JPH02296122A - Stress measuring method using magnetostruction type stress sensor - Google Patents

Stress measuring method using magnetostruction type stress sensor

Info

Publication number
JPH02296122A
JPH02296122A JP11502789A JP11502789A JPH02296122A JP H02296122 A JPH02296122 A JP H02296122A JP 11502789 A JP11502789 A JP 11502789A JP 11502789 A JP11502789 A JP 11502789A JP H02296122 A JPH02296122 A JP H02296122A
Authority
JP
Japan
Prior art keywords
stress
gap
magnetic sensor
detection
sensor
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.)
Pending
Application number
JP11502789A
Other languages
Japanese (ja)
Inventor
Hiroshi Yamamoto
浩 山本
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.)
Komatsu Ltd
Original Assignee
Komatsu 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 Komatsu Ltd filed Critical Komatsu Ltd
Priority to JP11502789A priority Critical patent/JPH02296122A/en
Publication of JPH02296122A publication Critical patent/JPH02296122A/en
Pending legal-status Critical Current

Links

Landscapes

  • Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)

Abstract

PURPOSE:To make it possible to measure stress accurately by dividing the detected value of a magnetic sensor for detecting stress by the detected value of a magnetic sensor for detecting a gap. CONSTITUTION:The high frequency signal from a transmitter 11 acts on both magnetic sensors 1 and 10. The detected signals from the sensors 1 and 10 are rectified in a lock-in amplifier 12 and an amplifier rectifier 13. Outputs V1 and V2 from the sensors are inputted into an operator 14. In the operator 14, the operation of the outputs V1/V2 is performed, and a measured value F(tau) of the stress is obtained. In this way, the accurate stress measurement can be performed.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、励磁式磁気センサを利用した磁歪式応力セン
サにおいて被測定物との間の距離を補正しながら応力J
l定を行なう方法に関するものである。
Detailed Description of the Invention [Industrial Application Field] The present invention provides a magnetostrictive stress sensor using an excitation type magnetic sensor, in which the stress J is
The present invention relates to a method for performing the l-determination.

〔従来の技術〕[Conventional technology]

この種の従来の技術としては、例えば特開昭Go−10
4230号公報に示されるように、軸トルク測定装置が
知られている。これはトルク検出器の磁気ヘッドを軸の
円周方向にマルチ化して各ヘッドの出力を平均化するこ
とで軸とトルク測定装置間のエアギャップ変動をなくす
ようにしている。
As this type of conventional technology, for example, Japanese Patent Application Laid-open No.
As shown in Japanese Patent No. 4230, a shaft torque measuring device is known. This eliminates air gap fluctuations between the shaft and the torque measuring device by multiplying the magnetic heads of the torque detector in the circumferential direction of the shaft and averaging the output of each head.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来の例えば上記トルク測定装置においては、軸と磁気
センサ間のエアギャップ変動は軸回周方向に磁気センサ
を複数個配列してその出力の平均をトルク値としている
が、この方法では、磁気センサが複数個必要となり、ま
た測定系を組立てるのに手間がかかるという問題がある
For example, in the conventional torque measuring device mentioned above, air gap fluctuations between the shaft and the magnetic sensor are measured by arranging a plurality of magnetic sensors in the rotational direction of the shaft and taking the average of their outputs as the torque value. There is a problem in that a plurality of measurement systems are required, and it takes time and effort to assemble the measurement system.

またセンサ1個であると、アライメントの調整に手間が
かかるし、精度も期待できなかった。
In addition, if only one sensor was used, it would take time and effort to adjust the alignment, and accuracy could not be expected.

本発明は上記のことにかんがみなされたもので、磁歪式
応力センサと被測定物間のギャップ変動に影響されない
正確な応力測定が可能な磁歪式応力センサによる応力測
定方法を提供することを目的とするものである。
The present invention has been made in view of the above, and an object of the present invention is to provide a stress measurement method using a magnetostrictive stress sensor that can accurately measure stress without being affected by gap fluctuations between the magnetostrictive stress sensor and the object to be measured. It is something to do.

〔課題を解決するための手段〕[Means to solve the problem]

上記目的を達成するために、本発明に係る磁歪式応力セ
ンサによる応力n1定方法は、励磁系と検出系とからな
る応力検出用の磁気センサを被測定物に対向させたとき
の検出値■、を、このときの被測定物の応力による磁気
特性変化に対して変化しなくなる位置に設けられて上記
応力検出用の磁気センサと被測定物間のギャップを測定
するギャップ検出用の磁気センサからの検出値V2にて
除し、その結果を応力測定値とする。
In order to achieve the above object, the stress n1 determination method using the magnetostrictive stress sensor according to the present invention is based on the detection value { , from a gap detection magnetic sensor that measures the gap between the stress detection magnetic sensor and the measurement object, which is installed at a position where the magnetic properties do not change due to the stress of the object to be measured. is divided by the detected value V2, and the result is taken as the stress measurement value.

〔作  用〕[For production]

応力検出用の磁気センサの検出値を、ギャップ検出用の
磁気センサの検出値にて除することにより、応力検出用
の磁気センサと被測定物間のギャップ変動によるこの応
力検出用の磁気センサの測定誤差が補正される。
By dividing the detected value of the magnetic sensor for stress detection by the detected value of the magnetic sensor for gap detection, it is possible to calculate Measurement errors are corrected.

〔実 施 例〕〔Example〕

本発明の実施例を図面に基づいて説明する。 Embodiments of the present invention will be described based on the drawings.

図中1は被測定物2の磁気特性の変化を検出することに
より、この彼、II定物2に作用する応力を測定するた
めの応力検出用の磁気センサであり、この磁気センサ1
は、コ字状に形成した励磁用コア3の両脚部に励磁用コ
イル4を巻回した励磁系と、コ字状に形成した検出用コ
ア5の両脚部に検出用コイル6を巻回した検出系とをあ
る角度をもって配置した構成となっており、この磁気セ
ンサ1に発振器より所定の高周波信号を発信することに
より、これに対向する被/l1ll定物2に作用してい
る応力が磁気特性の変化として検出され、この信号は整
流器等を介して応力演算回路に入力され、ここで上記応
力が演算されるようになっている。
In the figure, reference numeral 1 denotes a stress detection magnetic sensor for measuring the stress acting on the object 2 by detecting changes in the magnetic properties of the object 2.
The excitation system has an excitation coil 4 wound around both legs of an excitation core 3 formed in a U-shape, and a detection coil 6 wound around both legs of a detection core 5 formed in a U-shape. The detection system is arranged at a certain angle, and by transmitting a predetermined high frequency signal from an oscillator to this magnetic sensor 1, the stress acting on the object 2 facing the magnetic sensor 1 is magnetically This signal is detected as a change in characteristics, and is input to a stress calculation circuit via a rectifier or the like, where the stress is calculated.

上記説明した構成は従来の磁歪式応力センサと略同様で
あり、この構成によれば、応力検出値は、磁気センサ1
と被測定物2とのギャップ変動によって変化するので、
従来は、複数検出信号を平均してトルク値としている。
The configuration described above is almost the same as a conventional magnetostrictive stress sensor, and according to this configuration, the stress detection value is
Since it changes depending on the gap variation between and the measured object 2,
Conventionally, multiple detection signals are averaged to obtain a torque value.

本発明に係る磁歪式応力センサは上記ギヤツブの変動に
影響されない正確な応力all定を行なうことができる
ようにしたものである。
The magnetostrictive stress sensor according to the present invention is capable of accurately determining all stresses unaffected by the above-mentioned gear fluctuations.

すなわち、第1図に示すように、上記応力検出用の磁気
センサ1の励磁系の励磁用コア3に、応力検出用の磁気
センサ1と被測定物2との間のギャップXを検出するギ
ャップ検出用コイル9を巻回してなるギャップn1定用
の磁気センサ10を上記応力検出用の磁気センサ1のほ
かに設ける。
That is, as shown in FIG. 1, the excitation core 3 of the excitation system of the magnetic sensor 1 for stress detection has a gap for detecting the gap X between the magnetic sensor 1 for stress detection and the object to be measured 2. A magnetic sensor 10 for determining the gap n1, which is formed by winding a detection coil 9, is provided in addition to the magnetic sensor 1 for stress detection.

上記構成において、応力検出用の磁気センサ1のセンサ
出力V、と、ギャップ検出用の磁気センサ10のセンサ
出力V2のそれぞれのギャップ変動に対する関数は次の
ように同じ形になる。
In the above configuration, the functions of the sensor output V of the magnetic sensor 1 for stress detection and the sensor output V2 of the magnetic sensor 10 for gap detection with respect to gap fluctuations have the same form as follows.

ただし、f(r)、彼n1定物8に作用する応力、Vo
:応力検出用の磁気センサ1を 被測定物8に接触させた状態 (ギャップ−〇)での出力 X:ギャップ a、b:2つの磁気センサ1,10の 位置関係できまる定数 上記ギャップ検出用の磁気センサ10のセンサ出力v2
は、ギャップXがある値以上大きくなると被測定物2の
応力による磁気特性変化に対して変化しなくなる。
However, f(r), the stress acting on he n1 constant 8, Vo
: Output X when the magnetic sensor 1 for stress detection is in contact with the object to be measured 8 (gap - ○): Gap a, b: Constant determined by the positional relationship of the two magnetic sensors 1 and 10 The above gap detection Sensor output v2 of the magnetic sensor 10 of
When the gap X becomes larger than a certain value, it does not change with respect to changes in the magnetic properties due to the stress of the object to be measured 2.

このことから、応力検出用の磁気センサ1において、ギ
ャップ検出用の磁気センサ10を取付けた方の励磁系の
励磁用コア3を、検出系の検出用コア5に対してギャッ
プX方向に相対的に移動し、上記(1)式の両分母、x
十a、x+bが等しくなるようにセットする。
From this, in the magnetic sensor 1 for stress detection, the excitation core 3 of the excitation system to which the magnetic sensor 10 for gap detection is attached is relative to the detection core 5 of the detection system in the gap X direction. , and both denominators of equation (1) above, x
Set so that 10a and x+b are equal.

上記状態にした応力検出用の磁気センサ1にて被測定物
2の応力を測定したときに、応力検出用の磁気センサ1
のセンサ出力v1を、ギャップ検出用の磁気センサ10
のセンサ出力V2で除することにより、ギャップ変動の
影響を受けない応カフTPJ定値F(τ)が得られる。
When the stress of the object to be measured 2 is measured with the magnetic sensor 1 for stress detection in the above state, the magnetic sensor 1 for stress detection
The sensor output v1 of the gap detection magnetic sensor 10
By dividing by the sensor output V2, a constant cuff TPJ value F(τ) that is not affected by gap fluctuations can be obtained.

第2図は上記応力測定値F(τ)を得るための作用を示
すもので、発信器11よりの高周波信号が両磁気センサ
1,10に作用し、両磁気センサ1,10からの検出信
号はロックインアンプ12、整流器13にて整流されて
それぞれのセンサ出力V、、V2となって演算器14に
入力され、ここでV、/V2の演算が行なわれて応力測
定値F(τ)が得られる。
FIG. 2 shows the operation for obtaining the stress measurement value F(τ), in which a high frequency signal from the transmitter 11 acts on both magnetic sensors 1 and 10, and a detection signal from both magnetic sensors 1 and 10 is generated. are rectified by the lock-in amplifier 12 and the rectifier 13 to become the respective sensor outputs V, , V2, which are input to the calculator 14, where V, /V2 are calculated and the stress measurement value F(τ) is obtained. is obtained.

上記のように設定された磁気センサ1にてSNCM22
0Hにッケルクロムチリブデン鋼)の応力を測定した場
合の応力測定値F(τ)は第3図に示すようになり、F
(τ)のギャップXに対する応力の変化率σ(%)は、
ギャップXが0.25■lを越えた状態で一定となる。
SNCM22 with magnetic sensor 1 set as above
The stress measurement value F (τ) when measuring the stress of 0H (nickel chrome titanium steel) is shown in Fig. 3, and F
The rate of change in stress σ (%) with respect to the gap X of (τ) is:
It becomes constant when the gap X exceeds 0.25 ■l.

またギャップXを0.5mmから2.0mmまで段階的
に変化させ、各ギャップにおける!111定で、かつ応
力を変化した場合の応力測定値F(τ)はそれぞれ第4
図に示すようになり、ギャップXが変化してもその測定
値は変化しなかった。
In addition, the gap X was changed stepwise from 0.5 mm to 2.0 mm, and at each gap! 111 and the stress measurement value F(τ) when the stress is changed is the fourth
As shown in the figure, even if the gap X changed, the measured value did not change.

上記第3図、第4図に示す結果から、ギャップX変動の
影響を受けない応力測定が行なわれることがわかる。
From the results shown in FIGS. 3 and 4 above, it can be seen that stress measurement is performed without being affected by gap X fluctuations.

なお上記実施例では、ギャップ検出用の磁気センサ10
を応力検出用の磁気センサ1の構成部材の一部である励
磁用コアにギャップ検出用コイル9を巻回して構成した
例を示したが、このギャップ検出用の磁気センサ10は
応力検出用の磁気センサ1とは別の部材にギャップ検出
用コイル9と巻回して構成としてもよい。この場合上記
部材は応力検出用の磁気センサ1に対してギャップX方
向に位置調整して固定される。
Note that in the above embodiment, the magnetic sensor 10 for gap detection
An example has been shown in which the gap detection coil 9 is wound around the excitation core which is a part of the component of the magnetic sensor 1 for stress detection. The gap detection coil 9 may be wound around a separate member from the magnetic sensor 1. In this case, the above member is fixed in position with respect to the magnetic sensor 1 for detecting stress in the gap X direction.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、磁歪式応力センサと測定対象物間の距
離(ギャップ)変動に影響されない正確な化カバ1定を
行なうことができる。
According to the present invention, it is possible to carry out accurate chemical coverage unaffected by variations in the distance (gap) between the magnetostrictive stress sensor and the object to be measured.

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

図面は本発明の実施態様を示すもので、第1図は概略的
な構成説明図、第2図は作用説明図、第3図、第4図は
測定結果を示す線図である。 1は応力検出用の磁気センサミ2は被tP1定物、9は
ギャップ検出コイル、10はギャップ測定用の磁気セン
サ。
The drawings show embodiments of the present invention; FIG. 1 is a schematic diagram for explaining the configuration, FIG. 2 is a diagram for explaining the operation, and FIGS. 3 and 4 are diagrams showing measurement results. Reference numeral 1 denotes a magnetic sensor for stress detection; 2 denotes a constant object tP1; 9 denotes a gap detection coil; and 10 denotes a magnetic sensor for gap measurement.

Claims (1)

【特許請求の範囲】[Claims] 励磁系と検出系とからなる応力検出用の磁気センサ1を
被測定物2に対向させたときの検出値V_1を、このと
きの被測定物2の応力による磁気特性変化に対して変化
しなくなる位置に設けられて上記応力検出用の磁気セン
サ1と被測定物間のギャップを測定するギャップ検出用
の磁気センサ10からの検出値V_2にて除し、その結
果を応力測定値F(τ)とすることを特徴とする磁歪式
応力センサによる応力測定方法。
The detected value V_1 when the magnetic sensor 1 for stress detection consisting of an excitation system and a detection system is opposed to the object to be measured 2 does not change due to the change in magnetic properties due to the stress of the object to be measured 2 at this time. The result is divided by the detected value V_2 from the gap detection magnetic sensor 10 which is installed at a position to measure the gap between the stress detection magnetic sensor 1 and the object to be measured, and the result is the stress measurement value F(τ). A method for measuring stress using a magnetostrictive stress sensor, characterized in that:
JP11502789A 1989-05-10 1989-05-10 Stress measuring method using magnetostruction type stress sensor Pending JPH02296122A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11502789A JPH02296122A (en) 1989-05-10 1989-05-10 Stress measuring method using magnetostruction type stress sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11502789A JPH02296122A (en) 1989-05-10 1989-05-10 Stress measuring method using magnetostruction type stress sensor

Publications (1)

Publication Number Publication Date
JPH02296122A true JPH02296122A (en) 1990-12-06

Family

ID=14652410

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11502789A Pending JPH02296122A (en) 1989-05-10 1989-05-10 Stress measuring method using magnetostruction type stress sensor

Country Status (1)

Country Link
JP (1) JPH02296122A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06307948A (en) * 1993-04-27 1994-11-04 Osaka Gas Co Ltd Method for measuring magnetostrictive stress of anticorrosion pipe

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62121325A (en) * 1985-11-22 1987-06-02 Japanese National Railways<Jnr> Electromagnetic type stress measuring instrument not influenced by lift-off

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62121325A (en) * 1985-11-22 1987-06-02 Japanese National Railways<Jnr> Electromagnetic type stress measuring instrument not influenced by lift-off

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06307948A (en) * 1993-04-27 1994-11-04 Osaka Gas Co Ltd Method for measuring magnetostrictive stress of anticorrosion pipe

Similar Documents

Publication Publication Date Title
EP0598720B1 (en) Nonintrusive flow sensing system
US5360268A (en) Ultrasonic temperature measuring apparatus
US4708021A (en) Arrangement for contactless measurement of the velocity of a moving medium
US5419206A (en) Phase independent torque detection and processing circuit for sensing device
US6816808B2 (en) Peak switch detector for transit time ultrasonic meters
JPH033164B2 (en)
JPH02296122A (en) Stress measuring method using magnetostruction type stress sensor
US4672316A (en) Method for calibrating a muzzle velocity measuring device
US5652509A (en) Device for determining the velocity of a longitudinally traveling elongate textile material, especially a yarn, using electronic sensors
JPH0933204A (en) Measuring method surely measuring space between conductive reaction rail and functional surface relatively moved to conductive reaction rail and sensor fitted to measuring method thereof
JPH0815619B2 (en) Plate speed detection method in tandem rolling mill
US4467280A (en) System for measuring the length of a long magnetizable material
JPH04120456A (en) Non-destructive testing equipment using SQUID
JP2577456B2 (en) Thickness measuring device
JPH0833452B2 (en) Embedded cable position measuring instrument
JPS5950304A (en) Displacement measuring device
CA1230379A (en) Measuring the thickness of a non-metallic coating on an arcuate metal surface
JPS59109833A (en) Measuring device of temperature of metal surface
JPS5921483B2 (en) fluid measuring device
JPH01189511A (en) Non-magnetic sheet thickness measuring device
JP2582003Y2 (en) Fluidic flow meter
JPS63311103A (en) Thickness measurement
JPH04125407A (en) Measuring apparatus of roll profile
JPH1073614A (en) Current meter
SU1291912A1 (en) Method of automatic integrated calibration checking of instruments