurement points scattered at predetermined intervals in the illuminated area and perform measurement at each measurement point.

従来は、被照明領域をメジャーで図りながら各測定点に
印を付け、各測定点毎に輝度計で測定し、各測定点の位
置(座標)と測定値とから全体の評価を行っていた。
Conventionally, each measurement point is marked while measuring the illuminated area with a measure, the measurement is performed with a luminance meter at each measurement point, and the overall evaluation is performed from the position (coordinates) and measurement value of each measurement point. .

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

ところが、このような光学量分布計測方法は、道路のよ
うな長大な被照明領域の場合、測定点の位置を決めるた
めの計測を行い、かつ各測定点毎に輝度計による測定を
する必要があるため膨大な作業量となる。またそのため
粗い間隔での測定しかできなかった。
However, such an optical quantity distribution measuring method requires measurement for determining the position of the measurement point and measurement by a luminance meter at each measurement point in the case of a long illuminated area such as a road. There is a huge amount of work because of this. Therefore, it was possible to measure only at coarse intervals.

このような背景から、CCDカメラ等の高精細度の画像
入力手段を用いて測定を行うことが考えられる。この場
合、画像入力手段の画像出力と被照明領域の実際の輝度
との間の対応をとるため、変換係数を求める必要があ
る。
From such a background, it is conceivable to perform the measurement using a high-definition image input means such as a CCD camera. In this case, it is necessary to obtain the conversion coefficient in order to establish a correspondence between the image output of the image input means and the actual brightness of the illuminated area.

したがって、この発明の目的は、変換係数が簡単に得ら
れかつ精細な輝度分布が容易に得られる光学量分布計測
方法を提供するとともに、測定が容易な光学量分布計測
装置を提供することである。
Therefore, an object of the present invention is to provide an optical quantity distribution measuring method in which a conversion coefficient can be easily obtained and a fine luminance distribution can be easily obtained, and an optical quantity distribution measuring device that can be easily measured. .

〔課題を解決するための手段〕[Means for Solving the Problems]

請求項(1)の光学量分布計測方法は、高精細度で観測を
行なうことができる画像入力手段で計測対象を撮影し、
その画像の各部の部分的出力と変換係数とにより前記計
測対象の各部の輝度を計測する光学量分布計測方法であ
って、レーザスキャナからレーザビームを照射して前記
計測対象に予め照準図形を描き、この照準図形に照準を
設定して撮影することにより得られた前記画像入力手段
の平均的な画像出力と、前記照準図形に照準が設定され
て前記画像入力手段と同一の測定範囲に関する前記光学
量計測手段の平均的な測定値との間の前記変換係数を求
めることを特徴とするものである。
The optical quantity distribution measuring method according to claim (1), the object to be measured is photographed by an image input means capable of performing observation with high definition,
It is an optical quantity distribution measuring method for measuring the brightness of each part of the measurement target by the partial output of each part of the image and the conversion coefficient, and draws a sighting pattern in advance on the measurement target by irradiating a laser beam from a laser scanner. , An average image output of the image input means obtained by setting a sight on the aiming figure and photographing, and the optical about the same measurement range as the aiming figure set on the aiming figure. It is characterized in that the conversion coefficient between an average measurement value of the quantity measuring means is obtained.

請求項(2)の光学量分布計測装置は、計測対象に予め定
める照準図形を描くレーザビームを照射するレーザスキ
ャナと、このレーザスキャナと同じ位置に設けられ前記
照準図形に照準が設定されて平均の輝度を計測する変換
係数算出用の光学量計測手段と、前記レーザスキャナと
同じ位置に設けられ前記照準図形に照準が設定されて前
記画像入力手段と同一の測定範囲を撮影する高精細度で
観測可能な画像入力手段とを備え、前記光学量計測手段
の平均的な測定値と、前記画像入力手段の平均的な画像
出力との間の変換係数を算出するとともに、前記画像入
力手段により得られる各部の部分的出力と前記変換係数
とに基づいて、前記計測対象の各部の輝度を計測するこ
とを特徴とするものである。
The optical quantity distribution measuring device according to claim (2) is a laser scanner that irradiates a laser beam that draws a predetermined aiming figure on a measurement target, and the aiming is set on the aiming figure provided at the same position as this laser scanner and the average With an optical quantity measuring means for calculating the conversion coefficient for measuring the luminance of the, and a high definition for shooting the same measurement range as the image input means provided at the same position as the laser scanner and aiming in the aiming figure. An observable image input means is provided, and a conversion coefficient between an average measurement value of the optical quantity measuring means and an average image output of the image input means is calculated and obtained by the image input means. The brightness of each part of the measurement target is measured based on the partial output of each part and the conversion coefficient.

〔作用〕[Action]

請求項(1)の光学量分布計測方法によれば、レーザビー
ムにより描かれた照準図形に光学量計測手段および画像
入力手段の照準が共通に設定され、同一の測定範囲に関
する観測が行なわれ、光学量計測手段により得られた平
均の輝度と、画像入力手段により得られた平均的な画像
出力との間の変換係数が算出される。そして画像入力手
段の各部の画像出力と変換係数とに基づいて各部の輝度
が算出される。この場合、レーザビームは任意の場所に
簡単に照準図形を描くことができるので、被照明領域等
の現場で印を付ける等の面倒な作業が必要でなくなり、
変換係数が簡単に得られる。また画像入力手段の各部の
部分的出力は画素の精度で得られるので、精細な輝度の
分布を容易に測定することができる。
According to the optical quantity distribution measuring method of claim (1), the aiming figures of the optical quantity measuring means and the image input means are commonly set in the aiming figure drawn by the laser beam, and observation regarding the same measuring range is performed. A conversion coefficient between the average luminance obtained by the optical quantity measuring means and the average image output obtained by the image input means is calculated. Then, the brightness of each part is calculated based on the image output and the conversion coefficient of each part of the image input means. In this case, since the laser beam can easily draw a sighting figure at any place, there is no need for troublesome work such as marking on the spot such as the illuminated area,
The conversion factor is easily obtained. Further, since the partial output of each part of the image input means is obtained with pixel accuracy, it is possible to easily measure a fine luminance distribution.

請求項(2)の光学量分布計測装置によれば、レーザスキ
ャナ、光学量計測手段および画像入力手段を同じ位置に
設けることにより、装置の一体化が可能になり取扱いが
簡単になるとともに、測定が容易になる。
According to the optical quantity distribution measuring device of claim (2), by providing the laser scanner, the optical quantity measuring means and the image input means at the same position, the apparatus can be integrated and the handling becomes easy and the measurement can be performed. Will be easier.

〔実施例〕〔Example〕

この発明の一実施例を第1図および第2図に基づいて説
明する。すなわち、この光学量分布計測方法は、光学量
計測手段1と、画像入力手段2と、レーザスキャナ3と
を用いる。
An embodiment of the present invention will be described with reference to FIGS. 1 and 2. That is, this optical quantity distribution measuring method uses the optical quantity measuring means 1, the image input means 2, and the laser scanner 3.

光学量計測手段1は、輝度計を実施例としている。画像
入力手段2は高精細度で観測を行うことができるもので
いわゆるCCD(電荷結合素子)カメラを実施例として
いる。そして、レーザスキャナ3はレーザビームを照射
するもので、任意の場所に容易に照準図形を描くことが
できる。
The optical quantity measuring means 1 uses a luminance meter as an example. The image input means 2 is capable of observing with high definition, and a so-called CCD (charge coupled device) camera is used as an example. The laser scanner 3 irradiates a laser beam and can easily draw an aiming figure at any place.

この光学量分布計測方法は、計測対象4にレーザスキャ
ナ3からレーザビーム3aを照射する。さらにレーザビ
ーム3aで計測対象4に予め定めた所定の領域を囲む円
形を実施例とする照準図形を描く(第2図(3))。
In this optical quantity distribution measuring method, the measurement target 4 is irradiated with the laser beam 3a from the laser scanner 3. Furthermore, a laser beam 3a is used to draw an aiming figure with a circle surrounding a predetermined region on the measurement target 4 as an example (FIG. 2 (3)).

光学量計測手段1は、光軸1a上にある中心C1(第2図
(1))を照準図形の中心に合わせるように照準図形が設
定される。この光学量計測手段1は通常たとえば光軸1
aを含み、1/3゜,1/2゜,1゜,2゜などの見込み
角によって規定される測定視野を有しており、レーザス
キャナ3が描く照準図形はこの測定視野に対応する測定
範囲を示している。
The optical quantity measuring means 1 has a center C1 on the optical axis 1a (see FIG. 2).
The aiming figure is set so that (1)) is aligned with the center of the aiming figure. This optical quantity measuring means 1 is usually an optical axis 1, for example.
Including a, it has a measurement field of view defined by the angle of view such as 1/3 °, 1/2 °, 1 °, 2 °, etc., and the sighting pattern drawn by the laser scanner 3 is the measurement corresponding to this measurement field of view. Indicates the range.

画像入力手段2は、光軸2a上にある中心C2(第2図
(2))を照準図形の中心C4に合わせるように照準が設
定される(第2図(4))。
The image input means 2 has a center C2 on the optical axis 2a (see FIG. 2).
The aim is set so that (2)) is aligned with the center C4 of the aiming figure ((2) in FIG. 2).

変換係数は、光学量計測手段1の平均の計測値と画像入
力手段2の平均の画像出力とから算出される。
The conversion coefficient is calculated from the average measured value of the optical quantity measuring unit 1 and the average image output of the image input unit 2.

つぎに、画像入力手段2の各部の画像出力と変換係数と
に基づいて各部の輝度を算出する。この場合、画像入力
手段2は高精細度であり、たとえば、各画素毎または複
数の画素のグループ毎に輝度を細かく得ることができ
る。
Next, the brightness of each part of the image input means 2 is calculated based on the image output of each part and the conversion coefficient. In this case, the image input means 2 has a high definition and, for example, it is possible to finely obtain the luminance for each pixel or each group of a plurality of pixels.

この実施例の光学量分布計測方法によれば、レーザビー
ム3aにより描かれた照準図形に光学量計測手段1およ
び画像入力手段2の照準が共通に設定され、同一の測定
範囲に関する観測が行なわれ、光学量計測手段1により
得られた平均の輝度と、画像入力手段2により得られた
平均的な画像出力との間の変換係数が算出される。そし
て画像入力手段2の各部の画像出力と変換係数とに基づ
いて各部の輝度が算出される。この場合、レーザビーム
3aは任意の場所に簡単に照準図形を描くことができる
ので、被照明領域等の現場で印を付ける等の面倒な作業
が必要でなくなり、変換係数が簡単に得られる。また画
像入力手段2の各部の部分的出力は画素の精度で得られ
るので、精細な輝度の分布を容易に測定することができ
る。
According to the optical quantity distribution measuring method of this embodiment, the aiming figures of the optical quantity measuring means 1 and the image inputting means 2 are commonly set in the aiming figure drawn by the laser beam 3a, and the observation in the same measuring range is performed. A conversion coefficient between the average luminance obtained by the optical quantity measuring unit 1 and the average image output obtained by the image input unit 2 is calculated. Then, the brightness of each part is calculated based on the image output of each part of the image input means 2 and the conversion coefficient. In this case, since the laser beam 3a can easily draw a sighting figure at an arbitrary place, troublesome work such as marking on the spot such as an illuminated area is not required, and the conversion coefficient can be easily obtained. Further, since the partial output of each part of the image input means 2 is obtained with pixel accuracy, it is possible to easily measure a fine luminance distribution.

また光学量分布計測装置によれば、レーザスキャナ3、
光学量計測手段1および画像入力手段2を同じ位置に設
けることにより、装置の一体化が可能になり取扱いが簡
単になるとともに、測定が容易になる。
Further, according to the optical quantity distribution measuring device, the laser scanner 3,
By providing the optical quantity measuring means 1 and the image input means 2 at the same position, the apparatus can be integrated, the handling becomes simple, and the measurement becomes easy.

なお、計測対象4は、計測対象4を照明する光源の種類
や、光源の光によって照射される物体を組成する物質な
どによって異なるため、画像入力手段2による輝度の計
測にあたっては計測対象4が異なるごとに、前述のよう
な変換係数の算出が行われる。
Note that the measurement target 4 differs depending on the type of light source that illuminates the measurement target 4, the substance that composes the object illuminated by the light from the light source, and so on. The above-described calculation of the conversion coefficient is performed every time.

〔発明の効果〕〔The invention's effect〕

請求項(1)の光学量分布計測方法によれば、レーザビー
ムは任意の場所に簡単に照準図形を描くことができるの
で、被照明領域等の現場で印を付ける等の面倒な作業が
必要でなくなり、変換係数が簡単に得られる。また画像
入力手段の各部の部分的出力は画素の精度で得られるの
で、精細な輝度の分布を容易に測定することができると
いう効果がある。
According to the optical quantity distribution measuring method of claim (1), since the laser beam can easily draw an aiming figure at any place, it is necessary to perform a troublesome work such as marking on the spot such as an illuminated area. , And the conversion coefficient can be easily obtained. Further, since the partial output of each part of the image input means is obtained with pixel accuracy, there is an effect that a fine luminance distribution can be easily measured.

請求項(2)の光学量分布計測装置によれば、レーザスキ
ャナ、光学量計測手段および画像入力手段を同じ位置に
設けることにより、装置の一体化が可能になり取扱いが
簡単になるとともに、測定が容易になる。
According to the optical quantity distribution measuring device of claim (2), by providing the laser scanner, the optical quantity measuring means and the image input means at the same position, the apparatus can be integrated and the handling becomes easy and the measurement can be performed. Will be easier.

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

第1図はこの発明の一実施例の原理的な構成を示す概念
図、第2図は光学量計測手段および画像入力手段の光軸
の中心ならびにレーザスキャナによって描かれる図形の
一例を示す図である。 1……光学量計測手段、2……画像入力手段、3……レ
ーザスキャナ、3a……レーザビーム
FIG. 1 is a conceptual diagram showing the basic configuration of an embodiment of the present invention, and FIG. 2 is a diagram showing an example of the centers of the optical axes of the optical quantity measuring means and the image inputting means and a figure drawn by a laser scanner. is there. 1 ... Optical quantity measuring means, 2 ... Image input means, 3 ... Laser scanner, 3a ... Laser beam

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】高精細度で観測を行なうことができる画像
入力手段で計測対象を撮影し、その画像の各部の部分的
出力と変換係数とにより前記計測対象の各部の輝度を計
測する光学量分布計測方法であって、レーザスキャナか
らレーザビームを照射して前記計測対象に予め照準図形
を描き、この照準図形に照準を設定して撮影することに
より得られた前記画像入力手段の平均的な画像出力と、
前記照準図形に照準が設定されて前記画像入力手段と同
一の測定範囲に関する前記光学量計測手段の平均的な測
定値との間の前記変換係数を求めることを特徴とする光
学量分布計測方法。
1. An optical quantity for photographing an object to be measured with an image input means capable of observing with high definition and measuring the luminance of each part of the object to be measured by a partial output and a conversion coefficient of each part of the image. A distribution measuring method, irradiating a laser beam from a laser scanner to draw a sighting pattern in advance on the object to be measured, and setting the sighting on this sighting pattern to obtain an average of the image input means obtained by photographing. Image output,
An optical quantity distribution measuring method, wherein the aim is set on the aiming figure, and the conversion coefficient between the image input means and an average measurement value of the optical quantity measuring means in the same measurement range is obtained.
【請求項2】計測対象に予め定める照準図形を描くレー
ザビームを照射するレーザスキャナと、このレーザスキ
ャナと同じ位置に設けられ前記照準図形に照準が設定さ
れて平均の輝度を計測する変換係数算出用の光学量計測
手段と、前記レーザスキャナと同じ位置に設けられ前記
照準図形に照準が設定されて前記画像入力手段と同一の
測定範囲を撮影する高精細度で観測可能な画像入力手段
とを備え、前記光学量計測手段の平均的な測定値と、前
記画像入力手段の平均的な画像出力との間の変換係数を
算出するとともに、前記画像入力手段により得られる各
部の部分的出力と前記変換係数とに基づいて、前記計測
対象の各部の輝度を計測することを特徴とする光学量分
布計測装置。
2. A laser scanner for irradiating a laser beam for drawing a predetermined aiming figure on a measurement target, and a conversion coefficient calculation for measuring an average brightness provided at the same position as the laser scanner and aiming at the aiming figure. Optical quantity measuring means for use, and an image input means that is provided at the same position as the laser scanner and has an aiming pattern set on the aiming pattern and that can observe the same measurement range as the image inputting means and that can be observed with high definition. Comprising: calculating a conversion coefficient between an average measurement value of the optical quantity measuring means and an average image output of the image input means, and a partial output of each part obtained by the image input means and the An optical quantity distribution measuring device, characterized in that the brightness of each part of the measurement target is measured based on a conversion coefficient.
JP18922488A 1988-07-26 1988-07-26 Optical quantity distribution measuring method and optical quantity distribution measuring device Expired - Lifetime JPH0617824B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18922488A JPH0617824B2 (en) 1988-07-26 1988-07-26 Optical quantity distribution measuring method and optical quantity distribution measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18922488A JPH0617824B2 (en) 1988-07-26 1988-07-26 Optical quantity distribution measuring method and optical quantity distribution measuring device

Publications (2)

Publication Number Publication Date
JPH0236323A JPH0236323A (en) 1990-02-06
JPH0617824B2 true JPH0617824B2 (en) 1994-03-09

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JP (1) JPH0617824B2 (en)

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US6377400B1 (en) * 1999-07-02 2002-04-23 Milton Bernard Hollander Laser sighting beam modification for measuring or treatment instrument

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JPH0236323A (en) 1990-02-06

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