JPS5950922B2 - Principal stress measurement method for magnetic materials - Google Patents
Principal stress measurement method for magnetic materialsInfo
- Publication number
- JPS5950922B2 JPS5950922B2 JP6266679A JP6266679A JPS5950922B2 JP S5950922 B2 JPS5950922 B2 JP S5950922B2 JP 6266679 A JP6266679 A JP 6266679A JP 6266679 A JP6266679 A JP 6266679A JP S5950922 B2 JPS5950922 B2 JP S5950922B2
- Authority
- JP
- Japan
- Prior art keywords
- principal stress
- iron loss
- stress
- magnetic
- magnetic material
- 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
Links
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- Measuring Magnetic Variables (AREA)
Description
【発明の詳細な説明】
本発明は1個の磁気センサを用いて磁性材料の鉄損を測
定し、磁性材料に作用する主応力の方向及び大きさを求
める磁性材料の主応力測定方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring the principal stress of a magnetic material by measuring the core loss of the magnetic material using one magnetic sensor and determining the direction and magnitude of the principal stress acting on the magnetic material. It is.
組立構造物に使用される鉄鋼等の磁性材料では、一般に
、磁性材料に作用する応力と鉄損特性の間に、第1図に
示すような関係があり、この関係を利用して磁性材料に
作用している応力の方向と大きさを磁気センサを用いて
測定することができる。For magnetic materials such as steel used in assembled structures, there is generally a relationship between the stress acting on the magnetic material and the iron loss characteristics as shown in Figure 1. The direction and magnitude of the acting stress can be measured using a magnetic sensor.
即ち、第3図に示すように、磁気センサ2は、断面コの
字形の磁心5に励磁コイル(一次コイル)3及び出カニ
次電圧コイル(二次コイル)4を巻いて構成されている
。この磁気センサ2の中心を第2図に示すように、磁性
材料1の表面の応力を測定しようとする測定点6に一致
させて当て、励磁コイル3を交流励磁すれば、磁心5か
らの磁束は、第3図に示すように磁性材料1の中を矢印
の方向に流れ、再び磁心5に戻るような閉磁路を形成す
る。この時、二次コイルに誘起される出カニ次電圧を一
定に保持するように一次側電圧を制御して、一次コイル
を電力計(図示せず)の電流端子に、二次コイルを電力
計の電圧端子に接続して鉄損を測定すれば、磁性材料1
の測定点6に作用する磁気センサ2の中心線方向の応力
を第1図の関係から求めることができる。磁気センサ2
の中心線の方向は、第2図に示すように磁気センサ2の
長手方向にとつてもよいし、長手方向に直角方向にとつ
てもよい。いま、磁性材料1が或る応力状態(引長、圧
縮)にある時、測定点6の応力を測定するには、その測
定点6に作用する主応力の方向と大きさを求めなければ
ならない。That is, as shown in FIG. 3, the magnetic sensor 2 is constructed by winding an excitation coil (primary coil) 3 and an output voltage coil (secondary coil) 4 around a magnetic core 5 having a U-shaped cross section. As shown in FIG. 2, if the center of this magnetic sensor 2 is aligned with the measurement point 6 at which the stress on the surface of the magnetic material 1 is to be measured, and the excitation coil 3 is excited with alternating current, the magnetic flux from the magnetic core 5 is As shown in FIG. 3, the magnetic material 1 forms a closed magnetic path that flows in the direction of the arrow in the magnetic material 1 and returns to the magnetic core 5 again. At this time, the primary voltage is controlled to keep the output voltage induced in the secondary coil constant, and the primary coil is connected to the current terminal of the wattmeter (not shown), and the secondary coil is connected to the wattmeter. If you measure the iron loss by connecting it to the voltage terminal of magnetic material 1.
The stress in the center line direction of the magnetic sensor 2 acting on the measurement point 6 can be determined from the relationship shown in FIG. Magnetic sensor 2
The direction of the center line may be in the longitudinal direction of the magnetic sensor 2, as shown in FIG. 2, or may be in the direction perpendicular to the longitudinal direction. Now, in order to measure the stress at the measurement point 6 when the magnetic material 1 is in a certain stress state (tension, compression), it is necessary to find the direction and magnitude of the principal stress acting on the measurement point 6. .
そのために、従来は1個の磁気センサ2の中心が測定点
6と一致するようにして、磁気センサ2を測定点6の周
りに回動させて、最大または最小の鉄損を生ずる磁気セ
ンサ2の中心線の方向を求め、その方向及びその方向に
直角方向の鉄損を求め、その鉄損から主応力の大きさを
求めていた。この場合、磁性材料1の応力0の時の鉄損
をWoとすると、第1図から解るように、磁性材料1に
圧縮応力が作用している時は、その鉄損はWMはWoよ
り大きく、引張応力が作用している時は、その鉄損Wm
はWMより小さくなる。For this purpose, conventionally, the center of one magnetic sensor 2 is aligned with the measurement point 6, and the magnetic sensor 2 is rotated around the measurement point 6 to produce the maximum or minimum iron loss. The direction of the center line was determined, the iron loss in that direction and the direction perpendicular to that direction was determined, and the magnitude of the principal stress was determined from the iron loss. In this case, if the iron loss of the magnetic material 1 when the stress is 0 is Wo, then as can be seen from Figure 1, when compressive stress is acting on the magnetic material 1, the iron loss WM is larger than Wo. , when tensile stress is acting, the iron loss Wm
becomes smaller than WM.
また、任意の点における応力分布を鉄損によつて測定す
るために、磁気センサ2をその点を中心として回動゜さ
せて鉄損を測定すると第4図のように主応力に相当する
鉄損の最大及び最小の方向に対して左右対称に分布する
ことが実験でも確認された。この曲線より解るように、
鉄損の最大又は最小の点の近傍は曲線がなだらかなため
、1個の磁気センサワ2で鉄損の最大又は最小の方向及
びその方向の鉄損を直接正確に測定することは困難であ
る。従つて、正確に主応力の方向と大きさを求めること
ができないという欠点があつた。本発明は以上の点に鑑
み、1個の磁気センサを用いて、磁性材料の主応力の方
向と大きさを正確に求めることができる磁性材料の主応
力測定方法を提供するものである。In addition, in order to measure the stress distribution at an arbitrary point in terms of iron loss, when the magnetic sensor 2 is rotated around that point and the iron loss is measured, the iron loss corresponding to the principal stress is measured as shown in Figure 4. Experiments have also confirmed that the loss is distributed symmetrically with respect to the directions of maximum and minimum loss. As you can see from this curve,
Since the curve is gentle near the point where the iron loss is maximum or minimum, it is difficult to directly and accurately measure the direction of the maximum or minimum iron loss and the iron loss in that direction with one magnetic sensor 2. Therefore, there was a drawback that the direction and magnitude of the principal stress could not be determined accurately. In view of the above points, the present invention provides a method for measuring principal stress in a magnetic material that can accurately determine the direction and magnitude of the principal stress in the magnetic material using one magnetic sensor.
以下、本発明の方法の一実施例を図面について説明する
。An embodiment of the method of the present invention will be described below with reference to the drawings.
第5図に示すように、磁性材料7の主応力を測定しよう
とする点8に磁気センサ2の中心を一致させて取付け、
一次コイルを励磁して、磁気センサ2を点8を中心とし
て回動させ、鉄損が等しい相隣る二つの方向B,B″又
はB″,B″″(第4図参照)を求め、磁気センサ2の
最初の出発方向BOと為す角度をそれぞれα1,α2,
α3とすれば、求める主応力の方向は、又はWWの中心
を通る垂直線の方向或はα1−α2又は、α2α3の角
度の2等分線の方向である。As shown in FIG. 5, the magnetic sensor 2 is mounted with its center aligned with the point 8 at which the principal stress of the magnetic material 7 is to be measured.
Excite the primary coil, rotate the magnetic sensor 2 around point 8, and find two adjacent directions B, B'' or B'', B'''' (see Figure 4) with equal iron loss, The angles formed with the initial starting direction BO of the magnetic sensor 2 are α1, α2,
Assuming α3, the direction of the principal stress to be determined is the direction of the perpendicular line passing through the center of WW, or the direction of the bisector of the angle α1-α2 or α2α3.
次に応力が0のときの鉄損WOが既知の場合は、主応力
の方向の鉄損WM、この主応力と異る方向、例えば直角
方向の鉄損Wmを求め、第1図より直接主応力を求めて
もよいが、WM−WOの値はWO・,WM・,Wrrl
と比べて小さい値なので、第1図の曲線より読取つた値
はW。Next, if the iron loss WO when the stress is 0 is known, find the iron loss WM in the direction of the principal stress and the iron loss Wm in a direction different from this principal stress, for example, in a direction perpendicular to it, and directly use the main stress from Fig. 1. Although the stress may be calculated, the value of WM-WO is WO・,WM・,Wrrl
Since it is a small value compared to , the value read from the curve in Figure 1 is W.
が温度やわずかの入力電圧の変化等によつて変化するの
で、これにより求めた値も誤差が大きくなる。故に本発
明においては、WOを用いないで次式よりWM及びWr
rlより正確に主応力を求めることができることを確認
した。即ち、σを主応力、αを磁性材料の材質より決ま
る係数とするとより求めることができる。Since the value changes due to temperature, slight changes in input voltage, etc., the obtained value also has a large error. Therefore, in the present invention, WM and Wr are calculated from the following equation without using WO.
It was confirmed that the principal stress can be determined more accurately than rl. That is, it can be more easily determined by setting σ to be the principal stress and α to be a coefficient determined by the quality of the magnetic material.
この関係を図示したものが第6図である。以上のように
、本発明の磁性材料の主応力測定方法によるときは、1
個の磁気センサを磁性材料の主応力を測定しようとする
表面の一点に磁気センサの中心を合わせ、一次コイルを
励磁して、磁気センサをその点の周りに回動させ、鉄損
が等しiい相隣る二つの方向を測定するだけで主応力の
方向を正確に求めることができ、かつその主応力の方向
の鉄損と、その主応力に直角の方向の鉄損を測定して、
主応力の大きさを正確に求めることができるので、従来
の方法より、一層正確に磁性材.料の応力状態を知るこ
とができる。FIG. 6 illustrates this relationship. As described above, when using the principal stress measurement method for magnetic materials of the present invention, 1
Align the center of the magnetic sensor with a point on the surface where you want to measure the principal stress of the magnetic material, excite the primary coil, and rotate the magnetic sensor around that point until the core loss is equal. The direction of the principal stress can be determined accurately by simply measuring two adjacent directions, and the iron loss in the direction of the principal stress and the iron loss in the direction perpendicular to the principal stress can be determined. ,
Since the magnitude of the principal stress can be determined accurately, magnetic materials can be measured more accurately than conventional methods. It is possible to know the stress state of the material.
第1図は磁性材料の応力と鉄損の関係を示す特性曲線図
、第2図は従来の1個の磁気センサを用いた主応力測定
方法の説明図、第3図は第2図のA−A断面拡大図、第
4図は、磁性材料の表面上の測定点の周りの応力分布を
鉄損で表わした特性曲線図、第5図は本発明の主応力の
測定方法の一実施例の説明図、第6図は主応力σとの関
係を示す特性曲線図である。
1,7・・・・・・磁性材料、2・・・・・・磁気セン
サ、3・・・・・・励磁コイル(一次コイル)、4・・
・・・・出力[ヮ沒d圧コイル(二次コイル)、5・・・
・・・磁心。Figure 1 is a characteristic curve diagram showing the relationship between stress and iron loss of magnetic materials, Figure 2 is an explanatory diagram of the conventional principal stress measurement method using one magnetic sensor, and Figure 3 is A of Figure 2. - An enlarged cross-sectional view of A, FIG. 4 is a characteristic curve diagram showing the stress distribution around the measurement point on the surface of the magnetic material in terms of iron loss, and FIG. 5 is an example of the method for measuring principal stress of the present invention. FIG. 6 is a characteristic curve diagram showing the relationship with principal stress σ. 1, 7... Magnetic material, 2... Magnetic sensor, 3... Excitation coil (primary coil), 4...
...output [ヮ沒d pressure coil (secondary coil), 5...
···core.
Claims (1)
、磁性材料の測定点の周りに回動させ、鉄損が等しい相
隣る二つの方向を求めて、前記測定点の主応力の方向を
決定し、その主応力の方向の鉄損及びその主応力と異な
る方向の鉄損を求めて、主応力の大きさを決定すること
を特徴とする磁性材料の主応力測定方法。1 Rotate one magnetic sensor that can measure iron loss in any direction around a measurement point of the magnetic material, find two adjacent directions with equal iron loss, and calculate the principal stress at the measurement point. 1. A method for measuring principal stress in a magnetic material, characterized in that the direction is determined, and the magnitude of the principal stress is determined by determining the iron loss in the direction of the principal stress and the iron loss in a direction different from the principal stress.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6266679A JPS5950922B2 (en) | 1979-05-23 | 1979-05-23 | Principal stress measurement method for magnetic materials |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6266679A JPS5950922B2 (en) | 1979-05-23 | 1979-05-23 | Principal stress measurement method for magnetic materials |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55155223A JPS55155223A (en) | 1980-12-03 |
| JPS5950922B2 true JPS5950922B2 (en) | 1984-12-11 |
Family
ID=13206839
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6266679A Expired JPS5950922B2 (en) | 1979-05-23 | 1979-05-23 | Principal stress measurement method for magnetic materials |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5950922B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57161526A (en) * | 1981-03-31 | 1982-10-05 | Shibaura Eng Works Co Ltd | Measuring method for axial tension of bolt |
| CN106768504A (en) * | 2016-11-29 | 2017-05-31 | 中国特种设备检测研究院 | The detecting system of material principal stress, detection sensor and detection method |
-
1979
- 1979-05-23 JP JP6266679A patent/JPS5950922B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55155223A (en) | 1980-12-03 |
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