WO2017163319A1 - Dispositif de mesure de couleur - Google Patents

Dispositif de mesure de couleur Download PDF

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Publication number
WO2017163319A1
WO2017163319A1 PCT/JP2016/059076 JP2016059076W WO2017163319A1 WO 2017163319 A1 WO2017163319 A1 WO 2017163319A1 JP 2016059076 W JP2016059076 W JP 2016059076W WO 2017163319 A1 WO2017163319 A1 WO 2017163319A1
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WO
WIPO (PCT)
Prior art keywords
light
measurement
target surface
spacer
measurement target
Prior art date
Application number
PCT/JP2016/059076
Other languages
English (en)
Japanese (ja)
Inventor
和彦 松尾
Original Assignee
ゾンデックス株式会社
ストローブ株式会社
カーコンビニ倶楽部株式会社
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by ゾンデックス株式会社, ストローブ株式会社, カーコンビニ倶楽部株式会社 filed Critical ゾンデックス株式会社
Priority to PCT/JP2016/059076 priority Critical patent/WO2017163319A1/fr
Publication of WO2017163319A1 publication Critical patent/WO2017163319A1/fr

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    • 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
    • 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

Definitions

  • the present invention relates to a color measuring device for measuring the color of an object surface such as the color of paint applied to an automobile body and the color of ink used in printed matter.
  • a paint with a color close to the current body color is selected from the paints in stock, and this is used as the base paint.
  • the work is to prepare a paint with a color very close to the actual color.
  • the color of the paint is basically adjusted by mixing the three primary colors of red, blue, yellow, and white. Therefore, the blending is performed by mixing the base paint little by little with the base paint.
  • the redness of the paint is darker than the body color, it is not possible to reduce only the red component from the base paint, so it is necessary to select a lighter color for the base paint than the body color.
  • a colorimeter may be used to check whether the blended paint matches the body color, but it is true that the color data of the two paints measured by the colorimeter are completely the same. In the end, it is indispensable to mix until a similar color is obtained by visual observation by the operator and to put a blur around the periphery during the painting operation.
  • the colorimeter when used for such applications, it should be used for the purpose of obtaining reference data when selecting a base paint and for confirming the identity between the color of the blend paint and the body color. For example, it is not necessary to have an accuracy that can identify 1 trillion colors or more.
  • the scattered light irradiation type colorimeter 41 shown in FIG. 4A scatters the light irradiated from the light emitting element 42 into the integrating sphere 43 by the integrating sphere 43 and measures it from the light irradiation unit 44 opened at the lower end thereof.
  • the light irradiated onto the surface 45 and reflected along the preset optical axis 46 is guided to the outside of the integrating sphere 43 and detected by the light receiving element 47 (see Patent Document 1).
  • This type of colorimeter 41 requires an integrating sphere 43 with a diameter of at least about 40 mm in order to obtain scattered light, and the light emitting element 42 and the light receiving element 47 must be disposed around the integrating sphere 43. It is necessary to secure a space for installing the light emitting element 42 and the light receiving element 47, and the optical system becomes large.
  • the annular illumination type colorimeter 51 shown in FIG. 4B irradiates the measurement point 52 with light from a plurality of light emitting elements 53 arranged in an obliquely upward manner at an equal elevation angle with the measurement point 52 as the center.
  • the reflected light is detected by the light receiving element 54 arranged in the normal direction of the measurement point (see Patent Document 2). Since the colorimeter 51 requires a space for arranging the light emitting elements 53 in an annular shape, the optical system must be enlarged.
  • the multi-angle type colorimeter 61 shown in FIG. 4 (c) emits light in a radiation direction on a plane passing through a normal line set up at the measurement point 62 so that the measurement point 62 can be irradiated with light at different incident angles. Are arranged at an angle that does not coincide with the regular reflection direction of the light emitted from each light emitting element 63..., A plurality of light emitting elements 63. Detection is performed by a light receiving element 66 arranged on one measurement optical axis 65 (see Patent Document 3).
  • the colorimeter 61 has a problem that the optical system is enlarged because the optical axis from the measurement point 62 to each of the light emitting elements 63... And the light receiving element 66 must be fan-shaped.
  • JP-A-6-207857 Japanese Patent Laid-Open No. 10-253457 JP 2006-145374 A
  • the present invention has a technical problem to enable extremely miniaturization of a probe incorporating an optical system such as a light emitting element and a light receiving element while maintaining a certain degree of accuracy.
  • the present invention provides a colorimetric apparatus that irradiates a measurement target surface with measurement light and measures the color of the measurement target surface based on the RGB light intensity included in the reflected light.
  • a light source that irradiates the measurement target surface with white measurement light emitted from the light emitting element, and a light receiving element that detects the RGB light intensity included in the reflected light from the measurement target surface,
  • a spacer is formed at the tip transparent portion of the probe, The spacer maintains the length of the optical axis from the tip light transmitting portion to the measurement target surface at a predetermined constant distance in a state where the end surface is in contact with the measurement target surface, It is formed in a shape that maintains the optical axis at an angle at which specularly reflected measurement light is not incident on the light receiving element,
  • a light separating unit is provided for eliminating the influence of disturbance light incident on the
  • the tip of a light-shielding cylindrical body having a predetermined length is used as a spacer, which is cut at an angle of 75 °, for example, and fixed to the tip of the probe, the tip of the spacer In addition to being able to maintain the length of the optical axis from the tip translucent part to the measurement target surface at a constant distance, the optical axis is 75 ° with respect to the measurement target surface. Maintained in a tilted state.
  • the measurement light emitted from the light emitting element is emitted at 75 ° (incident angle of 15 °) with respect to the measurement surface, and the regular reflection light is reflected at a reflection angle of 15 ° across the normal. Since the light receiving element is arranged along the optical axis of the probe, it does not directly detect the specular reflection light, but in a direction inclined by 30 ° with respect to the specular reflection light among the light components irregularly reflected on the measurement surface. Since only the reflected reflected light is detected, a certain degree of measurement accuracy is guaranteed.
  • the optical axis from the light emitting element to the measurement point and the optical axis from the measurement point to the light receiving element when viewed from the measurement point are fan-shaped. Since they are arranged in parallel with each other without spreading, the probe itself can be formed extremely small.
  • FIG. 1 is a cross-sectional view showing an example of a color measuring device according to the present invention.
  • the whole block diagram The perspective view which shows another Example.
  • Explanatory drawing which shows the principle of the conventional colorimetry apparatus.
  • the measurement target surface is irradiated with measurement light and the reflected light
  • the color measurement device that measures the color of the measurement target surface based on the RGB light intensity included in the light source
  • a light source that irradiates the measurement target surface with white measurement light emitted from the light emitting element
  • a A light receiving element for detecting the RGB light intensity included in the reflected light is arranged along the optical axis in the probe in which light enters and exits from the tip light transmitting portion, and the tip light transmitting portion of the probe includes A spacer is formed, and the spacer maintains the length of the optical axis from the tip light transmitting portion to the measurement target surface at a predetermined constant distance in a state where the end surface is in contact with the measurement target surface.
  • Positive on the measurement target surface It is formed in a shape that maintains the optical axis at an angle at which the measured measurement light is not incident on the light receiving element, and the influence of disturbance light incident on the light receiving element is detected when the light intensity of RGB is detected by the light receiving element.
  • a light separation means for exclusion was provided.
  • the colorimetric device 1 shown in FIGS. 1 and 2 irradiates measurement light, reflects it on the measurement target surface S, and measures the color of the measurement target surface S based on the RGB light intensity included in the reflected light. belongs to.
  • a measuring optical system 4 and a control circuit 5 are built in a substantially cylindrical probe 3 having a diameter of about 3 cm and a length of about 10 cm through which light enters and exits from the tip light transmitting portion 2.
  • a screw 6 is formed on the outer peripheral surface of the distal end side of the probe 3, and a spacer 7 for maintaining the positional relationship between the measurement optical system 4 and the measurement target surface S is screwed to the screw 6 to transmit the distal end light transmitting Part 2 is provided.
  • the measurement optical system 4 reflects the white measurement light emitted from the light emitting element 11 by the concave mirror 12, and takes in the light source 13 that irradiates the measurement target surface S from the tip transparent part 2 and the tip transparent part 2.
  • Light receiving elements 14R, 14G, and 14B that detect the light intensity of each color of RGB included in the reflected light from the surface S to be measured.
  • the light emitting element 11 is a white LED or the like and is arranged on the optical axis X so as to face the concave mirror 12.
  • the concave mirror 12 has a diameter (about 25 mm) equal to the inner diameter of the probe 3, reflects the measurement light emitted from the light emitting element 11 so as to converge toward the measurement target surface S, and, for example, the distal end light transmitting portion 2
  • the light receiving elements 14R, 14G, and 14B are arranged on the back side of the concave mirror 12 along the optical axis X.
  • the light receiving elements 14R, 14G, and 14B are arranged equiangularly around the optical axis X at a central angle of 120 °.
  • the light receiving elements 14R, 14G, and 14B are made of Si photodiodes used as RGB color sensors.
  • the maximum sensitivity wavelength of the light receiving element 14R for detecting red light is 620 nm (sensitivity wavelength range: 590 to 720 nm), and green light is detected.
  • the maximum sensitivity wavelength of the light receiving element 14G for light is selected to be 540 nm (sensitivity wavelength range: 480 to 600 nm), and the maximum sensitivity wavelength of the light receiving element 14B for detecting blue light is selected to be 460 nm (sensitivity wavelength range: 590 to 720 nm).
  • the light receiving elements 14R, 14G, and 14B are arranged so as to detect the light reflected from the measurement target surface S and taken in from the distal end light transmitting portion 2 through the slit 15 formed in the concave mirror 12.
  • the slit 15 is formed at the intersection of the spot of measurement light reflected on the concave mirror 12 and formed on the measurement target surface S, and the straight line L1 connecting the light receiving elements 14R, 14G, and 14B and the concave mirror 12.
  • the light emitted from the light emitting element 11 and transmitted through the slit 15 is prevented from being directly incident on the light receiving elements 14R, 14G, and 14B through the slit 15.
  • the light receiving elements 14R, 14G, and 14B are arranged at positions that do not overlap with the light beam L2.
  • the spacer 7 cuts the pipe tip formed of a light-shielding material at a predetermined angle (75 ° in this example), and on the pipe rear end side of the inner surface, the probe 3 A screw 21 to be screwed with the screw 6 is formed, and is formed as an attachment that is detachably attached to the probe 3. Further, the end face 22 cut obliquely does not scratch the measurement target surface S when abutted against the measurement target surface S, and cushioning material such as felt so that leakage light is not incident. (Not shown) is pasted.
  • the measurement light when the measurement light is irradiated from the light emitting element 11, the light diffusely reflected by the measurement target surface S is diffusely reflected in the spacer 7 and does not reach the light receiving elements 14 R, 14 G, and 14 B through the slit 15.
  • the inner surface of the spacer 7 has a black matte finish.
  • the spacer 7 is screwed into the probe 3 and the end surface 22 of the spacer 7 is in contact with the surface S to be measured.
  • the length to the measurement target surface S is set so as to coincide with a preset standard working distance (for example, 5 cm)
  • the standard working distance WD 5 cm can be obtained simply by bringing the end face 22 into contact with the measurement target surface S. Since a light spot can be formed at a position, measurement is always possible at a constant working distance.
  • the optical axis X of the probe 3 is at an angle of 75 ° with respect to the measurement target surface S by bringing the end surface 22 into contact with the measurement target surface S. Therefore, the incident angle of the measurement light applied to the specific target surface S can always be maintained at a constant angle and measurement can be performed under a certain condition. Furthermore, since the spacer 7 is formed of a light-shielding material, disturbance light is not incident on the spacer 7 as long as the end face 22 is in close contact with the measurement target surface.
  • the control circuit 5 performs lighting control of the light emitting element 11 and arithmetic processing for detecting the light intensity of RGB based on the detection signals of the light receiving elements 14R, 14G, and 14B. At that time, the measurement light is emitted at a predetermined light emission period.
  • a light modulator (not shown) that controls the lighting of the light emitting element 11 so as to irradiate the measurement target surface S and performs synchronous detection in synchronization with the light emission cycle by the light receiving elements 14R, 14G, and 14B is incorporated. Yes.
  • synchronous detection it is possible to eliminate light having a period different from the light emission period of the measurement light.For example, if the light emission period is set to a sufficiently high frequency compared to the change in disturbance light, the high frequency component and the low frequency component are reduced. By detecting separately and subtracting the light intensity of the low frequency component from the light intensity of the high frequency component, it is possible to detect only the reflected light intensity of the light modulated measurement light.
  • the spacer 7 formed of a light-shielding material and the light modulator are used as light separating means for eliminating disturbance light. Accordingly, the disturbance light can be prevented from entering by bringing the end surface 22 of the spacer 7 into close contact with the measurement target surface S.
  • the disturbance light is incident when the measurement target surface S is curved and the end surface 22 cannot be completely brought into close contact. Even when the light cannot be blocked, only the reflected light intensity of the measurement light can be measured by the optical modulator without being affected by disturbance light.
  • the probe 3 is connected to a computer (not shown) by wire or wirelessly, and based on the measurement signal output from the probe 3, the measurement result is displayed on a computer display (not shown) and stored in a predetermined storage area as necessary. To do.
  • the optical axis X is at an angle of 75 ° with respect to the measurement target surface S simply by bringing the end surface 22 of the spacer 7 into close contact with an arbitrary portion of the automobile body serving as the measurement target surface S.
  • the white light is reflected by the concave reflecting mirror 12 to become a convergent light beam, passes from the tip translucent portion 2 along the optical axis X through the spacer 7 and onto the measurement target surface S.
  • it is irradiated with an inclination angle of 75 ° (incident angle of 15 °), and a light spot is formed at the position of the standard working distance WD.
  • surface reflection occurs on the measurement target surface S, and the reflected light is not only specularly reflected but also diffusely reflected to the surroundings.
  • diffuse reflected light is excluded except for specularly reflected light. taking measurement.
  • the light receiving elements 14R, 14G, and 14B are arranged along the optical axis X, the light reflected in the optical axis X direction out of the light diffusely reflected by the measurement target surface S, that is, regular reflection. Only the light reflected in the direction inclined about 30 ° from the direction passes through the spacer 7, passes through the slit 15 of the concave mirror 12, and is detected by the light receiving elements 14 R, 14 G, and 14 B. Therefore, the color of the measurement target surface S can be accurately measured without being affected by the regular reflection light.
  • the light receiving elements 14R, 14G, and 14B detect light intensities of red (620 nm), green (540 nm), and blue (460 nm), which are the three primary colors of light, so that the body color can be measured from these values.
  • the measurement result is returned to an arbitrary color system and displayed by a computer that does not use a conventionally known calculation formula.
  • reflected light changes with the irradiation directions of measurement light about a metallic paint, it is possible to specify the body color by comprehensively determining the measurement results irradiated from a plurality of directions as necessary.
  • the measurement surface of the measurement target surface S is covered with the end face 22 of the spacer 7 formed of a light-shielding material, the color can be accurately measured without incident disturbance light. it can. Further, since the light emitting element 11 is blinked by the control circuit 5 at a predetermined light emission period, and the light receiving elements 14R, 14G, and 14B perform synchronous detection in synchronization with the light emission period, the measurement target surface 7 is curved. Even in the case where ambient light is incident from the gap between the 22 end faces, the color can be accurately measured in this example.
  • the high frequency component and the low frequency component can be detected separately, so that even if disturbance light is incident Only the reflected light intensity of the light-modulated measurement light can be detected.
  • the light can be built in the small probe 3, and the colorimetric device 1 can be downsized.
  • a color measuring device 31 shown in FIG. 3 is obtained by attaching a frame type spacer 32 to the probe 3 instead of the spacer 7 made of a light shielding material.
  • the spacer 32 of this example includes a nut portion 33 that is screwed onto the screw 6 of the probe 3, a tapered surface 34 that is in contact with the measurement target surface S, and a plurality of rods 35 that connect them.
  • a flange 36 perpendicular to the optical axis X is formed in the nut portion 33, and a tapered surface 34 is formed with an inclination of 75 ° with respect to the optical axis X via the rod 35.
  • a cushion material (not shown) is provided on the tapered surface 34, and an observation hole 37 is formed at a portion intersecting the optical axis X, and the light spot of the measurement light emitted from the probe 3 is the observation hole 37. It is designed to be formed inside.
  • the taper surface 34 is formed in a state in which the length from the tip translucent portion 2 to the tip of the spacer 32 along the optical axis X matches the preset standard working distance WD. If they are brought into contact with the measurement target surface S, the distances between the light emitting element 11 and the light receiving elements 14R, 14G, and 14B and the measurement target surface S are maintained at a predetermined constant distance.
  • the tapered surface 34 is inclined at 75 ° with respect to the optical axis, the optical axis X of the probe 3 is 75 with respect to the measurement target surface S by bringing the tapered surface 34 into contact with the measurement target surface S. Maintained at an angle of °. Therefore, since the light spot can be formed at the position of the standard working distance WD simply by contacting the tapered surface 34 with the measurement target surface S, it is always possible to perform measurement under certain conditions.
  • the spacer 7 or 32 is detachably attached to the probe 3 has been described.
  • the spacer 7 or 32 may be integrally formed on the probe 3.
  • the light separating means the case where the spacer 7 formed of the light blocking material and the light modulator are used together is described in the first embodiment, and the case where only the light modulator is used is described in the second embodiment. Only the spacer 7 formed in (1) may be used.
  • the present invention can be applied to the use of a color measuring device that measures the color of an automobile body or any other surface to be measured.

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  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectrometry And Color Measurement (AREA)

Abstract

L'invention concerne un dispositif de mesure de couleur extrêmement petit, qui maintient un certain niveau de précision et a un système optique dans lequel sont incorporés un élément d'émission de lumière et un élément de réception de lumière. Une sonde (3), ayant une partie de transmission de lumière frontale (2) par laquelle la lumière entre et sort, comporte, disposés le long de son axe optique (X), une source de lumière (13) qui irradie une lumière de mesure blanche sur une surface à mesurer (S) et des éléments de réception de lumière (14R, 14G, 14B) pour détecter les intensités de lumière des lumières R, G et B comprises dans la lumière réfléchie par la surface à mesurer (S). Il est formé sur la partie de transmission de lumière frontale (2) de la sonde (3) un élément d'espacement (7) qui maintient une longueur constante le long de l'axe optique (X) entre la partie de transmission de lumière frontale (2) et la surface à mesurer (S) et maintient l'axe optique (X) incliné selon un angle prescrit. Un moyen de séparation de lumière est fourni pour éliminer l'influence de la lumière ambiante incidente sur les éléments de réception de lumière (14R, 14G, 14B) lorsque les intensités de lumière des lumières R, G et B réfléchies sont détectées.
PCT/JP2016/059076 2016-03-23 2016-03-23 Dispositif de mesure de couleur WO2017163319A1 (fr)

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PCT/JP2016/059076 WO2017163319A1 (fr) 2016-03-23 2016-03-23 Dispositif de mesure de couleur

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PCT/JP2016/059076 WO2017163319A1 (fr) 2016-03-23 2016-03-23 Dispositif de mesure de couleur

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108844634A (zh) * 2018-07-10 2018-11-20 张洋 颜色识别方法
CN108896184A (zh) * 2018-07-10 2018-11-27 张洋 颜色识别方法

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60262032A (ja) * 1984-06-09 1985-12-25 Mazda Motor Corp カラ−識別装置
JPH02179428A (ja) * 1988-12-29 1990-07-12 Kawasaki Steel Corp 鏡面的反射表面を有する移動物体の測色装置
JP2000512021A (ja) * 1996-09-12 2000-09-12 カラー サビイ システムズ リミテッド カラーセンサ
US20020171824A1 (en) * 2001-05-16 2002-11-21 Overbeck James L. Glare-directed imaging
JP2007114038A (ja) * 2005-10-20 2007-05-10 Agilent Technol Inc カラーセンサ装置
WO2013011778A1 (fr) * 2011-07-15 2013-01-24 オリンパスメディカルシステムズ株式会社 Sonde

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60262032A (ja) * 1984-06-09 1985-12-25 Mazda Motor Corp カラ−識別装置
JPH02179428A (ja) * 1988-12-29 1990-07-12 Kawasaki Steel Corp 鏡面的反射表面を有する移動物体の測色装置
JP2000512021A (ja) * 1996-09-12 2000-09-12 カラー サビイ システムズ リミテッド カラーセンサ
US20020171824A1 (en) * 2001-05-16 2002-11-21 Overbeck James L. Glare-directed imaging
JP2007114038A (ja) * 2005-10-20 2007-05-10 Agilent Technol Inc カラーセンサ装置
WO2013011778A1 (fr) * 2011-07-15 2013-01-24 オリンパスメディカルシステムズ株式会社 Sonde

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108844634A (zh) * 2018-07-10 2018-11-20 张洋 颜色识别方法
CN108896184A (zh) * 2018-07-10 2018-11-27 张洋 颜色识别方法
CN108896184B (zh) * 2018-07-10 2020-12-25 张洋 颜色识别方法

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