JP2007047055A - Magnetic susceptibility measuring method, manufacturing method of scale for magnetic susceptibility measurement, magnetic susceptibility measurer, and magnetic susceptibility measuring device - Google Patents
Magnetic susceptibility measuring method, manufacturing method of scale for magnetic susceptibility measurement, magnetic susceptibility measurer, and magnetic susceptibility measuring device Download PDFInfo
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Description
本発明は、反磁性材料の磁化率測定方法、磁化率測定用目盛の作製方法、磁化率測定器及び磁化率測定装置に関するものである。 The present invention relates to a method for measuring a magnetic susceptibility of a diamagnetic material, a method for producing a scale for measuring a magnetic susceptibility, a magnetic susceptibility measuring device, and a magnetic susceptibility measuring device.
従来から、磁性材料における磁化率などの磁気特性を測定するための手段として、超電導量子干渉計(SQUID)が用いられている。(例えば下記特許文献1参照)。
Conventionally, a superconducting quantum interferometer (SQUID) has been used as a means for measuring magnetic properties such as magnetic susceptibility of magnetic materials. (For example, refer to
しかし、SQUIDでは、一般的に、容器に入れた試料の磁化率を測定するため、容器の磁化率による誤差があり、これを補正する必要がある。また、ある程度の量の試料を用いないと感知できないため、当然微小な試料の磁化率を測定できない。 However, in SQUID, in general, since the magnetic susceptibility of a sample placed in a container is measured, there is an error due to the magnetic susceptibility of the container, and this needs to be corrected. In addition, since it cannot be sensed without using a certain amount of sample, naturally the magnetic susceptibility of a minute sample cannot be measured.
本発明は、上記問題点に鑑みてなされたものであって、磁気浮揚可能な反磁性材料の磁化率を容易に測定できる磁化率測定方法と、磁化率測定用目盛の作製方法と、誤差がほとんどなく、少量又は微小な反磁性材料でも磁化率を測定できる磁化率測定器及び磁化率測定装置を提供することを目的とする。 The present invention has been made in view of the above problems, and a magnetic susceptibility measuring method capable of easily measuring the magnetic susceptibility of a diamagnetic material capable of magnetic levitation, a method for producing a magnetic susceptibility measuring scale, and an error. An object of the present invention is to provide a magnetic susceptibility measuring apparatus and a magnetic susceptibility measuring apparatus that can measure the magnetic susceptibility with little or a small amount of diamagnetic material.
本発明の磁化率測定方法は、磁化率が判明している複数種の反磁性材料を、勾配磁場を有する鉛直方向磁場内に一つずつ又は複数同時に浮揚させる工程と、浮揚した前記反磁性材料の各位置及び各磁化率から、前記磁場内における反磁性材料における磁化率と浮揚位置との関係を算出する工程と、磁化率が判明していない反磁性材料を前記磁場内において浮揚させ、この浮揚した位置を特定し、算出された前記磁化率と浮揚位置との関係を用いて前記浮揚した位置を磁化率に変換する工程とを有する。また、別の観点として、本発明の磁化率測定方法は、種類の異なる反磁性材料を勾配磁場を有する鉛直方向磁場内に浮揚させる工程と、前記反磁性材料の浮揚位置における磁場及び磁場勾配を、測定又は数値計算処理によって算出する工程と、測定又は算出された前記磁場及び前記磁場勾配とを用いて前記反磁性材料の磁化率を算出する工程とを有する。 The magnetic susceptibility measuring method of the present invention includes a step of levitating a plurality of types of diamagnetic materials whose magnetic susceptibility is known one by one or a plurality simultaneously in a vertical magnetic field having a gradient magnetic field, and the levitated diamagnetic material The step of calculating the relationship between the magnetic susceptibility and the levitation position of the diamagnetic material in the magnetic field from the position and the magnetic susceptibility of the, and levitation of the diamagnetic material whose magnetic susceptibility is unknown in the magnetic field, Identifying the levitated position and converting the levitated position into a magnetic susceptibility using the calculated relationship between the magnetic susceptibility and the levitated position. As another aspect, the magnetic susceptibility measurement method of the present invention includes a step of levitating different types of diamagnetic materials in a vertical magnetic field having a gradient magnetic field, and a magnetic field and a magnetic field gradient at the levitation position of the diamagnetic material. A step of calculating by measurement or numerical calculation processing, and a step of calculating the magnetic susceptibility of the diamagnetic material using the measured or calculated magnetic field and magnetic field gradient.
上記構成によれば、磁気浮揚可能な反磁性材料の磁化率を容易に測定することができる。 According to the said structure, the magnetic susceptibility of the diamagnetic material which can be magnetically levitated can be measured easily.
本発明に係る磁化率測定用目盛の作製方法は、磁化率が判明している複数種の反磁性材料を、勾配磁場を有する鉛直方向磁場内に一つずつ又は複数同時に浮揚させる工程と、浮揚した前記複数種の反磁性材料の各位置を記録して目盛とする工程と、前記目盛を磁場と勾配磁場との積の値に対応するように分割して小目盛を作製する工程とを有している。 The method for producing a susceptibility measurement scale according to the present invention includes a step of levitating a plurality of types of diamagnetic materials whose susceptibility is known one by one or simultaneously in a vertical magnetic field having a gradient magnetic field, Recording each position of the plurality of types of diamagnetic materials to make a scale, and dividing the scale so as to correspond to the product of a magnetic field and a gradient magnetic field to produce a small scale. is doing.
上記構成によれば、磁化率が判明している複数種の反磁性材料の浮揚位置から得られた目盛が磁場と勾配磁場との積の値に対応するように分割されてなる小目盛を作製する工程を有していることから、様々な磁気浮揚可能な反磁性材料の磁化率を測定するのに使用できる磁化率測定用目盛の作製方法を提供できる。 According to the above configuration, a small scale is produced by dividing the scale obtained from the levitation position of multiple types of diamagnetic materials with known magnetic susceptibility so as to correspond to the product value of the magnetic field and the gradient magnetic field. Therefore, it is possible to provide a method for producing a magnetic susceptibility measuring scale that can be used to measure the magnetic susceptibility of various diamagnetic materials capable of magnetic levitation.
本発明に係る磁化率測定用目盛の作製方法は、前記目盛及び前記小目盛の値を、それぞれに対応した磁化率の値に変換する工程を有していることが好ましい。これにより、目盛が予め磁化率に変換されているため、測定ごとに磁化率に変換する必要がない。なお、例えば、目盛自体に磁化率の値を付加しておけば、測定された反磁性材料の磁化率を直接的に且つ容易に読み取ることができる。 The method for producing a magnetic susceptibility measurement scale according to the present invention preferably includes a step of converting the values of the scale and the small scale into values of magnetic susceptibility corresponding to the scales. Thereby, since the scale is previously converted into magnetic susceptibility, it is not necessary to convert into magnetic susceptibility for every measurement. For example, if the value of the magnetic susceptibility is added to the scale itself, the measured magnetic susceptibility of the diamagnetic material can be read directly and easily.
本発明に係る磁化率測定器は、所定位置を基準とした、勾配磁場を有する鉛直方向磁場内における反磁性材料に対する磁化率の目盛を有しており、前記所定位置から前記基準を移動させて、前記所定強度の鉛直方向磁場内における浮揚した反磁性材料の高さ位置に合わせた際、前記基準の前記所定位置からのずれ幅を前記目盛から読み取って磁化率を測定することを特徴とする。また、本発明に係る磁化率測定装置は、この磁化率測定器と、鉛直方向に磁場を発生させる超電導磁石と、勾配磁場を発生させる勾配磁場発生器とを備えていることを特徴とする。 The susceptibility measuring instrument according to the present invention has a susceptibility scale for a diamagnetic material in a vertical magnetic field having a gradient magnetic field with a predetermined position as a reference, and the reference is moved from the predetermined position. The magnetic susceptibility is measured by reading from the scale the deviation width of the reference from the predetermined position when the height is adjusted to the height position of the levitated diamagnetic material in the vertical magnetic field having the predetermined intensity. . The susceptibility measuring apparatus according to the present invention includes the susceptibility measuring instrument, a superconducting magnet that generates a magnetic field in the vertical direction, and a gradient magnetic field generator that generates a gradient magnetic field.
上記構成によれば、簡易な構成でありながら、容易な操作だけで反磁性材料の磁化率を測定できる磁化率測定器及び磁化率測定装置を提供できる。 According to the above configuration, it is possible to provide a magnetic susceptibility measuring device and a magnetic susceptibility measuring device that can measure the magnetic susceptibility of a diamagnetic material with a simple operation while having a simple configuration.
本発明に係る磁化率測定器は、鉛直方向に磁場を発生させ、かつ、勾配磁場を発生させる超電導磁石と、前記磁場内で浮揚した反磁性材料の浮揚位置を検出する浮揚位置検出器と、前記浮揚位置検出器で測定された前記浮揚位置の磁化率を算出する磁化率算出手段とを備えていることを特徴とする。前記磁化率算出手段は、前記浮揚位置の磁場及び勾配磁場を測定する磁場測定器と、測定された前記磁場及び前記勾配磁場とから前記反磁性材料の磁化率を演算し、算出する磁化率算出器とを備えていることが好ましい。また、前記磁化率算出手段は、前記浮揚位置の磁場及び勾配磁場を数値計算処理により算出し、算出した前記磁場及び前記勾配磁場とから前記反磁性材料の磁化率を演算し、算出する磁化率算出器とを備えているものであってもよい。 A magnetic susceptibility measuring device according to the present invention generates a magnetic field in a vertical direction and generates a gradient magnetic field, a levitation position detector that detects a levitation position of a diamagnetic material levitated in the magnetic field, Magnetic susceptibility calculating means for calculating the magnetic susceptibility of the levitation position measured by the levitation position detector. The magnetic susceptibility calculation means calculates the magnetic susceptibility of the diamagnetic material by calculating the magnetic susceptibility of the diamagnetic material from the magnetic field measuring device that measures the magnetic field and the gradient magnetic field at the levitation position, and the measured magnetic field and the gradient magnetic field. It is preferable to provide a container. The magnetic susceptibility calculating means calculates a magnetic field and a gradient magnetic field at the levitation position by numerical calculation processing, calculates a magnetic susceptibility of the diamagnetic material from the calculated magnetic field and the gradient magnetic field, and calculates the magnetic susceptibility. And a calculator.
上記構成によれば、簡易な構成でありながら、容易な操作だけで反磁性材料の磁化率を測定できる磁化率測定装置を提供できる。 According to the above configuration, it is possible to provide a magnetic susceptibility measuring apparatus capable of measuring the magnetic susceptibility of a diamagnetic material with a simple operation while having a simple configuration.
以下、本発明に係る磁化率測定器を含んだ磁化率測定装置の実施形態について説明する。図1は、本発明に係る磁化率測定器を含んだ磁化率測定装置の概略図である。 Hereinafter, embodiments of a magnetic susceptibility measuring apparatus including a magnetic susceptibility measuring device according to the present invention will be described. FIG. 1 is a schematic view of a magnetic susceptibility measuring apparatus including a magnetic susceptibility measuring device according to the present invention.
磁化率測定装置10は、超伝導コイルからなる筒状の超伝導磁石1と、磁化率測定器2と、試料供給用部材3と、超伝導磁石1によって発生した磁場に勾配磁場を発生させる勾配磁場発生器(図示せず)とを備えている。磁化率測定器2と、試料供給用部材3とは、超電導磁石1の影響を受けないように非磁性材料で形成されている。
The magnetic
超伝導磁石1は超電導線のコイルからなる円筒状のものであり、磁場が鉛直方向に発生するいわゆる縦型の超電導磁石である。図示しないが、クライオスタット内に収められており、冷却器又は液体ヘリウムなどで冷却され励磁されている。なお、この超伝導磁石1によって発生した磁場内に、例えば勾配磁場発生器を設けて、鉛直方向の高さによって磁場が変化する勾配磁場を発生させるが、この勾配磁場発生器は、超伝導磁石1とともに上記クライオスタット内に収められた超電導線からなる逆転コイルであってもよいし、磁場内に設けられた金属のリングであってもよい。または、勾配磁場発生器を用いずに、超伝導磁石1のみで磁場及び磁場勾配を発生させてもよい。
The
磁化率測定器2は、棒部材2aと、棒部材2a下部に設けられた試料4の位置を特定するためのCCDカメラ2bとを備えている。また、棒部材2aの上部には、磁化率を読み取るための目盛2cが形成されている。さらに、CCDカメラ2bのレンズの中心が存在する鉛直方向の中心断面が、目盛2cの基準5となっている。この基準5を試料4の浮揚位置と一致させて、所定位置からの基準5のずれ幅を目盛から読み取ることによって磁化率を測定できるようにしている。なお、上記所定位置は、例えば、予め磁化率が判明している複数の反磁性材料の一番高く浮揚したものの位置としてもよいし、逆に一番低く浮揚したものの位置としてもよく、これらに限られず、適宜決定してよい。つまり、この決定された所定位置を目盛2cの基準5の最初の位置(基準点)として、この最初の位置からのずれ幅を目盛から読み取るだけで磁化率を測定できる。
The magnetic
ここで、目盛2cは、以下のようにして形成する。予めSQUIDなどで測定され、磁化率が判明している複数の反磁性材料(例えば、後述する試料4で挙げる反磁性材料など)を超電導磁石1内の所定強度の鉛直方向磁場内に一つずつ又は複数同時に浮揚させ、この浮揚した反磁性材料の各位置を記録して目盛とする。このとき、磁化率が判明している複数の反磁性材料の磁化率の値を目盛に直接記録し、さらに、この目盛間を磁場と勾配磁場との積の値に対応するように分割して小目盛を形成する。なお、目盛の値をそれぞれの測定した試料に対応した磁化率の値に予め変換しておくことで、磁化率を容易に測定及び判明させることができる。このように目盛2cを形成すれば、反磁性材料の浮揚位置を特定し、目盛のずれ幅を読み取るだけで、様々な磁気浮揚可能な反磁性材料の磁化率を直接的にかつ容易に読み取ることができる。
Here, the scale 2c is formed as follows. A plurality of diamagnetic materials (for example, diamagnetic materials mentioned in the sample 4 to be described later) that have been measured in advance with SQUID and whose magnetic susceptibility is known are placed one by one in a vertical magnetic field having a predetermined strength in the
試料供給用部材3は、棒状部材と、この棒状部材の下部に設けられた試料4を載置自在な椀状部とを備えている。試料4は磁気浮揚が可能な反磁性材料であり、例えば、ポリプロピレン、ポリエチレン、ポリスチレン、ポリアミド、ポリカーボネートなどが挙げられる。これらの試料を磁場内で浮揚させ、目盛2cを形成する際に使用する。なお、試料4の浮揚位置は超電導磁石1の中心軸上である。
The sample supply member 3 includes a rod-shaped member and a bowl-shaped portion on which the sample 4 provided under the rod-shaped member can be placed. Sample 4 is a diamagnetic material capable of magnetic levitation, and examples thereof include polypropylene, polyethylene, polystyrene, polyamide, and polycarbonate. These samples are levitated in a magnetic field and used when the scale 2c is formed. The levitation position of the sample 4 is on the central axis of the
磁化率測定器2及び磁化率測定装置10によれば、反磁性材料の磁化率の目盛を有しているので、簡易な構成でありながら、容易な操作だけで反磁性材料の磁化率を測定できる。
According to the magnetic
次に、本発明に係る磁化率測定器及び磁化率測定装置における目盛について実施例を用いて説明する。 Next, the scale in the magnetic susceptibility measuring device and the magnetic susceptibility measuring device according to the present invention will be described using examples.
図1と同構成を有する磁化率測定装置における超伝導磁石には、鉛直方向に磁場を発生させるジャパンスーパーコンダクタテクノロジー(株)製のJMTD−LH15T40(15Tの最大磁場を発生でき、鉛直方向を中心軸とするφ40mmの筒形状の空間において、磁場と磁場勾配との積を1500T2/mとすることができる。超伝導磁石の大きさはφ800mm×高さ1800mmである。)を用いた。試料には、約3mm×2mm×2mmの大きさのポリエチレン(PE)、ポリカーボネート(PC)、ポリプロピレン(PP)、ポリスチレン(PS)(いずれも(株)サンプラテック製)、φ3.2mmの球形のポリアミド(PA)(アズワン(株)製)を用いた。 The superconducting magnet in the magnetic susceptibility measuring apparatus having the same configuration as in FIG. 1 has a JMTD-LH15T40 (manufactured by Japan Superconductor Technology Co., Ltd.) that generates a magnetic field in the vertical direction. In a cylindrical space of φ40 mm as the axis, the product of the magnetic field and the magnetic field gradient can be 1500 T 2 / m (the size of the superconducting magnet is φ800 mm × height 1800 mm). Samples include polyethylene (PE), polycarbonate (PC), polypropylene (PP), polystyrene (PS) (all manufactured by Sampratec Co., Ltd.), and a spherical polyamide of φ3.2 mm, each having a size of about 3 mm × 2 mm × 2 mm. (PA) (manufactured by ASONE Co., Ltd.) was used.
PE、PC、PP、PS、PAの各試料について、図1と同構成を有する磁化率測定装置を用いて、各試料が磁気浮揚するのに必要なB(z)dB(z)/dzの値を測定した。
この磁化率測定装置における各試料の超電導磁石の底部からの浮揚位置と併せて、各試料のB(z)dB(z)/dzの値を下記表1に示す。このとき、目盛に各試料のz軸方向についての浮揚位置を記録し、小目盛を上記実施形態で説明した要領で形成しておく。
For each sample of PE, PC, PP, PS, and PA, B (z) dB (z) / dz required for each sample to be magnetically levitated using the magnetic susceptibility measuring device having the same configuration as FIG. The value was measured.
The values of B (z) dB (z) / dz of each sample are shown in Table 1 below together with the levitation position of each sample from the bottom of the superconducting magnet in this susceptibility measuring apparatus. At this time, the levitation position of each sample in the z-axis direction is recorded on the scale, and the small scale is formed as described in the above embodiment.
ここで、χを試料の質量磁化率、μ0を真空の透磁率、B(z)を鉛直方向の位置zにおける磁束密度、dB(z)/dzを磁束密度の勾配、mを試料一粒の質量、gを重力加速度とすると、
(mχ/μ0)B(z)dB(z)/dz=mg (1)
と表すことができる。
Where χ is the mass magnetic susceptibility of the sample, μ 0 is the magnetic permeability of the vacuum, B (z) is the magnetic flux density at the position z in the vertical direction, dB (z) / dz is the gradient of the magnetic flux density, and m is the single grain of the sample. If the mass and g of gravitational acceleration are
(Mχ / μ 0 ) B (z) dB (z) / dz = mg (1)
It can be expressed as.
したがって、上記式(1)から各試料のχを求めることができる。この計算結果を上記表1に併せて示す。 Therefore, χ of each sample can be obtained from the above equation (1). The calculation results are also shown in Table 1 above.
また、上記各試料について、SQUIDでも磁化率を測定した。この結果も上記表1に示す。 Further, the magnetic susceptibility of each sample was also measured by SQUID. The results are also shown in Table 1 above.
表1からSQUIDで測定された磁化率と、本実施例に係る磁化率測定装置で測定された磁化率とで差異があることがわかるが、これは本実施例に係る磁化率測定装置において、浮揚位置zの測定精度又はB(z)dB(z)/dzの測定精度のために誤差が出たことが原因であると考えられる。したがって、SQUIDで測定された磁化率に値を補正する必要がある。なお、例えば最小二乗法などで各試料の浮揚位置と各試料に対応するSQUIDで測定された磁化率との比例関係における直線を作成し、この直線を用いて各目盛の値を決定すればよい。そうすることで、正確な又は正確な値に近似する磁化率の目盛を有した磁化率測定器及び磁化率測定装置となる。 It can be seen from Table 1 that there is a difference between the magnetic susceptibility measured by the SQUID and the magnetic susceptibility measured by the magnetic susceptibility measuring apparatus according to the present embodiment. This is considered to be caused by an error due to the measurement accuracy of the levitation position z or the measurement accuracy of B (z) dB (z) / dz. Therefore, it is necessary to correct the value to the magnetic susceptibility measured by SQUID. For example, a straight line in the proportional relationship between the levitation position of each sample and the magnetic susceptibility measured by the SQUID corresponding to each sample may be created by the least square method, and the value of each scale may be determined using this straight line. . By doing so, a magnetic susceptibility measuring device and a magnetic susceptibility measuring device having a susceptibility scale close to an accurate or accurate value are obtained.
なお、本発明は、特許請求の範囲を逸脱しない範囲で設計変更できるものであり、上記実施形態や実施例に限定されるものではない。例えば、CCDカメラを下向きにして、斜めにした反射鏡を介して試料を映し、レーザ光線によって試料の浮揚位置を測定し、磁化率測定器及び磁化率測定装置で使用される目盛を形成してもよい。 The present invention can be changed in design without departing from the scope of the claims, and is not limited to the above-described embodiments and examples. For example, with the CCD camera facing down, the sample is projected through an inclined reflector, the floating position of the sample is measured with a laser beam, and a scale used in a susceptibility measuring instrument and susceptibility measuring device is formed. Also good.
また、CCDカメラの代わりに顕微鏡などを使用したり、磁場強度や磁場勾配を変更したりすれば、細胞レベルの大きさのものでも磁化率を測定することが可能である。 Further, if a microscope or the like is used instead of the CCD camera, or the magnetic field strength or magnetic field gradient is changed, the magnetic susceptibility can be measured even with a cell level.
さらに、磁化率を測定したい試料の浮遊位置における磁場と磁場勾配の実測値(ガウスメーターなどの磁場測定器で測定)から上記(1)式により各試料の磁化率を求めてもよいし、磁化率を測定したい試料の浮遊位置における磁場と磁場勾配の計算値(シミュレーターなどで計算)から上記(1)式により各試料の磁化率を求めることとしてもよい。なお、これらの磁化率は、判明した反磁性材料の浮揚位置、磁場、磁場勾配の値からコンピュータによる演算を用いて求めてもよい。 Further, the magnetic susceptibility of each sample may be obtained by the above equation (1) from the measured values of magnetic field and magnetic field gradient (measured by a magnetic field measuring device such as a Gauss meter) at the floating position of the sample whose magnetic susceptibility is to be measured. The magnetic susceptibility of each sample may be obtained by the above equation (1) from the calculated value (calculated by a simulator or the like) of the magnetic field and magnetic field gradient at the floating position of the sample whose rate is to be measured. Note that these magnetic susceptibility values may be obtained by calculation using a computer from the levitation position, magnetic field, and magnetic field gradient value of the found diamagnetic material.
また、反磁性材料の浮揚位置の検出方法としては、様々なものあるが、次のような方法を使用してもよい。例えば、図2に示す磁化率測定装置20のように、CCDカメラ12で反射鏡13の映像を観測しながら反射鏡13を移動させ、超電導磁石11の磁場内で浮揚する反磁性材料である試料14の側面が反射鏡13の所定位置に映し出された位置を浮揚位置として検出する。他の方法としては、次のようなものがある。図3に示す磁化率測定装置30のように、超電導磁石21の上部から磁場内の反射鏡23bにレーザー光を入射させるとともに、CCDカメラ22で反射鏡23aの映像を観測しながら反射鏡23a及び反射鏡23bを上下方向かつ平行に同距離移動させる。そして、超電導磁石21の磁場内で浮揚している反磁性材料である試料24の側面にレーザー光が当たって散乱し、レーザー光強度が弱くなる位置を反射鏡23aでとらえ、これをCCDカメラ22で検出し、その位置を浮揚位置とする。なお、反射鏡13、23a、23bは、単なる鏡でもよいし、プリズムなどでもよい。
There are various methods for detecting the levitation position of the diamagnetic material, but the following method may be used. For example, like the magnetic
さらに、上記の反磁性材料の浮揚位置の各検出方法においては、CCDカメラ12やCCDカメラ22で捕らえた像を超電導磁石外に取り出して、ビデオレコーダーで録画し、反磁性材料の浮揚位置を確認することとしてもよい。
Furthermore, in each method of detecting the levitation position of the diamagnetic material, the image captured by the
1、11、21 超電導磁石
2 磁化率測定器
2a 棒部材
2b、12、22 CCDカメラ
2c 目盛
3 試料供給用部材
4、14、24 試料
5 (目盛2cの)基準
10、20、30 磁化率測定装置
13、23a、23b 反射鏡
DESCRIPTION OF
Claims (9)
浮揚した前記反磁性材料の各位置及び各磁化率から、前記磁場内における反磁性材料における磁化率と浮揚位置との関係を算出する工程と、
磁化率が判明していない反磁性材料を前記磁場内において浮揚させ、この浮揚した位置を特定し、算出された前記磁化率と浮揚位置との関係を用いて前記浮揚した位置を磁化率に変換する工程とを有する磁化率測定方法。 Levitation of a plurality of types of diamagnetic materials with known magnetic susceptibility, one by one or several simultaneously in a vertical magnetic field having a gradient magnetic field;
Calculating the relationship between the susceptibility and the levitation position of the diamagnetic material in the magnetic field from each position and each susceptibility of the levitated diamagnetic material;
A diamagnetic material whose magnetic susceptibility is unknown is levitated in the magnetic field, the levitated position is specified, and the levitated position is converted into a magnetic susceptibility using the calculated relationship between the magnetic susceptibility and the levitated position. And measuring the magnetic susceptibility.
前記反磁性材料の浮揚位置における磁場及び磁場勾配を、測定又は数値計算処理によって算出する工程と、
測定又は算出された前記磁場及び前記磁場勾配とを用いて前記反磁性材料の磁化率を算出する工程とを有する磁化率測定方法。 Levitating different types of diamagnetic materials in a vertical magnetic field with a gradient magnetic field;
Calculating the magnetic field and magnetic field gradient at the levitation position of the diamagnetic material by measurement or numerical calculation processing;
And a step of calculating a magnetic susceptibility of the diamagnetic material using the measured or calculated magnetic field and the magnetic field gradient.
浮揚した前記反磁性材料の各位置を記録して目盛とする工程と、
前記目盛を磁場と勾配磁場との積の値に対応するように分割し小目盛を作製する工程とを有していることを特徴とする磁化率測定用目盛の作製方法。 Levitation of a plurality of types of diamagnetic materials with known magnetic susceptibility, one by one or several simultaneously in a vertical magnetic field having a gradient magnetic field;
Recording each position of the levitated diamagnetic material to make a scale;
A method for producing a susceptibility measurement scale, comprising the step of dividing the scale so as to correspond to a product value of a magnetic field and a gradient magnetic field to produce a small scale.
前記所定位置から前記基準を移動させて、前記所定強度の鉛直方向磁場内における浮揚した反磁性材料の高さ位置に合わせた際、前記基準の前記所定位置からのずれ幅を前記目盛から読み取って磁化率を測定できる磁化率測定器。 It has a scale of magnetic susceptibility for diamagnetic material in a vertical magnetic field with a gradient magnetic field with respect to a predetermined position,
When the reference is moved from the predetermined position and adjusted to the height position of the levitated diamagnetic material in the vertical magnetic field having the predetermined intensity, the deviation width of the reference from the predetermined position is read from the scale. Magnetic susceptibility measuring instrument that can measure magnetic susceptibility.
前記磁場内で浮揚した反磁性材料の浮揚位置を検出する浮揚位置検出器と、
前記浮揚位置検出器で測定された前記浮揚位置の磁化率を算出する磁化率算出手段とを備えていることを特徴とする磁化率測定装置。 A superconducting magnet that generates a magnetic field in the vertical direction and a gradient magnetic field;
A levitation position detector for detecting a levitation position of a diamagnetic material levitated in the magnetic field;
A magnetic susceptibility measuring device comprising: a magnetic susceptibility calculating means for calculating a magnetic susceptibility at the floating position measured by the floating position detector.
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CN104007405A (en) * | 2014-05-19 | 2014-08-27 | 东北大学 | Magnetic susceptibility measuring device and method based on magneto-Archimedes levitation |
RU2680863C1 (en) * | 2018-05-15 | 2019-02-28 | Федеральное государственное бюджетное образовательное учреждение высшего образования "МИРЭА - Российский технологический университет" | Electromagnetic device for determining magnetic sensitivity of substance |
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CN104007405A (en) * | 2014-05-19 | 2014-08-27 | 东北大学 | Magnetic susceptibility measuring device and method based on magneto-Archimedes levitation |
RU2680863C1 (en) * | 2018-05-15 | 2019-02-28 | Федеральное государственное бюджетное образовательное учреждение высшего образования "МИРЭА - Российский технологический университет" | Electromagnetic device for determining magnetic sensitivity of substance |
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