JPH0245814B2 - HANTOMEIBUTSUTAINONAIBUSHOKUSOKUTEIHOHO - Google Patents
HANTOMEIBUTSUTAINONAIBUSHOKUSOKUTEIHOHOInfo
- Publication number
- JPH0245814B2 JPH0245814B2 JP5452982A JP5452982A JPH0245814B2 JP H0245814 B2 JPH0245814 B2 JP H0245814B2 JP 5452982 A JP5452982 A JP 5452982A JP 5452982 A JP5452982 A JP 5452982A JP H0245814 B2 JPH0245814 B2 JP H0245814B2
- Authority
- JP
- Japan
- Prior art keywords
- measured
- light
- measuring
- internal color
- translucent
- 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
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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
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N21/4738—Diffuse reflection, e.g. also for testing fluids, fibrous materials
- G01N21/474—Details of optical heads therefor, e.g. using optical fibres
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- 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)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Spectrometry And Color Measurement (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
【発明の詳細な説明】
この発明は、半透明物体の内部の色を非破壊的
に測定することのできる測定方法に関するもので
ある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a measuring method capable of non-destructively measuring the color inside a translucent object.
例えば、第1図に示すような表面に木目模様を
そなえた人工の突板1は、第2図に示すように複
数の染色単板2,2,…を接着剤層3,3,…を
介して重ね合わせたものに斜め方向の切目4,
4,…が入るようにスライスすることにより製造
される。したがつて、各染色単板2の色は製品の
品質に大きな影響を与えるのである。上記染色単
板22は、ロータリーレースされた例えば厚み
0.8〜1.0mmの素材単板を所望の色に染色して得ら
れるが、この場合、素材の染色特性の違いや染料
混合量の差等により色違いが生じたり、内部が目
的とする色に染まらなかつたりするようなことが
多かつた。内部が目的とする色に染まつていない
場合でも単板の表面は一応染色されているので、
内部の染色不良を外観から判定することはできな
かつた。このため、染色ロツトごとに抜取りで破
壊検査を行つていたが、木材の染色性は原木のロ
ツトによつて変化するとともに、同一ロツト内で
も芯材であるか辺材であるかによつて異なり、さ
らに含有成分等によつても影響を受けるので、抜
取検査では不良品を見逃すことが多かつた。 For example, an artificial veneer 1 with a wood grain pattern on the surface as shown in FIG. Make diagonal cuts 4,
It is manufactured by slicing it so that it contains 4,.... Therefore, the color of each dyed veneer 2 has a great influence on the quality of the product. The dyed veneer 22 has a rotary lace, for example, thickness.
It can be obtained by dyeing a 0.8 to 1.0 mm material veneer to the desired color, but in this case, color differences may occur due to differences in the dyeing characteristics of the material or differences in the amount of dye mixed, or the interior may not match the desired color. There were many cases where the dye did not get dyed and it smudged. Even if the inside is not dyed the desired color, the surface of the veneer is still dyed, so
It was not possible to determine internal staining defects from the appearance. For this reason, destructive tests were carried out on samples for each dyeing lot, but the dyeability of wood varies depending on the lot of raw wood, and even within the same lot, it varies depending on whether the wood is core material or sapwood. In addition, it is also affected by the contained ingredients, so sampling inspections often miss defective products.
この発明は上記事情に鑑みなされたもので、こ
のような半透明材料の内部の染色状態を非破壊的
に全数検査することのできるような検査方法を提
供するものである。これについて以下に説明す
る。 The present invention has been made in view of the above circumstances, and it is an object of the present invention to provide an inspection method capable of non-destructively inspecting the dyeing state inside such translucent materials. This will be explained below.
この発明にかかる半透明物体の内部色測定方法
は、半透明物体からなる試料の表面に垂直に光を
照射し、試料の裏面部に黒板を密着させて透過光
が戻つて来ないようにした状態での反射光と、被
検体を透過する光とを積分球を用いてそれぞれ測
定し、その測定結果から非破壊状態での三刺激値
を求めて、この値と実際に試料を破壊して測定し
た内部の三刺激値とを対比して、あらかじめ両者
を関係づける関係式を必要な複数組のデータから
求めておき、つぎに同様な半透明物体からなる実
際の被測定物について上記非波壊状態での三刺激
値の測定を行ない、その結果から、上記関係式に
よつて内部の色を求めることを特徴としている。 The method for measuring the internal color of a translucent object according to the present invention involves irradiating light perpendicularly to the surface of a sample made of a translucent object, and placing a blackboard in close contact with the back surface of the sample to prevent transmitted light from returning. Using an integrating sphere, measure the reflected light in the state and the light transmitted through the specimen, calculate the tristimulus values in a non-destructive state from the measurement results, and compare these values with the values obtained by actually destroying the specimen. Compare the measured internal tristimulus values and find a relational expression that relates the two in advance from the necessary multiple sets of data. The feature is that the tristimulus values are measured in a broken state, and the internal color is determined from the results using the above relational expression.
この内部色測定方法の原理は、カラーマツチン
グで用いられる混色理論(吸収・拡散理論とも云
われる)を応用するものである。すなわち、光が
物体に入射された場合の物体内部での吸収(K)と拡
散(S)について考え、K/Sなる光学濃度から
厚みが無限大(∞)で物体の裏面にある物の色の
影響が全くないような場合の理想的な反射率R∞
を、良く知られたクベルカ(Kubelka)、ムンク
(Munk)等の理論に従い求める。このR∞を可視
領域全体にわたつて求めると、次の式によつて三
刺激値を計算することにより、色として表示する
ことができるようになる。 The principle of this internal color measurement method is to apply the color mixing theory (also called absorption/diffusion theory) used in color matching. In other words, when light is incident on an object, we consider the absorption (K) and diffusion (S) inside the object, and from the optical density K/S, we can calculate the color of the object on the back side of the object when the thickness is infinite (∞). The ideal reflectance R∞ when there is no influence of
is determined according to the well-known theory of Kubelka, Munk, etc. When this R ∞ is determined over the entire visible region, it can be displayed as a color by calculating the tristimulus values using the following formula.
ここに、Pλは試料を照明する照明の分光分布、
Xλ、λ、λはCIE(国際照明委員会)のス
ペクトル三刺激値である。 Here, Pλ is the spectral distribution of the illumination that illuminates the sample,
Xλ, λ, λ are CIE (Commission Internationale de l'Eclairage) spectral tristimulus values.
このように、K/SよりR∞を求め、色として
XR∞、YR∞、ZR∞を求める方法を木材の単板に適用
すると次の通りである。すなわち、前述したよう
に単板の厚み方向の染まり方は均一ではなく、明
るさであらわすと第3図に示すようになる。この
ような被測定物の裏面側に黒板を密着させて、そ
の表面に垂直に白色光を照射した場合(透過光は
黒板に吸収されて表面側には戻つて来ない)の反
射率と、上記黒板のかわりに白板を密着させて測
定した反射率(この場合は透過光が白板によつて
反射されて戻つて来る)とからK/Sを求め、
R∞よりXR∞、YR∞、ZR∞を求めると、厚み方向の
分布が平均化された値が得られることになる。こ
のようにして求められたXR∞、YR∞、ZR∞と、被測
定物である染色単板を破壊して、内部の色を測色
計を用いて実際に測定した値(通常は厚みの中央
の値であるが、それに限らない)X、Y、Zとの
間には、次のような関係があることがわかつた。 In this way, find R ∞ from K/S and use it as a color.
The method for determining X R∞ , Y R∞ , and Z R∞ is applied to a wood veneer as follows. That is, as mentioned above, the dyeing in the thickness direction of the veneer is not uniform, and when expressed in terms of brightness, it becomes as shown in FIG. 3. The reflectance when a blackboard is closely attached to the back side of such an object to be measured and white light is irradiated perpendicularly to the surface (the transmitted light is absorbed by the blackboard and does not return to the front side), Calculate K/S from the reflectance measured by placing a white board in close contact with the blackboard (in this case, the transmitted light is reflected by the white board and returning),
When X R∞ , Y R∞ , and Z R∞ are determined from R ∞, values obtained by averaging the distribution in the thickness direction are obtained. The X R∞ , Y R∞ , and Z R∞ obtained in this way and the values actually measured using a colorimeter after destroying the dyed veneer that is the object to be measured (usually is the center value of the thickness, but is not limited thereto) It was found that there is the following relationship between X, Y, and Z.
X=fx(XR∞、YR∞、ZR∞)
Y=fy(XR∞、YR∞、ZR∞)
Z=fz(XR∞、YR∞、ZR∞) ……
したがつて、K/Sより求めたXR∞、YR∞、ZR∞
を用いれば、被測定物をいちいち破壊しなくて
も、内部の色(X、Y、Z)を計算推定すること
ができるのである。もつとも、前記の関係また
は以下に述べる関係において、各函数fx、fy、fz
の変数は、X分、Y分、Z分三つのすべてを用い
るのがもつとも精度的によいが、いずれかひとつ
もしくは二つのみを用いるようにしてもよい。X=f x (X R∞ , Y R∞ , Z R∞ ) Y=f y (X R∞ , Y R∞ , Z R∞ ) Z=f z (X R∞ , Y R∞ , Z R∞ ) ... Therefore, X R∞ , Y R∞ , Z R∞ found from K/S
By using , it is possible to calculate and estimate the internal color (X, Y, Z) without destroying the object to be measured. However, in the above relationship or the relationship described below, each function f x , f y , f z
Although it is better to use all three variables (X, Y, and Z) for better accuracy, it is also possible to use only one or two of them.
以上は、分光光度計により、可視光域のスペク
トルから得られた測定値にもとづいてXR∞、YR∞、
ZR∞を計算するものであるが、このままでは測定
に長時間を要し、しかも計算が複雑であるため、
オンライン化しての実用にはあまり向かない。そ
こで、発明者らが見出した以下の知見に基き、通
常は後述の如くにする。すなわち、あらかじめ三
刺激値のフイルタをそなえた色差計の如き構造の
測光具を用い、裏面部に黒板を密着させた状態お
よび白板を密着させた状態の測定値からK/S(x)、
K/S(y)、K/S(z)を計算し、これによつて求めら
れたR∞(x)、R∞(y)、R∞(z)を用いたところ、前記
式と同様な結果が得られた。さらに、黒板を裏面
に密着させた場合のX、Y、Z三刺激値領域の測
定値をXB、YB、ZBとし、白板を密着させた場合
の測定値をXW、YW、ZWとすると、
(内部色)
X=fx(XB、YB、ZB、XW、YW、ZW)
Y=fy(XB、YB、ZB、XW、YW、ZW)
Z=fz(XB、YB、ZB、XW、YW、ZW) ……
なる関係があることも解つた。そこで、測定にあ
たり、三刺激値のフイルタを備えた測光具を用い
るようにする。そうすれば、前記のように反射率
からK/Sを求め、R∞から三刺激値を計算する
という方法によらなくとも、測定値から直接内部
色を計算推定することができ、オンライン化をは
かるうえできわめて有利となるからである。以
下、この方法を具体化する例について説明する。 The above is based on the measured values obtained from the spectrum in the visible light range using a spectrophotometer .
This method calculates Z R∞ , but as it is, it takes a long time to measure and the calculation is complicated.
It is not very suitable for practical use online. Therefore, based on the following knowledge discovered by the inventors, the method is usually performed as described below. That is, using a photometer with a structure similar to a color difference meter equipped with a tristimulus value filter in advance, K/S (x) ,
By calculating K/S (y) and K/S (z) and using the R ∞(x) , R ∞(y) , and R ∞(z) obtained from these, the result is the same as the above formula. The results were obtained. Furthermore, the measured values of the X, Y, and Z tristimulus value regions when the blackboard is brought into close contact with the back side are taken as X B , Y B , and Z B , and the measured values when the white board is brought into close contact are taken as X W , Y W , If Z W , ( internal color ) _ _ _ _ _ W , Z W ) Z=f z (X B , Y B , Z B , X W , Y W , Z W ) ... It was also found that there is a relationship. Therefore, when making measurements, a photometer equipped with a tristimulus value filter is used. In this way, the internal color can be calculated and estimated directly from the measured values without having to calculate K/S from the reflectance and tristimulus values from R ∞ as described above, making it possible to go online. This is because it is extremely advantageous for measurement. An example of implementing this method will be described below.
第4図は、この測定方法を実施する場合に用い
る測定装置の構成例をあらわすもので、白色光源
5からスリツト6を通つて射出された白色光は、
コリメータレンズ7を通つて適当なビーム径の光
線となり、ミラー8によつて被測定物である染色
単板2の表面に垂直に照射される。染色単板2の
裏面部には黒板9または白板10が交互に密着さ
せられる。染色単板2からの反射光は、積分球1
1によつて受光され、フイルター12をそなえた
測光具13によつて測定される。測光具13は、
光電変換素子を内蔵し、第4図bにあらわれてい
るように120度間隔に3組設けられており、それ
ぞれの測光具にX用、Y用およびZ用のフイルタ
が1種類ずつ取り付けられている。したがつて、
被測定物からの反射光は積分球によつて受光さ
れ、X、Y、Zの三刺激値に分解され測定され
る。 FIG. 4 shows an example of the configuration of a measuring device used when carrying out this measuring method, and the white light emitted from the white light source 5 through the slit 6 is
The light beam passes through the collimator lens 7 and becomes a light beam having an appropriate beam diameter, and is irradiated perpendicularly to the surface of the dyed veneer 2, which is the object to be measured, by the mirror 8. Blackboards 9 or whiteboards 10 are alternately brought into close contact with the back side of the dyed veneer 2. The reflected light from the dyed veneer 2 is reflected by the integrating sphere 1
1 and measured by a photometer 13 equipped with a filter 12. The photometer 13 is
It has a built-in photoelectric conversion element, and as shown in Figure 4b, three sets are provided at 120 degree intervals, and each photometer is equipped with one type of filter for X, Y, and Z. There is. Therefore,
The reflected light from the object to be measured is received by an integrating sphere, decomposed into tristimulus values of X, Y, and Z and measured.
この装置の使用に際しては、先ず種々のロツト
から種々の染色状態を代表すると思われる染色単
板を必要数だけサンプリングし、それぞれについ
て前記XB、YB、ZBおよびXW、YW、ZWの6変数
を測定する。つぎに、測定に供されたサンプルを
破壊し、実際に色が問題となる部分について測定
を行ない、それぞれのX、Y、Zを得る。測定値
が得られたら、多変量解析等の手法を用い、目的
変数をX、Y、Zとし、その説明変数としてXB、
YB、ZB、XW、YW、ZWを用いて前記関係式を
求める。この関係式が得られたら、内部色が未知
のサンプルに対してもXB、YB、ZB、XW、YW、
ZWを測定するだけで内部色X、Y、Zが推定
(計算)できるわけである。この測定法(第1の
方法と呼ぶ)をブロツク線図であらわせば第5図
の通りである。図中Aは関係式作成部分をあらわ
し、Bは未知サンプル内部色の推定部分をあらわ
す。 When using this device , first sample the required number of stained veneers from various lots that are thought to represent various dyeing conditions, and then select the Measure six variables of W. Next, the sample subjected to measurement is destroyed, and measurements are taken on the areas where the color actually becomes a problem, to obtain the respective X, Y, and Z values. Once the measured values are obtained, use a method such as multivariate analysis to set the objective variables as X, Y, and Z, and set the explanatory variables as X B ,
The above relational expression is determined using Y B , Z B , X W , Y W , and Z W . Once this relational expression is obtained, X B , Y B , Z B , X W , Y W ,
The internal colors X, Y, and Z can be estimated (calculated) simply by measuring ZW . This measurement method (referred to as the first method) is shown in FIG. 5 as a block diagram. In the figure, A represents the relational expression creation part, and B represents the estimation part of the internal color of the unknown sample.
上記第1の方法では、黒板と白板とを取り換え
て繰り返し測定する必要があるため、測定に時間
がかかりすぎる。また、被測定物を面方向に移動
させつつ測定するという場合には、黒板による測
定点と白板による測定点とを一致させることが困
難であるため、推定値の信頼性が悪くなりやす
い。そこで、このようなことを避けるためには、
次のようにするとよい。すなわち、第4図および
第5図に示す測定方法において、白板を被測定物
の裏面部に密着させる場合について考えると、第
6図に示すように染色単板2に入射した光は、色
の吸収により減衰する分と、散乱により減衰する
分とがあるが、単板を完全に透過した光は、単板
裏面の白板10により再び単板内部に反射され、
この光も反射光として受光されていることがわか
る。このことは、白板を裏面部に密着させた場合
の測定値が、透過光量を測定していることを意味
している。そこで、第1の方法における白板密着
時の測定値を、裏面に白板を当てないことによつ
て得られる真の透過光についての測定値(透過光
を三刺激値に分解し、Xt、Yt、Ztとあらわす)
に変えてやると、前記式と同様に次のような関
係式が得られた。 In the first method, the measurement takes too much time because it is necessary to replace the blackboard and the whiteboard and repeat the measurement. Furthermore, when measuring the object while moving it in the plane direction, it is difficult to match the measurement points on the blackboard with the measurement points on the whiteboard, so the reliability of the estimated value tends to deteriorate. Therefore, in order to avoid such a thing,
You can do it like this: In other words, in the measurement method shown in FIGS. 4 and 5, if we consider the case where the white board is brought into close contact with the back surface of the object to be measured, the light incident on the dyed veneer 2 as shown in FIG. There is some attenuation due to absorption and some attenuation due to scattering, but the light that has completely passed through the veneer is reflected back into the veneer by the white plate 10 on the back of the veneer.
It can be seen that this light is also received as reflected light. This means that the measured value when the white board is brought into close contact with the back surface portion measures the amount of transmitted light. Therefore, the measurement value when the white board is in close contact with the first method is the measurement value of the true transmitted light obtained by not applying the white board to the back side (the transmitted light is decomposed into tristimulus values, X t , Y t , Z t )
By changing it to , we obtained the following relational expression, similar to the above expression.
X=fx(XB、YB、ZB、Xt、Yt、Zt)
Y=fy(XB、YB、ZB、Xt、Yt、Zt)
Z=fz(XB、YB、ZB、Xt、Yt、Zt)
……
このようにして、真の透過光値を測定すること
によつても、内部色の計算推定が可能となるので
あるが、このような測定法を実施するための測定
装置の構成例を第7図に示す。同図において、白
色光源5をコリメートして適当なビーム径とし、
被測定物2に対し垂直方向から光を照射する。こ
のときの反射拡散光と透過光を、被測定物の表裏
面側に配置したそれぞれの積分球11,11′で
受光し、それぞれ三刺激値X、Y、Zに分解す
る。図中、13′はフイルター12′を備えた測光
具である。積分球11,11′にはやはり第4図
bのようにして測光具13,13′が120度の位置
で3個ずつとりつけられ、各測光具はX用、Y
用、Z用のフイルタをもつている。X=f x (X B , Y B , Z B , X t , Y t , Z t ) Y=f y (X B , Y B , Z B , X t , Y t , Z t ) Z=f z (X B , Y B , Z B , X t , Y t , Z t ) ... In this way, it is possible to calculate and estimate the internal color even by measuring the true transmitted light value. However, an example of the configuration of a measuring device for carrying out such a measuring method is shown in FIG. In the figure, the white light source 5 is collimated to an appropriate beam diameter,
Light is irradiated onto the object 2 to be measured from the vertical direction. The reflected diffused light and the transmitted light at this time are received by integrating spheres 11 and 11' placed on the front and back surfaces of the object to be measured, respectively, and decomposed into tristimulus values X, Y, and Z, respectively. In the figure, 13' is a photometer equipped with a filter 12'. Three photometers 13, 13' are attached to the integrating spheres 11, 11' at 120 degree positions as shown in Figure 4b, and each photometer is one for X and one for Y.
It has filters for Z and Z.
このようにして得られた6変数を用い、あらか
じめ求めておいた関係式によつて内部色X、
Y、Zを推定計算したのち、例えばX*、a*、b*
等の色表示系に変換して、目標とする標準色との
色素、色相差等で良否を判定する。この測定法
(第2の方法と呼ぶ)のブロツク線図は第8図に
示す通りである。図中、L*、a*、b*、ΔEの計算
は次式による。 Using the six variables obtained in this way, the internal color X,
After estimating and calculating Y and Z, for example, X * , a * , b *
The color display system is converted to a color display system such as , and quality is judged based on the pigment, hue difference, etc. with the target standard color. A block diagram of this measurement method (referred to as the second method) is shown in FIG. In the figure, L * , a * , b * , and ΔE are calculated using the following formula.
L*=116×3√−16
a*=500×( 3√− 3√)
b*=200×( 3√− 3√)
ΔE=√(*−ST)2+(*−ST)
2+(*−ST)2
(LST、aST、bSTは標準値である。)
上記第2の方法によれば、6変数が同時に同地
点で測定できるため、高速処理が容易であり精度
も上がるため、オンラインでの検査法としてすぐ
れたものとなつている。L * = 116× 3 √−16 a * = 500× ( 3 √− 3 √) b * = 200× ( 3 √− 3 √) ΔE=√ ( * − ST ) 2 + ( * − ST )
2 + ( * - ST ) 2 (L ST , a ST , b ST are standard values.) According to the second method above, six variables can be measured at the same point at the same time, making high-speed processing easy. It is also highly accurate, making it an excellent online testing method.
つぎに、上記第2の方法をさらに改良するもの
として次に述べるような第3の方法がある。すな
わち、前記第1および第2の方法では、被測定物
の含水率に大きな差があると、推定値の誤差が大
きくなつてしまうという問題があり、また、反射
光の測定の際に被測定物の表面粗さが異なると、
散乱光に起因する測定誤差が生じるおそれもある
ので、これらを補正する必要がある。このために
は、反射光と透過光による前記6変数(X、Y、
Z)のほかに、一般的に知られている水分吸収波
長1450nm付近または1950nm付近のうちのいず
れかのフイルタをそなえた測光具と、これら水分
吸収波長以外の近赤外領域の波長、例えば1100n
m付近のフイルタをそなえた測光具を装置に追加
して、これらによつて得られる測定値(透過、反
射)を含む合計10個の変数を用いて推定を行なう
のが好ましい。この場合、波長1450nmまたは
1950nmのフイルタは、これらの値をピークに±
20nm程度の巾をもつものであれば良い。また、
水分吸収域以外の波長に対しては、水分吸収域を
含まなければ、ある程度の巾があつてもさしつか
えない。ここで、水分吸収域の反射光と透過光を
それぞれWB、Wtとし、水分吸収域を含まない近
赤外波長の反射光と透過光をIRB、IRtとすると、
内部色X、Y、Zとの間には、
X=fx(XB、YB、ZB、WB、IRB、Xt、Yt、Zt
、Wt、IRt)
Y=fy(XB、YB、ZB、WB、IRB、Xt、Yt、Zt
、Wt、IRt)
Z=fz(XB、YB、ZB、WB、IRB、Xt、Yt、Zt
、Wt、IRt)
という関係が成り立つ。この関係式には、水分補
正項と表面凹凸補正項とが組み込まれているた
め、含水量と表面粗さとの補正が可能となり、よ
り精度の高い内部色推定が可能となるのである。 Next, there is a third method which will be described below as a further improvement on the second method. That is, in the first and second methods, if there is a large difference in the moisture content of the object to be measured, there is a problem that the error in the estimated value becomes large. When the surface roughness of objects differs,
Since there is a possibility that measurement errors may occur due to scattered light, it is necessary to correct these errors. For this purpose, the six variables (X, Y,
In addition to Z), a photometer equipped with a filter that has a generally known water absorption wavelength of around 1450nm or around 1950nm, and a wavelength in the near-infrared region other than these water absorption wavelengths, such as 1100nm.
Preferably, a photometer equipped with a filter around m is added to the apparatus, and a total of 10 variables including the measured values (transmission, reflection) obtained by these are used for estimation. In this case, the wavelength is 1450nm or
The 1950nm filter peaks at these values.
It is sufficient if it has a width of about 20 nm. Also,
For wavelengths other than the water absorption range, a certain width is acceptable as long as the water absorption range is not included. Here, if the reflected light and transmitted light in the water absorption region are respectively W B and W t , and the reflected light and transmitted light at near-infrared wavelengths that do not include the water absorption region are IRB and IR t , then
Between the internal colors X , Y , and Z ,
, W t , IR t ) Y=f y (X B , Y B , Z B , W B , I R B , X t , Y t , Z t
, W t , IR t ) Z=f z (X B , Y B , Z B , W B , I R B , X t , Y t , Z t
, W t , IR t ) holds true. Since this relational expression incorporates a moisture correction term and a surface unevenness correction term, it is possible to correct the moisture content and surface roughness, and it is possible to estimate the internal color with higher accuracy.
以上の説明から明らかなように、この発明にか
かる半透明物体の内部色測定方法は、被測定物を
破壊することなく、その内部の色を推定すること
ができるものであるから、染色単板等の染色状態
の検査に適した実用性の高いものである。この測
定法を他の半透明物体の内部色の推定に用いるこ
とができることは云うまでもない。 As is clear from the above description, the method for measuring the internal color of a translucent object according to the present invention is capable of estimating the internal color of the object without destroying the object. It is highly practical and suitable for inspection of staining conditions such as. It goes without saying that this measurement method can be used to estimate the internal color of other translucent objects.
第1図は人工の突板の外観図、第2図はこの突
板の製法の説明図、第3図a,bは染色単板の内
部染色状態をあらわす説明図、第4図aは測定装
置例をあらわす構成図、第4図bは積分球と測光
具の関係を示す説明図、第5図は第1の測定方法
のブロツク線図、第6図は反射光測定原理の説明
図、第7図は測定装置の他の例をあらわす構成
図、第8図は第2の測定方法のブロツク線図であ
る。
1……基板、2……染色単板、3……接着剤
層、5……白色光源、6……スリツト、7……コ
リメータレンズ、8……ミラー、9……黒板、1
0……白板、11,11′……積分球、12,1
2′……フイルタ、13,13′……測光具。
Figure 1 is an external view of the artificial veneer, Figure 2 is an explanatory diagram of the manufacturing method of this veneer, Figures 3a and b are explanatory diagrams showing the internal staining state of the dyed veneer, and Figure 4a is an example of a measuring device. Fig. 4b is an explanatory diagram showing the relationship between the integrating sphere and the photometer, Fig. 5 is a block diagram of the first measurement method, Fig. 6 is an explanatory diagram of the principle of measuring reflected light, Fig. 7 The figure is a block diagram showing another example of the measuring device, and FIG. 8 is a block diagram of the second measuring method. 1... Substrate, 2... Dyed veneer, 3... Adhesive layer, 5... White light source, 6... Slit, 7... Collimator lens, 8... Mirror, 9... Blackboard, 1
0... White board, 11,11'... Integrating sphere, 12,1
2'...Filter, 13,13'...Photometering tool.
Claims (1)
照射し、試料の裏面部に黒板を密着させて透過光
が戻つて来ないようにした状態での反射光と、被
検体を透過する光とを積分球を用いてそれぞれ測
定し、その測定結果から非破壊状態での三刺激値
を求めて、この値と実際に試料を破壊して測定し
た内部の三刺激値とを対比して、あらかじめ両者
を関係づける関係式を必要な複数組のデータから
求めておき、つぎに同様な半透明物体からなる実
際の被測定物について上記非破壊状態での三刺激
値の測定を行ない、その結果から、上記関係式に
よつて内部の色を求めることを特徴とする半透明
物体の内部色測定方法。 2 被測定物を透過する光の測定を、被測定物の
裏面部に白板を密着させた状態で被測定物からの
反射光を積分球を用いて測定することにより行な
う特許請求の範囲第1項記載の半透明物体の内部
色測定方法。 3 被測定物の表裏両側に積分球を配置するよう
にし、被測定物に照射した光の反射光を表側の積
分球で測定するとともに、同じ照射光の透過光を
裏側の積分球で測定するようにした特許請求の範
囲第1項記載の半透明物体の内部色測定方法。 4 被測定物からの反射光および透過光の三刺激
値の測定を、三刺激値のフイルタをそれぞれそな
えた3組の測光具により行なう特許請求の範囲第
1項から第3項までのいずれかに記載の半透明物
体の内部色測定方法。 5 水分吸収波長のフイルタをそなえた測光具お
よび水分吸収波長以外で近赤外領域の波長のフイ
ルタをそなえた測光具を設け、三刺激値以外に水
分吸収波長域およびそれ以外の近赤外領域での強
度を反射光および透過光について測定し、これら
のデータを関係式に加えて被検体の内部色を求め
る特許請求の範囲第4項記載の半透明物体の内部
色測定方法。[Claims] 1. Light is irradiated perpendicularly to the surface of a sample made of a semi-transparent object, and reflected light is obtained when a blackboard is placed in close contact with the back surface of the sample to prevent the transmitted light from returning; The light that passes through the specimen is measured using an integrating sphere, and the tristimulus values in a non-destructive state are determined from the measurement results, and this value is compared with the internal tristimulus values measured by actually destroying the sample. A relational expression relating the two is found in advance from multiple sets of data, and then the tristimulus values in the above non-destructive state are calculated for an actual object to be measured consisting of a similar translucent object. 1. A method for measuring the internal color of a translucent object, comprising performing a measurement and determining the internal color from the result using the above relational expression. 2. Claim 1, in which the light transmitted through the object to be measured is measured by measuring the light reflected from the object using an integrating sphere with a white plate in close contact with the back surface of the object to be measured. Method for measuring internal color of translucent objects as described in Section 1. 3 Place integrating spheres on both sides of the object to be measured, and measure the reflected light of the light irradiated to the object with the integrating sphere on the front side, and measure the transmitted light of the same irradiated light with the integrating sphere on the back side. A method for measuring the internal color of a translucent object according to claim 1. 4. Any one of claims 1 to 3, in which the tristimulus values of reflected light and transmitted light from the object to be measured are measured using three sets of photometers each equipped with a tristimulus value filter. A method for measuring the internal color of a translucent object as described in . 5 A photometer equipped with a filter for water absorption wavelengths and a photometer equipped with a filter for wavelengths in the near-infrared region other than the water absorption wavelength are provided, and in addition to the tristimulus values, a photometer equipped with a filter for water absorption wavelengths and other near-infrared regions is provided. 5. A method for measuring an internal color of a translucent object according to claim 4, wherein the intensity of reflected light and transmitted light is measured, and these data are added to a relational expression to determine the internal color of the object.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5452982A JPH0245814B2 (en) | 1982-03-31 | 1982-03-31 | HANTOMEIBUTSUTAINONAIBUSHOKUSOKUTEIHOHO |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5452982A JPH0245814B2 (en) | 1982-03-31 | 1982-03-31 | HANTOMEIBUTSUTAINONAIBUSHOKUSOKUTEIHOHO |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58171641A JPS58171641A (en) | 1983-10-08 |
| JPH0245814B2 true JPH0245814B2 (en) | 1990-10-11 |
Family
ID=12973185
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5452982A Expired - Lifetime JPH0245814B2 (en) | 1982-03-31 | 1982-03-31 | HANTOMEIBUTSUTAINONAIBUSHOKUSOKUTEIHOHO |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0245814B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60209141A (en) * | 1984-04-02 | 1985-10-21 | Shin Etsu Chem Co Ltd | Method for inspecting quality of thermoplastic resin |
| DE4030836A1 (en) * | 1990-09-28 | 1992-04-02 | Kim Yoon Ok | DEVICE FOR QUALITATIVELY AND / OR QUANTITATIVELY DETERMINING THE COMPOSITION OF A SAMPLE TO BE ANALYZED |
-
1982
- 1982-03-31 JP JP5452982A patent/JPH0245814B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58171641A (en) | 1983-10-08 |
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