JPH0219420B2 - - Google Patents
Info
- Publication number
- JPH0219420B2 JPH0219420B2 JP26663885A JP26663885A JPH0219420B2 JP H0219420 B2 JPH0219420 B2 JP H0219420B2 JP 26663885 A JP26663885 A JP 26663885A JP 26663885 A JP26663885 A JP 26663885A JP H0219420 B2 JPH0219420 B2 JP H0219420B2
- Authority
- JP
- Japan
- Prior art keywords
- glossiness
- gloss
- light
- measured
- specular
- 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
Links
- 230000004907 flux Effects 0.000 claims description 7
- 238000012545 processing Methods 0.000 claims description 5
- 230000016776 visual perception Effects 0.000 claims description 3
- 238000000034 method Methods 0.000 description 11
- 230000000007 visual effect Effects 0.000 description 10
- 230000003746 surface roughness Effects 0.000 description 7
- 239000010960 cold rolled steel Substances 0.000 description 6
- 239000010935 stainless steel Substances 0.000 description 5
- 229910001220 stainless steel Inorganic materials 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 238000004364 calculation method Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000011156 evaluation Methods 0.000 description 3
- 229910000831 Steel Inorganic materials 0.000 description 2
- 230000006870 function Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 239000010959 steel Substances 0.000 description 2
- 238000012360 testing method Methods 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
- 239000003086 colorant Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000002265 prevention Effects 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 230000035807 sensation Effects 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
本発明は、物体表面の光沢度判定装置に係り、
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装置に改良に関する。
The present invention relates to an apparatus for determining glossiness of an object surface,
In particular, it is suitable for use in measuring and managing the surface quality of steel sheets, and is suitable for use in object surface gloss determination devices that classify and grade gloss based on the visual sensation based on the light reflection intensity distribution on the object surface. Regarding improvements.
【従来の技術】
物体表面の光沢度を定める装置として、従来よ
り種々の光反射測定による装置が提案されてお
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
る測定装置、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
る測定装置(JISZ8741)、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
度による測定装置がある。[Prior Art] Various types of light reflection measuring devices have been proposed as devices for determining the glossiness of an object's surface.A typical device measures the specular reflection intensity of a white beam projected at a fixed angle. A measuring device using specular gloss, a measuring device using contrastive gloss that uses the ratio of the specular reflection intensity and diffuse reflection intensity of white light projected at a certain angle (JISZ8741), and a measuring device that measures the reflected gloss by projecting another object onto the surface. There is a clear gloss measurement device that allows you to see the blur with the naked eye.
しかしながら、前記鏡面光沢度による測定装置
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測定
装置は、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測定装置
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, although the specular gloss measuring device is widely used industrially, it has the drawback that it does not match reality for specular objects with small surface roughness. In addition, the measuring device based on contrast glossiness has the characteristic of giving a glossiness close to visual perception even for objects of different colors, but this also tends to have lower judgment accuracy for objects that are close to mirror surfaces. . Furthermore, the above-mentioned clear gloss measuring device had a problem in that quantitative display could not 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面範囲に亘つて定
量的に光沢度を定めることができる物体表面の光
沢度判定装置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 object of the present invention is to provide a glossiness determination device for the surface of an object that closely matches the visual glossiness and can quantitatively determine the glossiness over a wide range of rough surfaces 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装置において、第1図にその
要旨構成を示す如く、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12A,12Bを、被測定物10の表面に対
しそれぞれ入射角θ1,θ2で投射する2つの光源1
4A,14Bと、各々の正反射強度I1,I2及び全
反射強度S1,S2を検出する2つの受光器16A,
16Bと、該正反射強度I1,I2及び全反射強度
S1,S2の2次元平面(I1/S1、I2/S2)上の座標
に基づいて被測定物10の光沢度を分別する演算
処理部18とを備えることにより、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10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10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 an object surface gloss determination device that classifies and grades the glossiness based on visual perception, as shown in Figure 1, the variance σ of the height distribution of the measured surface profile 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 ) onto the surface of the object to be measured 10 at incident angles θ 1 and θ 2 , respectively.
4A, 14B, and two light receivers 16A for detecting specular reflection intensities I 1 , I 2 and total reflection intensities S 1 , S 2 , respectively.
16B, the specular reflection intensities I 1 , I 2 and total reflection intensity
By including a calculation processing unit 18 that classifies the glossiness of the object to be measured 10 based on the coordinates of S 1 and S 2 on a two-dimensional plane (I 1 /S 1 , I 2 /S 2 ) , the above-mentioned purpose can be achieved. has been achieved. 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. 10 and the following equation. do. I=∫ + 〓 - 〓i(θ)dθ i(θ): Distribution of reflected luminous flux α: Receiving angle (direction of specular reflection α=0) Also, the total reflection intensity S is shown in Fig. 10 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。
即ち、前出第1図に示した如く、(1)、(2)式の各
条件を満足する波長λ1,λ2と入射角θ1,θ2を有す
る2つの光源14A,14Bから、光束12A,
12Bを被測定物10の表面に投射し、該被測定
物10の表面からの正反射強度I1,I2及び全反射
強度S1,S2を受光器16A,16Bで検出し、該
正反射強度I1,I2及び全反射強度S1,S2の2次元
平面(I1/S1、I2/S2)上の座標に基づいて、演
算処理部18で適当に演算処理すれば、被測定物
10の表面の光沢度を判定することができる。
正反射強度I1,I2及び全反射強度S1,S2を検出
する受光器16A,16Bとしては、例えば、第
2図に示す如く、フオトダイオード20A,20
B,20C、……を2次元アレイ状に並べてお
き、それぞれのフオトダイオードのうち、正反射
方向にあるフオトダイオードの受光量が正反射強
度I1,I2、全ての受光量の総和が全反射強度S1,
S2となるような受光器16A,16Bを用いるこ
とが考えられる。この時、フオトダイオード20
A,20B,20C,……の2次元アレイの広が
り(面積)は、全反射光を充分受光するだけの広
がりが必要である。又、第3図に示す如く、受光
器16A,16Bの前面に絞り22を設け、該絞
り22の開口面積を可変とすることで、正反射強
度I1,I2及び全反射強度S1,S2を検出するような
受光器16A,16Bを用いることも考えられ
る。
一方、演算処理部18で行う、正反射強度I1,
I2及び全反射強度S1,S2から、被測定物10の表
面の光沢度を判定する演算処理方法としては、例
えば出願人が既に特開昭61−130857で提案した如
く、第4図に示すように、2次元平面(I1/S1、
I2/S2)上に各目視光沢度の代表点をプロツト
し、これを滑かに結んで得られる曲線lを、例え
ば図面上での作図により定め、該曲線lと直交す
る直線mにより分別する方法や、第5図に示すよ
うに、更に、任意のサンプルの光沢度を、該サン
プルの前記2次元平面上における点Pから曲線l
に下した垂線の足Qの曲線l上の基準点Rからの
曲線lに沿つた距離(あるいはこれに相当する
量)で評価する方法、あるいは、同じく出願人が
既に特開昭61−130858で提案した如く、第6図に
示すように、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を、判別関数を用いて導出
し、この境界線Zで分別する方法を用いることが
できる。前記境回線Zは、例えば第7図に示すよ
うに、境界線Z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。
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 assumed to be 1. Here, if the total reflectance is taken into account, the above (3),
The left side of equation (4) is 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. That is, as shown in FIG. 1 above, from the two light sources 14A and 14B having wavelengths λ 1 and λ 2 and incident angles θ 1 and θ 2 that satisfy the conditions of equations (1) and (2), Luminous flux 12A,
12B onto the surface of the object to be measured 10, the specular reflection intensities I 1 and I 2 and the total reflection intensities S 1 and S 2 from the surface of the object to be measured 10 are detected by the receivers 16A and 16B. Based on the coordinates of the reflection intensities I 1 , I 2 and the total reflection intensities S 1 , S 2 on the two-dimensional plane (I 1 /S 1 , I 2 /S 2 ), the calculation processing unit 18 performs appropriate calculation processing. For example, the glossiness of the surface of the object to be measured 10 can be determined. As the light receivers 16A and 16B for detecting the specular reflection intensities I 1 and I 2 and the total reflection intensities S 1 and S 2 , for example, photodiodes 20A and 20 are used as shown in FIG.
B , 20C, . Reflection intensity S 1 ,
It is conceivable to use light receivers 16A and 16B such that S2 . At this time, photodiode 20
The spread (area) of the two-dimensional array of A, 20B, 20C, . . . must be large enough to receive the total reflected light. Further, as shown in FIG. 3, by providing a diaphragm 22 in front of the light receivers 16A, 16B and making the aperture area of the diaphragm 22 variable, the specular reflection intensities I 1 , I 2 and the total reflection intensity S 1 , It is also conceivable to use light receivers 16A and 16B that detect S2 . On the other hand, the specular reflection intensity I 1 ,
As an arithmetic processing method for determining the glossiness of the surface of the object to be measured 10 from I 2 and the total reflection intensities S 1 and S 2 , the method shown in FIG. As shown in , the two-dimensional plane (I 1 /S 1 ,
I 2 /S 2 ), plot the representative points of each visual gloss level, connect them smoothly, and determine the curve l obtained by drawing it on a drawing, for example, and draw a straight line m perpendicular to the curve l. As shown in FIG.
The evaluation method is based on the distance along the curve l from the reference point R on the curve l of the leg Q of the perpendicular drawn to the line (or an amount equivalent to this), or the method has already been proposed by the applicant in JP-A-61-130858. As proposed, as shown in Figure 6, a method is used in which a boundary line Z that minimizes the statistical overlap between two adjacent groups is derived using a discriminant function, and separation is performed using this boundary line Z. Can be done. The boundary line Z can be determined, for example, as shown in FIG. 7, so that when this two-dimensional distribution is projected onto the Zv axis perpendicular to the boundary line Z, the overlap thereon is minimized.
以下、本発明により、特開昭61−130857で提案
した方法を利用して、ステンレス鋼板の光沢度の
評価を行つた第1実施例を詳細に説明する。
この第1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。
ここで扱うステンレス鋼板の表面粗さパラメー
タσは、0.02〜0.2μmであり、使用する光束とし
てλ=0.45μmのAr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、ここで扱うステンレス鋼板の場合、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、(I1、I2)と等価であ
る。
第8図に、この第1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8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次元平面上での代表点(第
1実施例では重心点)C1〜C4を定めた後、これ
らを図面上で滑かに結んで曲線lを描いた。次
に、各光沢度毎にサンプルの分類がなされるよう
に、前記曲線lにそれぞれ直交する適切な境界線
ma,mb,mcを定めた。この境界線ma,mb,
mcを定める実用的な方法としては、例えば多数
のサンプル点をプロツトし、各隣接するグループ
につき誤判定となる点数が最小となるように定め
ることができる。
前記手順で求めた判定法により、多数のステン
レス鋼板サンプルを自動判定した結果、約97%の
サンプルについて正しく判定を行うことができ、
充分な性能を有することが確認できた。
なお、光沢度判定を更に細かく行う方法とし
て、代表点C1,C2,C3,C4の各点の光沢度を1.0、
2.0、3.0、4.0とし、一方の基準点Rs、曲線lと境
界線maの交点Ta、境界線mbとの交点Tb、境界
線mcとの交点Tc及び他方の基準点Reの各点の光
沢度を、それぞれ0.5、1.5、2.5、3.5、4.5とし、
更に、曲線l上の任意の点の光沢度を、各区間
(0.5〜1.0、1.0〜1.5、…4.0〜4.5)内で、曲線l
に沿つて比例的に内挿した値と定めておき、任意
のサンプルの光沢度を、2次元平面(I1,I2)上
の対応点Pから曲線lに下した垂線の足Qの位置
する点の光沢度とすることもできる。
この方法によれば、アナログ的な光沢度判定が
可能である。
次に、本発明により、特開昭61−130858で提案
した方法を利用して冷延鋼板の光沢度の評価を行
つた第2実施例を説明する。
この第2実施例も、又、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9図に、この第2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9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) ……(5)
Z23=0.0219(I2−1017)
−0.0035(I1−2113) ……(6)
Z12=0.03(I2−642)
+0.0007(I1−2011) ……(7)
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、本発明をステンレス鋼板や
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。
Hereinafter, a first embodiment of the present invention will be described in detail, in which the glossiness of a stainless steel plate was evaluated using the method proposed in Japanese Patent Application Laid-Open No. 61-130857. This first embodiment is based on the conventional method of determining glossiness by visual judgment (4 levels of glossiness 1 to 4).
This was done to test the performance of automatic determination with the aim of replacing it with automatic determination by measuring the light reflection intensities I 1 and I 2 . The surface roughness parameter σ of the stainless steel plate treated here is 0.02 to 0.2 μm, and if an Ar laser beam of λ = 0.45 μm is used as the luminous flux, the incident angle θ = 75°, and the equation (1) above is used. can satisfy you, and
Equation (2) above can be satisfied when the incident angle θ=10°. In addition, in the case of the stainless steel plate 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 equivalent to (I 1 , I 2 ). It is. FIG. 8 shows the results of the determination according to the first embodiment. Each sample was evaluated by multiple skilled judges.
The glossiness was classified into four levels from 1 to 4 based on visual judgment based on comparison with standard samples. In Figure 8, 〇, ▲, □, ● represent gloss levels of 1, 2, and 2, respectively.
Samples 3 and 4 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, the representative points (I 1 , I 2 ) on the two-dimensional plane (in the first example, the center of gravity) are measured. Points) After determining C 1 to C 4 , they were smoothly connected on the drawing to draw a curve l. Next, appropriate boundaries are drawn perpendicularly to the curve l so that the samples are classified for each gloss level.
Ma, mb, and mc were determined. This boundary line ma, mb,
A practical method for determining mc is, for example, by plotting a large number of sample points and determining mc so that the number of false positive points for each adjacent group is minimized. As a result of automatically judging a large number of stainless steel plate samples using the judgment method determined in the above procedure, we were able to correctly judge approximately 97% of the samples.
It was confirmed that it had sufficient performance. In addition, as a method for more finely determining the glossiness, the glossiness of each of the representative points C 1 , C 2 , C 3 , and C 4 is set to 1.0,
2.0, 3.0, and 4.0, and the glossiness of each point is one reference point Rs, the intersection Ta of the curve l and the boundary line ma, the intersection Tb with the boundary line mb, the intersection Tc with the boundary line mc, and the other reference point Re. are respectively 0.5, 1.5, 2.5, 3.5, and 4.5,
Furthermore, the glossiness of any point on the curve l is determined by the curve l within each interval (0.5-1.0, 1.0-1.5,...4.0-4.5).
The glossiness of any sample is defined as the value proportionally interpolated along It can also be defined as the glossiness of a point. According to this method, analog glossiness determination is possible. Next, a second embodiment of the present invention will be described in which the glossiness of a cold-rolled steel sheet was evaluated using the method proposed in Japanese Patent Application Laid-Open No. 61-130858. The purpose of this second embodiment is also to replace the conventional visual judgment of glossiness (4 levels of glossiness 1 to 4) with automatic judgment by measuring the light reflection intensities I 1 and I 2 . This was done to test the performance of automatic judgment. 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. 9 shows the results of the determination according to this second embodiment. Each sample was evaluated by multiple skilled judges.
The glossiness was classified into four levels from 1 to 4 based on visual judgment based on comparison with standard samples. In Figure 9, 〇, ▲, □, and ● represent gloss levels of 1, 2, and 2, respectively.
Samples 3 and 4 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. The boundary line Z 34 which is a function,
Z 23 and Z 12 were derived. The derived boundary line Z 34 ,
Z 23 and Z 12 were represented by the following formula. Z 34 =0.0043(I 2 −1278) +0.0029(I 1 −2269) ……(5) Z 23 =0.0219(I 2 −1017) −0.0035(I 1 −2113) ……(6) Z 12 = 0.03 (I 2 −642) +0.0007 (I 1 −2011) ...(7) 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. Note that in the above example, the present invention was applied to the determination of the glossiness of a stainless steel plate or a cold-rolled steel plate.
It is clear that the scope of application of the present invention is not limited to this, and can be similarly applied to determination of glossiness of the surface of a general object.
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
装置の要旨構成を示すブロツク線図、第2図は、
本発明で用いられる受光器の構成の一例を示す斜
視図、第3図は、同じく受光器の構成の他の例を
示す斜視図、第4図乃至第7図は、本発明で利用
する光沢度の判定方法の例を説明するための線
図、第8図は、本発明に係る装置を用いてステン
レス鋼板の光沢度評価を行つた第1実施例の判定
結果を示す線図、第9図は、同じく、冷延鋼板の
光沢度判定を行つた第2実施例の判定結果を示す
線図、第10図は、正反射強度及び全反射強度を
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、10……被測定物、12A,12B……光
束、14A,14B……光源、16A,16B…
…受光器、18……演算処理部、20A,20
B,20C,……フオトダイオード、22……絞
り。
FIG. 1 is a block diagram showing the gist of the apparatus for determining the glossiness of an object surface according to the present invention, and FIG.
FIG. 3 is a perspective view showing an example of the structure of the light receiver used in the present invention, FIG. 3 is a perspective view showing another example of the structure of the light receiver, and FIGS. 4 to 7 are glossy FIG. 8 is a diagram for explaining an example of the gloss determination method of the present invention, and FIG. Similarly, the figure is a diagram showing the determination results of the second example in which the glossiness of a cold rolled steel sheet was determined, and FIG. 10 is a diagram for explaining the specular reflection intensity and the total reflection intensity. σ...dispersion, λ1 , λ2 ...wavelength, θ1 , θ2 ...incident angle, I1 , I2 ...specular reflection intensity, S1 , S2 ...total reflection intensity, 10...subject Measurement object, 12A, 12B...Light flux, 14A, 14B...Light source, 16A, 16B...
...Photoreceiver, 18...Arithmetic processing unit, 20A, 20
B, 20C,...Photodiode, 22...Aperture.
Claims (1)
に基づく光沢度を分類、等級付けする物体表面の
光沢度判定装置において、 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で投射する2つの
光源と、 各々の正反射強度I1,I2及び全反射強度S1,S2
を検出する2つの受光器と、 該正反射強度I1,I2及び全反射強度S1,S2の2
次元平面(I1/S1、I2/S2)上の座標に基づい
て、被測定物の光沢度を分別する演算処理部と、 から構成される物体表面の光沢度判定装置。[Claims] 1. In an object surface gloss determination device for classifying and grading gloss based on visual perception based on the light reflection intensity distribution on the object surface, the variance 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 two light sources that project a luminous flux of ( including
two light receivers that detect the specular reflection intensities I 1 , I 2 and the total reflection intensities S 1 , S 2 .
An apparatus for determining the glossiness of an object surface, comprising: an arithmetic processing unit that classifies the glossiness of an object to be measured based on coordinates on a dimensional plane (I 1 /S 1 , I 2 /S 2 );
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP26663885A JPS62126331A (en) | 1985-11-27 | 1985-11-27 | Apparatus for judging surface glossiness of matter |
| 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 |
|---|---|---|---|
| JP26663885A JPS62126331A (en) | 1985-11-27 | 1985-11-27 | Apparatus for judging surface glossiness of matter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62126331A JPS62126331A (en) | 1987-06-08 |
| JPH0219420B2 true JPH0219420B2 (en) | 1990-05-01 |
Family
ID=17433607
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP26663885A Granted JPS62126331A (en) | 1984-11-30 | 1985-11-27 | Apparatus for judging surface glossiness of matter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62126331A (en) |
Families Citing this family (5)
| 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 |
| US6706959B2 (en) | 2000-11-24 | 2004-03-16 | Clean Venture 21 Corporation | Photovoltaic apparatus and mass-producing apparatus for mass-producing spherical semiconductor particles |
| JP3938184B2 (en) | 2005-03-22 | 2007-06-27 | キヤノン株式会社 | Information processing method and apparatus |
| JP5430871B2 (en) | 2007-03-22 | 2014-03-05 | ベーユプスィロンカー−ガードネル ゲーエムベーハー | Method and apparatus for quantitative measurement of surface properties |
| JP7701863B2 (en) * | 2021-11-26 | 2025-07-02 | 株式会社トヨタプロダクションエンジニアリング | Gloss surface distribution measurement device |
-
1985
- 1985-11-27 JP JP26663885A patent/JPS62126331A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62126331A (en) | 1987-06-08 |
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