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JPH0610645B2 - Stress intensity factor measuring gauge, stress intensity factor measuring method, and remaining life monitoring device for cracked member - Google Patents
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JPH0610645B2 - Stress intensity factor measuring gauge, stress intensity factor measuring method, and remaining life monitoring device for cracked member - Google Patents

Stress intensity factor measuring gauge, stress intensity factor measuring method, and remaining life monitoring device for cracked member

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Publication number
JPH0610645B2
JPH0610645B2 JP21195086A JP21195086A JPH0610645B2 JP H0610645 B2 JPH0610645 B2 JP H0610645B2 JP 21195086 A JP21195086 A JP 21195086A JP 21195086 A JP21195086 A JP 21195086A JP H0610645 B2 JPH0610645 B2 JP H0610645B2
Authority
JP
Japan
Prior art keywords
crack
intensity factor
stress intensity
gauge
stress
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
JP21195086A
Other languages
Japanese (ja)
Other versions
JPS6366428A (en
Inventor
義康 伊藤
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP21195086A priority Critical patent/JPH0610645B2/en
Publication of JPS6366428A publication Critical patent/JPS6366428A/en
Publication of JPH0610645B2 publication Critical patent/JPH0610645B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、き裂が生じた部材、ならびにき裂状切欠(以
下、き裂等という)を有する部材(以下、き裂部材とい
う)の先端部における応力拡大係数を非破壊的に測定す
る応力拡大係数測定用ゲージ、応力拡大係数測定方法お
よび前記き裂部材の余寿命を監視するき裂部材の余寿命
監視装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Field of Industrial Application) The present invention relates to a member having a crack, and a member having a crack-like notch (hereinafter, referred to as a crack) (hereinafter, referred to as a crack). A stress intensity factor measuring gauge for non-destructively measuring the stress intensity factor at the tip of a crack member, a stress intensity factor measuring method, and a remaining life monitoring device for a crack member for monitoring the remaining life of the crack member. .

(従来の技術) 一般に、欠陥を有していたり、あるいは使用中にき裂が
生じた構造物を安全に使用するために、破壊力学に基づ
いて各種の評価を行なっている。
(Prior Art) Generally, various evaluations are performed based on fracture mechanics in order to safely use a structure having a defect or a crack generated during use.

特に、今日では、破壊力学の基礎となるき裂を有するき
裂部材のき裂先端近傍の応力状態を代表するパラメータ
として、応力拡大係数という概念が提案されたことによ
り、線形破壊力学において、き裂を有するき裂部材の破
壊挙動を実用的に十分な精度で取扱うことができるよう
になった。すなわち、種々の形状のき裂部材について応
力拡大係数が解折され一般の利用に供され、構造物の安
全性が確保されている。
In particular, today, the concept of the stress intensity factor has been proposed as a parameter representing the stress state near the crack tip of a crack member having a crack that is the basis of fracture mechanics. It became possible to handle the fracture behavior of a cracked member with cracks with practically sufficient accuracy. That is, the stress intensity factors of crack members of various shapes are broken and provided for general use to ensure the safety of the structure.

ところが、応力拡大係数の解析解が得られているもの
は、比較的単純な形状のものであり、他の多くは大型電
算機を用いた数値解析しなければならないのが現状であ
る。しかしながら、実際の構造物においては、き裂まで
を考慮した数値解析が電算機の容量不足、あるいは境界
条件が不明確等の理由より正確に実施することができな
い場合もある。
However, the solution for which the stress intensity factor has been obtained has a relatively simple shape, and many others require numerical analysis using a large-scale computer. However, in an actual structure, there are cases where the numerical analysis considering even cracks cannot be performed accurately due to insufficient computer capacity or unclear boundary conditions.

そこで、最近では実際の構造物に生じた欠陥、あるいは
き裂に対して実験的な応力解析により応力拡大係数を求
めることが試みられている。
Therefore, recently, it has been attempted to obtain a stress intensity factor by experimental stress analysis for a defect or a crack generated in an actual structure.

すなわち、第8図に示す様に円形の薄いゲージベース1
1の上に2個の3軸ロゼット抵抗線ひずみゲージ12,
12を固着して形成されている応力拡大係数測定用ゲー
ジを本発明者自身が既に提案している(特願昭60−2
16810号参照)。
That is, as shown in FIG. 8, a circular thin gauge base 1
Two 3-axis rosette resistance wire strain gauges 12 on top of 1,
The present inventors have already proposed a stress intensity factor measuring gauge formed by fixing 12 (Japanese Patent Application No. 60-2).
16810).

このゲージパターンを詳述すると、各3軸ロゼット抵抗
線ひずみゲージ12のゲージ中心0の間の距離Lを、
応力拡大係数を測定すべきき裂あるいはき裂状状切欠の
全長の1/10以下に設定し、かつ、各ゲージ中心0とゲー
ジベース11の端縁との最短距離Lを同じくき裂等の
全長の1/10以下に設定している。
Explaining this gauge pattern in detail, the distance L 1 between the gauge centers 0 of the triaxial rosette resistance wire strain gauges 12 is
The stress intensity factor is set to 1/10 or less of the total length of the crack or crack-like notch to be measured, and the shortest distance L 2 between each gauge center 0 and the edge of the gauge base 11 is set to The length is set to 1/10 or less.

そして、このような応力拡大係数測定用ゲージを用い
て、本発明者が開発した比例外挿法(第9図に詳細を示
す)により応力拡大係数を決定する。すなわち、応力拡
大係数測定用ゲージを第9図(a)に示すように、ゲー
ジベース11をもってき裂13の先端部に貼付し、この
状態で各3軸ロゼット抵抗線ひずみゲージ12より第9
図(a)のrおよびrの位置の応力を求める。そし
て、その応力値にあらかじめ、そのゲージパターンに対
して求めておいた較正係数を乗じて、第9図(b)に示
すように、き裂先端(r=0)へ外挿し(これを比例外
挿法と呼ぶ)応力拡大係数を決定する。この応力拡大係
数と予め記憶してある材料定数の疲労き裂伝ぱ速度との
関係から、き裂部材の余寿命を評価する余寿命監視装置
を提案している。
Then, using such a stress intensity factor measuring gauge, the stress intensity factor is determined by the ratio exception insertion method (details are shown in FIG. 9) developed by the present inventor. That is, as shown in FIG. 9 (a), a stress intensity factor measuring gauge is attached to the tip of the crack 13 with the gauge base 11, and in this state, the triaxial rosette resistance wire strain gauge 12
The stress at the positions of r 1 and r 2 in FIG. Then, the stress value is multiplied by the calibration coefficient obtained for the gauge pattern in advance, and extrapolated to the crack tip (r = 0) as shown in FIG. The stress intensity factor is determined. From the relationship between the stress intensity factor and the fatigue crack propagation rate of the material constant stored in advance, a remaining life monitoring device for evaluating the remaining life of the crack member is proposed.

(発明が解決しようとする問題点) しかしながら、以前の提案には更に工夫する必要があっ
た。
(Problems to be Solved by the Invention) However, it was necessary to further devise the previous proposal.

すなわち、実際の構造部材においては、通常降伏応力の
1/2あるいは2/3程度の応力が作用するため応力拡大係数
測定用ゲージを、き裂13のごく先端近傍に貼付する
と、き裂先端の塑成変形のために応力拡大係数算定精度
が低下する。また、応力拡大係数測定用ゲージをき裂先
端からの規定位置に貼付することは困難な作業であり、
貼付位置にずれが発生すると、そのずれが、応力拡大係
数算定精度に大きな影響を及ぼす。更に実際の疲労き裂
の余寿命評価にあたっては疲労き裂の開閉口の挙動を明
確に把握しないと評価精度がきわめて悪くなる。すなわ
ち、疲労き裂は外荷重により開閉内を繰返して伝ぱする
が、その途中でき裂面の微視的な塑性変形あるいは酸化
物発生等により、必ずしも外荷重が引張であっても開口
しているとは限らず、閉口していることがあり、実際に
疲労き裂が開口している有効な応力拡大係数範囲を把握
する必要がある。
That is, in actual structural members, the yield stress
If a stress intensity factor measuring gauge is attached near the very tip of the crack 13 because a stress of about 1/2 or 2/3 is applied, the stress intensity factor calculation accuracy decreases due to plastic deformation of the crack tip. To do. Also, it is a difficult task to attach the stress intensity factor measuring gauge to the specified position from the crack tip.
When the attachment position is displaced, the displacement has a great influence on the calculation accuracy of the stress intensity factor. Furthermore, in the actual evaluation of the remaining life of a fatigue crack, the evaluation accuracy will be extremely poor unless the behavior of the opening / closing port of the fatigue crack is clearly understood. That is, a fatigue crack propagates repeatedly inside and outside due to an external load, but it is always open even when the external load is tensile due to microscopic plastic deformation of the crack surface or oxide generation in the middle of the fatigue crack. However, it is not always the case, and it may be closed, and it is necessary to grasp the effective stress intensity factor range in which the fatigue crack is actually open.

このような測定、評価の高精度化の実現が強く望まれて
いる。
It is strongly desired to realize such high accuracy of measurement and evaluation.

なぜなら、き裂が発生した場合に停止不可能な公共機械
も多いからである。また、緊急停止が不可能な機械にお
いても余寿命が十分あるのにただちに停止させて補修を
行なうのでは多大な損失を生じることとなり、また、定
量的な余寿命評価ができないままに、き裂を生じた機械
の運転を継続することは機械の大破壊を誘発させるおそ
れがある。
This is because many public machines cannot be stopped when a crack occurs. In addition, even in a machine where emergency stop is not possible, if the machine has a sufficient remaining life and is immediately stopped for repair, a large loss will occur, and cracks will be generated without quantitative remaining life evaluation. Continuing to operate the machine that has caused the risk may cause a major destruction of the machine.

本発明はこれらの点に鑑みてなされてものであり、き裂
部材のき裂先端部における応力拡大係数を、簡単な構成
でしかも高い精度で測定することのできる応力拡大係数
測定用ゲージと、この応力拡大係数測定用ゲージを用い
て、応力拡大係数を求めることのできる応力拡大係数測
定方法と、き裂部材の余寿命を高精度で求めて監視する
ことのできるき裂部材の余寿命監視装置とを提供するこ
とを目的とする。
The present invention is made in view of these points, the stress intensity factor at the crack tip of the crack member, a stress intensity factor measurement gauge that can be measured with a simple configuration and with high accuracy, Using this stress intensity factor measurement gauge, a stress intensity factor measuring method that can determine the stress intensity factor and a residual life monitoring of the crack member that can accurately determine and monitor the remaining life of the crack member It is intended to provide a device.

〔発明の構成〕[Structure of Invention]

(問題点を解決するための手段) 本発明の第1の発明の応力拡大係数測定用ゲージは、ゲ
ージベースの上に2個の3軸抵抗線ひずみゲージを間隔
をおいて取付け、前記ゲージベースをき裂部材のき裂近
傍に貼付した時に、き裂の延長線上に上記2個の3軸抵
抗線ひずみゲージの各ゲージ中心が位置するように配設
されてなることを特徴とする。
(Means for Solving Problems) A gauge for stress intensity factor measurement according to the first aspect of the present invention is configured such that two triaxial resistance line strain gauges are mounted on a gauge base with a space therebetween. Is attached in the vicinity of the crack of the crack member, the gauge centers of the two triaxial resistance line strain gauges are arranged on the extension line of the crack.

本発明の第2の発明は、ゲージベースの上に2個の3軸
抵抗線ひずみゲージを間隔をおいて取付け、前記ゲージ
ベースをき裂部材のき裂近傍に貼付した時に、き裂の延
長線上に上記2個の3軸抵抗線ひずみゲージのゲージ中
心が位置するように配設されてなる応力拡大係数測定用
ゲージを、き裂部材のき裂先端近傍に貼付し、次に前記
各3軸抵抗線ひずみゲージによって応力を検出し、この
検出応力に基づいて下式(1)(2) ただし、 σy|θ=0 :き裂の進行方向と直交する方向の引
張応力 τxy|θ=0 :せん断応力 r :き裂先端からの距離 α,αII:較正係数 T:き裂縁に外力が作用する場合の引張断力 Txy:き裂縁に外力が作用する場合のせん断力 により、各3軸抵抗線ひずみゲージの検出応力に較正係
数を乗じ、これをき裂先端へ外挿することにより応力拡
大係数を求めることを特徴とする。
A second aspect of the present invention is the extension of a crack when two triaxial resistance wire strain gauges are mounted on a gauge base at intervals and the gauge base is attached near the crack of a crack member. A stress intensity factor measuring gauge, which is arranged so that the gauge centers of the two triaxial resistance strain gauges are located on the line, is attached near the crack tip of the crack member, and then each of the above 3 Stress is detected by the axial resistance wire strain gauge, and the following equations (1) and (2) are used based on the detected stress. However, σ y | θ = 0 : Tensile stress in the direction orthogonal to the crack propagation direction τ xy | θ = 0 : Shear stress r: Distance from the crack tip α I , α II : Calibration coefficient T y : Crack Tensile breaking force when an external force acts on the crack edge T xy : The shearing force when an external force acts on the crack edge multiplies the detected stress of each triaxial resistance line strain gauge by a calibration coefficient, and this is the crack tip. It is characterized in that the stress intensity factor is obtained by extrapolating to.

本発明の第3の発明のき裂部材の余寿命監視装置は、ゲ
ージベースの上に2個の3軸抵抗線ひずみゲージを間隔
をおいて取付け、前記ゲージベースをき裂部材のき裂近
傍に貼付した時に、き裂延長線上に上記2個の3軸抵抗
線ひずみゲージのゲージ中心が位置するように配設され
てなる応力拡大係数測定用ゲージを、き裂部材のき裂先
端近傍に貼付し、次に前記各3軸抵抗線ひずみゲージに
よって応力を検出し、応力拡大係数を算出する応力拡大
係数演算器と、き裂縁部に新たに貼付したき裂開閉口点
測定用抵抗線ひずみゲージの出力により、き裂の開閉口
点を算出する開閉口点演算器と、この応力拡大係数とき
裂の開閉口点から有効応力拡大係数範囲を算出し、この
有効応力拡大係数範囲と予め記憶してある材料定数とを
比較してき裂部材の残余寿命を求める評価器とを有する
ことを特徴とする。
A third aspect of the present invention is a crack member residual life monitoring apparatus, in which two triaxial resistance line strain gauges are mounted on a gauge base at intervals, and the gauge base is located near the crack of the crack member. A stress intensity factor measuring gauge, which is arranged so that the gauge centers of the two triaxial resistance line strain gauges are located on the crack extension line when it is attached to the crack extension line near the crack tip of the crack member. A stress intensity factor calculator for pasting and then detecting stress with each of the triaxial resistance wire strain gauges, and a stress intensity factor calculator for calculating the stress intensity factor, and a resistance line for crack opening / closing point measurement newly attached at the crack edge portion. The opening and closing point calculator that calculates the opening and closing points of the crack from the output of the strain gauge, and the effective stress intensity factor range is calculated from this stress intensity factor and the opening and closing point of the crack. The cracked member is compared with the stored material constant. And having an evaluation device for determining the residual lifetime.

(作用) 本発明の第1の発明の応力拡大係数測定用ゲージによれ
ば、2個の3軸ロゼット抵抗線ひずみゲージを、それぞ
れのゲージ中心とき裂先端部との距離を、き裂等の全長
の1/10〜3/10の範囲に貼付けることができる。従って、
各3軸ロゼット抵抗線ひずみゲージの出力より算出され
る較正係数が、き裂部材の幅や、き裂の長さ、き裂のき
裂部材に対する傾斜角等に依存しないで、き裂先端とゲ
ージ中心との距離の変化に応じてほぼ一直線状に変化す
ることとなり、より精度の高い応力拡大係数を容易かつ
安定的に測定することができる。
(Operation) According to the stress intensity factor measuring gauge of the first aspect of the present invention, two triaxial rosette resistance wire strain gauges are provided, and the distance between the center of each gauge and the crack tip is measured. It can be pasted in the range of 1/10 to 3/10 of the total length. Therefore,
The calibration coefficient calculated from the output of each 3-axis rosette resistance strain gauge does not depend on the width of the crack member, the length of the crack, the inclination angle of the crack with respect to the crack member, etc. The stress intensity factor changes in a substantially straight line according to the change in the distance from the gauge center, and the stress intensity factor with higher accuracy can be measured easily and stably.

本発明の第2の発明の応力拡大係数測定方法によれば、
構成の簡単な第1の発明の応力拡大係数測定用ゲージを
用いて外挿に適切な位置の応力を検出し、その検出応力
に較正係数を乗じ、更にこれをき裂先端まで外挿して、
精度の高い応力拡大係数を極めて容易に求めることがで
きる。
According to the stress intensity factor measuring method of the second invention of the present invention,
The stress at a suitable position for extrapolation is detected using the stress intensity factor measuring gauge of the first invention having a simple structure, the detected stress is multiplied by a calibration factor, and the extrapolated to the crack tip,
A highly accurate stress intensity factor can be obtained very easily.

本発明の第3の発明のき裂部材の余寿命監視装置によれ
ば、一方の応力拡大係数演算器によって、第1の発明の
応力拡大係数測定用ゲージで検出した検出応力から第2
の発明の応力拡大係数測定方法に基づいて応力拡大係数
を算出し、他方の開閉口点演算器によって、き裂開閉口
点測定用抵抗線ひずみゲージの出力からき裂の開閉口点
を算出する。そして、算出された応力拡大係数とき裂の
開閉口点から有効応力拡大係数範囲を算出し、更に、評
価器によって予め記憶してあるき裂部材の材料定数と有
効応力拡大係数範囲とを比較してき裂部材の残余寿命を
正確に求めることができる。
According to the remaining life monitoring apparatus for a crack member of the third invention of the present invention, the stress intensity factor calculator for one of the second aspect is used to detect the stress detected by the stress intensity factor measuring gauge of the first aspect.
The stress intensity factor is calculated based on the stress intensity factor measuring method of the invention, and the opening / closing mouth point of the crack is calculated from the output of the resistance wire strain gauge for measuring the crack opening / closing mouth point by the other opening / closing mouth point calculator. Then, the effective stress intensity factor range is calculated from the calculated stress intensity factor and the opening / closing point of the crack, and the material constant of the crack member stored in advance by the evaluator is compared with the effective stress intensity factor range. The remaining life of the member can be accurately determined.

(実施例) 以下、本発明の実施例を説明する。(Example) Hereinafter, the Example of this invention is described.

先ず、本発明によって応力拡大係数を求める比例外挿法
の基礎式は次式(3)(4)である。
First, the basic equations of the ratio exception insertion method for obtaining the stress intensity factor according to the present invention are the following equations (3) and (4).

ただし、 σy|θ=0 :き裂の進行方向と直交する方向の引
張応力 τxy|θ=0 :せん断応力 r :き裂先端からの距離 T:き裂縁に外力が作用する場合の引張力 Txy:き裂縁に外力が作用する場合のせん断力 ただし、サフィックスA,Bは、それぞれ応力拡大係数
を求めたい問題に関する値を示し、Bはあらじめ較正係
数を求めておく問題に関する値である。
However, σ y | θ = 0 : Tensile stress in the direction orthogonal to the crack propagation direction τ xy | θ = 0 : Shear stress r: Distance from the crack tip T y : When an external force acts on the crack edge T xy : Shear force when an external force acts on the crack edge However, suffixes A and B show the values relating to the problem for which the stress intensity factor is to be obtained, and B is the preliminary calibration factor. This is a value related to the problem.

式(3),(4)による比例外挿法の基礎式の妥当性を
第2図以降で説明する。
The validity of the basic expression of the ratio exception insertion method by the expressions (3) and (4) will be described with reference to FIG.

第2図に示すように、上下方向に一様引張を受ける中央
部のななめき裂23の応力拡大係数は、すでに、写象関
数を用いて北川、結城らによって厳密な解が求められて
いる。
As shown in FIG. 2, the stress intensity factor of the licking crack 23 in the central portion subjected to uniform tension in the vertical direction has already been determined by Kitagawa, Yuki et al. Using a mapping function. .

従って、この問題について第2図のような境界要素分割
により、境界要素法(BEM)を用いて数値解析を行
い、式(3)(4)における較正係数α,αIIを α=KIB/(σylθ=0)B αII=KIIB/(τxylθ=0)B として算出した。この問題ではき裂縁に外力は作用して
いないのでT(0)=Txy(0)=0とした。その
結果を第3図の実線に示す。
Therefore, regarding this problem, the boundary element division as shown in FIG. 2 is performed to perform a numerical analysis using the boundary element method (BEM), and the calibration coefficients α I and α II in the equations (3) and (4) are α I = K It was calculated as IB / (σ yl θ = 0) B α II = K IIB / (τ xyl θ = 0) B. In this problem, no external force acts on the crack edge, so T y (0) = T xy (0) = 0. The result is shown by the solid line in FIG.

この第3図中には、破線により既提案によるき裂の開口
変位を用いた場合の較正係数を参考のため示したが、き
裂の開口変位の場合の較正係数は、き裂先端からの距離
rに強く影響されることがわかる。当然ながらき裂先端
近傍の応力を用いた本提案の較正係数も、き裂先端から
の距離rの関数となることは図より明らかである。以上
より実際の応力拡大係数決定に際しては、式(3)
(4)を書き変えた次式(5)(6)を用いることが妥
当で、有効なことがわかる。
In FIG. 3, the calibration coefficient when the opening displacement of the crack proposed by the present invention is used is shown by a broken line for reference, but the calibration coefficient when the opening displacement of the crack is calculated from the crack tip. It can be seen that it is strongly influenced by the distance r. Of course, it is clear from the figure that the calibration coefficient of the present proposal using the stress near the crack tip is also a function of the distance r from the crack tip. From the above, when determining the actual stress intensity factor, use the formula (3)
It is appropriate and effective to use the following equations (5) and (6) in which (4) is rewritten.

次に、本発明の第1の発明である応力拡大係数測定用ゲ
ージについて説明する。
Next, the stress intensity factor measuring gauge according to the first aspect of the present invention will be described.

第1図は第1の発明の一実施例である応力拡大係数測定
用ゲージ25を示している。本実施例の応力拡大係数測
定用ゲージ25は、四角形の薄いゲージベース21の上
に、2個の3軸ロゼット抵抗線ひずみゲージ22,22
を固着して形成されている。そして、各3軸ロゼット抵
抗線ひずみゲージ22のゲージ中心0と、ゲージベース
21をき裂部材に貼付した時に、き裂23の先端部から
の距離が、き裂等の全長2Cに対して、1/10≦L
/2C≦(L+L)≦3/10の範囲内となる様に
設定している。
FIG. 1 shows a stress intensity factor measuring gauge 25 which is an embodiment of the first invention. The gauge 25 for measuring the stress intensity factor of the present embodiment comprises two triaxial rosette resistance wire strain gauges 22, 22 on a square thin gauge base 21.
It is formed by fixing. When the gauge center 0 of each triaxial rosette resistance wire strain gauge 22 and the gauge base 21 are attached to the crack member, the distance from the tip of the crack 23 is 2C for the total length 2C of the crack or the like. 1/10 ≤ L 2
The setting is such that / 2C ≦ (L 2 + L 1 ) ≦ 3/10.

例えば、き裂23等の全長が27.5mm程度以上である
場合には、L=2.75mm、L=2.5mmに形成し
た応力拡大係数測定用ゲージ25が応力拡大係数の測定
に効果的である。
For example, when the total length of the crack 23 or the like is about 27.5 mm or more, the stress intensity factor measuring gauge 25 formed with L 2 = 2.75 mm and L 1 = 2.5 mm is used for measuring the stress intensity factor. It is effective.

また、ゲージベース21には、き裂先端の決められた位
置に貼付できる様に縦横のガイドライン24,24を入
れることも効果が高い。
It is also highly effective to insert vertical and horizontal guidelines 24, 24 in the gauge base 21 so that the gauge base 21 can be attached at a predetermined position of the crack tip.

また、き裂縁には、き裂23の開閉口点を決定するため
の1軸抵抗線ひずみゲージ26を貼付することが有効で
ある。
Further, it is effective to attach a uniaxial resistance line strain gauge 26 to the crack edge to determine the opening / closing point of the crack 23.

このようにしてL,Lを決めるのは次の理由に基づ
くものである。
The reason for determining L 1 and L 2 in this way is based on the following reasons.

すなわち、第2図に示した中央ななめき裂23を有する
帯板27が引張荷重を受ける場合についてき裂長さに対
する板幅の比2C/W=0.2,0.3,0.4,0.
5で、き裂の傾き角α=0度、30度,45度の各場合
に境界要素法(BEM)で解析し、較正係数α,αII
を α=KIB/σYB αII=KIIB/τxyB により算出した結果を第3図の実線に示す。
That is, in the case where the strip 27 having the central licking crack 23 shown in FIG. 2 is subjected to a tensile load, the ratio of the strip width to the crack length 2C / W = 0.2, 0.3, 0.4, 0 .
5, the inclination angle α of the crack was analyzed by the boundary element method (BEM) in the cases of α = 0 °, 30 °, and 45 °, and the calibration coefficients α I , α II
The result calculated by α I = K IB / σ YB α II = K IIB / τ xyB is shown by the solid line in FIG.

この結果上記の各条件にかかわらずr/2aC<0.3
5の範囲内では較正係数は、2C/W、あるいはαに依
存しないで、一本の曲線で表示できる。
As a result, r / 2aC <0.3 regardless of the above conditions.
Within the range of 5, the calibration coefficient can be displayed as a single curve without depending on 2C / W or α.

一方、抵抗線ひずみゲージがある有限の寸法を有してい
るので、き裂23のごく近傍の応力測定が困難である。
On the other hand, since the resistance wire strain gauge has a certain finite size, it is difficult to measure the stress in the vicinity of the crack 23.

また、第3図からも明らかなように、き裂23のごく先
端近傍では、較正係数がやや小さ目となり、較正係数を
取扱いの容易な直線で近似するには0.1≦r/2C≦
0.3の範囲内が、ほぼ妥当で有効な応力拡大係数測定
を行なうことができる。
Further, as is clear from FIG. 3, the calibration coefficient becomes slightly small in the vicinity of the very tip of the crack 23, and 0.1 ≦ r / 2C ≦ to approximate the calibration coefficient with a straight line which is easy to handle.
Within the range of 0.3, the stress intensity factor measurement which is almost reasonable and effective can be performed.

次に、この応力拡大係数測定用ゲージ25を用いて本発
明の第2の発明に基づく応力拡大係数の測定法を第4図
について説明する。
Next, a method of measuring the stress intensity factor according to the second aspect of the present invention using the stress intensity factor measuring gauge 25 will be described with reference to FIG.

この測定に用いたき裂部材37は構造用炭素鋼(SS4
1材)からなる厚さ5mmの帯板である。このき裂部材3
7の中央にはななめの切欠33を設けており、その切欠
先端に応力拡大係数測定用ゲージ25を貼付する。そし
て、引張荷重をき裂部材37に負荷し、この状態で各3
軸ロゼット抵抗線ひずみゲージ22により第9図(b)
のrおよびrの位置の応力を求める。そして求めた
応力から式(5)(6)に基づいてrおよびrの位
置のKおよびKIIを較正係数として第3図に示した値
を用いて算定する。そして、第9図(b)に示すように
およびrの2点のK,KII値からr=0の値に
外挿して、真の応力拡大係数を求める。
The crack member 37 used for this measurement is a structural carbon steel (SS4
It is a strip plate made of 1 material and having a thickness of 5 mm. This crack member 3
7 is provided with a notch 33 in the center, and a gauge 25 for measuring the stress intensity factor is attached to the tip of the notch. Then, a tensile load is applied to the crack member 37, and in this state, each 3
Axial rosette resistance wire strain gauge 22 shown in FIG. 9 (b)
The stresses at the positions r 1 and r 2 are calculated. Then, from the obtained stress, K I and K II at the positions of r 1 and r 2 are calculated using the values shown in FIG. 3 as calibration coefficients based on the equations (5) and (6). Then, as shown in FIG. 9 (b), the true stress intensity factor is obtained by extrapolating from the K I and K II values of the two points r 1 and r 2 to the value of r = 0.

このように本発明に基づいて求めたK,KIIから下式
(7)(8)によって算出される応力拡大係数F,F
KIIと北川による解析解とを比較して別表に示した。
As described above, the stress intensity factors F 1 and F calculated by the following equations (7) and (8) from K I and K II obtained based on the present invention.
KII and Kitagawa's analytical solution are compared and shown in the attached table.

この別表から判るように、本発明の応力拡大係数測定用
ゲージ25を用いて求められた応力拡大係数は工学的に
十分な精度である。
As can be seen from this attached table, the stress intensity factor obtained by using the stress intensity factor measuring gauge 25 of the present invention has sufficient precision in terms of engineering.

次に、本発明の第3の発明を説明する。Next, a third invention of the present invention will be described.

本発明は、第1の発明の応力拡大係数測定用ゲージ25
を用いて応力を求め、第2の発明により応力拡大係数を
求め、この応力拡大係数からき裂部材37の残余寿命を
求めて監視するものである。
The present invention relates to a stress intensity factor measuring gauge 25 of the first invention.
Is used to calculate the stress, the stress intensity factor is calculated according to the second aspect of the invention, and the residual life of the crack member 37 is determined and monitored from this stress intensity factor.

第5図は本発明の一実施例を示し、すみ肉溶接部の欠陥
からき裂が生じた場合のき裂部材37の余寿命を監視す
る状態を示している。
FIG. 5 shows an embodiment of the present invention, and shows a state in which the remaining life of the crack member 37 is monitored when a crack is caused by a defect in the fillet weld.

本実施例においては、き裂13の先端部に応力拡大係数
測定用ゲージ25ならびにき裂開閉口点測定用ひずみゲ
ージ26を貼付している。この応力拡大係数測定用ゲー
ジ25で得られた応力は増幅器38へ送られる。この増
幅器38には、式(5)(6)によって応力拡大係数を
算出する応力拡大係数演算器39が接続されている。ま
た、この演算器39では、き裂開閉口点測定用ひずみゲ
ージ26で測定されたひずみ値を増幅器40へ送り、開
閉口点演算器41において第6図に示すような手法でき
裂開閉口点を決定した結果から、有効応力拡大係数範囲
をも算出する。このように、有効応力拡大係数範囲を算
定しなければならない理由は、疲労き裂が完全に閉じて
上下面が接触した場合に、荷重は伝達されるため、き裂
が閉じている範囲での負荷は、き裂先端の疲労損傷に影
響を与えないと考えられるためである。応力拡大係数演
算器39には、算出された有効応力拡大係数範囲を記憶
器42に予め記憶されているき裂部材37の材料定数と
比較する評価器43が接続されている。この評価器43
には比較結果を表示する表示器44と、評価器43によ
って危険と判断された時に運転停止信号を発する運転制
御器45とが接続されている。
In this embodiment, a stress intensity factor measuring gauge 25 and a crack opening / closing point measuring strain gauge 26 are attached to the tip of the crack 13. The stress obtained by the stress intensity factor measuring gauge 25 is sent to the amplifier 38. The amplifier 38 is connected to a stress intensity factor calculator 39 that calculates the stress intensity factor according to equations (5) and (6). Further, in this calculator 39, the strain value measured by the strain gauge 26 for measuring crack opening and closing point is sent to the amplifier 40, and the opening and closing point calculator 41 can perform the method as shown in FIG. The effective stress intensity factor range is also calculated from the result of determining. In this way, the reason why the effective stress intensity factor range must be calculated is that the load is transferred when the fatigue crack is completely closed and the upper and lower surfaces are in contact with each other, so that the range in which the crack is closed is This is because the load is considered not to affect the fatigue damage at the crack tip. The stress intensity factor calculator 39 is connected to an evaluator 43 that compares the calculated effective stress intensity factor range with the material constant of the crack member 37 stored in advance in the memory 42. This evaluator 43
A display unit 44 for displaying a comparison result and an operation controller 45 for issuing an operation stop signal when the evaluator 43 determines that the operation is dangerous are connected to the.

次に、本発明の作用を説明する。Next, the operation of the present invention will be described.

先ず、応力拡大係数測定用ゲージ25によりき裂13の
先端の応力を検出し、また、き裂開閉口点測定用ゲージ
26を用いてき裂縁部のひずみを検出し、それぞれ増幅
器38,40によって増幅し、更に応力拡大係数演算器
39および開閉口点演算器41により、応力拡大係数と
き裂開閉口点を算出し、有効応力拡大係数を算出する。
この場合負荷変動に伴う最大応力係数KImax,K
IImaxと、最小応力拡大係数KImin,KIIminとの差
として応力拡大係数範囲を算定し、モードI成分につい
ては次式(9)(10)の様にき裂開閉口比(X−Y)
/(X−Z)を乗じて有効応力拡大係数範囲とする(第
6図参照)。
First, the stress intensity factor measuring gauge 25 detects the stress at the tip of the crack 13, the crack opening / closing point measuring gauge 26 detects the crack edge strain, and the amplifiers 38 and 40 respectively detect the strain. Amplification is performed, and the stress intensity factor calculator 39 and the opening / closing point calculator 41 calculate the stress intensity factor and the crack opening / closing point to calculate the effective stress intensity factor.
In this case, the maximum stress coefficient K Imax , K accompanying the load change
The stress intensity factor range was calculated as the difference between IImax and the minimum stress intensity factors K Imin and K IImin. For the mode I component, the crack opening / closing ratio (XY) was calculated as in the following equations (9) and (10).
It is multiplied by / (XZ) to obtain the effective stress intensity factor range (see FIG. 6).

△K=(KImax)KImin)(X-Y)(X-Z) ……(9) △KII=(KIImax)KIImin……(10) 混合モード下における破壊条件には最大主応力説を採用
することとし、式(9)(10)より次式(11)に示
される最大主応力拡大係数 △Kθmaxを算出する。
△ K I = (K Imax ) K Imin ) (XY) (XZ) ・ ・ ・ (9) △ K II = (K IImax ) K IImin ・ ・ ・ (10) The maximum principal stress theory is applied to the failure condition under mixed mode. The maximum principal stress intensity factor ΔK θmax shown in the following equation (11) is calculated from the equations (9) and (10).

ただし、 である。 However, Is.

このような△Kθmaxを用いて、評価器43において
は第7図に示す記憶器42に内蔵されている材料定数と
の比較検討を行う。
Using such ΔK θmax , the evaluator 43 makes a comparative examination with the material constants built in the memory 42 shown in FIG. 7.

すなわち、一般に疲労き裂の伝ぱ速度は応力拡大係数範
囲に依存し、応力拡大係数範囲が小さければき裂伝ぱ速
度は減速し、ある限界値△Kth以下になれば全く伝ぱ
しない。一方、応力拡大係数が大きくなければき裂伝ぱ
速度は加速され、限界値△KFC以上になれば不安定的
にき裂が伝ぱし、き裂部材37が破断される。この第7
図に示されるき裂伝ぱ速度{log(da/dN)}と
有効応力拡大係数の変動幅(log△Keff)の関係
は、平均応力に依存しない材料によって決まる材料定数
であり、一般の(da/dN−△K)の関係の様に平均
応力によって複数のデータを準備する必要がない。ま
た、△Kth,△KFCも同様な材料定数でそれぞれ予
め記憶器42に内蔵されている。そして、評価結果が△
eff≦△Kthであれば、き裂の伝ぱは停止してお
り、それ以上の進展はなく、機械は運転継続される。
That is, in general, the propagation speed of a fatigue crack depends on the stress intensity factor range, and if the stress intensity factor range is small, the crack propagation velocity slows down and does not propagate at all below a certain limit value ΔK th . On the other hand, if the stress intensity factor is not large, the crack propagation speed is accelerated, and if it exceeds the limit value ΔK FC , the crack propagates in an unstable manner and the crack member 37 is broken. This 7th
The relationship between the crack propagation rate {log (da / dN)} and the fluctuation range (log ΔK eff ) of the effective stress intensity factor shown in the figure is a material constant determined by the material that does not depend on the average stress, and is generally ( It is not necessary to prepare a plurality of data according to the average stress like the relationship of da / dN-ΔK). Further, ΔK th and ΔK FC are also built in the memory 42 in advance with the same material constants. And the evaluation result is △
If K eff ≦ ΔK th , the propagation of cracks has stopped, there is no further progress, and the machine continues to operate.

また、△Kth≦△Keff<△KFCの範囲であれ
ば、現在のき裂伝ぱ速度が判り、余寿命として近い将来
のき裂伝ぱ速度が近似的に得られ、運転を継続しなが
ら、補修時期等の判断を決定する。
Further, within the range of ΔK th ≦ ΔK eff <ΔK FC , the current crack propagation speed can be known, and the crack propagation speed in the near future as the remaining life can be approximately obtained, and while continuing the operation. , Determine the repair timing.

また、△Keffが第7図の領域IIIであれば、余寿命
はきわめて短く、早急な機械の停止と補修が必要であり
運転制御器45より運転停止信号が送られることにな
り、緊急停止が不可能な構造物においては、監視を継続
しながら、機械の出力低下などにより、応力を低下さ
せ、き裂の伝ぱを減速させる。
Further, if ΔK eff is the region III in FIG. 7, the remaining life is extremely short, the machine must be stopped and repaired promptly, and an operation stop signal will be sent from the operation controller 45, resulting in an emergency stop. In a structure that is impossible to do so, the stress is reduced and the propagation of cracks is slowed down due to the output reduction of the machine while continuing the monitoring.

このような判断結果は表示器45により表示される。Such a judgment result is displayed on the display unit 45.

〔発明の効果〕〔The invention's effect〕

このように本発明の応力拡大係数測定用ゲージは簡単な
構成でしかも容易に応力拡大係数を測定することができ
る。また、本発明の応力拡大係数測定方法は、応力拡大
係数測定用ゲージの出力を基に応力拡大係数を極めて容
易に測定することができ、しかも非破壊的に高精度で応
力拡大係数を測定することができる。また、本発明のき
裂部材の余寿命監視装置はき裂の開閉口点を考慮した有
効応力拡大係数を容易に測定できるとともに、き裂伝ぱ
速度、並びに近い将来のき裂長さ等を精度良く推定して
余寿命を監視することができるので、き裂部材の不安定
破壊を未然に防止することができ、有効に機械等の使用
メインテナンスができる等の効果を奏する。
Thus, the stress intensity factor measuring gauge of the present invention has a simple structure and can easily measure the stress intensity factor. Further, the stress intensity factor measuring method of the present invention can very easily measure the stress intensity factor based on the output of the gauge for measuring the stress intensity factor, and also nondestructively measures the stress intensity factor with high accuracy. be able to. Further, the residual life monitoring apparatus for a crack member of the present invention can easily measure the effective stress intensity factor in consideration of the opening / closing point of the crack, and also accurately propagates the crack propagation speed, and the crack length in the near future. Since it is possible to estimate and monitor the remaining life, it is possible to prevent unstable breakage of the crack member and to effectively use and maintain the machine.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の応力拡大係数測定用ゲージ、き裂開閉
口点測定用ゲージの一実施例を示す平面図、第2図
(a)(b)は本発明の妥当性ならびに較正係数の算出
のために行なった境界要素法解析対象を示す概略図、第
3図は本発明の妥当性を示す較正係数の解析結果を示す
特性図、第4図(a)(b)(c)は本発明の妥当性を
検討するために実施した試験材料の概要を示し、同図
(a)は正面図、同図(b)は同図(a)の右側面図、
同図(c)は応力拡大係数測定用ゲージ部分の拡大図、
第5図は本発明のき裂部材の余寿命監視装置の一実施例
を示すブロック図、第6図はき裂開閉口点測定用ゲージ
によるき裂開閉口点の決定法を示す線図、第7図はき裂
伝ぱ速度と有効応力拡大係数範囲との関係を示す特性
図、第8図は本発明者が以前に提案した応力拡大係数測
定用ゲージを示す平面図、第9図(a)(b)は第8図
のゲージを用いた比例外挿法による応力拡大係数の決定
法を示す概略図である。 21……ゲージベース、22……3軸ロゼット抵抗線ひ
ずみゲージ、23……き裂、24……ガイドライン、2
5……応力拡大係数測定用ゲージ、26……き列開閉口
点測定用ゲージ、37……き裂部材、38,40……増
幅器、39……応力拡大係数演算器、41……開閉口点
演算器、42……記憶器、43……評価器。
FIG. 1 is a plan view showing an embodiment of a stress intensity factor measuring gauge and a crack opening / closing point measuring gauge of the present invention, and FIGS. 2 (a) and 2 (b) are the validity and calibration coefficient of the present invention. A schematic diagram showing the boundary element method analysis target performed for the calculation, FIG. 3 is a characteristic diagram showing the analysis result of the calibration coefficient showing the validity of the present invention, and FIG. 4 (a) (b) (c) are The outline of the test material carried out in order to examine the adequacy of the present invention is shown, the figure (a) is a front view, the figure (b) is a right side view of the figure (a),
The figure (c) is an enlarged view of the gauge part for measuring the stress intensity factor,
FIG. 5 is a block diagram showing an embodiment of the remaining life monitoring apparatus for crack members according to the present invention, and FIG. 6 is a diagram showing a method for determining crack opening / closing points by a gauge for measuring crack opening / closing points, FIG. 7 is a characteristic diagram showing the relationship between crack propagation rate and effective stress intensity factor range, FIG. 8 is a plan view showing a stress intensity factor measuring gauge previously proposed by the present inventor, and FIG. 9 (a). ) (B) is a schematic diagram showing a method of determining a stress intensity factor by a ratio exception insertion method using the gauge of FIG. 21 ... Gauge base, 22 ... 3-axis rosette resistance wire strain gauge, 23 ... Crack, 24 ... Guideline, 2
5 ... Stress intensity factor measuring gauge, 26 ... Key row opening / closing port point measuring gauge, 37 ... Crack member, 38, 40 ... Amplifier, 39 ... Stress intensity factor calculator, 41 ... Opening / closing port Point calculator, 42 ... Memory, 43 ... Evaluator.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】ゲージベースの上に2個の3軸抵抗線ひず
みゲージを間隔をおいて取付け、前記ゲージベースをき
裂部材のき裂近傍に貼付した時に、き裂の延長線上に上
記2個の3軸抵抗線ひずみゲージの各ゲージ中心が位置
するように配設されてなる応力拡大係数測定用ゲージ。
1. When two triaxial resistance wire strain gauges are mounted on a gauge base at intervals and the gauge base is attached in the vicinity of a crack of a crack member, the above-mentioned 2 is formed on the extension line of the crack. A stress intensity factor measuring gauge arranged such that the center of each of the three triaxial resistance strain gauges is located.
【請求項2】ゲージベース上に、2個の3軸抵抗線ひず
みゲージのゲージ中心を結ぶ線分からなるガイドライン
と、このガイドラインに直交する他のガイドラインとを
付したことを特徴とする特許請求の範囲第1項記載の応
力拡大係数測定用ゲージ。
2. A guide line comprising a line segment connecting the gauge centers of two triaxial resistance line strain gauges and another guide line orthogonal to the guide line are attached on the gauge base. Gauge for measuring the stress intensity factor according to the first item of the range.
【請求項3】ゲージベースの上に2個の3軸抵抗線ひず
みゲージを間隔をおいて取付け、前記ゲージベースをき
裂部材のき裂近傍に貼付した時に、き裂の延長線上に上
記2個の3軸抵抗線ひずみゲージの各ゲージ中心が位置
するように配設されてなる応力拡大係数測定用ゲージ
を、き裂部材のき裂先端近傍に貼付し、次に前記各3軸
抵抗線ひずみゲージによって応力を検出し、この検出応
力に基づいて下式(1)(2) ただし、 σy|θ=0 :き裂の進行方向と直交する方向の引
張応力 τxy|θ=0 :せん断応力 r :き裂先端からの距離 α,αII:較正係数 T:き裂縁に外力が作用する場合の引張
力 Txy:き裂縁に外力が作用する場合のせん
断力 により、各3軸抵抗線ひずみゲージの検出応力に較正係
数を乗じ、これをき裂先端へ外挿することにより応力拡
大係数を求めることを特徴とする応力拡大係数測定方
法。
3. Two triaxial resistance wire strain gauges are mounted on a gauge base at intervals, and when the gauge base is attached in the vicinity of the crack of the crack member, the above-mentioned 2 is formed on the extension line of the crack. A stress intensity factor measuring gauge, which is arranged so that the center of each of the three triaxial resistance wire strain gauges is located, is attached in the vicinity of the crack tip of the crack member, and then each of the triaxial resistance wires The stress is detected by the strain gauge, and the following equations (1) and (2) are used based on the detected stress. However, σ y | θ = 0 : Tensile stress in the direction orthogonal to the crack propagation direction τ xy | θ = 0 : Shear stress r: Distance from the crack tip α I , α II : Calibration coefficient T y : Crack Tensile force when an external force acts on the crack edge T xy : The shearing force when an external force acts on the crack edge multiplies the detection stress of each triaxial resistance line strain gauge by a calibration factor and applies this to the crack tip. A method for measuring a stress intensity factor, characterized by obtaining a stress intensity factor by extrapolation.
【請求項4】ゲージベースの上に2個の3軸抵抗線ひず
みゲージを間隔をおいて取付け、前記ゲージベースをき
裂部材のき裂近傍に貼付した時に、き裂の延長線上に上
記2個の3軸抵抗線ひずみゲージの各ゲージ中心が位置
するように配設されてなる応力拡大係数測定用ゲージを
き裂部材のき裂先端近傍に貼付し、次に前記各3軸抵抗
線ひずみゲージによって応力を検出し、応力拡大係数を
算出する応力拡大係数演算器と;き裂縁部に新たに貼付
したき裂開閉口点測定用抵抗線ひずみゲージの出力によ
り、き裂の開閉口点を算出する開閉口点演算器と;この
応力拡大係数とき裂の開閉口点から有効応力拡大係数範
囲を算出し、この有効応力拡大係数範囲と予め記憶して
ある材料定数とを比較してき裂部材の残余寿命を求める
評価器:と;を有するき裂部材の余寿命監視装置。
4. Two triaxial resistance wire strain gauges are mounted on a gauge base at intervals, and when the gauge base is attached in the vicinity of a crack of a crack member, the above-mentioned 2 is formed on the extension line of the crack. A stress intensity factor measuring gauge, which is arranged such that the center of each of the three triaxial resistance line strain gauges is located, is attached near the crack tip of the crack member, and then each triaxial resistance line strain is measured. A stress intensity factor calculator that detects the stress with a gauge and calculates the stress intensity factor; and a crack opening / closing point newly attached to the crack edge by the output of the resistance wire strain gauge for measurement. An opening / closing point calculator for calculating the effective stress intensity factor range from this stress intensity factor and the opening / closing point of the crack, and comparing the effective stress intensity factor range with a previously stored material constant. Evaluator for determining the remaining life of Remaining life monitoring system Ruki cleft material.
JP21195086A 1986-09-09 1986-09-09 Stress intensity factor measuring gauge, stress intensity factor measuring method, and remaining life monitoring device for cracked member Expired - Lifetime JPH0610645B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21195086A JPH0610645B2 (en) 1986-09-09 1986-09-09 Stress intensity factor measuring gauge, stress intensity factor measuring method, and remaining life monitoring device for cracked member

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21195086A JPH0610645B2 (en) 1986-09-09 1986-09-09 Stress intensity factor measuring gauge, stress intensity factor measuring method, and remaining life monitoring device for cracked member

Publications (2)

Publication Number Publication Date
JPS6366428A JPS6366428A (en) 1988-03-25
JPH0610645B2 true JPH0610645B2 (en) 1994-02-09

Family

ID=16614380

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21195086A Expired - Lifetime JPH0610645B2 (en) 1986-09-09 1986-09-09 Stress intensity factor measuring gauge, stress intensity factor measuring method, and remaining life monitoring device for cracked member

Country Status (1)

Country Link
JP (1) JPH0610645B2 (en)

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JPH02230130A (en) * 1989-12-15 1990-09-12 Semiconductor Energy Lab Co Ltd Liquid crystal electrooptic device
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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Also Published As

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