JP2009178818A - Tool position measuring method and device - Google Patents
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- 238000005520 cutting process Methods 0.000 claims description 25
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Abstract
Description
この発明は、いわゆるマイクロエンドミル等の微小工具の位置を非接触で検出する工具位置測定方法と装置に関する。 The present invention relates to a tool position measuring method and apparatus for detecting the position of a micro tool such as a so-called micro end mill in a non-contact manner.
従来、マイクロレンズアレイなどの光学部品の金型や、マイクロ流体機械の切削加工には、直径φ=0.01mm〜0.2mm程度のマイクロエンドミル等の微小な工具を用いることが多い。このような工具を使用する際、高精度な加工を行うために、工具と被削材との距離を正確に測定しなければならない。 Conventionally, a micro tool such as a micro end mill having a diameter φ of about 0.01 mm to 0.2 mm is often used for a mold of an optical component such as a micro lens array or a cutting process of a micro fluid machine. When such a tool is used, the distance between the tool and the work material must be accurately measured in order to perform highly accurate machining.
工具位置の検出には種々の方法があり、一般的には特許文献1に開示されているように、工具に接触する摺動体を設けて、工具への接触を電気的に検知して、工具位置の検出を行っている。また、特許文献2に開示されているように透過型レーザ測定装置と電気マイクロメータ、及び顕微鏡等を用いて工具の測定を行う装置もある。その他、特許文献3に開示されているように、CCDカメラにより工具先端を撮像して、工具の位置合わせを行う方法もある。 There are various methods for detecting the tool position. Generally, as disclosed in Patent Document 1, a sliding body that contacts the tool is provided, and contact with the tool is electrically detected to detect the tool position. The position is detected. In addition, as disclosed in Patent Document 2, there is also a device that measures a tool using a transmission laser measurement device, an electric micrometer, a microscope, and the like. In addition, as disclosed in Patent Document 3, there is also a method of aligning the tool by imaging the tip of the tool with a CCD camera.
また、非特許文献1に開示されているように、レーザ光の回折を利用して微小工具の測定を行う方法も提案されている。 In addition, as disclosed in Non-Patent Document 1, a method for measuring a micro tool using diffraction of laser light has been proposed.
特許文献1に開示されている接触式の工具位置測定装置では、現実的には被削材に対して0.3N程度の測定力が加わり、極小径の工具の場合、切れ刃を破損することがしばしばある。また、特許文献2に開示されたような非接触式の工具位置測定装置のレーザ光透過方式の場合、工具刃先形状の違いによる測定誤差があるという問題があった。さらに、CCDカメラ方式では、工具刃先とベッド面の距離を直接測定することができず、タッチセンサを介する必要があるため、それに起因する誤差要因が増える。 In the contact-type tool position measuring device disclosed in Patent Document 1, in reality, a measuring force of about 0.3 N is applied to the work material, and in the case of a very small diameter tool, the cutting edge is damaged. There are often. In addition, in the case of the laser beam transmission method of the non-contact type tool position measuring device as disclosed in Patent Document 2, there is a problem that there is a measurement error due to a difference in the tool edge shape. Further, in the CCD camera system, the distance between the tool blade edge and the bed surface cannot be directly measured, and it is necessary to use a touch sensor, so that an error factor resulting therefrom increases.
また、非特許文献1に開示されたレーザ光回折方式では、測定対象が工具とナイフエッジであり、工具と被削材ではない。さらに、それらのすき間は、数十μmのオーダーになるため、それ以下の精度で工具位置を検出することはできず、マイクロエンドミル等の微小工具の位置を正確に検出することができないものである。 In the laser beam diffraction method disclosed in Non-Patent Document 1, the measurement object is a tool and a knife edge, not a tool and a work material. Furthermore, since the clearances are on the order of several tens of μm, the position of the tool cannot be detected with less accuracy, and the position of a micro tool such as a micro end mill cannot be accurately detected. .
この発明は、上記背景技術に鑑みて成されたもので、マイクロエンドミル等の微小工具の位置を、非接触で繰り返し精度が高く、工具刃先形状の違いによる測定誤差を受けにくく、工具刃先と被削材の位置を直接測定可能な工具位置測定方法と装置を提供することを目的とする。 The present invention has been made in view of the above-mentioned background art. The position of a micro tool such as a micro end mill is non-contact, has high repeatability, is less susceptible to measurement errors due to the difference in the shape of the tool edge, and the tool edge and the object to be covered. An object of the present invention is to provide a tool position measuring method and apparatus capable of directly measuring the position of a work material.
本発明の方法では、工具刃先と被削材の接近を側面から直接観察し、そこを通過する光強度が隙間の二乗に比例することを利用して、それらの位置を高い繰り返し精度で検出できることを特徴とする。 In the method of the present invention, the approach of the tool edge and the work material can be observed directly from the side surface, and the light intensity passing through the tool edge can be detected with high repetition accuracy by utilizing the fact that the light intensity passing therethrough is proportional to the square of the gap. It is characterized by.
この発明は、マイクロエンドミル等の刃先を有する切削加工用の工具と被削材との間隔を非接触で測定する工具位置測定方法であって、前記工具と被削材との隙間をインコヒーレントな光により照明して、前記工具と被削材及びその隙間を撮像して前記工具と被削材との間隙の光強度を測定し、前記工具を前記被削材に近づけて行くに従い、前記光強度が減少するような前記工具と被削材との間隙の領域で、前記光強度の測定値を基に前記被削材に対する前記工具の位置を測定する工具位置測定方法である。 The present invention relates to a tool position measuring method for measuring the distance between a cutting tool having a cutting edge, such as a micro end mill, and a work material in a non-contact manner, wherein the gap between the tool and the work material is incoherent. Illuminate with light, take an image of the tool and the work material and the gap between them, measure the light intensity of the gap between the tool and the work material, and as the tool approaches the work material, the light In the tool position measuring method, the position of the tool with respect to the work material is measured based on the measurement value of the light intensity in the region of the gap between the tool and the work material where the strength decreases.
またこの発明は、刃先を有する切削加工用の工具と被削材との間隔を非接触により測定する工具位置測定装置において、前記工具と被削材との隙間を照明可能なインコヒーレントな光源と、前記光源により照明された前記工具と被削材及びその隙間を撮像する撮像装置と、前記工具と前記被削材の距離により前記光強度が変化するような前記工具と被削材との間隙の領域で、前記光強度の測定値を基に前記被削材に対する前記工具の位置を測定する演算手段を備えた工具位置測定装置である。 Further, the present invention provides an incoherent light source capable of illuminating a gap between the tool and the work material in a tool position measuring device that measures the distance between the cutting tool having a cutting edge and the work material in a non-contact manner. An imaging device that images the tool illuminated by the light source, the work material, and a gap between the tool, and a gap between the tool and the work material such that the light intensity varies depending on the distance between the tool and the work material. In this region, the tool position measuring device includes a calculation means for measuring the position of the tool relative to the work material based on the measured value of the light intensity.
前記演算手段は、前記工具と前記被削材の距離により前記光強度が変化する領域の光強度と前記距離の対応を記憶し、前記光強度により前記距離を出力するコンピュータである。 The computing means is a computer that stores the correspondence between the light intensity and the distance in a region where the light intensity varies depending on the distance between the tool and the work material, and outputs the distance based on the light intensity.
この発明の工具位置測定方法と装置によれば、マイクロエンドミル等の微小工具の位置を、非接触で繰り返し精度が高い測定が可能であるとともに、工具刃先形状の違いによる測定誤差を受けにくいものであり、工具刃先と被削材の位置を直接高精度に検出することができる。また、コヒーレントなレーザ光の回折を利用すると、干渉性が高いためにスペックルノイズが発生するが、この発明では、インコヒーレントな光の回折を利用して、工具と被削材の隙間の画像を撮像することにより、スペックルノイズの問題もない。さらに、光源としては、レーザ光源と比較して安価なLEDやその他の一般的な光源を利用することができ、装置全体としても安価なものとなる。 According to the tool position measuring method and apparatus of the present invention, it is possible to measure the position of a micro tool such as a micro end mill in a non-contact and highly accurate manner, and is less susceptible to measurement errors due to differences in the tool edge shape. Yes, the position of the tool edge and the work material can be directly detected with high accuracy. In addition, when coherent laser light diffraction is used, speckle noise is generated due to high coherence, but in this invention, an image of the gap between the tool and the work material is used by using incoherent light diffraction. Therefore, there is no problem of speckle noise. Further, as the light source, an inexpensive LED or other general light source can be used as compared with the laser light source, and the entire apparatus is also inexpensive.
以下、この発明の工具欠陥検査装置の一実施形態について、図1、図2を基にして説明する。この実施形態の工具位置測定装置10は、図1に示すように、マイクロエンドミルである工具12とそのチャック部14を有し、チャック部14は図示しない加工機の主軸に連結されるものであるが、この実施形態では実験用に取り付け台16に固定されている。取り付け台16は、位置決め用のXYステージ18に固定され、XYステージ18には、水平方向であるXY軸方向にXYステージ18を位置合わせ可能なピエゾアクチュエータ20が設けられている。 Hereinafter, an embodiment of a tool defect inspection apparatus according to the present invention will be described with reference to FIGS. As shown in FIG. 1, the tool position measuring apparatus 10 of this embodiment includes a tool 12 that is a micro end mill and a chuck portion 14 thereof, and the chuck portion 14 is connected to a spindle of a processing machine (not shown). However, in this embodiment, it is fixed to the mount 16 for experiment. The mounting base 16 is fixed to an XY stage 18 for positioning, and the XY stage 18 is provided with a piezo actuator 20 capable of aligning the XY stage 18 in the horizontal XY axis direction.
工具12の先端側には、加工が施される被削材22が対向して位置している。工具12の側方には、図示しないハロゲンランプ等のインコヒーレントな光の光源に接続された光ファイバ24を備え、光ファイバ24からの光の出射端には、所定波長の光を通過させるバンドパスフィルタ26、及び工具12の側方に集光用のコンデンサーレンズ28が設けられている。バンドパスフィルタ26は、例えば波長450nmの光を通過させるものである。 On the tip side of the tool 12, a work material 22 to be machined is positioned so as to face. A side of the tool 12 is provided with an optical fiber 24 connected to a light source of incoherent light such as a halogen lamp (not shown), and a band through which light of a predetermined wavelength passes at an emission end of the light from the optical fiber 24. A condenser lens 28 for condensing light is provided on the side of the pass filter 26 and the tool 12. The band pass filter 26 allows light having a wavelength of, for example, 450 nm to pass therethrough.
工具12を挟んで反対側には、対物レンズ30と結像レンズ31が設けられている。さらに、工具12の先端部を拡大して撮影する対物レンズ30と、工具12の像を撮像するCCD等の撮像素子を内蔵したカメラ32が設けられ、カメラ32の撮像データの出力はコンピュータ等の記憶装置に出力される。 An objective lens 30 and an imaging lens 31 are provided on the opposite side of the tool 12. In addition, an objective lens 30 that captures an enlarged image of the tip of the tool 12 and a camera 32 that incorporates an image sensor such as a CCD that captures an image of the tool 12 are provided. It is output to the storage device.
この実施形態の工具欠陥検査装置10は、光源から光ファイバ24で導かれたインコヒーレントな光が、バンドパスフィルタ26を通り、コンデンサーレンズ28により集光され、被削材22と工具12の刃先の隙間を通過する。被削材22と工具12の刃先の隙間を通過した光は、対物レンズ30と結像レンズ31を介して、カメラ32の撮像素子に結像される。撮像素子から得られた画像情報は、画像入力ボードを経由してコンピュータに取り込まれ、光強度の測定が行われる。 In the tool defect inspection apparatus 10 of this embodiment, the incoherent light guided from the light source by the optical fiber 24 passes through the bandpass filter 26 and is condensed by the condenser lens 28, and the work material 22 and the cutting edge of the tool 12 are collected. Pass through the gap. The light that has passed through the gap between the work material 22 and the cutting edge of the tool 12 is imaged on the image sensor of the camera 32 via the objective lens 30 and the imaging lens 31. Image information obtained from the image sensor is taken into a computer via an image input board, and light intensity is measured.
なお、この実施形態では、取り付け台16に、工具12の軸方向の位置を測定するための電気式マイクロメータ34の検知部が接触している。これにより、XYステージ18に取り付けられたピエゾアクチュエータ18により、工具12が被削材22に対して進退すると、その変位量を電気マイクロメータ34により測定される。 In this embodiment, the detector 16 of the electric micrometer 34 for measuring the position of the tool 12 in the axial direction is in contact with the mounting base 16. Thereby, when the tool 12 advances and retreats with respect to the work material 22 by the piezo actuator 18 attached to the XY stage 18, the displacement amount is measured by the electric micrometer 34.
次に、この発明における工具12と被削材22との距離の測定方法について説明する。ここでは、工具12の刃先と被削材22の隙間をスリットに見立て、図2に示すようにインコヒーレントな光源・レンズ・結像面が位置している場合、工具12の刃先と被削材22との距離wと、結像面中央でのフランホーファー回折による光強度との関係を求める。 Next, a method for measuring the distance between the tool 12 and the work material 22 in the present invention will be described. Here, the gap between the cutting edge of the tool 12 and the work material 22 is regarded as a slit, and when the incoherent light source / lens / imaging surface is located as shown in FIG. 2, the cutting edge of the tool 12 and the work material The relationship between the distance w to 22 and the light intensity by Franhofer diffraction at the center of the image plane is obtained.
ここで、物体面での座標系をξ、結像面での座標系をxのそれぞれを一次元と考える。また、物体面から結像面までの距離をL、物体面での光の複素振幅をu0、結像面での光の複素振幅をu1、光源の波数をkとすると、結像面での光強度分布I1(x)は、
さらに、結像面中央(x=0)での光強度は、sinc(wX)=1から、
上述の原理により、工具12の刃先が被削材22に接近した際に、その隙間の光強度を測定することにより、隙間の距離に対して急激に光強度が減少することを利用して、繰り返し精度の高い工具位置測定が可能となる。 Based on the principle described above, when the cutting edge of the tool 12 approaches the work material 22, by measuring the light intensity of the gap, the light intensity rapidly decreases with respect to the distance of the gap, Tool position measurement with high repeatability is possible.
図3に、この発明の実施形態において、R=0.05mmのボールエンドミルが被削材22に近接している画像を示す。この時の工具12の中心での光強度を図4に示す。工具12の刃先と被削材22の隙間が十分開いているときの最大光強度を1として、隙間からの光強度を正規化して表している。以降、正規化された光強度を単に光強度と呼ぶことにし、単位を無次元化して表す。矢印の1から6の破線で示した各光強度分布は、工具12の刃先が被削材22に近づく際の光強度分布を模式的に表したものである。図4の光強度分布の破線の左側のみが移動しているのは、工具12の刃先側のみが移動していることを示している。また、図3の工具12の刃先と被削材22の距離での光強度分布は、図4の矢印4が指示する実線に対応する。 FIG. 3 shows an image in which the ball end mill with R = 0.05 mm is close to the work material 22 in the embodiment of the present invention. The light intensity at the center of the tool 12 at this time is shown in FIG. The maximum light intensity when the gap between the cutting edge of the tool 12 and the work material 22 is sufficiently open is set to 1, and the light intensity from the gap is normalized. Hereinafter, the normalized light intensity is simply referred to as light intensity, and the unit is expressed in a dimensionless manner. Each light intensity distribution indicated by broken lines 1 to 6 of the arrows schematically represents the light intensity distribution when the cutting edge of the tool 12 approaches the work material 22. Only the left side of the broken line in the light intensity distribution in FIG. 4 is moving indicates that only the cutting edge side of the tool 12 is moving. The light intensity distribution at the distance between the cutting edge of the tool 12 and the work material 22 in FIG. 3 corresponds to the solid line indicated by the arrow 4 in FIG.
以上述べたように、この実施形態の工具位置測定方法と装置によれば、図4に示す矢印4の位置から矢印5,6の位置への変化を検知して、比較的簡単で安価な装置で光学的に非接触で、直接的に工具12の刃先の位置を検出することができる。 As described above, according to the tool position measuring method and apparatus of this embodiment, it is possible to detect a change from the position of arrow 4 to the positions of arrows 5 and 6 shown in FIG. Thus, the position of the blade edge of the tool 12 can be directly detected without optical contact.
次に、この発明の工具位置測定方法と装置による工具位置の検出についての実験結果を説明する。ここでは、表1に示す2種類の工具を用い、図5に定義する3方向について実験を行った。観察される工具刃先の像を図6に示す。 Next, the experimental result about the detection of the tool position by the tool position measuring method and apparatus of this invention is demonstrated. Here, two types of tools shown in Table 1 were used, and experiments were performed in three directions defined in FIG. An image of the observed tool edge is shown in FIG.
上記実施形態で説明した理論的なスリット形状での光強度の変化について、ナイフエッジおよび表1の工具刃先と、被削材とのスリット形状の違いによる光強度の変化を測定した。まず、上述の実施形態の方法で、工具刃先と被削材の接触位置を推定し、その位置から、徐々に工具刃先を被削材から遠ざけ、その際の光強度を測定する。得られた光強度曲線を図7〜図9に示す。図の横軸は工具刃先と被削材の距離を示し、縦軸は正規化された光強度を示す。得られた曲線を、図7〜図9のように、それぞれA、B、C領域に分けて定義する。 Regarding the change in the light intensity in the theoretical slit shape described in the above embodiment, the change in the light intensity due to the difference in the slit shape between the knife edge and the tool blade edge in Table 1 and the work material was measured. First, the contact position between the tool edge and the work material is estimated by the method of the above-described embodiment, and the tool edge is gradually moved away from the work material from that position, and the light intensity at that time is measured. The obtained light intensity curves are shown in FIGS. The horizontal axis in the figure indicates the distance between the tool blade edge and the work material, and the vertical axis indicates the normalized light intensity. The obtained curves are defined by dividing them into A, B, and C regions as shown in FIGS.
図7に示すナイフエッジの場合、図7のA領域でuS 2=0.26μm-2の理論曲線とよく合致し、実際のボールエンドミル及びスクエアーエンドミルの場合は、図8および図9のA領域でuS 2=0.6μm-2の理論曲線とよく合致している。ナイフエッジと、各エンドミルの各方向での測定結果で、それぞれ曲線が異なるのは、光の回折による要因が支配的と考えられる。 In the case of the knife edge shown in FIG. 7, it agrees well with the theoretical curve of u S 2 = 0.26 μm −2 in the region A of FIG. 7, and in the case of an actual ball end mill and square end mill, the region A of FIGS. It is in good agreement with the theoretical curve of u S 2 = 0.6μm -2 . The reason for the difference in the curve between the knife edge and the measurement result in each direction of each end mill is considered to be due to the light diffraction factor.
即ち、エンドミルの測定では、3次元的な形状の工具刃先と被削材をスリットに見立てて、スリット幅に対する光強度を測定したが、実際は図6に示したように、理想的なスリットと異なり、測定している中心部でスリット幅が0に近づいても、その周辺のスリット幅は広いため、周辺部からの光の回折による影響を受ける。このため、エンドミルによって得られた光強度曲線は、光の回折による影響のために光強度が押し上げられていると考えられる。よって、ナイフエッジのuS 2は、実験で得られた光強度曲線に合致する値より小さい。この要因は、回転方向により各スリット周辺形状が変わることから、光強度曲線が回転方向により変化することによると考えられる。 That is, in the measurement of the end mill, the light intensity with respect to the slit width was measured with the three-dimensional shape of the tool edge and the work material as a slit, but actually, as shown in FIG. Even if the slit width approaches zero at the center of measurement, the slit width around the center is wide, and therefore, it is affected by light diffraction from the peripheral portion. For this reason, it is considered that the light intensity curve obtained by the end mill is pushed up due to the influence of light diffraction. Therefore, the knife edge u S 2 is smaller than the value that matches the experimentally obtained light intensity curve. This factor is considered to be due to the fact that the light intensity curve changes depending on the rotation direction because the shape around each slit changes depending on the rotation direction.
また、各領域においては、A領域では工具と被削材の距離wの二乗に比例する急激な光強度の変化が生じている。一方、C領域はカメラのCCDに入射する光強度が大きいために、出力信号が飽和している。B領域では、A領域のように理論曲線と一致せず、またC領域のように出力信号が飽和していない。 Moreover, in each area | region, the change of the light intensity which is proportional to the square of the distance w of a tool and a workpiece has arisen in A area | region. On the other hand, the output signal is saturated in the C region because the light intensity incident on the CCD of the camera is large. In the B region, it does not coincide with the theoretical curve as in the A region, and the output signal is not saturated as in the C region.
そこで、この要因として考えられるCCDのγ値について検討した。上記実施形態の測定装置から工具と被削材を取り外し、可変式NDフィルターを用いて、使用したCCDのγ曲線を求めた。その結果を図10に示す。入力される光強度が0.8以上で、γ=1.0の直線から大きく外れ、入力に対して出力が小さい。よって、図7等のB領域は、全域でγ=1.0に補正した場合、理論で求められた曲線に近づく。しかし、急激な変化のあるA領域を用いて測定する場合は、特に補正などは入れずA領域のみをもいても良い。 Therefore, the γ value of CCD, which is considered as this factor, was examined. The tool and the work material were removed from the measurement apparatus of the above embodiment, and the γ curve of the CCD used was obtained using a variable ND filter. The result is shown in FIG. The input light intensity is 0.8 or more, greatly deviating from the line of γ = 1.0, and the output is small with respect to the input. Therefore, the region B in FIG. 7 and the like approaches a curve obtained by theory when the entire region is corrected to γ = 1.0. However, when the measurement is performed using the A region having a sudden change, only the A region may be provided without any correction.
次に、工具刃先が被削材に接触する直前で、高い繰り返し位置決め精度が得られることを確認した。上記実施形態の図1の装置で、光強度が0.5となる位置に表1の各工具刃先を移動させ、その位置を電気マイクロメータで測定した。これを20回繰り返し、標準偏差σ、および全測定値の最大値から最小値の差を求めた。 Next, it was confirmed that high repeat positioning accuracy was obtained immediately before the tool blade edge contacted the work material. With the apparatus of FIG. 1 of the above embodiment, each tool blade edge in Table 1 was moved to a position where the light intensity was 0.5, and the position was measured with an electric micrometer. This was repeated 20 times, and the difference between the minimum value was obtained from the standard deviation σ and the maximum value of all measured values.
表2に結果を示し、図11、図12に度数分布を示す。横軸は光強度0.5を検出した位置を示し、プラス側は被削材に接近、マイナス側は被削材から遠ざかっていることを示している。
繰り返し位置決め精度は、各々の工具で方向3が最も高く、順に方向2、方向1となった。測定方向により繰り返し位置決め精度に差が生じる要因を、光強度曲線との相関から考えると、おおよそ光強度曲線の合致するuS 2が大きい測定方向ほど、測定感度が高くなるため、測定精度が高くなると推察される。 The repeat positioning accuracy was highest in the direction 3 for each tool, followed by the direction 2 and the direction 1 in order. Considering the factors that cause differences in positioning accuracy depending on the measurement direction from the correlation with the light intensity curve, the measurement sensitivity increases as the measurement direction with a larger u S 2 that matches the light intensity curve increases. It is assumed that
次に、上記実験で得られた繰り返し位置決め精度、および全測定値の最大値から最小値の差を、従来の接触式の刃先位置測定器(カタログ値2σ=±1μm)と比較した。まず、上述の実施形態の図1の測定装置を図13に示すように再構成した。接触式の刃先位置測定器40と工具12の刃先を対向させ、工具12を被削材22に徐々に接近させ、接触式の刃先位置測定器40が検出信号を出力したときの位置を電気マイクロメータ34で測定した。これを20回繰り返し、その結果を表3に示す。
この表3より、接触式の刃先位置測定器40の繰り返し位置決め精度がσ=0.100μmであるのに対して、本測定装置の実験結果は表2よりσ≦0.048μmであり、本装置の精度が2倍程度良いことが分かった。 From Table 3, the repeatable positioning accuracy of the contact-type edge position measuring device 40 is σ = 0.100 μm, whereas the experimental result of this measuring device is σ ≦ 0.048 μm from Table 2, and the accuracy of this device is Was found to be about twice as good.
以上の実験結果より、この発明の工具位置測定方法と装置は、非接触でかつ工具刃先と被削材の距離を直接測る位置測定装置として、十分な繰り返し位置決め精度をもつ。また、工具刃先形状を直接観察することにより工具刃先形状の違いによる誤差を受けないものである。 From the above experimental results, the tool position measuring method and apparatus according to the present invention have sufficient repeated positioning accuracy as a position measuring apparatus that directly measures the distance between the tool blade edge and the work material without contact. Further, by directly observing the tool edge shape, it is free from errors due to the difference in the tool edge shape.
10 工具位置測定装置
12 工具
22 被削材
24 光ファイバ
32 カメラ
DESCRIPTION OF SYMBOLS 10 Tool position measuring device 12 Tool 22 Work material 24 Optical fiber 32 Camera
Claims (3)
The computer according to claim 2, wherein the calculation means is a computer that stores a correspondence between the light intensity and the distance in a region where the light intensity varies depending on a distance between the tool and the work material, and outputs the distance based on the light intensity. Tool position measuring device.
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| CN104493641A (en) * | 2014-12-25 | 2015-04-08 | 苏州博众精工科技有限公司 | Lifting detection mechanism |
| CN104501782A (en) * | 2014-12-31 | 2015-04-08 | 苏州博众精工科技有限公司 | Angle-adjustable detection mechanism |
| CN105081880A (en) * | 2014-05-05 | 2015-11-25 | 天津职业技术师范大学 | Method and apparatus of non-contact on-line identification for radial jumping quantity of micro milling cutter |
| CN105973161A (en) * | 2016-06-17 | 2016-09-28 | 西安交通大学 | Three-dimensional full-field deformation measurement method of paddle |
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Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
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| WO2012014609A1 (en) | 2010-07-29 | 2012-02-02 | 国立大学法人九州工業大学 | System and method for measuring length of gap between rotating tool and workpiece |
| JP2012032222A (en) * | 2010-07-29 | 2012-02-16 | Kyushu Institute Of Technology | Measuring method and system for clearance length between rotary tool and workpiece |
| KR101379199B1 (en) * | 2010-07-29 | 2014-03-31 | 고쿠리츠 다이가쿠 호진 큐슈 코교 다이가쿠 | System and method for measuring length of gap between rotating tool and workpiece |
| US8755055B2 (en) | 2010-07-29 | 2014-06-17 | Kyushu Institute Of Technology | System and method for measuring length of gap between rotating tool and workpiece |
| CN105081880A (en) * | 2014-05-05 | 2015-11-25 | 天津职业技术师范大学 | Method and apparatus of non-contact on-line identification for radial jumping quantity of micro milling cutter |
| CN104493641A (en) * | 2014-12-25 | 2015-04-08 | 苏州博众精工科技有限公司 | Lifting detection mechanism |
| CN104501782A (en) * | 2014-12-31 | 2015-04-08 | 苏州博众精工科技有限公司 | Angle-adjustable detection mechanism |
| CN104501782B (en) * | 2014-12-31 | 2016-10-05 | 苏州博众精工科技有限公司 | A kind of adjustable angle testing agency |
| CN105973161A (en) * | 2016-06-17 | 2016-09-28 | 西安交通大学 | Three-dimensional full-field deformation measurement method of paddle |
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