JPH07103741A - Method for quantifying roughness of gloss surface - Google Patents

Method for quantifying roughness of gloss surface

Info

Publication number
JPH07103741A
JPH07103741A JP26991693A JP26991693A JPH07103741A JP H07103741 A JPH07103741 A JP H07103741A JP 26991693 A JP26991693 A JP 26991693A JP 26991693 A JP26991693 A JP 26991693A JP H07103741 A JPH07103741 A JP H07103741A
Authority
JP
Japan
Prior art keywords
sample surface
dark
light
sample
slit
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
JP26991693A
Other languages
Japanese (ja)
Inventor
Hiroshi Tajima
洋 田島
Kura Tomita
蔵 富田
Shinichi Nagata
紳一 永田
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.)
New Oji Paper Co Ltd
Original Assignee
New Oji Paper 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 New Oji Paper Co Ltd filed Critical New Oji Paper Co Ltd
Priority to JP26991693A priority Critical patent/JPH07103741A/en
Publication of JPH07103741A publication Critical patent/JPH07103741A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain an objective evaluation value matched to man's senses without constituting an apparatus strictly, by photographing a sample surface from vertically above while illuminating the sample surface by means of a light slantwise, and processing an obtained signal of a bright-and-dark distribution through a frequency analysis. CONSTITUTION:A surface of a sample S set on a sample stage 2 is irradiated through a slit 5 by a light from a light source 3 passing through an optical fiber flux 4. The sample surface is illuminated slantwise by a lower half of the luminous flux. A dark-and-bright image along a line on the sample surface parallel to the slit 5 is photographed by a camera 6 from vertically above at a position slightly retreated from a position where a lower side of the luminous flux crosses the sample surface. An output of the camera 6 is stored in a memory 7 and also displayed at a monitor screen 8. A data-processing device 9 obtains data of a spectral distribution of frequencies of the dark-and-bright image by Fourier-transforming a video signal. When a ratio of an area of a high frequency region on the spectrum to that, of an intermediate frequency region is obtained, a quantitative result with good reproducibility not influenced by a change of the illuminating direction or photographing position is obtained.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、光沢紙等のいわゆる
「ボコツキ」、すなわち光沢面の不規則かつなだらかな
肉眼的凹凸或は面の局部的傾斜の程度の定量化方法に関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a so-called "pimple" of glossy paper or the like, that is, a method for quantifying the degree of irregular and gentle macroscopic unevenness of the glossy surface or the local inclination of the surface.

【0002】[0002]

【従来の技術】タック紙は紙面に光沢シートを貼着した
光沢紙であるが、不規則な細かい波打ちが見られる。光
沢紙の表面は鏡のように平滑であることが理想であるの
で、上述したような波打ちを低減させる努力が色々なさ
れているが、その効果を適切に評価することは製造行程
の改善,品質管理上からも重要である。しかし従来はこ
の波打ち凹凸の評価は目視検査によるランク分けで行わ
れているに過ぎなかった。
2. Description of the Related Art Tack paper is a glossy paper in which a glossy sheet is attached to the paper surface, but irregular fine waviness is observed. Since it is ideal that the surface of glossy paper be smooth like a mirror, various efforts have been made to reduce the waviness as described above, but it is important to properly evaluate the effect to improve the manufacturing process and quality. It is also important for management. However, conventionally, the evaluation of the corrugated unevenness has been performed only by ranking by visual inspection.

【0003】[0003]

【発明が解決しようとする課題】本発明は光沢紙等の光
沢面の凹凸や局部的傾斜の程度を定量化して表示しよう
とするものである。この際その定量化の結果は従来の目
視判定と傾向的に一致すべきものである。
SUMMARY OF THE INVENTION The present invention is intended to quantify and display the degree of unevenness or local inclination of a glossy surface of glossy paper or the like. At this time, the result of the quantification should be consistent with the conventional visual judgment.

【0004】[0004]

【課題を解決するための手段】試料面を斜め方向から光
で照射し、照射された試料面を垂直方向から撮像し、得
られた明暗の分布信号を周波数分析して周波数と明暗の
振幅との関係つまり明暗のスペクトルデータを求め、こ
のスペクトルにおいて、高い周波数域の一定周波数範囲
の面積に対する中間周波数域の他の一定周波数範囲の面
積の比を以って試料面の凹凸の定量値とする。
[Means for Solving the Problems] A sample surface is irradiated with light from an oblique direction, the irradiated sample surface is imaged from a vertical direction, and the obtained distribution signal of brightness and darkness is subjected to frequency analysis to determine the frequency and the amplitude of the brightness and darkness. Relationship, that is, light and dark spectrum data, and in this spectrum, the quantitative value of the unevenness of the sample surface is determined by the ratio of the area of the constant frequency range of the high frequency range to the area of the other constant frequency range of the intermediate frequency range. .

【0005】[0005]

【作用】試料面を斜め照射することによって試料面の凹
凸による明暗が強調され、凹凸を明暗に変換したデータ
が得易くなる。試料面の凹凸は低い周波数から高い周波
数まで分布しているが、人間の目に凹凸として感じられ
る周波数は中間域にあり、低い明暗周期は試料面の曲が
りとして感じ、高い周波数の明暗に対しては凹凸を感じ
ない。従って明暗信号を周波数分析して得られた明暗ス
ペクトルにおいて、中間周波数域の明暗振幅を以って凹
凸の定量値としてもよいように思われるが、斜め照射し
ているので明暗の振幅は照射角度の変化によって敏感に
変化し、また試料面上のどの線に沿って撮像するかとい
う撮像位置によっても変化するから、単なる中間周波数
域の明暗振幅の絶対値では凹凸程度の絶対値を表わし得
ない。しかし高い周波数域も中間周波数域も照射方向と
か撮像位置に関して同じ影響を受けているので、スペク
トル上の高周波域の面積と中間周波数域の面積比を取る
ことにより、上記した照射方向とか撮像位置の変化の影
響を受けない再現性のよい定量結果が得られるのであ
る。
By obliquely irradiating the sample surface, the light and dark due to the unevenness of the sample surface is emphasized, and it becomes easy to obtain data in which the unevenness is converted into light and dark. The unevenness of the sample surface is distributed from low frequency to high frequency, but the frequency that human eyes perceive as unevenness is in the middle range, and the low light-dark cycle is felt as the bending of the sample surface, and it is against the high frequency light and dark. Does not feel unevenness. Therefore, in the light-dark spectrum obtained by frequency-analyzing the light-dark signal, it seems that the light-dark amplitude in the intermediate frequency range may be used as the quantitative value of the unevenness, but since the oblique irradiation is performed, the light-dark amplitude is the irradiation angle. Change sensitively depending on the change in the image, and also change depending on the imaging position such as along which line on the sample surface the image is picked up. Therefore, the absolute value of the light and dark amplitude in the intermediate frequency range cannot express the absolute value of unevenness. . However, since the high frequency region and the intermediate frequency region are affected by the irradiation direction and the imaging position in the same manner, by taking the area ratio of the high frequency region and the intermediate frequency region on the spectrum, Therefore, quantitative results with good reproducibility that are not affected by changes can be obtained.

【0006】[0006]

【実施例】図1に本発明方法を実行する装置の一例を示
す。1は試料ステージで試料台をx,y2方向に自由に
移動させる。試料台2上に試料Sが置かれる。3は光源
のランプで、その光はオプチカルファイバー束4を通し
て照射スリット5に導かれ、スリット5から試料面に放
射される。スリット5から放射される光は中心光線が試
料面と平行で、上下に夫々30°の範囲で広がる光束
で、試料面はこの光束の下半分の部分によって斜め照射
され、図1のBに示すようにこの光束の下辺が試料面を
切る位置より1〜2cm後退した位置でスリット5と平
行な試料面上の線に沿う明暗像が試料面の垂直上方のカ
メラ6によって撮像される。カメラ6にセットされてい
る撮像素子は1次元イメージセンサで、その出力は画像
メモリ7に格納される。この格納された1次元映像信号
はモニタ画面8に表示されるようになっている。9はデ
ータ処理装置で、画像メモリ7に格納された映像信号に
対してデータ処理を行い、その結果を表示する。
FIG. 1 shows an example of an apparatus for carrying out the method of the present invention. A sample stage 1 freely moves the sample table in the x and y2 directions. The sample S is placed on the sample table 2. Reference numeral 3 is a lamp of a light source, and the light is guided to an irradiation slit 5 through an optical fiber bundle 4 and emitted from the slit 5 to the sample surface. The light emitted from the slit 5 is a light beam whose central ray is parallel to the sample surface and spreads up and down in the range of 30 °, and the sample surface is obliquely illuminated by the lower half part of this light beam, as shown in FIG. 1B. As described above, at the position where the lower side of this light flux is retracted by 1 to 2 cm from the position where the lower side of the sample surface is cut, a bright-dark image along the line on the sample surface parallel to the slit 5 is captured by the camera 6 vertically above the sample surface. The image pickup device set in the camera 6 is a one-dimensional image sensor, and the output thereof is stored in the image memory 7. The stored one-dimensional video signal is displayed on the monitor screen 8. A data processing device 9 performs data processing on the video signal stored in the image memory 7 and displays the result.

【0007】データ処理装置は以下述べるようなデータ
処理を行う。画像メモリには試料面上の一つの線に沿う
明暗の映像信号が格納されている。これを図2Aに示
す。この図で明暗分布が中高になっているのは試料両縁
近くで照射光の照度が低下していることによる。図2A
に示す映像信号をフーリェ変換することにより明暗の周
波数の分布データ即ち明暗周波数のスペクトル分布デー
タを得る。図2Bにこのスペクトルを示す。色々な紙に
ついてこのスペクトルを見ると、低い周波数における明
暗振幅が大きく、高い周波数域(波長で表わして3mm
以上)では振幅分布は一定になると云う同じ傾向を示し
ていることが判明した。そして目視上凹凸が多いものと
少いものとでは中間周波数域(波長にして6〜3mmの
範囲)での明暗振幅の差が大きいことが判明した。そこ
で図2Bに示すスペクトルにおいて波長にして1.2〜
0.6mmの範囲の面積Hに対する波長6〜3mmの範
囲の面積Dの比を算出し、これを凹凸度として表示す
る。即ち凹凸度=D/Hである。
The data processing device performs data processing as described below. The image memory stores bright and dark video signals along one line on the sample surface. This is shown in Figure 2A. In this figure, the light-dark distribution is moderately high because the illuminance of the irradiation light is low near both edges of the sample. Figure 2A
By performing Fourier transform on the video signal shown in (1), light-dark frequency distribution data, that is, light-dark frequency spectrum distribution data is obtained. This spectrum is shown in FIG. 2B. Looking at this spectrum on various papers, the light and dark amplitudes at low frequencies are large, and the high frequency range (3 mm in terms of wavelength)
In the above), it has been found that the same tendency that the amplitude distribution becomes constant is shown. Then, it was found that the difference between the bright and dark amplitudes in the intermediate frequency range (6 to 3 mm wavelength range) was large between the one having a large number of irregularities and the one having a small number of irregularities. Therefore, in the spectrum shown in FIG.
The ratio of the area D in the wavelength range of 6 to 3 mm to the area H in the 0.6 mm range is calculated and displayed as the degree of unevenness. That is, the degree of unevenness = D / H.

【0008】上述のようにして得られた凹凸度と同じ試
料の目視判定によるランク分けとの対応関係を下に示
す。試料はキャスト紙でAからDに向かって目視の凹凸
度が大きくなっている。また対照として上質紙(光沢処
理なし、目視ランクはA)についての結果も示す。 目視評価 D H D/H A 24899 32125 0.775 B 36845 29567 1.25 C 46912 28165 1.66 D 47105 26232 1.8 上質 100231 158352 0.633 この結果から本発明方法による評価値は人間の感覚的評
価と良く一致していることが分かる。
The correspondence between the degree of unevenness obtained as described above and the rank classification of the same sample by visual judgment is shown below. The sample is cast paper, and the degree of unevenness in visual observation increases from A to D. As a control, the results for high-quality paper (no gloss treatment, visual rank A) are also shown. Visual evaluation DH D / HA A 24899 32125 0.775 B 36845 29567 1.25 C 46912 28165 1.66 D 47105 26232 1.8 Fine quality 100231 158352 0.633 From this result, the evaluation value by the method of the present invention is human sense. It turns out that it agrees well with the physical evaluation.

【0009】[0009]

【発明の効果】本発明によれば、スペクトルの高周波域
の面積と中間周波域の面積との比を採ることで、装置構
成を厳格にする必要なしに安定した結果を得ることがで
きて、方法の実施が容易であり、測定結果は目視評価と
良く一致しているので、光沢面の凹凸について安定して
客観的でしかも人間の感覚ともマッチした評価値が得ら
れる。
According to the present invention, by taking the ratio of the area of the high frequency region of the spectrum and the area of the intermediate frequency region, it is possible to obtain stable results without the need to make the device structure strict. Since the method is easy to carry out and the measurement results are in good agreement with the visual evaluation, it is possible to obtain an evaluation value that is stable and objective with respect to the unevenness of the glossy surface and that matches the human sense.

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

【図1】本発明方法を実施する装置の一例の斜視図FIG. 1 is a perspective view of an example of an apparatus for carrying out the method of the present invention.

【図2】上記装置による測定結果のグラフFIG. 2 is a graph of measurement results obtained by the above device

【符号の説明】[Explanation of symbols]

1 試料ステージ 2 試料台 S 試料 3 光源 4 オプチカルファイバー束 5 スリット 6 カメラ 7 画像メモリ 8 モニタ画面 9 データ処理装置 1 sample stage 2 sample stage S sample 3 light source 4 optical fiber bundle 5 slit 6 camera 7 image memory 8 monitor screen 9 data processing device

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】試料面を斜め方向から光で照射し、照射さ
れた試料面を垂直上方から撮像し、得られた明暗の分布
信号を周波数分析して明暗のスペクトルデータを求め、
このスペクトルにおいて、高い周波数域の一定周波数範
囲の面積に対する中間周波数域の他の一定周波数範囲の
面積の比を以って凹凸度とする光沢面の凹凸定量化方
法。
1. A sample surface is irradiated with light from an oblique direction, the irradiated sample surface is imaged from above vertically, and the obtained light-dark distribution signal is frequency-analyzed to obtain light-dark spectrum data.
In this spectrum, a method for quantifying unevenness of a glossy surface, wherein the unevenness degree is defined as a ratio of an area of a constant frequency range of a high frequency range to an area of another constant frequency range of an intermediate frequency range.
JP26991693A 1993-09-30 1993-09-30 Method for quantifying roughness of gloss surface Pending JPH07103741A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26991693A JPH07103741A (en) 1993-09-30 1993-09-30 Method for quantifying roughness of gloss surface

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26991693A JPH07103741A (en) 1993-09-30 1993-09-30 Method for quantifying roughness of gloss surface

Publications (1)

Publication Number Publication Date
JPH07103741A true JPH07103741A (en) 1995-04-18

Family

ID=17479006

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26991693A Pending JPH07103741A (en) 1993-09-30 1993-09-30 Method for quantifying roughness of gloss surface

Country Status (1)

Country Link
JP (1) JPH07103741A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112146598A (en) * 2020-08-13 2020-12-29 领胜城科技(江苏)有限公司 Quick flatness detection machine

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112146598A (en) * 2020-08-13 2020-12-29 领胜城科技(江苏)有限公司 Quick flatness detection machine

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