JPH0356838A - Magnetostrictive sensor built into tires - Google Patents
Magnetostrictive sensor built into tiresInfo
- Publication number
- JPH0356838A JPH0356838A JP19224289A JP19224289A JPH0356838A JP H0356838 A JPH0356838 A JP H0356838A JP 19224289 A JP19224289 A JP 19224289A JP 19224289 A JP19224289 A JP 19224289A JP H0356838 A JPH0356838 A JP H0356838A
- Authority
- JP
- Japan
- Prior art keywords
- magnetostrictive sensor
- stress
- tire
- sensor built
- shaped case
- 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.)
- Granted
Links
Landscapes
- Force Measurement Appropriate To Specific Purposes (AREA)
- Measuring Magnetic Variables (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は、磁歪センサを使用して材料に作用する応力
を測定する磁歪センサ、特に磁歪センサのりフトオフを
一定に保って、精度よく応力測定のできるタイヤ内組込
み型磁歪センサに関する.[従来技術コ
磁歪センサを使用して材料に作用する応力を測定する方
法は、橋梁等の大きな構造物あるいは配管等の長尺の構
造物に作用する応力を、場所を移動しながら連続的に測
定できるという利点があり、今後ますますこのような応
力の連続測定に適用されるものと思われる.
上記した磁歪センサによる応力測定の原理は、次のとお
りである.すなわち、一般に強磁性体の材料に応力が作
用すると、磁歪効果により応力の作用する方向の透磁率
が、応力の作用する方向と直交する方向の透磁率よりわ
ずかではあるが大きくなる.そして第3図の矢印方向に
σの応力が働いている状態にある材料に、磁歪センサ2
1を構成している直交して組合せたコア22およびコア
23を、それぞれのコアが材料24に作用する応力の方
向とは45度傾いた方向を示すような状態で対面させる
.そして、第4図のようにコア22に巻いたコイル(励
磁コイル)25に電流を流すと、コア22の足26から
出た磁束のうち、大部分は直接コア22の他の足27へ
向うが、一部は第3図に矢印で示すようにコア22の足
26から材料24の応力の作用している方向に流れてコ
ア23の足28に達し、コア23中を流れてコア23の
他の足29から再び材料24の応力の作用している方向
に流れてコア22の足27に達し、コア22中を流れて
コア22の足26に達する.磁束の一部がこのような経
路をたどるのは、材料23の応力の作用する方向の透磁
率が、応力の作用する方向と直交する方向の透磁率より
太きいがらである.以上のような磁気回路を、交流磁束
について考えると、コア23に巻いたコイル(異方性検
出コイル〉30には電圧が生じる.この電圧Vは(1)
式で表される.
V=M・K・ (μ8−μy) ・・・・・・・・〈1
〉ただし、
M:材料の磁気的特性およびセンサと材料との距離(リ
フト オフ)によりよる定数
(磁歪感度)
K:励磁条件、コイルの条件によって定まる定数
μX=材料の応力作用方向の透磁率
11y 二材料の応力作用方向と直交する方向の透磁率
すなわち、磁歪センサの出力電圧Vは、材科の透磁率の
差(μ、一μ,)に比例し、これはまた材料の応力作用
方向の応力6Xと材料の応力作用方向と直交する方向の
応力6yの差(5X−15y>に比例することになるの
で、この電圧■により材料に作用する応力を把握するこ
とができるのである.
〔発明が解決しようとする課題〕
上記した磁歪センサを用いて材料に作用する応力を測定
する方法においては、〈1〉式の定数Mが磁歪センサの
リフトオフによって異なってくるので、リフトオフが一
定していないと、同一の応力が作用していても、磁歪セ
ンサの出力電圧■が場所によって異なり、このVから応
力を把握することは、困難になるという問題点がある.
そして、連続的に測定箇所を移動しても、リフトオフを
一定に保つようにしたタイヤ内組込み型磁歪センサは従
来なかった.
この発明は、従来技術の上述のような問題点を解消し、
リフトオフを一定に保つことができるので、材料に作用
する応力を精度よく連続的に測定できるタイヤ内組込み
型磁歪センサを提供することを目的としている.
(3題を解決するための手段コ
この発明に係るタイヤ内組込み型磁歪センサは、磁歪セ
ンサを用い磁気異方性を検出して材料に作用する応力を
測定する磁歪センサにおいて、固定軸と、固定軸のまわ
りに軸受を介して回転するタイヤ状ケースと、タイヤ状
ケースの内部に前記固定軸に吊り下げて配備した磁歪セ
ンサとがらなるタイヤ内組込み型磁歪センサである.[
作用j
この発明に係るタイヤ内組込み型磁歪センサは、磁歪セ
ンサを用い磁気異方性を検出して材料に作用する応力を
測定する磁歪センサにおいて、固定軸と、固定軸のまわ
りに軸受を介して回転するタイヤ状ケースと、タイヤ状
ケースの内部に前記固定軸に吊り下げて配備した磁歪セ
ンサとがら構成されている.したがって、固定軸を測定
面に平行になるようにして、タイヤ状ケースを応力を測
定しようとする対称物に接触させ、タイヤ状ケースを回
転させながら連続的に磁気異方性を検出するようにする
と、タイヤ状ケース内の磁歪センサと対象物間のリフト
オフは一定に保たれるので、長区間にわたって材料に作
用する応力を連続的に、しかも精度よく測定することが
できる.[実施例]
本発明の1実施例のタイヤ内組込み型磁歪センサを、第
l図および第2図ににより説明する.第1図は、本発明
の1実施例のタイヤ内組込み型磁歪センサの側面図、第
2図は本発明の1実施例のタイヤ内組込み型磁歪センサ
の縦断面図である。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magnetostrictive sensor that measures stress acting on a material using a magnetostrictive sensor, and in particular to a magnetostrictive sensor that maintains a constant slip-off to accurately measure stress. This article relates to a magnetostrictive sensor that can be built into tires. [Conventional technology] A method of measuring stress acting on a material using a magnetostrictive sensor is to measure stress acting on large structures such as bridges or long structures such as piping continuously while moving from place to place. It has the advantage of being able to measure stress, and it is expected that it will be increasingly applied to continuous measurement of stress in the future. The principle of stress measurement using the magnetostrictive sensor described above is as follows. In other words, when stress is generally applied to a ferromagnetic material, the magnetic permeability in the direction in which the stress acts due to the magnetostrictive effect becomes slightly larger than the magnetic permeability in the direction orthogonal to the direction in which the stress acts. Then, the magnetostrictive sensor 2
The cores 22 and 23, which are orthogonally combined and make up the material 24, are made to face each other in such a way that each core presents a direction inclined at 45 degrees from the direction of the stress acting on the material 24. Then, when a current is passed through the coil (excitation coil) 25 wound around the core 22 as shown in FIG. However, as shown by the arrow in FIG. 3, a portion flows from the foot 26 of the core 22 in the direction of stress in the material 24, reaches the foot 28 of the core 23, flows through the core 23, and flows into the core 23. From the other leg 29, the material 24 flows again in the direction in which the stress is acting, reaches the leg 27 of the core 22, flows through the core 22, and reaches the leg 26 of the core 22. Part of the magnetic flux follows such a path because the magnetic permeability of the material 23 in the direction in which the stress acts is greater than the magnetic permeability in the direction perpendicular to the direction in which the stress acts. Considering the above magnetic circuit in terms of alternating current magnetic flux, a voltage is generated in the coil (anisotropy detection coil) 30 wound around the core 23. This voltage V is (1)
It is expressed by the formula. V=M・K・(μ8−μy) ・・・・・・・・・〈1
〉However, M: A constant (magnetostriction sensitivity) determined by the magnetic properties of the material and the distance (lift-off) between the sensor and the material K: A constant determined by the excitation conditions and coil conditions μX = Magnetic permeability of the material in the direction of stress action 11y The magnetic permeability of the two materials in the direction perpendicular to the direction of stress action, that is, the output voltage V of the magnetostrictive sensor, is proportional to the difference in magnetic permeability (μ, 1μ,) of the materials, which is also in the direction of stress action of the materials. Since it is proportional to the difference between stress 6X and stress 6y in the direction perpendicular to the direction of stress action on the material (5X - 15y>), the stress acting on the material can be determined from this voltage. [Invention] In the method of measuring stress acting on a material using the magnetostrictive sensor described above, the constant M in equation (1) changes depending on the lift-off of the magnetostrictive sensor, so the lift-off is not constant. Even if the same stress is applied, the output voltage (2) of the magnetostrictive sensor differs depending on the location, and there is a problem in that it is difficult to understand the stress from this V.
Furthermore, there has never been a magnetostrictive sensor built into a tire that maintains a constant lift-off even when the measurement location is continuously moved. This invention solves the above-mentioned problems of the prior art,
The purpose of this invention is to provide a magnetostrictive sensor built into a tire that can accurately and continuously measure the stress acting on a material because the lift-off can be kept constant. (Means for solving the three problems) A magnetostrictive sensor built into a tire according to the present invention uses a magnetostrictive sensor to detect magnetic anisotropy and measure stress acting on a material. This is a magnetostrictive sensor built into a tire, consisting of a tire-shaped case that rotates around a fixed shaft via a bearing, and a magnetostrictive sensor that is suspended from the fixed shaft inside the tire-shaped case.
Effect j The magnetostrictive sensor built into a tire according to the present invention is a magnetostrictive sensor that uses a magnetostrictive sensor to detect magnetic anisotropy and measure stress acting on a material. It consists of a tire-shaped case that rotates, and a magnetostrictive sensor that is suspended from the fixed shaft inside the tire-shaped case. Therefore, with the fixed axis parallel to the measurement surface, the tire-shaped case is brought into contact with the object whose stress is to be measured, and the magnetic anisotropy is continuously detected while rotating the tire-shaped case. Then, the lift-off between the magnetostrictive sensor inside the tire-shaped case and the target object is kept constant, making it possible to measure the stress acting on the material continuously and with high precision over a long period of time. [Example] An in-tire magnetostrictive sensor according to an example of the present invention will be explained with reference to FIGS. 1 and 2. FIG. 1 is a side view of a magnetostrictive sensor built into a tire according to an embodiment of the present invention, and FIG. 2 is a longitudinal sectional view of a magnetostrictive sensor built into a tire according to an embodiment of the present invention.
このタイヤ内組込み型磁歪センサは、図示していないが
台車のフレーム等に固定した固定!!lと、固定軸1の
まわりに軸受2を介して回転するタイヤ状ケース3と、
タイヤ状ケース3の内部にがり固定軸1に吊り下げ金具
4により吊り下げた磁歪センサ5とから楕或されている
。さらにタイヤ状ケース3は、側板6と、硬質樹脂でで
きており被測定物の表面に接触する車輪部分7がら構或
されている.
本発明の1実施例のタイヤ内組込み型磁歪センサは、上
記のように構成されているので、前記車輪部分7が被測
定物に密着するような状態でタイヤ内組込み型磁歪セン
サを移動させていくと、被測定物のどの場所においてら
、磁歪センサ5と被測定物間の距wL(リフトオフ〉は
一定であるので、被測定物に作用している応力の大きさ
に比例2た磁気異方性を検出することができる.したが
って、被測定物に作用している応力の応力分布を正確に
把握することができる.
[発明の効果]
この発明により、磁歪センサのリフトオフを一定に保つ
ことができ,11I造物に作用する応力の分布状態を正
確に把握することができる.Although this magnetostrictive sensor built into the tire is not shown, it is fixed to the frame of the truck! ! l, a tire-shaped case 3 that rotates around a fixed shaft 1 via a bearing 2,
The inside of the tire-shaped case 3 is oval shaped from a magnetostrictive sensor 5 suspended from a fixed shaft 1 by a hanging fitting 4. Furthermore, the tire-shaped case 3 is composed of a side plate 6 and a wheel portion 7 made of hard resin and in contact with the surface of the object to be measured. Since the magnetostrictive sensor built into a tire according to one embodiment of the present invention is configured as described above, the magnetostrictive sensor built into a tire can be moved in a state where the wheel portion 7 is in close contact with the object to be measured. Since the distance wL (lift-off) between the magnetostrictive sensor 5 and the object to be measured is constant at any location on the object to be measured, the magnetic difference is proportional to the magnitude of the stress acting on the object to be measured. The orientation can be detected. Therefore, the stress distribution of the stress acting on the object to be measured can be accurately grasped. [Effects of the Invention] With this invention, the lift-off of the magnetostrictive sensor can be kept constant. It is possible to accurately grasp the distribution of stress acting on the 11I structure.
第1図は本発明の1実施例のタイヤ内組込み型磁歪セン
サの側面図、第2図は本発明の1実施例のタイヤ内組込
み型磁歪センサの縦断面図、第3図は磁歪センサで応力
を測定している状態を示す斜視図、第4図は磁歪センサ
を示す斜視図である.FIG. 1 is a side view of a magnetostrictive sensor built into a tire according to an embodiment of the present invention, FIG. 2 is a longitudinal sectional view of a magnetostrictive sensor built into a tire according to an embodiment of the present invention, and FIG. A perspective view showing a state in which stress is being measured. FIG. 4 is a perspective view showing a magnetostrictive sensor.
Claims (1)
する応力を測定する磁歪センサにおいて、固定軸と、固
定軸のまわりに軸受を介して回転するタイヤ状ケースと
、タイヤ状ケースの内部に前記固定軸に吊り下げて配備
した磁歪センサとからなることを特徴とするタイヤ内組
込み型磁歪センサ。In a magnetostrictive sensor that uses a magnetostrictive sensor to detect magnetic anisotropy and measure stress acting on a material, there is a fixed shaft, a tire-shaped case that rotates around the fixed shaft via a bearing, and an interior of the tire-shaped case. and a magnetostrictive sensor suspended from the fixed shaft.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19224289A JP2727671B2 (en) | 1989-07-24 | 1989-07-24 | Magnetostrictive sensor built into the tire |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19224289A JP2727671B2 (en) | 1989-07-24 | 1989-07-24 | Magnetostrictive sensor built into the tire |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0356838A true JPH0356838A (en) | 1991-03-12 |
| JP2727671B2 JP2727671B2 (en) | 1998-03-11 |
Family
ID=16288025
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19224289A Expired - Fee Related JP2727671B2 (en) | 1989-07-24 | 1989-07-24 | Magnetostrictive sensor built into the tire |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2727671B2 (en) |
-
1989
- 1989-07-24 JP JP19224289A patent/JP2727671B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JP2727671B2 (en) | 1998-03-11 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |