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JPH0776683B2 - Latent distortion detection method - Google Patents
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JPH0776683B2 - Latent distortion detection method - Google Patents

Latent distortion detection method

Info

Publication number
JPH0776683B2
JPH0776683B2 JP15619193A JP15619193A JPH0776683B2 JP H0776683 B2 JPH0776683 B2 JP H0776683B2 JP 15619193 A JP15619193 A JP 15619193A JP 15619193 A JP15619193 A JP 15619193A JP H0776683 B2 JPH0776683 B2 JP H0776683B2
Authority
JP
Japan
Prior art keywords
strain
latent
measured
electrodes
external force
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 - Fee Related
Application number
JP15619193A
Other languages
Japanese (ja)
Other versions
JPH06341807A (en
Inventor
博司 中根
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.)
CHUO FUKUKEN KONSARUTANTSU KK
DOBOKU KEISOKU KENKYUSHO KK
SOGO KEISOKU KK
Original Assignee
CHUO FUKUKEN KONSARUTANTSU KK
DOBOKU KEISOKU KENKYUSHO KK
SOGO KEISOKU KK
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 CHUO FUKUKEN KONSARUTANTSU KK, DOBOKU KEISOKU KENKYUSHO KK, SOGO KEISOKU KK filed Critical CHUO FUKUKEN KONSARUTANTSU KK
Priority to JP15619193A priority Critical patent/JPH0776683B2/en
Publication of JPH06341807A publication Critical patent/JPH06341807A/en
Publication of JPH0776683B2 publication Critical patent/JPH0776683B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、未知の外力が作用して
いる被測定体、例えばトンネルの鋼支保工、コンクリー
ト内の鉄筋等に蓄積されている潜在歪みを非破壊的に検
出する方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention is a nondestructive method for non-destructively detecting latent strain accumulated in an object to be measured on which an unknown external force is applied, such as a steel support of a tunnel or a reinforcing bar in concrete. Regarding

【0002】[0002]

【従来の技術】従来、この種の検出方法として、磁気を
利用するもの、超音波を利用するもの、X線を利用する
もの等が知られている。
2. Description of the Related Art Conventionally, as a detection method of this kind, a method using magnetism, a method using ultrasonic waves, a method using X-rays, etc. are known.

【0003】[0003]

【発明が解決しようとする課題】しかし、磁気を利用す
るものでは、被測定体が磁性体でなければならず、その
検出対象が限定されるばかりでなく、鋼材にあっても組
成による磁気特性の相違によって検出される値が異なる
ため、その組成を予め知る必要があり、検出準備に手間
がかゝる。又、超音波を利用するものは、超音波発信源
を該被測定体の表面に密着させるために、その取付面を
研磨する作業を要する等その準備に手間がかゝる。又、
X線を利用するものでは、その取扱いに注意を要し、簡
単に使用できないなどの不具合がある。本発明は、かゝ
る不都合を解消した被測定体の潜在歪みの検出方法を提
供することをその目的とする。
However, in the case of utilizing magnetism, the object to be measured must be a magnetic material, and the object to be detected is not limited. Since the value to be detected differs depending on the difference, it is necessary to know the composition in advance, and it takes time to prepare for detection. Further, in the case of using ultrasonic waves, in order to bring the ultrasonic wave source into close contact with the surface of the object to be measured, the work of polishing the mounting surface thereof is required, and the preparation thereof is troublesome. or,
In the case of using X-rays, there is a problem that they need to be handled with care and cannot be used easily. An object of the present invention is to provide a method for detecting a latent strain of an object to be measured which eliminates such inconvenience.

【0004】[0004]

【課題を解決するための手段】かゝる目的を達成するた
めの本発明の潜在歪みの検出方法は、被測定体とダミー
片との表面に一対の電極を設け、これに未知の外力が潜
在する状態で、該電極間に瞬間的に直流電流を流して該
電流が流れるときに生じる電磁力と該外力との合成歪み
とから潜在歪みを検出することを特徴とする。
A method for detecting latent strain of the present invention for achieving such an object is to provide a pair of electrodes on the surface of an object to be measured and a dummy piece, and apply an unknown external force to them. In a latent state, a direct current is instantaneously passed between the electrodes, and the latent strain is detected from the combined strain of the electromagnetic force generated when the current flows and the external force.

【0005】[0005]

【作用】上記本発明の潜在歪みの検出方法によれば、両
電極間に瞬間的に電流を印加すると、フレーミングの左
手の法則によって、被測定体に電磁力が発生するので、
その表面歪み(外力と衝撃応力による合成歪み)を測定
する。外力による歪みと合成歪みとの相関関係を求めて
おけば、電磁力による歪みは、電流の大きさを特定する
ことで常数となるから、該合成歪みから簡単に潜在歪み
を知ることができる。上記の表面歪みの測定は、前記一
対の電極間と該電極間以外の被測定体との表面に互いに
間隔を存してストレーンゲージを取付け、その両ストレ
ーンゲージを用いて構成したホイートストンブリッジに
より前記表面歪みを測定し、これから潜在歪みを求め
る。
According to the latent strain detecting method of the present invention, when a current is instantaneously applied between both electrodes, an electromagnetic force is generated in the object to be measured by the left-hand rule of framing.
The surface strain (composite strain due to external force and impact stress) is measured. If the correlation between the strain due to the external force and the synthetic strain is obtained, the strain due to the electromagnetic force becomes a constant by specifying the magnitude of the electric current, so that the latent strain can be easily known from the synthetic strain. The measurement of the surface strain, the strain gauge is attached to the surface between the pair of electrodes and the object to be measured other than between the electrodes with a space therebetween, and the Wheatstone bridge configured using both strain gauges is used. The surface strain is measured and the latent strain is obtained from this.

【0006】[0006]

【実施例】本発明の測定方法の実施の1例を図1乃至図
5に基いて説明する。図1(a)(b)において、Mは
鉄筋などの被測定体、M′はこれに添わせて設けた被測
定体Mと同一材料からなるダミー片を示し、該ダミー片
M′は、電気的に絶縁性のある結合片cと導電性のある
結合片dとで被測定体Mに結合されて設ける。そして、
該結合片dを介して該被測定体Mとダミー片M′との相
平行する部分に電流が流れるように、被測定体Mとダミ
ー片M′とに電極a,bを設ける。Gは、該電極a,b
間に電流を流すとき該電極a,b間に入るように被測定
体Mの表面に設けたストレンゲージ、G′は、被測定体
Mの該電極a,b間から外れた位置に設けたストレンゲ
ージを示し、該ストレンゲージG,G′は図2に示すよ
うに整合部Aを介してホイートストンブリッジを組み、
記録計RECに接続する。図2において、Bは前記電極
a,b間に流す電流の通電時間を50mS以下に制御す
るタイマ、DCSは直流安定化電源を示し、該電源DC
Sは50アンペアに設定する。HSは手動スイッチ、T
はタイマBと記録計RECの起動を一致させるための同
期部を示す。次に本発明方法による潜在歪みの測定を説
明する。今、被測定体Mに外力(例えば引張力P)によ
って潜在歪みEX が存在する場合において、電極a,b
間に電流を流す。すると、被測定体Mとダミー片M′と
の間に、図1(b)示のように、互いに反対方向の電磁
力F1 、F2 がかゝる。そして、前記記録計RECに
は、潜在歪みEX と見合った合成歪みEa が検出され
る。以下これを説明する。図3は、外力Pによる潜在歪
みEX と電磁力F1 によって生じた歪みEF とによって
合成された歪みEM を示す。そして、合成歪みEM と潜
在歪みEX の間には常にEM >EX なる関係があるの
で、EM −EX =Ea なる関係がある。尚、EF は電流
の大きさを一定にすることで常に一定値とすることがで
きる。図4は、この差分Ea を潜在歪みEX の方向の分
力Eb と電磁力F1 に伴う歪みEF 方向の分力Ec に分
解したもので、前記ストレンゲージGの受感方向を歪み
X 方向に一致させておけば、記録計RECに分力Eb
を検出することができる。図5は、予め図1に示す検定
用ストレンゲージgによって検出され、外力Pの大きさ
によって特定される潜在歪みEX と歪み成分Ea の相関
関係を示す特性曲線Sを示す。この図において、前述し
た手段により現実の被測定体Mから記録計RECに検出
されたEa 線上の値Eaiが曲線と交わる点Pを求め、該
P点からEX 線上に垂線を下してその交点Qが求める潜
在歪みEx である。尚、上記実施例では、外力Pとして
引張力が被測定体Mにかゝる場合を説明したが、該力P
が圧縮力である場合は、歪みEX は負の値となる。
EXAMPLES An example of the implementation of the measuring method of the present invention will be described with reference to FIGS. In FIGS. 1 (a) and 1 (b), M is a measured object such as a reinforcing bar, M'is a dummy piece made of the same material as the measured object M provided along with it, and the dummy piece M'is The electrically conductive coupling piece c and the electrically conductive coupling piece d are provided so as to be coupled to the device under test M. And
Electrodes a and b are provided on the object to be measured M and the dummy piece M ′ so that a current flows through the coupling piece d to the portions of the object M to be measured and the dummy piece M ′ which are parallel to each other. G is the electrodes a, b
A strain gauge, G ', which is provided on the surface of the object to be measured M so as to enter between the electrodes a and b when a current is passed between them, is provided at a position apart from the electrodes a and b of the object to be measured M. A strain gauge is shown, and the strain gauges G and G'assemble a Wheatstone bridge via a matching portion A as shown in FIG.
Connect to the recorder REC. In FIG. 2, B is a timer for controlling the energization time of the current flowing between the electrodes a and b to be 50 mS or less, DCS is a DC stabilized power supply, and the power supply DC
Set S to 50 amps. HS is a manual switch, T
Indicates a synchronization unit for matching the activation of the timer B and the recorder REC. Next, the measurement of latent strain by the method of the present invention will be described. Now, when the potential distortion E X is present by an external force to the object to be measured M (such as tensile force P), the electrodes a, b
Apply current between them. Then, electromagnetic forces F 1 and F 2 in opposite directions are applied between the measured object M and the dummy piece M ′, as shown in FIG. 1B. Then, in the recorder REC, a synthetic strain E a commensurate with the latent strain E X is detected. This will be described below. FIG. 3 shows the strain E M synthesized by the latent strain E X due to the external force P and the strain E F caused by the electromagnetic force F 1 . Since there is always a relation of E M > E X between the synthetic strain E M and the latent strain E X , there is a relation of E M −E X = E a . Incidentally, E F can be always a constant value by a constant amount of current. FIG. 4 is a diagram in which the difference E a is decomposed into a component force E b in the direction of the latent strain E X and a component force E c in the strain E F direction due to the electromagnetic force F 1, and the sensing direction of the strain gauge G is shown. If the distortion is matched with the E X direction, the component force E b is applied to the recorder REC.
Can be detected. FIG. 5 shows a characteristic curve S showing the correlation between the latent strain E X and the strain component E a , which is previously detected by the verification strain gauge g shown in FIG. 1 and specified by the magnitude of the external force P. In this figure, the point P at which the value E ai on the E a line detected by the recorder M from the actual measured object M by the above-mentioned means intersects the curve is obtained, and a perpendicular line is drawn from the point P on the E X line. The intersection Q is the latent distortion E x required. In the above embodiment, the case where the tensile force acts on the measured object M as the external force P has been described.
Is a compressive force, the strain E X has a negative value.

【0007】[0007]

【発明の効果】このように本発明によるときは、両電極
間に電流を印加するだけで、被測定体にかゝる潜在歪み
を非破壊的に簡単に検出することができる。
As described above, according to the present invention, it is possible to easily and non-destructively detect the latent strain of the object to be measured by simply applying a current between both electrodes.

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

【図1(a)】本発明方法を説明する概略平面図であ
る。
FIG. 1 (a) is a schematic plan view illustrating a method of the present invention.

【図1(b)】図1の断面図である。FIG. 1 (b) is a cross-sectional view of FIG.

【図2】検出回路図である。FIG. 2 is a detection circuit diagram.

【図3】潜在歪みと電磁力との関係を示す線図である。FIG. 3 is a diagram showing the relationship between latent strain and electromagnetic force.

【図4】合成歪みの差分を潜在歪みと電磁力方向とに分
解した関係を示す線図である。
FIG. 4 is a diagram showing a relationship in which a difference between combined strains is decomposed into a latent strain and an electromagnetic force direction.

【図5】既知の潜在歪みと分成歪みの差分との特性を示
す線図である。
FIG. 5 is a diagram showing a characteristic between a known latent strain and a difference between component strains.

【符号の説明】[Explanation of symbols]

M 被測定体 M′ ダミー片 a
電極 b 電極 G ストレンゲージ
G′ ストレンゲージ
M DUT M'dummy piece a
Electrode b Electrode G Strain gauge
G'strain gauge

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 被測定体とダミー片との表面に一対の電
極を設け、該被測定体に未知の外力が潜在する状態で、
該電極間に瞬間的に直流電流を流して該電流が流れると
きに生じる電磁力と該外力との合成歪みとから潜在歪み
を検出することを特徴とする潜在歪みの検出方法。
1. A pair of electrodes are provided on the surfaces of the object to be measured and the dummy piece, and an unknown external force is latent in the object to be measured,
A method for detecting latent strain, which comprises detecting a latent strain from a combined strain of an electromagnetic force and an external force generated when a direct current is instantaneously passed between the electrodes and the current flows.
【請求項2】 前記電極間とそれ以外の被測定体との表
面に互いに間隔を存してストレーンゲージを配設し、そ
の両ストレーンゲージを用いて構成したホイートストン
ブリッジにより前記合成歪みを検出するようにしたこと
を特徴とする請求項1記載の潜在歪みの検出方法。
2. A strain gauge is provided on the surfaces of the electrodes and the surface of the other object to be measured with a space therebetween, and the Wheatstone bridge configured by using both of the strain gauges detects the composite strain. The latent distortion detecting method according to claim 1, wherein the latent distortion is detected.
JP15619193A 1993-06-02 1993-06-02 Latent distortion detection method Expired - Fee Related JPH0776683B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15619193A JPH0776683B2 (en) 1993-06-02 1993-06-02 Latent distortion detection method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15619193A JPH0776683B2 (en) 1993-06-02 1993-06-02 Latent distortion detection method

Publications (2)

Publication Number Publication Date
JPH06341807A JPH06341807A (en) 1994-12-13
JPH0776683B2 true JPH0776683B2 (en) 1995-08-16

Family

ID=15622365

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15619193A Expired - Fee Related JPH0776683B2 (en) 1993-06-02 1993-06-02 Latent distortion detection method

Country Status (1)

Country Link
JP (1) JPH0776683B2 (en)

Also Published As

Publication number Publication date
JPH06341807A (en) 1994-12-13

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