JPH07113626B2 - Steel plate flaw detection device - Google Patents
Steel plate flaw detection deviceInfo
- Publication number
- JPH07113626B2 JPH07113626B2 JP4241790A JP4241790A JPH07113626B2 JP H07113626 B2 JPH07113626 B2 JP H07113626B2 JP 4241790 A JP4241790 A JP 4241790A JP 4241790 A JP4241790 A JP 4241790A JP H07113626 B2 JPH07113626 B2 JP H07113626B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- voltage
- coil
- steel plate
- flaw detection
- 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
Links
Landscapes
- Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
Description
【発明の詳細な説明】 [産業上の利用分野] この発明は鋼板の疵検出装置、特に微小な疵の検出精度
の向上に関するものである。Description: TECHNICAL FIELD The present invention relates to a flaw detection device for a steel sheet, and more particularly to improvement in detection accuracy of minute flaws.
[従来の技術] 例えば鋼板や鋼管等に発生する疵を検出するために、超
音波探傷法,渦電流探傷法,漏洩磁束探傷法等が従来か
ら用いられている。[Prior Art] In order to detect a flaw generated in, for example, a steel plate or a steel pipe, an ultrasonic flaw detection method, an eddy current flaw detection method, a leakage magnetic flux flaw detection method or the like has been conventionally used.
これらの探傷法のうち漏洩磁束探傷法は他の方法と比べ
て悪環境でも測定できるため、従来からあらゆる場所で
利用されている。Among these flaw detection methods, the magnetic flux leakage flaw detection method is conventionally used in every place because it can measure even in a bad environment compared to other methods.
第9図は漏洩磁束探傷法を使用した従来の鋼板の疵検出
装置の構造を示す。図に示すように、疵検出装置は、鋼
板1の移動に伴って回転する非磁性の中空ロール2と、
中空ロール2内に設けられ鋼板1を磁化するため磁化コ
ア4に巻き回されたコイル3と、磁化コア4間に設けら
れ漏洩磁束を検出する例えばホール素子からなるセンサ
ー5とから構成されている。FIG. 9 shows the structure of a conventional flaw detection apparatus for steel plates using the magnetic flux leakage flaw detection method. As shown in the figure, the flaw detection device includes a non-magnetic hollow roll 2 that rotates as the steel plate 1 moves,
The hollow roll 2 is provided with a coil 3 wound around a magnetized core 4 for magnetizing the steel plate 1, and a sensor 5 provided between the magnetized cores 4 and configured to detect a leakage magnetic flux, such as a Hall element. .
鋼板1の疵を検出するときは、コイル3に直流電流を流
して磁界を生じさせる。そして、移動する鋼板1をロー
ル2を介して磁化コア4によって磁化する。この磁化さ
れた鋼板1に疵が存在すると、疵の部分に漏洩磁束が生
じる。この漏洩磁束をセンサー5によって検出し、セン
サー5からの出力信号の大小により鋼板1に存在する疵
を検出する。When detecting a flaw in the steel sheet 1, a direct current is passed through the coil 3 to generate a magnetic field. Then, the moving steel plate 1 is magnetized by the magnetizing core 4 via the roll 2. When the magnetized steel plate 1 has a flaw, a leakage magnetic flux is generated in the flaw portion. This leakage magnetic flux is detected by the sensor 5, and the flaw existing on the steel plate 1 is detected by the magnitude of the output signal from the sensor 5.
この場合、センサー5の出力信号にはノイズ信号が含ま
れるので、このノイズの影響を除去するため、あらかじ
め一定レベルのしきい値を定め、このしきい値を越えた
センサー5の出力信号により疵を検出し、疵の誤検出を
防止している。In this case, since the output signal of the sensor 5 contains a noise signal, in order to remove the influence of this noise, a threshold value of a certain level is set in advance, and the output signal of the sensor 5 exceeding this threshold value causes a flaw. Is detected to prevent false detection of defects.
[発明が解決しようとする課題] しかしながら、上記ノイズは鋼種や圧延条件等の違い、
あるいは測定場所の他の磁性体の影響を受け、種々のノ
イズレベルを有する。[Problems to be Solved by the Invention] However, the above noise is caused by differences in steel types, rolling conditions, etc.
Alternatively, it has various noise levels due to the influence of other magnetic substances at the measurement location.
この種々のノイズを除去し疵の誤検出を防止するため、
従来はノイズの中で最も高いレベルのものをしきい値と
して設定していた。このため、主要な疵は検出すること
はできるが、センサー5から出力するしきい値以下の信
号で示される微小な疵は検出できず、疵の測定精度が低
下するという短所があった。In order to remove these various noises and prevent false detection of defects,
Conventionally, the highest level of noise has been set as the threshold value. For this reason, although major flaws can be detected, minute flaws indicated by a signal below the threshold value output from the sensor 5 cannot be detected, and there is a disadvantage that the flaw measurement accuracy decreases.
他方、例えば特開願平1−308982号公報に示された原理
に基づく磁気センサのようにセンサ5の感度が高ければ
高いほど、より小さな疵(欠陥)を検出できるとはい
え、種々のノイズを拾う傾向が強まるため、ノイズ除去
と疵の高精度検出の要求は高まる。On the other hand, the higher the sensitivity of the sensor 5 such as the magnetic sensor based on the principle disclosed in Japanese Patent Application Laid-Open No. 1-308982, the smaller the flaw (defect) can be detected, but various noises can be detected. The demand for noise removal and high-accuracy detection of defects increases as the tendency to pick up defects increases.
この発明はかかる短所を解決するためになされたもので
あり、特に、欠陥ではなく鋼板の圧延条件などの変化に
より鋼板の幅方向にほぼ同時に発生する漏洩磁束の変化
やノイズの影響を除去し、微小な疵も高感度に検出する
ことができる鋼板の疵検出装置を得ることを目的とする
ものである。This invention has been made to solve the above disadvantages, and in particular, it eliminates the effects of changes in leakage magnetic flux and noise that occur almost simultaneously in the width direction of the steel sheet due to changes in rolling conditions of the steel sheet rather than defects, It is an object of the present invention to obtain a flaw detection device for a steel sheet, which is capable of detecting minute flaws with high sensitivity.
[課題を解決するための手段] この発明に係る鋼板の疵検出装置は、複数の磁気センサ
と、磁気センサの出力を受けてピーク値を検出する、少
なくとも2組のピーク値検出手段と、検出したピーク値
の差を演算する演算手段と、演算した結果とあらかじめ
設定されたしきい値とを比較する比較手段とを有する。[Means for Solving the Problems] A flaw detection device for a steel sheet according to the present invention includes a plurality of magnetic sensors, and at least two sets of peak value detection means for receiving the outputs of the magnetic sensors to detect peak values. It has a calculating means for calculating the difference between the peak values and a comparing means for comparing the calculated result with a preset threshold value.
磁気センサは強磁性体コアに巻き回されたコイルと、こ
のコイルに固定インピーダンスを介して一定周波数,一
定電圧の交流電力を供給する交流電力供給手段と、コイ
ルの両端から出力する電圧の正側電圧と負側電圧をそれ
ぞれ検出する直流電圧検出手段と、直流電圧検出手段で
検出した正側電圧と負側電圧の差を演算し磁界の強さを
検出する磁気検出手段とからなる。そして複数の磁気セ
ンサの強磁性体コアに巻き回されたコイルは連続的に移
動する鋼板の幅方向に沿って配設されている。The magnetic sensor includes a coil wound around a ferromagnetic core, an AC power supply unit that supplies AC power of a constant frequency and a constant voltage to the coil through a fixed impedance, and a positive side of a voltage output from both ends of the coil. It comprises a DC voltage detecting means for detecting the voltage and the negative voltage, and a magnetic detecting means for calculating the difference between the positive voltage and the negative voltage detected by the DC voltage detecting means to detect the strength of the magnetic field. The coils wound around the ferromagnetic cores of the plurality of magnetic sensors are arranged along the width direction of the continuously moving steel plate.
この複数の磁気センサからの出力信号を少なくとも2群
に分けてピーク値検出手段に送り、ピーク値検出手段で
各磁気センサ群毎の検出信号のピーク値を検出する。The output signals from the plurality of magnetic sensors are divided into at least two groups and sent to the peak value detecting means, and the peak value detecting means detects the peak value of the detection signal for each magnetic sensor group.
演算手段は検出した複数群のピーク値の差を演算し比較
手段に送る。The calculating means calculates the difference between the detected peak values of the plurality of groups and sends it to the comparing means.
また、各磁気センサのコイルに、直流バイアスを加算し
たパルス電流を供給することにより漏洩磁束の測定スパ
ンを拡大することができる。Further, by supplying a pulse current added with a DC bias to the coil of each magnetic sensor, the span of measurement of the leakage magnetic flux can be expanded.
さらに、パルス電流に加算する直流バイアスを各磁気セ
ンサの出力信号に応じて可変制御することにより、磁気
センサの動作点を自動的に補償することができる。Further, the operating point of the magnetic sensor can be automatically compensated by variably controlling the DC bias added to the pulse current according to the output signal of each magnetic sensor.
[作用] この発明における磁気センサは、強磁性体コアに巻き回
されコイルに一定周波数,一定電圧の交流電力を供給
し、このコイルに流れる交流電流により生じる磁界によ
ってヒステリシス特性を示す強磁性体コアの透磁率によ
りコイルのインピーダンスを変化させ、コイルの両端出
力電圧を正負対称のほぼ矩形波形に変化させる。このコ
イルを鋼板に近接して配置し鋼板からの漏洩磁束によ
り、コイルの両端出力電圧の正側電圧と負側電圧の電圧
値を変化させる。この変化する正側電圧と負側電圧をそ
れぞれ検出し、検出した正側電圧と負側電圧の差を算出
し、鋼板の漏洩磁束を電気信号として検出する。これに
より、漏洩磁束を極めて高感度に検出できる。[Operation] The magnetic sensor according to the present invention is a ferromagnetic core that is wound around a ferromagnetic core to supply AC power of a constant frequency and a constant voltage to a coil, and that exhibits a hysteresis characteristic by a magnetic field generated by an AC current flowing through the coil. The impedance of the coil is changed according to the magnetic permeability of, and the output voltage across the coil is changed to a substantially rectangular waveform with positive and negative symmetry. The coil is arranged close to the steel plate, and the leakage magnetic flux from the steel plate changes the positive and negative voltage values of the output voltage across the coil. The changing positive side voltage and negative side voltage are respectively detected, the difference between the detected positive side voltage and negative side voltage is calculated, and the leakage magnetic flux of the steel sheet is detected as an electric signal. Thereby, the leakage magnetic flux can be detected with extremely high sensitivity.
この磁気センサを複数使用し、各磁気センサのコイルを
連続的に移動する鋼板の幅方向に沿って配設し、各磁気
センサからの出力信号を少なくとも2群に分けて、各磁
気センサ群毎の検出信号のピーク値を検出する。この磁
気センサ群毎のピーク値の差を演算することにより、圧
延条件等によって鋼板の幅方向に沿って生じるノイズを
除去する。そして、ノイズ成分を除去した検出信号によ
り、鋼板の疵を検出する。A plurality of these magnetic sensors are used, the coils of each magnetic sensor are arranged along the width direction of the steel plate that moves continuously, and the output signals from each magnetic sensor are divided into at least two groups, and each magnetic sensor group The peak value of the detection signal of is detected. By calculating the difference in peak value for each magnetic sensor group, noise generated along the width direction of the steel sheet due to rolling conditions and the like is removed. Then, the flaw of the steel plate is detected by the detection signal from which the noise component is removed.
また、磁気センサのコイルに直流バイアスを加算したパ
ルス電流を供給することにより、漏洩磁束の測定スパン
を拡大することができる。Further, by supplying a pulse current to which a DC bias is added to the coil of the magnetic sensor, the measurement span of the leakage magnetic flux can be expanded.
また、パルス電流に加算する直流バイアスを磁気検出手
段からの磁気検出信号に応じて可変制御することによ
り、磁気センサの動作点を自動的に補償して、測定条件
が変化しても常に良好な測定スパンを確保することがで
きる。Further, the DC bias to be added to the pulse current is variably controlled according to the magnetic detection signal from the magnetic detection means, so that the operating point of the magnetic sensor is automatically compensated, and even if the measurement condition changes, it is always good. The measurement span can be secured.
[実施例] 第1図はこの発明の一実施例を示すブロック図である。
図に示すように、疵検出装置は複数の磁気センサ5と、
複数の磁気センサ5からの磁気検出信号を入力し、磁気
検出信号のピーク値を検出する2個のピーク値検出手段
6a,6bと、ピーク値検出手段6a,6bで検出したピーク値の
差を求める演算手段7と、演算手段7で求めたピーク値
との差と、しきい値設定手段9に設定されたしきい値と
を比較し、鋼板の疵を検出する比較手段8及び表示手段
10とを有する。[Embodiment] FIG. 1 is a block diagram showing an embodiment of the present invention.
As shown in the figure, the flaw detection device includes a plurality of magnetic sensors 5,
Two peak value detecting means for inputting magnetic detection signals from a plurality of magnetic sensors 5 and detecting peak values of the magnetic detection signals
6a, 6b, the calculating means 7 for obtaining the difference between the peak values detected by the peak value detecting means 6a, 6b, and the difference between the peak value obtained by the calculating means 7 and the threshold setting means 9. Comparing means 8 and display means for comparing a threshold value and detecting flaws in the steel sheet
Have 10 and.
磁気センサ5は棒状の強磁性体コア11と、強磁性体コア
11に巻き回されたコイル12,コイル12に固定インピーダ
ンス14を介して一定周波数,一定電圧の交流電力を供給
する交流電力供給手段13、コイル12の両端に接続された
直流電圧検出手段15及び磁気検出手段16とを有する。直
流電圧検出手段15は正極性検波器と負極性検波器とを有
し、コイル12の出力電圧の正側電圧と負側電圧をそれぞ
れ検出する。磁気検出手段16は直流電圧検出手段15の出
力を受けてコイル12の正側電圧と負側電圧の差を求め、
磁界の強さを検出する。The magnetic sensor 5 includes a rod-shaped ferromagnetic core 11 and a ferromagnetic core.
A coil 12 wound around 11, an AC power supply means 13 for supplying a constant frequency and a constant voltage AC power to the coil 12 via a fixed impedance 14, a DC voltage detection means 15 connected to both ends of the coil 12, and a magnetic field. And a detection means 16. The DC voltage detecting means 15 has a positive polarity detector and a negative polarity detector, and detects the positive side voltage and the negative side voltage of the output voltage of the coil 12, respectively. The magnetic detection means 16 receives the output of the DC voltage detection means 15 and obtains the difference between the positive side voltage and the negative side voltage of the coil 12,
Detects magnetic field strength.
上記のように構成された疵検出装置により鋼板1の疵を
検出する場合は、例えば、第2図(a)に示すように、
磁気センサ5の強磁性体コア11に巻き回されたコイル12
を、鋼板1の移動に伴って回転する、例えばオーステナ
イト系のステンレスやセラミックスからなる非磁性の中
空ロール2内に設けられ、鋼板1を磁化するコイル3が
巻き回された磁化コア4の間に設置する。なお、磁気セ
ンサ5の強磁性体コア11に巻き回されたコイル12は、第
2図(b)に示すように、鋼板1を磁化するコイル3が
巻き回された磁化コア4を有する中空ロール2と鋼板1
を挟んで設けられた、中空ロール2と同径の中空ロール
2a内に設置してもよい。When the flaw detection device configured as described above is used to detect a flaw in the steel sheet 1, for example, as shown in FIG.
The coil 12 wound around the ferromagnetic core 11 of the magnetic sensor 5.
Is provided in a non-magnetic hollow roll 2 made of, for example, austenitic stainless steel or ceramics, which rotates with the movement of the steel sheet 1, and a coil 3 for magnetizing the steel sheet 1 is wound between the magnetized cores 4. Install. The coil 12 wound around the ferromagnetic core 11 of the magnetic sensor 5 is a hollow roll having a magnetized core 4 around which a coil 3 for magnetizing the steel plate 1 is wound, as shown in FIG. 2 (b). 2 and steel plate 1
Hollow rolls having the same diameter as the hollow roll 2 sandwiched between
It may be installed in 2a.
上記のように構成された疵検出装置の動作を説明するに
あたり、まず上記磁気センサ5の原理を第3図の電圧波
形図と第4図の強磁性体コアの磁化特性図を参照して説
明する。In explaining the operation of the flaw detection device configured as described above, first, the principle of the magnetic sensor 5 will be described with reference to the voltage waveform diagram of FIG. 3 and the magnetization characteristic diagram of the ferromagnetic core of FIG. To do.
第3図(a)の電圧波形図に示すように一定周波数,一
定電圧の交流電圧Eをコイル12に供給すると、コイル12
の両端に発生する電圧E0は固定インピーダンス14の抵抗
値Rとコイル12のインピーダンスZSにより定まる。When an alternating voltage E having a constant frequency and a constant voltage is supplied to the coil 12 as shown in the voltage waveform diagram of FIG.
The voltage E 0 generated at both ends of the coil is determined by the resistance value R of the fixed impedance 14 and the impedance Z S of the coil 12.
コイル12のインピーダンスは強磁性体コア11の透磁率に
比例して変化する。すなわち外部磁界を加えない状態で
コイル12に交流電流を流すると、コイル12の磁束により
強磁性体コア11が磁化される。強磁性体コア11の透磁率
は一定でなく、磁界の強さによって変化し、第4図に示
すように磁化曲線がヒステリシス特性を示す。なお、第
4図において、Bは磁束密度、nはコイル2の巻数、i
はコイル電流である。The impedance of the coil 12 changes in proportion to the magnetic permeability of the ferromagnetic core 11. That is, when an alternating current is passed through the coil 12 without applying an external magnetic field, the magnetic flux of the coil 12 magnetizes the ferromagnetic core 11. The magnetic permeability of the ferromagnetic core 11 is not constant but changes depending on the strength of the magnetic field, and the magnetization curve exhibits a hysteresis characteristic as shown in FIG. In FIG. 4, B is the magnetic flux density, n is the number of turns of the coil 2, and i is
Is the coil current.
このためコイル12の両端に発生する出力電圧E0は第3図
(b)に示すように、正負対称のほぼ矩形波状の波形に
なる。そして外部磁界が加えられない状態では正側電圧
V1と負側電圧V2は等しくなる。Therefore, the output voltage E 0 generated at both ends of the coil 12 has a substantially rectangular waveform with positive and negative symmetry, as shown in FIG. 3 (b). And in the state where no external magnetic field is applied, the positive voltage
V 1 and the negative side voltage V 2 become equal.
この状態でコイル12に外部磁界を加えると強磁性体コア
11を交差する磁束はコイル12で発生する磁束と外部磁界
の磁束の合成磁束となる。このためコイル12の両端に発
生する波形は第3図(c)に示すように、正側電圧V1と
負側電圧V2に差が生じる。このコイル12の両端に発生す
る出力電圧の正側電圧V1と負側電圧V2を比較しその差を
求めることによって間接的に外部磁界を計測できる。When an external magnetic field is applied to the coil 12 in this state, the ferromagnetic core
The magnetic flux crossing 11 is a composite magnetic flux of the magnetic flux generated in the coil 12 and the magnetic flux of the external magnetic field. As a result, the waveform generated at both ends of the coil 12 has a difference between the positive voltage V 1 and the negative voltage V 2 as shown in FIG. 3 (c). The external magnetic field can be indirectly measured by comparing the positive side voltage V 1 and the negative side voltage V 2 of the output voltage generated at both ends of the coil 12 and obtaining the difference.
そして、この磁気センサ5で外部磁界の磁束密度を測定
すると、第5図に示すように、0〜10ガウスという微小
な磁束密度に対して0〜500mVという高い出力電圧を得
ることができ、従来のホール素子の出力電圧数mVと比べ
て非常に高い検出感度で磁束密度を測定することができ
る。Then, when the magnetic flux density of the external magnetic field is measured by the magnetic sensor 5, as shown in FIG. 5, a high output voltage of 0 to 500 mV can be obtained for a minute magnetic flux density of 0 to 10 Gauss. The magnetic flux density can be measured with a much higher detection sensitivity than the output voltage of the Hall element, which is several millivolts.
次に上記原理に基ずく磁気センサ5を使用した疵検出装
置の動作を説明する。Next, the operation of the flaw detection device using the magnetic sensor 5 based on the above principle will be described.
例えば、第2図(a)に示すように、連続して移動する
鋼板1の表面に近接して、幅方向に沿って設けられた中
空ロール2の磁化コア4の間に、強磁性体コア11に巻き
回されたコイル12を複数個設置する。この状態でコイル
12に交流電力供給手段13から固定インピーダンス14を介
して、第3図(a)の波形図に示すような一定周波数,
一定電圧の交流電力を供給する。コイル12は供給された
交流電流により磁界を生じ、その磁束が強磁性体コア11
を第4図に示すように、磁束密度Bが飽和状態になるま
で磁化する。この強磁性体コア11の磁界の強さはコイル
12に流れる交流電流によりヒステリシス特性を繰返し、
コイル12のインピーダンスを交流電流の周波数と同じ周
波数で変化させる。一方、コイル12には中空ロール2内
に設けられた磁化コア4で発生し鋼板1を通った磁束の
漏洩磁束が加えられる。この鋼板1からの漏洩磁束は鋼
板1の疵と疵の大きさにより変化する。このため、第3
図(c)に示すようにコイル2の両側出力電圧の正側電
圧V1と負側電圧V2に差が生じる。For example, as shown in FIG. 2 (a), a ferromagnetic core is provided between the magnetized cores 4 of the hollow roll 2 provided in the width direction in the vicinity of the surface of the steel plate 1 that moves continuously. A plurality of coils 12 wound around 11 are installed. Coil in this state
12 through the fixed impedance 14 from the AC power supply means 13 to a constant frequency as shown in the waveform diagram of FIG.
Supply constant voltage AC power. The coil 12 generates a magnetic field by the supplied alternating current, and its magnetic flux causes the magnetic core 11 to move.
Is magnetized until the magnetic flux density B becomes saturated as shown in FIG. The magnetic field strength of this ferromagnetic core 11 is the coil
The hysteresis characteristic is repeated by the alternating current flowing in 12,
The impedance of the coil 12 is changed at the same frequency as the frequency of the alternating current. On the other hand, a leakage magnetic flux of the magnetic flux generated in the magnetized core 4 provided in the hollow roll 2 and passing through the steel plate 1 is applied to the coil 12. The leakage magnetic flux from the steel plate 1 changes depending on the flaw and the size of the flaw of the steel sheet 1. Therefore, the third
As shown in FIG. 7C, a difference occurs between the positive side voltage V 1 and the negative side voltage V 2 of the output voltage on both sides of the coil 2.
そこで、直流電圧検出手段15でコイル12の正側電圧V1と
負側電圧V2をそれぞれ検出し磁気検出手段16に送る。磁
気検出手段16は送られた正側電圧V1と負側電圧V2の電圧
差を演算し、鋼板1の漏洩磁束に比例した磁気検出信号
を得る。Therefore, the DC voltage detecting means 15 detects the positive side voltage V 1 and the negative side voltage V 2 of the coil 12 and sends them to the magnetic detecting means 16. The magnetic detection means 16 calculates the voltage difference between the positive side voltage V 1 and the negative side voltage V 2 sent to obtain a magnetic detection signal proportional to the leakage magnetic flux of the steel plate 1.
このようにして検出した複数の磁気センサ5の磁気検出
信号を、例えば鋼板1の幅方向中央部を中心にして左右
の2群に分けて、各群毎にピーク値検出手段6a,6bに送
る。ピーク値検出手段6a,6bは左右2群に分けられた磁
気検出信号の、一定時間あるいは鋼板1の一定長さ毎の
ピーク値をそれぞれ検出して、演算手段7に送る。The magnetic detection signals of the plurality of magnetic sensors 5 thus detected are divided into, for example, two groups on the left and right centering on the widthwise central portion of the steel plate 1 and sent to the peak value detecting means 6a, 6b for each group. . The peak value detecting means 6a, 6b respectively detect the peak values of the magnetic detection signals divided into the left and right two groups for a certain period of time or for each certain length of the steel sheet 1, and send them to the calculating means 7.
演算手段7は送られた左右2群のピーク値の差を演算す
る。このように鋼板1の幅方向に分割された左右2群の
ピーク値の差を求めることにより、鋼種や圧延条件等に
よって鋼板の幅方向に沿ってほぼ同時に生じている漏洩
磁束の変化やノイズ成分の影響を除去することができ
る。The calculation means 7 calculates the difference between the peak values of the two left and right groups sent. In this way, by obtaining the difference between the peak values of the left and right two groups divided in the width direction of the steel sheet 1, changes in the leakage magnetic flux and noise components that occur almost simultaneously along the width direction of the steel sheet depending on the steel type, rolling conditions, etc. The effect of can be removed.
このノイズ成分等を除去した信号を演算手段7から比較
手段8に送り、しきい値設定手段9にあらかじめ設定さ
れたしきい値とを比較し、しきい値を越えた信号を鋼板
1の疵検出信号として表示手段10に表示する。The signal from which the noise component has been removed is sent from the calculating means 7 to the comparing means 8 and compared with a threshold value set in advance by the threshold value setting means 9, and the signal exceeding the threshold value is flawed on the steel sheet 1. It is displayed on the display means 10 as a detection signal.
このように、複数の磁気センサ5で高検出感度で検出し
た鋼板1からの漏洩磁束の検出信号を、鋼板1の幅方向
に左右2群に分割し、分割された漏洩磁束の検出信号の
ピーク値の差を求めることにより、鋼板の幅方向に沿っ
て生じているノイズ成分を除去することができるから、
主要な疵とともに微小な疵も検出することができ、鋼板
の疵検出精度を大幅に向上させることができる。In this way, the detection signal of the leakage magnetic flux from the steel sheet 1 detected by the plurality of magnetic sensors 5 with high detection sensitivity is divided into two groups on the left and right in the width direction of the steel sheet 1, and the peaks of the divided detection signals of the leakage magnetic flux are divided. By calculating the difference between the values, it is possible to remove the noise component generated along the width direction of the steel plate,
It is possible to detect small flaws as well as major flaws, and it is possible to significantly improve the flaw detection accuracy of the steel sheet.
さらに、漏洩磁束の測定の際に温度が変動してコイル12
の巻線抵抗と強磁性体コア11の透磁率が変化しても、こ
の変化によるコイル12のインピーダンスは磁化電流の正
負極性とも等しく変化するので相互に補償し合うから、
温度変化によるコイル11の正側電圧と負側電圧の差にド
リフトは発生せず、温度変動の影響なしに精度良く漏洩
磁束を測定することができる。Furthermore, when measuring the magnetic flux leakage, the temperature fluctuates and the coil 12
Even if the winding resistance and the magnetic permeability of the ferromagnetic core 11 change, the impedance of the coil 12 due to this change changes equally with the positive and negative polarities of the magnetizing current, so they compensate each other.
Drift does not occur in the difference between the positive side voltage and the negative side voltage of the coil 11 due to the temperature change, and the leakage magnetic flux can be accurately measured without the influence of the temperature change.
また強磁性体コア11をコイル12に流す電流で充分飽和す
るまで磁化することにより、コイル12の両端に発生する
出力電圧は一定値にクリップされ、コイル両端の出力電
圧は外部磁界の強弱のみによって正極と負極との振幅及
び位相が変化するようにしたから、交流電力供給手段13
の出力電圧や固定インピーダンス14の抵抗値が多少変化
しても検出感度は変化せず、高感度で漏洩磁束を測定す
ることができる。In addition, by magnetizing the ferromagnetic core 11 until it is sufficiently saturated with the current flowing through the coil 12, the output voltage generated at both ends of the coil 12 is clipped to a constant value, and the output voltage at both ends of the coil depends only on the strength of the external magnetic field. Since the amplitude and phase of the positive electrode and the negative electrode are changed, the AC power supply means 13
Even if the output voltage and the resistance value of the fixed impedance 14 change a little, the detection sensitivity does not change, and the leakage magnetic flux can be measured with high sensitivity.
なお、上記実施例においては、複数の磁気センサ5の漏
洩磁束の検出信号を、鋼板1の幅方向に左右2群に分割
してピーク値を求める場合について説明したが、複数の
磁気センサ5と漏洩磁束の検出信号を、一つ置きに分割
したり、2群以上に分割しても上記実施例と同様な作用
を奏することができる。In the above embodiment, the case where the detection signals of the leakage magnetic flux of the plurality of magnetic sensors 5 are divided into the left and right two groups in the width direction of the steel plate 1 to obtain the peak value has been described. Even if the detection signal of the leakage magnetic flux is divided into alternate groups or divided into two or more groups, the same operation as in the above embodiment can be achieved.
なお、上記実施例においては、複数の磁気センサ5の強
磁性体コア11に巻き回したコイル12に交流電力供給手段
13から、第3図(a)に示すような連続した交流電力を
供給する場合について説明したが、交流電力供給手段13
からパルス電流を出力し、このパルス電流に直流バイア
スを加算することにより、強磁性体コア11の磁化曲線の
基準点を変えて、磁束密度検出の測定スパンをシフトし
て移動し、疵の検出精度をより向上させることができ
る。In the above embodiment, the AC power supply means is provided to the coil 12 wound around the ferromagnetic cores 11 of the plurality of magnetic sensors 5.
The case of supplying continuous AC power as shown in FIG. 3 (a) from 13 has been described, but the AC power supply means 13
Pulse current is output from the pulse current, and the DC bias is added to this pulse current to change the reference point of the magnetization curve of the ferromagnetic core 11 to shift and move the measurement span for detecting the magnetic flux density to detect a flaw. The accuracy can be further improved.
第6図はコイル12に直流バイアスを加えたパルス電流を
供給する場合の実施例の磁気センサ5を示す。図に示す
ように、交流電力供給手段13から高周波電圧パルス電流
が加算器21に供給されるとともに直流電源22から直流バ
イアスが加算器21に供給される。加算器21では高周波電
圧に直流バイアスを加算して合成電圧を発生し、その合
成電圧が電力増幅器23で増幅され、抵抗からなる固定イ
ンピーダンス14を介してコイル12に供給される。FIG. 6 shows a magnetic sensor 5 of an embodiment in the case of supplying a pulse current with a DC bias applied to the coil 12. As shown in the figure, a high-frequency voltage pulse current is supplied from the AC power supply means 13 to the adder 21, and a DC bias is supplied from the DC power supply 22 to the adder 21. In the adder 21, a DC bias is added to the high frequency voltage to generate a combined voltage, and the combined voltage is amplified by the power amplifier 23 and supplied to the coil 12 via the fixed impedance 14 composed of a resistor.
この実施例において、直流電源22からの直流バイアス電
流の値を0mA,50mA,100mA,150mA,200mAと変化させて、外
部磁界の磁束密度の変化に対するコイル12の出力電圧を
測定した結果、第7図に示す検出感度特性が得られた。In this example, the value of the DC bias current from the DC power supply 22 was changed to 0 mA, 50 mA, 100 mA, 150 mA, and 200 mA, and the output voltage of the coil 12 was measured with respect to the change in the magnetic flux density of the external magnetic field. The detection sensitivity characteristics shown in the figure were obtained.
第7図からわかるように、パルス電流に直流バイアス電
流を加算すると、直流バイアス電流の値を変えても出力
電圧は極めて良好な線形特性を得ることができ、例えば
直流バイアス電流を100mA供給すると線形特性が得られ
る範囲が0〜40ガウス程度となり、直流バイアス電流が
0mAのときの0〜20ガウス程度と比べて磁束密度の測定
スパンを移動することができ、測定エリアの変更を容易
に行うことができる。As can be seen from FIG. 7, when the DC bias current is added to the pulse current, the output voltage can obtain a very good linear characteristic even if the value of the DC bias current is changed. The range where the characteristics are obtained is about 0 to 40 Gauss, and the DC bias current is
The measurement span of the magnetic flux density can be moved compared to 0 to 20 Gauss at 0 mA, and the measurement area can be easily changed.
また、直流電源22からの直流バイアス電流を磁気検出手
段16が出力する検出信号Sに応じて可変可能とし、測定
条件が変化しても常に良好な測定スパンを得るようにし
ても良い。Further, the DC bias current from the DC power supply 22 may be made variable according to the detection signal S output from the magnetic detection means 16 so that a good measurement span can always be obtained even if the measurement conditions change.
第8図は直流バイアス電流を可変する場合の実施例を示
すブロック図である。図に示すように、磁気検出手段16
の検出信号Sをローパスフィルタ24を介して差動増幅器
25に送る。差動増幅器25は検出信号Sと基準電圧発生器
26からの基準電圧とを比較し、その差電圧を直流電源22
に送る。この差電圧により直流電源22は直流バイアス電
流を可変して加算器21に送る。FIG. 8 is a block diagram showing an embodiment in which the DC bias current is varied. As shown in the figure, the magnetic detection means 16
Detection signal S of the differential amplifier through the low-pass filter 24
Send to 25. The differential amplifier 25 is a detection signal S and a reference voltage generator.
The reference voltage from 26 is compared and the difference voltage is compared with the DC power supply 22
Send to. The DC power supply 22 changes the DC bias current by this difference voltage and sends it to the adder 21.
このように磁気検出手段16を検出信号Sにより磁気セン
サ5の動作点を検出し、基準電圧発生器26の基準電圧と
の差電圧を差動増幅器26で求めて直流電源22からの直流
バイアスを制御することにより、欠陥が無い状態での磁
気検出手段16の検出信号Sが常に0Vになるように自動的
に補償する。In this way, the magnetic detection means 16 detects the operating point of the magnetic sensor 5 by the detection signal S, and the differential voltage from the reference voltage of the reference voltage generator 26 is obtained by the differential amplifier 26 to obtain the DC bias from the DC power supply 22. By the control, the detection signal S of the magnetic detection means 16 in the state where there is no defect is automatically compensated so that it is always 0V.
このように磁気センサ5の測定スパンの中央に動作点を
自動的に補償することにより、測定条件が変化しても常
に良好な測定スパンを確保でき、探傷性能をさらに向上
させることができる。By automatically compensating the operating point in the center of the measurement span of the magnetic sensor 5 as described above, a good measurement span can always be ensured even if the measurement conditions change, and the flaw detection performance can be further improved.
[発明の効果] 以上説明したように、この発明における磁気センサは、
強磁性体コアに巻き回されコイルに一定周波数,一定電
圧の交流電力を供給し、このコイルに流れる交流電流に
より生じる磁界によってヒステリシス特性を示す強磁性
体コアの透磁率によりコイルのインピーダンスを変化さ
せ、コイルの両端出力電圧を正負対称のほぼ矩形波状に
変化させる。このコイルを鋼板に近接して配置し鋼板か
らの漏洩磁束により、コイルの両端出力電圧の正側電圧
と負側電圧の電圧値を変化させる。この変化する正側電
圧と負側電圧をそれぞれ検出し、検出した正側電圧と負
側電圧の差を算出し、鋼板の漏洩磁束を電気信号として
検出するようにしたので、漏洩磁束を極めて高感度に検
出できる。As described above, the magnetic sensor according to the present invention is
AC power of constant frequency and voltage is supplied to the coil wound around the ferromagnetic core, and the magnetic field generated by the alternating current flowing in this coil changes the impedance of the coil by the permeability of the ferromagnetic core that exhibits hysteresis characteristics. , The output voltage across the coil is changed into a substantially rectangular wave with positive and negative symmetry. The coil is arranged close to the steel plate, and the leakage magnetic flux from the steel plate changes the positive and negative voltage values of the output voltage across the coil. The changing positive side voltage and the negative side voltage are detected respectively, the difference between the detected positive side voltage and the negative side voltage is calculated, and the leakage flux of the steel sheet is detected as an electric signal. It can be detected with sensitivity.
この磁気センサを複数使用し、各磁気センサのコイルを
連続的に移動する鋼板の幅方向に沿って配設し、各磁気
センサからの出力信号を少なくとも2群に分けて、各磁
気センサ群毎の検出信号のピーク値を検出し、磁気セン
サ群毎のピーク値の差を演算することにより、圧延条件
等によって鋼板の幅方向に沿って生じるノイズを除去す
るようにしたから、ノイズ成分を除去した検出信号によ
り鋼板の微小な疵も検出することができ、鋼板の疵検出
精度を向上させることができる。A plurality of these magnetic sensors are used, the coils of each magnetic sensor are arranged along the width direction of the steel plate that moves continuously, and the output signals from each magnetic sensor are divided into at least two groups, and each magnetic sensor group By detecting the peak value of the detection signal and calculating the difference between the peak values for each magnetic sensor group, the noise generated along the width direction of the steel sheet due to the rolling conditions etc. is removed, so the noise component is removed. The microscopic flaw of the steel plate can be detected by the detected signal, and the flaw detection accuracy of the steel plate can be improved.
また、磁気センサのコイルに直流バイアスを加算したパ
ルス電流を供給することにより、漏洩磁束の測定スパン
を拡大することができ、疵検出精度をより向上させるこ
とができる。Further, by supplying a pulse current added with a DC bias to the coil of the magnetic sensor, the measurement span of the leakage magnetic flux can be expanded and the flaw detection accuracy can be further improved.
また、パルス電流に加算する直流バイアスを磁気検出手
段からの磁気検出信号に応じて可変制御することによ
り、磁気センサの動作点を自動的に補償して、測定条件
が変化しても常に良好な測定スパンを確保することがで
き、探傷精度をさらに高めることができる。In addition, the DC bias added to the pulse current is variably controlled according to the magnetic detection signal from the magnetic detection means, so that the operating point of the magnetic sensor is automatically compensated, and even if the measurement condition changes, it is always good. The measurement span can be secured, and the flaw detection accuracy can be further improved.
第1図はこの発明の実施例を示すブロツク図、第2図
(a),(b)は各々上記実施例のコイルの配置図、第
3図,第4図は上記実施例の磁気センサの原理を示し、
第3図(a),(b),(c)はそれぞれ電圧波形図、
第4図は強磁性体コアの磁化特性図、第5図は上記実施
例の磁気センサの出力特性図、第6図は他の実施例を示
すブロック図、第7図は第6図に示した実施例の出力特
性図、第8図は第3の実施例を示すブロック図、第9図
は従来例を示す断面図である。 1……鋼板、5……磁気センサ、6a,6b……ピーク値検
出手段、7……演算手段、8……比較手段、11……強磁
性体コア、12……コイル、13……交流電力供給手段、14
……固定インピーダンス、15……直流電圧検出手段、16
……磁気検出手段、21……加算器、22……直流電源、25
……差動増幅器、26……基準電圧発生器。FIG. 1 is a block diagram showing an embodiment of the present invention, FIGS. 2 (a) and 2 (b) are layout diagrams of the coils of the above embodiments, and FIGS. 3 and 4 are of the magnetic sensor of the above embodiments. Showing the principle,
3 (a), (b), and (c) are voltage waveform diagrams,
FIG. 4 is a magnetization characteristic diagram of the ferromagnetic core, FIG. 5 is an output characteristic diagram of the magnetic sensor of the above embodiment, FIG. 6 is a block diagram showing another embodiment, and FIG. 7 is shown in FIG. FIG. 8 is a block diagram showing the output characteristic of the embodiment, FIG. 8 is a block diagram showing the third embodiment, and FIG. 9 is a sectional view showing the conventional example. 1 ... steel plate, 5 ... magnetic sensor, 6a, 6b ... peak value detecting means, 7 ... computing means, 8 ... comparing means, 11 ... ferromagnetic material core, 12 ... coil, 13 ... AC Power supply means, 14
...... Fixed impedance, 15 ...... DC voltage detection means, 16
...... Magnetic detection means, 21 …… Adder, 22 …… DC power supply, 25
...... Differential amplifier, 26 …… Reference voltage generator.
Claims (3)
コイルに固定インピーダンスを介して一定周波数,一定
電圧の交流電力を供給する交流電力供給手段と、上記コ
イルの両端から出力する電圧の正側電圧と負側電圧をそ
れぞれ検出する直流電圧検出手段と、該直流電圧検出手
段で検出した正側電圧と負側電圧の差を演算し磁界の強
さを検出する磁気検出手段とからなる磁気センサを、複
数個有する鋼板の疵検出装置であって、 上記複数の磁気センサの強磁性体コアに巻き回されたコ
イルを連続的に移動する鋼板の幅方向に沿って複数群に
分けて配設し、 上記複数の磁気センサからの出力信号を少なくとも2群
に分けて入力し、各磁気センサ群毎の検出信号のピーク
値を検出するピーク値検出手段と、 該ピーク値検出手段で検出した複数群のピーク値の差を
演算する演算手段と、 該演算手段で演算した結果とあらかじめ設定されたしき
い値とを比較する比較手段と、 を備えたことを特徴とする鋼板の疵検出装置。1. A coil wound around a ferromagnetic core, AC power supply means for supplying AC power having a constant frequency and a constant voltage to the coil through a fixed impedance, and a voltage output from both ends of the coil. DC voltage detecting means for detecting the positive side voltage and negative side voltage of the magnetic field, and magnetic detecting means for calculating the difference between the positive side voltage and the negative side voltage detected by the DC voltage detecting means to detect the strength of the magnetic field. A flaw detection device for a steel plate having a plurality of magnetic sensors, wherein the coils wound around the ferromagnetic cores of the plurality of magnetic sensors are divided into a plurality of groups along the width direction of the continuously moving steel plate. And a peak value detecting means for detecting the peak value of the detection signal for each magnetic sensor group by inputting the output signals from the plurality of magnetic sensors into at least two groups, and the peak value detecting means. Multiple detected A calculating means for calculating a difference between the peak value of flaw detection device steel sheet characterized by comprising a comparison means for comparing a preset threshold with the results calculated by said calculating means.
ス電流を出力し、該パルス電流に直流バイアスを加算す
る直流バイアス加算手段を設けた請求項1記載の鋼板の
疵検出装置。2. The flaw detection apparatus for a steel sheet according to claim 1, wherein the AC power supply means of the magnetic sensor outputs a pulse current, and a DC bias adding means for adding a DC bias to the pulse current is provided.
じて上記直流バイアス加算手段で加算する直流バイアス
を可変制御する制御手段を設けた請求項2記載の鋼板の
疵検出装置。3. A flaw detection device for a steel sheet according to claim 2, further comprising control means for variably controlling a DC bias added by said DC bias adding means in accordance with a magnetic detection signal from said magnetic detection means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4241790A JPH07113626B2 (en) | 1990-02-26 | 1990-02-26 | Steel plate flaw detection device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4241790A JPH07113626B2 (en) | 1990-02-26 | 1990-02-26 | Steel plate flaw detection device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03246463A JPH03246463A (en) | 1991-11-01 |
| JPH07113626B2 true JPH07113626B2 (en) | 1995-12-06 |
Family
ID=12635490
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4241790A Expired - Fee Related JPH07113626B2 (en) | 1990-02-26 | 1990-02-26 | Steel plate flaw detection device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH07113626B2 (en) |
-
1990
- 1990-02-26 JP JP4241790A patent/JPH07113626B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03246463A (en) | 1991-11-01 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US3609530A (en) | Magnetic leakage field flaw detector with compensation for variation in spacing between magnetizer and test piece | |
| JP2004503765A (en) | Magnetic transducer torque measurement | |
| JPS6352345B2 (en) | ||
| JP2841153B2 (en) | Weak magnetism measurement method and device, and nondestructive inspection method using the same | |
| JP2848081B2 (en) | Magnetic flaw detector | |
| JPH0989843A (en) | Eddy current flaw detection method and eddy current flaw detection device | |
| JPH0784021A (en) | Weak magnetic measurement device and nondestructive inspection method using the same | |
| JP4192708B2 (en) | Magnetic sensor | |
| JP2002257789A (en) | Leakage magnetic flux detector | |
| JP2617571B2 (en) | Magnetic measuring device | |
| JPH07113626B2 (en) | Steel plate flaw detection device | |
| JP2617615B2 (en) | Magnetic measurement method and device | |
| JPH07113625B2 (en) | Steel plate flaw detection device | |
| JP2020197381A (en) | Gradient magnetic field sensor | |
| JP2020165716A (en) | Gradient magnetic field sensor | |
| JP2617570B2 (en) | Magnetic measuring device | |
| JP2617605B2 (en) | Magnetic measuring device and diagnostic method for magnetic flaw detector | |
| EP0376095B1 (en) | Magnetic flux measuring method and apparatus for embodying the same | |
| JPH09166582A (en) | Electromagnetic flaw detection | |
| JPH0750711Y2 (en) | Magnetic flaw detector for thin steel strip | |
| Deyneka et al. | Non-destructive testing of ferromagnetic materials using hand inductive sensor | |
| JPS62294987A (en) | Method and apparatus for measuring magnetic property | |
| JP2663767B2 (en) | Transformation rate measuring method and apparatus | |
| RU2035745C1 (en) | Coercimeter attachment | |
| WO1991012524A1 (en) | Flaw detector for steel sheet |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |