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JPH0565083B2 - - Google Patents
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JPH0565083B2 - - Google Patents

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Publication number
JPH0565083B2
JPH0565083B2 JP20257786A JP20257786A JPH0565083B2 JP H0565083 B2 JPH0565083 B2 JP H0565083B2 JP 20257786 A JP20257786 A JP 20257786A JP 20257786 A JP20257786 A JP 20257786A JP H0565083 B2 JPH0565083 B2 JP H0565083B2
Authority
JP
Japan
Prior art keywords
straightness
measured
guide surface
value
detector
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP20257786A
Other languages
Japanese (ja)
Other versions
JPS6358108A (en
Inventor
Hiroaki Shimazutsu
Teruyuki Matsumoto
Junichi Nishizaki
Katsuzo Sudo
Hajime Ishikawa
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Ryomei Engineering Co Ltd
Mitsubishi Heavy Industries Ltd
Original Assignee
Ryomei Engineering Co Ltd
Mitsubishi Heavy Industries Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Ryomei Engineering Co Ltd, Mitsubishi Heavy Industries Ltd filed Critical Ryomei Engineering Co Ltd
Priority to JP20257786A priority Critical patent/JPS6358108A/en
Publication of JPS6358108A publication Critical patent/JPS6358108A/en
Publication of JPH0565083B2 publication Critical patent/JPH0565083B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 本発明は、測定対象物の真直度と移動案内面の
真直度および移動時の縦ゆれ量とを同時に高精度
で測定し得る方法に関する。 〔従来の技術〕 本発明は、本出願人等によつてすでに提案され
ている特願昭57−167561「真直度測定法」の改善
に関する。 近年、工作機械に対する高精度化への要求が高
まりつつあるなかで案内面(摺動面)の真直度管
理は重要な課題の一つとなつており、その測定の
容易化が望まれている。従来から行なわれている
真直度の測定方法としては、ストレートエツジ等
の基準バーやピアノ線を基準直線としたり、或い
はオートコリメータを利用する方法が知られてお
り、最近ではレーザ光による独立光学座標系を用
いた方法も開発されている。 ところが、これらの方法では、いずれも測定作
業に相当な準備と熟練度とが要求され、しかも能
率が悪い上に種々の雑音等による悪影響を受け易
い欠点があり、現場での実用化という点で多くの
問題を残している。 そこで、これらの問題を解決し得る真直度の新
しい測定方法として、三台の変位検出器を測定対
象物に沿つて移動させ、これら変位検出器による
測定値から逐次測定対象物の真直度と変位検出器
の移動案内面の真直度とを同時に測定する方法が
特願昭57−167561号にて報告されている。 これは、その原理を表わす第1図に示すよう
に、測定対象物1に沿つて案内面2上を移動する
検出器取付台3(例えば刃物取付台を利用)に測
定対象物1との距離を測定する3個の変位検出器
A,B,Cを、検出器取付台3の移動方向に一定
距離lを隔てて並置し、この検出器取付台3を図
中の矢印方向に移動して移動距離l毎に3個の変
位検出器A,B,Cの測定値を得、これら測定値
から逐次測定対象物1の真直度および案内面2の
真直度を分離して算出する方法である。 すなわち、測定開始位置における測定対象物1
および案内面2の真直度をそれぞれY0、X0とし、
K番目の測定位置における真直度をそれぞれYK
XKとすると、第1図中にYおよびXでそれぞれ
示される測定対象物1および案内面2の真直度曲
線が得られる(第1図では簡単のため区間毎の直
線で近似して示した)。 ここで、K番目の測定位置での変位検出器A,
B,Cでの測定値をDKA、DKB、DKC(K=0、1、
2、…)とすると、次式(1)、(2)、(3)が成立する。 DKA−YK−XK=DOA ……(1) DKB−YK+1−XK−l・θK=DOB−Y1−X0 ……(2) DKC−YK+2−XK−2l・θK=DOC−Y2−X0 ……(3) ただし、θKは図にも示すように検出器取付台3
のピツチング量である。 (2)式および(3)式を2×(2)式−(3)式に変形すると
次式(4)が得られる。 2DKB−DKC=XK +2YK+1−YK+2 −2Y1+Y2−X0 ……(4) また、(1)式において、K→K+1、K→K+2
とすることによつて得たYK+1、YK+2を(4)式に代
入すると、次式(5)が得られる。 XK+2=2・XK+1−XK −2・DK+1A+DK+2A +2DKB−DKC+2Y1−Y2+X0 ……(5) さらに、(2)式、(5)式および(1)式から求めた
YK+2により次式(6)、(7)が得られる。 YK+2=−XK+2+DK+2A ……(6) θK+2=−XK+2−YK+3+DK+2B+X0+Y1/l ……(7) ただし、(4)〜(7)式で測定開始位置での各変位検
出器A,B,Cの測定値DOA、DOB、DOCを0とし
た。 こうして、K=0、1、2、…の位置での変位
検出器A,B,Cの測定値DKA、DKB、DKCを用い
て、上記(5)式、(6)式および(7)式から逐次、測定対
象物1の真直度曲線Y、案内面2の真直度曲線X
および検出器取付台3のピツチングθを算出する
ことができる。 ところが、上記の算出方法において、X0、X1
Y1、Y2は(5)式、(6)式の漸化式からは求めること
ができない値であり、真直度曲線X、Yを求める
ためには、なんらかの方法、これらの値を推定す
るか、またはその影響分を除去する必要がある。
このための方法として特願昭57−167561号には次
の方法が提案されている。 すなわち、(5)式において、X1=α、2Y1−Y2
=β、X0=γ、とおくと、次式(8)が成立する。 XK=K・(α−γ)+K(K−1)/2 ・(β+γ)+CK ……(8) (K=2、3、…) XK:K番目の位置での真直度誤差(真の値) CK:K番目の位置での真直度誤差(計算値) また、このCKはα=β=γ=0と仮定して(5)
式により求めたXKの値である。 ここで、真直度誤差を『各測定点での誤差の二
乗平均値が最小になるような仮想直線からのへだ
たり』としてとらえることとすれば、最小二乗法
によつてXKの二乗平均値を最小とするようなα、
β、γを求め、このα、β、γ及びCKを用いて
(8)式によつてXKを求めることができる。そして
XKと(6)式とからYKを求める。 以上のような従来技術によれば、測定対象物1
の真直度と移動案内面2の真直度及び移動時の縦
ゆれ量とを同時に求めることができる。 〔発明が解決しようとする問題点〕 しかし、前記第(8)式から判るように、移動案内
面の真直度形状中に含まれるK2に比例する成分、
すなわちXK=b・K2と表現できる成分について
は、その係数bを(8)式の(β−γ)中に含めて評
価してしまいその成分を正しく求めることができ
ない。このことを第2図および第1表により説明
する。なお、Kに比例する成分すなわちXK
a・Kと表現できる成分については(8)式中の(α
−γ)に含めて評価される。しかし、真直度誤差
をある仮想直線からのへだたりとしてとらえる方
法である為、このことは真直度形状の評価には影
響を及ぼさない。さて、第2図は模擬データと演
算結果を示したものであり、第1表はその時の入
力データと演算結果を示している。また、第2図
中・印は模擬データであり○印は第1表中の計算
結果を示している。
[Industrial Application Field] The present invention relates to a method for simultaneously and highly accurately measuring the straightness of an object to be measured, the straightness of a moving guide surface, and the amount of pitch during movement. [Prior Art] The present invention relates to an improvement of Japanese Patent Application No. 57-167561 "Straightness Measuring Method" which has already been proposed by the present applicant and others. In recent years, with the increasing demand for higher precision in machine tools, the straightness control of guide surfaces (sliding surfaces) has become one of the important issues, and it is desired to make its measurement easier. Conventional methods for measuring straightness include using a reference bar such as Straight Edge, a piano wire as a reference straight line, or using an autocollimator. A system-based method has also been developed. However, all of these methods require a considerable amount of preparation and skill for measurement work, are inefficient, and are susceptible to adverse effects from various noises, etc., making them difficult to put to practical use in the field. Many problems remain. Therefore, as a new method for measuring straightness that can solve these problems, three displacement detectors are moved along the object to be measured, and the straightness and displacement of the object to be measured are sequentially calculated from the measured values by these displacement detectors. A method for simultaneously measuring the straightness of the moving guide surface of the detector is reported in Japanese Patent Application No. 167561/1983. As shown in Figure 1, which shows the principle, this is because the distance between the detector mount 3 (using a knife mount, for example) that moves along the measurement object 1 on the guide surface 2 and the measurement object 1 is Three displacement detectors A, B, and C that measure This is a method in which the measured values of three displacement detectors A, B, and C are obtained for each moving distance l, and the straightness of the object to be measured 1 and the straightness of the guide surface 2 are calculated separately from these measured values. . In other words, the measurement target 1 at the measurement start position
and the straightness of the guide surface 2 are Y 0 and X 0 respectively,
Let the straightness at the Kth measurement position be Y K and
If X K , then the straightness curves of the object to be measured 1 and the guide surface 2, respectively indicated by Y and ). Here, the displacement detector A at the Kth measurement position,
The measured values at B and C are D KA , D KB , D KC (K=0, 1,
2,...), the following equations (1), (2), and (3) hold true. D KA −Y K −X K =D OA …(1) D KB −Y K+1 −X K −l・θ K =D OB −Y 1 −X 0 …(2) D KC −Y K +2 −X K −2l・θ K = D OC −Y 2 −X 0 ...(3) However, θ K is the detector mounting base 3 as shown in the figure.
pitching amount. By transforming equations (2) and (3) into 2×(2)−(3), the following equation (4) is obtained. 2D KB −D KC = _ _ _
By substituting Y K+1 and Y K+2 obtained by , into equation (4), the following equation (5) is obtained. X K + 2 = 2 . _ _ _ Obtained from equation 5) and equation (1)
The following equations (6) and (7) are obtained by Y K+2 . Y K+2 =−X K+2 +D K+2A ……(6) θ K+2 =−X K+2 −Y K+3 +D K+2B +X 0 +Y 1 /l ……(7) However , (4) to (7), the measured values D OA , D OB , and D OC of each displacement detector A, B, and C at the measurement start position were set to 0. In this way, using the measured values D KA , D KB , and D KC of the displacement detectors A, B, and C at the positions of K=0, 1, 2, and so on, the above equations (5), (6), and ( 7) From equation 1, straightness curve Y of measurement object 1, straightness curve X of guide surface 2
And the pitching θ of the detector mount 3 can be calculated. However, in the above calculation method, X 0 , X 1 ,
Y 1 and Y 2 are values that cannot be obtained from the recurrence formulas of equations (5) and (6), and in order to obtain the straightness curves X and Y, these values must be estimated by some method. or its influence must be removed.
As a method for this purpose, the following method is proposed in Japanese Patent Application No. 167561/1983. That is, in equation (5), X 1 = α, 2Y 1 −Y 2
=β, X 0 =γ, the following equation (8) holds true. X K = K・(α−γ)+K(K−1)/2 ・(β+γ)+C K ……(8) (K=2, 3,…) X K : Straightness error at Kth position (True value) C K : Straightness error at the Kth position (calculated value) Also, assuming that α=β=γ=0 , (5)
This is the value of X K determined by the formula. Here, if we consider the straightness error as ``the deviation from the virtual straight line that minimizes the root mean square value of the error at each measurement point,'' then we can use the least squares method to calculate the square mean of X K. α such that the value is minimized,
Find β and γ and use these α, β, γ and C K to
X K can be found using equation (8). and
Find Y K from X K and equation (6). According to the conventional technology as described above, the measurement object 1
The straightness of the moving guide surface 2, the straightness of the moving guide surface 2, and the amount of vertical wobbling during movement can be determined simultaneously. [Problem to be solved by the invention] However, as can be seen from the above equation (8), the component proportional to K 2 included in the straightness shape of the moving guide surface,
That is, for a component that can be expressed as X K =b·K 2 , the coefficient b is included in (β−γ) in equation (8) and evaluated, making it impossible to correctly determine the component. This will be explained with reference to FIG. 2 and Table 1. Note that the component proportional to K, that is, X K =
For the component that can be expressed as a・K, (α
−γ). However, since this method considers the straightness error as a deviation from a certain virtual straight line, this does not affect the evaluation of the straightness shape. Now, FIG. 2 shows the simulated data and calculation results, and Table 1 shows the input data and calculation results at that time. In addition, the marks in FIG. 2 are simulated data, and the marks ○ indicate the calculation results in Table 1.

〔問題点を解決するための手段〕[Means for solving problems]

かかる目的を達成するための手段は次の通りで
ある。 (i) 検出器取付台と測定対象物とのいずれか一方
が案内面に沿つて移動する該検出器取付台に前
記測定対象物とのへだたりを測定する3個の検
出器を前記移動方向に等間隔lで載置し、 (ii) 前記3個の検出器を前記検出器取付台上に載
置した状態で十分真直な基準対象物とのへだた
り量を測定し、その時のA,B,C3個の検出
量での測定値DA、DB、DCから検出器の載置状
態によつて定まる量C(≡DA+DC−2・DB)を
求め、 (iii) 前記検出器取付台もしくは測定対象物を前記
間隔l毎に移動してその都度前記測定値を得、
測定開始位置での前記測定値をDO,A、DO,B
DO,Cとし、K番目の測定位置における値をそれ
ぞれDK,A、DK,B、DK,Cとして該測定値と前記の
値Cとから aK=DK,A+DK,C−2・DK,B/2−Cなる値を得、 K=0、1、2、…Nに対するaKの平均値=
NK=1 ak/(N+1)を求め、 (iv) これらの測定値DK,A、DK,B、DK,C(K=0、
1、2、…)によつて、前記(1)式〜(8)式の手順
に沿つて案内面の真直度形状XK(K=0、1、
2、…)との測定対象物の真直度形状YK(K=
0、1、2、…)を得、 (v) 例えば最小自乗法によつて、該測定対象物形
状YKが最も確からしくあてはまる曲線YK
a′・K2+b′・K+c′を求め、 (vi) 該曲線の係数a′と前記の項とによつて YK′=YK−(a′−)・K2 ……(9) XK′=XK+(a′−)・K2 ……(10) として測定対象物の真直度形状YK′と案内面の
真直度形状XK′を求める。 〔実施例〕 以下、本発明の実施例について説明する。 第1図からわかるように、K番目、(K+1)
番目、(K+2)番目の測定位置での測定対象物
形状YK、YK+1、YK+2と各検出器での測定値との
間には次のような関係が成り立つ。 YK−2・YK+1+YK+2 =DK,A−2・DK,B +DK,C−2・C ……(11) 一方、YK=aK・K2+bK・K+CKとすれば、次
式の関係が成立する。 YK−2・YK+1+YK+2=2・aK ……(12) (11)式及び(12)式から測定対象物形状YK(K=0、
1、2、…)中のK2に比例する成分の係数aKは aK=DK,A+DK,C−2・DK,B/2−C ……(3) となる。K=0、1、2、…の測定位置で求めた
aKの平均値が測定範囲全体を通じてのK2に比
例する成分となつている。K2に比例する形状成
分のみについて考えれば、(1)式〜(8)式の手順に沿
つて求めた測定対象物の真直度形状YKは真の測
定対象物形状に案内面の形状が加算された為のも
のであり、(1)式〜(8)式の手順に沿つて演算結果か
らこの成分a′・K2を引き去り、本発明の手順に
よつて求めた真の成分・K2を加算すればよい
ことになる。同様に、(10)式によつて、真の案内面
真直度形状が求められる。 〔発明の効果〕 以上説明したように本発明によれば、移動案内
面の真直度形状誤差にK2に比例する成分が含ま
れる場合に於ても、その影響分を補正して、測定
対象物の真直度と移動案内面の真直度及び移動時
の縦ゆれ量とを同時に高精度で測定することがで
きる。また、測定には3個の検出器を設置すれば
良く実機にも簡単に適用できると共に測定作業も
簡単で熟練度も必要としない。
The means to achieve this objective are as follows. (i) Either the detector mount or the object to be measured moves along the guide surface, and the three detectors for measuring the distance from the object to be measured are moved to the detector mount, which moves along the guide surface. (ii) With the three detectors placed on the detector mount, measure the amount of separation from a sufficiently straight reference object, and then Calculate the amount C (≡D A + D C -2・D B ) determined by the mounting state of the detector from the measured values D A , D B , and D C of the three detected amounts A, B, and C, and calculate ( iii) moving the detector mount or the object to be measured every interval l and obtaining the measured value each time;
The measured values at the measurement start position are D O,A , D O,B ,
Let D O,C be the values at the Kth measurement position, and let the values at the Kth measurement position be D K,A , D K,B , and D K,C , and from the measured values and the above value C, a K = D K,A + D K, Obtain the value C −2・D K,B /2−C, and average value of a K for K=0, 1, 2,...N=
NK=1 ak/(N+1), (iv) These measured values D K,A , D K,B , D K,C (K=0,
1, 2, ...), the straightness shape of the guide surface X K (K=0, 1,
2,...) and the straightness shape of the object to be measured Y K (K=
0, 1, 2, ...), and (v) For example, by the least squares method, find the curve Y K = to which the shape of the object to be measured Y K most likely fits.
Find a′・K 2 +b′・K+c′, (vi) Y K ′=Y K −(a′−)・K 2 ……(9) Find the straightness shape Y K of the object to be measured and the straightness shape X K ′ of the guide surface as follows: [Examples] Examples of the present invention will be described below. As can be seen from Figure 1, the Kth, (K+1)
The following relationships hold between the shapes of the object to be measured Y K , Y K+1 , Y K+2 at the (K+2)th and (K+2)th measurement positions and the measured values at each detector. Y K −2・Y K+1 +Y K+2 =D K,A −2・D K,B +D K,C −2・C ……(11) On the other hand, Y K =a K・K 2 +b K・If K+C K , the following relationship holds true. Y K −2・Y K+1 +Y K+2 =2・a K ...(12) From equations (11) and (12), the shape of the object to be measured Y K (K=0,
The coefficient a K of the component proportional to K 2 in 1, 2, ...) is a K = D K,A +D K,C -2.D K,B /2-C (3). Obtained at measurement positions of K=0, 1, 2,...
a The average value of K is a component proportional to K 2 over the entire measurement range. If only the shape component proportional to K 2 is considered, the straightness shape Y K of the object to be measured obtained according to the steps of equations (1) to (8) will be determined by the fact that the shape of the guide surface is equal to the true shape of the object to be measured. This component a′・K 2 is subtracted from the calculation result according to the steps of equations (1) to (8), and the true component・K obtained by the procedure of the present invention is All you have to do is add 2 . Similarly, the true guide surface straightness shape can be found using equation (10). [Effects of the Invention] As explained above, according to the present invention, even when the straightness shape error of the movable guide surface includes a component proportional to K 2 , the influence can be corrected and the measurement target can be corrected. The straightness of an object, the straightness of a moving guide surface, and the amount of vertical wobbling during movement can be simultaneously measured with high precision. In addition, it is only necessary to install three detectors for measurement, and it can be easily applied to actual equipment, and the measurement work is simple and does not require any skill.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は真直度測定方法にかかる原理図、第2
図は模擬データと計算結果とを示す真直度曲線
XK、YK、およびピツチングθKのグラフである。 図面中、1は測定対象物、2は案内面、3は検
出器取付台、A,B,Cは変位検出器である。
Figure 1 is a principle diagram of the straightness measurement method, Figure 2
The figure shows a straightness curve showing simulated data and calculation results.
It is a graph of X K , Y K , and pitching θ K . In the drawings, 1 is an object to be measured, 2 is a guide surface, 3 is a detector mounting base, and A, B, and C are displacement detectors.

Claims (1)

【特許請求の範囲】 1 検出器取付台と測定対象物とのいずれか一方
が案内面に沿つて移動する該検出器取付台に前記
測定対象物との距離を測定する3個の検出器を前
記移動方向に等間隔lで設置し、測定開始位置に
おける前記3個の検出器の測定値をそれぞれ
DOA、DOB、DOCとし、前記検出器取付台若しくは
測定対象物を前記間隔l毎に移動してその都度前
記検出器の測定値を得、K番目の測定位置におけ
る前記測定値をそれぞれDKA、DKB、DKCとし、測
定開始位置での案内面真直度誤差をX0、1番目
の位置のそれをX1、1番目の位置での測定対象
物の真直度誤差をY1、2番目の位置でのそれを
Y2とし、K+2番目位置での前記案内面の真直
度XK+2を XK+2=2・XK+1−XK−2・DK+1A+DK+2A+2・DKB
−DKC+2Y1−Y2+X0 によつて算出し、K=0、1、2、…について算
出したXK+2の値を、真直度誤差の二乗平均値が
最小となるよう演算した求めてX0、X1および
Y1、Y2に関係する数値によつて補正して前記案
内面の真直度XK、(K=0、1、2、…)を推
定・算出し、この位置における前記測定対象物の
真直度YK+2を YK+2=−XK+2+DK+2A によつて算出し、前記3個の検出器を前記検出器
取付台上に載置した状態で、十分真直な基準対象
物とのへだたり量を測定し、その時のA、B、
C3個の検出器での測定値DA、DB、DCから、C=
DA+DC−2・DBなる値を求め、前記K=0、1、
2、…の測定位置における検出器での測定値
DK,A、DK,B、DK,Cと前記の値Cとから、 aK=DK,A+DK,C−2・DK,B/2−Cなる値を得、K =0、1、2、…に対するaKの平均値=NK=1
aK/(N+1)を求め、前記算出した測定対象物
真直度形状YK(K=0、1、2、…)が最も確か
らしくあてはまる曲線YK=a′・K2+b′・K+c′を
求め、該曲線の係数a′と前記の値とによつて YK′=YK−(a′−)・K2 XK′=XK+(a′−)・K2 として測定対象物の真直度形状YK′と案内面の真
直度形状XK′とを求めることを特徴とする真直度
形状測定方法。
[Claims] 1. Either the detector mount or the object to be measured moves along a guide surface, and the detector mount is provided with three detectors for measuring the distance to the object to be measured. The three detectors are installed at equal intervals l in the movement direction, and the measured values of the three detectors at the measurement start position are respectively
D OA , D OB , D OC , the detector mounting base or the object to be measured is moved every interval l to obtain the measured value of the detector each time, and the measured value at the Kth measurement position is respectively Let D KA , D KB , and D KC be the guide surface straightness error at the measurement start position as X 0 , that at the first position as X 1 , and the straightness error of the object to be measured at the first position as Y 1 , that in the second position
Let Y 2 be the straightness of the guide surface at the K + 2nd position .
-D KC + 2Y 1 -Y 2 + Find X 0 , X 1 and
The straightness X K , (K=0, 1, 2,...) of the guide surface is estimated and calculated by correcting it with the values related to Y 1 and Y 2 , and the straightness of the measurement target at this position is calculated. Calculate the degree Y K+2 by Y K+2 = −X K+2 +D K+2A , and with the three detectors mounted on the detector mount, make sure that the standard is sufficiently straight. Measure the amount of separation from the object, and then measure A, B,
From the measured values D A , D B , D C at C3 detectors, C=
Find the value D A +D C -2・D B , and calculate the above K=0, 1,
2. Measured value with the detector at the measurement position of...
From D K,A , D K,B , D K,C and the above value C, we obtain the value a K = D K,A + D K,C −2・D K,B /2−C, and K = Average value of a K for 0, 1, 2,... = NK=1
Find a K / (N+1) and find the curve to which the straightness shape of the measured object Y K (K=0, 1, 2,...) calculated above most likely applies: Y K = a′・K 2 +b′・K +c ′ is determined and measured as Y K ′=Y K −(a′−)・K 2 X K ′=X K +(a′−)・K 2 using the coefficient a′ of the curve and the above value. A straightness shape measuring method characterized by determining the straightness shape Y K ′ of an object and the straightness shape X K ′ of a guide surface.
JP20257786A 1986-08-28 1986-08-28 Measurement of straightness Granted JPS6358108A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20257786A JPS6358108A (en) 1986-08-28 1986-08-28 Measurement of straightness

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20257786A JPS6358108A (en) 1986-08-28 1986-08-28 Measurement of straightness

Publications (2)

Publication Number Publication Date
JPS6358108A JPS6358108A (en) 1988-03-12
JPH0565083B2 true JPH0565083B2 (en) 1993-09-17

Family

ID=16459793

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20257786A Granted JPS6358108A (en) 1986-08-28 1986-08-28 Measurement of straightness

Country Status (1)

Country Link
JP (1) JPS6358108A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5009653B2 (en) * 2007-03-15 2012-08-22 株式会社岡本工作機械製作所 Method and apparatus for measuring surface shape of long body

Also Published As

Publication number Publication date
JPS6358108A (en) 1988-03-12

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