JPS58214805A - Measuring device of pattern area rate - Google Patents

Measuring device of pattern area rate

Info

Publication number
JPS58214805A
JPS58214805A JP57098339A JP9833982A JPS58214805A JP S58214805 A JPS58214805 A JP S58214805A JP 57098339 A JP57098339 A JP 57098339A JP 9833982 A JP9833982 A JP 9833982A JP S58214805 A JPS58214805 A JP S58214805A
Authority
JP
Japan
Prior art keywords
light
interference filter
printing plate
laser
reflected
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
JP57098339A
Other languages
Japanese (ja)
Inventor
Akihide Saito
斎藤 明秀
Toshiji Fujita
藤田 利治
Masaki Nojima
野島 正樹
Shosuke Fujio
藤生 昌介
Toshiaki Masuda
増田 俊朗
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.)
Toppan Inc
Original Assignee
Toppan Printing 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 Toppan Printing Co Ltd filed Critical Toppan Printing Co Ltd
Priority to JP57098339A priority Critical patent/JPS58214805A/en
Publication of JPS58214805A publication Critical patent/JPS58214805A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/28Measuring arrangements characterised by the use of optical techniques for measuring areas

Abstract

PURPOSE:To improve stability and accuracy in the measurement of pattern area rate in a light room by an apparatus wherein a spherical interference filter selectively transmissible for only the light of laser wavelength is provided in front of a photo detector for detecting the intensity of the reflected light from a printed plate. CONSTITUTION:An interference filter 11 having a characteristic as shown by a curve A is provided in front of a light receiving part 10 of a photo detector 7 to make only the light of laser wavelength transmissible therethrough. The interference filter is shaped into the spherical form which has a radius (r) with the light receiving surface being as the origin. This permits the reflected light to enter the interference filter at a nearly right angle even when a laser spot is scanned over a printed plate from one end to the other end, whereby a shift amount of the spherical characteristic can be restrained to the minimun and the intensity of the reflected laser beam can be made uniform all over the surface of the printed plate. Thus, only the light near the laser wavelength is allowed to pass through the filter and enter the light receiving part 10 without suffering significant influence from the external light, so that the measurement may be always carried out with stability and high accuracy.

Description

【発明の詳細な説明】 この発明はレーザスキャンによる印刷版の絵柄面積率測
定装置に関し特に螢光灯等の点灯した比較的明るい室内
で作業しても#=練外光の影響の受けにくい絵柄面積率
測定装置に関し、明るし・室内で作業可能としたことを
特色とする装置である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for measuring the pattern area ratio of a printing plate using laser scanning, and in particular, even when working in a relatively bright room with fluorescent lights etc. Regarding the area ratio measuring device, this device is characterized by the fact that it is bright and can be operated indoors.

以下、図面に基づき本発明の詳細な説明する。Hereinafter, the present invention will be explained in detail based on the drawings.

第1図は本発明の絵柄面積率測定装置の概略説明図であ
る。
FIG. 1 is a schematic explanatory diagram of a picture area ratio measuring device of the present invention.

レーザ光諒(2)からのレーザビーム(4)はコリメー
タレンズ(3)によりあるビーム径(例えば2×8Mの
隋円ビーム)に調整され、さらにミラー(5)により反
射さハ印刷版(1)に照射される。
The laser beam (4) from the laser beam (2) is adjusted to a certain beam diameter (for example, a 2 x 8M round beam) by a collimator lens (3), and is further reflected by a mirror (5) to the printing plate (1). ) is irradiated.

前記照射さt″Lだレーザビーム(4)は印刷版(11
の程柄により一部は吸収され、一部は乱反射されて受光
素子(7)の受光部uO)に入射される。
The irradiated t''L laser beam (4) is applied to the printing plate (11).
A part of the light is absorbed by the handle, and a part of the light is diffusely reflected and enters the light-receiving portion uO) of the light-receiving element (7).

前記受光素子(7)(例えはフォトマル)は、受光部0
0)に入射さn y、−入射光量乞電気信号に変換し、
この信号ycpU(91に入カイる。
The light-receiving element (7) (for example, a photomultiplier) has a light-receiving section 0.
0) is incident on n y, - the amount of incident light is converted into an electrical signal,
This signal ycpU (enters 91).

CP U t9)は前記電気信号を処理して印刷版(1
)の絵柄面積率?:′S出てる。
CPU t9) processes the electric signal and prints the printing plate (1
) picture area ratio? :'S is out.

しかして印刷版(1)の寸法は最大1200X1360
mとなるためガルバノメーター(6)によりミラー(5
)ヲ回転させて印刷版(1)をスキャンするためには印
刷版m 1・ら受光素子(7)迄の距離はミラー(5)
の振り角か50°〜60°の場合には1220〜146
01EII+とかなりの高さになる。
However, the maximum dimensions of the printing plate (1) are 1200 x 1360
m, so the galvanometer (6) is used to measure the mirror (5
) To scan the printing plate (1) by rotating it, the distance from the printing plate m1 to the light receiving element (7) is the mirror (5).
If the swing angle is 50° to 60°, 1220 to 146
01EII+, which is quite high.

このような大きな装置にて印刷版(1)の絵柄面積率を
演11定する場合にはどうしても例えは螢光灯等照明用
外光の影響を受は易く、そのためレーザスキャンされた
印刷版(11のエリア以外力)らの光(外光)心含めた
反射光量を受光素子(力が受光して、電気信号レベルに
変換している1こめ測定さnた転柄面撹率はノイズを含
んで多く出やすい傾向にあり常に精度良く測定すること
ができない欠点がある−0 上記欠点を改香する手法として転柄面槓王辿1定時に測
定室内を完全に暗室にしてやnは問題な℃・が装置の構
造や作業性の点から好ましい状態ではない。
When determining the image area ratio of the printing plate (1) using such a large device, it is likely to be easily affected by external light for illumination, such as a fluorescent lamp, and therefore the laser scanned printing plate ( The light receiving element (force) receives the reflected light amount including the light (outside light) from outside the area of 11 and converts it into an electrical signal level. There is a drawback that it is difficult to measure accurately at all times as it tends to contain a lot of light. °C is not a desirable condition from the viewpoint of the structure of the equipment and workability.

なぜなら通常、印刷版を測定する時間は30秒ぐらいで
あるため前記時間毎に測定室内を照明すると共に外光遮
蔽板(例えは黒色のカーテン等)を開くとい−った手を
連続して長時間行う事は作業能率を低下させると共に装
着保守の点n・らも長時間完全に外元乞遮断することは
困鼾であり、旦つ経済的でない。
This is because the time it takes to measure a printing plate is usually about 30 seconds. Doing it for a long time reduces work efficiency, and also in terms of installation and maintenance, it is difficult to completely shut off the outside for a long time, and it is not economical.

本発明者は上記の廓に―みて通常の作業条件即ち室内及
び装置内の照明tつけたままで常に安定して精度良く絵
柄面積率を測定できる装置を提供するものである。
In view of the above, the present inventor provides an apparatus that can always measure the picture area ratio stably and accurately under normal working conditions, that is, indoors and with the lights inside the apparatus turned on.

即ち、前述の如く、レーザ(2)からのレーザビームは
コリメータレンズ(3)によりあるビーム径に調整さt
ガルバノメーター(6)によ、り回転制御されるミラー
(5)により反射さf印刷版(1)に2×8膜の隔日ビ
ームで照射さねる。ここで印刷版(1)をスキャンする
構成につ(・てより詳細に述べt″Lは印刷版fIjを
御1足スる際にレーザビームは予じめ印刷版(1)の原
点(121にくるよう設定さfて(・る。
That is, as mentioned above, the laser beam from the laser (2) is adjusted to a certain beam diameter by the collimator lens (3).
The printing plate (1) is irradiated with a 2×8 film beam every other day, which is reflected by a mirror (5) whose rotation is controlled by a galvanometer (6). Here, we will discuss in more detail the configuration for scanning the printing plate (1). It is set so that it comes to (・ru).

前記レーザビームは原点u21よりスタートしてガルバ
ノメーター(6)によりミラー(5)を少しうつ回転さ
せて印刷版(1)の横方向にあるピッチ(例えは1m)
にて送−リスキャンしてゆく。
The laser beam starts from the origin U21 and rotates the mirror (5) slightly downward using a galvanometer (6) to produce a pitch (for example, 1 m) in the lateral direction of the printing plate (1).
Send and rescan.

そして原点力・ら印刷版(1)の横方向の端までスキャ
ンし1こらパルスモータ(8)ヲ駆動させてガルレノく
ノメータ(6)とミラー(5) ?:載會し−て(・る
円板を回転させて印刷版(1)の天地方向にあるピッチ
(例えば5mm)にて送る。
Then, the origin force scans the printing plate (1) to the lateral edge, and then the pulse motor (8) is driven to move the gallenometer (6) and mirror (5). : The disk is rotated and fed at a certain pitch (for example, 5 mm) in the vertical direction of the printing plate (1).

この際レーザビームは同時にガルバノメータ(6)によ
りミラー(5)を回転させて印刷版の原点側p端に移動
させる。
At this time, the laser beam is simultaneously rotated by a galvanometer (6) to move the mirror (5) to the p end on the origin side of the printing plate.

そして前回同様に印刷版の横方向をあるピッチ(例えは
1關)にてスキャンしてゆく。
Then, like last time, the printing plate is scanned in the horizontal direction at a certain pitch (for example, one step).

こ九乞繰返して印刷版全体をスキャンする。Scan the entire print version repeatedly.

以上の様に印刷版をスキャンしたレーザビームは印刷版
の表面にて一部は吸収さn、一部は乱反射されて印刷版
(1)の上方に置かnて(・る受光素子(7)の受光部
(10)に人射さnる。
As described above, the laser beam that scans the printing plate is partially absorbed by the surface of the printing plate, and part is diffusely reflected and placed above the printing plate (1). Human radiation is emitted onto the light receiving section (10) of the light receiving section (10).

ここで印刷版(主としてホジタイプのPS版)の感光層
の色はシアン、グリーンか主に使用されている。
Here, the color of the photosensitive layer of the printing plate (mainly a photosensitive type PS plate) is mainly cyan or green.

従って画線部は前記感光層の色を呈しており非画線部は
前記感光層が除去さnて砂目型てされTこアルミニウム
素地の色乞呈している。
Therefore, the image area has the color of the photosensitive layer, and the non-image area has the photosensitive layer removed and is grained, giving it the color of the aluminum substrate.

従って、レーザ光源(2)としてHe−Ne(波長63
28X)等を用いた場合、前記レーザビームの入射光量
は画線部では殆んど吸収されると共に非mm部では前記
砂目型ての素地により乱反射さnる。オフセット印刷版
は網点の大小により色の階調をつけている為にノ・イラ
イト部では画勝部に相当する網点は少ないために乱反射
される量は多くなり逆にシャドウ部ではimm部に相当
する網点面積は大きくなるために乱反射さ/れる量は少
なくなる。
Therefore, as the laser light source (2), He-Ne (wavelength 63
28X), etc., the incident light amount of the laser beam is almost absorbed in the image area, and is diffusely reflected by the grained substrate in the non-mm area. Offset printing plates have color gradation based on the size of the halftone dots, so in the light and bright areas there are fewer halftone dots that correspond to the bright areas, so the amount of diffused reflection increases, and conversely, in the shadow areas, the amount of diffused reflection increases. Since the corresponding halftone dot area becomes larger, the amount of diffused reflection becomes smaller.

従って、乱反射さfる量を受光素子にて受光してJ?F
nは印刷版の転柄面槓率乞両定することができる。
Therefore, if the amount of diffused reflection f is received by the light receiving element, J? F
n can be determined depending on the rate of printing.

ここで前記乱反射さtた光量を受光する際にレーザ波長
(例え1dHe−Neでは6328 ;−’ )の他に
装置内や室内の蛍光灯からの外光も受光してしまうため
に常に安定して精度良く辿j定することができなくなる
Here, when receiving the amount of diffusely reflected light, in addition to the laser wavelength (for example, 6328;-' for 1 dHe-Ne), external light from the fluorescent lamp inside the device or indoors is also received, so it is not always stable. Therefore, it becomes impossible to trace accurately.

そこで受光素子(7)の受光部tlolの前面に第2図
の曲線Aに示すような特性の干渉フィルター旧)を設は
レーザ波長のみを選択的に透過させるようにしたもので
ある。
Therefore, in front of the light receiving portion tlol of the light receiving element (7), an interference filter having characteristics as shown in curve A in FIG. 2 is provided to selectively transmit only the laser wavelength.

ここで前記干渉フィルターの形状が重要である。Here, the shape of the interference filter is important.

第2図に於いて曲線Aに示される波長6528Xにピー
クを持つ特性の分光感度分布を有する干渉フィルターを
受光素子(力の前に設置した場合、第3図(a+に示さ
れるように干渉フィルター■)に対し、直角に入射さn
る光量に関しては第2図の曲#!Aの分光特性によりレ
ーザー波長例えは6328X近辺の元は透過させるがそ
の他の波長はすべてカットされる。
If an interference filter with a characteristic spectral sensitivity distribution having a peak at wavelength 6528 ■) is incident at right angles to n
Regarding the amount of light, please refer to the song #! in Figure 2. Due to the spectral characteristics of A, laser wavelengths around 6328X are transmitted, but all other wavelengths are cut off.

しn)シ、第3図fblに示されるように、糾めから入
射さnる光に対しては、干渉フィルター旧)は第2図の
曲MAの分光特性力)らシフトしてしま(・、第2図1
の曲線Bの分光特性のものになってしまう。
As shown in Figure 3 fbl, for the light incident from the filter, the interference filter (old) shifts from the spectral characteristic of the song MA in Figure 2 (・, Figure 2 1
The spectral characteristics will be that of curve B.

実際レーザスポットは印刷版の端から端まで移動してい
るため前記レーザスホノトの印刷版力)らの反射−光は
干渉フィルターに入射する際には第3図(alの如くす
べて直角に入射するのではなく第3図(blの如く種々
の角度で入射じてくる。
In fact, since the laser spot moves from one end of the printing plate to the other, the reflected light from the printing plate force of the laser beam is incident on the interference filter as shown in Figure 3 (al). Rather, they are incident at various angles as shown in Figure 3 (bl).

従って光が入射してくる角度により干渉フィルターの分
光特性は変蛎してしまうため印刷版(1)ハ・らの反射
光量を正確に受光できなくなる欠点を有する。
Therefore, the spectral characteristics of the interference filter vary depending on the angle at which the light is incident, so that the interference filter has the disadvantage that it cannot accurately receive the amount of light reflected from the printing plate (1).

例えは、干渉フィルターの半値巾が80〜100λのも
のを使用した場合、干渉フィルターに入射する印刷版か
らの乱反射光の入射角が45°の場合には分光特注が短
波長側に約100久シフトしてしまい6328′iの信
号光であるレーザービーム反射光量Yx%にまで減衰さ
せてしまう現家か発生する。
For example, when using an interference filter with a half-width of 80 to 100λ, if the incident angle of the diffusely reflected light from the printing plate that enters the interference filter is 45°, the spectroscopic customization will shift approximately 100 degrees to the short wavelength side. This causes the signal light of 6328'i, which is the signal light of the laser beam, to be attenuated to Yx% in the amount of reflected light.

そこで干渉フィルターの形状を第3図FC+の様に受光
面を原点にして半径rの球面形状に丁nは印に分光特性
のシフト童を極力抑えることができレーザビームの反射
光量を印刷版全面にわたって均一化させることができる
Therefore, the shape of the interference filter is changed to a spherical shape with the light receiving surface as the origin and the radius r as shown in Figure 3 FC+.The shift of the spectral characteristics can be suppressed as much as possible, and the amount of reflected light of the laser beam can be reduced to the entire surface of the printing plate. can be made uniform over the entire range.

従って、読取り精度が向上し、且つ受光部に入る光量は
レーザ波長近辺のものだけが透過されるために外光(主
として螢光灯)の影響ば殆んど無視できるレベルに抑え
ることができ、−宮に安定して精度良く測定イることが
又きる。
Therefore, the reading accuracy is improved, and since only light near the laser wavelength is transmitted through the light receiving section, the influence of external light (mainly fluorescent lamps) can be suppressed to a level that can be almost ignored. - It is possible to perform stable and accurate measurements again.

更に螢光灯等の外光をシアンやグリーン等のフィルター
で被覆させてやnはより完全に外光な除去することがで
きる。
Furthermore, by covering external light such as from a fluorescent lamp with a cyan or green filter, it is possible to remove external light more completely.

なお、干渉フィルターの半径rは取付位置及び印刷版と
受光素子の受光部の大きさ等により決定されるものであ
る。
Note that the radius r of the interference filter is determined by the mounting position, the size of the printing plate and the light-receiving portion of the light-receiving element, etc.

本発明は以上の如き構成であるから下記に示す如き優れ
た効果を有イる。
Since the present invention has the above structure, it has excellent effects as shown below.

即ち、本発明に於いてはレーザ光源ヲ使用して印刷版の
版面の網点面積率を辿1定する定め印刷版面の濃度差の
かなり小さな部分に於ける画線部と非画線部の比率を精
度良く測定できる。
That is, in the present invention, a laser light source is used to trace and determine the halftone dot area ratio on the printing plate surface, and to determine the density difference between the printed area and the non-printed area in a portion of the printing plate surface where the difference in density is quite small. The ratio can be measured with high accuracy.

さらにレーザ光源と干渉フィルターを用いろfこめ比較
的明る(・室内に於(・てもそn等の外光の影響がなく
作業ができるため通常の作業環境下に於(・ても作業で
きこ乙により極めて作業効率の高(・装置とすることが
できる、 また、干渉フィルターを球面形状とし1こため、信号光
であるレーザービ一台、の反射光を印刷版全面に於いて
均一に透過させることができ、より一層測定精度を向上
せしめることができるものであ
Furthermore, by using a laser light source and an interference filter, it is possible to work in a relatively bright room (even in a normal work environment) without being affected by outside light. In addition, the interference filter has a spherical shape, so that the reflected light from the laser beam, which is the signal light, is transmitted uniformly over the entire surface of the printing plate. It is possible to further improve measurement accuracy.

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

図面は本発明の一実施例を示すものであり、第1図は本
装置の概略説明図、第2図は干渉フィルターの特性図、
第6図は干渉フィルターの説明図である。 (1)・・・印刷版  (2)・・・レーザ光源(31
・・・コ11メータレンズ  (4)−・・レーザビー
ム  +5)−°゛ミラー6)・・ガルバノメーター 
 (7)・・・受光素子  (9)・・・cPU   
QO)・・・受光部  旧)・・干渉フィルター特許出
願人 凸版印刷株式会社 代表者鈴木相夫 グー+4\ (− 第1図 第2図
The drawings show one embodiment of the present invention; FIG. 1 is a schematic explanatory diagram of the present device, FIG. 2 is a characteristic diagram of an interference filter,
FIG. 6 is an explanatory diagram of the interference filter. (1)...Printing plate (2)...Laser light source (31
... 11 meter lens (4) -... Laser beam +5) -°゛mirror 6)... Galvanometer
(7)...Photodetector (9)...cPU
QO) ... Light receiving section Old) ... Interference filter Patent applicant Toppan Printing Co., Ltd. Representative Aio Suzuki Goo +4\ (- Figure 1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 印刷版にレーザ光を照射してその反射光量を受光して印
刷版の絵柄面at率を測定する装置に於(・て、前記印
刷版からの反射光量を受光する受光素子の前にレーザ光
の波長を選択的に透過する球面形状の干渉フィルターを
設けたことを特徴とする絵柄面積率測定装置。
In a device that measures the pattern surface at ratio of a printing plate by irradiating a laser beam onto a printing plate and receiving the amount of reflected light, a laser beam is placed in front of a light-receiving element that receives the amount of reflected light from the printing plate. A pattern area ratio measuring device characterized by being provided with a spherical interference filter that selectively transmits wavelengths of .
JP57098339A 1982-06-08 1982-06-08 Measuring device of pattern area rate Pending JPS58214805A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57098339A JPS58214805A (en) 1982-06-08 1982-06-08 Measuring device of pattern area rate

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57098339A JPS58214805A (en) 1982-06-08 1982-06-08 Measuring device of pattern area rate

Publications (1)

Publication Number Publication Date
JPS58214805A true JPS58214805A (en) 1983-12-14

Family

ID=14217140

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57098339A Pending JPS58214805A (en) 1982-06-08 1982-06-08 Measuring device of pattern area rate

Country Status (1)

Country Link
JP (1) JPS58214805A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63167246U (en) * 1987-04-22 1988-10-31
JP2013019790A (en) * 2011-07-12 2013-01-31 Ihi Corp Laser radar device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63167246U (en) * 1987-04-22 1988-10-31
JP2013019790A (en) * 2011-07-12 2013-01-31 Ihi Corp Laser radar device

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