JPS6212847B2 - - Google Patents
Info
- Publication number
- JPS6212847B2 JPS6212847B2 JP54107687A JP10768779A JPS6212847B2 JP S6212847 B2 JPS6212847 B2 JP S6212847B2 JP 54107687 A JP54107687 A JP 54107687A JP 10768779 A JP10768779 A JP 10768779A JP S6212847 B2 JPS6212847 B2 JP S6212847B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- sample
- white
- value
- integrating sphere
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/46—Measurement of colour; Colour measuring devices, e.g. colorimeters
- G01J3/50—Measurement of colour; Colour measuring devices, e.g. colorimeters using electric radiation detectors
- G01J3/51—Measurement of colour; Colour measuring devices, e.g. colorimeters using electric radiation detectors using colour filters
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/02—Details
- G01J3/0205—Optical elements not provided otherwise, e.g. optical manifolds, diffusers, windows
- G01J3/0251—Colorimeters making use of an integrating sphere
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/46—Measurement of colour; Colour measuring devices, e.g. colorimeters
- G01J3/52—Measurement of colour; Colour measuring devices, e.g. colorimeters using colour charts
- G01J3/524—Calibration of colorimeters
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/46—Measurement of colour; Colour measuring devices, e.g. colorimeters
- G01J3/465—Measurement of colour; Colour measuring devices, e.g. colorimeters taking into account the colour perception of the eye; using tristimulus detection
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Physics & Mathematics (AREA)
- Spectrometry And Color Measurement (AREA)
Description
本発明は、物体色をXYZに分けてはかる測色装
置の長期安定性に関する。
従来の測色装置は、温度変化等による測定値変
動が大きい欠点がある。その概略を次に説明す
る。第1図は従来の測色装置説明図である。光源
1よりの光は、防熱フイルター2レンズ3を経て
平行光となり、試料5に垂直に当る。試料によつ
て拡散反射した光を積分球4にて受け、さらに
XYZの各受光器6,7,8で受けて電流に変え
る。各電流は夫々増幅器9,10,11で電圧増
幅されて計測部12によつて値を表示する。基準
合わせは、XYZ値既知の基準板を試料5の位置に
固定し、計測部12にてXYZ値に合わせる。この
状態で試料の測定が可能となるが、光源光量の変
動、受光器6,7,8及増幅器9,10,11の
温度による変動がある場合に測定値が不正確とな
る。そのため、光源光量の変動を少なくし受光器
及増幅器の温度による変動を少なくする方法がと
られているが、それでも正確な測定を要する時
は、度々基準合わせを行う必要がある。
この安定性を改良した方法に、交照測光法があ
る。第2図はその説明図である。光源13から発
した光は、レンズ14,14′を通り平行光線と
なりミラー15,15′で反射し、モーター16
によつて回転する円板17(切欠孔17′付)の
ために間欠的にしや断され、試料19と基準板2
0とに間欠的に当たり拡散反射する。この光を積
分球18で捕え、受光器21で光電流に変換して
計測部23に入る。位置検出器22は、光束が基
準板に当たつているか試料に当たつているかを判
別する。すなわち、基準板に当つたときと試料に
当つたときとの比によつて測色する方法が交照測
光法である。この方法は2光路を要するため、光
路上のレンズ等が汚れて変化した場合にバランス
を失う欠点がある。また常に基準板を固定してお
くことを要する欠点も大きい。
本発明は以上述べた従来法の欠点を解消して安
定した測定値を得ることができる測色装置を提供
するものである。
実施例によつて本発明を説明する。第3図にお
いて、光源31より発した光は防熱フイルター3
2レンズ33を経て平行光束となり、試料35に
垂直に当たり、拡散反射して積分球34に捕えら
れる。さらにX,Y,Z用各受光器36,37,
38にて受光され、夫々光電流となり、各増幅器
39,40,41を通り、切換器42で切換えら
れた信号をアナログ・デジタル変換器43でデジ
タル量に変換し、マイクロコンピユータ・システ
ム44に入る。この点までは従来の測色装置と同
じであるが、本装置ではレンズ33と積分球34
との間に黒色円板(光不透過性)48、積分球3
4と試料35との間に白色円板49をおく。この
2枚の円板はモーター47の軸に結合固定して等
速回転する。黒色円板48、白色円板49は第4
図に示す形状であつて、48′,49′は光が透過
するように切欠いた孔であるから、この2枚の円
板が同時に等速回転すると第1表に示む3状態
A,B,Cを現わす。第1表において、Aは黒色
円板48白色円板49の○イの位置が光路上にある
状態で、光路を黒色円板でしや断して積分球に光
を導入しない状態であり、受光器及増幅器の零点
のズレを知るための状態である。Bは黒色円板4
8、白色円板49の○ロの位置が光路上にある状態
で黒色円板でさえぎられず白色円板で反射した光
を受光する状態である。この状態は光源及受光
器、増幅器等の総合出力の変動を確認するために
ある。Cは黒色円板48、白色円板49の○ハの位
置が光路上にある状態であつて、両円板によつて
光束はさえぎられず試料の反射光を受光する状態
である。A,B,C各状態は、黒色円板48に対
応する位置検出器50によつてマイクロコンピユ
ーターシステムに知らせる。マイクロコンピユー
ターシステムは、各状態でのXYZ値を読込み、次
に記す計算を行い、結果を表示または印字する。
また、必要に応じてXYZ値より他の表色系に変換
することができる。次に実際操作に合わせて計算
式を説明する。
基準合わせ時:XYZ値既知の白色基準板を試料
位置に固定し基準合わせスイツチ45を入れる
と、マイクロコンピユーターシステムは状態A,
B,Cにおける各XYZ値を入力する。ついで次の
計算を行う。
状態AのXYZの入力値をXOYOZO
状態BのXYZの入力値をXBYBZB
状態CのXYZの入力値をXWYWZW
とし、白色基準板の真値をあらかじめマイクロコ
ンピユーターシステムに記憶しておきその値をX
TYTZTとすると、
XW−XO……零点補正後の白色基準板入力値
XB−XO……零点補正後の白色円板入力値
XT=KX(XW−XO)
同様にしてY,Zについても
YT=KY(YW−YO)
ZT=KZ(ZW−ZO)
となるので、マイクロコンピユーターシステムは
KX,KY,KZとXB−XO,YB−YO,ZB−Z
O,XW−XO,YW−YO,ZW−ZOを記憶してお
く。
試料測定時:試料を試料位置に固定し、測定開
始スイツチ46を入れると、マイクロコンピユー
ターシステムは状態A,B,Cの各状態でのXYZ
値を入力する。
状態AのXYZの入力値をX′OY′OZ′O
状態BのXYZの入力値をX′BY′BZ′B
状態CのXYZの入力値をXSYSZS
とし、試料の真値をXDとすると
XD=K′X(XS−X′O)
KXとK′Xとの関係は光源の変動、受光素子、増
幅器の変動によるものであるから次の関係が得ら
れる。
K′X=XB−XO/X′B−X′OKX
∴XD=XB−XO/X′B−X′OKX(XS−X′O)
同様にして
YD=YB−YO/Y′B−Y′OKY(YS−Y′O)
ZD=ZB−ZO/Z′B−Z′OKZ(ZS−Z′O)
試料測定時にマイクロコンピユーターシステム
はXDYDZDを算出する。マイクロコンピユータ
ーシステムはXDYDZDを表示または印字し、必
要に応じて他の表色系にも変換することができ
る。
本発明は以上説明の如く、黒色円板48と白色
円板49を設けることにより、試料測定をする毎
に零点と白色円板49の反射光を測定して測定系
全体の安定性に変化が生じていれば、その変化分
を計算して試料の測定値に補正係数をかけて、変
動がなかつたときの数値にもどす演算を加えるこ
とにより、従来方式より格段に安定した測定値を
得ることができる。
また、従来方式で安定した測定を行うために
は、測定試料2〜3点を測る毎に白色基準板を固
定して基準値の合わせを行う必要があつたが、本
発明ではその作業は白色円板の回転が代行してい
るので、電源投入時に1回だけ白色基準板を固定
してKXKYKZの定数を記憶させれば、その後は
電源を切らない限り試料測定がいつでも可能とな
つた。
本発明による装置での時間経過による変動と、
従来方式の装置との変動との比較を第2表に示
す。以上本発明による測色装置の特色を要約する
と、自動的に零合わせできるから操作の必要がな
い。標準合わせについては光学系に基準板を固定
して標準合わせスイツチを投入するだけでよくそ
の後の較正不要、安定性については試料測定のた
び毎に回転する白色円板も自動的に測定し、その
値が変化したときはその変化分だけ測定値を補正
することにより著しく改善された。
The present invention relates to the long-term stability of a colorimeter that measures the color of an object by dividing it into XYZ. Conventional colorimetric devices have the disadvantage of large fluctuations in measured values due to temperature changes and the like. The outline will be explained next. FIG. 1 is an explanatory diagram of a conventional colorimetric device. Light from a light source 1 passes through a heat shielding filter 2 and a lens 3, becomes parallel light, and hits the sample 5 perpendicularly. The light diffusely reflected by the sample is received by the integrating sphere 4, and then
It is received by each XYZ light receiver 6, 7, and 8 and converted into electric current. Each current is voltage amplified by amplifiers 9, 10, and 11, respectively, and the value is displayed by a measuring section 12. For reference alignment, a reference plate with known XYZ values is fixed at the position of the sample 5, and the measurement unit 12 aligns it with the XYZ values. Although it is possible to measure the sample in this state, the measured value becomes inaccurate if there is a variation in the amount of light from the light source or a variation in temperature of the light receivers 6, 7, 8 and amplifiers 9, 10, 11. For this reason, methods have been adopted to reduce fluctuations in the amount of light from the light source and to reduce fluctuations due to temperature in the photoreceiver and amplifier, but it is still necessary to perform reference adjustment frequently when accurate measurements are required. A method that improves this stability is cross-illumination photometry. FIG. 2 is an explanatory diagram thereof. The light emitted from the light source 13 passes through the lenses 14 and 14', becomes a parallel beam, is reflected by the mirrors 15 and 15', and is reflected by the motor 16.
The specimen 19 and the reference plate 2
0 intermittently and is diffusely reflected. This light is captured by the integrating sphere 18, converted into photocurrent by the photodetector 21, and enters the measurement section 23. The position detector 22 determines whether the light beam is hitting the reference plate or the sample. That is, cross-illumination photometry is a method of measuring color based on the ratio of when the light hits the reference plate and when it hits the sample. Since this method requires two optical paths, it has the disadvantage of losing balance if a lens or the like on the optical path becomes dirty or changes. Another major drawback is that the reference plate must be fixed at all times. The present invention provides a color measurement device that can eliminate the drawbacks of the conventional methods described above and obtain stable measurement values. The invention will be explained by way of examples. In FIG. 3, the light emitted from the light source 31 is filtered through the heat shield filter 3.
The light beam passes through two lenses 33 and becomes a parallel beam of light, hits the sample 35 perpendicularly, is diffusely reflected, and is captured by the integrating sphere 34 . Furthermore, each of the X, Y, and Z receivers 36, 37,
The light is received at 38, becomes a photocurrent, passes through each amplifier 39, 40, and 41, and the signal switched by a switch 42 is converted into a digital quantity by an analog-to-digital converter 43, and then enters a microcomputer system 44. . Up to this point, it is the same as the conventional color measurement device, but in this device, the lens 33 and integrating sphere 34
Black disc (light-opaque) 48, integrating sphere 3 between
A white disk 49 is placed between the sample 4 and the sample 35. These two discs are connected and fixed to the shaft of a motor 47 and rotate at a constant speed. The black disk 48 and the white disk 49 are the fourth
In the shape shown in the figure, 48' and 49' are holes cut out to allow light to pass through, so if these two discs rotate at the same time at a constant speed, the three states A and B shown in Table 1 will occur. , C appears. In Table 1, A is a state in which the black disc 48 and the white disc 49 are on the optical path, and the optical path is cut off by the black disc so that no light is introduced into the integrating sphere. This is a state to know the deviation of the zero point of the photoreceiver and amplifier. B is black disk 4
8. This is a state in which the white disc 49 is located on the optical path and receives light reflected by the white disc without being blocked by the black disc. This state is used to check fluctuations in the overall output of the light source, receiver, amplifier, etc. C is a state in which the black disc 48 and the white disc 49 are located on the optical path, and the light beam is not blocked by both discs and the reflected light from the sample is received. The A, B, and C states are communicated to the microcomputer system by a position detector 50 corresponding to the black disk 48. The microcomputer system reads the XYZ values in each state, performs the calculations described below, and displays or prints the results.
Also, if necessary, it is possible to convert the XYZ values to other color systems. Next, the calculation formula will be explained according to the actual operation. When adjusting the reference: When the white reference plate with known XYZ values is fixed at the sample position and the reference adjustment switch 45 is turned on, the microcomputer system changes to state A,
Input each XYZ value in B and C. Then perform the next calculation. The input value of XYZ in state A is X O Y O Z O The input value of XYZ in state B is X B Y B Z B The input value of XYZ in state C is X W Y W Z W , and the true value of the white reference plate is is stored in the microcomputer system in advance and its value is
If T Y T Z T , then X W −X O ...White reference plate input value after zero point correction X B -X O ... White disk input value after zero point correction O ) Similarly, for Y and Z, Y T = K Y (Y W - Y O ) Z T = K Z (Z W - Z O ), so the microcomputer system has K X , K Y , K Z and X B −X O , Y B −Y O , Z B −Z
O , X W −X O , Y W −Y O , and Z W −Z O are memorized. During sample measurement: When the sample is fixed at the sample position and the measurement start switch 46 is turned on, the microcomputer system performs
Enter the value. The input value of XYZ in state A is X′ O Y′ O Z′ O The input value of XYZ in state B is X′ B Y′ B Z′ B The input value of XYZ in state C is X S Y S Z S , Letting the true value of the sample be X D , then X D = K' X (X S - X' O ) Since the relationship between K X and K ' You get a relationship. K' X = X B -X O / X ' B -X ' O K D =Y B -Y O /Y' B -Y' O K Y (Y S -Y' O ) Z D =Z B -Z O /Z' B -Z' O K Z (Z S -Z' O ) When measuring the sample, the microcomputer system calculates X D Y D Z D. The microcomputer system displays or prints X D Y D Z D and can also convert to other color systems if necessary. As explained above, by providing the black disk 48 and the white disk 49, the present invention measures the reflected light of the zero point and the white disk 49 every time a sample is measured, and changes the stability of the entire measurement system. If any change has occurred, the change is calculated, the sample measurement value is multiplied by a correction coefficient, and an operation is added to return the value to the value when there was no change. By doing so, it is possible to obtain a much more stable measurement value than with conventional methods. I can do it. In addition, in order to perform stable measurements with the conventional method, it was necessary to fix a white reference plate and adjust the reference value every time two or three measurement samples were measured, but with the present invention, this work is done using a white Since the rotation of the disc takes over, you only need to fix the white reference plate once when the power is turned on and memorize the constants of K It became. Fluctuations over time in the device according to the invention;
Table 2 shows a comparison of the fluctuations with the conventional system. To summarize the features of the color measuring device according to the present invention, zero adjustment is possible automatically, so no operation is required. For standard adjustment, all you need to do is fix the reference plate to the optical system and turn on the standard adjustment switch, and there is no need for subsequent calibration.As for stability, the white disk that rotates each time the sample is measured is automatically measured, and the When the value changed, significant improvement was achieved by correcting the measured value by the amount of change.
【表】【table】
第1図は従来の測色装置の説明図、第2図は交
照測光法の説明図、第3図は本発明に係る装置の
説明図、第4図は本発明に係る円板の形状図であ
る。
1……光源、2……防熱フイルター、3……レ
ンズ、4……積分球、5……試料、6……X受光
器、7……Y受光器、8……Z受光器、9……X
増幅器、10……Y増幅器、11……Z増幅器、
12……計測部、13……光源、14……レン
ズ、15……ミラー、16……モーター、17…
…円板、17′……切欠孔、18……積分球、1
9……試料、20……基準板、21……受光器、
22……位置検出器、23……計測部、31……
光源、32……防熱フイルター、33……レン
ズ、34……積分球、35……試料、36……X
用受光器、37……Y用受光器、38……Z用受
光器、39……X用増幅器、40……Y用増幅
器、41……Z用増幅器、42……切換器、43
……アナログ・デジタル変換器、44……マイク
ロコンピユーターシステム、45……基準合わせ
スイツチ、46……測定開始スイツチ、47……
モーター、48……黒色円板、48′……切欠
孔、49……白色円板、49′……切欠孔、50
……位置検出器。
Fig. 1 is an explanatory diagram of a conventional colorimetric device, Fig. 2 is an explanatory diagram of cross-reflection photometry, Fig. 3 is an explanatory diagram of a device according to the present invention, and Fig. 4 is a diagram of the shape of a disk according to the present invention. It is a diagram. DESCRIPTION OF SYMBOLS 1... Light source, 2... Heat shielding filter, 3... Lens, 4... Integrating sphere, 5... Sample, 6... X receiver, 7... Y receiver, 8... Z receiver, 9... ...X
Amplifier, 10...Y amplifier, 11...Z amplifier,
12...Measuring unit, 13...Light source, 14...Lens, 15...Mirror, 16...Motor, 17...
...disc, 17'...notch hole, 18...integrating sphere, 1
9...sample, 20...reference plate, 21...light receiver,
22...Position detector, 23...Measurement section, 31...
Light source, 32...Heat filter, 33...Lens, 34...Integrating sphere, 35...Sample, 36...X
receiver for Y, 37... receiver for Y, 38... receiver for Z, 39... amplifier for X, 40... amplifier for Y, 41... amplifier for Z, 42... switch, 43
...Analog-digital converter, 44...Microcomputer system, 45...Reference adjustment switch, 46...Measurement start switch, 47...
Motor, 48...Black disc, 48'...Notch hole, 49...White disc, 49'...Notch hole, 50
...Position detector.
Claims (1)
器を有する積分球をはさんで、光の入口側に一部
切欠き孔を有する光不透過性円板を、光の出口側
に一部切欠き孔を有する白色円板を配し、その両
円板が同一回転軸によつて等速回転する機構を特
徴とする測色装置。1. In the integrating sphere optical system of a colorimeter, an integrating sphere with a light receiver is sandwiched between the light-impermeable disk, which has a partially cutout hole on the light entrance side, and a part on the light exit side. A color measurement device characterized by a mechanism in which a white disk having a notch hole is arranged, and both disks rotate at a constant speed about the same rotation axis.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10768779A JPS5633516A (en) | 1979-08-25 | 1979-08-25 | Color measuring device with automatic compensation based on standard value |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10768779A JPS5633516A (en) | 1979-08-25 | 1979-08-25 | Color measuring device with automatic compensation based on standard value |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5633516A JPS5633516A (en) | 1981-04-04 |
| JPS6212847B2 true JPS6212847B2 (en) | 1987-03-20 |
Family
ID=14465416
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10768779A Granted JPS5633516A (en) | 1979-08-25 | 1979-08-25 | Color measuring device with automatic compensation based on standard value |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5633516A (en) |
Families Citing this family (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5949935U (en) * | 1982-09-24 | 1984-04-03 | 東京電色株式会社 | Automatic standard calibration device for photoelectric colorimeter |
| CH651664A5 (en) * | 1982-10-14 | 1985-09-30 | Nestle Sa | METHOD AND APPARATUS FOR MEASURING THE BRIGHTNESS OF A COLOR. |
| JPS6148734A (en) * | 1984-08-16 | 1986-03-10 | Nippon Steel Corp | Measuring device for concentration and partial pressure of gas |
| JPH0638058B2 (en) * | 1984-08-16 | 1994-05-18 | 新日本製鐵株式会社 | Gas concentration and partial pressure measuring device |
| JPS6148735A (en) * | 1984-08-16 | 1986-03-10 | Nippon Steel Corp | Measuring device for concentration and partial pressure of gas |
| JPS6150230U (en) * | 1984-09-05 | 1986-04-04 | ||
| JPS62184906A (en) * | 1986-02-12 | 1987-08-13 | Isao Matsui | Spike tire |
| JPH0346524A (en) * | 1989-07-14 | 1991-02-27 | Yokogawa Electric Corp | Colorimeter |
| JP7760237B2 (en) * | 2020-11-12 | 2025-10-27 | セイコーエプソン株式会社 | color measurement device |
| JP7707522B2 (en) | 2020-11-12 | 2025-07-15 | セイコーエプソン株式会社 | color measurement device |
| JP7631747B2 (en) | 2020-11-12 | 2025-02-19 | セイコーエプソン株式会社 | Colorimeter |
-
1979
- 1979-08-25 JP JP10768779A patent/JPS5633516A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5633516A (en) | 1981-04-04 |
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