JP2019219190A - Measuring device, image forming device, and measuring method - Google Patents

Measuring device, image forming device, and measuring method Download PDF

Info

Publication number
JP2019219190A
JP2019219190A JP2018114857A JP2018114857A JP2019219190A JP 2019219190 A JP2019219190 A JP 2019219190A JP 2018114857 A JP2018114857 A JP 2018114857A JP 2018114857 A JP2018114857 A JP 2018114857A JP 2019219190 A JP2019219190 A JP 2019219190A
Authority
JP
Japan
Prior art keywords
light
light source
light receiving
optical axis
receiving unit
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.)
Granted
Application number
JP2018114857A
Other languages
Japanese (ja)
Other versions
JP7164329B2 (en
Inventor
龍人 有村
Tatsuto Arimura
龍人 有村
京子 松田
Kyoko Matsuda
京子 松田
真 和泉
Makoto Izumi
真 和泉
直井 宏夫
Hiroo Naoi
宏夫 直井
徳山 満
Mitsuru Tokuyama
満 徳山
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Sharp Corp
Original Assignee
Sharp Corp
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 Sharp Corp filed Critical Sharp Corp
Priority to JP2018114857A priority Critical patent/JP7164329B2/en
Publication of JP2019219190A publication Critical patent/JP2019219190A/en
Application granted granted Critical
Publication of JP7164329B2 publication Critical patent/JP7164329B2/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Accessory Devices And Overall Control Thereof (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

To accurately predict the weight per unit area of printing paper.SOLUTION: A measuring device (10) includes a light source (1), a light receiving unit (2), a light limiting unit (3) for limiting light received by the light receiving unit (2), and a CPU (4). The CPU (4) calculates the grammage of printing paper (P) on the basis of the amount of light applied to the printing paper (P) from the light source (1) and the amount of light received by the light receiving unit (2).SELECTED DRAWING: Figure 1

Description

本開示は、印刷用紙などのオブジェクトの吸光度を測定し、その吸光度からオブジェクトの所定の特性を測定する測定装置、画像形成装置、および測定方法に関する。   The present disclosure relates to a measurement apparatus, an image forming apparatus, and a measurement method that measure absorbance of an object such as printing paper and measure predetermined characteristics of the object from the absorbance.

複写機などの画像形成装置において、印刷用紙に画像を適切に形成するためには、印刷用紙の種類および厚さに応じた設定が必要である。それゆえ、印刷用紙の種類および厚さを判定するために、画像形成前の設定項目として印刷用紙の坪量予測が行われている。ここで、印刷用紙の坪量予測とは、印刷用紙の単位面積当たりの重さ(坪量)を算出するための処理である。   In an image forming apparatus such as a copying machine, in order to appropriately form an image on print paper, it is necessary to make settings according to the type and thickness of the print paper. Therefore, in order to determine the type and thickness of the printing paper, the basis weight of the printing paper is predicted as a setting item before image formation. Here, the prediction of the basis weight of the printing paper is a process for calculating the weight (basis weight) per unit area of the printing paper.

画像形成装置における坪量予測は、多くの場合、印刷用紙の吸光度を測定することによって行われる。吸光度は、例えばランベルト・ベールの式を用いて算出される。具体的には、印刷用紙に照射した光の光量と、その印刷用紙を透過した透過光の光量とに基づいて、印刷用紙の吸光度が算出され、算出された吸光度に基づいて、印刷用紙の単位面積当たりの重さが見積もられる。   The basis weight prediction in the image forming apparatus is often performed by measuring the absorbance of the printing paper. The absorbance is calculated using, for example, the Lambert-Beer equation. Specifically, the absorbance of the printing paper is calculated based on the amount of light irradiated on the printing paper and the amount of transmitted light transmitted through the printing paper, and the unit of the printing paper is calculated based on the calculated absorbance. The weight per area is estimated.

光を利用して印刷用紙の種類および厚さを判別する技術の例としては、特許文献1〜3などが挙げられる。特許文献1には、印刷開始前に給紙トレイから印刷用紙を引き出し停止させたのち、印刷用紙を横切る光軸を形成する光透過型センサによって、印刷用紙を透過する光を検出し、光量に応じた電圧から印刷用紙の種類を判別する用紙種類判別方法が開示されている。また、特許文献2には、搬送される紙葉類の透過光の拡散分布に基づいて紙葉類の重送を検知する装置などが開示されている。特許文献3には、異なる波長または波長領域の照射光を記録媒体へ照射する光源部と、照射光が記録媒体を透過した透過光を受光する受光手段と、を備え、異なる波長または波長領域の光の受光量の相違に基づいて、記録媒体の厚さを判別する画像形成装置が開示されている。   Examples of techniques for determining the type and thickness of print paper using light include Patent Documents 1 to 3. In Patent Document 1, after printing paper is pulled out from a paper feed tray before printing is started and stopped, light transmitted through the printing paper is detected by a light transmission type sensor that forms an optical axis crossing the printing paper, and the amount of light is detected. A paper type determination method for determining the type of printing paper from a corresponding voltage is disclosed. Patent Document 2 discloses an apparatus that detects double feeding of paper sheets based on the diffusion distribution of transmitted light of the paper sheets being conveyed. Patent Literature 3 includes a light source unit that irradiates a recording medium with irradiation light of a different wavelength or wavelength region, and a light receiving unit that receives transmitted light having the irradiation light transmitted through the recording medium. An image forming apparatus that determines the thickness of a recording medium based on a difference in the amount of received light has been disclosed.

特開平7−196207号公報(1995年8月1日公開)JP-A-7-196207 (published August 1, 1995) 特開2001−341895号公報(2001年12月11日公開)JP 2001-341895 A (published December 11, 2001) 特開2017−102046号公報(2017年6月8日公開)JP-A-2017-102046 (published on June 8, 2017)

従来の坪量予測では、図9に示すように、光を印刷用紙に照射する発光素子と、紙を透過した透過光を受光する受光素子とは、互いの光軸がほぼ一致するように配置される。なぜならば、ランベルト・ベールの式を用いて印刷用紙の吸光度を算出するような場合、印刷用紙の吸光度を正確に測定するためには、発光素子の光軸と受光素子の光軸とをほぼ一致させることが望ましいからである。   In the conventional basis weight prediction, as shown in FIG. 9, a light emitting element that irradiates light to printing paper and a light receiving element that receives transmitted light transmitted through the paper are arranged such that their optical axes are substantially coincident with each other. Is done. This is because when calculating the absorbance of printing paper using the Lambert-Beer equation, the optical axis of the light-emitting element and the optical axis of the light-receiving element must be almost the same in order to accurately measure the absorbance of the printing paper. This is because it is desirable.

しかし、印刷用紙の吸光度は、印刷用紙内における光の散乱の程度によって影響される。すなわち、同じ坪量の印刷用紙であっても、印刷用紙内における光の散乱が大きい場合には、印刷用紙を透過した透過光の量は少なくなり、印刷用紙内における光の散乱が小さい場合には、印刷用紙を透過した透過光の量は多くなる。それゆえ、印刷用紙内における光の散乱の程度が異なる印刷用紙に対して、図9に示すように配置された発光素子および受光素子を用いて坪量予測を行った場合、正しく判別できない可能性がある。   However, the absorbance of the printing paper is affected by the degree of light scattering within the printing paper. That is, even if the printing paper has the same basis weight, when the scattering of light in the printing paper is large, the amount of transmitted light transmitted through the printing paper is small, and when the scattering of light in the printing paper is small. In this case, the amount of transmitted light transmitted through the printing paper increases. Therefore, when the basis weight is estimated using the light emitting element and the light receiving element arranged as shown in FIG. 9 on the printing paper having different degrees of light scattering in the printing paper, it may not be possible to determine correctly. There is.

印刷用紙の銘柄によって、使用されている填料および紙力増強剤などの種類および量が異なる場合もあり、このような場合、印刷用紙内における光の散乱の程度が銘柄ごとに異なっている。ここで、填料とは、紙の平滑性、不透明性、色調、および印刷適性などを改善するために添加されるものであり、例えば、白土、タルク、および炭酸カルシウムなどが挙げられる。また、紙力増強剤とは、紙の強度を増強させるために添加される薬剤であり、例えば、でんぷん、およびポリアクリルアミド系ポリマーなどが挙げられる。なお、紙力とは、破裂強度およびインターナルボンドなどの評価基準によって評価される紙の特性である。   Depending on the brand of the printing paper, the type and amount of the filler and the paper strength agent used may be different. In such a case, the degree of light scattering in the printing paper is different for each brand. Here, the filler is added to improve the smoothness, opacity, color tone, printability and the like of the paper, and examples thereof include clay, talc, and calcium carbonate. The paper strength enhancer is a chemical added to enhance the strength of paper, and includes, for example, starch and polyacrylamide-based polymers. The paper strength is a property of the paper evaluated based on evaluation criteria such as burst strength and internal bond.

例えば、特許文献1に開示されている技術を坪量予測に適用する場合、印刷用紙内における光の散乱の程度によって、印刷用紙を透過する光が影響を受ける点を考慮していないため、正確な坪量予測が困難である、という問題があった。   For example, when the technique disclosed in Patent Document 1 is applied to the basis weight prediction, since the light transmitted through the printing paper is not affected by the degree of light scattering in the printing paper, accurate There is a problem that it is difficult to predict a proper basis weight.

また、特許文献2および3に開示されている技術を坪量予測に適用する場合、コストアップが避けられないという問題があった。具体的には、特許文献2に開示されている技術では、複数の発光素子および受光素子を導入する必要があり、特許文献3に開示されている技術では、異なる波長または波長領域の照射光を記録媒体へ照射可能なレーザー、および複数の受光素子を備える必要がある。   Further, when the techniques disclosed in Patent Documents 2 and 3 are applied to the basis weight prediction, there is a problem that an increase in cost cannot be avoided. Specifically, in the technique disclosed in Patent Document 2, it is necessary to introduce a plurality of light-emitting elements and light-receiving elements, and in the technique disclosed in Patent Document 3, irradiation light of different wavelengths or wavelength regions is used. It is necessary to provide a laser capable of irradiating a recording medium and a plurality of light receiving elements.

本開示の一態様は、コストアップを抑制しつつ、印刷用紙などのオブジェクトの光の散乱の程度が異なる場合であっても、オブジェクトの所定の特性を正確に測定する測定装置、画像形成装置、および測定方法を実現することを目的とする。   One aspect of the present disclosure is a measuring device that accurately measures a predetermined characteristic of an object, even when the degree of light scattering of an object such as printing paper is different while suppressing an increase in cost, an image forming apparatus, And a measurement method.

上記の課題を解決するために、本開示の一態様に係る測定装置は、オブジェクトに照射する光を発する光源と、前記オブジェクトからの透過光を受光する受光部と、前記受光部に向かう前記透過光の一部を制限する光制限部と、を備える測定装置であって、前記光源の光軸が前記オブジェクトと交差する位置と、前記受光部の受光面の中心を通る法線が前記オブジェクトと交差する位置とは、所定の距離離れており、前記光源から前記オブジェクトに照射した光の光量と、前記受光部が受光した光の光量とに基づいて該オブジェクトの所定の特性を算出する算出部をさらに備える。   In order to solve the above-described problems, a measurement device according to an embodiment of the present disclosure includes a light source that emits light to irradiate an object, a light receiving unit that receives transmitted light from the object, and the light that is transmitted toward the light receiving unit. A light restricting unit that restricts a part of light, and a measuring device including: a position where an optical axis of the light source intersects with the object; and a normal passing through a center of a light receiving surface of the light receiving unit. The intersection is at a predetermined distance from the intersection, and a calculation unit that calculates predetermined characteristics of the object based on the amount of light emitted from the light source to the object and the amount of light received by the light receiving unit. Is further provided.

上記の課題を解決するために、本開示の一態様に係る測定方法は、オブジェクトに光源からの光を照射する光照射ステップと、前記オブジェクトからの透過光の一部を制限する光制限部を通過した光を受光部によって受光する受光ステップと、を含む測定方法であって、前記光源の光軸が前記オブジェクトと交差する位置と、前記受光部の受光面の中心を通る法線が前記オブジェクトと交差する位置とは、所定の距離離れており、前記光源から前記オブジェクトに照射した光の光量と、前記受光ステップにて受光した光の光量とに基づいて該オブジェクトの所定の特性を算出する算出ステップをさらに含む。   In order to solve the above problem, a measurement method according to an aspect of the present disclosure includes a light irradiation step of irradiating an object with light from a light source, and a light restricting unit that restricts a part of transmitted light from the object. A light receiving step of receiving the passed light by a light receiving unit, wherein the position at which the optical axis of the light source intersects the object and the normal passing through the center of the light receiving surface of the light receiving unit are the object. Is located at a predetermined distance from the light source, and calculates a predetermined characteristic of the object based on the amount of light emitted from the light source to the object and the amount of light received in the light receiving step. The method further includes a calculating step.

本開示の一態様によれば、コストアップを抑制しつつ、印刷用紙内における光の散乱の程度が異なる印刷用紙であっても、印刷用紙などのオブジェクトの所定の特性を正確に測定することができる。   According to an aspect of the present disclosure, it is possible to accurately measure a predetermined characteristic of an object such as a printing paper even if the printing paper has a different degree of light scattering within the printing paper while suppressing an increase in cost. it can.

本開示の一実施形態に係る測定装置の要部構成の一例を示す図である。FIG. 1 is a diagram illustrating an example of a main configuration of a measurement device according to an embodiment of the present disclosure. 印刷用紙内での光の散乱の度合いに応じて、印刷用紙を透過する光の強度および拡散領域の広がりが異なることを説明する図である。FIG. 4 is a diagram illustrating that the intensity of light transmitted through the printing paper and the spread of the diffusion region are different depending on the degree of scattering of light in the printing paper. 光制限部が有する開口部の例を示す図である。It is a figure showing the example of the opening which a light restricting part has. 測定装置を備える画像形成装置の構成例を示すブロック図である。FIG. 2 is a block diagram illustrating a configuration example of an image forming apparatus including a measuring device. 測定装置を備える画像形成装置の処理の流れの一例を示すフローチャートである。9 is a flowchart illustrating an example of a processing flow of the image forming apparatus including the measurement device. 光源および受光部の別の配置例を示す断面図である。It is sectional drawing which shows another example of arrangement | positioning of a light source and a light receiving part. 光源および受光部の他の配置例を示す断面図である。It is sectional drawing which shows the other example of arrangement | positioning of a light source and a light receiving part. 光源および受光部の他の配置例を示す断面図である。It is sectional drawing which shows the other example of arrangement | positioning of a light source and a light receiving part. 本開示の一実施形態に係る測定方法の有効性を実証する結果を示す図である。FIG. 7 is a diagram illustrating results demonstrating the effectiveness of the measurement method according to an embodiment of the present disclosure. 従来の坪量予測における、発光素子と受光素子との配置例を示す図である。It is a figure in the conventional basis weight prediction which shows the example of arrangement | positioning of the light emitting element and the light receiving element.

〔実施形態1〕
本開示の一態様に係る測定装置10は、オブジェクトに照射する光を発する光源1と、オブジェクトからの透過光を受光する受光部2と、受光部2に向かう透過光の一部を制限する光制限部3と、を備えている。測定装置10は、光源1からオブジェクトに照射した光の光量と、受光部2が受光した光の光量とに基づいて、オブジェクトの所定の特性を算出する装置である。ここでは、坪量対象となるオブジェクトとして、印刷に供される紙である印刷用紙Pを例に挙げて説明するが、これに限定されない。例えば、測定装置10は、布、樹脂製品、シート状のさまざまなオブジェクトに対しても適用され得る。測定装置10は、上記所定の特性として、オブジェクトの坪量、散乱係数、および異方散乱パラメータの少なくとも何れかを算出する装置である。また、測定装置10は、算出したオブジェクトの坪量、散乱係数、および異方散乱パラメータの少なくとも何れかに基づいて、印刷用紙Pの種別などを特定する構成とすることも可能である。
[Embodiment 1]
The measuring device 10 according to an aspect of the present disclosure includes a light source 1 that emits light to irradiate an object, a light receiving unit 2 that receives transmitted light from the object, and a light that limits a part of the transmitted light directed to the light receiving unit 2. A limiting unit 3. The measuring device 10 is a device that calculates a predetermined characteristic of an object based on the amount of light emitted from the light source 1 to the object and the amount of light received by the light receiving unit 2. Here, a description will be given by taking as an example the printing paper P that is the paper to be printed as the object to be weighed, but the object is not limited to this. For example, the measuring device 10 can be applied to various objects such as cloth, resin products, and sheets. The measuring device 10 is a device that calculates at least one of the basis weight, the scattering coefficient, and the anisotropic scattering parameter of the object as the predetermined characteristics. Further, the measuring device 10 may be configured to specify the type of the printing paper P based on at least one of the calculated basis weight, scattering coefficient, and anisotropic scattering parameter of the object.

以下、本開示の一実施形態について、詳細に説明する。   Hereinafter, an embodiment of the present disclosure will be described in detail.

(測定装置10の構成)
まず、測定装置10の構成について、図1を用いて説明する。図1は、本実施形態に係る測定装置10の要部構成の一例を示す図である。
(Configuration of measuring device 10)
First, the configuration of the measuring device 10 will be described with reference to FIG. FIG. 1 is a diagram illustrating an example of a main configuration of a measuring device 10 according to the present embodiment.

測定装置10は、光源1、受光部2、光制限部3、CPU4(算出部)を備えている。また、測定装置10は、定電流源5、可変抵抗6、増幅回路7、およびA/Dコンバータ8をさらに備えている。   The measuring device 10 includes a light source 1, a light receiving unit 2, a light limiting unit 3, and a CPU 4 (calculating unit). The measuring device 10 further includes a constant current source 5, a variable resistor 6, an amplifier circuit 7, and an A / D converter 8.

光源1は、典型的には発光素子であり、印刷用紙Pに照射する光を発する。光源1から印刷用紙Pに照射される光は一定の照射角θを有し、その照射角θは50〜70°であることが望ましい。ここで、光源1の照射角θとは、光源1から光を照射することが可能な角度を意図している。光源1から照射される光の強度は、光軸L1上で高く、照射角θが大きくなるにつれて低下する。一般に、光源1の照射角θは、光軸L1における光の強度から、光の強度が一定割合(例えば50%)低下するまでの角度によって表される。ここで、光源1の形状が曲線部を有する場合、光源1の「光軸」とは、光源1の発光中心部から延びる法線を意味する。なお、光源1の発光中心部から延びる法線には、光源1に垂直な垂線を含み得る。   The light source 1 is typically a light emitting element and emits light for irradiating the printing paper P. Light emitted from the light source 1 to the printing paper P has a constant irradiation angle θ, and the irradiation angle θ is desirably 50 to 70 °. Here, the irradiation angle θ of the light source 1 intends an angle at which light can be emitted from the light source 1. The intensity of light emitted from the light source 1 is high on the optical axis L1, and decreases as the irradiation angle θ increases. In general, the irradiation angle θ of the light source 1 is represented by an angle from the light intensity on the optical axis L1 until the light intensity decreases by a fixed ratio (for example, 50%). Here, when the shape of the light source 1 has a curved portion, the “optical axis” of the light source 1 means a normal extending from the light emission center of the light source 1. The normal extending from the light emission center of the light source 1 may include a perpendicular line perpendicular to the light source 1.

なお、光源1は発光中心部から放射状に光を発するものであってもよいし、発光中心部から平行光であってもよい。   In addition, the light source 1 may emit light radially from the light emission central portion, or may emit parallel light from the light emission central portion.

受光部2は、典型的には受光素子であり、印刷用紙Pを透過した光の拡散領域Bの光を受光する受光部であって、光源1の光軸L1から外れた位置に光軸L2が位置するように配置される。換言すれば、受光部2は、光源1の光軸L1から外れた位置の透過光に対して受光感度のピークを持つように配置されている。受光部2の受光角は50〜70°であることが望ましい。なお、図1に示す例では、光源1から照射される光の中心は光源1の光軸L1と一致しており、受光部2の受光角の中心は受光部2の光軸L2と一致している。なお、受光角とは、受光部2が入射光を受光することが可能な角度を意図している。受光部2の受光感度は、光軸L2上で高く、受光角が大きくなるにつれて低下する。受光部2の受光角は、光軸L2における受光感度から感度が一定割合(例えば50%)低下する角度によって表される。また、上記で受光部2の光軸L2と記載しているが、受光部2の受光面の中心を通る法線を便宜上「光軸」と表現したものである。なお、受光部2の受光面の中心を通る法線は、受光部2の受光面の中心を通る、該受光部2に垂直な垂線を含み得る。受光面の中心とは、受光感度が最も高い位置を意図しており、例えば受光面が円形の場合は円の中心である。図1に示すように、光源1の光軸L1が印刷用紙Pと交差する位置と、受光部2の受光面の中心を通る法線(光軸L2)が印刷用紙Pと交差する位置とは、所定の距離D1離れている。   The light receiving unit 2 is typically a light receiving element, and receives light in the diffusion region B of light transmitted through the printing paper P. The light receiving unit 2 is located at a position off the optical axis L1 of the light source 1. Are arranged to be located. In other words, the light receiving unit 2 is arranged so as to have a peak of the light receiving sensitivity with respect to the transmitted light at a position deviated from the optical axis L1 of the light source 1. The light receiving angle of the light receiving section 2 is desirably 50 to 70 °. In the example shown in FIG. 1, the center of the light emitted from the light source 1 matches the optical axis L1 of the light source 1, and the center of the light receiving angle of the light receiving unit 2 matches the optical axis L2 of the light receiving unit 2. ing. The light receiving angle is intended to mean an angle at which the light receiving unit 2 can receive incident light. The light receiving sensitivity of the light receiving unit 2 is high on the optical axis L2, and decreases as the light receiving angle increases. The light receiving angle of the light receiving unit 2 is represented by an angle at which the sensitivity is reduced by a fixed rate (for example, 50%) from the light receiving sensitivity on the optical axis L2. In addition, although described above as the optical axis L2 of the light receiving unit 2, the normal passing through the center of the light receiving surface of the light receiving unit 2 is expressed as "optical axis" for convenience. The normal passing through the center of the light receiving surface of the light receiving unit 2 may include a perpendicular line passing through the center of the light receiving surface of the light receiving unit 2 and perpendicular to the light receiving unit 2. The center of the light receiving surface is intended to be a position having the highest light receiving sensitivity. For example, when the light receiving surface is circular, it is the center of the circle. As shown in FIG. 1, the position where the optical axis L1 of the light source 1 intersects the printing paper P and the position where the normal (optical axis L2) passing through the center of the light receiving surface of the light receiving unit 2 intersects the printing paper P are as follows. , A predetermined distance D1.

光制限部3は、印刷用紙Pを透過して拡散した光であって、受光部2に向かう光の一部を制限する。光制限部3は、遮光性の部材であり、印刷用紙Pを透過した光の一部を遮光する。光制限部3は、受光部2に受光させる光を通過させる開口部Wを有している。すなわち、光制限部3は、光源1の光軸L1上および光軸L1に近い位置における透過光が受光部2によって受光されるのを防ぐための部材である。なお、透過光とは、光源1から印刷用紙Pに光を照射したとき、光を照射した側の面(すなわち、照射面)の裏側の面から出射される光を意味している。透過光には、照射面から印刷用紙P内に入射した光が、印刷用紙P内で拡散して、裏側の面から出射した光が含まれる。   The light restricting unit 3 restricts a part of light that is transmitted through the printing paper P and diffused, and is directed to the light receiving unit 2. The light restricting unit 3 is a light-blocking member, and blocks part of the light transmitted through the printing paper P. The light restricting unit 3 has an opening W through which light received by the light receiving unit 2 passes. That is, the light restricting unit 3 is a member for preventing the transmitted light at the position on the optical axis L1 of the light source 1 and near the optical axis L1 from being received by the light receiving unit 2. The transmitted light means light emitted from the light source 1 onto the printing paper P, which is emitted from the surface on the back side of the surface on which the light is irradiated (that is, the irradiated surface). The transmitted light includes light that enters the printing paper P from the irradiation surface, diffuses in the printing paper P, and exits from the back surface.

CPU4は、光源1へ供給する電流の制御、および受光部2から出力される受光信号に基づいて各種演算を実行する。具体的には、CPU4は、印刷用紙Pを介さずに受光部2によって受光される、光源1から印刷用紙Pに照射した光の光量と、印刷用紙Pを透過して受光部2によって受光される光の光量とを用いて(例えば、ランベルト・ベールの式)、印刷用紙Pの吸光度を算出する。また、CPU4は、予め規定された、吸光度と坪量値との対応関係に基づいて、算出した吸光度に対応する坪量を算出する。なお、坪量とは、印刷用紙Pの単位面積当たりの重量を示す値である。なお、CPU4が行う制御および演算は、集積回路(ICチップ)等に形成された論理回路(ハードウェア)によって実行されてもよい。   The CPU 4 controls the current supplied to the light source 1 and performs various calculations based on the light receiving signal output from the light receiving unit 2. Specifically, the CPU 4 receives the light received by the light receiving unit 2 without passing through the printing paper P, the amount of light emitted from the light source 1 to the printing paper P, and the light received by the light receiving unit 2 through the printing paper P. Then, the absorbance of the printing paper P is calculated using the amount of light (for example, Lambert-Beer equation). Further, the CPU 4 calculates the grammage corresponding to the calculated absorbance based on the correspondence between the absorbance and the grammage value defined in advance. The grammage is a value indicating the weight per unit area of the printing paper P. The control and calculation performed by the CPU 4 may be executed by a logic circuit (hardware) formed in an integrated circuit (IC chip) or the like.

定電流源5は、光源1に定電流を供給する部材であり、可変抵抗6は、光源1に供給する電流を制御するための抵抗である。増幅回路7は、受光部2で受光した光の光量に応じて取得される信号を増幅するための回路であり、A/Dコンバータ8は、増幅回路7にて増幅された受光信号をA/D変換してCPU4に出力する。   The constant current source 5 is a member for supplying a constant current to the light source 1, and the variable resistor 6 is a resistor for controlling the current supplied to the light source 1. The amplifying circuit 7 is a circuit for amplifying a signal obtained according to the amount of light received by the light receiving unit 2, and the A / D converter 8 converts the received light signal amplified by the amplifying circuit 7 into an A / D signal. D-converted and output to CPU4.

(印刷用紙Pを透過した光を受光する位置と透過光の強度との関係)
次に、印刷用紙Pを透過した光を受光する位置と透過光の強度との関係について、図2を用いて説明する。図2は、印刷用紙P内での光の散乱の度合いに応じて、印刷用紙Pを透過する光の強度および拡散領域Bの広がりが異なることを説明する図である。
(Relationship between position of receiving light transmitted through printing paper P and intensity of transmitted light)
Next, the relationship between the position at which the light transmitted through the printing paper P is received and the intensity of the transmitted light will be described with reference to FIG. FIG. 2 is a diagram for explaining that the intensity of light transmitted through the printing paper P and the spread of the diffusion region B differ depending on the degree of light scattering within the printing paper P.

図2に示すように、光源1から印刷用紙Pに向けて光が照射されたとき、当該印刷用紙Pを透過した光の光量は、光源1の光軸L1に近いほど高く、光源1の光軸L1から外れるほど低くなる。光源1から印刷用紙Pに照射された光が印刷用紙Pを透過するとき、当該光は印刷用紙Pの内部における光散乱によって拡散する。それゆえ、印刷用紙Pを透過した光の拡散領域Bは、印刷用紙Pに照射された光の照射領域Aよりも広くなる(図1参照)。   As shown in FIG. 2, when light is emitted from the light source 1 toward the printing paper P, the amount of light transmitted through the printing paper P is higher as the light source 1 is closer to the optical axis L1. It becomes lower as it deviates from the axis L1. When light emitted from the light source 1 onto the printing paper P passes through the printing paper P, the light is diffused by light scattering inside the printing paper P. Therefore, the diffusion area B of the light transmitted through the printing paper P is wider than the irradiation area A of the light applied to the printing paper P (see FIG. 1).

図2に示すように、高散乱の印刷用紙P(以下、高散乱用紙と記す)における透過光の強度は、印刷用紙Pに照射された光の中心付近では低く、拡散領域B2で透過光が検出される。一方、低散乱の印刷用紙P(以下、低散乱用紙と記す)では、印刷用紙Pに照射された光の中心付近では高く、拡散領域B2よりも狭い拡散領域B1で透過光が検出される。   As shown in FIG. 2, the intensity of the transmitted light in the high-scattering printing paper P (hereinafter, referred to as high-scattering paper) is low near the center of the light irradiated on the printing paper P, and the transmitted light is low in the diffusion region B2. Is detected. On the other hand, in the case of the low-scattering printing paper P (hereinafter, referred to as low-scattering paper), transmitted light is detected in the diffusion region B1 which is high near the center of the light applied to the printing paper P and narrower than the diffusion region B2.

このような印刷用紙Pの内部における光散乱の度合い(光散乱特性)は印刷用紙Pの紙質、および銘柄によって異なっている。光散乱特性の差異は、受光部2によって受光される、印刷用紙Pを透過する光の強度に影響するため、坪量に誤差を生じさせる。例えば、同程度の坪量の印刷用紙Pであっても、低散乱用紙の場合、拡散領域B1における透過光の強度は高く、高散乱用紙の場合、拡散領域B2における透過光の強度は低くなる。この傾向は、光源1の光軸L1上および光軸L1に近い位置における透過光で顕著である。それゆえ、光源1の光軸L1上および光軸L1に近い位置における透過光を受光した受光信号に基づいて印刷用紙Pの吸光度を算出した場合、低散乱用紙の見かけの吸光度は低く算出される傾向があり、高散乱用紙の見かけ吸光度は高く算出される傾向がある。その結果、本来の坪量に対して低散乱用紙では低めの坪量が算出され、高散乱用紙では高めの坪量が算出される。   The degree of light scattering inside the printing paper P (light scattering characteristics) differs depending on the quality and brand of the printing paper P. Since the difference in the light scattering characteristics affects the intensity of the light received by the light receiving unit 2 and transmitted through the printing paper P, an error occurs in the basis weight. For example, even if the printing paper P has the same basis weight, the intensity of the transmitted light in the diffusion region B1 is high in the case of the low scattering paper, and the intensity of the transmitted light in the diffusion region B2 is low in the case of the high scattering paper. . This tendency is remarkable in transmitted light on the optical axis L1 of the light source 1 and at a position close to the optical axis L1. Therefore, when the absorbance of the printing paper P is calculated based on the light receiving signal that receives the transmitted light on the optical axis L1 of the light source 1 and at a position close to the optical axis L1, the apparent absorbance of the low scattering paper is calculated to be low. There is a tendency that the apparent absorbance of the high scattering paper tends to be calculated high. As a result, a lower basis weight is calculated for low scattering paper with respect to the original basis weight, and a higher basis weight is calculated for high scattering paper.

出願人らは、受光部2が受光する光を、光源1の光軸から所定の距離D1離れた位置における透過光に制限することで、印刷用紙Pの散乱特性の差異による影響を軽減し、坪量を高精度で算出できることを見出した(後述の実施例1参照)。   The applicants limit the light received by the light receiving unit 2 to transmitted light at a position away from the optical axis of the light source 1 by a predetermined distance D1, thereby reducing the influence of the scattering characteristic of the printing paper P, It has been found that the basis weight can be calculated with high accuracy (see Example 1 described later).

そこで、測定装置10において、光源1の光軸L1上および光軸L1に近い位置の透過光を受光することを回避するために、受光部2は、光源1の光軸L1と印刷用紙Pの交点から所定の距離D1離れた位置に光軸L2と印刷用紙Pの交点が位置するように配置される。また、測定装置10は、受光部2に印刷用紙Pを透過した光の一部であって、光源1の光軸L1から所定の距離D1離れた位置の光を受光させるように光制限部3を備えている。ここで、所定の距離D1は、受光部2の受光角内に、光源1の光軸が含まれないような距離であればよく、例えば、(光源1から印刷用紙Pまでの距離)×{tan(光源1の照射角θ)}で求められる距離以上であることが望ましい。ここで照射角θとは、光軸L1と、光の強度が光軸L1における光の強度の50%に低下した光線との角度を意味する。光源1の光軸L1が、光源L1からオブジェクトに下ろした垂線に対して角度α(図示せず)だけ傾きを持っている場合、所定の距離D1は、(光源1から印刷用紙Pまでの距離)×{tan(光源の傾きα)+tan(光源1の照射角θと光源1の傾きαとの差)}で求められる距離以上が望ましい。   Therefore, in the measuring device 10, in order to avoid receiving the transmitted light on the optical axis L1 of the light source 1 and at a position close to the optical axis L1, the light receiving unit 2 is configured such that the optical axis L1 of the light source 1 is It is arranged so that the intersection of the optical axis L2 and the printing paper P is located at a position separated by a predetermined distance D1 from the intersection. In addition, the measuring device 10 controls the light restricting unit 3 so that the light receiving unit 2 receives a part of the light transmitted through the printing paper P and a position at a predetermined distance D1 from the optical axis L1 of the light source 1. It has. Here, the predetermined distance D1 may be any distance that does not include the optical axis of the light source 1 within the light receiving angle of the light receiving unit 2, for example, (distance from the light source 1 to the printing paper P) × {. It is desirable that the distance be equal to or longer than tan (irradiation angle θ of light source 1)}. Here, the irradiation angle θ means an angle between the optical axis L1 and a light beam whose light intensity is reduced to 50% of the light intensity on the optical axis L1. When the optical axis L1 of the light source 1 is inclined by an angle α (not shown) with respect to a perpendicular drawn from the light source L1 to the object, the predetermined distance D1 is (distance from the light source 1 to the printing paper P). ) × {tan (tilt α of light source) + tan (difference between irradiation angle θ of light source 1 and tilt α of light source 1)}.

この構成によれば、光の散乱の程度が異なる印刷用紙Pのそれぞれに対する坪量の誤差の発生を抑制することができる。それゆえ、測定装置10を画像形成装置100(例えば、複写機、プリンター、および複合機など)に適用した場合、各印刷用紙Pについて算出された坪量に応じて適切な印刷条件を制御して印刷を実行することができる。   According to this configuration, it is possible to suppress occurrence of an error in the basis weight for each of the printing papers P having different degrees of light scattering. Therefore, when the measuring apparatus 10 is applied to the image forming apparatus 100 (for example, a copying machine, a printer, and a multifunction peripheral), appropriate printing conditions are controlled according to the basis weight calculated for each printing paper P. Printing can be performed.

さらに、上記の構成は、複数の受光素子を備えることも、光源1として専用のレーザーを備えることも必要としていない。それゆえ、測定装置10および画像形成装置100の製造に要するコストが増大するという問題も生じない。   Further, the above configuration does not require providing a plurality of light receiving elements or providing a dedicated laser as the light source 1. Therefore, there is no problem that the cost required for manufacturing the measuring apparatus 10 and the image forming apparatus 100 increases.

(光制限部3の開口部W)
ここでは、光制限部3の開口部Wについて図3を用いて説明する。図3は、光制限部3が備える開口部Wのいくつかの例を示す図である。
(Opening W of light restricting unit 3)
Here, the opening W of the light restricting unit 3 will be described with reference to FIG. FIG. 3 is a view showing some examples of the opening W provided in the light restricting unit 3.

光制限部3は、遮光性を有する材料からなり、光源1の光軸L1上の光を遮光する。また、光制限部3は、拡散領域B内の光のうち、辺縁の光が通過するように開口部Wを備えている。これにより、受光部2によって受光される光を適切に制限することができる。   The light restricting section 3 is made of a material having a light blocking property, and blocks light on the optical axis L1 of the light source 1. In addition, the light restricting unit 3 includes an opening W so that light on the periphery of the light in the diffusion region B passes. Thereby, the light received by the light receiving unit 2 can be appropriately limited.

開口部Wは、図3の(a)および(b)に示すように、光制限部3に設けられた孔であってもよいし、図3の(c)に示すような光制限部3に設けられた切り欠きであってもよい。なお、開口部Wは、光制限部3の他の部位と異なり、光透過性を有する材料を用いて実現されていてもよい。   The opening W may be a hole provided in the light restricting portion 3 as shown in FIGS. 3A and 3B, or may be a light restricting portion 3 as shown in FIG. May be provided in the notch. Note that the opening W may be realized using a material having light transmittance, unlike the other parts of the light restricting unit 3.

(画像形成装置100)
次に、画像形成装置100の構成について、図4Aを用いて説明する。図4Aは、測定装置10を備える画像形成装置100の構成例を示すブロック図である。画像形成装置100は、測定装置10、給紙装置20、制御装置30、および印刷装置40を備えている。
(Image forming apparatus 100)
Next, the configuration of the image forming apparatus 100 will be described with reference to FIG. 4A. FIG. 4A is a block diagram illustrating a configuration example of an image forming apparatus 100 including the measuring apparatus 10. The image forming apparatus 100 includes a measuring device 10, a paper feeding device 20, a control device 30, and a printing device 40.

給紙装置20は、測定装置10に印刷用紙Pを供給する。給紙された印刷用紙Pは、光源1と受光部2との間に搬送される。   The paper feeding device 20 supplies the printing paper P to the measuring device 10. The fed printing paper P is transported between the light source 1 and the light receiving unit 2.

制御装置30は、測定装置10、給紙装置20、および印刷装置40の動作を統括して制御する。たとえば、制御装置30は、測定装置10によって算出した坪量に応じた印刷条件の制御を行う。また制御装置30は、指定した印刷条件にて印刷用紙P上に画像を形成するよう印刷装置40を制御する。   The control device 30 controls the operations of the measuring device 10, the paper feeding device 20, and the printing device 40 in an integrated manner. For example, the control device 30 controls printing conditions according to the basis weight calculated by the measuring device 10. Further, the control device 30 controls the printing device 40 to form an image on the printing paper P under the designated printing conditions.

(画像形成装置100の処理の流れ)
続いて、画像形成装置100における動作例を、図4Bを用いて説明する。図4Bは、画像形成装置100の処理の流れの一例を示すフローチャートである。
(Process Flow of Image Forming Apparatus 100)
Subsequently, an operation example in the image forming apparatus 100 will be described with reference to FIG. 4B. FIG. 4B is a flowchart illustrating an example of a processing flow of the image forming apparatus 100.

ユーザーからの印刷指示を受け付けると(ステップS1にてYES)、画像形成装置100は、印刷用紙Pが測定装置10に供給される前に、受光部2によって受光される光の光量測定を行う(ステップS2)。ステップS2の測定後、給紙装置20は、光源1と受光部2との間に印刷用紙Pが来るように印刷用紙Pを搬送し、測定装置10に印刷用紙Pを供給する(ステップS3)。   When receiving a print instruction from the user (YES in step S1), image forming apparatus 100 measures the amount of light received by light receiving unit 2 before printing paper P is supplied to measuring apparatus 10 (step S1). Step S2). After the measurement in step S2, the paper feeding device 20 conveys the printing paper P so that the printing paper P comes between the light source 1 and the light receiving unit 2, and supplies the printing paper P to the measuring device 10 (step S3). .

次に、測定装置10は、印刷用紙Pに光源1から光を照射したときに印刷用紙Pを透過する光の光量測定を行う(ステップS4:光照射ステップ、受光ステップ)。このとき、印刷用紙Pを測定装置10へ搬送するときの状態によって、測定される透過光の光量がばらつく可能性がある。そこで、CPU4は、測定される透過光の光量のばらつきが、予め設定された値(図中では、設定値)の範囲内に収まっているか否かを判定する(ステップS5:光照射ステップ、受光ステップ)。CPU4は、測定される透過光の光量のばらつきが、予め設定された値の範囲内に収まっていない場合(ステップS5にてNO)、測定された光量の平均値を算出し(ステップS6)、ばらつきが予め設定された値の範囲内に収まるまでステップS4およびS5を繰り返す。   Next, the measuring device 10 measures the amount of light transmitted through the printing paper P when the printing paper P is irradiated with light from the light source 1 (step S4: light irradiation step, light receiving step). At this time, the amount of transmitted light to be measured may vary depending on the state in which the printing paper P is transported to the measuring device 10. Therefore, the CPU 4 determines whether or not the variation in the amount of transmitted light to be measured falls within a range of a preset value (set value in the figure) (step S5: light irradiation step, light receiving step). Steps). When the variation in the amount of transmitted light that is measured is not within the range of the preset value (NO in step S5), the CPU 4 calculates an average value of the measured amounts of light (step S6). Steps S4 and S5 are repeated until the variation falls within a preset value range.

ステップS4にて測定された透過光の光量と、ステップS6にて算出された光量の平均値との差が、設定された範囲内に収まっている場合(ステップS5にてYES)、CPU4は、ステップS2にて測定した光量と、ステップS5にてYESとなったときの透過光の光量の平均値とを用いて、印刷用紙Pの吸光度を算出する(ステップS7)。そして、CPU4は、算出した吸光度から印刷用紙Pの坪量を算出する(ステップS8:算出ステップ)。   If the difference between the amount of transmitted light measured in step S4 and the average value of the amount of light calculated in step S6 falls within the set range (YES in step S5), CPU 4 The absorbance of the printing paper P is calculated using the light amount measured in step S2 and the average value of the amount of transmitted light when YES is obtained in step S5 (step S7). Then, the CPU 4 calculates the basis weight of the printing paper P from the calculated absorbance (Step S8: calculation step).

制御装置30は、測定装置10のCPU4が算出した坪量に応じて、印刷条件の制御を行い(ステップS9)、この印刷条件で印刷用紙Pに印刷を実行するよう印刷装置40を制御する(ステップS10)。   The control device 30 controls printing conditions according to the basis weight calculated by the CPU 4 of the measuring device 10 (step S9), and controls the printing device 40 to execute printing on the printing paper P under the printing conditions (step S9). Step S10).

このように構成すれば、さまざまな紙質、および銘柄の印刷用紙Pに対して、適切な印刷条件を制御して印刷を実行することができる。   With this configuration, it is possible to execute printing on the printing paper P of various paper qualities and brands by controlling appropriate printing conditions.

〔実施形態2〕
本開示の他の実施形態について、以下に説明する。なお、説明の便宜上、上記実施形態にて説明した部材と同じ機能を有する部材については、同じ符号を付記し、その説明を繰り返さない。
[Embodiment 2]
Another embodiment of the present disclosure will be described below. For convenience of explanation, members having the same functions as the members described in the above embodiment are denoted by the same reference numerals, and the description thereof will not be repeated.

受光角が狭い受光部2を用いた場合、光散乱特性が大きい印刷用紙Pに対しては、受光する透過光の光量が少なくなるため、見かけ吸光度は高く算出され、その結果、坪量は高く算出されてしまう傾向がある。   When the light receiving portion 2 having a narrow light receiving angle is used, the apparent light absorbance is calculated to be high because the amount of transmitted light to be received is small for the printing paper P having a large light scattering characteristic, and as a result, the basis weight is high. It tends to be calculated.

この誤差を回避するためには、受光部2の光軸L2の向きを調整すればよい。このような構成を備える測定装置10aの構成について、図5を用いて説明する。図5は、光源1および受光部2の別の配置例を示す断面図である。なお、測定装置10aは、図1に示す測定装置10と同様、CPU4(算出部)、定電流源5、可変抵抗6、増幅回路7、およびA/Dコンバータ8も備えている。   To avoid this error, the direction of the optical axis L2 of the light receiving section 2 may be adjusted. The configuration of the measuring device 10a having such a configuration will be described with reference to FIG. FIG. 5 is a cross-sectional view illustrating another arrangement example of the light source 1 and the light receiving unit 2. Note that the measurement device 10a also includes a CPU 4 (calculation unit), a constant current source 5, a variable resistor 6, an amplifier circuit 7, and an A / D converter 8, similarly to the measurement device 10 illustrated in FIG.

測定装置10aは、受光部光軸制御部21をさらに備えている点で、図1に示す測定装置10と異なっている。受光部光軸制御部21は、図5に示すように、受光部2の光軸L2の向きを、光制限部3の開口部Wを通過した光が受光部2によって受光されるように調節する。この受光部光軸制御部21による受光部2の光軸L2の向きの制御は、例えば、CPU4によって実行され得る。その結果、図5に示すように、光源1の光軸L1が印刷用紙Pと交差する横切る位置と、受光部2の受光面の中心を通る法線(光軸L2)が印刷用紙Pと交差する位置とは、所定の距離D2離れている。所定の距離D2は、例えば、(光源1から印刷用紙Pまでの距離)×{tan(光源1の照射角θ)}で求められる距離以上が望ましい。   The measuring device 10a is different from the measuring device 10 shown in FIG. 1 in that the measuring device 10a further includes a light receiving unit optical axis control unit 21. The light receiving unit optical axis control unit 21 adjusts the direction of the optical axis L2 of the light receiving unit 2 so that the light passing through the opening W of the light limiting unit 3 is received by the light receiving unit 2, as shown in FIG. I do. The control of the direction of the optical axis L2 of the light receiving unit 2 by the light receiving unit optical axis control unit 21 can be executed by, for example, the CPU 4. As a result, as shown in FIG. 5, the position where the optical axis L1 of the light source 1 intersects the printing paper P and the normal (optical axis L2) passing through the center of the light receiving surface of the light receiving unit 2 intersect the printing paper P. And a predetermined distance D2. The predetermined distance D2 is desirably equal to or more than a distance obtained by, for example, (distance from the light source 1 to the printing paper P) × {tan (irradiation angle θ of the light source 1)}.

受光部2の光軸L2の向きを調節することによって、受光部2が受光可能な光の領域を拡大することが可能となる。それゆえ、受光角が狭い受光部2が使用される場合であっても、上述の実施形態と同様に、高精度の坪量予測が可能である。   By adjusting the direction of the optical axis L2 of the light receiving unit 2, it is possible to enlarge the region of light that can be received by the light receiving unit 2. Therefore, even when the light receiving unit 2 having a narrow light receiving angle is used, the basis weight can be predicted with high accuracy as in the above-described embodiment.

〔実施形態3〕
本開示の他の実施形態について、以下に説明する。なお、説明の便宜上、上記実施形態にて説明した部材と同じ機能を有する部材については、同じ符号を付記し、その説明を繰り返さない。
[Embodiment 3]
Another embodiment of the present disclosure will be described below. For convenience of explanation, members having the same functions as the members described in the above embodiment are denoted by the same reference numerals, and the description thereof will not be repeated.

照射角θが狭い光源1を用いた場合、光制限部3によって光源1の光軸L1上および光軸L1に近い位置の透過光を遮光したり、光軸L1から所定の距離離れた位置の透過光を開口部Wから通過させたりすることが困難となる場合が考えられる。その結果、坪量が正しく算出されなくなる可能性がある。   When the light source 1 having a small irradiation angle θ is used, the light restricting unit 3 blocks the transmitted light on the optical axis L1 of the light source 1 and a position close to the optical axis L1, and the light restricting unit 3 controls the light at a position separated by a predetermined distance from the optical axis L1. It may be difficult to allow the transmitted light to pass through the opening W. As a result, the basis weight may not be calculated correctly.

この問題を解消するためには、光源1の光軸L1の向きを調整すればよい。このような構成を備える測定装置10bの構成について、図6を用いて説明する。図6は、光源1および受光部2の他の配置例を示す断面図である。なお、測定装置10aは、図1に示す測定装置10と同様、CPU4(算出部)、定電流源5、可変抵抗6、増幅回路7、およびA/Dコンバータ8も備えている。   To solve this problem, the direction of the optical axis L1 of the light source 1 may be adjusted. The configuration of the measuring device 10b having such a configuration will be described with reference to FIG. FIG. 6 is a cross-sectional view illustrating another arrangement example of the light source 1 and the light receiving unit 2. Note that the measurement device 10a also includes a CPU 4 (calculation unit), a constant current source 5, a variable resistor 6, an amplifier circuit 7, and an A / D converter 8, similarly to the measurement device 10 illustrated in FIG.

測定装置10bは、光源光軸制御部11をさらに備えている点で、図1に示す測定装置10と異なっている。光源光軸制御部11は、図6に示すように、光源1の光軸L1の向きを調節する。光源光軸制御部11は、例えば、光源1の光軸L1が印刷用紙Pに対して垂直に光を照射する向きとは異なる向きに制御する。その結果、図6に示すように、光源1の光軸L1が印刷用紙Pと交差する位置と、受光部2の受光面の中心を通る法線(光軸L2)が印刷用紙Pと交差する位置とは、所定の距離D3離れている。所定の距離D3は、例えば、(光源1から印刷用紙Pまでの距離)×{tan(光源の傾きα)+tan(光源1の照射角θと光源1の傾きαとの差)}で求められる距離以上が望ましい。この光源光軸制御部11による光源1の光軸L1の向きの制御は、例えば、CPU4によって実行され得る。   The measuring device 10b is different from the measuring device 10 shown in FIG. 1 in that the measuring device 10b further includes a light source optical axis control unit 11. The light source optical axis control unit 11 adjusts the direction of the optical axis L1 of the light source 1, as shown in FIG. The light source optical axis control unit 11 controls, for example, a direction in which the optical axis L1 of the light source 1 irradiates the printing paper P with light vertically. As a result, as shown in FIG. 6, the position where the optical axis L1 of the light source 1 intersects the printing paper P and the normal (optical axis L2) passing through the center of the light receiving surface of the light receiving unit 2 intersect the printing paper P. The position is apart from the position by a predetermined distance D3. The predetermined distance D3 is obtained, for example, by (distance from the light source 1 to the printing paper P) × {tan (tilt α of the light source) + tan (difference between the irradiation angle θ of the light source 1 and the tilt α of the light source 1)}. It is desirable that the distance be longer than the distance. The control of the direction of the optical axis L1 of the light source 1 by the light source optical axis control unit 11 can be executed by, for example, the CPU 4.

光源1の光軸L1が印刷用紙Pに対して垂直に光を照射する向きとは異なる向きに制御されることにより、印刷用紙Pに照射された光の照射領域Aを拡大することができる。これにより、光軸L1から所定の距離D3離れた位置の透過光を開口部Wから通過させて、受光部2に受光させることが容易となる。   By controlling the optical axis L1 of the light source 1 to a direction different from the direction in which light is emitted perpendicularly to the printing paper P, the irradiation area A of the light applied to the printing paper P can be enlarged. Thereby, it becomes easy to transmit the transmitted light at a position separated by a predetermined distance D3 from the optical axis L1 through the opening W and make the light receiving unit 2 receive the transmitted light.

〔実施形態4〕
本開示の他の実施形態について、以下に説明する。なお、説明の便宜上、上記実施形態にて説明した部材と同じ機能を有する部材については、同じ符号を付記し、その説明を繰り返さない。
[Embodiment 4]
Another embodiment of the present disclosure will be described below. For convenience of explanation, members having the same functions as the members described in the above embodiment are denoted by the same reference numerals, and the description thereof will not be repeated.

照射角θが狭い光源1と受光角が狭い受光部2とを併せて用いた場合、光源1の光軸L1から所定の距離離れた位置の透過光を受光部2が受光することが困難となり、高散乱用紙の場合には受光部2によって受光される光の光量が低くなるという問題が生じ得る。その結果、坪量に誤差が生じる可能性がある。   When the light source 1 having a narrow irradiation angle θ and the light receiving section 2 having a narrow light receiving angle are used together, it becomes difficult for the light receiving section 2 to receive the transmitted light at a position away from the optical axis L1 of the light source 1 by a predetermined distance. On the other hand, in the case of high scattering paper, there may be a problem that the amount of light received by the light receiving unit 2 is low. As a result, an error may occur in the grammage.

この誤差を回避するためには、光源1の光軸L1の向きを調整するとともに、受光部2の光軸L2の向きも調整すればよい。このような構成を備える測定装置10cの構成について、図7を用いて説明する。図7は、光源1および受光部2の他の配置例を示す断面図である。なお、測定装置10aは、図1に示す測定装置10と同様、CPU4(算出部)、定電流源5、可変抵抗6、増幅回路7、およびA/Dコンバータ8も備えている。   In order to avoid this error, the direction of the optical axis L1 of the light source 1 and the direction of the optical axis L2 of the light receiving section 2 may be adjusted. The configuration of the measuring apparatus 10c having such a configuration will be described with reference to FIG. FIG. 7 is a cross-sectional view illustrating another arrangement example of the light source 1 and the light receiving unit 2. Note that the measurement device 10a also includes a CPU 4 (calculation unit), a constant current source 5, a variable resistor 6, an amplifier circuit 7, and an A / D converter 8, similarly to the measurement device 10 illustrated in FIG.

測定装置10cは、光源光軸制御部11および受光部光軸制御部21の双方をさらに備えている点で、図1に示す測定装置10と異なっている。光源光軸制御部11および受光部光軸制御部21はそれぞれ、光源1および受光部2の光軸L2の向きを、光制限部3の開口部Wを通過した光が受光部2によって受光されるように調節する。その結果、図7に示すように、光源1の光軸L1が印刷用紙Pと交差する位置と、受光部2の受光面の中心を通る法線(光軸L2)が印刷用紙Pと交差する位置とは、所定の距離D4離れている。所定の距離D4は、例えば、(光源1から印刷用紙Pまでの距離)×{tan(光源の傾きα)+tan(光源1の照射角θと光源1の傾きαとの差)}で求められる距離以上が望ましい。この受光部光軸制御部21による受光部2の光軸L2の向きの制御は、例えば、CPU4によって実行され得る。   The measuring device 10c is different from the measuring device 10 shown in FIG. 1 in that both the light source optical axis control unit 11 and the light receiving unit optical axis control unit 21 are further provided. The light source optical axis control unit 11 and the light receiving unit optical axis control unit 21 determine the direction of the optical axis L2 of the light source 1 and the light receiving unit 2, respectively, and the light passing through the opening W of the light limiting unit 3 is received by the light receiving unit 2. To adjust. As a result, as shown in FIG. 7, the position where the optical axis L1 of the light source 1 intersects the printing paper P and the normal (optical axis L2) passing through the center of the light receiving surface of the light receiving unit 2 intersect the printing paper P. The position is apart from the position by a predetermined distance D4. The predetermined distance D4 is obtained by, for example, (distance from the light source 1 to the printing paper P) × {tan (inclination α of the light source) + tan (difference between the irradiation angle θ of the light source 1 and the inclination α of the light source 1)}. It is desirable that the distance be longer than the distance. The control of the direction of the optical axis L2 of the light receiving unit 2 by the light receiving unit optical axis control unit 21 can be executed by, for example, the CPU 4.

光源光軸制御部11および受光部光軸制御部21の双方を備えることにより、照射領域Aの拡大、および受光部2が受光可能な光の領域の拡大との両方を実現することができる。それゆえ、照射角θが狭い光源1と受光角が狭い受光部2とが併せて用いられている場合であっても、高精度の坪量予測が可能である。   By providing both the light source optical axis control unit 11 and the light receiving unit optical axis control unit 21, both the expansion of the irradiation area A and the expansion of the area of light that can be received by the light receiving unit 2 can be realized. Therefore, even when the light source 1 having a narrow irradiation angle θ and the light receiving unit 2 having a narrow light receiving angle are used together, it is possible to accurately estimate the basis weight.

本開示は上述した各実施形態に限定されるものではなく、請求項に示した範囲で種々の変更が可能であり、異なる実施形態にそれぞれ開示された技術的手段を適宜組み合わせて得られる実施形態についても本開示の技術的範囲に含まれる。さらに、各実施形態にそれぞれ開示された技術的手段を組み合わせることにより、新しい技術的特徴を形成することができる。   The present disclosure is not limited to the above embodiments, and various modifications are possible within the scope of the claims, and embodiments obtained by appropriately combining the technical means disclosed in different embodiments. Is also included in the technical scope of the present disclosure. Furthermore, new technical features can be formed by combining the technical means disclosed in each embodiment.

本開示の一実施例について以下に説明する。   One embodiment of the present disclosure will be described below.

図8は、本開示の一実施形態に係る測定方法の有効性を実証する結果を示す図である。なお、以下では、印刷用紙Pの秤量を測定した場合を例に挙げ、その結果について記載する。   FIG. 8 is a diagram illustrating results that demonstrate the effectiveness of the measurement method according to an embodiment of the present disclosure. In the following, a case where the weighing of the printing paper P is measured will be described as an example, and the results will be described.

印刷用紙Pに光を照射して、その印刷用紙Pの吸光度を算出し、吸光度から坪量を測定した。印刷用紙Pの試料としては、市販されている4種類の印刷用紙a、b、c、およびdを用いた。印刷用紙a、b、c、およびdについて、予め実測された坪量値はそれぞれ、67.55g/m、68.85g/m、75.36g/m、90.25g/mであった。 The printing paper P was irradiated with light, the absorbance of the printing paper P was calculated, and the basis weight was measured from the absorbance. As samples of the printing paper P, four types of printing papers a, b, c, and d which are commercially available were used. For the printing papers a, b, c, and d, the previously measured basis weight values were 67.55 g / m 2 , 68.85 g / m 2 , 75.36 g / m 2 , and 90.25 g / m 2 , respectively. there were.

光源1として、940nmの波長の光を発する発光LED(epitex社製のSMT940D)を用い、受光部2として、シリコンPINフォトダイオード(Vishay社製)を用いた。   As the light source 1, a light emitting LED (SMT940D manufactured by epitex) emitting light having a wavelength of 940 nm was used, and as the light receiving unit 2, a silicon PIN photodiode (manufactured by Vishay) was used.

本実施例で用いた光源の照射角θは61°で、光源からオブジェクトまでの距離は2mmで、光源の傾きは0°であることから、所定の距離(図1の所定の距離D1参照)の目安としては、前記計算式より2mm×tan(61°)=3.61mm以上となる。   The irradiation angle θ of the light source used in this embodiment is 61 °, the distance from the light source to the object is 2 mm, and the inclination of the light source is 0 °, so that the predetermined distance (see the predetermined distance D1 in FIG. 1) Is 2 mm × tan (61 °) = 3.61 mm or more from the above formula.

光制限部3としては、開口部Wが直径3mmの円形の孔であるものを用いた。   As the light restricting portion 3, an opening W having a circular hole with a diameter of 3 mm was used.

光源1の光軸L1が印刷用紙Pに対してほぼ垂直になるように光を照射した。受光部2は、その光軸L2が印刷用紙Pに対してほぼ垂直になるように設置された。その上で、光源1の光軸L1に対して、受光部2の位置を変更して、印刷用紙a、b、c、およびdの吸光度を測定した。図8の(a)は、各測定位置において算出された印刷用紙a、b、c、およびdの吸光度をプロットしたグラフである。   The light was irradiated such that the optical axis L1 of the light source 1 was substantially perpendicular to the printing paper P. The light receiving section 2 is installed such that its optical axis L2 is substantially perpendicular to the printing paper P. Then, the position of the light receiving unit 2 was changed with respect to the optical axis L1 of the light source 1, and the absorbance of the printing papers a, b, c, and d was measured. FIG. 8A is a graph in which the absorbances of the printing papers a, b, c, and d calculated at each measurement position are plotted.

印刷用紙a、b、c、およびdの散乱特性が同じであれば、坪量と吸光度は正の相関を持つ。吸光度が高いほど坪量が大きくなる。しかし、実際には、印刷用紙a、b、c、およびdの散乱特性がそれぞれ異なるため、坪量と吸光度は正の相関を示さない。例えば、図8の(a)によれば、実測坪量値が67.55g/mの印刷用紙aの方が、実測坪量値が75.36g/mの印刷用紙cよりも高い吸光度を示している。 If the scattering properties of the printing papers a, b, c, and d are the same, the basis weight and the absorbance have a positive correlation. The higher the absorbance, the greater the basis weight. However, in practice, since the scattering properties of the printing papers a, b, c, and d are different from each other, the basis weight and the absorbance do not show a positive correlation. For example, according to (a) in FIG. 8, the measured basis weight values found the following printing paper a of 67.55g / m 2, high absorbance than the printing paper c of the measured basis weight values 75.36g / m 2 Is shown.

図8の(b)は、光源1の光軸L1上で測定された光量から算出された吸光度と実測坪量値との関係をプロットしたグラフである。プロットされた各点について直線近似を行い、相関係数Rを求めたところ、0.4654となった。光源1の光軸L1上で測定された吸光度と実測坪量値との間に高い相関は認められなかった。 FIG. 8B is a graph in which the relationship between the absorbance calculated from the amount of light measured on the optical axis L1 of the light source 1 and the measured basis weight value is plotted. Performs straight-line approximation for each point plotted, The correlation coefficient R 2, became 0.4654. No high correlation was observed between the absorbance measured on the optical axis L1 of the light source 1 and the measured basis weight value.

一方、図8の(c)は、光源1の光軸L1から所定の距離(この実施例では、4mm)離れた位置において測定された光量から算出された吸光度と実測坪量値との関係をプロットしたグラフである。プロットされた各点について直線近似を行い、相関係数Rを求めたところ、0.9972となった。光源1の光軸L1上で測定された吸光度と実測坪量値との間に高い相関が認められた。他の位置についても確認したところ、前記計算式から求められる距離(3.61mm)以上の位置において、同様に高い相関が認められた。なお、距離があまりにも大きくなる(光軸L1から離れる)と、受光部2が受光する光が減少してしまう。すなわち、坪量等を高精度で測定するための距離の上限は、受光部2の受光感度との兼ね合いで適宜設計され得る。 On the other hand, FIG. 8C shows the relationship between the absorbance calculated from the amount of light measured at a position separated from the optical axis L1 of the light source 1 by a predetermined distance (4 mm in this embodiment) and the measured basis weight value. It is a graph plotted. Performs straight-line approximation for each point plotted, The correlation coefficient R 2, became 0.9972. A high correlation was observed between the absorbance measured on the optical axis L1 of the light source 1 and the measured basis weight value. When other positions were confirmed, similarly, a high correlation was recognized at a position equal to or longer than the distance (3.61 mm) obtained from the above formula. If the distance is too large (away from the optical axis L1), the light received by the light receiving unit 2 will decrease. That is, the upper limit of the distance for measuring the grammage or the like with high accuracy can be appropriately designed in consideration of the light receiving sensitivity of the light receiving unit 2.

このように、受光部2が受光する光を、光源1の光軸から所定の距離離れた位置における透過光を用いて算出された吸光度を用いることで、印刷用紙Pが高散乱特性であるか低散乱特性であるかに依らず、高精度で坪量を算出できた。   As described above, by using the light received by the light receiving unit 2 with the absorbance calculated using the transmitted light at a position separated from the optical axis of the light source 1 by a predetermined distance, the printing paper P has high scattering characteristics. Regardless of the low scattering characteristics, the basis weight could be calculated with high accuracy.

1 光源
2 受光部
3 光制限部
4 CPU(算出部)
10、10a、10b、10c 測定装置
11 光源光軸制御部
21 受光部光軸制御部
100 画像形成装置
L1 光源の光軸
L2 受光部の光軸
B、B1、B2 拡散領域
W 開口部
θ 光源の照射角
Reference Signs List 1 light source 2 light receiving unit 3 light limiting unit 4 CPU (calculation unit)
10, 10a, 10b, 10c Measuring device 11 Light source optical axis control unit 21 Light receiving unit optical axis control unit 100 Image forming device L1 Optical axis of light source L2 Optical axis B, B1, B2 of light receiving unit Diffusion area W Opening θ Light source Illumination angle

Claims (11)

オブジェクトに照射する光を発する光源と、
前記オブジェクトからの透過光を受光する受光部と、
前記受光部に向かう前記透過光の一部を制限する光制限部と、
を備える測定装置であって、
前記光源の光軸が前記オブジェクトと交差する位置と、前記受光部の受光面の中心を通る法線が前記オブジェクトと交差する位置とは、所定の距離離れており、
前記光源から前記オブジェクトに照射した光の光量と、前記受光部が受光した光の光量とに基づいて該オブジェクトの所定の特性を算出する算出部をさらに備えることを特徴とする測定装置。
A light source that emits light to illuminate the object,
A light receiving unit that receives transmitted light from the object,
A light limiting unit that limits a part of the transmitted light toward the light receiving unit,
A measuring device comprising:
The position at which the optical axis of the light source intersects with the object and the position at which the normal passing through the center of the light receiving surface of the light receiving unit intersects with the object are separated by a predetermined distance,
A measuring apparatus, further comprising a calculating unit that calculates a predetermined characteristic of the object based on a light amount of light emitted from the light source to the object and a light amount of light received by the light receiving unit.
前記光制限部は、前記光源の光軸上の光を遮光することを特徴とする請求項1に記載の測定装置。   The measuring device according to claim 1, wherein the light restricting unit blocks light on an optical axis of the light source. 前記光制限部は、前記光源の光軸から所定の距離離れた位置の光が通過する開口部を備えることを特徴とする請求項1または2に記載の測定装置。   The measuring device according to claim 1, wherein the light restricting unit includes an opening through which light at a position separated by a predetermined distance from an optical axis of the light source passes. 前記開口部は、切り欠きまたは孔であることを特徴とする請求項3に記載の測定装置。   The measuring device according to claim 3, wherein the opening is a notch or a hole. 前記所定の距離は、前記受光部の受光角内に、前記光源の光軸が含まれないような距離であることを特徴とする請求項1から4のいずれか1項に記載の測定装置。   The measuring device according to claim 1, wherein the predetermined distance is a distance that does not include an optical axis of the light source within a light receiving angle of the light receiving unit. 前記所定の距離は、前記光源から前記オブジェクトまでの距離と、前記光源の照射角の正接との積で求められる値以上であることを特徴とする請求項1から5のいずれか1項に記載の測定装置。   The said predetermined distance is more than the value calculated | required by the product of the distance from the said light source to the said object, and the tangent of the irradiation angle of the said light source, The Claim 1 characterized by the above-mentioned. Measuring device. 前記受光部の光軸の向きを制御する受光部光軸制御部をさらに備えることを特徴とする請求項1から6のいずれか1項に記載の測定装置。   The measuring apparatus according to claim 1, further comprising a light receiving unit optical axis control unit configured to control a direction of an optical axis of the light receiving unit. 前記光源の光軸の向きを制御する光源光軸制御部をさらに備えることを特徴とする請求項1から7のいずれか一項に記載の測定装置。   The measuring apparatus according to claim 1, further comprising a light source optical axis control unit configured to control a direction of an optical axis of the light source. 前記オブジェクトの坪量、散乱係数、および異方散乱パラメータの少なくとも何れかを算出することを特徴とする請求項1から8のいずれか1項に記載の測定装置。 The measuring device according to claim 1, wherein at least one of a basis weight, a scattering coefficient, and an anisotropic scattering parameter of the object is calculated. 請求項1から9のいずれか1項に記載の測定装置を備えることを特徴とする画像形成装置。   An image forming apparatus, comprising: the measuring device according to claim 1. オブジェクトに光源からの光を照射する光照射ステップと、
前記オブジェクトからの透過光の一部を制限する光制限部を通過した光を受光部によって受光する受光ステップと、
を含む測定方法であって、
前記光源の光軸が前記オブジェクトと交差する位置と、前記受光部の受光面の中心を通る法線が前記オブジェクトと交差する位置とは、所定の距離離れており、
前記光源から前記オブジェクトに照射した光の光量と、前記受光ステップにて受光した光の光量とに基づいて該オブジェクトの所定の特性を算出する算出ステップをさらに含むことを特徴とする測定方法。
A light irradiation step of irradiating the object with light from a light source;
A light receiving step of receiving, by a light receiving unit, light that has passed through a light limiting unit that limits a part of transmitted light from the object,
A measurement method comprising:
The position at which the optical axis of the light source intersects with the object and the position at which the normal passing through the center of the light receiving surface of the light receiving unit intersects with the object are separated by a predetermined distance,
A measuring step of calculating a predetermined characteristic of the object based on a light amount of light emitted from the light source to the object and a light amount of light received in the light receiving step.
JP2018114857A 2018-06-15 2018-06-15 Measuring device and image forming device Active JP7164329B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2018114857A JP7164329B2 (en) 2018-06-15 2018-06-15 Measuring device and image forming device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2018114857A JP7164329B2 (en) 2018-06-15 2018-06-15 Measuring device and image forming device

Publications (2)

Publication Number Publication Date
JP2019219190A true JP2019219190A (en) 2019-12-26
JP7164329B2 JP7164329B2 (en) 2022-11-01

Family

ID=69096125

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2018114857A Active JP7164329B2 (en) 2018-06-15 2018-06-15 Measuring device and image forming device

Country Status (1)

Country Link
JP (1) JP7164329B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2022215453A1 (en) * 2021-04-07 2022-10-13 ウシオ電機株式会社 Optical measuring device and optical measuring method
JP7447556B2 (en) 2020-03-05 2024-03-12 コニカミノルタ株式会社 Image forming apparatus, image forming apparatus control method, and image forming apparatus control program

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57155469U (en) * 1981-03-26 1982-09-30
US20040189977A1 (en) * 2003-03-31 2004-09-30 Nihon Kohden Corporation Flow cytometer for classifying leukocytes and method for determining detection angle range of the same
JP2010008351A (en) * 2008-06-30 2010-01-14 Arkray Inc Scattered light measuring method and scattered light measuring device used for the same
JP2010189137A (en) * 2009-02-18 2010-09-02 Toshiba Corp Device and method for determining kind of paper sheet, and image forming apparatus

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57155469U (en) * 1981-03-26 1982-09-30
US20040189977A1 (en) * 2003-03-31 2004-09-30 Nihon Kohden Corporation Flow cytometer for classifying leukocytes and method for determining detection angle range of the same
JP2010008351A (en) * 2008-06-30 2010-01-14 Arkray Inc Scattered light measuring method and scattered light measuring device used for the same
JP2010189137A (en) * 2009-02-18 2010-09-02 Toshiba Corp Device and method for determining kind of paper sheet, and image forming apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7447556B2 (en) 2020-03-05 2024-03-12 コニカミノルタ株式会社 Image forming apparatus, image forming apparatus control method, and image forming apparatus control program
WO2022215453A1 (en) * 2021-04-07 2022-10-13 ウシオ電機株式会社 Optical measuring device and optical measuring method

Also Published As

Publication number Publication date
JP7164329B2 (en) 2022-11-01

Similar Documents

Publication Publication Date Title
US8971749B2 (en) Optical sensor and image forming apparatus
US11249020B2 (en) Determination apparatus for determining type of recording medium and image forming apparatus using the same
US8942583B2 (en) Optical sensor and image forming apparatus
JP6083119B2 (en) Optical sensor and image forming apparatus
US20130216246A1 (en) Optical sensor and image forming apparatus
US7813891B2 (en) Methods and systems for detecting spectrophotometer misalignment
JP2006177960A (en) Light-emitting diode spectrophotometer with improved spectrum range
JP7164329B2 (en) Measuring device and image forming device
JP2007187570A (en) Reflection-type optical sensor and surface roughness detecting method of measuring surface
WO2018029884A1 (en) Image formation device and determination method
US6713775B2 (en) Method to correct for sensitivity variation of media sensors
US20110222892A1 (en) Density sensor and image forming apparatus including the same
JP4640064B2 (en) Image forming apparatus
US10031457B2 (en) Optical sensor, recording medium discrimination device, and image forming apparatus
JP2008096617A (en) Image forming apparatus
US20190235435A1 (en) Sheet distinguishing device and image forming device
JP2011034173A (en) Method and apparatus for determining authenticity of paper sheet using terahertz light
JP2007206167A (en) Image forming apparatus and control method therefor
JP2007057892A (en) Image forming apparatus
JP4362745B2 (en) Paper identification sensor
JP2007108569A (en) Image forming apparatus
JPH10281991A (en) Gloss sensor
US12032315B2 (en) Paper discriminating device, image forming apparatus, paper type discriminating method, and recording medium
US20230185223A1 (en) Paper discriminating device, image forming apparatus, paper type discriminating method, and recording medium
JP2001301273A (en) Printer

Legal Events

Date Code Title Description
A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20210324

A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20211228

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20220201

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20220323

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20220621

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20220810

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20221004

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20221020

R150 Certificate of patent or registration of utility model

Ref document number: 7164329

Country of ref document: JP

Free format text: JAPANESE INTERMEDIATE CODE: R150