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JP6976107B2 - Inclined surface boundary position identification method, inclined surface boundary position identification device, inclined surface boundary position identification program - Google Patents
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JP6976107B2 - Inclined surface boundary position identification method, inclined surface boundary position identification device, inclined surface boundary position identification program - Google Patents

Inclined surface boundary position identification method, inclined surface boundary position identification device, inclined surface boundary position identification program Download PDF

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JP6976107B2
JP6976107B2 JP2017160370A JP2017160370A JP6976107B2 JP 6976107 B2 JP6976107 B2 JP 6976107B2 JP 2017160370 A JP2017160370 A JP 2017160370A JP 2017160370 A JP2017160370 A JP 2017160370A JP 6976107 B2 JP6976107 B2 JP 6976107B2
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裕一 尾崎
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本発明は、傾斜面境界位置同定方法、傾斜面境界位置同定装置、傾斜面境界位置プログラムに関する。 The present invention relates to an inclined surface boundary position identification method, an inclined surface boundary position identification device, and an inclined surface boundary position program.

ある点から測定点までの絶対距離を高精度で測定する装置としてレーザ距離計が知られている。たとえば、特許文献1には、測定光の干渉信号と基準光の干渉信号の時間差から距離を測定する距離計が記載されている。 A laser range finder is known as a device for measuring an absolute distance from a certain point to a measurement point with high accuracy. For example, Patent Document 1 describes a rangefinder that measures a distance from a time difference between an interference signal of measurement light and an interference signal of reference light.

特開2010−14549号公報Japanese Unexamined Patent Publication No. 2010-14549

レーザ距離計の応用例として、傾斜の異なる二つの面の境界位置の同定を挙げることができる。これは、たとえば、機械部品の加工精度の検証のため有用である。図11(A)、(B)に境界位置の同定の例を示す。図11(A)は、測定対象物100の一部の断面図であり、測定対象物100は、傾斜の異なる二つの傾斜面101、102を有している。傾斜面101と傾斜面102の境界103は、図11(B)に示すように円形であり、一つの平面105に含まれているものとする。 As an application example of the laser range finder, identification of the boundary position between two surfaces having different inclinations can be mentioned. This is useful, for example, for verifying the machining accuracy of machine parts. 11 (A) and 11 (B) show an example of identification of the boundary position. FIG. 11A is a cross-sectional view of a part of the object to be measured 100, and the object 100 to be measured has two inclined surfaces 101 and 102 having different inclinations. It is assumed that the boundary 103 between the inclined surface 101 and the inclined surface 102 is circular as shown in FIG. 11B and is included in one plane 105.

測定対象物100を図11(B)のX方向及びY方向にスキャンし各測定点104の基準面111からの距離yを求めることができれば、境界103の位置を同定すること、すなわち、境界103を含む平面105の基準面からの距離hを求めることが可能である。たとえば、測定結果に基づいて各測定点に対応するピクセルの色を距離yに応じて定めた2次元画像を生成し、その画像から輪郭を抽出することにより同定することができる。 If the measurement object 100 can be scanned in the X and Y directions of FIG. 11B and the distance y of each measurement point 104 from the reference plane 111 can be obtained, the position of the boundary 103 can be identified, that is, the boundary 103. It is possible to obtain the distance h from the reference plane of the plane 105 including the above. For example, it can be identified by generating a two-dimensional image in which the color of the pixel corresponding to each measurement point is determined according to the distance y based on the measurement result and extracting the contour from the image.

レーザ距離計では、測定光110が測定対象物100で反射・散乱した光を検出器113で検出する必要があるが、図11(A)の傾斜面102のように測定光110の入射角θが小さい場合には、反射・散乱光のうち測定器113の方向に向かう光112の強度は小さいため、距離yの測長精度が低下して境界103を正確に同定できないという問題があった。また、切削加工された金属材料のように測定対象物の表面が金属光沢を持つ場合も同様の問題があった。 In the laser distance meter, it is necessary for the detector 113 to detect the light reflected / scattered by the measurement object 100 by the measurement light 110, but the incident angle θ of the measurement light 110 is as shown in the inclined surface 102 of FIG. 11 (A). When is small, the intensity of the light 112 directed toward the measuring instrument 113 among the reflected / scattered light is small, so that there is a problem that the measurement accuracy of the distance y is lowered and the boundary 103 cannot be accurately identified. Further, there is a similar problem when the surface of the object to be measured has a metallic luster, such as a machined metal material.

そこで、本発明は、測定対象物で反射・散乱し検出器で検出される光の強度が小さい場合でも正確に傾斜面の境界位置を同定することができる傾斜面境界位置同定方法等を提供することを目的する。 Therefore, the present invention provides a method for identifying the boundary position of an inclined surface, which can accurately identify the boundary position of an inclined surface even when the intensity of light reflected / scattered by the object to be measured and detected by the detector is small. Aim for that.

本発明の傾斜面位置同定方法は、互いに傾斜の異なる第1の面と第2の面を備える設計寸法が既知の測定対象物の前記第1の面と前記第2の面の境界を含む平面である境界面の仮想面測定光と直交する基準面に対して前記設計寸法に基づいて予め与えられた傾きで設定し、仮想面と基準面との距離である仮想面高さを変化させながら、境界を含む測定領域内の各測定点のうち光学的に測定された基準面からの距離である測定点高さが仮想面高さより小さいものを抽出する抽出工程と、抽出工程で抽出した測定点について測定点高さの測定に利用した測定光の第1の面または第2の面からの反射光の輝度である測定点輝度を対数変換して合計し積算輝度を算出する積算輝度算出工程と、積算輝度と仮想面高さとの関係を示す曲線の変曲点を特定することにより境界面の位置を同定する同定工程を含む。 The method for identifying an inclined surface position of the present invention is a plane including a boundary between the first surface and the second surface of a measurement object having a first surface and a second surface having different inclinations and having known design dimensions. The virtual surface of the boundary surface is set with an inclination given in advance based on the design dimensions with respect to the reference surface orthogonal to the measurement light, and the virtual surface height, which is the distance between the virtual surface and the reference surface, is changed. However, among the measurement points in the measurement area including the boundary, those whose measurement point height, which is the distance from the optically measured reference plane, is smaller than the virtual surface height are extracted by the extraction step and the extraction step. About the measurement point The integrated brightness calculation that calculates the integrated brightness by logarithmically converting the measurement point brightness, which is the brightness of the reflected light from the first surface or the second surface of the measurement light used for measuring the measurement point height, and totaling them. It includes a step and an identification step of identifying the position of the boundary surface by identifying the turning point of the curve showing the relationship between the integrated brightness and the virtual surface height.

本発明の傾斜面位置同定装置は、互いに傾斜の異なる第1の面と第2の面を備える設計寸法が既知の測定対象物の前記第1の面と前記第2の面の境界を含む平面である境界面の仮想面測定光と直交する基準面に対して前記設計寸法に基づいて予め与えられた傾きで設定し、仮想面と基準面との距離である仮想面高さを変化させながら、境界を含む測定領域内の各測定点のうち光学的に測定された基準面からの距離である測定点高さが仮想面高さより小さいものを抽出する抽出手段と、抽出工程で抽出した測定点について測定点高さの測定に利用した測定光の第1の面または第2の面からの反射光の輝度である測定点輝度を対数変換して合計し積算輝度を算出する積算輝度算出手段と、積算輝度と仮想面高さとの関係を示す曲線の変曲点を特定することにより境界面の位置を同定する同定手段を含む。 The inclined surface position identifying device of the present invention includes a first surface and a second surface having different inclinations, and a plane including a boundary between the first surface and the second surface of a measurement object whose design dimensions are known. The virtual surface of the boundary surface is set with an inclination given in advance based on the design dimensions with respect to the reference surface orthogonal to the measurement light, and the virtual surface height, which is the distance between the virtual surface and the reference surface, is changed. However, among the measurement points in the measurement area including the boundary, those whose measurement point height, which is the distance from the optically measured reference plane, is smaller than the virtual surface height are extracted by the extraction means and the extraction step. About the measurement point The integrated brightness calculation that calculates the integrated brightness by logarithmically converting the measurement point brightness, which is the brightness of the reflected light from the first surface or the second surface of the measurement light used for measuring the measurement point height, and totaling them. The means include identification means for identifying the position of the boundary surface by identifying the turning point of the curve showing the relationship between the integrated brightness and the virtual surface height.

本発明の傾斜面位置同定プログラムは、コンピュータに、互いに傾斜の異なる第1の面と第2の面を備える設計寸法が既知の測定対象物の前記第1の面と前記第2の面の境界を含む平面である境界面の仮想面測定光と直交する基準面に対して前記設計寸法に基づいて予め与えられた傾きで設定し、仮想面と基準面との距離である仮想面高さを変化させながら、境界を含む測定領域内の各測定点のうち光学的に測定された基準面からの距離である測定点高さが仮想面高さより小さいものを抽出する抽出処理と、抽出処理で抽出した測定点について測定点高さの測定に利用した測定光の第1の面または第2の面からの反射光の輝度である測定点輝度を対数変換して合計し積算輝度を算出する積算輝度算出処理と、積算輝度と仮想面高さとの関係を示す曲線の変曲点を特定することにより境界面の位置を同定する同定処理を実行させることを特徴とする。 The inclined surface position identification program of the present invention comprises a first surface and a second surface having different inclinations from each other, and the boundary between the first surface and the second surface of a measurement object whose design dimensions are known. based on the design dimension set in inclination previously given with respect to a reference plane orthogonal to the measurement light a virtual plane of the boundary surface is a plane including the virtual surface height is the distance between the virtual plane and the reference plane Extraction process and extraction process to extract those whose measurement point height, which is the distance from the optically measured reference plane, is smaller than the virtual surface height among each measurement point in the measurement area including the boundary. For the measurement points extracted in step 1, the measurement point brightness, which is the brightness of the reflected light from the first surface or the second surface of the measurement light used for measuring the measurement point height, is logarimetrically converted and totaled to calculate the integrated brightness. It is characterized in that the integrated brightness calculation process and the identification process of identifying the position of the boundary surface by specifying the bending point of the curve showing the relationship between the integrated brightness and the virtual surface height are executed.

本発明によれば、測定対象物で反射・散乱し検出器で検出される光の強度が小さい場合でも正確に傾斜面の境界位置を同定することができる。 According to the present invention, it is possible to accurately identify the boundary position of the inclined surface even when the intensity of the light reflected / scattered by the object to be measured and detected by the detector is small.

測定対象物の一例であるエンジンのバルブシート部の形状を示す図で、(A)は断面図、(B)は平面図である。It is a figure which shows the shape of the valve seat part of an engine which is an example of a measurement object, (A) is a sectional view, (B) is a plan view. 境界位置同定方法の原理を説明する図である。It is a figure explaining the principle of the boundary position identification method. 境界位置同定方法の手順を説明するフローチャートである。It is a flowchart explaining the procedure of the boundary position identification method. 仮想面の高さと積算輝度の関係を示すグラフである。It is a graph which shows the relationship between the height of a virtual surface and the integrated luminance. 図4の微分値を示すグラフである。It is a graph which shows the differential value of FIG. 境界が長方形の測定対象物の例を示す図で、(A)は断面図、(B)は平面図である。It is a figure which shows the example of the measurement object which the boundary is rectangular, (A) is a sectional view, (B) is a plan view. 凸部を有する測定対象物の例を示す図で、(A)は断面図、(B)は平面図である。It is a figure which shows the example of the measurement object which has a convex part, (A) is a sectional view, (B) is a plan view. 開いた境界を有する測定対象物の例を示す図で、(A)は断面図、(B)は平面図である。It is a figure which shows the example of the measurement object which has an open boundary, (A) is a sectional view, (B) is a plan view. 境界位置同定装置の構造図である。It is a structural diagram of the boundary position identification apparatus. 光源の出力を模式的に示す図である。It is a figure which shows the output of a light source schematically. 従来の傾斜面境界位置同定方法を説明する図である。It is a figure explaining the conventional method of identifying the boundary position of an inclined surface.

以下、図面を参照しながら本発明の一実施形態である傾斜面境界位置同定方法について詳細に説明する。測定対象物としてエンジンのバルブシート部を例に説明するが、本発明は他の測定対象物にも適用することができる。 Hereinafter, the method for identifying the boundary position of the inclined surface, which is an embodiment of the present invention, will be described in detail with reference to the drawings. Although the valve seat portion of the engine will be described as an example of the object to be measured, the present invention can be applied to other objects to be measured.

図1は、測定対象物の一例であるエンジンのバルブシート部の形状を示す図で、(A)は断面図、(B)は平面図である。バルブシート10はシリンダヘッド1のシリンダ2と吸気または排気ポート3との連接部分に設けられ、バルブ4と当接する円錐面状のバルブ当たり面11(第1の面の一例)と、バルブ当たり面11の外側に設けられバルブ当たり面11より傾斜の緩い円錐面状の外周面12(第2の面の一例)により構成されている。本方法では、レーザ距離計により図1(B)に示したバルブシート10を含む測定領域23をX方向及びY方向にスキャンして各測定点の基準面からの距離及び反射光の強度を測定し、これらのデータに基づいてのバルブ当たり面11と外周面12との境界13を同定する。 1A and 1B are views showing the shape of a valve seat portion of an engine, which is an example of an object to be measured, where FIG. 1A is a cross-sectional view and FIG. 1B is a plan view. The valve seat 10 is provided at a connecting portion between the cylinder 2 of the cylinder head 1 and the intake or exhaust port 3, and has a conical valve contact surface 11 (an example of the first surface) that abuts on the valve 4 and a valve contact surface. It is composed of a conical outer peripheral surface 12 (an example of a second surface) provided on the outside of the valve 11 and having a gentle inclination from the valve contact surface 11. In this method, the measurement region 23 including the valve seat 10 shown in FIG. 1 (B) is scanned in the X direction and the Y direction by a laser range finder to measure the distance from the reference plane of each measurement point and the intensity of the reflected light. Then, the boundary 13 between the valve contact surface 11 and the outer peripheral surface 12 is identified based on these data.

図2は傾斜面境界位置同定方法の原理を説明する図、図3は傾斜面境界位置同定方法の手順を説明するフローチャートである。これらの図を参照して、本方法の詳細な手順を説明する。
同定の前提として、バルブシート10の設計寸法は既知であり、加工精度を検証するために境界13の位置(図2の上下方向の位置)を同定するものとする。また、境界13はバルブ4の摺動軸16に垂直な平面である境界面15に含まれているものとする。
FIG. 2 is a diagram illustrating the principle of the inclined surface boundary position identification method, and FIG. 3 is a flowchart illustrating a procedure of the inclined surface boundary position identification method. The detailed procedure of this method will be described with reference to these figures.
As a premise for identification, the design dimensions of the valve seat 10 are known, and the position of the boundary 13 (the position in the vertical direction in FIG. 2) is identified in order to verify the machining accuracy. Further, it is assumed that the boundary 13 is included in the boundary surface 15 which is a plane perpendicular to the sliding shaft 16 of the valve 4.

測定領域23(図1参照)を、たとえばレーザ距離計60(距離計の一例)によりスキャンして各測定点17の高さyと測定光の反射強度を測定する(ST1、測定工程の一例)。高さyは図2に示すように測定点17の測定光20に対して垂直な基準面21からの距離である。なお、本実施形態では、測定光20をテレセントリック(どの測定点17を測定する際も測定光20の向きが一定)とするが、これは必須ではなく、測定光20がバルブ当たり面11と外周面12を照射することができればテレセントリックでなくてもよい。測定領域23は、1辺の長さがバルブシート10の設計上の直径よりもやや大きい正方形の領域とする。測定点17のX方向及びY方向の間隔は、所望の同定精度や測定時間を考慮して適宜定める。 The measurement area 23 (see FIG. 1) is scanned by, for example, a laser rangefinder 60 (an example of a rangefinder) to measure the height y of each measurement point 17 and the reflection intensity of the measurement light (ST1, an example of a measurement process). .. As shown in FIG. 2, the height y is the distance from the reference plane 21 perpendicular to the measurement light 20 at the measurement point 17. In the present embodiment, the measurement light 20 is telecentric (the direction of the measurement light 20 is constant when measuring any measurement point 17), but this is not essential, and the measurement light 20 is the valve contact surface 11 and the outer periphery. It does not have to be telecentric as long as the surface 12 can be irradiated. The measurement area 23 is a square area in which the length of one side is slightly larger than the design diameter of the valve seat 10. The distance between the measurement points 17 in the X direction and the Y direction is appropriately determined in consideration of the desired identification accuracy and the measurement time.

境界面15仮想面22を初期位置に設定する(ST2)。境界面15の仮想面22は、バルブ4の摺動軸16と直交する面であって、測定光と直交する基準面21に対して前記設計寸法に基づいて予め与えられた傾きで設定される。初期位置は、仮想面22が境界面15よりも下になるように高さhを設定する。ここでは、hを摺動軸16と仮想面22の交点と基準面21との間の測定光20に平行な方向の距離とする。 The virtual surface 22 of the boundary surface 15 is set to the initial position (ST2). The virtual surface 22 of the boundary surface 15 is a surface orthogonal to the sliding axis 16 of the bulb 4, and is set with an inclination given in advance with respect to the reference surface 21 orthogonal to the measurement light based on the design dimensions. .. For the initial position, the height h is set so that the virtual surface 22 is below the boundary surface 15. Here, h is the distance between the intersection of the sliding shaft 16 and the virtual surface 22 and the reference surface 21 in the direction parallel to the measurement light 20.

ステップST1で取得した高さyの情報を用いて、仮想面17よりも上に位置する(y<hである)測定点17を抽出する(ST3、抽出工程)。 Using the information of the height y acquired in step ST1, the measurement point 17 located above the virtual surface 17 (y <h) is extracted (ST3, extraction step).

ステップST3で抽出された各測定点の反射強度を対数変換し、各測定点の対数変換された反射強度を合計することにより積算輝度を算出する(ST4、積算輝度算出工程)。 The integrated brightness is calculated by logarithmically converting the reflection intensity of each measurement point extracted in step ST3 and summing the logarithmically converted reflection intensity of each measurement point (ST4, integrated brightness calculation step).

仮想面22の位置を上方に移動しながら、上記のST3、ST4を仮想面の位置が所定の終了位置になるまで繰り返す(ST5、ST6)。終了位置は、境界面15の設計上の位置よりも上になるように予め設定しておく。 While moving the position of the virtual surface 22 upward, the above ST3 and ST4 are repeated until the position of the virtual surface reaches a predetermined end position (ST5, ST6). The end position is set in advance so as to be above the design position of the boundary surface 15.

積算輝度と仮想面の高さhの関係を示す積算輝度−仮想面グラフを作成する(ST7)。図4は積算輝度−仮想面グラフの一例である。図4では高さhを初期位置からの相対的な高さで示している。積算輝度−仮想面グラフは理想的には図4のように、仮想面22がバルブ当たり面11内に位置する区間の勾配の小さい直線25と仮想面22が外周面22内に位置する区間の勾配の大きい直線26とから成る折れ線となり、曲線の勾配が急変する点である変曲点27に対応する高さy1が境界面15の位置となる。しかし、実際には測定ノイズが多く含まれるため、図4のような理想的な形にはならず、このグラフから直接明確な変曲点を求めることは困難である場合が多い。言い換えると、図4のような理想的なグラフが得られる場合には、積算輝度を求めるまでもなく、高さ情報だけから境界を同定できる可能性が高い。 An integrated luminance-virtual area graph showing the relationship between the integrated luminance and the height h of the virtual surface is created (ST7). FIG. 4 is an example of an integrated luminance-virtual area graph. In FIG. 4, the height h is shown as a relative height from the initial position. The integrated brightness-virtual surface graph is ideally as shown in FIG. 4, in which a straight line 25 having a small gradient in the section where the virtual surface 22 is located in the valve contact surface 11 and a section in which the virtual surface 22 is located in the outer peripheral surface 22. It is a polygonal line composed of a straight line 26 having a large gradient, and the height y1 corresponding to the inflection point 27, which is a point where the gradient of the curve suddenly changes, is the position of the boundary surface 15. However, in reality, since a large amount of measurement noise is included, the ideal shape as shown in FIG. 4 is not obtained, and it is often difficult to obtain a clear inflection point directly from this graph. In other words, when an ideal graph as shown in FIG. 4 is obtained, it is highly possible that the boundary can be identified only from the height information without obtaining the integrated luminance.

積算輝度−仮想面グラフの変曲点を求める方法は任意であるが、たとえば本実施形態では、積算輝度−仮想面グラフを微分することにより変曲点を求める(ST8、ST9、ST7〜ST9は同定工程の一例)。図5は、図4の積算輝度−仮想面グラフを微分したグラフである。図4のような理想的な積算輝度−仮想面グラフを微分すると、図5のように段差28が明りょうな階段状のグラフとなり、段差28の位置を境界の位置とすることができる。しかし、前述のように積算輝度−仮想面グラフは理想的な形状とはならないことが多いため、実際には、その微分値に図5のような明りょうな段差は表れない。 The method of finding the inflection point of the integrated luminance-virtual area graph is arbitrary, but in the present embodiment, for example, the inflection point is obtained by differentiating the integrated luminance-virtual area graph (ST8, ST9, ST7 to ST9 are An example of the identification process). FIG. 5 is a graph obtained by differentiating the integrated luminance-virtual area graph of FIG. When the ideal integrated luminance-virtual area graph as shown in FIG. 4 is differentiated, the step 28 becomes a clear stepped graph as shown in FIG. 5, and the position of the step 28 can be set as the boundary position. However, as described above, the integrated luminance-virtual area graph often does not have an ideal shape, so that the differential value does not actually have a clear step as shown in FIG.

そこで、微分値の閾値Tを設定し、閾値Tに対応する高さy1を境界面15の高さとして同定する。このようにすることで、たとえば、図5に破線29で示したように段差が明りょうに表れなかった場合でも、境界の高さを同定することができる。 Therefore, the threshold value T of the differential value is set, and the height y1 corresponding to the threshold value T is identified as the height of the boundary surface 15. By doing so, for example, the height of the boundary can be identified even when the step does not clearly appear as shown by the broken line 29 in FIG.

以上、バルブシートを例に境界が円形である場合について説明したが、本方法は境界の形状が円形以外の閉じた図形の場合にも適用することができる。図6(A)に断面図、図6(B)に平面図を示す測定対象物30は、上面33に底面31と側面32により形成された凹部を備えている。底面31と側面32の境界34および側面32と上面33の境界35の平面形状は長方形となっている。このように、境界の形状が円形以外であっても図6(A)のように測定光20を境界を同定しようとする二つの面に照射することができれば、本方法を適用して境界34、35の上下方向の位置を同定することができる。 The case where the boundary is circular has been described above using the valve seat as an example, but this method can also be applied to the case where the boundary shape is a closed figure other than the circular shape. The measurement object 30, whose cross-sectional view is shown in FIG. 6A and whose plan view is shown in FIG. 6B, has a concave portion formed by a bottom surface 31 and a side surface 32 on the upper surface 33. The planar shape of the boundary 34 between the bottom surface 31 and the side surface 32 and the boundary 35 between the side surface 32 and the top surface 33 is rectangular. In this way, even if the shape of the boundary is not circular, if the measurement light 20 can be applied to the two surfaces for which the boundary is to be identified as shown in FIG. 6 (A), this method is applied to the boundary 34. , 35 can be identified in the vertical direction.

図7(A)に断面図、図7(B)に平面図を示す測定対象物40は、上面43に頂面41と側面42により形成された凸部を備えている。頂面41と側面42の境界44および側面42と上面43の境界45の平面形状は円形となっている。このように、境界が凸部の隅角部や立ち上がり部となる場合であっても図7(A)のように測定光20を境界を同定しようとする二つの面に照射することができれば、本方法により境界44、45の上下方向の位置を同定することができる。 The measurement object 40, whose cross-sectional view is shown in FIG. 7A and a plan view shown in FIG. 7B, has a convex portion formed by a top surface 41 and a side surface 42 on the upper surface 43. The planar shape of the boundary 44 between the top surface 41 and the side surface 42 and the boundary 45 between the side surface 42 and the upper surface 43 is circular. In this way, even if the boundary is a corner portion or a rising portion of the convex portion, if the measurement light 20 can be applied to the two surfaces for which the boundary is to be identified as shown in FIG. 7 (A), By this method, the positions of the boundaries 44 and 45 in the vertical direction can be identified.

図8(A)に断面図、図8(B)に平面図を示す測定対象物50は、帯状の部材で左側上面51と右側上面53の間に段差があり、左側上面51と右側上面53との間の部分は傾斜面52となっている。左側上面51と傾斜面52の境界54および傾斜面52と右側上面53の境界線55は測定対象物50の幅方向に伸びる直線となっている。このように、境界が直線、曲線、折れ線等の開いた図形である場合であっても図8(A)のように測定光20を境界を同定しようとする二つの面に照射することができれば、本方法により境界54、55の上下方向の位置を同定することができる。境界が直線の場合は、境界を含む境界面の仮想面が、設計寸法に基づいて測定光20と直交する基準面に対して予め与えられた傾きで設定されるThe measurement object 50, whose cross section is shown in FIG. 8 (A) and is shown in plan view in FIG. 8 (B), is a strip-shaped member having a step between the left upper surface 51 and the right upper surface 53, and the left upper surface 51 and the right upper surface 53. The portion between and is an inclined surface 52. The boundary line 54 between the left upper surface 51 and the inclined surface 52 and the boundary line 55 between the inclined surface 52 and the right upper surface 53 are straight lines extending in the width direction of the object to be measured 50. In this way, even if the boundary is an open figure such as a straight line, a curved line, or a polygonal line, if the measurement light 20 can be applied to the two surfaces for which the boundary is to be identified as shown in FIG. 8 (A). By this method, the positions of the boundaries 54 and 55 in the vertical direction can be identified. When the boundary is a straight line, the virtual surface of the boundary surface including the boundary is set with a predetermined inclination with respect to the reference surface orthogonal to the measurement light 20 based on the design dimensions.

図9は、図2のレーザ距離計60の概略構造図である。レーザ距離計60は、基準光Sを出射する第1の光源61と、測定光Sを出射する第2の光源62と、基準光Sと測定光Sとの干渉光Sを検出する基準光検出器63と、基準光Sが照射される基準面64と、測定光が照射される測定面65(たとえば、図2のバルブ当たり面11、外周面12)と、基準面64により反射された基準光S’と測定面65により反射された測定光S’との干渉光Sを検出する測定光検出器66と、基準光検出器63により干渉光Sを検出して得られる干渉信号と測定光検出器66により干渉光Sを検出して得られる干渉信号が供給される信号処理部67を備える。 FIG. 9 is a schematic structural diagram of the laser rangefinder 60 of FIG. Laser rangefinder 60 includes a first light source 61 for emitting reference light S 1, a second light source 62 for emitting measuring light S 2, the reference light S 1 interference light S 3 of the measuring beam S 2 a reference photodetector 63 to be detected, a reference plane 64 the reference light S 1 is being irradiated, the measurement surface 65 is the measuring light is irradiated (for example, the valve contact surface 11 in FIG. 2, the outer circumferential surface 12), the reference plane and the measurement light detector 66 for detecting the interference light S 4 of the 'measurement luminous S 2 reflected by the measurement surface 65 and' criteria light S 1 reflected by 64, the interference light S 3 by the reference photodetector 63 comprising a signal processing unit 67 that the interference signal obtained by detecting interference light S 4 detected interference signal obtained by the by the measurement photodetector 66 are supplied.

第1及び第2の光源61、62は、それぞれ周期的に強度又は位相が変調され、互いに変調周期が異なる干渉性のある基準光Sと測定光Sを出射するものであって、それぞれ周期的に強度又は位相を変調され、互いに変調周期が異なる干渉性のある基準光Sと測定光Sを出射するための光変調器を備える2台の光源、光周波数コムモード間隔が異なる2台の光周波数コム発生器、或いは、光パルス繰り返し周波数が異なる2台のパルス光源からなる。 The first and second light sources 61 and 62 emit the reference light S 1 and the measurement light S 2 , which are cyclically modulated in intensity or phase and have different modulation cycles from each other, respectively. modulated periodically intensity or phase, two light sources, an optical frequency comb mode spacing different comprising a light modulator for emitting reference light S 1 and the measurement light S 2 with the modulation period different interfering with each other It consists of two optical frequency comb generators or two pulse light sources with different optical pulse repetition frequencies.

第1及び第2の光源61,62から出射された基準光Sと測定光Sは、半透鏡又は偏光ビームスプリッタからなる光混合素子71により混合されて重ね合わされ、半透鏡からなる光分離素子72により、基準光検出器63に向かう光と測定対象に向かう光に分離される。 The emitted reference light S 1 from the first and second light sources 61 and 62 measuring beam S 2 is superposed is mixed by the light mixing element 71 comprising a semi-transparent mirror or a polarizing beam splitter, light separating consisting half mirror The element 72 separates the light toward the reference photodetector 63 and the light toward the measurement target.

ここでは、第1及び第2の光源61,62から出射された基準光Sと測定光Sは、互いに偏光面が直交しているものとし、半透鏡からなる光混合素子71により混合され、その混合光が光分離素子72により反射されて偏光子73を介して基準光検出器63に入射されるとともに、光分離素子72を通過した混合光が偏光ビームスプリッタ74により偏光に応じて基準光Sと測定光Sに分離されて、基準光Sが基準面64に入射され、また、測定光Sが測定面65に入射されるようになっている。 Here, the measuring beam S 2 emitted reference light S 1 from the first and second light sources 61 and 62, it is assumed that orthogonal polarization planes with each other are mixed by the light mixing device 71 made of semi-transparent mirror The mixed light is reflected by the light separating element 72 and incident on the reference light detector 63 via the polarizing element 73, and the mixed light passing through the light separating element 72 is referred to by the polarizing beam splitter 74 according to the polarization. The light S 1 and the measurement light S 2 are separated, and the reference light S 1 is incident on the reference surface 64, and the measurement light S 2 is incident on the measurement surface 65.

さらに、基準面64により反射された基準光S’と、測定面65により反射された測定光S’は、偏光ビームスプリッタ74により混合され、その混合光が光分離素子72により反射されて偏光子75を介して測定光検出器66に入射されるようになっている。 Furthermore, the reference light S 1 that is reflected by the reference surface 64 'and, measurement luminous S 2 reflected by the measuring surface 65' is mixed by the polarization beam splitter 74, the mixed light is reflected by the light splitting element 72 It is adapted to be incident on the measuring light detector 66 via the polarizing element 75.

そして、基準光検出器63は、偏光子73を介して入射される基準光Sと測定光Sとの混合光を受光することより、第1及び第2の光源61,62から出射された基準光Sと測定光Sの干渉光Sを検出するようになっている。 The reference photodetector 63, than to receive mixed light of the reference light S 1 that is incident through the polarizer 73 and the measuring light S 2, emitted from the first and second light sources 61 and 62 and it detects the reference light S 1 and the interference light S 3 of the measuring beam S 2 was.

また、測定光検出器66は、偏光子75を介して入射される基準光S’と測定光S’の混合光を受光することにより、基準面64により反射された基準光S’と測定面5により反射された測定光S’の干渉光Sを検出するようになっている。 The measurement photodetector 66, by receiving the mixed light of the 'measurement beam S 2 and' reference beam S 1 is incident through the polarizer 75, the reference light S 1 that is reflected by the reference surface 64 ' and it is adapted to detect the interference light S 4 of the measuring light S 2 'that is reflected by the measurement surface 5.

基準光検出器63によって得られる干渉信号は、キャリア周波数が第1及び第2の光源61,62から出射された基準光Sと測定光Sのキャリア光周波数の差であり、基準光Sと測定光Sの光パルス繰り返し周波数の差の周波数で同じ干渉波形が繰り返される。 The interference signal obtained by the reference photodetector 63, the difference in the emitted reference light S 1 and a carrier light frequency of the measuring beam S 2 from the carrier frequency first and second light sources 61 and 62, the reference beam S 1 and the same interference wave at a frequency of the difference between the optical pulse repetition frequency of the measuring beam S 2 is repeated.

このレーザ距離計60において、基準光検出器63の役割は、遅延時間計測の基準を生成することである。第1及び第2の光源61,62から出射された基準光Sと測定光Sは、繰り返し周波数が等しくないので、光源が動作を開始した時にタイミングがずれていても、少しずつタイミングがずれていき、必ずどこかで基準光Sの光パルスと測定光Sの光パルスが重なる瞬間が現れる。また、その重なる瞬間は基準光Sと測定光Sの繰り返し周波数の差の繰り返し周波数で周期的に現れる。この光パルスと光パルスの重なる瞬間が、遅延時間計測の基準となる。 In this laser rangefinder 60, the role of the reference photodetector 63 is to generate a reference for delay time measurement. Reference light S 1 and the measurement light S 2 emitted from the first and second light sources 61 and 62, since unequal repetition frequency, be shifted timing when the light source starts operating, the timing slightly There will always be a moment when the optical pulse of the reference light S 1 and the optical pulse of the measurement light S 2 overlap each other. Further, the overlapping moment appears periodically at a repetition frequency of the difference between the repetition frequency of the reference light S 1 and the measurement light S 2. The moment when the optical pulse and the optical pulse overlap is the standard for measuring the delay time.

また、測定光検出器66によって得られる干渉信号は、基準光検出器3によって得られる干渉信号と同じくキャリア周波数が基準光S’と測定光S’のキャリア光周波数の差であり、基準光Sと測定光Sの光パルス繰り返し周波数の差と同じ繰り返し周波数を持つ。しかし、測定光検出器66に入力される光パルスは、基準反射鏡64までの距離Lと測定反射鏡65までの距離Lの距離差の絶対値(L−L)の分だけ、光パルスのタイミングが遅れるため、光パルスと光パルスの重なる瞬間が基準光検出器63によって得られる干渉信号と比較して遅れる。この遅れ時間が距離差の絶対値(L−L)の2倍の距離を光パルスが伝搬することによる遅延時間であり、真空中の光速Cをかけて屈折率ngで割ることにより距離が得られる。 Furthermore, interference signal obtained by the measurement photodetector 66 is the difference of the carrier light frequency of the interference signal obtained by the reference photodetector 3 also carrier frequencies 'and measuring light S 2' reference light S 1, the reference light pulses of light S 1 and the measuring beam S 2 repeated with the same repetition frequency as the difference frequency. However, the light pulse input to the measurement photodetector 66, the absolute value of the distance difference between the distance L 2 between the distance L 1 to the reference reflector 64 to a measurement reflector 65 min only (L 2 -L 1) Since the timing of the optical pulse is delayed, the moment when the optical pulse and the optical pulse overlap is delayed as compared with the interference signal obtained by the reference optical detector 63. This delay time is the delay time due to the propagation of the optical pulse at a distance twice the absolute value of the distance difference (L 2- L 1 ), and is the distance obtained by multiplying the speed of light C in vacuum and dividing by the refractive index ng. Is obtained.

このように、周期の異なる2台のパルス光源の干渉によって距離計測を行う場合、時間基準を与える干渉信号の基準光検出器63が不可欠であり、基準光検出器63と測定光検出器66により得られる各干渉信号の時間差を比較することによって初めて距離測定が可能となる。 As described above, when the distance is measured by the interference of two pulse light sources having different periods, the reference light detector 63 for the interference signal that gives a time reference is indispensable, and the reference light detector 63 and the measurement light detector 66 are used. Distance measurement is possible only by comparing the time difference of each of the obtained interference signals.

そこで、レーザ距離計60において、信号処理部67は、基準光検出器63により干渉光S3を検出して得られる干渉信号と測定光検出器66により干渉光Sを検出して得られる干渉信号の時間差から、光速と測定波長における屈折率から基準面までの距離Lと測定面までの距離Lの距離差の絶対値(L−L)を求める処理を行う。 Therefore, the laser rangefinder 60, the signal processing unit 67, the interference signal obtained by detecting interference light S 3 by the interference signal obtained by detecting interference light S3 and the measurement light detector 66 by the reference photodetector 63 from the time difference, performs a process for obtaining the speed of light and the absolute value of the distance difference between the distance L 2 of a distance L 1 and the measurement surface to the reference plane from the refractive index at a measurement wavelength (L 2 -L 1).

すなわち、このレーザ距離計60では、第1及び第2の光源61,62から出射されるそれぞれ周期的に強度又は位相が変調され、互いに変調周期が異なる干渉性のある基準光Sと測定光Sを基準面64と測定面65に照射し、基準面64と測定面65に照射する基準光Sと測定光Sとの干渉光Sを基準光検出器63により検出するとともに、基準面64により反射された基準光S’と測定面65により反射された測定光S’との干渉光Sを測定光検出器66により検出し、信号処理部67により、基準光検出器63により干渉光Sを検出した干渉信号と測定光検出器66により干渉光S4を検出した干渉信号の時間差から、光速と測定波長における屈折率から基準面までの距離と測定面までの距離の差を求める(図3のST1のうち高さの測定)。 That is, in the laser rangefinder 60, respectively cyclically intensity or phase emitted from the first and second light sources 61 and 62 is modulated, the reference light S 1 and the measuring light with the modulation period different interfering with each other with irradiated with S 2 to the reference plane 64 and the measuring surface 65 is detected by the reference light S 1 and the measurement light S 2 reference photodetector 63 an interference light S 3 and irradiating the reference surface 64 to the measurement surface 65, the interference light S 4 of the 'measurement luminous S 2 reflected by the measurement surface 65 and' criteria light S 1 reflected by the reference surface 64 is detected by measuring light detector 66, the signal processing unit 67, the reference light detected distance from the time difference of the interference signal detected interference light S4 by the interference signal detected interference light S 3 and the measurement light detector 66 by the vessel 63, until the distance between the measurement surface from the refractive index at the speed of light and the measuring wavelength to the reference plane (Measurement of height in ST1 in FIG. 3).

距離測定の原理は、光パルスの時間遅延から距離を求める距離計に準ずる。すなわち、距離(L−L)を往復する際の時間遅延ΔT=2×ng×(L−L)/cを計測して、光路の群屈折率ng、真空中の光速cから(L−L)を計算する。 The principle of distance measurement is based on a rangefinder that calculates the distance from the time delay of an optical pulse. That is, the time delay ΔT = 2 × ng × (L 2- L 1 ) / c when reciprocating the distance (L 2- L 1 ) is measured, and the group refractive index ng of the optical path and the speed of light c in vacuum are used. Calculate (L 2- L 1 ).

信号処理部67は、たとえばマイクロコンピュータで構成され、上記の距離計算処理に加えて、反射光の強度を計算する(図3のST1のうち反射光強度の測定)。信号処理部67は、さらに、図3のST2〜ST9の処理を行うコンピュータプログラムを実行し境界線の位置の同定を行う。 The signal processing unit 67 is composed of, for example, a microcomputer, and calculates the intensity of the reflected light in addition to the above-mentioned distance calculation process (measurement of the reflected light intensity in ST1 of FIG. 3). The signal processing unit 67 further executes a computer program that performs the processing of ST2 to ST9 in FIG. 3 to identify the position of the boundary line.

ここで、レーザ距離計60における第1、第2の光源61,62として2台の光周波数コム発生器を使用する場合、例えば、図10に示すような構成の光源80とされる。 Here, when two optical frequency comb generators are used as the first and second light sources 61 and 62 in the laser rangefinder 60, for example, the light source 80 having the configuration shown in FIG. 10 is used.

すなわち、この光源80では、1台の単一周波数発振のレーザ光源81から出射されるレーザ光がビームスプリッタ82により分割されて2台の光周波数コム発生器(OFCG1、OFCG2)86A,86Bに入力されるようになっている。 That is, in this light source 80, the laser light emitted from one single frequency oscillation laser light source 81 is split by the beam splitter 82 and input to the two optical frequency comb generators (OFCG1, OFCG2) 86A, 86B. It is supposed to be done.

2台の光周波数コム発生器86A,86Bは、互いに異なる周波数fm+Δfmと周波数fmで発振する発振器83A,83Bにより駆動される。それぞれの発振器83A,83Bは、共通の基準発振器84により位相同期されることにより、fm+Δfmとfmの相対周波数が安定になる。光周波数コム発生器(OFCG1)86Aの前には、音響光学周波数シフタ(AOFS)のような周波数シフタ85を設けて、入力されたレーザ光にこの周波数シフタ85により周波数faの光周波数シフトを与えるようになっている。これにより、キャリア周波数間のビート周波数が直流信号ではなく周波数faの交流信号になる。その結果、キャリア周波数の高周波側サイドバンドのビート信号と低周波側サイドバンドのビート信号がビート信号のキャリア周波数間のビート周波数faを挟んで相対する周波数領域に発生するため位相比較に都合が良い。 The two optical frequency comb generators 86A and 86B are driven by oscillators 83A and 83B that oscillate at different frequencies fm + Δfm and frequency fm. The respective oscillators 83A and 83B are phase-locked by the common reference oscillator 84, so that the relative frequencies of fm + Δfm and fm become stable. In front of the optical frequency comb generator (OFCG1) 86A, a frequency shifter 85 such as an acoustic optical frequency shifter (AOFS) is provided, and the input laser beam is given an optical frequency shift of frequency fa by this frequency shifter 85. It has become like. As a result, the beat frequency between the carrier frequencies becomes an AC signal having a frequency fa instead of a DC signal. As a result, the beat signal of the high frequency side band of the carrier frequency and the beat signal of the low frequency side side band are generated in the opposite frequency regions with the beat frequency fa between the carrier frequencies of the beat signal, which is convenient for phase comparison. ..

本実施形態では、レーザ距離計60の信号処理部67が傾斜面境界位置同定プログラムを実行するものとしたが、レーザ距離計60では高さと反射光強度の測定(図3のステップS1)のみを行い、境界の同定は他の装置、たとえばパーソナルコンピュータで、図3のステップST2〜ST9の処理を行う傾斜面境界位置同定プログラムを実行しレーザ距離計60による測定結果を解析することにより行うこともできる。すなわち、本発明は、傾斜面境界位置同定方法としてのほか、境界位置同定方法の各処理を実行する手段を備えた装置、境界位置同定方法の各処理をコンピュータに実行させるコンピュータプログラム、そのようなコンピュータプログラムを格納したコンピュータ読み取り可能な記憶媒体としても実施することができる。 In the present embodiment, the signal processing unit 67 of the laser rangefinder 60 executes the inclined surface boundary position identification program, but the laser rangefinder 60 only measures the height and the reflected light intensity (step S1 in FIG. 3). The boundary can be identified by executing the inclined surface boundary position identification program that performs the processing of steps ST2 to ST9 in FIG. 3 on another device, for example, a personal computer, and analyzing the measurement result by the laser range finder 60. can. That is, the present invention is a device provided with means for executing each process of the boundary position identification method, a computer program for causing a computer to execute each process of the boundary position identification method, in addition to the method of identifying the boundary position of an inclined surface. It can also be implemented as a computer-readable storage medium that stores a computer program.

また、レーザ距離計60は、距離計の一例であり、光を用いて測定点の高さと測定光の反射強度を測定することができるのもであれば、他の方式の距離計を用いることもできる。 Further, the laser rangefinder 60 is an example of a rangefinder, and if the height of the measurement point and the reflection intensity of the measurement light can be measured using light, another type of rangefinder may be used. You can also.

本方法では、積算輝度−仮想面位置グラフを作成し、このグラフの変曲点を求めることにより境界面の位置を同定する。そのため、測定光の反射強度が弱く測定点高さの測定精度が悪い場合でも、高精度で境界面位置を同定することができる。距離計の一例として示したレーザ距離計60のように測定光の照射と反射光の検出を同軸上で行う形式のものでは、一方の傾斜面に対する測定光の入射角が小さくなる場合が多く、特に、本発明が有用である。 In this method, an integrated luminance-virtual plane position graph is created, and the position of the boundary plane is identified by finding the inflection point of this graph. Therefore, even when the reflection intensity of the measurement light is weak and the measurement accuracy of the measurement point height is poor, the boundary surface position can be identified with high accuracy. In a type such as the laser rangefinder 60 shown as an example of a rangefinder, in which the irradiation of the measurement light and the detection of the reflected light are performed coaxially, the incident angle of the measurement light on one inclined surface is often small. In particular, the present invention is useful.

10 バルブシート、11 バルブ当たり面、12 外周面、13 境界、15 境界面、16 バルブの摺動軸、17 測定点、20 測定光、21 基準面、22 仮想面、60 レーザ距離計、61 第1の光源、62 第2の光源、63 基準光検出器、66 測定光検出器、67 信号処理部 10 valve seat, 11 valve contact surface, 12 outer peripheral surface, 13 boundary, 15 boundary surface, 16 valve sliding shaft, 17 measurement point, 20 measurement light, 21 reference surface, 22 virtual surface, 60 laser rangefinder, 61st 1 light source, 62 2nd light source, 63 reference light detector, 66 measurement light detector, 67 signal processing unit

Claims (9)

互いに傾斜の異なる第1の面と第2の面を備える設計寸法が既知の測定対象物の前記第1の面と前記第2の面の境界を含む平面である境界面の仮想面測定光と直交する基準面に対して前記設計寸法に基づいて予め与えられた傾きで設定し、前記仮想面と前記基準面との距離である仮想面高さを変化させながら、前記境界を含む測定領域内の各測定点のうち光学的に測定された前記基準面からの距離である測定点高さが前記仮想面高さより小さいものを抽出する抽出工程と、
前記抽出工程で抽出した前記測定点について前記測定点高さの測定に利用した測定光の前記第1の面または前記第2の面からの反射光の輝度である測定点輝度を対数変換して合計し積算輝度を算出する積算輝度算出工程と、
前記積算輝度と前記仮想面高さとの関係を示す曲線の変曲点を特定することにより前記境界面の位置を同定する同定工程を含む傾斜面境界位置同定方法。
A measurement light of a virtual surface of a boundary surface which is a plane including a boundary between the first surface and the second surface of a measurement object having a first surface and a second surface having different inclinations and having known design dimensions. the set with the inclination given in advance based on the design dimensions, while changing the virtual surface height is the distance between the virtual plane and the reference plane relative to a reference plane orthogonal to the measurement area including the boundary An extraction step of extracting those whose measurement point height, which is the distance from the reference plane optically measured, is smaller than the virtual plane height, among the measurement points in the
For the measurement point extracted in the extraction step, the measurement point brightness, which is the brightness of the reflected light from the first surface or the second surface of the measurement light used for measuring the measurement point height, is logarithmically converted. The integrated brightness calculation process that totals and calculates the integrated brightness, and
A method for identifying an inclined surface boundary position, which comprises an identification step of identifying the position of the boundary surface by specifying an inflection point of a curve showing a relationship between the integrated luminance and the virtual surface height.
前記抽出工程に先立って、前記測定点高さを光学的に測定すると共に前記測定点輝度を測定する測定工程を備えることを特徴とする請求項1に記載の傾斜面境界位置同定方法。 The method for identifying an inclined surface boundary position according to claim 1, further comprising a measurement step of optically measuring the height of the measurement point and measuring the brightness of the measurement point prior to the extraction step. 前記測定工程は、前記測定光の照射と反射光の検出を同軸上で行う距離計により行うことを特徴とする請求項2に記載の傾斜面境界位置同定方法。 The method for identifying an inclined surface boundary position according to claim 2, wherein the measurement step is performed by a range finder that irradiates the measurement light and detects the reflected light coaxially. 前記同定工程では、前記積算輝度と前記仮想面高さとの関係を示す曲線を微分し、微分値が所定の閾値となる前記仮想面高さを前記境界の位置とすることを特徴とする請求項1ないし請求項3のいずれか1項に記載の傾斜面境界位置同定方法。 The identification step is characterized in that a curve showing the relationship between the integrated luminance and the virtual surface height is differentiated, and the virtual surface height at which the differential value is a predetermined threshold value is set as the boundary position. The method for identifying an inclined surface boundary position according to any one of 1 to 3. 前記境界は閉じた図形であることを特徴とする請求項1ないし請求項4のいずれか1項に記載の傾斜面境界位置同定方法。 The method for identifying an inclined surface boundary position according to any one of claims 1 to 4, wherein the boundary is a closed figure. 前記測定対象物はバルブシートであり、前記第1の面はバルブ当たり面であり、前記第2の面は前記バルブ当たり面の外周に設けられ前記バルブ当たり面より傾斜の小さい外周面であり、前記仮想面の傾きは前記バルブ当たり面と前記バルブ当たり面の外周面が作る面の傾きであることを特徴とする請求項5 に記載の傾斜面境界位置同定方法。 The measurement object is a valve seat, said first surface is a surface per valve, said second surface Ri smaller outer circumference der inclination than the surface per valve provided on an outer periphery of surface per said valve the inclination of the imaginary plane inclined surface boundary localization method according to claim 5, wherein the inclination der Rukoto face the outer circumferential surface of the surface per valve and the valve contact surface make. 前記境界は開いた図形であることを特徴とする請求項1ないし請求項4のいずれか1項に記載の傾斜境界位置同定方法。 The inclined boundary position identification method according to any one of claims 1 to 4, wherein the boundary is an open figure. 互いに傾斜の異なる第1の面と第2の面を備える設計寸法が既知の測定対象物の前記第1の面と前記第2の面の境界を含む平面である境界面の仮想面測定光と直交する基準面に対して前記設計寸法に基づいて予め与えられた傾きで設定し、前記仮想面と前記基準面との距離である仮想面高さを変化させながら、前記境界を含む測定領域内の各測定点のうち光学的に測定された前記基準面からの距離である測定点高さが前記仮想面高さより小さいものを抽出する抽出手段と、
前記抽出手段で抽出した前記測定点について前記測定点高さの測定に利用した測定光の前記第1の面または前記第2の面からの反射光の輝度である測定点輝度を対数変換して合計し積算輝度を算出する積算輝度算出手段と、
前記積算輝度と前記仮想面高さとの関係を示す曲線の変曲点を特定することにより前記境界面の位置を同定する同定手段を含む傾斜面境界位置同定装置。
A measurement light of a virtual surface of a boundary surface which is a plane including a boundary between the first surface and the second surface of a measurement object having a first surface and a second surface having different inclinations and having known design dimensions. the set with the inclination given in advance based on the design dimensions, while changing the virtual surface height is the distance between the virtual plane and the reference plane relative to a reference plane orthogonal to the measurement area including the boundary An extraction means for extracting those whose measurement point height, which is the distance from the optically measured reference plane, is smaller than the virtual plane height, among the measurement points in the
For the measurement point extracted by the extraction means, the measurement point brightness, which is the brightness of the reflected light from the first surface or the second surface of the measurement light used for measuring the measurement point height, is logarithmically converted. An integrated brightness calculation means that totals and calculates the integrated brightness,
An inclined surface boundary position identification device including an identification means for identifying the position of the boundary surface by specifying an inflection point of a curve showing a relationship between the integrated luminance and the virtual surface height.
コンピュータに、
互いに傾斜の異なる第1の面と第2の面を備える設計寸法が既知の測定対象物の前記第1の面と前記第2の面の境界を含む平面である境界面の仮想面測定光と直交する基準面に対して前記設計寸法に基づいて予め与えられた傾きで設定し、前記仮想面と前記基準面との距離である仮想面高さを変化させながら、前記境界を含む測定領域内の各測定点のうち光学的に測定された前記基準面からの距離である測定点高さが前記仮想面高さより小さいものを抽出する抽出処理と、
前記抽出処理で抽出した前記測定点について前記測定点高さの測定に利用した測定光の前記第1の面または前記第2の面からの反射光の輝度である測定点輝度を対数変換して合計し積算輝度を算出する積算輝度算出処理と、
前記積算輝度と前記仮想面高さとの関係を示す曲線の変曲点を特定することにより前記境界面の位置を同定する同定処理を実行させる傾斜面境界位置同定プログラム。
On the computer
A measurement light of a virtual surface of a boundary surface which is a plane including a boundary between the first surface and the second surface of a measurement object having a first surface and a second surface having different inclinations and having known design dimensions. the set with the inclination given in advance based on the design dimensions, while changing the virtual surface height is the distance between the virtual plane and the reference plane relative to a reference plane orthogonal to the measurement area including the boundary Extraction processing for extracting those whose measurement point height, which is the distance from the reference plane optically measured, is smaller than the virtual plane height, among the measurement points in the
For the measurement point extracted by the extraction process, the measurement point brightness, which is the brightness of the reflected light from the first surface or the second surface of the measurement light used for measuring the measurement point height, is logarithmically converted. The integrated brightness calculation process that totals and calculates the integrated brightness,
An inclined surface boundary position identification program that executes an identification process for identifying the position of the boundary surface by specifying an inflection point of a curve showing the relationship between the integrated luminance and the virtual surface height.
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