JP2013050390A - Magnetic characteristic measurement sensor, and magnetic characteristic measurement method using the same sensor - Google Patents

Magnetic characteristic measurement sensor, and magnetic characteristic measurement method using the same sensor Download PDF

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JP2013050390A
JP2013050390A JP2011188653A JP2011188653A JP2013050390A JP 2013050390 A JP2013050390 A JP 2013050390A JP 2011188653 A JP2011188653 A JP 2011188653A JP 2011188653 A JP2011188653 A JP 2011188653A JP 2013050390 A JP2013050390 A JP 2013050390A
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permanent magnet
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JP5576840B2 (en
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Kazu Nakahata
和 中畑
Borkowski Bartosz
ボルコヴスキー バルトッシュ
Masato Ezono
正人 榎園
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OITA-KEN SANGYOSOZOKIKO
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Abstract

PROBLEM TO BE SOLVED: To decrease a measurement error when measuring a magnetic characteristic of a permanent magnet.SOLUTION: In a magnetic characteristic measurement sensor (1) for measuring the magnetic characteristic of the permanent magnet, a B coil (4) for measuring a magnetic flux density of the permanent magnet, and an H coil (5) for measuring an intensity of the magnetic field of the permanent magnet and/or an M coil (6) for measuring a magnetization intensity of the permanent magnet are wound coaxially around the periphery of the permanent magnet. The number of turns of the H coil (5) is the same as that of the B coil (4). A product of the cross sectional area and the number of the turns of the M coil (6) is the same as that of the B coil (4). The intensity of the magnetic field and the magnetization intensity of the permanent magnet are measured with the H coil (5) and/or the M coil (6), and the B coil (4).

Description

本発明は、永久磁石の磁気特性を測定するための磁気特性測定センサー及び同センサーを用いた磁気特性測定方法に関するものである。   The present invention relates to a magnetic property measuring sensor for measuring magnetic properties of a permanent magnet and a magnetic property measuring method using the sensor.

永久磁石は、磁束密度や磁界強度や磁化をパラメーターとして用いて磁気特性が評価される。そして、永久磁石の磁気特性を測定する方法としては、日本工業規格に「永久磁石試験方法」として規格されている(非特許文献1参照。)。   Permanent magnets are evaluated for magnetic properties using magnetic flux density, magnetic field strength, and magnetization as parameters. And as a method of measuring the magnetic characteristic of a permanent magnet, it is standardized as a “permanent magnet test method” in Japanese Industrial Standards (see Non-Patent Document 1).

この日本工業規格で定められた「永久磁石試験方法」によれば、測定対象となる永久磁石と電磁石とで閉磁気回路を構成し、磁束密度を測定するためのBコイルと磁気分極の測定に用いるJコイルと磁界強度を測定するHセンサーとを用いて、永久磁石の磁気特性を測定する。   According to the “permanent magnet test method” defined in the Japanese Industrial Standard, a closed magnetic circuit is constituted by a permanent magnet and an electromagnet to be measured, and the B coil and magnetic polarization for measuring the magnetic flux density are measured. The magnetic characteristics of the permanent magnet are measured using the J coil to be used and the H sensor for measuring the magnetic field strength.

ここで、永久磁石の磁束密度は、永久磁石の周囲にBコイルを巻回し、Bコイルの誘導電圧を積分することで測定する。また、永久磁石の磁化(磁気分極)は、永久磁石の周囲にJコイルを巻回するとともに永久磁石の周囲に巻回していないBコイルをJコイルに互いに電気的に打ち消し合うように接続することでBコイルを空隙補償コイルとして用い、Jコイルの誘導電圧を積分することで測定する。また、磁界強度は、永久磁石の側方近傍にフラットサーチコイルや磁気ポテンショメーターやホールプローブなどのHセンサーを配置して測定する。   Here, the magnetic flux density of the permanent magnet is measured by winding a B coil around the permanent magnet and integrating the induced voltage of the B coil. The magnetization (magnetic polarization) of the permanent magnet is such that the J coil is wound around the permanent magnet and the B coil not wound around the permanent magnet is electrically connected to the J coil so as to cancel each other. The B coil is used as the air gap compensation coil, and the measurement is performed by integrating the induced voltage of the J coil. The magnetic field strength is measured by arranging an H sensor such as a flat search coil, a magnetic potentiometer, or a hall probe near the side of the permanent magnet.

日本工業規格 JIS C2501 「永久磁石試験方法」Japanese Industrial Standard JIS C2501 “Permanent Magnet Test Method”

ところが、上記した日本工業規格で定められた「永久磁石試験方法」では、永久磁石の磁界強度や磁化の測定において必ずしも測定誤差が十分小さいものとは言えず、永久磁石の磁界強度や磁化といった磁気特性を正確に評価することが困難であった。   However, the “permanent magnet test method” defined in the above Japanese Industrial Standards does not necessarily have a sufficiently small measurement error in the measurement of the magnetic field strength and magnetization of the permanent magnet. It was difficult to accurately evaluate the characteristics.

そこで、請求項1に係る本発明では、永久磁石の磁気特性を測定するための磁気特性測定センサーにおいて、永久磁石の磁束密度を測定するためのBコイルと、永久磁石の磁界強度の測定に用いるHコイル及び/又は永久磁石の磁化の測定に用いるMコイルとを、永久磁石の周囲に同軸上に巻回することにした。   Therefore, in the present invention according to claim 1, in the magnetic characteristic measuring sensor for measuring the magnetic characteristics of the permanent magnet, the B coil for measuring the magnetic flux density of the permanent magnet and the magnetic field strength of the permanent magnet are used. The H coil and / or the M coil used for measuring the magnetization of the permanent magnet were coaxially wound around the permanent magnet.

また、請求項2に係る本発明では、前記請求項1に係る本発明において、前記Hコイルは、巻数が前記Bコイルと同一であることにした。   Further, in the present invention according to claim 2, in the present invention according to claim 1, the number of turns of the H coil is the same as that of the B coil.

また、請求項3に係る本発明では、前記請求項1に係る本発明において、前記Mコイルは、断面積と巻数との積が前記Bコイルと同一であることにした。   In the present invention according to claim 3, in the present invention according to claim 1, the M coil has the same product of the cross-sectional area and the number of turns as the B coil.

また、請求項4に係る本発明では、永久磁石の磁気特性を磁気特性測定センサーを用いて測定する磁気特性測定方法において、磁気特性測定センサーは、永久磁石の磁束密度を測定するためのBコイルと、永久磁石の磁界強度の測定に用いるHコイル及び/又は永久磁石の磁化の測定に用いるMコイルとを、永久磁石の周囲に同軸上に巻回し、前記Hコイル及び/又はMコイルと前記Bコイルとで永久磁石の磁界強度及び/又は磁化を測定することにした。   According to a fourth aspect of the present invention, in the magnetic property measuring method for measuring the magnetic property of the permanent magnet using the magnetic property measuring sensor, the magnetic property measuring sensor is a B coil for measuring the magnetic flux density of the permanent magnet. And an H coil used for measuring the magnetic field strength of the permanent magnet and / or an M coil used for measuring the magnetization of the permanent magnet are wound coaxially around the permanent magnet, and the H coil and / or M coil and the It was decided to measure the magnetic field strength and / or magnetization of the permanent magnet with the B coil.

そして、本発明では、永久磁石の磁気特性を測定するための磁気特性測定センサーにおいて、永久磁石の磁束密度を測定するためのBコイルと、永久磁石の磁界強度の測定に用いるHコイル及び/又は永久磁石の磁化の測定に用いるMコイルとを、永久磁石の周囲に同軸上に巻回することにより、永久磁石の磁気特性を測定するにあたって永久磁石の磁界強度や磁化の測定誤差を小さくすることができ、永久磁石の磁気特性を従来よりも正確に評価することができる。   In the present invention, in the magnetic property measuring sensor for measuring the magnetic property of the permanent magnet, the B coil for measuring the magnetic flux density of the permanent magnet, the H coil used for measuring the magnetic field strength of the permanent magnet, and / or The M coil used for measuring the magnetization of the permanent magnet is coaxially wound around the permanent magnet to reduce the measurement error of the magnetic field strength and magnetization of the permanent magnet when measuring the magnetic characteristics of the permanent magnet. The magnetic characteristics of the permanent magnet can be evaluated more accurately than before.

本発明に係る磁気特性測定センサーを示す正面断面図。1 is a front sectional view showing a magnetic property measuring sensor according to the present invention. 同側面断面図。FIG.

以下に、本発明に係る磁気特性測定センサー及び同センサーを用いた磁気特性測定方法の具体的な構成について図面を参照しながら説明する。   Hereinafter, a specific configuration of a magnetic characteristic measurement sensor and a magnetic characteristic measurement method using the same according to the present invention will be described with reference to the drawings.

図1に示すように、磁気特性測定センサー1は、所定長さの円柱状に形成した永久磁石の試験片2を挿通させたホルダー3にBコイル4とHコイル5とMコイル6とを巻回している。ここで、Bコイル4は、試験片2の磁束密度を測定するためのコイルであり、Hコイル5は、Bコイル4とともに用いて試験片2の磁界強度を測定するためのコイルであり、Mコイル6は、Bコイル4とともに用いて試験片2の磁化を測定するためのコイルである。   As shown in FIG. 1, the magnetic characteristic measuring sensor 1 has a B coil 4, an H coil 5, and an M coil 6 wound around a holder 3 through which a test piece 2 of a permanent magnet formed in a cylindrical shape having a predetermined length is inserted. It is turning. Here, the B coil 4 is a coil for measuring the magnetic flux density of the test piece 2, and the H coil 5 is a coil for measuring the magnetic field strength of the test piece 2 together with the B coil 4. The coil 6 is a coil for use with the B coil 4 to measure the magnetization of the test piece 2.

ホルダー3は、試験片2を挿通させた円筒状の内側ホルダー7と、内側ホルダー7の外周に装着した円筒状の外側ホルダー8とで構成している。   The holder 3 includes a cylindrical inner holder 7 through which the test piece 2 is inserted, and a cylindrical outer holder 8 attached to the outer periphery of the inner holder 7.

内側ホルダー7は、試験片2を挿通させるために試験片2の径の寸法公差を考慮した内径の中空部9を形成するとともに、外周部にコイル溝10を円周方向に向けて形成している。コイル溝10には、Bコイル4を巻回するとともに、Bコイル4の外周部にHコイル5を絶縁シート11を介して巻回している。これにより、Hコイル5は、試験片2の周囲において試験片2に対してBコイル4と同軸上、かつ、同心円上に配置されている。また、Hコイル5は、巻数がBコイル4と同一となるようにしている。   The inner holder 7 is formed with a hollow portion 9 having an inner diameter in consideration of the dimensional tolerance of the diameter of the test piece 2 in order to allow the test piece 2 to be inserted, and a coil groove 10 is formed on the outer peripheral portion in the circumferential direction. Yes. A B coil 4 is wound around the coil groove 10, and an H coil 5 is wound around the outer periphery of the B coil 4 via an insulating sheet 11. Accordingly, the H coil 5 is arranged coaxially with the B coil 4 and concentrically with respect to the test piece 2 around the test piece 2. Further, the H coil 5 has the same number of turns as the B coil 4.

外側ホルダー8は、内側ホルダー7を挿通させるために中空部12を形成するとともに、外周部にコイル溝13を円周方向に向けて形成している。コイル溝13には、Mコイル6を巻回するとともに、Mコイル6の外周部に絶縁シート14を被覆している。Mコイル6は、巻数と断面積との積がBコイル4と同一となるようにしている。この外側ホルダー8は、コイル溝13を内側ホルダー7のコイル溝10の外周部に位置させており、これにより、Mコイル6は、試験片2の周囲において試験片2に対してBコイル4及びHコイル5と同軸上、かつ、同心円上に配置されている。   The outer holder 8 is formed with a hollow portion 12 so that the inner holder 7 can be inserted therethrough, and a coil groove 13 is formed on the outer peripheral portion in the circumferential direction. An M coil 6 is wound around the coil groove 13, and an outer periphery of the M coil 6 is covered with an insulating sheet 14. The M coil 6 is configured such that the product of the number of turns and the cross-sectional area is the same as that of the B coil 4. In the outer holder 8, the coil groove 13 is positioned on the outer peripheral portion of the coil groove 10 of the inner holder 7, so that the M coil 6 has the B coil 4 and the B coil 4 and the test piece 2 around the test piece 2. It is arranged coaxially with the H coil 5 and concentrically.

上記磁気特性測定センサー1では、試験片2と各コイル4,5,6とを近接させて配置するとともに、各コイル4,5,6やホルダー3の熱等による変形を防止することで、測定精度をより一層向上させることができる。そのため、上記磁気特性測定センサー1では、ホルダー3(内側ホルダー7、外側ホルダー8)を薄くても強度を確保でき耐熱性に優れたセラミック材で形成し、また、薄くて耐熱性を有する絶縁シート11を介してBコイル4にHコイル5を巻回している。   In the magnetic property measuring sensor 1, the test piece 2 and the coils 4, 5, 6 are arranged close to each other, and the coils 4, 5, 6 and the holder 3 are prevented from being deformed by heat, etc. The accuracy can be further improved. Therefore, in the magnetic property measuring sensor 1, the insulating sheet is made of a ceramic material that can ensure strength even when the holder 3 (inner holder 7 and outer holder 8) is thin and has excellent heat resistance, and is thin and has heat resistance. The H coil 5 is wound around the B coil 4 via 11.

磁気特性測定センサー1は、以上に説明したように構成しており、この磁気特性測定センサー1を用いて試験片2の磁気特性を測定することができる。   The magnetic characteristic measurement sensor 1 is configured as described above, and the magnetic characteristic of the test piece 2 can be measured using the magnetic characteristic measurement sensor 1.

磁気特性を測定するには、試験片2の伸延方向の略中央部に磁気特性測定センサー1を装着するとともに、日本工業規格で定められた「永久磁石試験方法」と同様に測定対象と試験片2と電磁石とで閉磁気回路を構成し、試験片2の磁束密度や磁化や磁界強度を測定する。   In order to measure the magnetic properties, the magnetic property measuring sensor 1 is attached to the substantially central portion of the test piece 2 in the extending direction, and the measurement object and the test piece are similar to the “permanent magnet test method” defined by the Japanese Industrial Standards. 2 and an electromagnet constitute a closed magnetic circuit, and the magnetic flux density, magnetization, and magnetic field strength of the test piece 2 are measured.

磁束密度を測定する場合には、試験片2の周囲に巻回したBコイル4の誘導電圧を積分することで測定できる。   When measuring the magnetic flux density, it can be measured by integrating the induced voltage of the B coil 4 wound around the test piece 2.

磁化を測定する場合には、試験片2の周囲に同軸上に巻回したBコイル4とMコイル6とを用い、以下に説明するように、Mコイル6を空隙補償コイルとして利用することで測定できる。   When measuring the magnetization, the B coil 4 and the M coil 6 wound coaxially around the test piece 2 are used, and the M coil 6 is used as a gap compensation coil as described below. It can be measured.

まず、それぞれのBコイル4とMコイル6とで得られる磁束密度BB、BMは、磁界強度をH、磁化をM、透磁率をμ0とすると、式1で示される。

Figure 2013050390
First, the magnetic flux densities B B and B M obtained by each of the B coil 4 and the M coil 6 are expressed by Equation 1, where the magnetic field strength is H, the magnetization is M, and the magnetic permeability is μ 0 .
Figure 2013050390

この式1を、Bコイル4とMコイル6とで得られる磁束φB、φMで表すと、Bコイル4とMコイル6と試験片2の断面積をそれぞれSB、SM、SSとすると、式2に変形できる。

Figure 2013050390
When Expression 1 is expressed by magnetic fluxes φ B and φ M obtained by the B coil 4 and the M coil 6, the cross-sectional areas of the B coil 4, the M coil 6 and the test piece 2 are respectively represented by S B , S M and S S. Then, it can be transformed into Equation 2.
Figure 2013050390

そして、Bコイル4とMコイル6とを直列接続したときに計測される電圧eBMは、Bコイル4とMコイル6の巻数をそれぞれNB、NMとすると、式3で示される。この式3に上記式2を代入して展開すると、電圧eBMは、式4に変形できる。

Figure 2013050390
The voltage e BM measured when the B coil 4 and the M coil 6 are connected in series is expressed by Equation 3 when the number of turns of the B coil 4 and the M coil 6 is N B and N M , respectively. When the above expression 2 is substituted into the expression 3 and developed, the voltage e BM can be transformed into the expression 4.
Figure 2013050390

ここで、Bコイル4とMコイル6は、巻数と断面積との積が同一(NBB=NMM)であることから、式4は、式5と表せる。

Figure 2013050390
Here, since the product of the number of turns and the cross-sectional area of the B coil 4 and the M coil 6 is the same (N B S B = N M S M ), the expression 4 can be expressed as the expression 5.
Figure 2013050390

したがって、磁化は、式5を積分して変形することで式6を用いて求めることができ、Bコイル4とMコイル6とを直列接続したときに経時的に計測される電圧eBMを積分回路で積分した値から測定することができる。

Figure 2013050390
Therefore, the magnetization can be obtained by using Equation 6 by integrating and transforming Equation 5, and integrating the voltage e BM measured over time when the B coil 4 and the M coil 6 are connected in series. It can be measured from the value integrated by the circuit.
Figure 2013050390

ここで、磁化は、試験片2に巻回していない空隙補償コイルをBコイル4に互いに電気的に打ち消し合うように接続したときに計測される電圧eから式7を用いて測定することもできる。

Figure 2013050390
Here, the magnetization can also be measured by using Equation 7 from the voltage e measured when the air gap compensation coils that are not wound around the test piece 2 are connected to the B coil 4 so as to electrically cancel each other. .
Figure 2013050390

しかしながら、直径10mm、長さ20mmの純度99.99%のニッケル、コバルト、鉄からなる試験片2について実際に測定し、理論値との相対的な誤差を算出したところ、式6を用いた場合には、各試験片2について1.3%、2.74%、1.52%であったのに対して、式7を用いた場合には、各試験片2について16.1%、17.2%、14.7%となった。   However, when actual measurement was performed on a test piece 2 made of nickel, cobalt, and iron with a diameter of 10 mm and a length of 20 mm and a purity of 99.99%, the relative error from the theoretical value was calculated. In contrast, the values of 1.3%, 2.74%, and 1.52% for each test piece 2 were 16.1%, 17.2%, and 14.7% for each test piece 2 when Equation 7 was used.

このことから、上記磁気特性測定センサー1のように試験片2の周囲に同軸上に巻回したBコイル4とMコイル6とを用いて測定することにより、測定誤差を小さくできることが示された。   From this, it was shown that the measurement error can be reduced by measuring using the B coil 4 and M coil 6 coaxially wound around the test piece 2 like the magnetic characteristic measuring sensor 1. .

また、試験片2の端部近傍では反磁界の影響を大きく受けるために、測定誤差が大きくなるおそれがある。そこで、直径10mm、純度99.99%の長さ4mm、10mm、20mm、30mmの試験片2について伸延方向の中央部に磁気特性測定センサー1を装着して実際に測定し、理論値との相対的な誤差を算出したところ、各試験片2について26.7%、7.6%、1.1%、0.9%となった。   Further, the measurement error may be increased because the demagnetizing field is greatly influenced near the end of the test piece 2. Therefore, a test piece 2 having a diameter of 10 mm and a purity of 99.99% and a length of 4 mm, 10 mm, 20 mm, and 30 mm was actually measured by mounting the magnetic property measuring sensor 1 at the center in the distraction direction, and the relative value to the theoretical value. When the error was calculated, it was 26.7%, 7.6%, 1.1%, and 0.9% for each test piece 2.

このことから、上記磁気特性測定センサー1を試験片2に装着する場合には、反磁界の影響が無くなるように試験片2の端部から磁気特性測定センサー1をなるべく離して装着する必要があり、長さ20mm以上の試験片2の伸延方向の中央部に装着することが望ましい。   For this reason, when the magnetic property measuring sensor 1 is attached to the test piece 2, it is necessary to attach the magnetic property measuring sensor 1 as far as possible from the end of the test piece 2 so as to eliminate the influence of the demagnetizing field. It is desirable to attach the test piece 2 having a length of 20 mm or more to the central portion in the extending direction.

以上のようにして磁化を精度良く測定することができるため、上記磁束密度と磁化とを用いて式8に示される関係式から磁界強度を算出することができる。

Figure 2013050390
Since the magnetization can be accurately measured as described above, the magnetic field strength can be calculated from the relational expression shown in Expression 8 using the magnetic flux density and the magnetization.
Figure 2013050390

また、磁界強度は、試験片2の周囲に同軸上に巻回したBコイル4とHコイル5とを用い、以下に説明するように、Hコイル5を空隙補償コイルとして利用することで測定することもできる。   The magnetic field strength is measured by using the B coil 4 and the H coil 5 coaxially wound around the test piece 2 and using the H coil 5 as a gap compensation coil as will be described below. You can also.

まず、それぞれのBコイル4とHコイル5とで得られる磁束密度BB、BHは、磁界強度をH、磁化をM、透磁率をμ0とすると、式9で示される。

Figure 2013050390
First, the magnetic flux densities B B and B H obtained by the respective B coils 4 and H coils 5 are expressed by Equation 9 where the magnetic field strength is H, the magnetization is M, and the magnetic permeability is μ 0 .
Figure 2013050390

この式9を、Bコイル4とHコイル5とで得られる磁束ΦB、ΦHで表すと、Bコイル4とHコイル5と試験片2の断面積をそれぞれSB、SH、SSとし、Bコイル4とHコイル5の巻数をそれぞれNB、NHとすると、式10に変形できる。

Figure 2013050390
When Expression 9 is expressed by magnetic fluxes Φ B and Φ H obtained by the B coil 4 and the H coil 5, the cross-sectional areas of the B coil 4, the H coil 5 and the test piece 2 are respectively represented by S B , S H and S S. Assuming that the numbers of turns of the B coil 4 and the H coil 5 are N B and N H , respectively, the equation 10 can be obtained.
Figure 2013050390

そして、Hコイル5とBコイル4とでそれぞれ計測される電圧eH、eBの差は、式11で示される。この式11に上記式10を代入して展開すると、電圧eH、eBの差は、式12に変形できる。

Figure 2013050390
The difference between the voltages e H and e B measured by the H coil 5 and the B coil 4 is expressed by Expression 11. When the above equation 10 is substituted into the equation 11 and developed, the difference between the voltages e H and e B can be transformed into the equation 12.
Figure 2013050390

ここで、Bコイル4とHコイル5は、巻数が同一(NB=NH)であることから、式12は、式13と表せる。

Figure 2013050390
Here, since the B coil 4 and the H coil 5 have the same number of turns (N B = N H ), Expression 12 can be expressed as Expression 13.
Figure 2013050390

したがって、磁界強度は、式13を積分して変形することで式14を用いて求めることができ、Hコイル5とBコイル4とでそれぞれ経時的に計測される電圧eH、eBの差を積分回路で積分した値から測定することができる。

Figure 2013050390
Therefore, the magnetic field strength can be obtained by using Equation 14 by integrating and transforming Equation 13, and the difference between voltages e H and e B measured with time in H coil 5 and B coil 4 respectively. Can be measured from the value integrated by the integration circuit.
Figure 2013050390

以上に説明したように、本発明では、試験片2の磁気特性を測定する磁気特性測定センサー1において、磁束密度を測定するためのBコイル4と、Bコイル4とともに用いて磁界強度を測定するためのHコイル5と、Bコイル4とともに用いて磁化を測定するためのMコイル6とを、試験片2の周囲に同軸上に巻回している。   As described above, in the present invention, in the magnetic property measuring sensor 1 for measuring the magnetic property of the test piece 2, the magnetic field strength is measured using the B coil 4 for measuring the magnetic flux density and the B coil 4. An H coil 5 for use with the B coil 4 and an M coil 6 for measuring magnetization are wound around the test piece 2 on the same axis.

そのため、本発明では、試験片2の磁気特性を測定するにあたって磁界強度や磁化の測定誤差を小さくすることができ、試験片2の磁気特性を従来よりも正確に評価することができる。   For this reason, in the present invention, when measuring the magnetic characteristics of the test piece 2, the measurement error of the magnetic field strength and the magnetization can be reduced, and the magnetic characteristics of the test piece 2 can be evaluated more accurately than before.

特に、本発明では、Hコイル5又はMコイル6とBコイル4とを試験片2の周囲に同軸上、かつ、同心円上に配置することで、磁気特性測定センサー1及び同センサー1を用いた測定システムの小型化を図ることもできる。   In particular, in the present invention, the magnetic property measuring sensor 1 and the sensor 1 are used by arranging the H coil 5 or the M coil 6 and the B coil 4 coaxially and concentrically around the test piece 2. It is also possible to reduce the size of the measurement system.

また、本発明では、Hコイル5の巻数をBコイル4の巻数と同一とし、或いは、Mコイル6の断面積と巻数との積をBコイル4の断面積と巻数との積と同一とすることで、経時的に計測される電圧を積分回路で積分することで磁界強度や磁化を容易に測定することができる。   In the present invention, the number of turns of the H coil 5 is the same as the number of turns of the B coil 4, or the product of the sectional area and the number of turns of the M coil 6 is the same as the product of the sectional area and the number of turns of the B coil 4. Thus, the magnetic field strength and the magnetization can be easily measured by integrating the voltage measured over time with the integration circuit.

1 磁気特性測定センサー 2 試験片
3 ホルダー 4 Bコイル
5 Hコイル 6 Mコイル
7 内側ホルダー 8 外側ホルダー
9 中空部 10 コイル溝
11 絶縁シート 12 中空部
13 コイル溝 14 絶縁シート
DESCRIPTION OF SYMBOLS 1 Magnetic characteristic measurement sensor 2 Test piece 3 Holder 4 B coil 5 H coil 6 M coil 7 Inner holder 8 Outer holder 9 Hollow part 10 Coil groove
11 Insulation sheet 12 Hollow part
13 Coil groove 14 Insulation sheet

Claims (4)

永久磁石の磁気特性を測定するための磁気特性測定センサーにおいて、
永久磁石の磁束密度を測定するためのBコイルと、永久磁石の磁界強度の測定に用いるHコイル及び/又は永久磁石の磁化の測定に用いるMコイルとを、永久磁石の周囲に同軸上に巻回したことを特徴とする磁気特性測定センサー。
In a magnetic property measurement sensor for measuring the magnetic properties of a permanent magnet,
A B coil for measuring the magnetic flux density of the permanent magnet and an H coil used for measuring the magnetic field strength of the permanent magnet and / or an M coil used for measuring the magnetization of the permanent magnet are wound coaxially around the permanent magnet. Magnetic characteristic measurement sensor characterized by turning.
前記Hコイルは、巻数が前記Bコイルと同一であることを特徴とする請求項1に記載の磁気特性測定センサー。   The magnetic property measuring sensor according to claim 1, wherein the H coil has the same number of turns as the B coil. 前記Mコイルは、断面積と巻数との積が前記Bコイルと同一であることを特徴とする請求項1に記載の磁気特性測定センサー。   The magnetic property measuring sensor according to claim 1, wherein the M coil has the same cross-sectional area and number of turns as the B coil. 永久磁石の磁気特性を磁気特性測定センサーを用いて測定する磁気特性測定方法において、
磁気特性測定センサーは、永久磁石の磁束密度を測定するためのBコイルと、永久磁石の磁界強度の測定に用いるHコイル及び/又は永久磁石の磁化の測定に用いるMコイルとを、永久磁石の周囲に同軸上に巻回し、
前記Hコイル及び/又はMコイルと前記Bコイルとで永久磁石の磁界強度及び/又は磁化を測定することを特徴とする磁気特性測定方法。
In a magnetic property measurement method for measuring the magnetic properties of a permanent magnet using a magnetic property measurement sensor,
The magnetic characteristic measurement sensor includes a B coil for measuring the magnetic flux density of the permanent magnet, an H coil used for measuring the magnetic field strength of the permanent magnet, and / or an M coil used for measuring the magnetization of the permanent magnet. Wound around the same axis,
A magnetic characteristic measuring method, comprising: measuring magnetic field strength and / or magnetization of a permanent magnet with the H coil and / or M coil and the B coil.
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CN105319520A (en) * 2014-07-16 2016-02-10 山东省明康安托山特种机电有限公司 Forming method and structure of device for detecting magnetic force of permanent magnet
JP2018179660A (en) * 2017-04-10 2018-11-15 日本電磁測器株式会社 Magnetization measurement device and magnetization measurement method
AT520256A1 (en) * 2017-07-17 2019-02-15 Minebea Mitsumi Inc Method and device for testing the magnetic properties of a permanent magnet
RU2718641C1 (en) * 2019-09-04 2020-04-10 Федеральное государственное бюджетное образовательное учреждение высшего образования "Омский государственный технический университет"(ОмГТУ) Method and device for permanent magnets identification by volume magnetization
RU2743072C1 (en) * 2020-06-23 2021-02-15 Федеральное государственное бюджетное образовательное учреждение высшего образования "Омский государственный технический университет"(ОмГТУ) Method and device for identifying permanent magnets on the basis of three-dimensional magnetization

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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105319520A (en) * 2014-07-16 2016-02-10 山东省明康安托山特种机电有限公司 Forming method and structure of device for detecting magnetic force of permanent magnet
JP2018179660A (en) * 2017-04-10 2018-11-15 日本電磁測器株式会社 Magnetization measurement device and magnetization measurement method
AT520256A1 (en) * 2017-07-17 2019-02-15 Minebea Mitsumi Inc Method and device for testing the magnetic properties of a permanent magnet
RU2718641C1 (en) * 2019-09-04 2020-04-10 Федеральное государственное бюджетное образовательное учреждение высшего образования "Омский государственный технический университет"(ОмГТУ) Method and device for permanent magnets identification by volume magnetization
RU2743072C1 (en) * 2020-06-23 2021-02-15 Федеральное государственное бюджетное образовательное учреждение высшего образования "Омский государственный технический университет"(ОмГТУ) Method and device for identifying permanent magnets on the basis of three-dimensional magnetization

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