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JPH0226172B2 - - Google Patents
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JPH0226172B2 - - Google Patents

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Publication number
JPH0226172B2
JPH0226172B2 JP54095036A JP9503679A JPH0226172B2 JP H0226172 B2 JPH0226172 B2 JP H0226172B2 JP 54095036 A JP54095036 A JP 54095036A JP 9503679 A JP9503679 A JP 9503679A JP H0226172 B2 JPH0226172 B2 JP H0226172B2
Authority
JP
Japan
Prior art keywords
iron loss
magnetic sensor
stress
primary coil
magnetic
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
JP54095036A
Other languages
Japanese (ja)
Other versions
JPS5619466A (en
Inventor
Tadamasa Nakamura
Hiroshi Yasojima
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.)
Shibaura Mechatronics Corp
Original Assignee
Shibaura Engineering Works 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 Shibaura Engineering Works Co Ltd filed Critical Shibaura Engineering Works Co Ltd
Priority to JP9503679A priority Critical patent/JPS5619466A/en
Publication of JPS5619466A publication Critical patent/JPS5619466A/en
Publication of JPH0226172B2 publication Critical patent/JPH0226172B2/ja
Granted legal-status Critical Current

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  • Force Measurement Appropriate To Specific Purposes (AREA)
  • Measuring Magnetic Variables (AREA)
  • Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)

Description

【発明の詳細な説明】 本発明は、磁性材料に応力が作用すると、その
応力に関連してその磁性材料の鉄損が変化するこ
とを利用して、磁性材料の表面に磁気センサを接
触させて配置し、磁性材料の応力を測定する応力
測定装置に関するものである。
Detailed Description of the Invention The present invention utilizes the fact that when stress acts on a magnetic material, the core loss of the magnetic material changes in relation to the stress, and a magnetic sensor is brought into contact with the surface of the magnetic material. The present invention relates to a stress measuring device that is placed in a magnetic material and measures stress in a magnetic material.

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又は応
力と鉄損変化率の間には、第1図又は第2図に示
すような関係がある。即ち、第1図は磁性材料に
作用する応力と鉄損の関係を、第2図は磁性材料
に作用する応力と鉄損変化率の関係を示した図で
ある。ここに鉄損変化率とは、磁性材料に応力が
作用しないときの鉄損をWo、或る大きさの応力
が作用したときの鉄損をWiとしたとき、(Wi−
Wo)/Wo×100(%)で表わしたものである。
従つて、第1図又は第2図から、磁性材料の鉄損
を測定することにより、その磁性材料に作用して
いる応力を求めることができる。
For magnetic materials such as steel used in assembled structures, there is generally a relationship between stress and iron loss acting on the magnetic material, or between stress and iron loss change rate, as shown in Figure 1 or Figure 2. . That is, FIG. 1 shows the relationship between the stress acting on the magnetic material and iron loss, and FIG. 2 shows the relationship between the stress acting on the magnetic material and the rate of change in iron loss. Here, the rate of change in iron loss is defined as (Wi−
It is expressed as Wo)/Wo×100 (%).
Therefore, by measuring the iron loss of the magnetic material from FIG. 1 or 2, the stress acting on the magnetic material can be determined.

両図から明らかなように、圧縮応力と鉄損又は
鉄損変化率はほぼ線形関係にあるので、引張応力
を求める場合、引張応力の作用している方向と直
角方向の圧縮応力の作用している方向の鉄損を測
定して、先ず圧縮応力を求め、ボアゾン比の関係
より引張応力に換算した方が、正確な応力を求め
ることができる。
As is clear from both figures, there is a nearly linear relationship between compressive stress and iron loss or rate of change in iron loss, so when calculating tensile stress, it is necessary to calculate the A more accurate stress can be obtained by measuring the iron loss in the direction in which the iron is located, first obtaining the compressive stress, and then converting it to tensile stress based on the relationship of the Boisson ratio.

通常、応力を測定するには、第3図のA−A断
面を拡大した第4図に示すように、断面略コの字
形の磁心5に一次コイル(励磁コイル)3と二次
コイル(出力二次電圧コイル)4を巻いて構成し
た磁気センサ2(磁気センサ2の二次コイル4の
代りに磁気素子例えばホール素子を用いてもよい
が、以下の説明は二次コイル4を用いた場合につ
いて述べる)を用いて、第3図に示すように、磁
性材料1の測定点30に磁気センサ2の中心を合
わせ、かつ応力状態に応じて磁気センサ2の長手
方向又は長手方向に直角方向の中心線を測定しよ
うとする応力の方向に合わせて、磁気センサ2を
磁性材料1の表面に密着させ配置する。第5図
は、上述のように、磁性材料1に磁気センサ2を
密着させて配置し、鉄損を測定しその測定した鉄
損より鉄損変化率を求め、第2図の関係より応力
に換算して、磁性材料1に作用している応力を求
める従来の応力測定装置のブロツク線図である。
この従来の鉄損を利用した磁性材料の応力測定装
置は、鉄損測定装置19、A/D変換器12、鉄
損指示計13、初期値設定器14、演算器15、
応力指示計16及び指示計17より構成され、ま
た鉄損測定装置19は交流電源6、磁気センサ
2、第1増幅器7、第2増幅器8、電流計11、
出力二次電圧設定器9及び第1演算増幅器10よ
り構成されている。即ち、磁気センサ2の一次コ
イル3は、交流電源6と、第一増幅器7を介して
電力計11の電流端子に接続され、二次コイル4
は、整流器(図示せず)を介して第1演算増幅器
10に、また第2増幅器8を介して電力計11の
電圧端子に接続されている。出力二次電圧設定器
9は第1演算増幅器10に接続されている。この
第1演算増幅器10の出力側は交流電源6に接続
されている。電力計11は、A/D変換器12に
接続され、このA/D変換器12の出力側は、鉄
損指示計13と演算器15に接続されている。な
お、デイジタルに変換しない場合はA/D変換器
12よりでなく、電力計11を演算器15に直接
接続しても良いことは自明である。この演算器1
5には初期値設定器14と応力指示計16も接続
されている。指示計17はスイツチ18を介して
第1増幅器7と第2増幅器8の出力側に接続され
ている。
Normally, to measure stress, as shown in FIG. 4, which is an enlarged cross-section of A-A in FIG. A magnetic sensor 2 configured by winding a secondary voltage coil 4 (a magnetic element such as a Hall element may be used in place of the secondary coil 4 of the magnetic sensor 2, but the following explanation is based on the case where the secondary coil 4 is used) As shown in FIG. The magnetic sensor 2 is placed in close contact with the surface of the magnetic material 1 so that the center line is aligned with the direction of the stress whose center line is to be measured. Figure 5 shows that, as mentioned above, the magnetic sensor 2 is placed in close contact with the magnetic material 1, the iron loss is measured, the iron loss change rate is determined from the measured iron loss, and the stress FIG. 2 is a block diagram of a conventional stress measuring device for determining the stress acting on the magnetic material 1 in terms of conversion.
This conventional stress measuring device for magnetic materials using iron loss includes an iron loss measuring device 19, an A/D converter 12, an iron loss indicator 13, an initial value setting device 14, a calculator 15,
It is composed of a stress indicator 16 and an indicator 17, and the iron loss measuring device 19 includes an AC power source 6, a magnetic sensor 2, a first amplifier 7, a second amplifier 8, an ammeter 11,
It is composed of an output secondary voltage setting device 9 and a first operational amplifier 10. That is, the primary coil 3 of the magnetic sensor 2 is connected to the current terminal of the wattmeter 11 via the AC power source 6 and the first amplifier 7, and the secondary coil 4
is connected to a first operational amplifier 10 via a rectifier (not shown) and to a voltage terminal of a power meter 11 via a second amplifier 8. The output secondary voltage setter 9 is connected to the first operational amplifier 10. The output side of the first operational amplifier 10 is connected to the AC power supply 6. The wattmeter 11 is connected to an A/D converter 12 , and the output side of the A/D converter 12 is connected to an iron loss indicator 13 and a calculator 15 . It is obvious that if the data is not converted into digital data, the wattmeter 11 may be connected directly to the arithmetic unit 15 instead of the A/D converter 12. This computing unit 1
5 is also connected to an initial value setter 14 and a stress indicator 16. The indicator 17 is connected to the output sides of the first amplifier 7 and the second amplifier 8 via a switch 18.

いま、鉄損測定装置19の磁気センサ2の一次
コイル3を交流電源6により励磁すると、磁心5
からの磁束は第4図に示すように、磁性材料1の
中を矢印で示すように応力の方向に平行に流れ、
再び磁心5に戻る閉磁路を形成する。この時、磁
気センサ2の二次コイル4に誘起される出力二次
電圧は第1演算増幅器10において、出力二次電
圧設定器9に設定された電圧と比較減算され、そ
の減算結果は交流電源6にフイードバツクされ、
常に出力二次電圧を一定電圧、即ち出力二次電圧
設定器9の設定電圧に等しくなるように一次コイ
ル3の励磁電流を制御する。この出力二次電圧
と、一次コイル3の励磁電流はそれぞれ第1増幅
器7、第2増幅器8を介して電力計11の電圧端
子及び電流端子に導入され、これら電圧、電流の
瞬時値の乗算された値の平均値を電力計11は、
鉄損として表示するもので、磁性材料1の鉄損を
正しく測定することができる。このようにして測
定された鉄損は、A/D変換器12により数字表
示の鉄損Wiに変換されて、鉄損指示計13に指
示されると共に、演算器15に送られる。演算器
15では、初期値設定器14より送られて来た磁
性材料1に応力が作用しない時の鉄損W0と、前
記の応力が作用している時の鉄損Wiより、既述
の鉄損変化率の式より、鉄損変化率を計算し、そ
の鉄損変化率を第2図の関係より応力に換算し、
その応力を応力指示計16に指示する。初期値設
定器14に設定する鉄損W0の値は、磁性材料1
に応力が作用しない場合の鉄損を鉄損指示計13
より読取ればよい。また、指示計17は、スイツ
チ18を励磁電流側25又は出力二次電圧側26
に切換えることにより、磁気センサ2の一次コイ
ル3の励磁電流又は二次コイル4の出力二次電圧
を指示するので、必要の場合には、出力二次電圧
設定器9の設定電圧の点検等に利用することがで
きる。
Now, when the primary coil 3 of the magnetic sensor 2 of the iron loss measuring device 19 is excited by the AC power supply 6, the magnetic core 5
As shown in Fig. 4, the magnetic flux from flows in the magnetic material 1 parallel to the direction of stress as shown by the arrow,
A closed magnetic path returning to the magnetic core 5 is formed again. At this time, the output secondary voltage induced in the secondary coil 4 of the magnetic sensor 2 is compared and subtracted from the voltage set in the output secondary voltage setting device 9 in the first operational amplifier 10, and the subtraction result is Feedback was given to 6.
The excitation current of the primary coil 3 is controlled so that the output secondary voltage is always a constant voltage, that is, equal to the set voltage of the output secondary voltage setting device 9. This output secondary voltage and the exciting current of the primary coil 3 are introduced into the voltage terminal and current terminal of the wattmeter 11 via the first amplifier 7 and the second amplifier 8, respectively, and are multiplied by the instantaneous values of these voltages and currents. The wattmeter 11 calculates the average value of the values.
Since it is displayed as iron loss, the iron loss of the magnetic material 1 can be measured correctly. The thus measured iron loss is converted into a numerically displayed iron loss Wi by the A/D converter 12, and is indicated to the iron loss indicator 13 and sent to the calculator 15. The calculator 15 calculates the iron loss W 0 when no stress is applied to the magnetic material 1 sent from the initial value setting device 14 and the iron loss Wi when the stress is applied, as described above. Calculate the iron loss change rate from the iron loss change rate formula, convert the iron loss change rate to stress using the relationship shown in Figure 2,
The stress is indicated to the stress indicator 16. The value of iron loss W 0 set in the initial value setting device 14 is based on the magnetic material 1.
Iron loss indicator 13 measures the iron loss when no stress is applied to
You can read it more. The indicator 17 also switches the switch 18 to the excitation current side 25 or the output secondary voltage side 26.
By switching to , the excitation current of the primary coil 3 of the magnetic sensor 2 or the output secondary voltage of the secondary coil 4 is indicated, so if necessary, the setting voltage of the output secondary voltage setting device 9 can be checked. can be used.

従来の応力測定装置は以上のような構成を有す
るので、磁性材料1の表面に磁気センサ2が空〓
が最小になるように密着して配置されている場合
には、磁気センサ2の一次コイル3の励磁電流を
制御して、磁心5に生ずる磁束を一定にし、磁気
センサ2の二次コイル4に誘起される出力二次電
圧を出力二次電圧設定器9の設定電圧に等しくし
て一定に保てば磁性材料1の中を流れる磁束が一
定に保たれるので、既述のようにして、磁性材料
1の鉄損を測定して、磁性材料1に作用している
応力を正確に求めることができる。しかし、磁性
材料1の表面に凹凸があつて、その表面に配置し
た磁気センサ2との接触部の空〓が大きくなる
と、その空〓の大きさに比例して、磁気抵抗が大
きくなるので、大きな起磁力が必要となり、磁気
センサ2の一次コイル3には大きな励磁電流が流
れ、場合によつては、磁気センサ2の励磁回路や
一次コイルを焼損する。また、多数の磁性材料の
応力を連続して測定する場合に、電源スイツチを
切らないで、一つの磁性材料の応力測定を終り、
次の磁性材料に磁気センサを移動させるために、
磁気センサと磁性材料で形成されている閉磁路を
開放すると過大な励磁電流が磁気センサの一次コ
イルに流れ、磁気センサの一次コイルや励磁回路
を焼損するという欠点があつた。
Since the conventional stress measuring device has the above configuration, the magnetic sensor 2 is placed on the surface of the magnetic material 1.
If they are arranged in close contact with each other so that the If the induced output secondary voltage is made equal to the set voltage of the output secondary voltage setting device 9 and kept constant, the magnetic flux flowing through the magnetic material 1 is kept constant, so as described above, By measuring the core loss of the magnetic material 1, the stress acting on the magnetic material 1 can be accurately determined. However, if the surface of the magnetic material 1 is uneven and the area in contact with the magnetic sensor 2 placed on the surface becomes large, the magnetic resistance increases in proportion to the size of the area. A large magnetomotive force is required, and a large excitation current flows through the primary coil 3 of the magnetic sensor 2, which may burn out the excitation circuit and primary coil of the magnetic sensor 2. In addition, when measuring the stress of a large number of magnetic materials continuously, you can finish the stress measurement of one magnetic material without turning off the power switch.
To move the magnetic sensor to the next magnetic material,
When the closed magnetic circuit formed by the magnetic sensor and the magnetic material is opened, an excessive excitation current flows through the primary coil of the magnetic sensor, resulting in burnout of the primary coil and excitation circuit of the magnetic sensor.

本発明は以上の点に鑑み、磁性材料の応力を測
定するために磁気センサを磁性材料の表面に接触
させて配置した場合、磁気センサと磁性材料の接
触部に空〓が生じても、また磁気センサと磁性材
料で形成される閉磁路を開放しても、磁気センサ
の一次コイルや励磁回路を焼損するような過大な
励磁電流が流れないように、一次コイルの励磁電
流を制限する制限装置を設けた応力測定装置と、
これに警報器を付加して一次コイルの励磁電流が
制限電流値を超えると警報を発する応力測定装置
を提供するものである。
In view of the above points, when a magnetic sensor is placed in contact with the surface of a magnetic material in order to measure the stress of the magnetic material, even if an air gap occurs in the contact area between the magnetic sensor and the magnetic material, A limiting device that limits the excitation current of the primary coil so that an excessive excitation current that could burn out the primary coil or excitation circuit of the magnetic sensor does not flow even if the closed magnetic path formed by the magnetic sensor and magnetic material is opened. a stress measuring device equipped with a
The present invention provides a stress measuring device which is equipped with an alarm and issues an alarm when the excitation current of the primary coil exceeds a limit current value.

以下、本発明の応力測定装置の一実施例を図面
について説明する。
An embodiment of the stress measuring device of the present invention will be described below with reference to the drawings.

第6図は、第5図の従来の鉄損を利用した磁性
材料の応力測定装置のブロツク線図において、そ
の鉄損測定装置19の代りに、鉄損測定装置24
を設けたもので、その他の構成は第5図と同じで
ある。鉄損測定装置24は、第5図の鉄損測定装
置19に制限電流設定器21と第2演算増幅器2
0より成る励磁電流制限器23を付加したもので
ある。すなわち、第1演算増幅器10の出力側を
制限電流設定器21を介して第2演算増幅器20
に接続し、この第2演算増幅器20には一次コイ
ル3を接続する。第2演算増幅器20の出力側は
交流電源6に接続する。これ以外は、第5図の回
路と同様の接続となつている。いま、出力二次電
圧設定器9に設定電圧を、制限電流設定器21に
磁気センサ2の励磁回路に許容できる最大電流を
設定し、第3図に示すように応力を測定しようと
する磁性材料1の表面に磁気センサ2を配置し、
交流電源6により磁気センサ2の一次コイル3を
励磁すると、一次コイル3の励磁電流は、励磁電
流制限器23の第2演算増幅器20に導入され、
制限電流設定器21の設定電流と比較減算され、
その演算結果は交流電源6にフイードバツクさ
れ、磁気センサ2の一次コイル3の励磁電流が制
限電流設定器21の設定電流を超えないように制
御される。また、磁気センサ2の二次コイル4に
誘起される出力二次電圧は、第1演算増幅器10
に導入され、出力二次電圧設定器9の設定電圧と
比較減算され、その演算結果は、励磁電流制限器
23を介して交流電源6にフイードバツクされ、
磁気センサ2の二次コイル4の出力二次電圧を設
定電圧に等しくして一定に保持する。この磁気セ
ンサ2の励磁電流と出力二次電圧は、それぞれ第
1増幅器7、第2増幅器8を介して電力計11に
導入され、磁性材料1の鉄損を表示する。以後こ
の鉄損より磁性材料1に作用する応力を求める過
程は第5図の従来例で述べたものと同じである。
FIG. 6 is a block diagram of the conventional stress measuring device for magnetic materials using iron loss shown in FIG.
The other configuration is the same as that shown in FIG. 5. The iron loss measuring device 24 includes a limiting current setting device 21 and a second operational amplifier 2 in addition to the iron loss measuring device 19 shown in FIG.
An excitation current limiter 23 consisting of 0 is added. That is, the output side of the first operational amplifier 10 is connected to the second operational amplifier 20 via the limiting current setting device 21.
The second operational amplifier 20 is connected to the primary coil 3. The output side of the second operational amplifier 20 is connected to the AC power supply 6. Other than this, the connections are the same as in the circuit shown in FIG. Now, set the set voltage in the output secondary voltage setting device 9 and the maximum allowable current for the excitation circuit of the magnetic sensor 2 in the limiting current setting device 21, and as shown in FIG. A magnetic sensor 2 is placed on the surface of 1,
When the primary coil 3 of the magnetic sensor 2 is excited by the AC power supply 6, the exciting current of the primary coil 3 is introduced into the second operational amplifier 20 of the exciting current limiter 23,
It is compared and subtracted from the set current of the limit current setting device 21,
The calculation result is fed back to the AC power supply 6, and the excitation current of the primary coil 3 of the magnetic sensor 2 is controlled so as not to exceed the current set by the limit current setting device 21. Further, the output secondary voltage induced in the secondary coil 4 of the magnetic sensor 2 is transmitted through the first operational amplifier 10.
is introduced into the AC power source 6 and compared with and subtracted from the set voltage of the output secondary voltage setting device 9, and the calculation result is fed back to the AC power source 6 via the excitation current limiter 23.
The output secondary voltage of the secondary coil 4 of the magnetic sensor 2 is made equal to the set voltage and held constant. The excitation current and output secondary voltage of the magnetic sensor 2 are introduced into a wattmeter 11 via a first amplifier 7 and a second amplifier 8, respectively, to display the iron loss of the magnetic material 1. Thereafter, the process of determining the stress acting on the magnetic material 1 from this iron loss is the same as that described in the conventional example shown in FIG.

第7図は、第6図の応力測定装置のブロツク線
図において、その鉄損測定装置24の代りに、鉄
損測定装置27を設けたもので、第1演算増幅器
10と励磁電流制限器23の制限電流設定器21
との間に警報器22を接続した他は第6図と同じ
である。
FIG. 7 is a block diagram of the stress measuring device shown in FIG. 6, except that an iron loss measuring device 27 is provided in place of the iron loss measuring device 24, and the first operational amplifier 10 and the excitation current limiter 23 are provided. limit current setting device 21
The structure is the same as in FIG. 6 except that an alarm device 22 is connected between the two.

従つて、磁性材料の応力測定時、磁気センサ2
の一次コイル3の励磁電流が制限電流設定器21
の設定電流を超えると、第2演算増幅器20より
一次コイル3の励磁電流を減少するよう信号が交
流電源6へフイードバツクされる。磁気センサ2
の一次コイル3の励磁電流が減少すると、二次コ
イル4の出力二次電圧は低下し、この低下した電
圧は、第1演算増幅器10で、出力二次電圧設定
器9の設定電圧と比較減算され、その差だけ出力
二次電圧を高くするよう第1演算増幅器10より
出力される。この第1演算増幅器10よりの出力
電圧が一定値になると、警報器22が作動し、ブ
ザー又はランプで警報を発し、測定者に磁気セン
サ2の励磁電流が制限値を超えたことを知らせて
測定を中止させる。このようにして、常に磁気セ
ンサ2の一次コイルの励磁電流は設定電流になる
ように制御されるので、磁気センサ2の励磁回路
及び一次コイルを焼損することはない。
Therefore, when measuring stress in a magnetic material, the magnetic sensor 2
The excitation current of the primary coil 3 is limited by the current setting device 21
When the set current is exceeded, the second operational amplifier 20 feeds back a signal to the AC power supply 6 to reduce the excitation current of the primary coil 3. Magnetic sensor 2
When the excitation current of the primary coil 3 decreases, the output secondary voltage of the secondary coil 4 decreases, and this decreased voltage is compared and subtracted from the set voltage of the output secondary voltage setting device 9 in the first operational amplifier 10. is outputted from the first operational amplifier 10 so as to increase the output secondary voltage by the difference. When the output voltage from the first operational amplifier 10 reaches a certain value, the alarm 22 is activated and issues an alarm with a buzzer or lamp to notify the measuring person that the excitation current of the magnetic sensor 2 has exceeded the limit value. Stop the measurement. In this way, the excitation current of the primary coil of the magnetic sensor 2 is always controlled to be the set current, so the excitation circuit and the primary coil of the magnetic sensor 2 will not be burnt out.

また、第6図及び第7図において、出力二次電
圧設定器9及び第1演算増幅器10の代りに、フ
の字形過電流保護特性を有する電流制限装置を用
いれば短絡電流を小さくできるので、熱的に有利
にすることができる。
Furthermore, in FIGS. 6 and 7, if a current limiting device having a fold-back overcurrent protection characteristic is used instead of the output secondary voltage setting device 9 and the first operational amplifier 10, the short circuit current can be reduced. It can be made thermally advantageous.

以上のように第6図に示す本発明の応力測定装
置を使用すれば、磁気センサの一次コイルの励磁
電流は、制限電流設定器に設定された制限電流値
を超えないように制御され、磁気センサの励磁電
流は常に設定制限電流値以下になるように制御さ
れるので、磁気センサの励磁回路や一次コイルを
焼損することはない。また、第7図に示す本発明
の他の実施例の応力測定装置を使用すれば、第6
図の実施例の効果に他に制限電流値を超えると警
報器により警報を発するので、測定者に測定を中
止させることができる効果もある。
As described above, by using the stress measuring device of the present invention shown in FIG. 6, the excitation current of the primary coil of the magnetic sensor is controlled so as not to exceed the limiting current value set in the limiting current setting device, Since the excitation current of the sensor is always controlled to be below the set limit current value, the excitation circuit and primary coil of the magnetic sensor will not be burnt out. Furthermore, if the stress measuring device according to another embodiment of the present invention shown in FIG. 7 is used, the sixth
Another advantage of the embodiment shown in the figure is that when the current limit value is exceeded, an alarm is issued by the alarm device, allowing the operator to stop the measurement.

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

第1図は磁性材料に作用する応力と鉄損の関係
を示す図、第2図は磁性材料に作用する応力と鉄
損変化率の関係を示す図、第3図は磁性材料に磁
気センサを配置した平面図、第4図は第3図のA
−A断面拡大図、第5図は従来の鉄損測定装置を
使用した磁性材料の応力装置のブロツク線図、第
6図は本発明の一実施例である磁性材料の応力測
定装置のブロツク線図、第7図は本発明の他の実
施例の磁性材料の応力測定装置のブロツク線図で
ある。 1……磁性材料、2……磁気センサ、3……一
次コイル、4……二次コイル、5……磁心、6…
…交流電源、7……第1増幅器、8……第2増幅
器、9……出力二次電圧設定器、10……第1演
算増幅器、11……電力計、20……第2演算増
幅器、21……制限電流設定器、22……警報
器、23……励磁電流制限器、24,27……鉄
損測定装置。
Figure 1 is a diagram showing the relationship between stress acting on magnetic material and iron loss, Figure 2 is a diagram showing the relationship between stress acting on magnetic material and iron loss change rate, and Figure 3 is a diagram showing the relationship between stress acting on magnetic material and iron loss change rate. The arranged plan view, Figure 4 is A in Figure 3.
- An enlarged cross-sectional view of A; FIG. 5 is a block diagram of a stress measuring device for magnetic materials using a conventional iron loss measuring device; FIG. 6 is a block diagram of a stress measuring device for magnetic materials that is an embodiment of the present invention. 7 are block diagrams of a stress measuring device for magnetic materials according to another embodiment of the present invention. DESCRIPTION OF SYMBOLS 1...Magnetic material, 2...Magnetic sensor, 3...Primary coil, 4...Secondary coil, 5...Magnetic core, 6...
...AC power supply, 7...First amplifier, 8...Second amplifier, 9...Output secondary voltage setter, 10...First operational amplifier, 11...Power meter, 20...Second operational amplifier, 21... Limit current setting device, 22... Alarm device, 23... Excitation current limiter, 24, 27... Iron loss measuring device.

Claims (1)

【特許請求の範囲】 1 断面略コの字形の磁心に一次コイルと二次コ
イルを巻いて構成した磁気センサと、この磁気セ
ンサの一次コイルを励磁する交流電源と、前記磁
気センサの一次コイル、二次コイルに接続され鉄
損値を表示する電力計と、所定の出力二次電圧を
設定できる出力二次電圧設定器と、この出力二次
電圧設定器の設定電圧と磁気センサの二次コイル
の出力二次電圧とを比較減算する第1演算増幅器
と、この第1演算増幅器に接続され前記磁気セン
サの一次コイルの最大許容電流を設定する制限電
流設定器と、この制限電流設定器の設定値と前記
磁気センサの一次コイルの励磁電流とを比較減算
し、減算結果を前記交流電源にフイードバツクす
る第2演算増幅器とからなる鉄損測定装置と;磁
性材料に応力が作用していない時の鉄損値を設定
する初期値設定器と;この初期値設定器よりの鉄
損値と磁性材料に応力が作用しているときの鉄損
値を前記電力計より入力して、鉄損変化率を計算
し、この鉄損変化率より応力を演算する演算器
と;この演算器よりの出力を表示する応力指示計
よりなることを特徴とする応力測定装置。 2 断面略コの字形の磁心に一次コイルと二次コ
イルを巻いて構成した磁気センサと、この磁気セ
ンサの一次コイルを励磁する交流電源と、前記磁
気センサの一次コイル、二次コイルに接続され鉄
損値を表示する電力計と、所定の出力二次電圧を
設定できる出力二次電圧設定器と、この出力二次
電圧設定器の設定電圧と磁気センサの二次コイル
の出力二次電圧とを比較減算する第1演算増幅器
と、この第1演算増幅器に接続され前記磁気セン
サの一次コイルの最大許容電流を設定する制限電
流設定器と、この制限電流設定器の設定値と前記
磁気センサの一次コイルの励磁電流とを比較減算
し、減算結果を前記交流電源にフイードバツクす
る第2演算増幅器とからなる鉄損測定装置と;磁
性材料に応力が作用していない時の鉄損値を設定
する初期値設定器と;この初期値設定器よりの鉄
損値と磁性材料に応力が作用しているときの鉄損
値を前記電力計より入力して、鉄損変化率を計算
し、この鉄損変化率より応力を演算する演算器
と;この演算器よりの出力を表示する応力指示計
と;前記第1演算増幅器と交流電源を接続するフ
イードバツク回路に設けられた警報器よりなるこ
とを特徴とする応力測定装置。
[Scope of Claims] 1. A magnetic sensor configured by winding a primary coil and a secondary coil around a magnetic core having a substantially U-shaped cross section, an AC power source that excites the primary coil of this magnetic sensor, and a primary coil of the magnetic sensor; A wattmeter that is connected to the secondary coil and displays the iron loss value, an output secondary voltage setting device that can set a predetermined output secondary voltage, and the setting voltage of this output secondary voltage setting device and the secondary coil of the magnetic sensor. a first operational amplifier that compares and subtracts the output secondary voltage of the magnetic sensor; a limit current setter that is connected to the first operational amplifier and sets the maximum allowable current of the primary coil of the magnetic sensor; and a setting of the limit current setter. a second operational amplifier that compares and subtracts the value from the excitation current of the primary coil of the magnetic sensor and feeds back the subtraction result to the AC power supply; when no stress is acting on the magnetic material; An initial value setting device for setting the iron loss value; enter the iron loss value from this initial value setting device and the iron loss value when stress is acting on the magnetic material from the wattmeter, and calculate the iron loss change rate. 1. A stress measuring device comprising: a computing unit that calculates stress based on the rate of change in iron loss; and a stress indicator that displays the output from the computing unit. 2. A magnetic sensor configured by winding a primary coil and a secondary coil around a magnetic core having a substantially U-shaped cross section, an AC power source that excites the primary coil of this magnetic sensor, and a magnetic sensor that is connected to the primary coil and secondary coil of the magnetic sensor. A wattmeter that displays the iron loss value, an output secondary voltage setting device that can set a predetermined output secondary voltage, and the setting voltage of this output secondary voltage setting device and the output secondary voltage of the secondary coil of the magnetic sensor. a first operational amplifier that compares and subtracts a value, a limit current setter that is connected to the first operational amplifier and sets the maximum allowable current of the primary coil of the magnetic sensor, and a limit current setter that sets the maximum allowable current of the primary coil of the magnetic sensor; an iron loss measuring device comprising a second operational amplifier that compares and subtracts the excitation current of the primary coil and feeds back the subtraction result to the AC power supply; and sets an iron loss value when no stress is acting on the magnetic material. Initial value setting device: Input the iron loss value from this initial value setting device and the iron loss value when stress is acting on the magnetic material from the wattmeter, calculate the iron loss change rate, and calculate the iron loss change rate. It is characterized by comprising: a computing unit that calculates stress from the rate of change in loss; a stress indicator that displays the output from the computing unit; and an alarm provided in a feedback circuit that connects the first operational amplifier and the AC power source. Stress measuring device.
JP9503679A 1979-07-27 1979-07-27 Method and device for measuring iron loss Granted JPS5619466A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9503679A JPS5619466A (en) 1979-07-27 1979-07-27 Method and device for measuring iron loss

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9503679A JPS5619466A (en) 1979-07-27 1979-07-27 Method and device for measuring iron loss

Publications (2)

Publication Number Publication Date
JPS5619466A JPS5619466A (en) 1981-02-24
JPH0226172B2 true JPH0226172B2 (en) 1990-06-07

Family

ID=14126847

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9503679A Granted JPS5619466A (en) 1979-07-27 1979-07-27 Method and device for measuring iron loss

Country Status (1)

Country Link
JP (1) JPS5619466A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60185157A (en) * 1983-11-04 1985-09-20 インスチツート、プリクラドノイ、フイジキ、アカデミー、ナウク、ベロルススコイ、エスエスエル Device for measuring physical and mechanical characteristic of ferromagnetic substance piece

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5495034A (en) * 1978-01-10 1979-07-27 Gen Electric Microwave oven

Also Published As

Publication number Publication date
JPS5619466A (en) 1981-02-24

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