JPH0318451B2 - - Google Patents

Info

Publication number
JPH0318451B2
JPH0318451B2 JP60072200A JP7220085A JPH0318451B2 JP H0318451 B2 JPH0318451 B2 JP H0318451B2 JP 60072200 A JP60072200 A JP 60072200A JP 7220085 A JP7220085 A JP 7220085A JP H0318451 B2 JPH0318451 B2 JP H0318451B2
Authority
JP
Japan
Prior art keywords
coil
conductor
cylindrical
winding
pattern
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
JP60072200A
Other languages
Japanese (ja)
Other versions
JPS61231444A (en
Inventor
Hiroshi Ikeda
Naoaki Yokoyama
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.)
Jeol Ltd
Original Assignee
Nihon Denshi KK
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 Nihon Denshi KK filed Critical Nihon Denshi KK
Priority to JP60072200A priority Critical patent/JPS61231444A/en
Publication of JPS61231444A publication Critical patent/JPS61231444A/en
Publication of JPH0318451B2 publication Critical patent/JPH0318451B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/28Details of apparatus provided for in groups G01R33/44 - G01R33/64
    • G01R33/32Excitation or detection systems, e.g. using radio frequency signals
    • G01R33/34Constructional details, e.g. resonators, specially adapted to MR
    • G01R33/343Constructional details, e.g. resonators, specially adapted to MR of slotted-tube or loop-gap type

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は核磁気共鳴装置(NMR装置)に用い
られるコイルに関し、特に製作が簡単で精度及び
感度の優れたコイルに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a coil used in a nuclear magnetic resonance apparatus (NMR apparatus), and particularly to a coil that is easy to manufacture and has excellent precision and sensitivity.

[従来技術] NMR装置では、試料を収容したプローブを一
様な静磁場内に配置し、プローブ内の試料に近接
して配置されたコイルから励起用高周波磁界を照
射すると共に、試料からの共鳴信号をこのコイル
によつて受信し、受信回路を介してコンピユータ
へ送り、フーリエ変換処理によりNMRスペクト
ルを得ている。その際、コイルの幾何学的対称性
及びコイルと試料の共鳴子との結合の良否が
NMR装置の感度を大きく左右するため、コイル
の製作精度及びコイルの形状、構造には大きな注
意が払われている。
[Prior art] In an NMR device, a probe containing a sample is placed in a uniform static magnetic field, and a high-frequency magnetic field for excitation is irradiated from a coil placed close to the sample in the probe, and resonance from the sample is emitted. A signal is received by this coil, sent to a computer via a receiving circuit, and an NMR spectrum is obtained by Fourier transform processing. At that time, the geometric symmetry of the coil and the quality of the coupling between the coil and the resonator of the sample are checked.
Great attention is paid to the manufacturing precision of the coil, as well as the shape and structure of the coil, as this greatly affects the sensitivity of the NMR device.

超伝導磁石を用いるNMR装置の場合、例えば
第4図に示すような円筒状の鞍形コイルが通常用
いられて来た。第4図の鞍形コイルは、試料を収
容した試料管が配置される半径Rの円筒状領域の
周囲に、2つの渦巻状巻線コイル部分1,2が円
筒軸Zの回りに対称に配置されている。この渦巻
状巻線コイル部分は、円筒軸Zに平行な直線状導
体部分1A,2Aと、円筒軸Zに直角な平面内に
ある円弧状部分1B,2Bとから成つている。
In the case of NMR devices using superconducting magnets, for example, a cylindrical saddle-shaped coil as shown in FIG. 4 has been commonly used. In the saddle-shaped coil shown in Fig. 4, two spirally wound coil parts 1 and 2 are arranged symmetrically around the cylindrical axis Z around a cylindrical region of radius R in which a sample tube containing a sample is arranged. has been done. This spirally wound coil portion consists of straight conductor portions 1A, 2A parallel to the cylindrical axis Z, and arcuate portions 1B, 2B lying in a plane perpendicular to the cylindrical axis Z.

従来、円筒ボビンの表面に円形断面の導体ワイ
ヤを巻きつけてこのようなコイルを製作している
が、ワイヤがずれやすいので製作精度の面で問題
がある。
Conventionally, such coils have been manufactured by winding a conductor wire with a circular cross section around the surface of a cylindrical bobbin, but this poses a problem in terms of manufacturing accuracy because the wire tends to shift.

第5図は特開昭57−147041号に提案されている
コイルの原形パターンを示す。この従来例では、
コイルパターンがプリント板上にプリント回路と
して製作されたり、導体薄板から幅広の平形導体
を押し抜いて製作されるため製作精度の面で優れ
ている。また、このように平形導体でコイルを作
つた場合、同じ断面積の円形断面の導体ワイヤで
作られたコイルに比べ表面積が大きいため表層を
流れる高周波電流に対する抵抗が小さくなりコイ
ルのQは格段に高くなるし、平形導体に流れる高
周波電流によつて作られる高周波磁界は導体面に
対し平行に走るため試料に照射する高周波磁界の
均一度も高くなるという優れた効果が得られる。
FIG. 5 shows the original pattern of the coil proposed in Japanese Patent Application Laid-Open No. 57-147041. In this conventional example,
The coil pattern is manufactured as a printed circuit on a printed board or by punching out a wide flat conductor from a thin conductor plate, so it has excellent manufacturing accuracy. In addition, when a coil is made from a flat conductor like this, the surface area is larger than a coil made from a conductor wire with a circular cross-section of the same cross-sectional area, so the resistance to high-frequency current flowing through the surface layer is small, and the Q of the coil is significantly increased. Since the high-frequency magnetic field created by the high-frequency current flowing through the flat conductor runs parallel to the conductor surface, the excellent effect of increasing the uniformity of the high-frequency magnetic field irradiated onto the sample can be obtained.

[発明が解決しようとする問題点] しかしながら、このような平形導体でコイルを
作る場合、所謂一筆書きのコイルパターンを導体
板から押し抜いたりあるいは切出したりしなけれ
ばならない関係上、コイルの巻き始め部S及び巻
き終り部Eをそのままコイル外部へ取出すことが
できず、外部回路に接続するための導線をS,E
部に半田付けしなければならなかつた。
[Problems to be Solved by the Invention] However, when making a coil using such a flat conductor, the so-called single-stroke coil pattern must be punched out or cut out from the conductor plate, so it is difficult to start winding the coil. The part S and the winding end part E cannot be taken out of the coil as they are, and the conductor wires for connecting to the external circuit are connected to S and E.
I had to solder the parts.

このように、外部回路との接続をコイル巻線内
で行うことは、信号検出面で不利となるばかりで
なく、コイル製作面でも慎重な配慮が必要になる
という問題がある。
In this way, connecting to an external circuit within the coil winding is not only disadvantageous in terms of signal detection, but also requires careful consideration in manufacturing the coil.

本発明はこの点に鑑みてなされたものであり、
製作が簡単で精度及び感度の優れたコイルを提供
することを目的としている。
The present invention has been made in view of this point,
The purpose is to provide a coil that is easy to manufacture and has excellent precision and sensitivity.

[問題点を解決するための手段] この目的を達成するため、本発明にかかる
NMR装置用コイルは、導体の薄板から切出した
一筆書きコイルパターンを所定の折り線に沿つて
180゜折り返すと共に、巻き始め部と巻き終り部が
コイルの外部に存在するようにされたコイルを円
筒状の鞍型コイルに成型したことを特徴としてい
る。
[Means for solving the problem] In order to achieve this objective, the present invention
Coils for NMR devices are made by cutting out a single-stroke coil pattern from a thin conductor plate along a predetermined fold line.
It is characterized by being folded back 180 degrees and formed into a cylindrical saddle-shaped coil with the winding start and winding ends located outside the coil.

[実施例] 以下、図面を用いて本発明の一実施例を詳述す
る。
[Example] Hereinafter, an example of the present invention will be described in detail using the drawings.

第1図aは本発明にかかる2ターンのNMR装
置用コイルの原形パターンであり、導体薄板から
の押し抜きあるいは切出しによつて作成される。
このパターン中の1A,2Aが直線状導体、1
B,2Bが円弧状導体に相当する。
FIG. 1a shows the original pattern of a two-turn coil for an NMR apparatus according to the present invention, which is produced by punching or cutting out a thin conductive plate.
1A and 2A in this pattern are straight conductors, 1
B and 2B correspond to arc-shaped conductors.

第1図bは、このコイルパターンを折り線Lで
2つ折りにした時の状態を示す。折返しにより上
下の導体が接触する部分には、間に絶縁フイルム
Fを挿入し絶縁を図つている。
FIG. 1b shows the state when this coil pattern is folded in half along the fold line L. An insulating film F is inserted between the parts where the upper and lower conductors come into contact with each other due to the folding, thereby providing insulation.

第1図cは更に円筒ボビン3に巻きつけて固定
しコイルに成型した時の状態を示す。コイルに成
型した時に渦巻状巻線部分1,2が対称になるよ
う、このボビンの径R及び高さに合わせてパター
ンの寸法l1〜l3が決められることは言うまでもな
い。
FIG. 1c shows the state when the coil is further wound around the cylindrical bobbin 3, fixed, and formed into a coil. Needless to say, the dimensions l 1 to l 3 of the pattern are determined according to the diameter R and height of the bobbin so that the spiral winding portions 1 and 2 are symmetrical when formed into a coil.

このようにして作成した本発明のコイルでは、
コイルが1つの連続した平形導体で形成され、し
かもコイル巻き始め部Sと巻き終り部Eがコイル
の外に出るため、コイル内にS,E部があつた従
来に比べ信号検出面での不利はなく、製作も簡単
である。
In the coil of the present invention created in this way,
Since the coil is formed from one continuous flat conductor, and the coil winding start part S and winding end part E are outside the coil, it is disadvantageous in terms of signal detection compared to the conventional method where parts S and E were inside the coil. It is easy to manufacture.

第2図aは本発明にかかる3ターンのコイルの
原形パターンであり、これを折り線L1で折返せ
ば第2図bの状態になり、更に引出し部分4のみ
を折り線L2で折返せば第2図cの状態となる。
そして更に円筒ボビンに巻きつけて円筒状に成型
すれば3ターンのコイルとなる。尚、円弧状導体
1Bには円弧状導体2Bが占める幅に見合つた幅
が与えられており、導体の分布の対称化を図り、
静磁場の均一度低下を防いでいる。
Figure 2a shows the original pattern of the 3-turn coil according to the present invention, and if this is folded back along the fold line L1 , the state shown in Figure 2b will be obtained.Furthermore, only the drawer portion 4 can be folded along the fold line L2 . If it is returned, it will be in the state shown in Figure 2c.
Then, if it is further wound around a cylindrical bobbin and formed into a cylindrical shape, it becomes a three-turn coil. Incidentally, the arc-shaped conductor 1B is given a width commensurate with the width occupied by the arc-shaped conductor 2B, and the distribution of the conductor is made symmetrical.
This prevents a decrease in the uniformity of the static magnetic field.

第3図aは同じく4ターンのコイルの原形パタ
ーンであり、これを折り線L1で折返せば第3図
bの状態になり、更に引出し部分4のみを折り線
L2で折返せば第3図cの状態となる。そして更
に円筒ボビンに巻きつけて円筒状に成型すれば4
ターンのコイルとなる。
Figure 3a shows the original pattern of the same 4-turn coil, and if you fold it back along the fold line L1 , you will get the state shown in Figure 3b.
If you turn around at L 2 , you will be in the situation shown in Figure 3c. Then, if you wrap it around a cylindrical bobbin and form it into a cylindrical shape, 4
It becomes a coil of turns.

尚、第2図及び第3図の実施例においても、上
下の導体が接触する部分には絶縁フイルムFが挿
入されている。
In the embodiments shown in FIGS. 2 and 3, an insulating film F is also inserted in the portion where the upper and lower conductors come into contact.

又、上述した実施例ではコイルを円筒ボビンに
巻きつけて固定したが、平形導体の強度が十分あ
ればコイル自体で自身を支えるようにすれば良
く、ボビン等の支持体は必ずしも必要ではない。
Further, in the above-described embodiments, the coil is wound around a cylindrical bobbin and fixed, but as long as the flat conductor has sufficient strength, the coil itself can support itself, and a support such as a bobbin is not necessarily necessary.

[発明の効果] 以上詳述した如く、本発明によれば、製作が簡
単で精度及び感度の優れたコイルが提供される。
[Effects of the Invention] As detailed above, according to the present invention, a coil that is easy to manufacture and has excellent precision and sensitivity is provided.

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

第1図、第2図、第3図は夫々本発明を実施し
たNMR装置用コイルの一例を示す図、第4図は
従来の円筒状の鞍形コイルを示す図、第5図は特
開昭57−147041号に提案されているコイルの原形
パターンを示す図である。 1,2:渦巻状巻線コイル部分、1A,2A:
直線状導体部分、1B,2B:円弧状導体部分、
3:ボビン、4:引出し部分、L1,L2:折り線、
F:絶縁フイルム。
Figures 1, 2, and 3 each show an example of a coil for an NMR device embodying the present invention, Figure 4 shows a conventional cylindrical saddle-shaped coil, and Figure 5 shows the It is a figure showing the original pattern of the coil proposed in No. 57-147041. 1, 2: Spiral winding coil part, 1A, 2A:
Straight conductor part, 1B, 2B: arcuate conductor part,
3: Bobbin, 4: Drawer part, L 1 , L 2 : Folding line,
F: Insulating film.

Claims (1)

【特許請求の範囲】[Claims] 1 導体の薄板から切出した一筆書きコイルパタ
ーンを所定の折り線に沿つて180゜折り返すと共
に、巻き始め部と巻き終り部がコイルの外部に存
在するようにされたコイルを円筒状の鞍型コイル
に成型してなるNMR装置用コイル。
1 A single-stroke coil pattern cut from a thin conductor plate is folded back 180 degrees along a predetermined fold line, and the coil is made into a cylindrical saddle-shaped coil with the winding start and winding ends located outside the coil. A coil for NMR equipment formed by molding.
JP60072200A 1985-04-05 1985-04-05 Coil for nmr apparatus Granted JPS61231444A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60072200A JPS61231444A (en) 1985-04-05 1985-04-05 Coil for nmr apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60072200A JPS61231444A (en) 1985-04-05 1985-04-05 Coil for nmr apparatus

Publications (2)

Publication Number Publication Date
JPS61231444A JPS61231444A (en) 1986-10-15
JPH0318451B2 true JPH0318451B2 (en) 1991-03-12

Family

ID=13482352

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60072200A Granted JPS61231444A (en) 1985-04-05 1985-04-05 Coil for nmr apparatus

Country Status (1)

Country Link
JP (1) JPS61231444A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5084311A (en) * 1988-12-28 1992-01-28 General Electric Company Electromagnetic transducers and method of making them
JP5156190B2 (en) * 2005-12-21 2013-03-06 株式会社 Jeol Resonance Combined cylindrical coil for NMR

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4439733A (en) * 1980-08-29 1984-03-27 Technicare Corporation Distributed phase RF coil
JPS57147071A (en) * 1981-03-06 1982-09-10 Toshiba Corp Detection system for minute ground fault
JPS6172665U (en) * 1984-10-18 1986-05-17

Also Published As

Publication number Publication date
JPS61231444A (en) 1986-10-15

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