JP6027375B2 - Method for determining the degree of contamination of the surface to be cleaned and cleaning method - Google Patents
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本発明は、床面や壁面等の被清掃面を清掃するために、被清掃面上に光を照射して、被清掃面上の塵埃粒子を確認し、前記被清掃面を清掃する被清掃面の塵埃可視化方法及び清掃方法に関する。ここで、塵埃粒子とはハウスダスト、毛髪、繊維屑、その他室内で浮遊落下した被清掃面上に存在する種々の埃、塵、その他の粒子を総称する。 In order to clean a surface to be cleaned such as a floor surface or a wall surface, the present invention irradiates light on the surface to be cleaned, confirms dust particles on the surface to be cleaned, and cleans the surface to be cleaned The present invention relates to a surface dust visualization method and a cleaning method. Here, the dust particles are a general term for house dust, hair, fiber scraps, and other various dust, dust, and other particles present on the surface to be cleaned that has been suspended and dropped in the room.
従来から、家庭や職場の清掃用具として清掃用払拭体(清掃用モップとも云う)や、電気掃除機が広く利用されている。清掃作業者が清掃を行う時期に関しては、被清掃面の汚れ度合いとは無関係に定期的に行う場合と、被清掃面が汚れていることを確認してから清掃を行う場合の二通りが通例である。後者において、被清掃面の汚れ度合いの確認は、清掃作業者が肉眼で判断するのが通例である。ところが、近年における電子技術の発達によって、被清掃面に光を照射して被清掃面上の塵埃粒子からの散乱光により、塵埃粒子を可視化して確認する塵埃可視化技術が提案されている。 Conventionally, a cleaning wiping body (also called a cleaning mop) and a vacuum cleaner have been widely used as household and workplace cleaning tools. There are two general timings when the cleaning worker performs cleaning, regardless of the degree of contamination of the surface to be cleaned, and when cleaning is performed after confirming that the surface to be cleaned is dirty. It is. In the latter case, it is customary for the cleaning operator to determine the degree of contamination of the surface to be cleaned with the naked eye. However, in recent years, with the development of electronic technology, there has been proposed a dust visualization technology for visualizing and confirming dust particles by irradiating the surface to be cleaned with light and scattering light from the dust particles on the surface to be cleaned.
特開2007−282912号公報(特許文献1)の発明は、長い柄の先端にブラシ付きヘッドが設けられた清掃用具に関しており、ヘッドの背面にCCDカメラが設けられ、このCCDカメラの映像が、下方に配置された液晶ディスプレイに表示されるように構成されている。この清掃用具の使用方法は、手の届かない高所の清掃面をLED等のランプで光照射し、清掃面を前記CCDカメラで撮影しながら液晶ディスプレイで清掃面の汚れ具合を判別し、汚れている場合に、前記ヘッドの前面にあるブラシで清掃面を擦過して、汚れを除去し清掃面を清浄化するものである。 The invention of Japanese Patent Application Laid-Open No. 2007-282912 (Patent Document 1) relates to a cleaning tool in which a head with a brush is provided at the end of a long handle, and a CCD camera is provided on the back of the head. It is configured to be displayed on a liquid crystal display disposed below. The cleaning tool is used by irradiating a high-level cleaning surface that is out of reach with a lamp such as an LED, and using a liquid crystal display to determine how dirty the cleaning surface is while photographing the cleaning surface with the CCD camera. In this case, the cleaning surface is rubbed with a brush in front of the head to remove dirt and clean the cleaning surface.
特開2008−212195号公報(特許文献2)の発明は、電機掃除機の吸口体の中央及び左右位置の合計3箇所にLEDを取着して構成されている。前記吸口体は清掃時に畳又はフローリングの表面に当接する部材であるから、前記LEDの取着位置は、畳又はフローリング表面から数cm離れているに過ぎない。特に、ベッドや机の下側を清掃するときに、それらの位置は暗いから、前記LEDにより光照射して塵埃を確認しながら清掃可能であることがセールスポイントになっている。 The invention of Japanese Patent Application Laid-Open No. 2008-212195 (Patent Document 2) is configured by attaching LEDs at a total of three locations in the center and the left and right positions of the suction body of the electric vacuum cleaner. Since the mouthpiece is a member that comes into contact with the surface of the tatami or flooring during cleaning, the mounting position of the LED is only a few cm away from the surface of the tatami or flooring. In particular, when cleaning the underside of a bed or desk, their position is dark, so it is a selling point that the LED can be cleaned while irradiating light and checking dust.
特開2010−240271号公報(特許文献3)の発明は、床に当接する吸口体を長手の取付パイプに連結し、取付パイプの先端に突起を設けてその突起部分にLEDと小型カメラを装着して構成される電気掃除機である。前記LEDと小型カメラは床面を撮影するように配置されており、床面から十数cm上方に位置するように配置されている。小型カメラの映像は、電気掃除機本体に装着されたモニターで確認できるように構成されている。従って、清掃時に床面をLEDにより光照射して、目視することが困難な小さなゴミを前記照明により照らすことで、使用者に床面上の塵埃粒子をモニターで確認しながら清掃できることをセールスポイントとしている。 In the invention of Japanese Patent Application Laid-Open No. 2010-240271 (Patent Document 3), a suction body that is in contact with the floor is connected to a long mounting pipe, a protrusion is provided at the tip of the mounting pipe, and an LED and a small camera are mounted on the protruding portion. It is the vacuum cleaner comprised. The LED and the small camera are arranged so as to take a picture of the floor surface, and are arranged so as to be located more than a dozen cm above the floor surface. The image of the small camera can be confirmed on the monitor attached to the main body of the vacuum cleaner. Therefore, it is a selling point that the floor surface is irradiated with light at the time of cleaning, and small dust that is difficult to see is illuminated with the above-mentioned illumination, so that the user can clean while checking the dust particles on the floor surface with a monitor. It is said.
特許文献1の清掃用具は、高所の被清掃面の汚れ具合を光照射して液晶ディスプレイで汚れを確認しながら清掃すると記載されているが、清掃面の汚れを光照射で確認するということは、光照射による塵埃粒子の散乱光をCCDカメラで撮影することを意味する。ところが、前記散乱光は極めて微弱な散乱光であり、その散乱光の強度を高める為には、光の照射角度やLEDと被清掃面との離間距離の調整が極めて敏感に影響し、その調整は長い柄を上下したり軸回転したりするだけでは困難を極める弱点がある。また、柄の先端のヘッドの前面がブラシであり、背面がLED及びCCDカメラであるから、ブラシ清掃するときに舞い上がった塵埃粒子がLEDやCCDカメラの表面に付着して撮影機能の劣化を招く欠点がある。根本的には、清掃時にはLEDやCCDカメラがヘッドから分離されることが好ましいから、ヘッドの前面と背面にブラシとLED・CCDカメラを配置する構成に問題がある。 Although the cleaning tool of patent document 1 is described as cleaning while confirming dirt on a liquid crystal display by irradiating dirt on the surface to be cleaned at high places, it means that the dirt on the cleaning surface is confirmed by light irradiation. Means photographing the scattered light of dust particles by light irradiation with a CCD camera. However, the scattered light is very weak scattered light, and in order to increase the intensity of the scattered light, the adjustment of the irradiation angle of the light and the separation distance between the LED and the surface to be cleaned influences very sensitively and the adjustment. Has a weak point that is extremely difficult just by moving a long handle up and down and rotating the shaft. In addition, since the front of the head at the tip of the handle is a brush, and the back is an LED and a CCD camera, dust particles that have risen when cleaning the brush adhere to the surface of the LED or the CCD camera and cause a deterioration of the photographing function. There are drawbacks. Fundamentally, it is preferable that the LED and the CCD camera are separated from the head at the time of cleaning. Therefore, there is a problem in the configuration in which the brush and the LED / CCD camera are arranged on the front and back of the head.
特許文献2の電気掃除機は、吸口体の中央及び左右にLEDを固定的に配置しているから、被清掃面の塵埃粒子が確認できた場合に、吸口体で塵埃粒子を吸引清掃する際にもLEDが吸口体に存在し、LEDが粉塵により汚染される可能性が多分にある。被清掃面が床面であるときには、通常室内を点灯しながら清掃するのが通常であり、LEDの投光による塵埃粒子の微弱散乱光は前記点灯による照明光の中に埋没してしまい、床面から約1.5m上方に位置する電気掃除機を操作する作業者の肉眼には前記微弱散乱光はほとんど到達しないと考えられる。このような広い床面の清掃にはLEDの投光自体が不要であると思量する。この電気掃除機で、例えばベッド下の床面や机と箪笥の間の狭い床面を掃除する場合には、LEDで床面を光照射しながら清掃するが、そのような床面を作業者が覗き込みながら清掃するということはほとんどない。結論から言えば、LEDを掃除機の吸口体に固定配置することに弱点がある。また、床面の塵埃粒子を確認する場合には、光照射角度やLEDの取付高さが極めて敏感に影響し、特許文献2のようなLEDの吸口体への固定配置は角度調整や高さ調整が不可能であるから、塵埃粒子の確認作業自体も十分には機能しない欠点がある。 Since the vacuum cleaner of patent document 2 has arrange | positioning LED fixedly in the center of a mouthpiece, and right and left, when dust particles of a to-be-cleaned surface can be confirmed, when sucking and cleaning dust particles with a mouthpiece In addition, there is a possibility that the LED exists in the mouthpiece and the LED is contaminated with dust. When the surface to be cleaned is a floor surface, it is normal to clean the room while lighting it, and the weakly scattered light of the dust particles from the LED projection is buried in the lighting light from the lighting, and the floor It is considered that the weak scattered light hardly reaches the naked eye of the operator who operates the vacuum cleaner located about 1.5 m above the surface. It is assumed that LED flooding itself is unnecessary for cleaning such a large floor. For example, when cleaning a floor under a bed or a narrow floor between a desk and a bowl with this electric vacuum cleaner, the floor is light-irradiated with an LED. There is almost no cleaning while looking into. If it says from a conclusion, there exists a weak point in fixedly arrange | positioning LED in the suction body of a cleaner. In addition, when confirming dust particles on the floor surface, the light irradiation angle and the LED mounting height are very sensitively affected, and the fixing arrangement of the LED on the mouthpiece as in Patent Document 2 is angle adjustment and height. Since adjustment is impossible, there is a drawback that the dust particle checking operation itself does not function sufficiently.
特許文献3の電気掃除機は、取付パイプの先端に突起を設けてその突起部分にLEDと小型カメラを装着して構成されているから、特許文献2の電気掃除機と同様に、床面の塵埃粒子を確認する場合には、光照射角度やLEDの取付高さが極めて敏感に影響するので、特許文献3のようなLEDの固定配置は角度調整や高さ調整が不可能であるから、塵埃粒子の確認作業自体も十分には機能しない欠点がある。特に、LEDの取付位置が床面から十数cm上方にあり、LEDの床面に対する照射角度は数十度に達し、床面上の塵埃粒子の散乱光を確認することはほとんど不可能である。しかも、作業者の肉眼は床面から約1.5mも上方に離れており、仮に散乱光が存在したとしても肉眼で確認することは物理的に困難である。また、小型カメラを固定的に配置しているから、被清掃面の塵埃粒子が確認できた場合に、吸口体で塵埃粒子を吸引清掃する際にも、粉塵が舞う等して小型カメラに付着し、小型カメラが粉塵により汚染される可能性が多分にある。さらに、使用者が電気掃除機を使用する際には、通常、勢い良く一気に被清掃面を清掃するのであり、モニターを確認しながら時間をかけて被清掃面を清掃するという工程は手間となり、非常に効率が悪い清掃方法になりかねない。 Since the vacuum cleaner of Patent Document 3 is configured by providing a protrusion at the tip of the mounting pipe and mounting an LED and a small camera on the protrusion, the surface of the floor surface is similar to the vacuum cleaner of Patent Document 2. When confirming dust particles, the light irradiation angle and LED mounting height are very sensitive, so the LED fixed arrangement as in Patent Document 3 cannot be adjusted in angle or height. There is a drawback that the dust particle checking operation itself does not function sufficiently. In particular, the mounting position of the LED is a few tens of centimeters above the floor surface, the irradiation angle of the LED to the floor surface reaches several tens of degrees, and it is almost impossible to confirm the scattered light of the dust particles on the floor surface. . Moreover, the operator's naked eye is about 1.5 m away from the floor surface, and even if scattered light exists, it is physically difficult to check with the naked eye. In addition, since the small camera is fixedly arranged, when dust particles on the surface to be cleaned can be confirmed, when dust particles are sucked and cleaned with the suction mouth, dust will fly and adhere to the small camera. However, the small camera is likely to be contaminated with dust. Furthermore, when a user uses a vacuum cleaner, usually the surface to be cleaned is vigorously cleaned at once, and the process of cleaning the surface to be cleaned over time while checking the monitor is troublesome, It can be a very inefficient cleaning method.
従って、本発明は、被清掃面の塵埃粒子の観察動作と清掃作業を分離して、LEDやディスプレイ等の付属機器が清掃時の塵埃によって汚染されることを防止できる被清掃面の汚れ具合判別方法及び清掃方法を提供することを目的とする。
また、本発明は、被清掃面上の塵埃粒子を観察する際には、被清掃面に対する光照射角度や光源からの投光距離と塵埃粒子からの明瞭反射光との関係を明らかにすることを目的とし、迅速かつ確実に被清掃面の汚れ具合を判別することができ、汚れていると判断した場合には、上記清掃用具により被清掃面の清掃動作に着手することが可能になる。更に、本発明は、近年急速に普及している前方指向性の強いLEDやレーザー光源などの指向性投光器を利用して、被清掃面上の塵埃粒子の微弱散乱光により前記照射角度や投光距離の関係性を明確にすることを目的とする。
Therefore, the present invention separates the observation operation of the dust particles on the surface to be cleaned from the cleaning operation, and can determine whether the surface of the surface to be cleaned can be prevented from being contaminated by dust during cleaning. It is an object to provide a method and a cleaning method.
In addition, when observing dust particles on the surface to be cleaned, the present invention clarifies the relationship between the light irradiation angle with respect to the surface to be cleaned, the projection distance from the light source, and the clear reflected light from the dust particles. Therefore, it is possible to quickly and surely determine the degree of contamination of the surface to be cleaned. When it is determined that the surface is dirty, the cleaning tool can start the cleaning operation of the surface to be cleaned. Furthermore, the present invention uses a directional projector such as an LED or a laser light source having a strong forward directivity that has been rapidly spreading in recent years, and the irradiation angle and light projection are caused by weakly scattered light of dust particles on the surface to be cleaned. The purpose is to clarify the relationship of distance.
本発明は上記課題を解決するためになされたものであり、本発明の第1の形態は、投光レンズから指向性の光線を放出する指向性投光器により被清掃面に投光し、被清掃面上の塵埃粒子からの散乱光により塵埃粒子を観察して被清掃面の汚れ具合を判別する汚れ具合判別方法であり、まず、特定被清掃面上で指向性投光器の光軸高さHと、投光レンズから塵埃可視化良好領域の開始端である境界Sまでの境界投光距離Lsとの一次関数を近似的に導出する第一段階と、次に観察しようとする被清掃面上で、前記一次関数を利用して塵埃可視化良好領域の出現領域を効率的に推定して前記被清掃面の汚れ具合を判別する第二段階を組み合わせた2段階判別方法が提案される。
第一段階では、図2に示すように、前記被清掃面が関数導出用の特定被清掃面であるときに、前記特定被清掃面から前記指向性投光器の光軸までの光軸高さがHとなるように前記特定被清掃面に平行に前記指向性投光器を配置し、前記投光レンズの近傍において塵埃粒子が明瞭に観察されない領域を塵埃可視化不十分領域とし、この塵埃可視化不十分領域の遠方に境界Sを介して連接する塵埃粒子が明瞭に観察される領域を塵埃可視化良好領域としたとき、投光レンズから前記境界Sまでの距離を境界投光距離Lsとし、前記光軸高さHを大きくすると前記境界投光距離Lsも増大する関係を近似的にH=aLs+b(a,b:定数、a>0)の1次関数を導出する。
第二段階では、図12に示すように、塵埃粒子による汚れ具合を判別しようとする被清掃面に対し、光軸高さがHになるように前記指向性投光器を前記被清掃面に水平に配置して、この光軸高さHに対応する境界投光距離Lsを前記1次関数H=aLs+bから導出し、前記被清掃面上でその投光レンズからの投光距離をLとすると、導出された前記境界投光距離Lsに対し、L≧Lsの関係を満足する投光距離Lの領域が塵埃可視化良好領域と推定され、この推定された塵埃可視化良好領域内で塵埃粒子を観察して、前記被清掃面の汚れ具合を判別する。
以上のように、この第1形態では上記第一段階と上記第二段階を組み合わせた被清掃面の汚れ具合判別方法が提案される。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-described problems. In the first embodiment of the present invention, a surface to be cleaned is projected onto a surface to be cleaned by a directional projector that emits a directional light beam from a light projecting lens. This is a method for determining the degree of dirt on a surface to be cleaned by observing the dust particles from the scattered light from the dust particles on the surface. First, the optical axis height H of the directional projector on the specific surface to be cleaned The first step of approximately deriving a linear function of the boundary projection distance Ls from the projection lens to the boundary S that is the starting end of the dust visualization good region, and on the surface to be cleaned next, A two-stage discrimination method is proposed that combines the second stage of efficiently estimating the appearance region of the dust visualization good region using the linear function and discriminating the degree of dirt on the surface to be cleaned.
In the first stage, as shown in FIG. 2, when the surface to be cleaned is a specific surface to be cleaned for function derivation, the optical axis height from the specific surface to be cleaned to the optical axis of the directional projector is The directional projector is arranged in parallel with the specific surface to be cleaned so as to be H, and an area in which dust particles are not clearly observed in the vicinity of the projection lens is defined as an insufficiently visible area of the dust. When a region in which dust particles connected to the far side through the boundary S are clearly observed is a dust visualization good region, a distance from the light projecting lens to the boundary S is defined as a boundary light projection distance Ls, and the optical axis height When the height H is increased, a linear function of H = aLs + b (a, b: constant, a> 0) is approximately derived so that the boundary projection distance Ls also increases.
In the second stage, as shown in FIG. 12, the directional projector is placed horizontally on the surface to be cleaned so that the optical axis height is H with respect to the surface to be cleaned to determine the degree of contamination by dust particles. The boundary projection distance Ls corresponding to the optical axis height H is derived from the linear function H = aLs + b, and the projection distance from the projection lens on the surface to be cleaned is L. A region with a projection distance L that satisfies the relationship of L ≧ Ls with respect to the derived boundary projection distance Ls is estimated as a dust visualization good region, and dust particles are observed within the estimated dust visualization good region. Then, the degree of dirt on the surface to be cleaned is determined.
As described above, this first embodiment proposes a method for determining the degree of contamination of the surface to be cleaned by combining the first stage and the second stage.
本発明の第2の形態は、投光レンズから指向性の光線を放出する指向性投光器により被清掃面に投光し、被清掃面上の塵埃粒子からの散乱光により塵埃粒子を観察して被清掃面の汚れ具合を判別する汚れ具合判別方法であり、まず、特定被清掃面上で指向性投光器の前傾角θと、投光レンズから塵埃可視化良好領域の開始端である左側境界Tまでの左側境界投光距離Ltとの一次関数を近似的に導出する第一段階と、次に観察しようとする被清掃面上で、前記一次関数を利用して塵埃可視化良好領域の出現領域を効率的に推定して前記被清掃面の汚れ具合を判別する第二段階を組み合わせた二段階判別方法が提案される。
第一段階では、図7に示すように、前記被清掃面が関数導出用の特定被清掃面であるときに、前記指向性投光器の前縁を前記特定被清掃面に当接させた状態で前記指向性投光器の後縁を前記特定被清掃面から上昇させて前記指向性投光器の光軸を前記特定被清掃面に対し前傾角θで前傾させたとき、前記投光レンズの近傍において塵埃粒子が明瞭に観察されない領域を塵埃可視化不十分領域とし、この塵埃可視化不十分領域の遠方に左側境界Tを介して連接する塵埃粒子が明瞭に観察される領域を塵埃可視化良好領域としたとき、投光レンズから前記左側境界Tまでの距離を左側境界投光距離Ltとし、前記前傾角θを大きくすると前記左側境界投光距離Ltが減少する関係を近似的にθ=cLt+d(c,d:定数、c<0)の1次関数で導出する。
第二段階では、図13に示すように、塵埃粒子による汚れ具合を判別しようとする被清掃面に対し、前記指向性投光器の前縁を前記被清掃面に当接させた状態で前記指向性投光器の後縁を前記被清掃面から上昇させて前記指向性投光器の光軸を前記被清掃面に対し前傾角θで前傾させて、この前傾角θに対応する左側境界投光距離Ltを前記1次関数θ=cLt+dから導出し、前記被清掃面上でその投光レンズからの投光距離をLとすると、導出された前記左側境界投光距離Ltに対し、L≧Ltの関係を満足する投光距離Lの領域が塵埃可視化良好領域と推定され、この推定された塵埃可視化良好領域内で塵埃粒子を観察して、前記被清掃面の汚れ具合を判別する。
以上のように、この第2形態では上記第一段階と上記第二段階を組み合わせた被清掃面の汚れ具合判別方法が提案される。
In the second aspect of the present invention, the surface to be cleaned is projected by a directional projector that emits a directional light beam from the light projecting lens, and the dust particles are observed by scattered light from the dust particles on the surface to be cleaned. This is a method for determining the degree of contamination on the surface to be cleaned. First, the forward tilt angle θ of the directional projector on the specific surface to be cleaned and the left boundary T, which is the starting end of the dust visualization good region, from the projection lens The first step of approximately deriving a linear function with the left boundary projection distance Lt of the object, and the appearance area of the good dust visualization area using the linear function on the surface to be cleaned next is efficiently A two-stage discrimination method is proposed that combines a second stage for estimating the degree of contamination of the surface to be cleaned by estimating the condition.
In the first stage, as shown in FIG. 7, when the surface to be cleaned is a specific surface to be cleaned for function derivation, the front edge of the directional projector is in contact with the specific surface to be cleaned. When the rear edge of the directional projector is raised from the specific surface to be cleaned and the optical axis of the directional projector is tilted forward with respect to the specific surface to be cleaned at a forward tilt angle θ, dust is generated in the vicinity of the light projecting lens. When an area where particles are not clearly observed is an area where dust is insufficiently visualized, and an area where dust particles connected to the far side of the area where the dust is insufficiently visualized via the left boundary T is clearly defined as an area where dust is visualized satisfactorily, The distance from the projection lens to the left boundary T is the left boundary projection distance Lt, and when the forward tilt angle θ is increased, the relationship in which the left boundary projection distance Lt decreases is approximately θ = cLt + d (c, d: Derived by a linear function of constant, c <0) To do.
In the second stage, as shown in FIG. 13, the directivity is set in a state where the front edge of the directivity projector is in contact with the surface to be cleaned with respect to the surface to be cleaned to determine the degree of contamination by dust particles. The rear edge of the projector is raised from the surface to be cleaned, the optical axis of the directional projector is tilted forward with respect to the surface to be cleaned at a forward tilt angle θ, and the left boundary light projection distance Lt corresponding to the forward tilt angle θ is set. Derived from the linear function θ = cLt + d, and assuming that the projection distance from the projection lens on the surface to be cleaned is L, the relationship of L ≧ Lt is established with respect to the derived left boundary projection distance Lt. A region with a satisfactory projection distance L is estimated to be a dust visualization good region, and dust particles are observed in the estimated dust visualization good region to determine the degree of contamination of the surface to be cleaned.
As described above, this second embodiment proposes a method for determining the degree of contamination of the surface to be cleaned by combining the first stage and the second stage.
本発明の第3の形態は、指向性投光器を前傾させた時に、塵埃可視化良好領域の終了端(右側境界U)に関する発明であり、塵埃可視化良好領域の開始端(左側境界T)に関する前記第2形態の補完をなすものである。この第3形態では、まず、特定被清掃面上で指向性投光器の前傾角θと、投光レンズから塵埃可視化良好領域の終了端である右側境界Uまでの右側境界投光距離Luとの一次関数を近似的に導出する第一段階と、次に観察しようとする被清掃面上で、前記一次関数を利用して塵埃可視化良好領域の出現領域を効率的に推定して前記被清掃面の汚れ具合を判別する第二段階を組み合わせた二段階判別方法が提案される。
第一段階では、前記特定被清掃面上で前記塵埃可視化良好領域の右側境界Uに連続してその遠方に塵埃可視化不十分領域が出現し、投光レンズから前記右側境界Uまでの距離を右側境界投光距離Luとし、前記前傾角θを大きくすると前記右側境界投光距離Luが減少する関係を近似的にθ=eLu+f(e,f:定数、e<0)の1次関数で導出する。
第二段階では、図13に示すように、塵埃粒子による汚れ具合を判別しようとする被清掃面に対し、前記指向性投光器の前縁を前記被清掃面に当接させた状態で前記指向性投光器の後縁を前記被清掃面から上昇させて前記指向性投光器の光軸を前記被清掃面に対し前傾角θで前傾させて、この前傾角θに対応する右側境界投光距離Luを前記1次関数θ=eLu+fから導出し、前記被清掃面上でその投光レンズからの投光距離をLとすると、導出された前記左側境界投光距離Lt及び前記右側境界投光距離Luに対し、Lt≦L≦Luの関係を満足する投光距離Lの領域が塵埃可視化良好領域と推定され、この推定された塵埃可視化良好領域内で塵埃粒子を観察して、前記被清掃面の汚れ具合を判別する。Lt≦Lの不等式は第2形態によって得られたものであり、L≦Luの不等式は第3形態によって得られたものであり、この二つの不等式を組み合わせることによって本第3形態は構成される。
以上のように、この第3形態では上記第一段階と上記第二段階を組み合わせた被清掃面の汚れ具合判別方法が提案される。
The third aspect of the present invention is an invention related to the end of the dust visualization good region (right boundary U) when the directional projector is tilted forward, and the above-mentioned related to the start end (left boundary T) of the dust visualization good region. It complements the second form. In the third embodiment, first, the primary tilt angle θ of the directional projector on the specific surface to be cleaned and the right boundary light projection distance Lu from the light projection lens to the right boundary U that is the end of the dust visualization good region. A first step of approximately deriving a function, and a surface to be cleaned next to be observed, the first-order function is used to efficiently estimate an appearance region of a good dust visualization region and A two-stage discrimination method combining a second stage for judging the degree of contamination is proposed.
In the first stage, an area where the dust visualization is insufficient appears continuously on the specific surface to be cleaned on the right boundary U of the dust visualization good area, and the distance from the light projecting lens to the right boundary U is set to the right side. When the boundary projection distance Lu is set to be larger and the forward tilt angle θ is increased, the right boundary projection distance Lu is reduced by a linear function of θ = eLu + f (e, f: constant, e <0). To derive.
In the second stage, as shown in FIG. 13, the directivity is set in a state where the front edge of the directivity projector is in contact with the surface to be cleaned with respect to the surface to be cleaned to determine the degree of contamination by dust particles. The rear edge of the projector is raised from the surface to be cleaned, and the optical axis of the directional projector is tilted forward with respect to the surface to be cleaned at a forward tilt angle θ, and the right boundary light projection distance Lu corresponding to the forward tilt angle θ is set. Derived from the linear function θ = eLu + f, and assuming that the projection distance from the projection lens on the surface to be cleaned is L, the left boundary projection distance Lt and the right boundary projection distance Lu are derived. On the other hand, the region of the projection distance L that satisfies the relationship of Lt ≦ L ≦ Lu is estimated to be a dust visualization good region, and dust particles are observed in the estimated dust visualization good region, and the surface to be cleaned is contaminated. Determine the condition. The inequality of Lt ≦ L is obtained by the second form, the inequality of L ≦ Lu is obtained by the third form, and the third form is constructed by combining these two inequalities. .
As described above, the third embodiment proposes a method for determining the degree of contamination of the surface to be cleaned by combining the first stage and the second stage.
本発明の第4の形態は、被清掃面に対し指向性投光器を光軸高さHに平行配置したときの第1形態と、前傾角θで前傾させたときの左側境界Tに関連した第2形態を組み合わせた発明に関係している。この第4形態では、まず、特定被清掃面に平行に指向性投光器を光軸高さHの位置に配置して、光軸高さHと境界投光距離Lsとの一次関数を近似的に導出する第一段階と、指向性投光器の前縁を特定被清掃面に接触させた状態で指向性投光器を前傾角θで前傾させ前傾角θと左側境界投光距離Ltとの一次関数を近似的に導出する第二段階と、次に観察しようとする被清掃面上で、二つの前記一次関数を利用して塵埃可視化良好領域の出現領域を効率的に推定して前記被清掃面の汚れ具合を判別する第三段階を組み合わせた三段階判別方法が提案される。この三段階判別方法を詳しく述べる。
第一段階では、図12に示すように、前記被清掃面が関数導出用の特定被清掃面であるときに、前記特定被清掃面から前記指向性投光器の光軸までの光軸高さがHとなるように前記特定被清掃面に平行に前記指向性投光器を配置し、前記投光レンズの近傍において塵埃粒子が明瞭に観察されない領域を塵埃可視化不十分領域とし、この塵埃可視化不十分領域の遠方に境界Sを介して連接する塵埃粒子が明瞭に観察される領域を塵埃可視化良好領域としたとき、投光レンズから前記境界Sまでの距離を境界投光距離Lsとし、前記光軸高さHを大きくすると前記境界投光距離Lsも増大する関係を近似的にH=aLs+b(a,b:定数、a>0)の1次関数で導出する。
第二段階では、図13に示すように、前記指向性投光器の前縁を前記特定被清掃面に当接させた状態で前記指向性投光器の後縁を前記特定被清掃面から上昇させて前記指向性投光器の光軸を前記特定被清掃面に対し前傾角θで前傾させたとき、前記投光レンズの近傍において塵埃粒子が明瞭に観察されない領域を塵埃可視化不十分領域とし、この塵埃可視化不十分領域の遠方に左側境界Tを介して連接する塵埃粒子が明瞭に観察される領域を塵埃可視化良好領域としたとき、投光レンズから前記左側境界Tまでの距離を左側境界投光距離Ltとし、前記前傾角θを大きくすると前記左側境界投光距離Ltが減少する関係を近似的にθ=cLt+d(c,d:定数、c<0)の1次関数で導出する。
第三段階では、図14に示すように、塵埃粒子による汚れ具合を判別しようとする被清掃面に対し、前記指向性投光器を前記被清掃面から光軸高さHの距離だけ上方に前記被清掃面に対し平行線となるように配置し、且つ前記指向性投光器の前縁を前記平行線から移動させずに前記指向性投光器の後縁を上昇移動させて前記指向性投光器の光軸を前記平行線に対し前傾角θで前傾させたとき、前記投光レンズの近傍において生じる塵埃可視化不十分領域に連続する塵埃可視化良好領域の開始端は、前記投光レンズから前記開始端までの開始端投光距離をLcとすると、Lc=Lt+Ls+d/cで与えられ、前記被清掃面上でその投光レンズからの投光距離をLとすると、L≧Lcの関係を満足する投光距離Lの領域が塵埃可視化良好領域と推定され、この推定された塵埃可視化良好領域内で塵埃粒子を観察して、前記被清掃面の汚れ具合を判別する。
以上のように、この第4形態では上記第一段階と上記第二段階と上記第三段階を組み合わせた被清掃面の汚れ具合判別方法が提案される。
The fourth embodiment of the present invention relates to the first embodiment when the directional projector is disposed in parallel to the optical axis height H with respect to the surface to be cleaned, and the left boundary T when tilted forward at the forward tilt angle θ. It relates to the invention combining the second form. In the fourth embodiment, first, a directional projector is arranged at the position of the optical axis height H in parallel to the specific surface to be cleaned, and a linear function of the optical axis height H and the boundary projection distance Ls is approximated. A linear function of the first stage of derivation and the forward tilt angle θ and the left boundary projection distance Lt by tilting the directional projector forward by the forward tilt angle θ with the front edge of the directional projector in contact with the specific surface to be cleaned. On the surface to be cleaned that is to be approximated and the surface to be cleaned next, the appearance area of the dust visualization good region is efficiently estimated by using the two linear functions, and the surface to be cleaned is A three-stage discrimination method combining a third stage for judging the degree of contamination is proposed. This three-stage discrimination method will be described in detail.
In the first stage, as shown in FIG. 12, when the surface to be cleaned is a specific surface to be cleaned for function derivation, the optical axis height from the specific surface to be cleaned to the optical axis of the directional projector is The directional projector is arranged in parallel with the specific surface to be cleaned so as to be H, and an area in which dust particles are not clearly observed in the vicinity of the projection lens is defined as an insufficiently visible area of the dust. When a region in which dust particles connected to the far side through the boundary S are clearly observed is a dust visualization good region, a distance from the light projecting lens to the boundary S is defined as a boundary light projection distance Ls, and the optical axis height The relation that the boundary projection distance Ls increases as the height H is increased is approximately derived by a linear function of H = aLs + b (a, b: constant, a> 0).
In the second stage, as shown in FIG. 13, the rear edge of the directional projector is raised from the specific cleaned surface in a state where the front edge of the directional projector is in contact with the specific cleaned surface. When the optical axis of the directional projector is tilted forward with respect to the specific surface to be cleaned at a forward tilt angle θ, an area where dust particles are not clearly observed in the vicinity of the light projecting lens is defined as an insufficiently visible area. When a region in which dust particles connected to the far side of the insufficient region via the left boundary T are clearly observed is a dust visualization good region, the distance from the light projecting lens to the left boundary T is the left boundary projection distance Lt. And the relationship that the left boundary projection distance Lt decreases as the forward tilt angle θ is increased is approximately derived by a linear function of θ = cLt + d (c, d: constant, c <0).
In the third stage, as shown in FIG. 14, the directional projector is positioned above the surface to be cleaned by a distance of the optical axis height H with respect to the surface to be cleaned to determine the degree of contamination by dust particles. It arranges so that it may become a parallel line with respect to a cleaning surface, and without moving the front edge of the directional floodlight from the parallel line, the rear edge of the directional floodlight is moved up, and the optical axis of the directional floodlight is changed. When tilted forward at a forward tilt angle θ with respect to the parallel line, the start end of the dust visualization good region that is continuous with the dust visualization insufficient region that occurs in the vicinity of the projection lens is from the projection lens to the start end. Lc = Lt + Ls + d / c, where Lc = Lt + Ls + d / c, and L = Lc, which satisfies the relationship of L ≧ Lc, where L is the projection distance from the projection lens on the surface to be cleaned. The area of L is the area where dust visualization is good It is a constant, and observed the dust particles in the estimated dust visualized well region, to determine the contamination degree of the surface to be cleaned.
As described above, in the fourth embodiment, a method for determining the degree of contamination on the surface to be cleaned, which combines the first stage, the second stage, and the third stage, is proposed.
本発明の第5の形態は、第4形態の指向性投光器を前傾させた時に、塵埃可視化良好領域の終了端(右側境界U)に関する発明であり、塵埃可視化良好領域の開始端(左側境界T)に関する前記第4形態の補完をなすものである。この第5形態では、まず、特定被清掃面上で指向性投光器の前傾角θと、投光レンズから塵埃可視化良好領域の終了端である右側境界Uまでの右側境界投光距離Luとの一次関数を近似的に導出する第一段階と、次に観察しようとする被清掃面上で、前記一次関数を利用して塵埃可視化良好領域の出現領域を効率的に推定して前記被清掃面の汚れ具合を判別する第二段階を組み合わせた二段階判別方法が提案される。
第一段階では、図13に示すように、前記指向性投光器の前縁を前記特定被清掃面に当接させた状態で前記指向性投光器の後縁を前記特定被清掃面から上昇させて前記指向性投光器の光軸を前記特定被清掃面に対し前傾角θで前傾させたとき、前記特定被清掃面上で前記塵埃可視化良好領域の右側境界Uに連続してその遠方に塵埃可視化不十分領域が出現し、投光レンズから前記右側境界Uまでの距離を右側境界投光距離Luとし、前記前傾角θを大きくすると前記右側境界投光距離Luが減少する関係を近似的にθ=eLu+f(e,f:定数、e<0)の1次関数で導出する。
第二段階では、図14に示すように、塵埃粒子による汚れ具合を判別しようとする被清掃面に対し、前記指向性投光器を前記被清掃面から光軸高さHの距離だけ上方に前記被清掃面に対し平行線となるように配置し、且つ前記指向性投光器の前縁を前記平行線から移動させずに前記指向性投光器の後縁を上昇移動させて前記指向性投光器の光軸を前記平行線に対し前傾角θで前傾させたとき、前記投光レンズの近傍において生じる塵埃可視化不十分領域に連続する塵埃可視化良好領域の終了端は、前記投光レンズから前記終了端までの終了端投光距離をLeとすると、Le=Lu+Ls+d/cで与えられ、前記被清掃面上でその投光レンズからの投光距離をLとすると、導出された前記開始端投光距離Lc及び前記終了端投光距離Leに対し、Lc≦L≦Leの関係を満足する投光距離Lの領域が塵埃可視化良好領域と推定され、この推定された塵埃可視化良好領域内で塵埃粒子を観察して、前記被清掃面の汚れ具合を判別する。Lc≦Lの不等式は第4形態によって得られたものであり、L≦Leの不等式は第5形態によって得られたものであり、この二つの不等式を組み合わせることによって本第5形態は構成される。
以上のように、この第5形態では上記第一段階と上記第二段階を組み合わせた被清掃面の汚れ具合判別方法が提案される。
The fifth aspect of the present invention is an invention relating to the end of the dust visualization good region (right boundary U) when the directional projector of the fourth form is tilted forward, and the start end (left boundary of the dust visualization good region) It complements the fourth embodiment relating to T). In this fifth embodiment, first, the primary tilt angle θ of the directional projector on the specific surface to be cleaned and the right boundary light projection distance Lu from the light projection lens to the right boundary U that is the end of the dust visualization good region. A first step of approximately deriving a function, and a surface to be cleaned next to be observed, the first-order function is used to efficiently estimate an appearance region of a good dust visualization region and A two-stage discrimination method combining a second stage for judging the degree of contamination is proposed.
In the first stage, as shown in FIG. 13, the rear edge of the directional projector is raised from the specific surface to be cleaned while the front edge of the directional projector is in contact with the specific surface to be cleaned. When the optical axis of the directional projector is tilted forward with respect to the specific surface to be cleaned at a forward tilt angle θ, the dust is not visible on the specific surface to be cleaned continuously to the right boundary U of the good dust visualization region. When a sufficient area appears and the distance from the light projecting lens to the right boundary U is the right boundary light projection distance Lu, and the forward tilt angle θ is increased, the right boundary light projection distance Lu decreases approximately by θ = Derived by a linear function of eLu + f (e, f: constant, e <0).
In the second stage, as shown in FIG. 14, the directional projector is placed above the surface to be cleaned by a distance of the optical axis height H with respect to the surface to be cleaned to determine the degree of contamination by dust particles. It arranges so that it may become a parallel line with respect to a cleaning surface, and without moving the front edge of the directional floodlight from the parallel line, the rear edge of the directional floodlight is moved up, and the optical axis of the directional floodlight is changed. When tilted forward with a forward tilt angle θ with respect to the parallel line, the end end of the dust visualization good region continuous with the dust visualization inadequate region generated in the vicinity of the projection lens is from the projection lens to the end end. When the end edge projection distance is Le, Le = Lu + Ls + d / c is given, and when the projection distance from the projection lens on the surface to be cleaned is L, the derived start end projection distance Lc and For the end-end projection distance Le , Lc ≦ L ≦ Le satisfying the relationship of the projection distance L is estimated as the dust visualization good region, the dust particles are observed in the estimated dust visualization good region, and the degree of contamination of the surface to be cleaned is estimated. Is determined. The inequality of Lc ≦ L is obtained by the fourth form, the inequality of L ≦ Le is obtained by the fifth form, and the fifth form is constituted by combining these two inequalities. .
As described above, this fifth embodiment proposes a method for determining the degree of contamination of the surface to be cleaned by combining the first stage and the second stage.
本発明の第6の形態は、前記指向性投光器の光度を強弱調整することによって、前記指向性投光器により光照射される被清掃面の照度を可変調整し、被清掃面上の前記塵埃粒子による微弱散乱光の観察を容易にする被清掃面の汚れ具合判別方法である。 The sixth aspect of the present invention variably adjusts the illuminance of the surface to be cleaned that is irradiated with light by the directional projector by adjusting the intensity of the directional projector, and is based on the dust particles on the surface to be cleaned. This is a method for determining the degree of contamination of a surface to be cleaned that facilitates observation of weak scattered light.
本発明の第7の形態は、前記指向性投光器がLED、レーザー光源又はランプを光源として用いた前方指向性を有した指向性投光器である被清掃面の汚れ具合判別方法である。 A seventh aspect of the present invention is a method for determining the degree of contamination of a surface to be cleaned, wherein the directional projector is a directional projector having forward directivity using an LED, a laser light source, or a lamp as a light source.
本発明の第8の形態は、上述した被清掃面の汚れ具合判別方法を用いて、被清掃面上の塵埃可視化良好領域内で塵埃粒子を観察し、この観察結果を判断して前記被清掃面を清掃する被清掃面の清掃方法である。 The eighth aspect of the present invention uses the above-described method for determining the degree of contamination of the surface to be cleaned, observes dust particles in the dust visualization good region on the surface to be cleaned, and judges the observation result to determine the object to be cleaned. It is the cleaning method of the surface to be cleaned for cleaning the surface.
本発明の第1の形態において、図2及び図12に示すように、光軸高さHと境界投光距離Lsとの一次関数H=aLs+bは簡単に測定することが可能である。まず、指向性投光器の投光レンズの中心とその底面との間隔が最小の光軸高さH0になる。その後、特定被清掃面上に指向性投光器を載置し、特定被清掃面の上方に指向性投光器を上昇配置させると、投光レンズと特定被清掃面との間隔が光軸高さHに相当する。従って、光軸高さHはH≧H0の範囲に設定できる。光軸高さH毎に境界投光距離Lsを測定していく。HとLsとの関係を一次関数で回帰することによって前記一次関数H=aLs+bを容易に導出することができる。この様にして、測定用の指向性投光器が決まれば、その指向性投光器に特有の一次関数H=aLs+bを事前に決定することができる。高軸高さHを大きくすると、塵埃可視化良好領域は投光レンズから遠ざかるから、境界投光距離Lsは大きくなることは明らかである。つまり、前記一次関数の傾きaはa>0であることは当然である。この一次関数が事前に分かっていると、清掃しようとする任意の被清掃面上に前記指向性投光器を載置しなくても、もし塵埃粒子が被清掃面上に存在する場合には、投光レンズの前方で境界投光距離Lsよりも遠方に塵埃粒子が明瞭に確認できることが予測できる。従って、実際に前記指向性投光器を被清掃面上に載置したときには、肉眼を境界投光距離Lsよりも遠方の位置に向けておくことによって、塵埃粒子の存否を迅速且つ容易に判断することが可能になる。もし、前記一次関数が不明の場合には、指向性投光器を被清掃面に載置しても塵埃粒子がどの位置に観察されるかは試行錯誤により判断するしかない。即ち、この一次関数により塵埃粒子の出現位置を予測できるだけでなく、実際の観察動作においても迅速且つ容易な塵埃粒子の存否確認が可能になる。
塵埃粒子の確認を電子装置で行う場合には、指向性投光器により被清掃面を光照射していても、電子装置は被清掃面の全体を一気に観察することが不可能であるから、前記被清掃面の投光レンズ位置から前方に向かって隈なく走査しながら塵埃粒子を確認する以外にない。つまり、塵埃可視化不十分領域をも走査しなければならないから、それだけ不要な時間を浪費することになる。本発明を利用すると、前記一次関数が既に分かっているから、塵埃可視化良好領域だけを走査すればよく、投光レンズから測って境界投光距離Lsより遠方の位置に塵埃粒子が容易に確認できるはずである。従って、前記電子装置による塵埃粒子の観察は、境界投光距離Lsの位置より遠方に設定すればよく、電子装置による塵埃粒子の観察時間を急激に短縮することが可能になる。
総括すると、前記一次関数により、作業者が塵埃粒子を観察する場合には塵埃粒子の出現位置を予測できる技術的効果があり、電子装置により塵埃粒子を観察する場合には、走査時間の短縮化という技術的効果がある。
In the first embodiment of the present invention, as shown in FIGS. 2 and 12, the linear function H = aLs + b between the optical axis height H and the boundary projection distance Ls can be easily measured. First, the distance between the center of the projection lens of the directional light projector and its bottom surface is minimized optical axis height H 0. After that, when the directional projector is placed on the specific surface to be cleaned, and the directional projector is raised above the specific surface to be cleaned, the distance between the light projecting lens and the specific surface to be cleaned becomes the optical axis height H. Equivalent to. Accordingly, the optical axis height H can be set in the range of H ≧ H 0. The boundary projection distance Ls is measured for each optical axis height H. The linear function H = aLs + b can be easily derived by regressing the relationship between H and Ls with a linear function. In this manner, when a directional projector for measurement is determined, a linear function H = aLs + b unique to the directional projector can be determined in advance. Obviously, when the high-axis height H is increased, the dust visualization good region is moved away from the projection lens, and therefore the boundary projection distance Ls is increased. In other words, the slope a of the linear function is naturally a> 0. If this linear function is known in advance, even if the directional projector is not placed on any surface to be cleaned, if dust particles are present on the surface to be cleaned, It can be predicted that dust particles can be clearly confirmed in front of the optical lens and far from the boundary projection distance Ls. Therefore, when the directional projector is actually placed on the surface to be cleaned, the presence or absence of dust particles can be quickly and easily determined by keeping the naked eye at a position farther than the boundary projection distance Ls. Is possible. If the linear function is unknown, the position where dust particles are observed can only be determined by trial and error even if the directional projector is placed on the surface to be cleaned. That is, not only can the appearance position of dust particles be predicted by this linear function, but also the presence / absence of dust particles can be confirmed quickly and easily in an actual observation operation.
When the dust particles are confirmed by the electronic device, the electronic device cannot observe the entire surface to be cleaned at a stretch even if the surface to be cleaned is irradiated with light by a directional projector. There is no other way but to confirm dust particles while scanning forward from the position of the projection lens on the cleaning surface. That is, since it is necessary to scan a region where dust is insufficiently visualized, unnecessary time is wasted. When the present invention is used, since the linear function is already known, it is only necessary to scan the dust visualization good region, and dust particles can be easily confirmed at a position farther than the boundary projection distance Ls as measured from the projection lens. It should be. Therefore, the observation of the dust particles by the electronic device may be set far from the position of the boundary projection distance Ls, and the observation time of the dust particles by the electronic device can be drastically shortened.
In summary, the linear function has a technical effect that allows the operator to predict the appearance position of dust particles when observing the dust particles, and shortens the scanning time when observing the dust particles with an electronic device. There is a technical effect.
本発明の第2の形態においても、図7及び図13に示すように、前傾角θと左側境界投光距離Ltとの一次関数θ=cLt+dは簡単に測定することが可能である。まず、指向性投光器を特定被清掃面に載置した場合には、指向性投光器の底面が光軸に平行であると仮定すると、前傾角θ=0になる。その後、指向性投光器の前縁を特定被清掃面上に当接させてその後縁を上昇させて指向性投光器を前傾角θで前傾させる。従って、前傾角θはθ≧0の範囲に設定できる。前傾角θ毎に左側境界投光距離Ltを測定していく。θとLtとの関係を一次関数で回帰することによって前記一次関数θ=cLt+dを容易に導出することができる。この様にして、測定用の指向性投光器が決まれば、その指向性投光器に特有の一次関数θ=cLt+dを事前に決定することができる。前傾角θを大きくすると、塵埃可視化良好領域は投光レンズ側に接近するから、左側境界投光距離Ltは小さくなることは明らかである。つまり、前記一次関数の傾きcはc<0であることは当然である。
この一次関数が事前に分かっていると、清掃しようとする任意の被清掃面上に前記指向性投光器を載置前傾しなくても、もし塵埃粒子が被清掃面上に存在する場合には、投光レンズの前方で左側境界投光距離Ltよりも遠方に塵埃粒子が明瞭に確認できることが予測できる。従って、実際に前記指向性投光器を被清掃面上に載置前傾させたときには、肉眼を左側境界投光距離Ltよりも遠方の位置に向けておくことによって、塵埃粒子の存否を迅速且つ容易に判断することが可能になる。もし、前記一次関数が不明の場合には、指向性投光器を被清掃面に載置前傾させても塵埃粒子がどの位置に観察されるかは試行錯誤により判断するしかない。つまり、この一次関数により塵埃粒子の出現位置を予測できるだけでなく、実際の観察動作においても迅速且つ容易な塵埃粒子の存否確認が可能になる。
また、塵埃粒子の確認を電子装置で行う場合には、指向性投光器により被清掃面を光照射していても、電子装置は被清掃面の全体観察を一気に為すことが不可能であるから、前記被清掃面の投光レンズ位置から遠方に向かって隈なく走査しながら塵埃粒子を確認せざるを得ない。つまり、塵埃可視化不十分領域をも走査しなければならないから、それだけ不要な時間を浪費することになる。本発明を利用すると、前記一次関数が既に分かっているから、塵埃可視化良好領域だけを集中的に走査すればよく、投光レンズから測って左側境界投光距離Ltより遠方の位置に塵埃粒子が容易に確認できるはずである。従って、前記電子装置による塵埃粒子の観察は、左側境界投光距離Ltの位置より遠方に設定すればよく、電子装置による塵埃粒子の観察時間を急激に短縮することが可能になる。
即ち、前記一次関数により、作業者が塵埃粒子を観察する場合には塵埃粒子の出現位置を予測できる技術的効果を有し、電子装置により塵埃粒子を観察する場合には、走査時間の短縮化という技術的効果を有することは言うまでも無い。
Also in the second embodiment of the present invention, as shown in FIGS. 7 and 13, the linear function θ = cLt + d of the forward tilt angle θ and the left boundary light projection distance Lt can be easily measured. First, when the directional projector is placed on the specific surface to be cleaned, assuming that the bottom surface of the directional projector is parallel to the optical axis, the forward tilt angle θ = 0. Thereafter, the front edge of the directional projector is brought into contact with the specific surface to be cleaned, the rear edge is raised, and the directional projector is tilted forward by the forward tilt angle θ. Therefore, the forward tilt angle θ can be set in a range of θ ≧ 0. The left boundary projection distance Lt is measured for each forward tilt angle θ. The linear function θ = cLt + d can be easily derived by regressing the relationship between θ and Lt with a linear function. In this way, when a directional projector for measurement is determined, a linear function θ = cLt + d unique to the directional projector can be determined in advance. When the forward tilt angle θ is increased, the dust visualization good region approaches the light projection lens side, so it is clear that the left boundary light projection distance Lt becomes small. In other words, the slope c of the linear function is naturally c <0.
If this linear function is known in advance, even if the directional projector is not tilted before placing on any surface to be cleaned, if dust particles are present on the surface to be cleaned It can be predicted that dust particles can be clearly confirmed in front of the projection lens and farther than the left boundary projection distance Lt. Therefore, when the directional projector is actually tilted before being placed on the surface to be cleaned, the presence or absence of dust particles can be determined quickly and easily by directing the naked eye toward a position farther than the left boundary projection distance Lt. It becomes possible to judge. If the linear function is unknown, the position where the dust particles are observed can only be determined by trial and error even if the directional projector is tilted before being placed on the surface to be cleaned. That is, not only can the appearance position of dust particles be predicted by this linear function, but also the presence / absence of dust particles can be confirmed quickly and easily in an actual observation operation.
In addition, when the dust particles are confirmed by the electronic device, even if the surface to be cleaned is irradiated with light by the directional projector, the electronic device cannot perform the entire observation of the surface to be cleaned at once. The dust particles must be confirmed while scanning from the projection lens position on the surface to be cleaned far away. That is, since it is necessary to scan a region where dust is insufficiently visualized, unnecessary time is wasted. When the present invention is used, since the linear function is already known, only the dust visualization good region needs to be intensively scanned, and dust particles are measured at a position farther from the left boundary projection distance Lt as measured from the projection lens. It should be easy to confirm. Therefore, the observation of the dust particles by the electronic device may be set farther than the position of the left boundary projection distance Lt, and the observation time of the dust particles by the electronic device can be shortened rapidly.
That is, the linear function has a technical effect that allows the operator to predict the appearance position of dust particles when observing the dust particles, and shortens the scanning time when observing the dust particles with an electronic device. Needless to say, it has a technical effect.
本発明の第3形態によれば、図7及び図13に示すように、前傾角θと右側境界投光距離Luとの一次関数θ=eLu+fは簡単に測定することが可能である。まず、第2形態において述べたように、指向性投光器を特定被清掃面上に前傾角θで前傾させる。前傾角θを増大させながら、前傾角θ毎に右側境界投光距離Luを測定していく。θとLuとの関係を一次関数で回帰することによって前記一次関数を容易に導出することができる。この様にして、測定用の指向性投光器が決まれば、その指向性投光器に特有の一次関数θ=eLu+fを事前に決定することができる。前傾角θを大きくすると、塵埃可視化良好領域は投光レンズ側に接近するから、右側境界投光距離Luも小さくなることは明らかである。つまり、前記一次関数の傾きeはe<0であることは明白である。
この一次関数が事前に分かっていると、清掃しようとする任意の被清掃面上に前記指向性投光器を載置前傾しなくても、もし塵埃粒子が被清掃面上に存在する場合には、投光レンズの前方で右側境界投光距離Luよりも手前側に塵埃粒子が明瞭に確認できることが予測できる。従って、実際に前記指向性投光器を被清掃面上に載置前傾させたときには、肉眼を右側境界投光距離Luよりも手前側の位置に向けておくことによって、塵埃粒子の存否を迅速且つ容易に判断することが可能になる。前記第2形態では、左側境界投光距離Ltより遠方に塵埃粒子は確認できるから、この第3形態と組み合わせると、Lt≦L≦Luの範囲内に塵埃粒子が明瞭に確認できることになる。前記一次関数が不明の場合には、指向性投光器を被清掃面に載置前傾させても塵埃粒子がどの範囲まで観察されるかは試行錯誤により判断するしかない。つまり、この一次関数により塵埃粒子の出現位置を予測できるだけでなく、実際の観察動作においても迅速且つ容易な塵埃粒子の存否確認が可能になる。
また、塵埃粒子の確認を電子装置で行う場合には、指向性投光器により被清掃面を光照射していても、電子装置は被清掃面の全体観察を一気に為すことが不可能であるから、前記被清掃面の投光レンズ位置から遠方に向かって隈なく走査しながら塵埃粒子を確認せざるを得ない。つまり、塵埃可視化良好領域の更に遠方に存在する塵埃可視化不十分領域をも走査しなければならないから、極めて長大な不要時間を空費することになる。本発明を利用すると、前記一次関数が既に分かっているから、Lt≦L≦Luで表される塵埃可視化良好領域だけを集中的に走査すればよく、投光レンズから測って左側境界投光距離Lt〜右側境界投光距離Luの範囲内に塵埃粒子が容易に確認できるはずである。従って、前記電子装置による塵埃粒子の観察は、Lt≦L≦Luの範囲内に設定すればよく、電子装置による塵埃粒子の観察時間を劇的に短縮することが可能になる。
即ち、前記一次関数により、作業者が塵埃粒子を観察する場合には塵埃粒子の出現範囲を予測できる技術的効果を有し、電子装置により塵埃粒子を観察する場合には、走査時間の超短縮化という技術的効果を有する。
According to the third embodiment of the present invention, as shown in FIGS. 7 and 13, the linear function θ = eLu + f between the forward tilt angle θ and the right boundary light projection distance Lu can be easily measured. First, as described in the second embodiment, the directional projector is tilted forward at a forward tilt angle θ on the specific surface to be cleaned. While increasing the forward tilt angle θ, the right boundary light projection distance Lu is measured for each forward tilt angle θ. The linear function can be easily derived by regressing the relationship between θ and Lu with a linear function. In this way, if a directional projector for measurement is determined, a linear function θ = eLu + f unique to the directional projector can be determined in advance. When the forward tilt angle θ is increased, the dust visualization good region approaches the light projection lens side, so it is clear that the right boundary light projection distance Lu also decreases. That is, it is obvious that the slope e of the linear function is e <0.
If this linear function is known in advance, even if the directional projector is not tilted before placing on any surface to be cleaned, if dust particles are present on the surface to be cleaned It can be predicted that dust particles can be clearly confirmed in front of the right projection lens and in front of the right boundary projection distance Lu. Therefore, when the directional projector is actually tilted before being placed on the surface to be cleaned, the presence or absence of dust particles can be determined quickly by keeping the naked eye at a position closer to the front side than the right boundary projection distance Lu. It becomes possible to easily judge. In the second embodiment, dust particles can be confirmed farther than the left boundary projection distance Lt. Therefore, when combined with the third embodiment, the dust particles can be clearly confirmed within the range of Lt ≦ L ≦ Lu. When the linear function is unknown, it is only possible to determine to what extent the dust particles are observed by trial and error even if the directional projector is tilted before being placed on the surface to be cleaned. That is, not only can the appearance position of dust particles be predicted by this linear function, but also the presence / absence of dust particles can be confirmed quickly and easily in an actual observation operation.
In addition, when the dust particles are confirmed by the electronic device, even if the surface to be cleaned is irradiated with light by the directional projector, the electronic device cannot perform the entire observation of the surface to be cleaned at once. The dust particles must be confirmed while scanning from the projection lens position on the surface to be cleaned far away. That is, since a dust visualization insufficient region that is further away from the dust visualization good region must be scanned, a very long unnecessary time is wasted. When the present invention is used, since the linear function is already known, only the dust visualization good region represented by Lt ≦ L ≦ Lu needs to be intensively scanned, and the left boundary light projection distance measured from the light projection lens. Dust particles should be easily confirmed within the range of Lt to the right boundary projection distance Lu. Therefore, the observation of dust particles by the electronic device may be set within the range of Lt ≦ L ≦ Lu, and the observation time of dust particles by the electronic device can be dramatically shortened.
That is, the linear function has the technical effect that the operator can predict the appearance range of the dust particles when observing the dust particles, and the scanning time is extremely shortened when the dust particles are observed by the electronic device. Has the technical effect of
本発明の第4の形態では、指向性投光器を特定被清掃面の上方に光軸高さHだけ離間して平行配置し、次に、前縁を固定して後縁を上昇させて前傾角θだけ前傾させたとき、投光レンズから塵埃可視化良好領域の開始端(左側境界T)までの開始端投光距離は前記第1形態と前記第2形態を組み合わせることにより近似的に導出する方法が与えられている。前記第1形態では、光軸高さHだけ上昇させて平行配置させた場合に、光軸高さHと境界投光距離Lsの関係はH=aLs+bで与えられ、前記第2形態では、特定被清掃面上に前傾角θで前傾させた場合に、前傾角θと左側境界投光距離Ltとの関係はθ=cLt+dで与えられることが示されている。
上述した第1形態と第2形態を如何に近似的に組み合わせて本第4形態を導出するかは図14に示されている。従って、図14を参照しながらその近似的導出法を説明する。光軸高さHだけ上方に指向性投光器を水平配置した場合に、一次関数H=aLs+bが成立し、光軸高さHのときの境界投光距離Lsは点P1で示されている。この点P1を固定して指向性投光器を前傾させたと考えると、この点P1を始点として一次関数θ=cLt+dを作図することが近似の導入になる。前傾角θのときに左側境界投光距離Ltの点は点P2に相当する。この第4形態において、光軸高さHの空中で前傾角θだけ前傾させた場合には、塵埃可視化良好領域の開始端投光距離Lcは式(12−9)によりLc=Lt+P4P5で与えらえる。式(12−8)によりP4P5=Ls−P1P4であり、式(12−7)によりP1P4=−d/cであるから、式(12−8)に代入するとP4P5=Ls−(−d/c)=Ls+d/cになる。従って、式(12−9)により、Lc=Lt+Ls+d/cになることが分かった。以上から、開始端投光距離LcはLc=Lt+Ls+d/cで与えられることが近似的に証明された。
従って、本第4形態において、指向性投光器を光軸高さHに配置し、且つ前傾角θで前傾させた場合には、塵埃可視化良好領域の開始端投光距離LcはLc=Lt+Ls+d/cで与えられる。投光レンズからの投光距離をLとすると、L≧Lcの領域が塵埃可視化良好領域に相当し、肉眼や電子装置によりL≧Lcの領域を観察すれば、塵埃粒子が存在する場合には塵埃粒子からの微弱散乱光を迅速且つ容易に検出することが可能になる。
この不等式が事前に分かっていると、清掃しようとする任意の被清掃面上に前記指向性投光器を載置しなくても、もし塵埃粒子が被清掃面上に存在する場合には、投光レンズの前方で開始端投光距離Lcよりも遠方に塵埃粒子が明瞭に確認できることが予測できる。従って、実際に前記指向性投光器を被清掃面上に載置したときには、肉眼を開始端投光距離Lcよりも遠方の位置に向けておくことによって、塵埃粒子の存否を迅速且つ容易に判断することが可能になる。もし、前記不等式が不明の場合には、指向性投光器を被清掃面に載置しても塵埃粒子がどの位置に観察されるかは試行錯誤により判断するしかない。即ち、この不等式により塵埃粒子の出現位置を予測できるだけでなく、実際の観察動作においても迅速且つ容易な塵埃粒子の存否確認が可能になる。
更に、前述したように、塵埃粒子の確認を電子装置で行う場合には、指向性投光器により被清掃面を光照射していても、電子装置は被清掃面の全体を一気に観察することが不可能であるから、前記被清掃面の投光レンズ位置から前方に向かって隈なく走査しながら塵埃粒子を確認する以外にない。つまり、塵埃可視化不十分領域をも走査しなければならないから、それだけ不要な時間を浪費することになる。本発明を利用すると、前記不等式が既に分かっているから、塵埃可視化良好領域だけを走査すればよく、投光レンズから測ってより遠方の位置に塵埃粒子が容易に確認できるはずである。従って、前記電子装置による塵埃粒子の観察は、開始端投光距離Lcの位置より遠方に設定すればよく、電子装置による塵埃粒子の観察時間を急激に短縮することが可能になる。
In the fourth embodiment of the present invention, the directional projector is disposed in parallel above the specific surface to be cleaned, spaced apart by the optical axis height H, and then the front edge is fixed and the rear edge is raised to increase the forward tilt angle. When tilted forward by θ, the start end projection distance from the projection lens to the start end (left boundary T) of the dust visualization good region is approximately derived by combining the first form and the second form. A method is given. In the first embodiment, when the optical axis height H is raised and arranged in parallel, the relationship between the optical axis height H and the boundary projection distance Ls is given by H = aLs + b. It is shown that the relationship between the forward tilt angle θ and the left boundary light projection distance Lt is given by θ = cLt + d when tilted forward on the surface to be cleaned by the forward tilt angle θ.
FIG. 14 shows how the first embodiment and the second embodiment described above are approximately combined to derive the fourth embodiment. Therefore, the approximate derivation method will be described with reference to FIG. When the horizontally disposed directional projector upwards by the optical axis height H, satisfied a linear function H = ALS + b, the boundary projection distance Ls when the optical axis height H indicated by a point P 1. Assuming that the point P 1 is fixed and the directional projector is tilted forward, drawing the linear function θ = cLt + d from this point P 1 is an introduction of approximation. The points left boundary projection distance Lt when the forward inclination θ corresponding to the point P 2. In this fourth embodiment, when the forward tilt angle θ is tilted forward in the air with the optical axis height H, the start end projection distance Lc of the dust visualization good region is expressed by Lc = Lt + P 4 P according to the equation (12-9). 5 is given. Since P 4 P 5 = Ls−P 1 P 4 according to the equation (12-8) and P 1 P 4 = −d / c according to the equation (12-7), when substituting into the equation (12-8) P 4 P 5 = Ls − (− d / c) = Ls + d / c. Therefore, it was found from the equation (12-9) that Lc = Lt + Ls + d / c. From the above, it was approximately proved that the start end projection distance Lc is given by Lc = Lt + Ls + d / c.
Therefore, in the fourth embodiment, when the directional projector is disposed at the optical axis height H and tilted forward at the forward tilt angle θ, the start-end projection distance Lc in the dust visualization good region is Lc = Lt + Ls + d / c. If the projection distance from the projection lens is L, the region of L ≧ Lc corresponds to the dust visualization good region, and if dust particles are present if the region of L ≧ Lc is observed with the naked eye or an electronic device. It becomes possible to quickly and easily detect weakly scattered light from dust particles.
If this inequality is known in advance, even if the directional projector is not placed on any surface to be cleaned, if the dust particles are present on the surface to be cleaned, It can be predicted that dust particles can be clearly confirmed in front of the lens and far from the start end projection distance Lc. Therefore, when the directional projector is actually placed on the surface to be cleaned, the presence or absence of dust particles can be quickly and easily determined by keeping the naked eye at a position farther than the start-end projection distance Lc. It becomes possible. If the inequality is unknown, the position where the dust particles are observed can only be determined by trial and error even when the directional projector is placed on the surface to be cleaned. That is, not only can the appearance position of the dust particles be predicted by this inequality, but also the presence / absence of the dust particles can be quickly and easily confirmed in the actual observation operation.
Furthermore, as described above, when the dust particles are confirmed by the electronic device, the electronic device cannot observe the entire surface to be cleaned at a stretch even if the surface to be cleaned is irradiated with light by a directional projector. Since it is possible, there is nothing but to confirm the dust particles while scanning all the way forward from the position of the projection lens on the surface to be cleaned. That is, since it is necessary to scan a region where dust is insufficiently visualized, unnecessary time is wasted. When the present invention is used, since the inequality is already known, it is only necessary to scan the dust visualization good region, and dust particles should be easily confirmed at a farther position as measured from the light projecting lens. Therefore, the observation of the dust particles by the electronic device may be set far from the position of the start end projection distance Lc, and the observation time of the dust particles by the electronic device can be shortened rapidly.
本発明の第5の形態では、指向性投光器を特定被清掃面の上方に光軸高さHだけ離間して平行配置し、次に、前縁を固定して後縁を上昇させて前傾角θだけ前傾させたとき、投光レンズから塵埃可視化良好領域の終了端(右側境界U)までの終了端投光距離Luは前記第1形態と前記第3形態を組み合わせることにより近似的に導出する方法が与えられている。前記第1形態では、光軸高さHだけ上昇させて平行配置させた場合に、光軸高さHと境界投光距離Lsの関係はH=aLs+bで与えられ、前記第3形態では、特定被清掃面上に前傾角θで前傾させた場合に、前傾角θと右側境界投光距離Luとの関係はθ=eLu+fで与えられることが示されている。
上述した第1形態と第3形態を如何に近似的に組み合わせて本第5形態を導出するかは図14に示されている。従って、図14を参照しながらその近似的導出法を説明する。
光軸高さHだけ上方に指向性投光器を水平配置した場合に、一次関数H=aLs+bが成立し、光軸高さHのときの境界投光距離Lsは点P1で示されている。この点P1を固定して指向性投光器を前傾させたと考えると、この点P1を始点として一次関数θ=eLu+fを作図することが近似の導入になる。前傾角θのときに右側境界投光距離Luの点は点P3に相当する。この第5形態において、光軸高さHの空中で前傾角θだけ前傾させた場合には、塵埃可視化良好領域の終了端投光距離Leは式(12−10)によりLe=Lu+P4P5で与えらえる。式(12−8)によりP4P5=Ls−P1P4であり、式(12−7)によりP1P4=−d/cであるから、式(12−8)に代入するとP4P5=Ls−(−d/c)=Ls+d/cになる。従って、式(12−10)により、Le=Lu+Ls+d/cになることが分かった。以上から、終了端投光距離LeはLe=Lu+Ls+d/cで与えられることが近似的に証明された。
従って、本第5形態において、指向性投光器を光軸高さHに配置し、且つ前傾角θで前傾させた場合には、塵埃可視化良好領域の終了端投光距離LeはLe=Lu+Ls+d/cで与えられる。投光レンズからの投光距離をLとすると、L≦Leの領域が塵埃可視化良好領域に相当し、肉眼や電子装置によりL≦Leの領域を観察すれば、塵埃粒子が存在する場合には塵埃粒子からの微弱散乱光を迅速且つ容易に検出することが可能になる。しかも、第4形態からL≧Lcの領域が塵埃可視化良好領域に相当するから、L≦Leと組み合わせると、Lc≦L≦Leの範囲が塵埃可視化良好領域であることが確定する。
この不等式が事前に分かっていると、清掃しようとする任意の被清掃面上に前記指向性投光器を載置しなくても、もし塵埃粒子が被清掃面上に存在する場合には、投光レンズの前方で開始端投光距離Lcよりも遠方で、且つ終了端投光距離Leよりも手前に塵埃粒子が明瞭に確認できることが予測できる。従って、実際に前記指向性投光器を被清掃面上に載置したときには、肉眼をLc≦L≦Leの範囲に向けておくことによって、塵埃粒子の存否を迅速且つ容易に判断することが可能になる。もし、前記不等式が不明の場合には、指向性投光器を被清掃面に載置しても塵埃粒子がどの位置に観察されるかは試行錯誤により判断するしかない。即ち、この不等式により塵埃粒子の出現位置を予測できるだけでなく、実際の観察動作においても迅速且つ容易な塵埃粒子の存否確認が可能になる。
更に、前述したように、塵埃粒子の確認を電子装置で行う場合には、指向性投光器により被清掃面を光照射していても、電子装置は被清掃面の全体を一気に観察することが不可能であるから、前記被清掃面の投光レンズ位置から前方に向かって隈なく走査しながら塵埃粒子を確認する以外にない。つまり、塵埃可視化不十分領域をも走査しなければならないから、それだけ不要な時間を浪費することになる。本発明を利用すると、前記不等式が既に分かっているから、塵埃可視化良好領域だけを走査すればよく、投光レンズから測って手前側の塵埃可視化不十分領域及び更に遠方にある塵埃可視化不十分領域を避けることにより、塵埃粒子を迅速且つ容易に観察できるはずである。従って、前記電子装置による塵埃粒子の観察は、投光距離LをLc≦L≦Leの範囲に限定的に設定すればよく、電子装置による塵埃粒子の観察時間を急激に短縮することが可能になる。
In the fifth aspect of the present invention, the directional projector is disposed in parallel above the specific surface to be cleaned, spaced apart by the optical axis height H, and then the front edge is fixed and the rear edge is raised to increase the forward tilt angle. When tilted forward by θ, the end-end projection distance Lu from the projection lens to the end of the good dust visualization region (right boundary U) is approximately derived by combining the first form and the third form. A way to do is given. In the first embodiment, when the optical axis height H is increased and arranged in parallel, the relationship between the optical axis height H and the boundary projection distance Ls is given by H = aLs + b. It is shown that the relationship between the forward tilt angle θ and the right boundary light projection distance Lu is given by θ = eLu + f when tilted forward on the surface to be cleaned by the forward tilt angle θ.
FIG. 14 shows how the first embodiment and the third embodiment described above are approximately combined to derive the fifth embodiment. Therefore, the approximate derivation method will be described with reference to FIG.
When the horizontally disposed directional projector upwards by the optical axis height H, satisfied a linear function H = ALS + b, the boundary projection distance Ls when the optical axis height H indicated by a point P 1. Considering that the point P 1 is fixed and the directional projector is tilted forward, it is an approximation to draw a linear function θ = eLu + f with this point P 1 as a starting point. The terms of the right boundary projection distance Lu at forward inclination θ corresponding to the point P 3. In the fifth embodiment, when the forward tilt angle θ is tilted forward in the air with the optical axis height H, the end projection distance Le of the dust visualization good region is Le = Lu + P 4 P according to the equation (12-10). 5 is given. Since P 4 P 5 = Ls−P 1 P 4 according to the equation (12-8) and P 1 P 4 = −d / c according to the equation (12-7), when substituting into the equation (12-8) P 4 P 5 = Ls − (− d / c) = Ls + d / c. Therefore, it was found from the formula (12-10) that Le = Lu + Ls + d / c. From the above, it has been approximately proved that the end-end projection distance Le is given by Le = Lu + Ls + d / c.
Therefore, in the fifth embodiment, when the directional projector is disposed at the optical axis height H and tilted forward at the forward tilt angle θ, the end projection distance Le in the dust visualization good region is Le = Lu + Ls + d / c. When the light projection distance from the light projection lens is L, the region of L ≦ Le corresponds to the region of good dust visualization. If the region of L ≦ Le is observed with the naked eye or an electronic device, dust particles are present. It becomes possible to quickly and easily detect weakly scattered light from dust particles. Moreover, since the region of L ≧ Lc corresponds to the dust visualization good region from the fourth embodiment, when combined with L ≦ Le, it is determined that the range of Lc ≦ L ≦ Le is the dust visualization good region.
If this inequality is known in advance, even if the directional projector is not placed on any surface to be cleaned, if the dust particles are present on the surface to be cleaned, It can be predicted that dust particles can be clearly confirmed in front of the lens and farther than the start end projection distance Lc and before the end end projection distance Le. Therefore, when the directional projector is actually placed on the surface to be cleaned, it is possible to quickly and easily determine the presence or absence of dust particles by keeping the naked eye in the range of Lc ≦ L ≦ Le. Become. If the inequality is unknown, the position where the dust particles are observed can only be determined by trial and error even when the directional projector is placed on the surface to be cleaned. That is, not only can the appearance position of the dust particles be predicted by this inequality, but also the presence / absence of the dust particles can be quickly and easily confirmed in the actual observation operation.
Furthermore, as described above, when the dust particles are confirmed by the electronic device, the electronic device cannot observe the entire surface to be cleaned at a stretch even if the surface to be cleaned is irradiated with light by a directional projector. Since it is possible, there is nothing but to confirm the dust particles while scanning all the way forward from the position of the projection lens on the surface to be cleaned. That is, since it is necessary to scan a region where dust is insufficiently visualized, unnecessary time is wasted. By using the present invention, since the inequality is already known, it is only necessary to scan the dust visualization good region, the dust visualization insufficient region on the near side as measured from the projection lens, and the dust visualization insufficient region farther away. By avoiding this, dust particles should be able to be observed quickly and easily. Therefore, the observation of the dust particles by the electronic device may be performed by setting the projection distance L limited to the range of Lc ≦ L ≦ Le, and the observation time of the dust particles by the electronic device can be drastically shortened. Become.
本発明の第6形態によれば、前記指向性投光器の光度を強弱調整することによって、前記指向性投光器により光照射される被清掃面の照度が可変調整され、被清掃面上における前記塵埃粒子の観察が容易になる被清掃面の汚れ具合判別方法が提供される。単純に、光度をC倍にすれば被清掃面の照度もC倍になることは容易に予想がつく。一般に、光度、光束、照度は次のように定義されている。光源である指向性投光器の光度をC(カンデラ)とすると、単位立体角(1ステラジアン)当たりにCルーメンの光束を放出する。光源からR(m)離れた位置で光束に直交する面積S(m2)の張る立体角はS/R2(ステラジアン)であるから、面積Sに入る光束はC×S/R2(ルーメン)である。従って、その面の照度はC×S/R2(ルックス)、即ちC×S/R2(lx)になる。即ち、その面が被清掃面であれば、被清掃面上の塵埃粒子による微弱散乱光はC×S/R2に比例するから、単純に光源の光度C(カンデラ)に比例すると考えることができる。従って、前記指向性投光器の光度を強弱調整することによって、塵埃粒子の観察が最良になる光度を選択することが、本発明に係る被清掃面の汚れ具合判別方法の技術的効果を高めることは明らかである。 According to the sixth aspect of the present invention, by adjusting the intensity of the directional projector, the illuminance of the surface to be cleaned that is irradiated by the directional projector is variably adjusted, and the dust particles on the surface to be cleaned are adjusted. A method for determining the degree of contamination of the surface to be cleaned is provided. Simply, it can be easily predicted that if the luminous intensity is increased by C times, the illuminance of the surface to be cleaned will also increase by C times. In general, luminous intensity, luminous flux, and illuminance are defined as follows. If the luminous intensity of the directional projector as the light source is C (candela), a C lumen luminous flux is emitted per unit solid angle (1 steradian). Since the solid angle spanned by the area S (m2) orthogonal to the light beam at a position away from the light source by R (m) is S / R2 (steradian), the light beam entering the area S is C × S / R2 (lumen). . Accordingly, the illuminance on the surface is C × S / R2 (look), that is, C × S / R2 (lx). That is, if the surface is a surface to be cleaned, the weakly scattered light from the dust particles on the surface to be cleaned is proportional to C × S / R2, and therefore can be considered to be simply proportional to the light intensity C (candela) of the light source. . Therefore, by adjusting the intensity of the directional projector, it is possible to increase the technical effect of the method for determining the degree of contamination of the surface to be cleaned according to the present invention by selecting the intensity at which the dust particles are best observed. it is obvious.
本発明の第7の形態によれば、指向性投光器としてLED、レーザー光源又はランプからなる前方指向性を有した光源を用いることにより迅速且つ確実な被清掃面の汚れ具合判別方法を提供することができる。特に、近年のLEDの開発は凄まじく、LEDとレンズを組み合わせることにより強光度且つ高指向性で低価格の指向性投光器が市場に提供されるようになった。また、低価格の半導体レーザー光源も開発されており、その光指向性はLEDを遥かに超えるものである。更に、従来型のランプであっても、反射鏡の開発により高指向性の投光器を実現することができる。従って、これらの指向性投光器を用いることにより、本発明を容易に実現することが可能になる。 According to the seventh aspect of the present invention, there is provided a quick and reliable method for determining the degree of contamination of a surface to be cleaned by using a light source having forward directivity composed of an LED, a laser light source or a lamp as a directional projector. Can do. In particular, the development of LEDs in recent years has been tremendous, and by combining LEDs and lenses, directional projectors with high brightness, high directivity, and low price have come to be provided to the market. In addition, low-cost semiconductor laser light sources have been developed, and their light directivity far exceeds that of LEDs. Furthermore, even with a conventional lamp, a highly directional projector can be realized by developing a reflecting mirror. Therefore, the present invention can be easily realized by using these directional projectors.
本発明の第8の形態によれば、上述した被清掃面の汚れ具合判別方法を用いて、被清掃面上の塵埃可視化良好領域内で塵埃粒子を観察し、この観察結果を判断して前記被清掃面を清掃する被清掃面の清掃方法を提供することができる。本発明の特徴は、既に述べたように、モップや電機掃除機から光源を分離して、指向性投光器による塵埃の観察と、それに続く清掃行為とを分離するものである。従って、まず指向性投光器により被清掃面上に塵埃粒子が有るか無いかを判別し、もし有ればモップや電機掃除機により前記被清掃面を清掃し、もし無ければ前記被清掃面は清浄であるから清掃の必要は無い。即ち、本発明に係る被清掃面の汚れ具合判別方法により、まず被清掃面の汚れ具合を判別し、この判断によって清掃行為を行うかどうかを決断させることが本発明の特徴である。 According to the eighth aspect of the present invention, by using the above-described method for determining the degree of contamination of the surface to be cleaned, the dust particles are observed within the dust visualization good region on the surface to be cleaned, and the observation result is determined and The cleaning method of the to-be-cleaned surface which cleans to-be-cleaned surface can be provided. As described above, the feature of the present invention is that the light source is separated from the mop or the electric vacuum cleaner, and the observation of dust by the directional projector and the subsequent cleaning action are separated. Therefore, it is first determined whether or not dust particles are present on the surface to be cleaned with a directional projector, and if so, the surface to be cleaned is cleaned with a mop or an electric vacuum cleaner, and if not, the surface to be cleaned is clean. Therefore, there is no need for cleaning. That is, it is a feature of the present invention that the method of determining the degree of contamination of the surface to be cleaned according to the present invention first determines the degree of contamination of the surface to be cleaned and determines whether or not to perform the cleaning action based on this determination.
以下に、本発明に係る被清掃面の汚れ具合判別方法及び清掃方法の実施形態を図面及び表に従って詳細に説明する。 Hereinafter, embodiments of a method for determining the degree of contamination of a surface to be cleaned and a cleaning method according to the present invention will be described in detail with reference to the drawings and tables.
図1は、本発明において、指向性投光器を被清掃面に水平配置して散乱光により塵埃粒子を可視化する観察斜視図である。清掃対象となる被清掃面2の上に指向性投光器4が載置され、投光レンズ6から前方に向けて無数の光線が光コーン8として照射され、その前方断面がハッチングにより光コーン断面10として図示されている。被清掃面2の表面には粒子、繊維屑、毛髪等からなる塵埃粒子12が散乱しており、前記光コーン8の照射により、夫々の塵埃粒子12から微弱散乱光が上空に反射されている。前記微弱散乱光には、観察者16から見て、塵埃粒子12が明瞭に確認される実線で描かれた良好散乱光14と、不明瞭にしか見えない点線で描かれた不十分散乱光15が含まれる。良好散乱光14は指向性投光器4の投光レンズ6からかなり遠方に出現し、不十分散乱光15は投光レンズ6の近傍に出現することが分かる。良好散乱光14と不十分散乱光15に分かれる理由は、次のように考えることができる。投光レンズ6の近傍では入射光が塵埃粒子12に高角度で入射するため、塵埃粒子12の背後に形成される影の領域が小さくなり、塵埃粒子12の明るい部分と影との間のコントラストが低下して観察者16には観察し難い微弱散乱光になる。他方、投光レンズ6の遠方では入射光が塵埃粒子12に低角度で入射する為、塵埃粒子12の背後に形成される影が長くなり、影と塵埃粒子12とのコントラストが強くなって、観察者16には良好散乱光14になると考えられる。また、高角度に入射すると、被清掃面2からの反射光が観察者16にも到達し、塵埃粒子12からの微弱散乱光が明るい反射光の中に埋没する為、微弱散乱光が見え難くなり、近傍では不十分散乱光15になるとも考えられる。従って、近傍ではコントラストの低下と微弱散乱光の埋没性が相乗して観察し難くなると考えることによって説明がつく。 FIG. 1 is an observation perspective view in which dust particles are visualized by scattered light by horizontally arranging a directional projector on a surface to be cleaned in the present invention. A directional projector 4 is placed on the surface to be cleaned 2 to be cleaned, and an infinite number of light beams are emitted from the light projecting lens 6 toward the front as a light cone 8. As shown. Dust particles 12 made of particles, fiber scraps, hair, etc. are scattered on the surface 2 to be cleaned, and weak scattered light is reflected from the dust particles 12 to the sky by the irradiation of the light cone 8. . The weak scattered light includes a good scattered light 14 drawn by a solid line where the dust particles 12 are clearly confirmed as viewed from the observer 16 and an insufficient scattered light 15 drawn by a dotted line that can only be seen indefinitely. Is included. It can be seen that the good scattered light 14 appears considerably far from the light projecting lens 6 of the directional projector 4, and the insufficient scattered light 15 appears in the vicinity of the light projecting lens 6. The reason why the light is separated into good scattered light 14 and insufficient scattered light 15 can be considered as follows. In the vicinity of the light projecting lens 6, incident light is incident on the dust particles 12 at a high angle. Therefore, a shadow area formed behind the dust particles 12 is reduced, and the contrast between the bright part of the dust particles 12 and the shadow is reduced. Decreases and becomes weak scattered light that is difficult for the observer 16 to observe. On the other hand, since the incident light is incident on the dust particles 12 at a low angle in the distance from the light projecting lens 6, the shadow formed behind the dust particles 12 becomes longer, and the contrast between the shadow and the dust particles 12 becomes stronger. It is considered that the observer 16 has good scattered light 14. Further, when the light is incident at a high angle, the reflected light from the surface to be cleaned 2 reaches the observer 16 and the weak scattered light from the dust particles 12 is buried in the bright reflected light, so that the weak scattered light is difficult to see. Therefore, it is considered that the scattered light 15 is insufficient in the vicinity. Therefore, in the vicinity, explanation can be made by considering that the decrease in contrast and the buried property of weakly scattered light are difficult to observe.
図2は、本発明において、指向性投光器4を被清掃面2からH(mm)だけ水平上昇配置したときの塵埃可視化不十分領域(A)と塵埃可視化良好領域(B)の水平測定図である。指向性投光器4の投光レンズ6を通る中心線が光軸となり、その光軸高さH0(mm)は指向性投光器4の断面半径に相当する。この指向性投光器4の光軸を被清掃面2から光軸高さH(mm)だけ上昇させる為に、前記指向性投光器4の前縁と後縁の底面側に厚さnΔh(mm)の厚紙18、18を積層する。前記厚紙18は、厚さΔh(mm)の紙板をn枚重ねて形成される。この状態で指向性投光器4を点灯すると、投光レンズ6から前方に光コーン8が照射される。点線で表される不十分散乱光15は投光レンズ6から境界Sまでの塵埃可視化不十分領域(A)に生じ、その長さは境界投光距離Ls(cm)により与えられる。更に境界Sの遠方に塵埃可視化良好領域(B)が形成され、塵埃粒子12による良好散乱光14は実線により表示されている。投光レンズ6から被清掃面2に平行に引かれた実線が光軸20である。不十分散乱光15の反射角は良好散乱光14の反射角よりも大きくなり、その結果不十分散乱光15は観察者16により不明瞭にしか観察されず、他方良好散乱光14はより低角度での散乱光であるから、観察者16にとって明瞭に観察されることが分かる。 FIG. 2 is a horizontal measurement diagram of a dust visualization insufficient region (A) and a dust visualization good region (B) when the directional projector 4 is horizontally raised by H (mm) from the surface to be cleaned 2 in the present invention. is there. The center line passing through the light projecting lens 6 of the directional projector 4 is the optical axis, and the optical axis height H 0 (mm) corresponds to the cross-sectional radius of the directional projector 4. In order to raise the optical axis of the directional projector 4 from the surface 2 to be cleaned by the optical axis height H (mm), the directional projector 4 has a thickness nΔh (mm) on the bottom side of the front edge and the rear edge. Thick papers 18 and 18 are stacked. The thick paper 18 is formed by stacking n paper plates having a thickness Δh (mm). When the directional projector 4 is turned on in this state, the light cone 8 is irradiated forward from the projector lens 6. Insufficient scattered light 15 represented by a dotted line is generated in a dust visualization insufficient region (A) from the projection lens 6 to the boundary S, and the length is given by the boundary projection distance Ls (cm). Further, a dust visualization good region (B) is formed far from the boundary S, and the good scattered light 14 by the dust particles 12 is indicated by a solid line. A solid line drawn in parallel to the surface to be cleaned 2 from the light projecting lens 6 is the optical axis 20. The reflection angle of the insufficiently scattered light 15 is larger than the reflection angle of the good scattered light 14, so that the insufficiently scattered light 15 is only observed indefinitely by the observer 16, while the good scattered light 14 is at a lower angle. It can be seen that it is clearly observed for the observer 16 because of the scattered light at.
前記紙板の枚数をn枚とすると、光軸高さH(mm)はH=H0+nΔhになることがわかる。この実施形態では、Δh=0.40(mm)が用いられたが、その厚さは自在に調整できることは言うまでもない。枚数nを0〜16枚へと次第に増やしていくと、光軸高さH(mm)はH=H0+6.40(mm)に達する。また第1例として、指向性投光器4の断面半径H0がH0=8.00(mm)であるとすると、H=8.00〜14.40(mm)の範囲で光軸高さHを変化させることができる。光軸高さHを増大させると、光コーン8は上方に移動するから、光コーン8と被清掃面2との交点Q1は次第に遠方へ移動し、境界投光距離Lsもそれに連れて大きくなる。 Assuming that the number of paper plates is n, the optical axis height H (mm) is H = H0 + nΔh. In this embodiment, Δh = 0.40 (mm) is used, but it goes without saying that the thickness can be freely adjusted. As the number n is gradually increased from 0 to 16, the optical axis height H (mm) reaches H = H0 + 6.40 (mm). As a first example, if the cross-sectional radius H0 of the directional projector 4 is H0 = 8.00 (mm), the optical axis height H is changed in the range of H = 8.00 to 14.40 (mm). Can be made. When the optical axis height H is increased, the light cone 8 moves upward, so that the intersection point Q1 between the light cone 8 and the surface to be cleaned 2 gradually moves farther, and the boundary light projection distance Ls increases accordingly. .
表1は被清掃面2から指向性投光器4(第1例)の光軸をH(mm)だけ水平上昇させたときの可視化状態の一覧表である。光軸高さH毎に投光距離L=5、10・・・50(cm)の位置で可視化状態を、最も良く見える(◎)、見える(○)、やや見える(△)、見えない(×)の4段階で肉眼判断したものである。 Table 1 is a list of visualization states when the optical axis of the directional projector 4 (first example) is raised horizontally from the surface to be cleaned 2 by H (mm). Visualization state is best seen (◎), visible (O), somewhat visible (△), invisible at the position of projection distance L = 5, 10 ... 50 (cm) for each optical axis height H ( The visual judgment was made in four stages (x).
表1において、光軸高さH(mm)の各値毎に、投光距離Lの一番小さな値の位置に出現する○印の枠が太線によって形成されている。これらの太線枠を連ねた境界線が、塵埃可視化不十分領域(A)と塵埃可視化良好領域(B)の境界線S(境界とも言う)になる。即ち、塵埃可視化不十分領域(B)は△印より左側の投光領域(×と△の領域)であり、塵埃可視化良好領域(A)は○印より右側の投光領域(○と◎の領域)である。 In Table 1, for each value of the optical axis height H (mm), a frame marked with a circle that appears at the position of the smallest value of the projection distance L is formed by a thick line. A boundary line connecting these thick line frames is a boundary line S (also referred to as a boundary) between the dust visualization insufficient region (A) and the dust visualization good region (B). That is, the dust visualization insufficient region (B) is a light projection region on the left side of the Δ mark (× and Δ regions), and the dust visualization good region (A) is a light projection region on the right side of the ○ mark (circles of ○ and ◎). Area).
表2は指向性投光器(第1例)の水平配置の可視化状態表(表1)から得られる塵埃可視化良好領域(B)の開始座標、即ち良好領域(B)と不十分領域(A)の境界Sの座標群を示している。言い換えれば、投光距離L(cm)と限界光軸高さHmax(mm)の座標群である。表1において、太線枠で囲われた位置の座標群であり、Hmaxは、投光距離L(cm)の位置で、塵埃が見える状態(○)を与える光軸高さH(mm)のうち、最大の値になる限界光軸高さである。従って、特定の投光距離L(cm)の位置におけるH(mm)≦Hmax(mm)の光軸高さ領域は塵埃が見える領域(○及び◎)である。 Table 2 shows the start coordinates of the dust visualization good region (B) obtained from the horizontal state visualization state table (Table 1) of the directional projector (first example), that is, the good region (B) and the insufficient region (A). The coordinate group of the boundary S is shown. In other words, the coordinate group includes a light projection distance L (cm) and a limit optical axis height Hmax (mm). In Table 1, it is a coordinate group of the position surrounded by the thick line frame, and Hmax is the optical axis height H (mm) that gives a state (◯) in which dust can be seen at the position of the projection distance L (cm). The optical axis height is the maximum value. Therefore, the optical axis height region of H (mm) ≦ Hmax (mm) at the position of the specific projection distance L (cm) is a region where the dust can be seen (◯ and ◎).
これらの座標群に対して最小二乗法を適用し、L=10、15、20、25、30(cm)における境界線Sの回帰式を一次関数で導出する。即ち、表2の中で式(3−1)のようにH=aLs+bの一次関数で回帰すると、a=0.336、b=4.16が導出されるから、式(3)は、即ちH(mm)=0.336Ls(cm)+4.16が境界線Sとして得られる。 The least square method is applied to these coordinate groups, and the regression equation of the boundary line S at L = 10, 15, 20, 25, 30 (cm) is derived as a linear function. That is, when regression is performed with a linear function of H = aLs + b as shown in Equation (3-1) in Table 2, a = 0.336 and b = 4.16 are derived, and thus Equation (3) is expressed as follows: H (mm) = 0.336 Ls (cm) +4.16 is obtained as the boundary line S.
図3は、本発明(第1例)において、図4の境界線Sを与える1次関数H=aLs+bを最小二乗法により推定する境界線推定演算図である。図中に示される表において、(X、Y)は(L、Hmax)を意味しており、Xはcm単位、Yはmm単位である。これら5点の座標点により最小二乗法を用いて傾きaと切片bを式(1)及び式(2)により演算する。その結果、a=0.336及びb=4.16が得られた。従って、境界線Sを与える1次関数は式(3)のようにH=0.336Ls+4.16になることが分かった。 FIG. 3 is a boundary line estimation calculation diagram for estimating the linear function H = aLs + b giving the boundary line S of FIG. 4 by the least square method in the present invention (first example). In the table shown in the figure, (X, Y) means (L, Hmax), where X is in cm and Y is in mm. The inclination a and the intercept b are calculated by the equations (1) and (2) using the least squares method with these five coordinate points. As a result, a = 0.336 and b = 4.16 were obtained. Therefore, it was found that the linear function that gives the boundary line S is H = 0.336Ls + 4.16 as shown in Equation (3).
図4は、本発明において断面半径H0=8mmの指向性投光器(第1例)を用いた場合に、表2の境界値をプロットして、表1の塵埃可視化良好領域(B)と塵埃可視化不十分領域(A)を示したH−L関係図である。境界線Sより左側は塵埃可視化不十分領域(A)であり、境界線Sより右側は塵埃可視化良好領域(B)である。この表の使用方法は次の通りである。指向性投光器の光軸を被清掃面の上方H(mm)に水平配置したとき、前記Hに対応する境界線S上の投光距離Lが境界投光距離Lsになる。従って、L≦Lsの領域が塵埃可視化不十分領域(A)であり、L≧Lsの領域が塵埃可視化良好領域(B)である。使用する指向性投光器に対応した境界線Sの一次関数が事前に分かっておれば、塵埃粒子が明瞭に確認される領域は塵埃可視化良好領域(B)であるから、観察者はL≧Lsの領域に注目して塵埃粒子の存否を判断すればよいことになる。観察者が肉眼であるときには、肉眼は被清掃面の全体を瞬時に判断する能力を有しているから、L≧Lsの領域にあえて注目する必要性は少ないであろう。しかし、観察者が電子機器である場合には、電子機器は被清掃面の全体を瞬時に判断する能力を有していないから、L≧Lsの領域に着目して電子機器を操作することにより、塵埃粒子の存否の判断を短時間で行うことが可能になる。もしL≧Lsの情報がない場合には、電子機器はL≧0の全領域を走査しなければならず、0≦L≦Lsの領域を走査する時間が無駄になることは明らかである。従って、L≧Lsの情報を与える図4は電子機器を用いた塵埃粒子の確認走査では画期的であるといえる。 FIG. 4 shows the case where a directional projector (first example) having a cross-sectional radius H 0 = 8 mm is used in the present invention, the boundary values in Table 2 are plotted, and the dust visualization good region (B) and dust in Table 1 are plotted. It is the HL relationship figure which showed the visualization insufficient area | region (A). The area on the left side of the boundary line S is a dust visualization insufficient area (A), and the area on the right side of the boundary line S is a dust visualization good area (B). The usage of this table is as follows. When the optical axis of the directional projector is horizontally arranged above the surface to be cleaned H (mm), the projection distance L on the boundary line S corresponding to the H becomes the boundary projection distance Ls. Therefore, the region of L ≦ Ls is the dust visualization insufficient region (A), and the region of L ≧ Ls is the dust visualization good region (B). If the linear function of the boundary line S corresponding to the directional projector to be used is known in advance, the region where the dust particles are clearly confirmed is the dust visualization good region (B). What is necessary is just to judge the presence or absence of a dust particle paying attention to an area | region. When the observer is the naked eye, the naked eye has the ability to instantaneously determine the entire surface to be cleaned, so there is little need to pay attention to the region where L ≧ Ls. However, when the observer is an electronic device, the electronic device does not have the ability to instantaneously determine the entire surface to be cleaned, and therefore, by operating the electronic device while paying attention to the region of L ≧ Ls. In addition, it is possible to determine whether dust particles are present in a short time. If there is no information of L ≧ Ls, the electronic device must scan the entire region of L ≧ 0, and it is clear that the time to scan the region of 0 ≦ L ≦ Ls is wasted. Therefore, it can be said that FIG. 4 which gives information of L ≧ Ls is epoch-making in the confirmation scanning of dust particles using an electronic device.
図5は、本発明において、指向性投光器を水平から前傾角θだけ前傾させたときの塵埃可視化状態の変化図である。この図5では、指向性投光器4を前傾角θだけ前傾させたときに、光線が被清掃面と交叉する点までの距離、即ち水平状態の投光距離Lnがどれだけ小さくなるかを理論的に検討することになる。この小さくなった投光距離を前傾投光距離Xで表す。破線で表される図形が水平状態を示し、実線で表される図形が傾斜状態を示す。指向性投光器4の中心を4aとし、光軸20は中心4aから伸び、また光線も前記中心4aから被清掃面に投射される。被清掃面から中心4aまでの高さが光軸高さHであり、中心から投光レンズまでの長さが半軸長L0である。投光距離Lnに至る光線(破線表示)と光軸高さHを示す鉛直線とのなす角度が投光角度αである。 FIG. 5 is a change diagram of the dust visualization state when the directional projector is tilted forward from the horizontal by the forward tilt angle θ in the present invention. In FIG. 5, when the directional projector 4 is tilted forward by the forward tilt angle θ, the distance to the point where the light beam intersects the surface to be cleaned, that is, the light projection distance Ln in the horizontal state, is theoretically reduced. Will be considered. This reduced projection distance is represented by a forward tilt projection distance X. A graphic represented by a broken line indicates a horizontal state, and a graphic represented by a solid line indicates an inclined state. The center of the directional projector 4 is 4a, the optical axis 20 extends from the center 4a, and the light beam is projected from the center 4a onto the surface to be cleaned. Height from a surface to be cleaned to the center 4a is an optical axis height H, the length from the center to the projection lens is Hanjikucho L 0. The angle formed by the light beam reaching the projection distance Ln (shown by a broken line) and the vertical line indicating the optical axis height H is the projection angle α.
図6は、本発明において、図5のように前傾角θだけ前傾させたとき、投光距離Lnから前傾投光距離Xの導出過程図である。図5を参照すると、tan(α)及びtan(α−θ)は式(4)及び式(5)により与えられる。式(4)及び式(5)から投光角度αを消去することによって投光距離Lnと前傾投光距離Xの関係を導出する。まずtan(α−θ)を展開すると式(6)が得られる。式(4)と式(5)を式(6)に代入すると式(7)を得ることができる。この式(7)を解いて前傾投光距離Xを求めると、式(8)が得られる。この式(8)を見ると分かるように、XはL0、Ln、H、θの4パラメータによって表現されることが分かる。XはLnより小さいから、X/Lnを求めると、式(9)が得られる。θ≧0であるから、X/Ln≦1であることは当然である。式(9)がX/Ln≦1の性質を有することを数値計算により示す。この数値計算の結果は表3に示されている。 FIG. 6 is a derivation process diagram of the forward tilt projection distance X from the projection distance Ln when the forward tilt angle θ is tilted forward as shown in FIG. 5 in the present invention. Referring to FIG. 5, tan (α) and tan (α−θ) are given by Equation (4) and Equation (5). The relationship between the projection distance Ln and the forward tilt projection distance X is derived by eliminating the projection angle α from the formulas (4) and (5). First, when tan (α−θ) is expanded, Equation (6) is obtained. By substituting Equation (4) and Equation (5) into Equation (6), Equation (7) can be obtained. When this formula (7) is solved to find the forward tilted projection distance X, formula (8) is obtained. As can be seen from this equation (8), it can be seen that X is expressed by four parameters L0, Ln, H, and θ. Since X is smaller than Ln, when X / Ln is obtained, Equation (9) is obtained. Since θ ≧ 0, it is natural that X / Ln ≦ 1. It is shown by numerical calculation that the formula (9) has the property of X / Ln ≦ 1. The results of this numerical calculation are shown in Table 3.
表3は、L0(mm)、Ln(mm)、θ(度)、H(mm)の各数値を用いて、X(mm)とX/Lnを式(8)及び式(9)により夫々演算した結果を示している。半軸長L0を46.5mmに固定し、Ln=100mm且つH=8.8mmにしたときに、前傾角θを0度、0.7度、1.34度と増大させた場合に、X(mm)とX/Lnが演算された。その結果、Xは100.0mm〜58.8mmに小さくなり、X/Lnは1.000〜0.588へと小さくなることが分かった。また、Ln=700mmの遠地点での挙動を調べた。H=10mmに固定して、前傾角θを0度〜5度まで増大させた場合に、X(mm)とX/Lnが演算された。その結果、Xは700.0mm〜52.6mmに小さくなり、X/Lnは1.000〜0.075へと小さくなることが分かった。これらの結果から、指向性投光器を前傾させると、投光レンズの近傍及び遠方における投光距離Lnは急速に投光レンズ側へと接近することが分かった。図5、図6及び表3は、指向性投光器を前傾させたときに、投光距離が短縮化する傾向を数値的に検討したものである。これらの数値計算を踏まえた上で、実際に指向性投光器の前傾実験を以下に行った。 Table 3 uses the numerical values of L 0 (mm), Ln (mm), θ (degrees), and H (mm) to calculate X (mm) and X / Ln according to Equation (8) and Equation (9). The calculation results are shown. When the semi-axial length L0 is fixed to 46.5 mm, Ln = 100 mm and H = 8.8 mm, the forward tilt angle θ is increased to 0 degrees, 0.7 degrees, and 1.34 degrees. (Mm) and X / Ln were calculated. As a result, it was found that X was reduced to 100.0 mm to 58.8 mm, and X / Ln was reduced to 1.000 to 0.588. Further, the behavior at a far point of Ln = 700 mm was examined. X (mm) and X / Ln were calculated when the forward tilt angle θ was increased from 0 to 5 degrees with H = 10 mm fixed. As a result, it was found that X decreased to 700.0 mm to 52.6 mm and X / Ln decreased to 1.000 to 0.075. From these results, it was found that when the directional projector is tilted forward, the projection distance Ln near and at a distance from the projection lens rapidly approaches the projection lens side. FIG. 5, FIG. 6, and Table 3 numerically examine the tendency of the light projection distance to be shortened when the directional projector is tilted forward. Based on these numerical calculations, a forward tilt experiment of a directional projector was actually performed.
図7は、本発明において、指向性投光器の前縁を被清掃面に接触させ、後縁を厚紙で上昇させて前傾させたときの塵埃可視化状態図である。図7に示されるように、指向性投光器4の前縁4bを被清掃面に接地させ、後縁4cの下に紙厚Δhの紙板をn枚積層して厚紙18とし、指向性投光器4を前傾角θで前傾配置させる。傾斜長Cは厚紙18から前縁4bまでの長さを示している。指向性投光器4の中心4aは被清掃面2から高さH(mm)だけ上方の位置にあり、前傾状態にある指向性投光器4の平均の光軸高さに相当する。従って、厚紙厚さをhとすると平均の光軸高さHはH=H0+h/2で与えられる。H0は指向性投光器4の断面半径である。この指向性投光器4においてはC=68mm、Δh=0.40mmであるから、厚紙厚さhはh=n×Δh=0.40n(mm)になる。従って、sin(θ)=nΔh/Cであるから、前傾角θはθ=sin−1(nΔh/C)=sin−1(0.40n/68)で計算される。図7において、被清掃面2の投光領域は投光レンズ6側から塵埃可視化不十分領域(A)、塵埃可視化良好領域(B)、塵埃可視化不十分領域(A)と順次広がっていく。塵埃可視化良好領域(B)の開始端は左側境界Tとなり、その終了端は右側境界Uになる。つまり、左側境界Tの手前側と右側境界Uの遠方側に塵埃可視化不十分領域(A)が存在している。投光レンズ6から左側境界Tまでの投光距離Lは左側境界投光距離Ltと呼ばれ、投光レンズ6から右側境界Uまでの投光距離Lは右側境界投光距離Luと称する。従って、L≦LtとL≧Luの領域は塵埃可視化不十分領域(A)に相当し、Lt≦L≦Luの領域は塵埃可視化良好領域(B)に相当する。塵埃可視化不十分領域(A)からの不十分散乱光15は点線で表示され、塵埃可視化良好領域(B)からの良好散乱光14は実線で表示されている。水平状態及び前傾状態の光軸は符号20で示されている。 FIG. 7 is a dust visualization state diagram when the front edge of the directional projector is brought into contact with the surface to be cleaned and the rear edge is lifted with cardboard and tilted forward in the present invention. As shown in FIG. 7, the front edge 4b of the directional projector 4 is grounded to the surface to be cleaned, and n sheets of paper sheets with a paper thickness Δh are stacked under the rear edge 4c to form the thick paper 18, and the directional projector 4 is A forward tilt is arranged at a forward tilt angle θ. The inclined length C indicates the length from the cardboard 18 to the leading edge 4b. The center 4a of the directional projector 4 is at a position above the surface to be cleaned 2 by a height H (mm), which corresponds to the average optical axis height of the directional projector 4 in the forward tilt state. Therefore, when the thickness of the cardboard is h, the average optical axis height H is given by H = H 0 + h / 2. H 0 is the cross-sectional radius of the directional projector 4. In this directional projector 4, since C = 68 mm and Δh = 0.40 mm, the cardboard thickness h is h = n × Δh = 0.40 n (mm). Therefore, since sin (θ) = nΔh / C, the forward tilt angle θ is calculated as θ = sin −1 (nΔh / C) = sin −1 (0.40 n / 68). In FIG. 7, the light projecting area of the surface to be cleaned 2 sequentially spreads from the light projecting lens 6 side to a dust visualization insufficient area (A), a dust visualization good area (B), and a dust visualization insufficient area (A). The start end of the dust visualization good region (B) is the left boundary T, and the end end is the right boundary U. In other words, the dust visualization insufficient region (A) exists on the near side of the left boundary T and the far side of the right boundary U. The light projection distance L from the light projection lens 6 to the left boundary T is referred to as the left boundary light projection distance Lt, and the light projection distance L from the light projection lens 6 to the right boundary U is referred to as the right boundary light projection distance Lu. Therefore, the region of L ≦ Lt and L ≧ Lu corresponds to the dust visualization insufficient region (A), and the region of Lt ≦ L ≦ Lu corresponds to the dust visualization good region (B). Insufficient scattered light 15 from the dust visualization insufficient region (A) is displayed by a dotted line, and good scattered light 14 from the dust visualization good region (B) is displayed by a solid line. The optical axes in the horizontal state and the forward tilt state are indicated by reference numeral 20.
表4は、第1例の指向性投光器の光軸を被清掃面2に対し前傾角θ(度)だけ前傾させたときの可視化状態の表を示している。表4において、H(mm)は平均の光軸高さであり、θ(度)は前傾角、n枚は厚紙18を構成する紙板の枚数を示している。n=0〜16まで枚数nを変化させると、厚紙厚さhはh(mm)=0〜6.40になり、平均の光軸高さHはH(mm)=8.00〜11.20まで変化する。その結果、前傾角θはθ(度)=0〜5.40まで分布することになる。この条件下で、平均の光軸高さH毎に被清掃面上の塵埃粒子を観察して、投光距離LをL(cm)=0〜50の範囲に亘って塵埃粒子の見え方を判定する。判定基準は4段階で、◎=最も良く見える、○=見える、△=やや見える、×=見えない、である。表4には観察者の肉眼で判定された可視化状態の一覧が与えられている。 Table 4 shows a table of visualization states when the optical axis of the directional projector of the first example is tilted forward by a forward tilt angle θ (degrees) with respect to the surface 2 to be cleaned. In Table 4, H (mm) is the average optical axis height, θ (degrees) is the forward tilt angle, and n is the number of paper plates constituting the thick paper 18. When the number n is changed from n = 0 to 16, the cardboard thickness h becomes h (mm) = 0 to 6.40, and the average optical axis height H is H (mm) = 8.01 to 11.10. Changes to 20. As a result, the forward tilt angle θ is distributed from θ (degrees) = 0 to 5.40. Under these conditions, the dust particles on the surface to be cleaned are observed for each average optical axis height H, and the projection distance L is set in a range of L (cm) = 0 to 50 to determine how the dust particles are seen. judge. Judgment criteria are four stages: ◎ = visible best, ○ = visible, Δ = slightly visible, x = not visible. Table 4 gives a list of visualization states determined with the naked eye of the observer.
表4において、太枠線で示された領域は、各投光距離における最上位にある○印を示している。特定の平均光軸高さHについて考察すると、投光レンズの近傍に位置する○印(左側境界Tに相当する)と遠方に位置する○印(右側境界Uに相当する)の間の領域が塵埃可視化良好領域(B)に相当する。また、近傍に位置する○印(左側境界Tに相当する)より内側の領域は塵埃可視化不十分領域(A)であり、遠方に位置する○印(右側境界Uに相当する)より外側の領域も塵埃可視化不十分領域(A)である。 In Table 4, a region indicated by a thick frame line indicates a mark at the top of each projection distance. Considering a specific average optical axis height H, an area between a circle mark (corresponding to the left boundary T) located in the vicinity of the light projecting lens and a circle mark (corresponding to the right boundary U) located far away is shown. This corresponds to the dust visualization good region (B). Further, the area inside the circle mark (corresponding to the left boundary T) located in the vicinity is the dust visualization insufficient area (A), and the area outside the circle mark (corresponding to the right boundary U) located far away. Is an area (A) where the dust visualization is insufficient.
表5は第1例の指向性投光器における限界前傾角θ0(度)と投光距離L(cm)の一覧表である。表4で示された太枠線だけに着目して、その太枠線の前傾角θ(度)と投光距離L(cm)を一覧化したものである。その太枠線の前傾角θ(度)を限界前傾角θ0(度)と呼び、左側境界Tの投光距離Lを左側境界投光距離Lt(cm)とし、右側境界Uの投光距離Lを右側境界投光距離L(cm)とする。塵埃可視化良好領域(B)の左側境界Tでは、限界前傾角θ0は塵埃粒子が見える状態(○)の最小角を示すから、θ≧θ0の領域では塵埃が良く見える。塵埃可視化良好領域(B)の右側境界Uでは、限界前傾角θ0は塵埃粒子が見える状態(○)の最大角を示すから、θ≦θ0の領域では塵埃が良く見えることになる。 Table 5 is a list of the limit forward tilt angle θ 0 (degrees) and the projection distance L (cm) in the directional projector of the first example. Focusing only on the thick frame lines shown in Table 4, the forward tilt angle θ (degrees) and the projection distance L (cm) of the thick frame lines are listed. The forward tilt angle θ (degrees) of the thick frame line is called the limit forward tilt angle θ 0 (degrees), the projection distance L of the left boundary T is the left boundary projection distance Lt (cm), and the projection distance of the right boundary U is Let L be the right boundary projection distance L (cm). At the left boundary T of the good dust visualization region (B), the limit front tilt angle θ 0 indicates the minimum angle in the state where the dust particles can be seen (◯), and therefore dust can be seen well in the region of θ ≧ θ 0 . At the right boundary U of the dust visualization good region (B), the limit front tilt angle θ 0 indicates the maximum angle of the state where the dust particles can be seen (◯), so that the dust can be seen well in the region of θ ≦ θ 0 .
投光距離L=5、10(cm)の2点からなる左側境界(T)に対し式(10−1)のように最小二乗法により直線回帰する。その直線をθ=c×Lt+dの一次直線とすると、傾きcと切片dとしてc=−0.268及びd=2.68が得られた。従って、左側境界線(T)として式(10)のようにθ(度)=−0.268Lt(cm)+2.68が得られた。投光距離L=25、30、35、40、45、50(cm)の6点からなる右側境界(U)に対し式(11−1)のように最小二乗法により直線回帰する。その直線をθ=e×Lu+fの一次直線とすると、傾きeと切片fとしてe=−0.196及びf=9.72が得られた。従って、右側境界線(U)として式(11)のようにθ(度)=−0.196Lu(cm)+9.72が得られた。 A linear regression is performed by the least square method as shown in Expression (10-1) with respect to the left boundary (T) composed of two points of the projection distance L = 5, 10 (cm). When the straight line was a linear line of θ = c × Lt + d, c = −0.268 and d = 2.68 were obtained as the slope c and the intercept d. Therefore, θ (degrees) = − 0.268 Lt (cm) +2.68 was obtained as the left boundary line (T) as shown in Expression (10). A linear regression is performed by the least square method as shown in Equation (11-1) with respect to the right boundary (U) consisting of six points of the projection distance L = 25, 30, 35, 40, 45, 50 (cm). When the straight line was a linear line of θ = e × Lu + f, e = −0.196 and f = 9.72 were obtained as the slope e and the intercept f. Therefore, θ (degrees) = − 0.196 Lu (cm) +9.72 was obtained as the right boundary line (U) as shown in Expression (11).
図8は、本発明において第1例の指向性投光器を用いた場合に、表5の境界値をプロットして、塵埃可視化良好領域(B)と塵埃可視化不十分領域(A)を示した前傾可視化図である。左側境界Tの2点に対する一次関数(左側境界線T)はθ(度)=−0.268Lt(cm)+2.68となった。右側境界Uの5点に対する一次関数(右側境界線U)はθ(度)=−0.196Lu(cm)+9.724となった。左側境界線Tの左側領域は塵埃可視化不十分領域(A)であり、右側境界線Uの右側領域も塵埃可視化不十分領域(A)である。左側境界線Tと右側境界線Uの間の領域は塵埃可視化良好領域(B)であり、投光距離Lの範囲で示すと、前記塵埃可視化良好領域(B)はLt≦L≦Luで表される。前傾角θが増大すると、Lt≦L≦Luで表される前記塵埃可視化良好領域(B)は次第に投光レンズの方に接近してくることが図8から理解される。このように、左側境界線Tと右側境界線Uの一次関数が数値的に決定されていると、前傾角θに対応するも数値的に決定される。指向性投光器を前傾角θだけ前傾させて、被清掃面上の塵埃粒子を観察者が観察する場合に、数値的に決定されたLt≦L≦Luの範囲に注目して塵埃粒子の存否を確認すれば、被清掃面の汚れ具合を即座に判断することができる利点がある。前記観察者が肉眼の場合には、肉眼を上記範囲に集中して観察すれば良いから、比較的簡単に塵埃粒子の存否を判断できる。但し、人間は被清掃面の全体を瞬時に判断する能力を有しているから、前記範囲、即ちLt≦L≦Luの範囲が事前に分かっていても、その効果は十分ではないと言えるだろう。しかしながら、前記観察者が電子機器の場合には、電子機器では被清掃面の全体を瞬時に判断することは不可能であるから、Lt≦L≦Luの範囲を走査すれば良いという利点は極めて大きい。もしこの範囲が不明な場合、電子機器は投光レンズからかなり遠方まで全ての領域を走査しなければならないから、塵埃粒子の存否確認に長時間を要することになる。本発明では、観察者が肉眼であっても、電子機器であっても、塵埃粒子の存否確認を短時間に完了できる利点がある。 FIG. 8 is a graph showing the dust visualization good region (B) and the dust visualization insufficient region (A) by plotting the boundary values in Table 5 when the directional projector of the first example is used in the present invention. FIG. The linear function (left boundary line T) for the two points on the left boundary T was θ (degrees) = − 0.268 Lt (cm) +2.68. The linear function (right boundary line U) for the five points on the right boundary U was θ (degrees) = − 0.196 Lu (cm) +9.724. The left region of the left boundary line T is a dust visualization insufficient region (A), and the right region of the right boundary line U is also a dust visualization insufficient region (A). A region between the left boundary line T and the right boundary line U is a dust visualization good region (B), and the dust visualization good region (B) is expressed by Lt ≦ L ≦ Lu in the range of the projection distance L. Is done. It can be seen from FIG. 8 that as the forward tilt angle θ increases, the dust visualization good region (B) represented by Lt ≦ L ≦ Lu gradually approaches the light projecting lens. As described above, when the linear function of the left boundary line T and the right boundary line U is numerically determined, the one corresponding to the forward tilt angle θ is also numerically determined. When the directional projector is tilted forward by a forward tilt angle θ and the observer observes dust particles on the surface to be cleaned, the presence or absence of dust particles paying attention to the numerically determined range of Lt ≦ L ≦ Lu If this is confirmed, there is an advantage that the degree of contamination of the surface to be cleaned can be immediately determined. When the observer is unaided, it is only necessary to observe the unaided eye in the above range, so it is possible to determine the presence or absence of dust particles relatively easily. However, since humans have the ability to instantaneously determine the entire surface to be cleaned, even if the range, that is, the range of Lt ≦ L ≦ Lu, is known in advance, the effect is not sufficient. Let's go. However, when the observer is an electronic device, it is impossible to instantaneously determine the entire surface to be cleaned by the electronic device, so that the advantage of scanning the range of Lt ≦ L ≦ Lu is extremely great. large. If this range is unknown, the electronic device must scan the entire region far away from the light projecting lens, so that it takes a long time to check for the presence of dust particles. The present invention has the advantage that confirmation of the presence or absence of dust particles can be completed in a short time regardless of whether the observer is the naked eye or an electronic device.
図8において、左側境界線Tと右側境界線Uの一次関数は既に表5で与えられている。以下には、表5に示された一次関数を最小二乗法により導出する具体的方法が述べられている。
図9は、本発明(第1例)において、図8の左側境界線Tを与える1次関数θ=cLt+dを最小二乗法により推定する境界線推定演算図である。又、図10は、本発明(第1例)において、図8の右側境界線Uを与える1次関数θ=eLu+fを最小二乗法により推定する境界線推定演算図である。
両図において、Xは投光距離L(cm)であり、Yは前傾角θ(度)である。左側境界線Tの傾きcと切片dは式(1)及び式(2)により決定される。同時に、右側境界線Uの傾きeと切片fも式(1)及び式(2)により決定される。両図に記載される表の値は式(1)及び式(2)の演算に必要な諸量を与えている。これらの諸量により式(1)及び式(2)が計算される。その結果、c=−0.268、d=2.68、e=−0.196及びf=9.724が得られる。従って、左側境界線Tは、式(10)により、θ=−0.268Lt+2.68となり、右側境界線Uは、式(11)により、θ=−0.196Lu+9.724となる。左側境界線T及び右側境界線U共に、傾きが負であるから、左上がりの直線であることが分かる。換言すれば、前傾角θが増大するに従って、左側境界投光距離Ltと右側境界投光距離Luは次第に減少することになる。つまり、前傾角が増大するに従って塵埃可視化良好領域(B)は投光レンズ側へ接近することを示す。この接近関係が前述した図8の挙動を説明している。
In FIG. 8, the linear functions of the left boundary line T and the right boundary line U are already given in Table 5. A specific method for deriving the linear function shown in Table 5 by the least square method is described below.
FIG. 9 is a boundary line estimation calculation diagram for estimating the linear function θ = cLt + d that gives the left boundary line T of FIG. 8 by the least square method in the present invention (first example). FIG. 10 is a boundary line estimation calculation diagram for estimating the linear function θ = eLu + f that gives the right boundary line U of FIG. 8 by the least square method in the present invention (first example).
In both figures, X is the projection distance L (cm), and Y is the forward tilt angle θ (degrees). The slope c and the intercept d of the left boundary line T are determined by the equations (1) and (2). At the same time, the slope e and the intercept f of the right boundary line U are also determined by the equations (1) and (2). The values in the tables shown in both figures give various quantities necessary for the calculations of the equations (1) and (2). Equations (1) and (2) are calculated from these quantities. As a result, c = −0.268, d = 2.68, e = −0.196 and f = 9.724 are obtained. Therefore, the left boundary line T is θ = −0.268Lt + 2.68 according to the equation (10), and the right boundary line U is θ = −0.196Lu + 9.724 according to the equation (11). Since both the left boundary line T and the right boundary line U have negative slopes, it can be seen that they are straight lines going up to the left. In other words, as the forward tilt angle θ increases, the left boundary light projection distance Lt and the right boundary light projection distance Lu gradually decrease. That is, as the forward tilt angle increases, the dust visualization good region (B) approaches the light projecting lens side. This approach relation explains the behavior of FIG. 8 described above.
図11は、本発明において、第1例(H0=8mm)の指向性投光器の光軸を被清掃面からH(mm)だけ水平上昇させ、且つ前傾角θだけ前傾させたとき、図4と図8を組み合わせて塵埃可視化良好領域(B)を図式導出する塵埃可視化導出図である。
今、第1例の指向性投光器4の光軸高さHをH=10mmに設定し、その後指向性投光器4の前縁4bをその位置に保持したまま後縁4cを上昇させて指向性投光器4を前傾角θで前傾させる。この状態で塵埃可視化良好領域(B)の左側境界と右側境界の位置を決定する。下記に示す図式決定方法はあくまで近似的方法である。
FIG. 11 is a diagram of the present invention when the optical axis of the directional projector of the first example (H 0 = 8 mm) is horizontally raised by H (mm) from the surface to be cleaned and is tilted forward by a forward tilt angle θ. FIG. 9 is a dust visualization derivation diagram that graphically derives a dust visualization good region (B) by combining FIG. 4 and FIG. 8.
Now, the optical axis height H of the directional projector 4 of the first example is set to H = 10 mm, and then the trailing edge 4c is raised while the front edge 4b of the directional projector 4 is held in that position, thereby the directional projector. 4 is tilted forward at a forward tilt angle θ. In this state, the positions of the left and right boundaries of the dust visualization good region (B) are determined. The schema determination method shown below is only an approximate method.
図8を図4の上に重ね、図8のL軸(θ=0度のX軸に相当)を図4のH=10mmの位置に水平に配置し、θ=0度の左側境界線Tの点を図4の境界線S上に移動する。上記L軸の太矢印で示す領域が、光軸高さH=10mm且つ前傾角θ=0度における塵埃可視化良好領域(10−0B)である。前傾角θを0から増大させてゆくと塵埃可視化良好領域は次第に左上方へと上昇移動してゆく。θ=1度だけ前傾させると、光軸高さH=10mm且つ前傾角θ=1度における塵埃可視化良好領域(10−1B)の太矢印領域に移動する。又、θ=2度だけ前傾させると、光軸高さH=10mm且つ前傾角θ=2度における塵埃可視化良好領域(10−2B)の太矢印領域に移動する。更に、θ=3度だけ前傾させると、光軸高さH=10mm且つ前傾角θ=3度における塵埃可視化良好領域(10−3B)の太矢印領域に移動する。前記太矢印領域を下側に位置する図4(L−H座標)の原点から観測すると、左側境界Tの点の投光距離Lは開始端投光距離Lcになり、右側境界Uの点の投光距離Lは終了端投光距離Leになる。即ち、図示するように、塵埃可視化良好領域(B)の投光距離Lの範囲は、Lc≦L≦Leで与えられることになる。 8 is superimposed on FIG. 4, the L axis (corresponding to the X axis of θ = 0 degree) in FIG. 8 is horizontally arranged at the position of H = 10 mm in FIG. 4, and the left boundary line T of θ = 0 degree. Is moved on the boundary S in FIG. The region indicated by the thick arrow on the L axis is the dust visualization good region (10-0B) at the optical axis height H = 10 mm and the forward tilt angle θ = 0 degrees. When the forward tilt angle θ is increased from 0, the dust visualization good region gradually moves upward to the left. When it is tilted forward by θ = 1 degree, it moves to the thick arrow area of the dust visualization good area (10-1B) at the optical axis height H = 10 mm and the forward tilt angle θ = 1 degree. Further, when tilted forward by θ = 2 degrees, it moves to the thick arrow area of the dust visualization good area (10-2B) at the optical axis height H = 10 mm and the forward tilt angle θ = 2 degrees. Further, when tilted forward by θ = 3 degrees, the optical axis moves to the thick arrow area of the dust visualization good area (10-3B) at the optical axis height H = 10 mm and the forward tilt angle θ = 3 degrees. When the thick arrow region is observed from the origin of FIG. 4 (LH coordinates) located on the lower side, the light projection distance L of the point on the left boundary T becomes the start end light projection distance Lc, and the point of the right boundary U The light projection distance L is the end end light projection distance Le. That is, as shown in the drawing, the range of the projection distance L in the dust visualization good region (B) is given by Lc ≦ L ≦ Le.
図12は、本発明の第1形態において、境界投光距離Lsを用いてL≧Lsにより塵埃可視化良好領域を与える説明図である。図12では、指向性投光器4を被清掃面2の上方に光軸高さHで水平配置した場合において、塵埃可視化良好領域(B)を図式的に推定する方法が描かれている。L−H座標において、斜線は境界線Sであり、その一次関数はH=aLs+bである。光軸高さHで水平線を点線で引くと、境界線Sとの交点がP1となる。点P1のL座標はLsであるから、塵埃可視化良好領域(B)の領域は、式(12−1)によりLs≦Lで与えられる。境界線Sの一次関数が分かっておれば、Ls≦Lの不等式により直ちに塵埃可視化良好領域(B)の領域が導出される。 FIG. 12 is an explanatory diagram for giving a good dust visualization region by L ≧ Ls using the boundary projection distance Ls in the first embodiment of the present invention. FIG. 12 illustrates a method for schematically estimating the dust visualization good region (B) when the directional projector 4 is horizontally disposed above the surface to be cleaned 2 with the optical axis height H. In the LH coordinates, the diagonal line is the boundary line S, and the linear function thereof is H = aLs + b. Pulling the horizontal line by a dotted line in the optical axis height H, the intersection of the boundary line S is P 1. Since the L coordinate of the point P1 is Ls, the region of the dust visualization good region (B) is given by Ls ≦ L by the equation (12-1). If the linear function of the boundary line S is known, the dust visualization good region (B) is immediately derived from the inequality of Ls ≦ L.
図13は、本発明の第2形態又は第3形態において、左側境界投光距離Lt及び右側境界投光距離Luを用いてL≧Lt又はLt≦L≦Luにより塵埃可視化良好領域を与える説明図である。図13では、指向性投光器4の前縁を被清掃面2上に接地させ、その後縁を上昇させて指向性投光器4を前傾角θで前傾させる。このように、前傾角θで前傾配置した場合において、塵埃可視化良好領域(B)を図式的に推定する方法が描かれている。L−θ座標において、塵埃可視化良好領域(B)の左側境界線Tの一次関数はθ=cLt+dであり、右側境界線Uの一次関数はθ=eLu+fで与えられる。縦軸上でθの点から水平に実線を引くと、左側境界線Tとの交点はP2となり、右側境界線Uとの交点はP3となる。点P2と点P3で挟まれる領域が塵埃可視化良好領域(B)である。従って、塵埃可視化良好領域(B)の領域は、Lt≦Lであり、且つL≦Luの範囲である。本発明においては、Ltは左側境界投光距離と呼ばれ、Luは右側境界投光距離と呼ばれる。即ち、塵埃可視化良好領域(B)の領域は、Lt≦L≦Luの不等式で与えられる。本発明の第2形態は式(12−2)で示されるLt≦Lの範囲であり、本発明の第3形態は式(12−3)で示されるLt≦L≦Luの範囲である。左側境界線Tと右側境界線Uの一次関数が分かっておれば、L≦Lu又はLt≦L≦Luの不等式により直ちに塵埃可視化良好領域(B)の領域が導出される。 FIG. 13 is an explanatory diagram for giving a good dust visualization region by L ≧ Lt or Lt ≦ L ≦ Lu using the left boundary projection distance Lt and the right boundary projection distance Lu in the second or third embodiment of the present invention. It is. In FIG. 13, the front edge of the directional projector 4 is grounded on the surface to be cleaned 2, the rear edge is raised, and the directional projector 4 is tilted forward by the forward tilt angle θ. As described above, a method of schematically estimating the dust visualization good region (B) when the forward tilting angle θ is arranged forward is depicted. In the L-θ coordinate, the linear function of the left boundary T of the dust visualization good region (B) is θ = cLt + d, and the linear function of the right boundary U is given by θ = eLu + f. When a solid line is drawn horizontally from the point θ on the vertical axis, the intersection with the left boundary line T is P2, and the intersection with the right boundary line U is P3. A region sandwiched between the points P2 and P3 is a dust visualization good region (B). Therefore, the area | region of a dust visualization favorable area | region (B) is the range of Lt <= L and L <= Lu. In the present invention, Lt is called the left boundary projection distance, and Lu is called the right boundary projection distance. That is, the region of the good dust visualization region (B) is given by an inequality of Lt ≦ L ≦ Lu. The second form of the present invention is a range of Lt ≦ L represented by the formula (12-2), and the third form of the present invention is a range of Lt ≦ L ≦ Lu represented by the formula (12-3). If the linear function of the left boundary line T and the right boundary line U is known, the region of the good dust visualization region (B) is immediately derived from the inequality of L ≦ Lu or Lt ≦ L ≦ Lu.
図14は、本発明の第4形態又は第5形態において、開始端投光距離Lc及び終了端投光距離Leを用いてL≧Lc又はLc≦L≦Leにより塵埃可視化良好領域を与える説明図である。この図14は、図12の上に図13を重ねることにより、指向性投光器を光軸高さHに水平配置して、前傾角θで前傾させた場合における塵埃可視化良好領域(B)の図式的導出方法を説明するものである。指向性投光器4を被清掃面2から光軸高さHだけ上昇させて水平配置した状態が図12で与えられている。この状態で指向性投光器4をその前縁を固定して後縁を上昇させることにより前傾角θで前傾させると、図13のL軸(横軸)を光軸高さHの点P5に合わせ、左側境界線Tの最下点P1を境界線S上に位置するまでθ−L座標(図13)を水平に右側へと移動する。そして、前傾角θに対応する点は、θ軸の前傾角θの点を通るように水平線を引き、点P2〜点P3の領域が光軸高さH及び前傾角θでの塵埃可視化良好領域となる。H軸〜点P2までの距離が開始端投光距離Lcであり、H軸〜点P3までの距離が終了端投光距離Leである。 FIG. 14 is an explanatory diagram for giving a good dust visualization region by L ≧ Lc or Lc ≦ L ≦ Le using the start end projection distance Lc and the end end projection distance Le in the fourth embodiment or the fifth embodiment of the present invention. It is. FIG. 14 shows the dust visualization good region (B) when the directional projector is horizontally arranged at the optical axis height H and tilted forward at the forward tilt angle θ by superimposing FIG. 13 on FIG. A schematic derivation method will be described. FIG. 12 shows a state in which the directional projector 4 is raised horizontally from the surface to be cleaned 2 by the optical axis height H and arranged horizontally. In this state, when the directional projector 4 is tilted forward at a forward tilt angle θ by fixing the leading edge and raising the trailing edge, the L axis (horizontal axis) in FIG. combined, it moves the lowermost point P 1 of the left boundary line T to the theta-L coordinates (Figure 13) horizontally right up to a position on the boundary line S. The point corresponding to the forward tilt angle θ draws a horizontal line so as to pass through the point of the forward tilt angle θ of the θ axis, and the region between the points P 2 to P 3 is the dust visualization at the optical axis height H and the forward tilt angle θ. It becomes a good area. The distance to the H axis to the point P 2 is the starting end projection distance Lc, the distance to the H axis to the point P 3 is an end edge projection distance Le.
図14の式(12−4)〜式(12−10)までの数式によってLcとLeを以下に導出する。指向性投光器4を被清掃面2からHだけ上昇させてθだけ前傾させたときの塵埃可視化良好領域の開始領域は、開始端投光距離がLcであるから、(12−4)によりLc≦Lで与えられる。また、終了端投光距離がLeであるから、塵埃可視化良好領域の全領域は式(12−5)によりLc≦L≦Leで表される。前傾角=0のとき、左側境界線のθ=cLt+dにθ=0を代入すると、式(12−6)によりLt=−d/cが得られる。このLtはP1P4を与えるから、式(12−7)によりP1P4=−d/cになる。従って、式(12−8)によりP4P5=Ls−P1P4であるから、式(12−8)によりP4P5=Ls+d/cが得られる。このP4P5=Ls+d/cを用いると、式(12−9)によりLc=Lt+P4P5であるから、Lc=Lt+Ls+d/cを得ることができる。同様に、式(12−10)によりLe=Lu+P4P5であるから、Le=Lu+Ls+d/cが得られる。
以上のようにH−L座標とθ−L座標を組み合わせると、光軸高さH且つ前傾角θにおける開始端投光距離Lcと終了端投光距離Leが上述のように得られ、その結果塵埃可視化良好領域(Lの領域)がLc≦L、或いはLc≦L≦Leによって簡単に求めることができる。
Lc and Le are derived below using equations (12-4) to (12-10) in FIG. Since the start region of the dust visualization good region when the directional projector 4 is raised from the surface to be cleaned 2 by H and tilted forward by θ, the start end projection distance is Lc, Lc is expressed by (12-4). ≤L. In addition, since the end-end projection distance is Le, the entire region of the dust visualization good region is expressed by Lc ≦ L ≦ Le according to Expression (12-5). When θ = 0 is substituted for θ = cLt + d on the left boundary line when the forward tilt angle = 0, Lt = −d / c is obtained by Expression (12-6). Since this Lt gives P1P4, P 1 P 4 = −d / c according to the equation (12-7). Therefore, since P 4 P 5 = Ls−P 1 P 4 according to the equation (12-8), P 4 P 5 = Ls + d / c is obtained according to the equation (12-8). When this P 4 P 5 = Ls + d / c is used, Lc = Lt + P 4 P 5 is obtained from the equation (12-9), so that Lc = Lt + Ls + d / c can be obtained. Similarly, since Le = Lu + P 4 P 5 according to the equation (12-10), Le = Lu + Ls + d / c is obtained.
As described above, when the HL coordinate and the θ-L coordinate are combined, the start end projection distance Lc and the end end projection distance Le at the optical axis height H and the forward tilt angle θ are obtained as described above. The dust visualization good region (L region) can be easily obtained by Lc ≦ L or Lc ≦ L ≦ Le.
表6は、第2例の指向性投光器を用いた場合に、その光軸をH(mm)だけ水平上昇させたときの可視化状態の表である。第1の指向性投光器では断面半径H0=8mmであるのに対し、第2の指向性投光器では断面半径H=15mmである。断面半径Hを8mmから15mmに増やしても、本発明の要旨が変わらないことを以下に証明してゆく。光軸高さH毎に投光距離L=5、10・・・50(cm)の位置で可視化状態を、最も良く見える(◎)、見える(○)、やや見える(△)、見えない(×)の4段階で肉眼判断した。H0=15mmであるから、H=15.00mm〜21.40mmまでの可視化状態が観察される。その他の条件は表1と同等である。表6において、光軸高さH(mm)の各値毎に、投光距離Lの一番小さな値の位置に出現する○印の枠が太線によって形成されている。これらの太線枠を連ねた境界線が、塵埃可視化不十分領域(A)と塵埃可視化良好領域(B)の境界線S(境界とも言う)になる。即ち、塵埃可視化不十分領域(B)は△印より左側の投光領域(×と△の領域)であり、塵埃可視化良好領域(A)は○印より右側の投光領域(○と◎の領域)である。 Table 6 is a table of the visualization state when the optical axis is horizontally raised by H (mm) when the directional projector of the second example is used. In the first directional projector, the cross-sectional radius H0 = 8 mm, whereas in the second directional projector, the cross-sectional radius H = 15 mm. It will be proved below that the gist of the present invention does not change even when the cross-sectional radius H is increased from 8 mm to 15 mm. Visualization state is best seen (◎), visible (O), somewhat visible (△), invisible at the position of projection distance L = 5, 10 ... 50 (cm) for each optical axis height H ( The visual judgment was made in 4 stages. Since H 0 = 15 mm, a visualization state from H = 15.00 mm to 21.40 mm is observed. Other conditions are the same as in Table 1. In Table 6, for each value of the optical axis height H (mm), a frame marked with a circle that appears at the position of the smallest value of the projection distance L is formed by a thick line. A boundary line connecting these thick line frames is a boundary line S (also referred to as a boundary) between the dust visualization insufficient region (A) and the dust visualization good region (B). That is, the dust visualization insufficient region (B) is a light projection region on the left side of the Δ mark (× and Δ regions), and the dust visualization good region (A) is a light projection region on the right side of the ○ mark (circles of ○ and ◎). Area).
表7は、第2例の指向性投光器について、表6の太枠に対する限界光軸高さHmax(mm)と投光距離L(cm)の座標群の一覧表である。また、表7は前述した表2と実質的に同等であるから、表2で説明した内容をここでは省略する。
これらの座標群に対して最小二乗法を適用し、L=15、20、25、30、35、40(cm)における境界線Sの回帰式を一次関数で導出する。即ち、表7の中で式(13−1)のようにH=aLs+bの一次関数で回帰すると、a=0.256、b=11.29が導出されるから、式(13)は、即ちH(mm)=0.256Ls(cm)+11.29が境界線Sとして得られる。
Table 7 is a list of coordinate groups of the limit optical axis height Hmax (mm) and the projection distance L (cm) with respect to the thick frame in Table 6 for the directional projector of the second example. Since Table 7 is substantially equivalent to Table 2 described above, the contents described in Table 2 are omitted here.
The least square method is applied to these coordinate groups, and the regression equation of the boundary line S at L = 15, 20, 25, 30, 35, and 40 (cm) is derived as a linear function. That is, when regression is performed with a linear function of H = aLs + b as shown in Expression (13-1) in Table 7, a = 0.256 and b = 1.29 are derived. H (mm) = 0.256 Ls (cm) +11.29 is obtained as the boundary line S.
図15は、本発明において断面半径H0=15mmの指向性投光器(第2例)を用いた場合に、表7の境界値をプロットして、表6の塵埃可視化良好領域(B)と塵埃可視化不十分領域(A)を示した水平可視化図である。この図15は前述した第1例の図4と実質的に同等である。
境界線Sより左側は塵埃可視化不十分領域(A)であり、境界線Sより右側は塵埃可視化良好領域(B)である。この図の使用方法は次の通りである。指向性投光器の光軸を被清掃面の上方H(mm)に水平配置したとき、前記Hに対応する境界線S上の投光距離Lが境界投光距離Lsになる。従って、L≦Lsの領域が塵埃可視化不十分領域(A)であり、L≧Lsの領域が塵埃可視化良好領域(B)である。使用する指向性投光器に対応した境界線Sの一次関数が事前に分かっているから、塵埃粒子が明瞭に確認される領域は塵埃可視化良好領域(B)であり、観察者はL≧Lsの領域に注目して塵埃粒子の存否を判断すればよいことになる。観察者が肉眼であるときには、肉眼は被清掃面の全体を瞬時に判断する能力を有しているから、L≧Lsの領域にあえて注目する必要性は少ないであろう。しかし、観察者が電子機器である場合には、電子機器は被清掃面の全体を瞬時に判断する能力を有していないから、L≧Lsの領域に着目して電子機器を操作することにより、塵埃粒子の存否の判断を短時間で行うことが可能になる。もしL≧Lsの情報がない場合には、電子機器はL≧0の全領域を走査しなければならず、0≦L≦Lsの領域を走査する時間が無駄になることは明らかである。従って、L≧Lsの情報を与える図15は電子機器を用いた塵埃粒子の確認走査では画期的であるといえる。この図15が示す上記事項は前述した図4及び図12から得られる事項とほぼ同様である。従って、指向性投光器の第1例で得られた発明内容は第2例でも適用できることが証明された。
FIG. 15 is a graph showing boundary values in Table 7 plotted when the directional projector (second example) having a cross-sectional radius H 0 = 15 mm is used in the present invention. It is the horizontal visualization figure which showed the visualization insufficient area | region (A). FIG. 15 is substantially equivalent to FIG. 4 of the first example described above.
The area on the left side of the boundary line S is a dust visualization insufficient area (A), and the area on the right side of the boundary line S is a dust visualization good area (B). The usage of this figure is as follows. When the optical axis of the directional projector is horizontally arranged above the surface to be cleaned H (mm), the projection distance L on the boundary line S corresponding to the H becomes the boundary projection distance Ls. Therefore, the region of L ≦ Ls is the dust visualization insufficient region (A), and the region of L ≧ Ls is the dust visualization good region (B). Since the linear function of the boundary line S corresponding to the directional projector to be used is known in advance, the region where the dust particles are clearly confirmed is the dust visualization good region (B), and the observer is a region where L ≧ Ls It is sufficient to determine whether dust particles exist by paying attention to the above. When the observer is the naked eye, the naked eye has the ability to instantaneously determine the entire surface to be cleaned, so there is little need to pay attention to the region where L ≧ Ls. However, when the observer is an electronic device, the electronic device does not have the ability to instantaneously determine the entire surface to be cleaned, and therefore, by operating the electronic device while paying attention to the region of L ≧ Ls. In addition, it is possible to determine whether dust particles are present in a short time. If there is no information of L ≧ Ls, the electronic device must scan the entire region of L ≧ 0, and it is clear that the time to scan the region of 0 ≦ L ≦ Ls is wasted. Therefore, it can be said that FIG. 15 which gives information of L ≧ Ls is epoch-making in the confirmation scanning of dust particles using an electronic device. The above items shown in FIG. 15 are substantially the same as the items obtained from FIGS. 4 and 12 described above. Therefore, it was proved that the contents of the invention obtained in the first example of the directional projector can also be applied in the second example.
表8は、第2例の指向性投光器の光軸を被清掃面に対し前傾角θ(度)だけ前傾させたときの可視化状態の一覧表である。換言すれば、図7で示されるように、H0=15mmの指向性投光器4を前傾させて塵埃可視化不十分領域(A)と塵埃可視化良好領域(B)の詳細を表に表したもので、第1例の表4に対応する。指向性投光器4の前縁を被清掃面に接地させた状態で後縁を厚紙で上昇させて指向性投光器4を前傾させる。 Table 8 is a list of visualization states when the optical axis of the directional projector of the second example is tilted forward by a forward tilt angle θ (degrees) with respect to the surface to be cleaned. In other words, as shown in FIG. 7, the directional projector 4 with H 0 = 15 mm is tilted forward and the details of the dust visualization insufficient region (A) and the dust visualization good region (B) are tabulated. This corresponds to Table 4 of the first example. With the front edge of the directional projector 4 in contact with the surface to be cleaned, the rear edge is raised with cardboard to tilt the directional projector 4 forward.
被清掃面から指向性投光器4の中心までの高さが光軸高さHであり、H=15.00mm〜19.80mmまでの9段階で測定され、前傾角θはθ=0.00度〜4.04度まで分布する。各前傾角θにおいて、投光距離L=5cm〜70cmの12点の塵埃粒子の可視化状態が肉眼で判定された。判定基準は、最も良く見える(◎)、見える(○)、やや見える(△)、見えない(×)の4段階である。各前傾角θにおいて、投光距離Lを可変したとき、×と△からなる領域が塵埃可視化不十分領域(A)であり、○と◎からなる領域が塵埃可視化良好領域(B)である。塵埃可視化良好領域(B)の左側境界Tと右側境界Uを示す枠が太線枠として描かれている。従って、投光レンズに近い側から、塵埃可視化不十分領域(A)→塵埃可視化良好領域(B)→塵埃可視化不十分領域(A)のように展開することが分かる。 The height from the surface to be cleaned to the center of the directional projector 4 is the optical axis height H, which is measured in 9 steps from H = 15.00 mm to 19.80 mm, and the forward tilt angle θ is θ = 0.00 degrees. Distributed up to ~ 4.04 degrees. At each forward tilt angle θ, the visibility of 12 dust particles with a projection distance L = 5 cm to 70 cm was determined with the naked eye. The judgment criteria are four stages: best visible (◎), visible ((), slightly visible (Δ), and invisible (x). When the projection distance L is varied at each forward tilt angle θ, the region consisting of x and Δ is the dust visualization insufficient region (A), and the region consisting of ◯ and ◎ is the dust visualization good region (B). A frame indicating the left boundary T and the right boundary U of the dust visualization good region (B) is drawn as a thick line frame. Therefore, it can be seen from the side close to the light projecting lens that the development is as follows: Dust visualization insufficient region (A) → Dust visualization good region (B) → Dust visualization insufficient region (A).
表9は、限界前傾角θ0(度)と投光距離Lの関係を表8から選択して表示したものであり、表8の太線枠に対応したLとθ0の座標群を示している。太枠線の前傾角θ(度)を限界前傾角θ0(度)と呼び、左側境界Tの投光距離Lを左側境界投光距離Lt(cm)とし、右側境界Uの投光距離Lを右側境界投光距離L(cm)とする。塵埃可視化良好領域(B)の左側境界Tでは、限界前傾角θ0は塵埃粒子が見える状態(○)の最小角を示すから、θ≧θ0の領域では塵埃が良く見える。塵埃可視化良好領域(B)の右側境界Uでは、限界前傾角θ0は塵埃粒子が見える状態(○)の最大角を示すから、θ≦θ0の領域では塵埃が良く見えることになる。 Table 9 shows the relationship between the limit forward tilt angle θ 0 (degrees) and the projection distance L selected from Table 8, and shows the coordinate group of L and θ 0 corresponding to the bold frame in Table 8. Yes. The forward tilt angle θ (degrees) of the thick frame line is called the limit forward tilt angle θ 0 (degrees), the light projection distance L of the left boundary T is the left boundary light projection distance Lt (cm), and the light projection distance L of the right boundary U is Is the right boundary projection distance L (cm). At the left boundary T of the good dust visualization region (B), the limit front tilt angle θ 0 indicates the minimum angle in the state where the dust particles can be seen (◯), and therefore dust can be seen well in the region of θ ≧ θ 0 . At the right boundary U of the dust visualization good region (B), the limit front tilt angle θ 0 indicates the maximum angle of the state where the dust particles can be seen (◯), so that the dust can be seen well in the region of θ ≦ θ 0 .
投光距離L=10、15、20(cm)の3点からなる左側境界(T)に対し式(14−1)のように最小二乗法により直線回帰する。その直線をθ=c×Lt+dの一次直線とすると、傾きcと切片dとしてc=−0.101及びd=1.965が得られた。従って、左側境界線(T)として式(14)のようにθ(度)=−0.101Lt(cm)+1.965が得られた。
投光距離L=30、35、40、45、50、60、70(cm)の7点からなる右側境界(U)に対し式(15−1)のように最小二乗法により直線回帰する。その直線をθ=e×Lu+fの一次直線とすると、傾きeと切片fとしてe=−0.097及びf=6.364が得られた。従って、右側境界線(U)として式(15)のようにθ(度)=−0.097Lu(cm)+6.364が得られた。
A linear regression is performed by the least square method as shown in the equation (14-1) with respect to the left boundary (T) including the three projection distances L = 10, 15, 20 (cm). When the straight line is a linear line of θ = c × Lt + d, c = −0.101 and d = 1.965 are obtained as the slope c and the intercept d. Therefore, θ (degrees) = − 0.101 Lt (cm) +1.965 was obtained as the left boundary line (T) as shown in Expression (14).
A linear regression is performed by the least square method as shown in Equation (15-1) with respect to the right boundary (U) consisting of seven points of the projection distance L = 30, 35, 40, 45, 50, 60, 70 (cm). When the straight line was a linear line of θ = e × Lu + f, e = −0.097 and f = 6.364 were obtained as the slope e and the intercept f. Therefore, θ (degrees) = − 0.097Lu (cm) +6.364 was obtained as the right boundary line (U) as shown in Expression (15).
図16は、本発明において第2例の指向性投光器を用いた場合に、表9の境界値をプロットして、塵埃可視化良好領域(B)と塵埃可視化不十分領域(A)を示した前傾可視化図である。この図16は、第1例の指向性投光器に関する図8と実質的に同等であることが以下に示され、本発明の要旨が第2例に対しても成立することが証明される。左側境界Tの3点に対する一次関数(左側境界線T)はθ(度)=−0.101Lt(cm)+1.965となった。右側境界Uの7点に対する一次関数(右側境界線U)はθ(度)=−0.097Lu(cm)+6.364となった。左側境界線Tの左側領域は塵埃可視化不十分領域(A)であり、右側境界線Uの右側領域も塵埃可視化不十分領域(A)である。左側境界線Tと右側境界線Uの間の領域は塵埃可視化良好領域(B)であり、投光距離Lの範囲で示すと、前記塵埃可視化良好領域(B)はLt≦L≦Luで表される。前傾角θが増大すると、Lt≦L≦Luで表される前記塵埃可視化良好領域(B)は次第に投光レンズの方に接近してくることが図16から理解される。
このように、左側境界線Tと右側境界線Uの一次関数が数値的に決定されていると、次のような利点がある。指向性投光器を前傾角θだけ前傾させて、被清掃面上の塵埃粒子を観察者が観察する場合に、数値的に決定されたLt≦L≦Luの範囲に注目して塵埃粒子の存否を確認すれば、被清掃面の汚れ具合を即座に判断することができる。前記観察者が肉眼の場合には、肉眼を上記範囲に集中して観察すれば良いから、比較的簡単に塵埃粒子の存否を判断できる。但し、人間は被清掃面の全体を瞬時に判断する能力を有しているから、前記範囲、即ちLt≦L≦Luの範囲が事前に分かっていても、その効果は十分ではないと言えるだろう。しかしながら、前記観察者が電子機器の場合には、電子機器では被清掃面の全体を瞬時に判断することは不可能であるから、Lt≦L≦Luの範囲を走査すれば良いという利点は極めて大きい。もしこの範囲が不明な場合、電子機器は投光レンズからかなり遠方まで全ての領域を走査しなければならないから、塵埃粒子の存否確認に長時間を要することになる。本発明では、観察者が肉眼であっても、電子機器であっても、塵埃粒子の存否確認を短時間に完了できる利点がある。
FIG. 16 is a graph showing the dust visualization good region (B) and the dust visualization insufficient region (A) by plotting the boundary values in Table 9 when the directional projector of the second example is used in the present invention. FIG. This FIG. 16 is shown below to be substantially equivalent to FIG. 8 relating to the directional projector of the first example, and it is proved that the gist of the present invention is also valid for the second example. The linear function (left boundary line T) for the three points on the left boundary T was θ (degrees) = − 0.101 Lt (cm) +1.965. The linear function (right boundary line U) for 7 points on the right boundary U was θ (degrees) = − 0.097 Lu (cm) +6.364. The left region of the left boundary line T is a dust visualization insufficient region (A), and the right region of the right boundary line U is also a dust visualization insufficient region (A). A region between the left boundary line T and the right boundary line U is a dust visualization good region (B), and the dust visualization good region (B) is expressed by Lt ≦ L ≦ Lu in the range of the projection distance L. Is done. It can be understood from FIG. 16 that when the forward tilt angle θ increases, the dust visualization good region (B) represented by Lt ≦ L ≦ Lu gradually approaches the light projecting lens.
Thus, if the linear function of the left boundary line T and the right boundary line U is determined numerically, the following advantages are obtained. When the directional projector is tilted forward by a forward tilt angle θ and the observer observes dust particles on the surface to be cleaned, the presence or absence of dust particles paying attention to the numerically determined range of Lt ≦ L ≦ Lu If it is confirmed, it is possible to immediately determine the degree of contamination of the surface to be cleaned. When the observer is unaided, it is only necessary to observe the unaided eye in the above range, so it is possible to determine the presence or absence of dust particles relatively easily. However, since humans have the ability to instantaneously determine the entire surface to be cleaned, even if the range, that is, the range of Lt ≦ L ≦ Lu, is known in advance, the effect is not sufficient. Let's go. However, when the observer is an electronic device, it is impossible to instantaneously determine the entire surface to be cleaned by the electronic device, so that the advantage of scanning the range of Lt ≦ L ≦ Lu is extremely great. large. If this range is unknown, the electronic device must scan the entire region far away from the light projecting lens, so that it takes a long time to check for the presence of dust particles. The present invention has the advantage that confirmation of the presence or absence of dust particles can be completed in a short time regardless of whether the observer is the naked eye or an electronic device.
図17は、本発明において、第2例(H0=15mm)の指向性投光器の光軸を被清掃面からH(mm)だけ水平上昇させ、且つ前傾角θだけ前傾させたとき、図15と図16を組み合わせて塵埃可視化良好領域(B)を図式導出する塵埃可視化導出図である。この図17は第1例の指向性投光器を用いた場合の重ね図、即ち図11と実質的に同等であり、この重ね合わせ導出方法が指向性投光器の全般に対して成立することを実証している。以下に図17の詳細を説明する。 FIG. 17 is a diagram showing a state in which the optical axis of the directional projector of the second example (H 0 = 15 mm) is horizontally raised by H (mm) from the surface to be cleaned and is tilted forward by a forward tilt angle θ in the present invention. FIG. 17 is a dust visualization derivation diagram that graphically derives a dust visualization good region (B) by combining 15 and FIG. 16. FIG. 17 is an overlap diagram in the case where the directional projector of the first example is used, that is, substantially equivalent to FIG. 11, and it has been demonstrated that this overlay derivation method is valid for the entire directional projector. ing. Details of FIG. 17 will be described below.
今、第2例の指向性投光器4の光軸高さHをH=20mmに設定し、その後指向性投光器4の前縁4bをその位置に保持したまま後縁4cを上昇させて指向性投光器4を前傾角θで前傾させる。この状態で塵埃可視化良好領域(B)の左側境界と右側境界の位置を決定する。下記に示す図式決定方法はあくまで近似的方法である。
図16を図15の上に重ね、図16のL軸(θ=0度のX軸に相当)を図15のH=20mmの位置に水平に配置し、θ=0度の左側境界線Tの点を図15の境界線S上に移動する。上記L軸の太矢印で示す領域が、光軸高さH=20mm且つ前傾角θ=0度における塵埃可視化良好領域(20−0B)である。前傾角θを0から増大させてゆくと塵埃可視化良好領域は次第に左上方へと上昇移動してゆく。θ=1度だけ前傾させると、光軸高さH=20mm且つ前傾角θ=1度における塵埃可視化良好領域(20−1B)の太矢印領域に移動する。又、θ=2度だけ前傾させると、光軸高さH=20mm且つ前傾角θ=2度における塵埃可視化良好領域(20−2B)の太矢印領域に移動する。図中には示さないが、前傾角θを更に増大させると塵埃可視化良好領域は更に左上方へと上昇することは言うまでもない。前記太矢印領域を下側に位置する図15(L−H座標)の原点から観測すると、左側境界Tの点の投光距離Lは開始端投光距離Lcになり、右側境界Uの点の投光距離Lは終了端投光距離Leになる。即ち、図示するように、塵埃可視化良好領域(B)の投光距離Lの範囲は、Lc≦L≦Leで与えられることになる。
Now, the optical axis height H of the directional projector 4 of the second example is set to H = 20 mm, and then the trailing edge 4c is lifted while the front edge 4b of the directional projector 4 is held in that position, so that the directional projector 4 is tilted forward at a forward tilt angle θ. In this state, the positions of the left and right boundaries of the dust visualization good region (B) are determined. The schema determination method shown below is only an approximate method.
FIG. 16 is superimposed on FIG. 15, the L axis (corresponding to the X axis of θ = 0 degree) in FIG. 16 is horizontally arranged at the position of H = 20 mm in FIG. 15, and the left boundary line T of θ = 0 degree. Is moved on the boundary line S in FIG. The region indicated by the thick arrow on the L axis is the dust visualization good region (20-0B) at the optical axis height H = 20 mm and the forward tilt angle θ = 0 degree. When the forward tilt angle θ is increased from 0, the dust visualization good region gradually moves upward to the left. When it is tilted forward by θ = 1 degree, it moves to the thick arrow area of the dust visualization good area (20-1B) at the optical axis height H = 20 mm and the forward tilt angle θ = 1 degree. Further, when tilted forward by θ = 2 degrees, it moves to the thick arrow area of the dust visualization good area (20-2B) at the optical axis height H = 20 mm and the forward tilt angle θ = 2 degrees. Although not shown in the drawing, it goes without saying that when the forward tilt angle θ is further increased, the dust visualization good region further rises to the upper left. When the thick arrow region is observed from the origin in FIG. 15 (LH coordinates) located on the lower side, the light projection distance L of the point on the left boundary T becomes the start end light projection distance Lc, and the point on the right boundary U The light projection distance L is the end end light projection distance Le. That is, as shown in the drawing, the range of the projection distance L in the dust visualization good region (B) is given by Lc ≦ L ≦ Le.
指向性投光器4を第1例から第2例に変更しても、塵埃可視化良好領域(B)の左側境界線Tと右側境界線Uを一次関数により近似的に導出し、前記塵埃可視化良好領域(B)の左側境界と右側境界を理論的且つ数値的に導出するという本発明の要旨は不変に成立することが実証された。従って、本発明の上記要旨は多くの指向性投光器に対して適用できることが分かった。
本発明の要旨の詳細は、図12、図13及び図14に明示されており、これらの図式導出法が本発明の特許請求の範囲に明記されている。
Even if the directional projector 4 is changed from the first example to the second example, the left boundary line T and the right boundary line U of the dust visualization good region (B) are approximately derived by a linear function, and the dust visualization good region It was proved that the gist of the present invention of theoretically and numerically deriving the left boundary and the right boundary in (B) was established unchanged. Therefore, it has been found that the above gist of the present invention can be applied to many directional projectors.
Details of the subject matter of the present invention are set forth in FIGS. 12, 13 and 14, and these graphical derivations are specified in the claims of the present invention.
以上詳述したように、本発明では、被清掃面の塵埃粒子の観察動作と清掃作業を分離する。まず、条件を試験的に導出する為に特定の被清掃面(特定被清掃面と称する)を選び出し、この特定被清掃面上で塵埃粒子を明瞭に観察できる条件を実験的且つ理論的に導出する。次に、実際に清掃しようとする被清掃面に前記条件を適用し、この被清掃面上に指向性投光器により光照射して塵埃粒子がどの程度存在するかを観察する。更に、塵埃粒子が所定量以上存在すれば、この被清掃面をモップや電機掃除機などの清掃手段を用いて清掃すればよい。もし塵埃粒子が所定量以下であれば、清掃作業を行う必要がないと判断できる。
従って、本発明が利用できる産業分野は、家庭・会社・ホテル等の施設、清掃業、モップや電機掃除機などの製造業、清掃用具の販売業・レンタル業、衛生設備業、その他関連産業である。
As described above in detail, in the present invention, the observation operation of the dust particles on the surface to be cleaned is separated from the cleaning operation. First, a specific surface to be cleaned (referred to as a specific surface to be cleaned) is selected in order to derive the conditions on a trial basis, and the conditions under which dust particles can be clearly observed on this specific surface to be cleaned are experimentally and theoretically derived. To do. Next, the above condition is applied to the surface to be cleaned which is actually cleaned, and light is irradiated onto the surface to be cleaned by a directional projector to observe how much dust particles are present. Furthermore, if dust particles are present in a predetermined amount or more, the surface to be cleaned may be cleaned using a cleaning means such as a mop or an electric vacuum cleaner. If the amount of dust particles is less than a predetermined amount, it can be determined that there is no need to perform a cleaning operation.
Therefore, the industrial fields in which the present invention can be used include households, companies, hotels, etc., cleaning industries, manufacturing industries such as mops and electric vacuum cleaners, cleaning tool sales / rentals, sanitary equipment, and other related industries. is there.
2 被清掃面
4 指向性投光器
4a 指向性投光器の中心
4b 前縁
4c 後縁
6 投光レンズ
8 光コーン
10 光コーン断面
12 塵埃粒子
14 良好散乱光
15 不十分散乱光
16 観察者
18 厚紙
20 光軸
A 塵埃可視化不十分領域
B 塵埃可視化良好領域
C 傾斜長
H 光軸高さ
H0 指向性投光器の断面半径
Hmax 限界光軸高さ
L 投光距離
Ls 境界投光距離
Lt 左側境界投光距離
Lu 右側境界投光距離
Lc 開始端投光距離
Le 終了端投光距離
Ln 投光距離
L0 半軸長
S 境界
T 左側境界
U 右側境界
a 境界線Sの傾き
b 境界線Sの切片
c 左側境界線Tの傾き
d 左側境界線Tの切片
e 右側境界線Uの傾き
f 右側境界線Uの切片
h 厚紙厚さ
Δh 紙板厚さ
n 紙板の枚数
x 前傾投光距離
α 投光角度
θ 前傾角
H=aLs+b 境界線Sの1次関数
θ=cLt+d 左側境界線Tの1次関数
θ=eLu+f 右側境界線Uの1次関数
2 Surface to be cleaned 4 Directional projector 4a Center of directional projector 4b Front edge 4c Rear edge 6 Projection lens 8 Light cone 10 Light cone cross section 12 Dust particle 14 Good scattered light 15 Insufficient scattered light 16 Observer 18 Cardboard 20 Light Axis A Dust visualization insufficient area B Dust visualization good area C Inclination length H Optical axis height H 0 Cross-sectional radius of directional projector Hmax Limit optical axis height L Projection distance Ls Boundary projection distance Lt Left boundary projection distance Lu Right boundary floodlight distance Lc Start edge floodlight distance Le End edge floodlight distance Ln Floodlight distance L 0 Half axis length S Boundary T Left boundary U Right boundary a Boundary S slope b Boundary S intercept c Left boundary Inclination of T d Intersection of left boundary T e Inclination of right boundary U f Intersection of right boundary U h Thick paper thickness Δh Thickness of paper board n Number of paper boards x Forward tilt projection distance α Projection angle θ Forward tilt angle H = ALs + b Linear function of boundary line S = cLt + d Linear function of left boundary line T = eLu + f Linear function of right boundary line U
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| US9907336B2 (en) | 2005-03-29 | 2018-03-06 | British American Tobacco (Investments) Limited | Porous carbon materials and smoking articles and smoke filters therefor incorporating such materials |
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