JPH0621031Y2 - Superconducting magnetometer - Google Patents

Superconducting magnetometer

Info

Publication number
JPH0621031Y2
JPH0621031Y2 JP1986070148U JP7014886U JPH0621031Y2 JP H0621031 Y2 JPH0621031 Y2 JP H0621031Y2 JP 1986070148 U JP1986070148 U JP 1986070148U JP 7014886 U JP7014886 U JP 7014886U JP H0621031 Y2 JPH0621031 Y2 JP H0621031Y2
Authority
JP
Japan
Prior art keywords
pickup coil
inner tank
center line
superconducting
skid element
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
JP1986070148U
Other languages
Japanese (ja)
Other versions
JPS62182475U (en
Inventor
康晴 山田
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.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
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 Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP1986070148U priority Critical patent/JPH0621031Y2/en
Publication of JPS62182475U publication Critical patent/JPS62182475U/ja
Application granted granted Critical
Publication of JPH0621031Y2 publication Critical patent/JPH0621031Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】 (イ)産業上の利用分野 この考案は、超伝導磁力計(スキッド磁力計)、特にス
キッド素子とピックアップコイルの接続機構に特徴を有
する超伝導磁力計に関する。
DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a superconducting magnetometer (skid magnetometer), and more particularly to a superconducting magnetometer characterized by a connection mechanism between a skid element and a pickup coil.

(ロ)従来の技術 一般に、超伝導磁力計は、極低温容器中に収容されたス
キッド素子とピックアップコイルからなる検出部で微小
磁気を検出するものである。この種の超伝導磁力計のス
キッド素子は、第4図に示すように、入力コイル2、J
J素子3、タンク回路4から構成されている。そしてこ
のスキッド素子1の入力コイル2は、2本の細線からな
る接続線6によってピックアップコイル7に接続されて
いる。従来、接続線6は、インダクタンス分を小さくす
るために、第5図に示すように2本の細線6a、6bが
ねじり合わされている。さらに、外部磁気の侵入を防ぐ
ために、接続線6が超伝導シールドパイプ8で覆われて
いる。
(B) Conventional Technology In general, a superconducting magnetometer detects micro magnetism with a detection unit which is housed in a cryogenic container and includes a skid element and a pickup coil. As shown in FIG. 4, the skid element of this type of superconducting magnetometer has an input coil 2, J
It is composed of a J element 3 and a tank circuit 4. The input coil 2 of the skid element 1 is connected to the pickup coil 7 by a connecting wire 6 composed of two thin wires. Conventionally, in the connecting wire 6, two thin wires 6a and 6b are twisted together as shown in FIG. 5 in order to reduce the inductance. Further, the connecting wire 6 is covered with a superconducting shield pipe 8 in order to prevent invasion of external magnetism.

(ハ)考案が解決しようとする問題点 上記従来の超伝導磁力計では、スキッド素子とピックア
ップコイルを接続するのに2本の細線をねじり合わせて
いるので、線間の絶縁被覆がはがれ、時として絶縁不良
が生じ、ピックアップコイルからの信号がスキッド素子
の入力コイルに伝達されないことがあるという問題があ
った。
(C) Problems to be solved by the device In the above conventional superconducting magnetometer, two thin wires are twisted together to connect the skid element and the pickup coil. As a result, there is a problem that a signal from the pickup coil may not be transmitted to the input coil of the skid element due to insulation failure.

また、ピックアップコイルを出来るだけ被検知物体に近
づけ、磁力計の感度を上げようとして、ピックアップコ
イルをFRPで構成される内槽外に設置しようとする
と、シールドパイプと接続線間の空間より内槽中の寒剤
(液体ヘリウム)の漏れが生じ、内槽と外槽間の真空度
を劣化させるという問題があった。
Also, if the pickup coil is placed as close as possible to the object to be detected and the pickup coil is to be installed outside the inner tank composed of the FRP in order to increase the sensitivity of the magnetometer, the inner tank will be removed from the space between the shield pipe and the connecting line. There was a problem that the cryogen (liquid helium) in the inside leaked and the degree of vacuum between the inner tank and the outer tank was deteriorated.

この考案は、上記に鑑み、インダクタンスが小さくて、
しかも線間の接触が生じない、さらには必要により寒剤
の漏れが生じないスキッド素子とピックアップコイルの
接続機構を有する超伝導磁力計を提供することを目的と
している。
In consideration of the above, this device has a small inductance,
Moreover, it is an object of the present invention to provide a superconducting magnetometer having a connection mechanism between a skid element and a pickup coil in which contact between wires does not occur and, if necessary, cryogen does not leak.

(ニ)問題点を解決するための手段及び作用 この考案の超伝導磁力計は、内槽と外槽とからなる極低
温容器に、スキッド素子及びピックアップコイルが収納
されるものにおいて、前記内槽内に寒剤を入れ、この寒
剤中にスキッド素子を配置するとともに、前記ピックア
ップコイルを前記内槽と外槽の間の底部に配置し、超伝
導材からなる中心線と、この中心線を囲む超伝導材から
なる同軸筒材と、この中心線と同軸筒材間に充填した低
温モールド材からなる接続線を、内槽壁底部に貫装し、
この接続線でスキッド素子とピックアップコイルを接続
している。
(D) Means and Actions for Solving Problems The superconducting magnetometer of the present invention is a cryogenic container comprising an inner tank and an outer tank, in which a skid element and a pickup coil are housed. A cryogen is placed inside, a skid element is placed in the cryogen, and the pickup coil is placed at the bottom between the inner tank and the outer tank. A coaxial tubular material made of a conductive material and a connecting wire made of a low temperature molding material filled between the center line and the coaxial tubular material are penetrated into the bottom of the inner tank wall,
This connection line connects the skid element and the pickup coil.

この接続機構では、中心線及び同軸筒材とも超伝導体で
構成されるものであるから、外部からの磁気ノイズの侵
入が防止され、また、接続線をねじり合わせなくてもイ
ンダクタンスを小さくできるので、接続線の絶縁不良の
発生を回避できる。また、中心線と同軸筒間にモールド
材を充填しているので、内槽から外槽に、寒剤が漏れる
ことはない。
In this connection mechanism, since the center line and the coaxial tubular member are both made of a superconductor, magnetic noise is prevented from entering from the outside, and the inductance can be reduced without twisting the connection lines. It is possible to avoid the occurrence of insulation failure of the connection line. Further, since the molding material is filled between the center line and the coaxial cylinder, the cryogen does not leak from the inner tank to the outer tank.

(ホ)実施例 以下、実施例により、この考案をさに詳細に説明する。(E) Embodiment Hereinafter, the present invention will be described in detail with reference to an embodiment.

第2図は、この考案の一実施例を示す超伝導磁力計の極
低温容器の断面図である。
FIG. 2 is a sectional view of a cryogenic container of a superconducting magnetometer showing an embodiment of the present invention.

この極低温容器11は、外槽12と内槽13の二重構造
であり、外槽壁14、内槽壁15はいずれもFRP(ガ
ラス繊維強化プラスチック)で構成されている。内槽1
3内には液体ヘリウム16が満たされ、さらにスキッド
素子17が収納されている。また、外槽12は真空に保
たれ、検出感度を上げるため、つまり出来るだけ被検知
物体に近づけるため、ピックアップコイル18がスキッ
ド素子17の下方の槽12内に配設されている。
The cryogenic container 11 has a double structure of an outer tank 12 and an inner tank 13, and both the outer tank wall 14 and the inner tank wall 15 are made of FRP (glass fiber reinforced plastic). Inner tank 1
Liquid helium 16 is filled in the chamber 3, and a skid element 17 is housed therein. Further, the outer tank 12 is kept in a vacuum, and a pickup coil 18 is disposed in the tank 12 below the skid element 17 in order to increase detection sensitivity, that is, to bring the object to be detected as close as possible.

スキッド素子17の内部回路は、第4図のものと同様で
あり、このスキッド素子17の入力コイル18は、内槽
壁15に貫装される接続線19によって接続されてい
る。
The internal circuit of the skid element 17 is similar to that shown in FIG. 4, and the input coil 18 of this skid element 17 is connected by a connecting wire 19 penetrating the inner tank wall 15.

接続線19は、第1図に拡大図を示すように、中心線2
0と、この中心線20から離隔して同軸に設けられる同
軸円筒体21と、中心線20と同軸円筒体21間に充填
されるスタイキャスト等の低温モールド材22とから構
成されている。中心線20及び同軸円筒体21は、いず
れもニオブ等の超伝導材で構成されている。また、中心
線20の上下両端に、同軸円筒体21と同径の頂部20
a、20aが設けられている。この接続線19の上端で
入力コイルの2線が中心線20と同軸円筒体21に接続
され、下端でピックアップコイル18の2線が中心線2
0と同軸円筒体21に接続されている。
The connecting line 19 has a center line 2 as shown in the enlarged view of FIG.
0, a coaxial cylindrical body 21 provided coaxially with being separated from the center line 20, and a low temperature molding material 22 such as stycast which is filled between the center line 20 and the coaxial cylindrical body 21. The center line 20 and the coaxial cylinder 21 are both made of a superconducting material such as niobium. In addition, the top 20 having the same diameter as the coaxial cylindrical body 21 is provided at both upper and lower ends of the center line 20.
a and 20a are provided. Two lines of the input coil are connected to the center line 20 and the coaxial cylindrical body 21 at the upper end of the connection line 19, and two lines of the pickup coil 18 are connected to the center line 2 at the lower end.
0 and the coaxial cylindrical body 21.

今、ピックアップコイル18に磁束Φxが入ると、ピッ
クアップコイル18のインダクタンスをLp、入力コイ
ルのインダクタンスをLin、接続線19のインダクタン
スLdとすると、ピックアップコイル18にこれらイン
ダクタンスに反比例する遮蔽電流i=Φx/(Lp+Ld+Lin) が誘起される。この遮蔽電流iが入力コイルを流れる
ことにより、磁束Φsが発生し、スキッド素子17に伝
達される。
Now, when the magnetic flux Φx enters the pickup coil 18, the inductance of the pickup coil 18 Lp, Lin inductance of the input coil, the inductance Ld of the connection line 19, the shielding current i s i which is inversely proportional to these inductance pickup coil 18 s = Φx / (Lp + Ld + Lin) is induced. By flowing through the shielding current i s is the input coil, the magnetic flux Φs is generated and transmitted to the skid elements 17.

一般には、外部磁束Φxはピックアップコイル18のみ
に入ることが望ましいが、接続線部や入力コイル部に外
部磁束が入ると、遮蔽電流is′は、 is′=i+Δi =Φx/(Lp+Ld+Lin)+ΔΦx/(Lp+Ld+Lin) となり、誤差信号Δiが発生することになる。
In general, the external magnetic flux [Phi] x is desirably enters only the pickup coil 18, the external magnetic flux entering the connecting line section and the input coil unit, shielding current is 'is, is' = i s + Δi s = Φx / (Lp + Ld + Lin) + ΔΦx / (Lp + Ld + Lin) becomes, so that the error signal .DELTA.i s is generated.

しかるに、この実施例超伝導磁力計では、接続線19が
中心線20と同軸円筒体21からなり、しかも超伝導材
が使用されているので、外部磁気ノイズの侵入を防ぐこ
とができる。そのためΔiの如き誘起電流が発生せ
ず、誤差が小さく抑えられる。また、中心線20と同軸
円筒体21間に低温モールド材22が充填されているた
め、内槽13内の流体ヘリウム16が外槽12に漏れ出
すこともない。なお、内槽13内の極低温は、接続線1
9を通してピックアップコイル18に伝達されるので、
ピックアップコイル18は所要の低温に保つことができ
る。
However, in the superconducting magnetometer of this embodiment, since the connecting line 19 is composed of the center line 20 and the coaxial cylindrical body 21 and the superconducting material is used, the intrusion of external magnetic noise can be prevented. Therefore no induced current is generated such as .DELTA.i s, errors can be suppressed small. Further, since the low temperature molding material 22 is filled between the center line 20 and the coaxial cylindrical body 21, the fluid helium 16 in the inner tank 13 does not leak to the outer tank 12. In addition, the cryogenic temperature in the inner tank 13 is the same as the connection line 1
Since it is transmitted to the pickup coil 18 through 9,
The pickup coil 18 can be kept at a required low temperature.

(ヘ)考案の効果 以上のように、この考案によれば、スキッド素子とピッ
クアップコイルを接続するのに、超伝導材で構成される
中心線と同軸筒体からなる接続線を用いるものであるか
ら、従来のように細線のねじり合わせを行うものではな
く、線間短絡のおそれがない上、超伝導材によって外部
磁気ノズルが遮断されるので、その分、誤差を軽減でき
る。また、ピックアップコイルを内槽の外に配置するの
で、中心線と同軸筒体間に低温モールド材を充填するこ
とにより、液漏れを防止することも可能である。
(F) Effect of the Invention As described above, according to this invention, the connecting line composed of the center line made of the superconducting material and the coaxial cylinder is used to connect the skid element and the pickup coil. Therefore, unlike the conventional method, twisting of thin wires is not performed, and there is no risk of short-circuiting between wires, and since the external magnetic nozzle is blocked by the superconducting material, the error can be reduced accordingly. Further, since the pickup coil is arranged outside the inner tank, it is possible to prevent liquid leakage by filling the low temperature molding material between the center line and the coaxial cylinder.

【図面の簡単な説明】 第1図は、この考案の一実施例超伝導磁力計の要部であ
る接続線部の拡大図、第2図は、同超伝導磁力計の極低
温容器の断面図、第3図は、スキッド素子の内部回路を
示す図、第4図は、従来例を説明するための図である。 17:スキッド素子、 18:ピックアップコイル、 19:接続線、20:中心線、 21:同軸円筒体、22:低温モールド材。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is an enlarged view of a connecting line portion which is a main part of a superconducting magnetometer according to an embodiment of the present invention, and FIG. 2 is a cross section of a cryogenic container of the superconducting magnetometer. FIG. 3 is a diagram showing an internal circuit of the skid element, and FIG. 4 is a diagram for explaining a conventional example. 17: skid element, 18: pickup coil, 19: connection line, 20: center line, 21: coaxial cylindrical body, 22: low temperature molding material.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】内槽と外槽とからなる極低温容器に、スキ
ッド素子及びピックアップコイルが収納される超伝導磁
力計において、 前記内槽内に寒剤を入れ、この寒剤中にスキッド素子を
配置するとともに、前記ピックアップコイルを前記内槽
と外槽の間の底部に配置し、超伝導材からなる中心線
と、この中心線を囲む超伝導材からなる同軸筒材と、こ
の中心線と同軸筒材間に充填した低温モールド材からな
る接続線を、内槽壁底部に貫装し、この接続線でスキッ
ド素子とピックアップコイルを接続するようにしたこと
を特徴とする超伝導磁力計。
1. A superconducting magnetometer in which a skid element and a pickup coil are housed in a cryogenic container consisting of an inner tank and an outer tank. A cryogen is placed in the inner tank, and the skid element is placed in the cryogen. In addition, the pickup coil is arranged at the bottom between the inner tank and the outer tank, and a center line made of a superconducting material, a coaxial cylindrical member made of a superconducting material surrounding the center line, and a coaxial line with the center line. A superconducting magnetometer characterized in that a connecting wire made of a low-temperature mold material filled between tubular materials is penetrated into the bottom of the inner tank wall, and the skid element and the pickup coil are connected by this connecting wire.
JP1986070148U 1986-05-09 1986-05-09 Superconducting magnetometer Expired - Lifetime JPH0621031Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1986070148U JPH0621031Y2 (en) 1986-05-09 1986-05-09 Superconducting magnetometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1986070148U JPH0621031Y2 (en) 1986-05-09 1986-05-09 Superconducting magnetometer

Publications (2)

Publication Number Publication Date
JPS62182475U JPS62182475U (en) 1987-11-19
JPH0621031Y2 true JPH0621031Y2 (en) 1994-06-01

Family

ID=30911517

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1986070148U Expired - Lifetime JPH0621031Y2 (en) 1986-05-09 1986-05-09 Superconducting magnetometer

Country Status (1)

Country Link
JP (1) JPH0621031Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2624828B2 (en) * 1988-04-06 1997-06-25 株式会社日立製作所 Magnetometer and method for detecting deterioration of metal material using the same

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50114587A (en) * 1974-02-26 1975-09-08
JPS55131784A (en) * 1979-03-30 1980-10-13 Shimadzu Corp Magnetism measuring apparatus
JP2501311B2 (en) * 1983-08-17 1996-05-29 株式会社東芝 Active low-pass filter

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
「ジョセフソン効果基礎と応用」電気学会p.74−75

Also Published As

Publication number Publication date
JPS62182475U (en) 1987-11-19

Similar Documents

Publication Publication Date Title
JP3663266B2 (en) Open magnetic resonance imaging magnet
US7126343B1 (en) Conductivity probe with toroid keeper
EP0375656A2 (en) Cryogenic vessel for a superconducting apparatus
CN106683819A (en) Magnet device
JPH0621031Y2 (en) Superconducting magnetometer
US6289681B1 (en) Superconducting magnet split cryostat interconnect assembly
US4707676A (en) Superconducting magnet
JPS62264683A (en) Current lead for superconductive equipment
US5349291A (en) Superconducting magnetic sensor having a cryostat for improved sensitivity of magnetic detection
US5053706A (en) Compact low-distortion squid magnetometer
JPS60173883A (en) Superconductive magnet
US6667676B2 (en) Superconducting magnet and magnetic resonance imaging apparatus using the same
CN114675224A (en) Testing device and testing method for superconducting quantum interference device
US6358888B1 (en) Shielded superconducting magnet joints
JP4056967B2 (en) Nuclear magnetic resonance apparatus
JP2016178779A (en) Terminal connection part for cryogenic cable
JPH0785905A (en) Bushing device for superconducting device
JP3021970B2 (en) Functional superconducting magnetic shield and magnetometer using the same
JPH08220201A (en) Superconducting quantum interferometer
JPH0750716Y2 (en) Biomagnetic measurement device
JPH05126297A (en) Cryostat
JPS63138710A (en) Cryogenic temperature container
JPS58210683A (en) Differentiation type squid
JPS6244550Y2 (en)
JPS607374A (en) Magnetic flux measuring sensor