JPH0224458B2 - - Google Patents
Info
- Publication number
- JPH0224458B2 JPH0224458B2 JP25353084A JP25353084A JPH0224458B2 JP H0224458 B2 JPH0224458 B2 JP H0224458B2 JP 25353084 A JP25353084 A JP 25353084A JP 25353084 A JP25353084 A JP 25353084A JP H0224458 B2 JPH0224458 B2 JP H0224458B2
- Authority
- JP
- Japan
- Prior art keywords
- glossiness
- gloss
- visual
- boundary line
- determining
- 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
Links
- 238000000034 method Methods 0.000 claims description 21
- 230000000007 visual effect Effects 0.000 claims description 12
- 230000006870 function Effects 0.000 claims description 8
- 230000016776 visual perception Effects 0.000 claims description 4
- 239000006185 dispersion Substances 0.000 claims description 2
- 230000003746 surface roughness Effects 0.000 description 7
- 239000010960 cold rolled steel Substances 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 230000004907 flux Effects 0.000 description 3
- 229910000831 Steel Inorganic materials 0.000 description 2
- 239000003086 colorant Substances 0.000 description 2
- 230000000052 comparative effect Effects 0.000 description 2
- 239000010959 steel Substances 0.000 description 2
- 241001507928 Aria Species 0.000 description 1
- 235000004494 Sorbus aria Nutrition 0.000 description 1
- 238000005311 autocorrelation function Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000002265 prevention Effects 0.000 description 1
- 230000035807 sensation Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/55—Specular reflectivity
- G01N21/57—Measuring gloss
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/30—Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces
- G01B11/303—Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces using photoelectric detection means
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N2021/4704—Angular selective
- G01N2021/4711—Multiangle measurement
- G01N2021/4716—Using a ring of sensors, or a combination of diaphragm and sensors; Annular sensor
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/55—Specular reflectivity
- G01N2021/555—Measuring total reflection power, i.e. scattering and specular
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/55—Specular reflectivity
- G01N2021/556—Measuring separately scattering and specular
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/314—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
【産業上の利用分野】
本発明は、物体表面の光沢度判定方法に係り、
特に、鋼板の表面品質を計測して管理する際に用
いるのみに好適な、物体表面の光反射強度分布に
より、その視感に基づく光沢度を分類、等級付け
する物体表面の光沢度判定度方法の改良に関す
る。[Industrial Application Field] The present invention relates to a method for determining the glossiness of an object surface,
In particular, a method for determining the glossiness of an object's surface that classifies and grades the glossiness based on the visual sensation based on the light reflection intensity distribution on the object's surface, which is suitable only for measuring and managing the surface quality of steel plates. Regarding the improvement of
物体表面の光沢度を定める方法として、従来よ
り種々の光反射測定による方法が提案されてお
り、代表的なものとしては、一定角度で投射した
白色光束の正反射強度を測定する鏡面光沢度によ
る方法、一定角度で投射した白色光の正反射強度
と拡散反射強度の比を用いる対比光沢度による方
法、及び表面に他の物体を映し、その反射像のぼ
けを肉眼で見る鮮明光沢度による方法がある。
As a method for determining the glossiness of an object's surface, various methods using light reflection measurements have been proposed in the past.A typical method is based on specular glossiness, which measures the specular reflection intensity of a white beam projected at a fixed angle. method, a contrast gloss method that uses the ratio of specular reflection intensity and diffuse reflection intensity of white light projected at a certain angle, and a clear gloss method that reflects another object on the surface and observes the blurring of the reflected image with the naked eye. There is.
しかしながら、前記鏡面光沢度による方法は、
広く工業的に用いられているが、表面粗さの小さ
い鏡面的対象について実際と一致しないという欠
点を有する。又、前記対比光沢度による方法は、
色の異なる対象に対しても視感に近い光沢度を与
えるという特徴を有するが、これも又鏡面に近い
対象について判定精度が低くなる傾向にある。
However, the method based on specular gloss,
Although it is widely used industrially, it has the disadvantage that it does not match reality for specular objects with small surface roughness. In addition, the method using the comparative glossiness,
Although it has the characteristic of giving a gloss level close to visual perception even to objects of different colors, it also tends to have low determination accuracy for objects that are close to mirror surfaces.
しかしながら、前記鏡面光沢度による方法は、
広く工業的に用いられているが、表面粗さの小さ
い鏡面的対象について実際と一致しないという欠
点を有する。又、前記対比光沢度による方法は、
色の異なる対象に対しても視感に近い光沢度を与
えるという特徴を有するが、これも又鏡面に近い
対象については判定精度が低くなる傾向にある。
更に、前記鮮明光沢度による方法は、定量的な
表示が得られないという問題点を有していた。
However, the method based on specular gloss,
Although it is widely used industrially, it has the disadvantage that it does not match reality for specular objects with small surface roughness. In addition, the method using the comparative glossiness,
Although it has the characteristic of giving a gloss level close to visual perception even to objects of different colors, the determination accuracy also tends to be low for objects that are close to mirror surfaces. Furthermore, the method using the sharp glossiness has a problem in that a quantitative display cannot be obtained.
本発明は、前記従来の問題点を解消するべくな
されたもので、同一色(明度は異なつてもよい)
の対象について、目視光沢度に良く一致し、且
つ、鏡面から粗面までの広い粗度範囲に亘つて定
量的に光沢度を定めることができる物体表面の光
沢度判定方法を提供することを目的とする。
The present invention was made to solve the above-mentioned conventional problems, and has the same color (brightness may be different).
The purpose of the present invention is to provide a method for determining the glossiness of the surface of an object that closely matches the visual glossiness and that can quantitatively determine the glossiness over a wide roughness range from specular to rough surfaces. shall be.
本発明は、物体表面の光反射強度分布により、
その視感に基づく光沢度を分類、等級付けする物
体表面の光沢度判定方法において、第1図にその
要旨を示す如く、被測定表面プロフイルの高さ分
布の分散σが次式の関係
{(4πσ/λ1)・cosθ1}2≦1 …(1)
{(4πσ/λ2)・cosθ2}2≧4 …(2)
を満足するような波長λ1,λ2(λ1=λ2も含む)の
光束を、それぞれ入射角θ1,θ2で投射し、各々の
正反射強度I1,I2及び全反射強度S1,S2を検出
し、予め2次元平面(I1/S1,I2/S2)上に各目
視光沢度を統計的に充分表わすサンプル数をプロ
ツトし、2次元平面に存在する複数の光沢度群に
ついて、各々の隣り合う光沢度群間の重なりが最
小となるような判別関数である境界線Zを定めて
おき、該境界線Zにより、任意の被測定物の光沢
度を分別するようにして、前記目的を達成したも
のである。
ここで、正反射強度Iとは、第6図及び次式に
示す如く、入射光の入射角θに対して、光学的な
正反射方向(α=0)の微小領域の光束の強度を
意味する。
I=∫+〓-〓i(θ)dθ
i(θ):反射光束の分布
α:受光角(正反射方向α=0)
又、全反射強度Sとは、第6図及び次式に示す
如く、入射光に対して、光学的に反射する光束の
全方向にわたつて積分された全強度を意味する。
S=∫〓〓-〓〓i(θ)dθ
The present invention uses the light reflection intensity distribution on the object surface to
In a method for determining glossiness of an object's surface that classifies and ranks glossiness based on visual perception, as shown in Figure 1, the variance σ of the height distribution of the surface profile to be measured is expressed by the following equation {( 4πσ/λ 1 )・cosθ 1 } 2 ≦1 …(1) {(4πσ/λ 2 )・cosθ 2 } 2 ≧4 …(2) Wavelengths λ 1 , λ 2 (λ 1 = λ 2 ) are projected at incident angles θ 1 and θ 2 respectively, and the specular reflection intensities I 1 and I 2 and total reflection intensities S 1 and S 2 are detected . /S 1 , I 2 /S 2 ), plot the number of samples that statistically sufficiently represent each visual gloss level, and calculate the difference between each adjacent gloss level group for multiple gloss levels existing on a two-dimensional plane. The above object is achieved by determining a boundary line Z, which is a discriminant function that minimizes the overlap, and using the boundary line Z to classify the glossiness of any object to be measured. Here, the specular reflection intensity I means the intensity of the luminous flux in a minute area in the optical specular reflection direction (α=0) with respect to the incident angle θ of the incident light, as shown in Fig. 6 and the following equation. do. I=∫ + 〓 - 〓i(θ)dθ i(θ): Distribution of reflected light flux α: Receiving angle (direction of regular reflection α=0) Also, the total reflection intensity S is shown in Fig. 6 and the following formula , it means the total intensity integrated over all directions of the optically reflected light beam with respect to the incident light. S=∫〓〓 - 〓〓i(θ)dθ
本発明は、物体、例えば鋼板表面の目視光沢度
が、平均粗さ及び平均山間隔の2つの表面粗度パ
ラメータに依存し、平均粗さのみでは評価できな
いことに着目してなされたものである。
即ち、ほぼ同一色の対象物の光沢を決める主要
因として表面粗さがあり、基本的には該表面粗さ
の情報を的確に把握することにより、光沢度を評
価できると考えられる。
表面粗さの情報は、概括的には、表面プロフイ
ルの高さ分布の分散σと、自己相関距離T(自己
相関関数が1/eとなる距離)で表現でき、これ
らの量と光反射強度分布には、例えば1963年に
Pergamon Pressより発行された、P.Beckmann
とA.Spizzichino著“The Scattering of
Electromagnetic Waves from Rough
Surfaces”に示される如く、一定の関係がある。
更に、「鉄と鋼、70巻(1984)」の1095頁以降に
掲載された、浅野有一郎他による、これらの関係
の詳細な検討結果に従えば、前出(1),(2)式の各範
囲を満すことにより、各々の条件による正反射強
度I1,I2は、粗度パラメータσ及びTと次式の関
係にある。
I1=f1(σ) …(3)
I2=f2(σ,T) …(4)
但し、入射光強度を単位強度、全反射率を1と
している。
ここで、全反射率を考慮に入れれば、前出(3),
(4)式の左辺は各々、I1/S1,I2/S2(S1,S2は、
(1),(2)式の各条件における全反射強度)に置き換
えられ、粗度パラメータσ及びTの情報は、I1/
S1,I2/S2の両情報に確実に含まれている。従つ
て、I1/S1,I2/S2の両情報により光沢度が決定
され、これを定量化することが可能である。
他方、同一種類の材質で目視光沢度が異なる多
数のサンプルについて考えれば、これらを前記2
次元平面(I1/S1,I2/S2)上にプロツトした場
合、これらのサンプルは、例えば第2図に示す如
く、その光沢度に応じて前記2次元平面上で複数
の群に分かれて分布する。第2図において、〇は
目視光沢度1のサンプル、▲は目視光沢度2のサ
ンプル、□は目視光沢度3のサンプルをそれぞれ
示すものである。
これらのサンプルの光沢度を(I1/S1,I2/
S2)の2次元平面上で分別する場合、各々の隣り
合う光沢度群間の重なりが統計的に最小となるよ
うに境界線Zを定め、分別するのが適切である。
隣り合う2群間の統計的な重なりを最小とする境
界線Zは、判別関数を用いて導出され、この境界
線Zは、例えば第3図に示す如く、これに垂直な
Zv軸上にこの2次元の分布を投影した時、そこ
での重なりが最小となるように定めることができ
る。この方法で、第2図の光沢度群の光沢度1と
光沢度2の境界線Z12及び光沢度2と光沢度3の
境界線Z23を求め、分別した様子を第4図に示す。
例えば、この第4図の例における光沢度3と光
沢度2の境界線Z23は、次のようにして求められ
ている。即ち、各光沢度について、第1表に示す
ようなデータが得られた時、これらのデータから
次式により次の統計量を計算する。
The present invention was made based on the fact that the visual gloss of the surface of an object, such as a steel plate, depends on two surface roughness parameters: the average roughness and the average peak interval, and cannot be evaluated based on the average roughness alone. . That is, surface roughness is the main factor that determines the gloss of objects of substantially the same color, and it is basically considered that the degree of gloss can be evaluated by accurately grasping information on the surface roughness. Information on surface roughness can be roughly expressed by the variance σ of the height distribution of the surface profile and the autocorrelation distance T (distance at which the autocorrelation function is 1/e), and these quantities and the light reflection intensity The distribution includes e.g.
Published by Pergamon Press, P. Beckmann
and “The Scattering of
Electromagnetic Waves from Rough
There is a certain relationship as shown in ``Surfaces''.Furthermore, the results of detailed examination of these relationships by Yuichiro Asano et al. Accordingly, by satisfying each range of equations (1) and (2) above, the specular reflection intensities I 1 and I 2 under each condition have a relationship with the roughness parameters σ and T as shown in the following equation. I 1 =f 1 (σ) ...(3) I 2 =f 2 (σ, T) ...(4) However, the incident light intensity is assumed to be a unit intensity and the total reflectance is 1. Here, if the total reflectance is taken into account, the above (3),
The left sides of equation (4) are I 1 /S 1 and I 2 /S 2 (S 1 and S 2 are
(1) and (2) (total reflection intensity under each condition), and the information on the roughness parameters σ and T is I 1 /
It is definitely included in both S 1 and I 2 /S 2 information. Therefore, the glossiness is determined by both information of I 1 /S 1 and I 2 /S 2 and can be quantified. On the other hand, if we consider many samples of the same type of material but with different visual gloss levels, we can
When plotted on a dimensional plane (I 1 /S 1 , I 2 /S 2 ), these samples are divided into groups on the two-dimensional plane according to their glossiness, as shown in Figure 2, for example. Separately distributed. In FIG. 2, ◯ indicates a sample with visual gloss level 1, ▲ indicates a sample with visual gloss level 2, and □ indicates a sample with visual gloss level 3. The glossiness of these samples was determined by (I 1 /S 1 , I 2 /
When classifying on the two-dimensional plane of S 2 ), it is appropriate to define the boundary line Z and perform the classification so that the overlap between adjacent glossiness groups is statistically minimized.
The boundary line Z that minimizes the statistical overlap between two adjacent groups is derived using a discriminant function.
When this two-dimensional distribution is projected onto the Zv axis, it can be determined so that the overlap there will be minimized. Using this method, the boundary line Z 12 between glossiness 1 and glossiness 2 and the boundary line Z 23 between glossiness 2 and glossiness 3 in the glossiness group shown in FIG. 2 are obtained, and the classification is shown in FIG. For example, the boundary line Z23 between glossiness 3 and glossiness 2 in the example of FIG. 4 is determined as follows. That is, when data as shown in Table 1 is obtained for each gloss level, the following statistics are calculated from these data using the following formula.
【表】【table】
【表】
(1)=n
〓a=1
Xai(1)/n …(3)
(2)=n
〓b=1
Xbi(2)/m …(4)
Xi=((1)+(2))/2 …(5)
di=(1)−(2)(i=1,2,…p) …(6)
Sij=n
〓a=1
(Xai(1)−(1))(Xaj(1)−(1))+n
〓b=1
(Xbi(2)
−(2))(Xbj(2)−(2))(i,j=1,
2,…p)…(7)
Vij=Sij/(n+m−2) …(8)
ここで、(3),(4)式は平均、(7)式は群内平方和・
積和、(8)式は群内分散・共分散をそれぞれ求めた
ものである。
以上の統計量から、次式を用いて判別関数であ
る境界線Zを求めることができる。
Z=P
〓i=1
ai(Xi−Xi) …(9)
ai=P
〓i=1
Vij・dj …(10)
∴a=V-1d …(11)
なお、前記説明においては、2変数の判別関数
を求める方法について説明していたが、この判別
関数の求め方で、2変数以上の判別関数について
も同様に求めることができる。[Table] (1) = n 〓 a=1 Xai (1) /n …(3) (2) = n 〓 b=1 Xbi (2) /m …(4) Xi=( (1) + (2 ) )/2 …(5) di= (1) − (2) (i=1,2,…p) …(6) Sij= n 〓 a=1 (Xai (1) − (1) ) (Xaj (1) − (1) )+ n 〓 b=1 (Xbi (2) − (2) ) (Xbj (2) − (2) ) (i, j=1,
2,...p)...(7) Vij=Sij/(n+m-2)...(8) Here, equations (3) and (4) are the average, and equation (7) is the within-group sum of squares.
The sum of products, Equation (8), calculates the within-group variance and covariance, respectively. From the above statistics, the boundary line Z, which is a discriminant function, can be determined using the following equation. Z= P 〓 i=1 ai (Xi−Xi) …(9) ai= P 〓 i=1 Vij・dj …(10) ∴a=V -1 d …(11) In addition, in the above explanation, 2 Although the method for determining the discriminant function of variables has been described, this method of determining the discriminant function can also be used to similarly determine the discriminant functions of two or more variables.
以下、本発明により、冷延鋼板の光沢度判定を
行つた実施例を詳細に説明する。
本実施例は、従来から行われている目視判断に
よる光沢度判定(光沢度1〜4の4段階)を、光
反射強度I1,I2の測定による自動判定に置き換え
る目的で、自動判定の性能を試験するために行つ
たものである。
ここで扱う冷延鋼板の表面粗さパラメータσ
は、0.1〜0.5μmであり、使用する光束として波長
λ=0.633μmのHe−Neレーザ光を用いれば、入
射角θ=75゜で前出(1)式を満足することができ、
又、入射角θ=10゜で前出(2)式を満足することが
できる。又、ここで扱う冷延鋼板の場合、全反射
率はほぼ一定であり、光沢評価に用いる2次元平
面(I1/S1,I2/S2)は、2次元平面(I1/I2)
と等価である。
第5図に、本実施例による判定の結果を示す。
各サンプルは、熟練した複数の判定者の、標準
サンプルとの比較による目視判定により、光沢度
1〜4の4段階に分類された。第5図において、
〇、▲、□、●は、それぞれ光沢度1,2,3,
4のサンプルを示す。
他方、これらのサンプルにつき、前記正反射強
度I1,I2を測定し、各光沢度に属するサンプルに
ついて、(I1,I2)2次元平面上での各々の光沢
度群間について、判別関数である境界線Z34,Z23
及びZ12を導出した。導出された境界線Z34,Z23
及びZ12は、次式で表わされるものであつた。
Z34=0.0043(I2−1278)
+0.0029(I1−2269) …(12)
Z23=0.0219(I2−1017)
−0.0035(I1−2113) …(13)
Z12=0.03(I2−642)
+0.0007(I1−2011) …(14)
このようにして求められた境界線Z34,Z23及び
Z12を用いて、多数の冷延鋼板サンプルについて
光沢度判定を行つた結果、90%程度のサンプルに
ついて正しく判定が行われ、充分な判定能力を有
することが確認された。
なお前記実施例は、本発明を冷延鋼板の光沢度
判定に適用したものであるが、本発明の適用範囲
はこれに限定されず、一般の物体表面の光沢度判
定にも同様に適用できることは明らかである。
EXAMPLES Hereinafter, an example in which the glossiness of a cold rolled steel sheet was determined according to the present invention will be described in detail. This embodiment aims to replace the conventional visual determination of glossiness (4 levels of glossiness 1 to 4) with automatic determination by measuring the light reflection intensities I 1 and I 2 . This was done to test performance. Surface roughness parameter σ of cold rolled steel sheet treated here
is 0.1 to 0.5 μm, and if a He-Ne laser beam with a wavelength λ = 0.633 μm is used as the luminous flux, the above equation (1) can be satisfied at an incident angle θ = 75°,
Furthermore, the above equation (2) can be satisfied when the incident angle θ=10°. In addition, in the case of the cold-rolled steel sheet treated here, the total reflectance is almost constant, and the two-dimensional plane (I 1 /S 1 , I 2 /S 2 ) used for gloss evaluation is the same as the two-dimensional plane (I 1 /I 2 )
is equivalent to FIG. 5 shows the results of determination according to this example. Each sample was visually judged by a plurality of skilled judges in comparison with a standard sample, and was classified into four levels of glossiness, 1 to 4. In Figure 5,
〇, ▲, □, ● are gloss levels 1, 2, 3, and 3, respectively.
4 samples are shown. On the other hand, for these samples, the specular reflection intensities I 1 and I 2 are measured, and for the samples belonging to each gloss level, discrimination is made between each gloss level group on the (I 1 , I 2 ) two-dimensional plane. Boundary lines Z 34 , Z 23 which are functions
and Z 12 were derived. Derived boundaries Z 34 , Z 23
and Z 12 were expressed by the following formula. Z 34 =0.0043(I 2 −1278) +0.0029(I 1 −2269) …(12) Z 23 =0.0219(I 2 −1017) −0.0035(I 1 −2113) …(13) Z 12 =0.03( I 2 −642) +0.0007 (I 1 −2011) …(14) The boundary lines Z 34 , Z 23 and
As a result of using Z 12 to judge the brightness of a large number of cold-rolled steel sheet samples, the judgment was made correctly for about 90% of the samples, confirming that it has sufficient judgment ability. In addition, although the present invention is applied to the determination of the glossiness of a cold-rolled steel plate in the above example, the scope of application of the present invention is not limited thereto, and can be similarly applied to determination of the glossiness of the surface of a general object. is clear.
以上説明した通り、本発明によれば、同一色
(明度は異なつてもよい)の対象について、目視
光沢度に良く一致し、且つ、鏡面から粗面までの
広い粗度範囲に亘り定量的に光沢度を定めること
が可能となる。従つて、オンラインで表面品質を
適確に計測、管理することが可能となり、不良発
生の防止等、実用上の効果が大きいという優れた
効果を有する。
As explained above, according to the present invention, for objects of the same color (brightness may differ), the visual glossiness closely matches the visual glossiness and can be quantitatively measured over a wide roughness range from specular to rough surfaces. It becomes possible to determine the gloss level. Therefore, it is possible to accurately measure and manage the surface quality online, which has excellent practical effects such as prevention of defects.
第1図は、本発明に係る物体表面の光沢度判定
方法の要旨を示す流れ図、第2図は、本発明の原
理を説明するための、(I1/S1,I2/S2)2次元
平面上のサンプルの分布状況の例を示す線図、第
3図は、同じく、各光沢度群の分別方法の例を示
す線図、第4図は、同じく、本発明により光沢度
群を分別した例を示す線図、第5図は、本発明を
適用して冷延鋼板の光沢度判定を行つた実施例の
判定結果を示す線図、第6図は、正反射強度と全
反射強度を説明するための線図である。
σ……分散、λ1,λ2……波長、θ1,θ2……入射
角、I1,I2……正反射強度、S1,S2……全反射強
度、Z,Z12,Z23,Z34……境界線。
FIG. 1 is a flowchart showing the gist of the method for determining the glossiness of an object surface according to the present invention, and FIG . FIG. 3 is a diagram showing an example of the distribution of samples on a two-dimensional plane; FIG. 3 is a diagram showing an example of how to classify each gloss group; FIG. Fig. 5 is a diagram showing the judgment results of an example in which the present invention was applied to judge the glossiness of cold-rolled steel sheets. FIG. 3 is a diagram for explaining reflection intensity. σ...Dispersion, λ1 , λ2 ...Wavelength, θ1 , θ2 ...Incident angle, I1 , I2 ...Specular reflection intensity, S1 , S2 ...Total reflection intensity, Z, Z 12 , Z 23 , Z 34 ... Boundary line.
Claims (1)
に基づく光沢度を分類、等級付けする物体表面の
光沢度判定方法において、 被測定表面プロフイルの高さ分布の分散σが次
式の関係 {(4πσ/λ1)・cosθ1}2≦1 {(4πσ/λ2)・cosθ2}2≧4 を満足するような波長λ1,λ2(λ1=λ2も含む)の
光束を、それぞれ入射角θ1,θ2で投射し、 各々の正反射強度I1,I2及び全反射強度S1,S2
を検出し、 予め2次元平面(I1/S1,I2/S2)上に各目視
光沢度を統計的に充分表わすサンプル数をプロツ
トし、2次元平面に存在する複数の光沢度群につ
いて、各々の隣り合う光沢度群間の重なりが最小
となるような判別関数である境界線Zを定めてお
き、 該境界線Zにより、任意の被測定物の光沢度を
分別することを特徴とする物体表面の光沢度判定
度方法。[Claims] 1. In a method for determining the glossiness of an object surface, which classifies and ranks the glossiness based on the visual perception based on the light reflection intensity distribution on the surface of the object, the dispersion σ of the height distribution of the surface profile to be measured is The wavelengths λ 1 and λ 2 ( λ 1 = λ 2 also ) are projected at incident angles θ 1 and θ 2 , respectively, and the specular reflection intensities I 1 and I 2 and total reflection intensities S 1 and S 2 are respectively
The number of samples that statistically sufficiently represent each visual gloss level is plotted in advance on a two-dimensional plane (I 1 /S 1 , I 2 /S 2 ), and multiple gloss levels existing on the two-dimensional plane are plotted. A boundary line Z, which is a discriminant function that minimizes the overlap between adjacent glossiness groups, is determined for each, and the glossiness of an arbitrary object to be measured is classified by the boundary line Z. A method for determining the glossiness of the surface of an object.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59253530A JPS61130858A (en) | 1984-11-30 | 1984-11-30 | Decision for gloss of object surface |
| CA000496546A CA1240052A (en) | 1984-11-30 | 1985-11-29 | Method of and apparatus for determining glossinesses of surface of body |
| EP85115140A EP0183270B1 (en) | 1984-11-30 | 1985-11-29 | Method of determining glossinesses of surface of body |
| DE8585115140T DE3579119D1 (en) | 1984-11-30 | 1985-11-29 | METHOD FOR DETERMINING THE SURFACE GLOSS OF A BODY. |
| US06/802,742 US4750140A (en) | 1984-11-30 | 1985-11-29 | Method of and apparatus for determining glossiness of surface of a body |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59253530A JPS61130858A (en) | 1984-11-30 | 1984-11-30 | Decision for gloss of object surface |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61130858A JPS61130858A (en) | 1986-06-18 |
| JPH0224458B2 true JPH0224458B2 (en) | 1990-05-29 |
Family
ID=17252648
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59253530A Granted JPS61130858A (en) | 1984-11-30 | 1984-11-30 | Decision for gloss of object surface |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61130858A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2705842B2 (en) * | 1989-09-26 | 1998-01-28 | 川崎製鉄株式会社 | Method and apparatus for measuring surface properties of metal plate |
| US20060169051A1 (en) * | 2005-01-13 | 2006-08-03 | Alman David H | Method to specify acceptable surface appearance of a coated article |
-
1984
- 1984-11-30 JP JP59253530A patent/JPS61130858A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61130858A (en) | 1986-06-18 |
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