JPS6345549A - Coil for nmr - Google Patents
Coil for nmrInfo
- Publication number
- JPS6345549A JPS6345549A JP61190278A JP19027886A JPS6345549A JP S6345549 A JPS6345549 A JP S6345549A JP 61190278 A JP61190278 A JP 61190278A JP 19027886 A JP19027886 A JP 19027886A JP S6345549 A JPS6345549 A JP S6345549A
- Authority
- JP
- Japan
- Prior art keywords
- coil
- coils
- nmr
- arc
- bobbins
- 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.)
- Granted
Links
- 238000005481 NMR spectroscopy Methods 0.000 abstract description 27
- 230000008878 coupling Effects 0.000 abstract description 10
- 238000010168 coupling process Methods 0.000 abstract description 10
- 238000005859 coupling reaction Methods 0.000 abstract description 10
- 238000010586 diagram Methods 0.000 description 8
- 230000035945 sensitivity Effects 0.000 description 4
- 230000003068 static effect Effects 0.000 description 3
- 230000004888 barrier function Effects 0.000 description 2
- 239000000919 ceramic Substances 0.000 description 2
- 238000001514 detection method Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 239000004020 conductor Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000002861 polymer material Substances 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
Landscapes
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、サンプルが装填される円筒空間の外周に2組
のコイルを同心円筒上に配置してなるNMR(核磁気共
鳴)用コイルに関する。Detailed Description of the Invention [Field of Industrial Application] The present invention relates to an NMR (nuclear magnetic resonance) coil comprising two sets of coils arranged on a concentric cylinder around the outer periphery of a cylindrical space into which a sample is loaded. .
第4図はNMR用コイルの構成例を示す図、第5図は従
来のNMR用コイルの形状例を示す図である0図中、1
1と12はコイル、13は観測用端子、14は照射用端
子、15はロック用端子、16と17はボビンを示す。Fig. 4 is a diagram showing an example of the configuration of an NMR coil, and Fig. 5 is a diagram showing an example of the shape of a conventional NMR coil.
1 and 12 are coils, 13 is an observation terminal, 14 is an irradiation terminal, 15 is a lock terminal, and 16 and 17 are bobbins.
核スピン系を外部静磁場H0の中におくと、核磁化M、
は、静磁場H0の周りに
ω・−γH0・・・・・・ (1)
のラーモア周波数で歳差運動する。ここで、Tは磁気角
運動量比と呼ばれ、それぞれの磁性核に固有な定数であ
る。NMR(核磁気共鳴)では、このラーモア周波数と
同じ周波数で静磁場H0に垂直な面内で回転する高周波
磁場(ラジオ波)を加えると、共鳴が起こりて高周波磁
場からエネルギーが吸収される。そこで、NMR装置で
は、−4磁場内にサンプルをおき、RF発振器からNM
R用コイルに共鳴周波数を与えて高周波磁場を発生させ
、共鳴によって吸収されるエネルギーを横比する。When a nuclear spin system is placed in an external static magnetic field H0, the nuclear magnetization M,
precesses around the static magnetic field H0 at the Larmor frequency of ω・−γH0 (1). Here, T is called the magnetic angular momentum ratio and is a constant specific to each magnetic nucleus. In NMR (nuclear magnetic resonance), when a high frequency magnetic field (radio wave) rotating in a plane perpendicular to the static magnetic field H0 at the same frequency as the Larmor frequency is applied, resonance occurs and energy is absorbed from the high frequency magnetic field. Therefore, in an NMR device, the sample is placed in a -4 magnetic field, and the NM
A resonance frequency is given to the R coil to generate a high frequency magnetic field, and the energy absorbed by resonance is compared horizontally.
NMR装置では、第4図に示すようにNMR用コイルと
して2つのコイル11及びコイル12を備えている。そ
して、それぞれコイル11を観測用として観測用端子1
3に接続し、コイル12を高周波磁場の照射用とNMR
ロック用として照射用端子14及びロック用端子15に
接続している。The NMR apparatus is equipped with two coils 11 and 12 as NMR coils, as shown in FIG. Then, each coil 11 is used as an observation terminal 1 for observation.
3, and the coil 12 is used for high frequency magnetic field irradiation and for NMR.
It is connected to the irradiation terminal 14 and the locking terminal 15 for locking.
このN M R用コイルは、第5図に示すように相互に
適度な距離を保つようにして同心円筒のボビン16.1
7を配置し、これらにRF[界の方向が直交する(円筒
空間の輪方向をZ軸、円筒空間の断面をXY平面とする
と、コイル11のRF[界をX方向、コイル12のRF
I界をY方向とする)ようにそれぞれのコイル11及び
コイル12を配置している。The NMR coils are connected to a concentric cylindrical bobbin 16.1 while keeping an appropriate distance from each other as shown in FIG.
7, and the direction of the RF [field is perpendicular to these (assuming that the ring direction of the cylindrical space is the Z axis and the cross section of the cylindrical space is the XY plane), the RF [field of the coil 11 is in the
The coils 11 and 12 are arranged so that the I field is in the Y direction.
また、図示しないが、NMR用コイルの形状として第5
図に示すボビン16.17を共通にしてその内側と外側
にそれぞれコイル11及びコイル12を配置するものも
ある。Although not shown, there is also a fifth shape of the NMR coil.
Some coils 11 and 12 are arranged on the inside and outside of a common bobbin 16, 17 shown in the figure, respectively.
NMR共鳴信号は、サンプルに近ければそれだけ強い信
号が検出できる。しかし、基本的な形状としてヘルムホ
ルツ(馬蹄)型を採用しているため、コイル11とコイ
ル12とをあまり近接して配置すると、第5図(blか
ら明らかなように円筒断面に沿って配置される円弧形の
アークコイル部では、相互の電磁結合がかなり強くなっ
てしまうため、最も重視される観測側の共鳴信号がコイ
ル12に吸収され、感度低下をもたらすという問題が生
じる。The closer the NMR resonance signal is to the sample, the stronger the signal can be detected. However, since a Helmholtz (horseshoe) shape is adopted as the basic shape, if the coils 11 and 12 are placed too close to each other, they will be placed along the cylindrical cross section as shown in Fig. 5 (bl). Since mutual electromagnetic coupling becomes considerably strong in the arc-shaped arc coil portion, a problem arises in that the resonance signal on the observation side, which is most important, is absorbed by the coil 12, resulting in a decrease in sensitivity.
そこで従来は、第5図に示すようにボビン16と17と
の径の差を大きくすることによって前記の問題の改善を
圀っている。しかし、この場合、相互に離す距離が無視
できなくなる。なぜなら、コイル11とコイル12との
間で相互に離す距離を大きくすればするほどコイル12
により検出される共鳴信号の強度が弱まり、照射、NM
Rt:lツクの効率低下を引き起こし前記とは別の問題
が生じる。従って、この距離は、橿端に太き(とれない
。Conventionally, this problem has been solved by increasing the difference in diameter between the bobbins 16 and 17, as shown in FIG. However, in this case, the distance between them cannot be ignored. This is because the larger the distance between the coils 11 and 12, the more the coils 12
The intensity of the resonance signal detected by the irradiation, NM
This causes a decrease in the efficiency of the Rt:l block and causes a problem different from the above. Therefore, this distance is thick (cannot be taken) at the end of the rod.
本発明は、上記の問題点を解決するものであって、コイ
ル11及びコイル12のアークコイル部における相互の
電磁結合をなくし、相互に近接配置できるNMR用コイ
ルを提供することを目的とするものである。The present invention solves the above-mentioned problems, and aims to provide an NMR coil that eliminates mutual electromagnetic coupling in the arc coil portions of the coils 11 and 12 and can be arranged close to each other. It is.
そのために本発明のNMR用コイルは、サンプルが装填
される円筒空間の外周に、円弧形のアークコイル部と紬
に平行な軸方同コイル部とにより構成される2組のコイ
ルを同心円筒上に配置してなるNMR用コイルにおいて
、前記2&llのコイルのアークコイル部間にシールド
環を挟み込むように配置したことを特徴とするものであ
る。To this end, the NMR coil of the present invention has two sets of coils, each consisting of an arc-shaped arc coil part and an axial co-coil part parallel to the pongee, arranged in a concentric cylinder around the outer periphery of a cylindrical space in which a sample is loaded. The NMR coil disposed above is characterized in that a shield ring is disposed between the arc coil portions of the 2&ll coils.
本発明のNMR用コイルでは、シールド環が2組のコイ
ルのアークコイル部間に挟み込まれるので、両コイルを
近接して配置しても電磁結合がなくなり、観測側の共鳴
信号が照射/ロック用のコイルに吸収されて感度低下を
もたらすことがなくなる。また、照射/ロック用のコイ
ルをサンプルの近くに配置しても観測用のコイルとの電
磁結合が遮断でき、共鳴信号の強度が弱まることもなく
なるので、照射、NMRロックの効率低下を防止するこ
とができる。In the NMR coil of the present invention, the shield ring is sandwiched between the arc coil parts of the two sets of coils, so there is no electromagnetic coupling even if both coils are placed close to each other, and the resonance signal on the observation side is used for irradiation/locking. It will no longer be absorbed by the coil and cause a decrease in sensitivity. In addition, even if the irradiation/locking coil is placed near the sample, electromagnetic coupling with the observation coil can be blocked and the strength of the resonance signal will not weaken, thus preventing a decrease in the efficiency of irradiation and NMR locking. be able to.
以下、図面を参照しつつ実施例を説明する。 Examples will be described below with reference to the drawings.
第1図は本発明に係るNMR用コイルの1実施例を示す
図、第2図は本発明に係るNMR用コイルの回路図、第
3図はシールド環の他の実施例を示す図である0図中、
1と3はボビン、2はシールド環、4と5はコイルを示
す。FIG. 1 is a diagram showing one embodiment of the NMR coil according to the present invention, FIG. 2 is a circuit diagram of the NMR coil according to the present invention, and FIG. 3 is a diagram showing another embodiment of the shield ring. In figure 0,
1 and 3 are bobbins, 2 is a shield ring, and 4 and 5 are coils.
本発明に係るNMR用コイルは、第1図に示すように同
心円筒のボビン1,3を配置し、これらにRF磁界の方
向が直交する(円筒空間の輪方向をZ軸、円筒空間の断
面をXY平面とすると、コイル4のRF[界をX方向、
コイル5のRF磁界をY方向とする)ようにそれぞれの
コイル4及びコイル5を配置する。そして、コイル4及
びコイル5のアークコイル部が相対する部分のボビン1
.3間にシールド環2を挟み込むようにしたものである
。その横断面図(平面図)が第1図ta>、斜視図が第
1図(bl、縦断面図が第1図+c+であり、内側のコ
イル4が観測用、外側のコイル5が照射/ロック用であ
る。The NMR coil according to the present invention has concentric cylindrical bobbins 1 and 3 arranged as shown in FIG. is the XY plane, the RF field of the coil 4 is in the X direction,
The coils 4 and 5 are arranged so that the RF magnetic field of the coil 5 is in the Y direction. Then, the bobbin 1 is located at the portion where the arc coil portions of the coil 4 and the coil 5 face each other.
.. The shield ring 2 is sandwiched between the shield rings 3 and 3. Its cross-sectional view (plan view) is shown in Figure 1 ta>, its perspective view is shown in Figure 1 (BL), and its vertical cross-sectional view is shown in Figure 1+C+. The inner coil 4 is for observation, and the outer coil 5 is for irradiation. It is for locking.
第1図(bl、tc+に示すようにコイル4及びコイル
5のアークコイル部と円筒空間の紬に平行な輪方向コイ
ル部とにより形成される窓部をあけ、アークコイル部の
間にシールド環2を挟み込むことによって、アークコイ
ル部の間に電磁障壁を設けている。このため、両コイル
4.5を近接して配置しても相互で問題となる電磁結合
をなくすことができ、コイル5もコイル4との@磁結合
を意識することがないので、コイル4と同様にサンプル
の近くに配置することができる。As shown in Figure 1 (bl, tc+), a window formed by the arc coil parts of the coils 4 and 5 and the circular coil part parallel to the pongee of the cylindrical space is opened, and a shield ring is formed between the arc coil parts. By sandwiching the coils 4 and 2, an electromagnetic barrier is provided between the arc coil parts.For this reason, even if the coils 4 and 5 are placed close to each other, it is possible to eliminate the electromagnetic coupling that causes problems between them. Since the magnetic coupling with the coil 4 is not conscious, it can be placed near the sample like the coil 4.
コイル4.5のそれぞれのアークコイル部及び輪方向コ
イル部の関係を表すと第2図のようになる。この第2図
に示すようにアークコイル部の断面方向(Z)は、コイ
ル4.5のいずれもが同じ方向であるのに対して、輪方
向コイル部の断面方向(X、Y)は、それぞれが直交す
る方向である。The relationship between the arc coil portion and the annular coil portion of each coil 4.5 is shown in FIG. 2. As shown in FIG. 2, the cross-sectional direction (Z) of the arc coil portion is the same for all coils 4.5, whereas the cross-sectional direction (X, Y) of the annular coil portion is The directions are perpendicular to each other.
本発明のNMR用コイルでは、この同じ方向で電磁結合
するアークコイル部の間に点線で示すシールドを施した
ものである。なお、このシールドは、アースしてもよい
し、アースから浮かしてもよい。In the NMR coil of the present invention, a shield shown by dotted lines is provided between the arc coil parts that are electromagnetically coupled in the same direction. Note that this shield may be grounded or floated from the ground.
また、シールド環2は、第2図に示すように円筒状のパ
イプでもよいが、相互のコイルのアークコイル部間で電
磁障壁の作用をするものであれば、第3図(alに示す
ようなバイブを半分に割った形状のものを用意してこれ
を向き合わせるようにして使ってもよいし、第3図(b
lに示すような円盤型のものを使ってもよい。The shield ring 2 may be a cylindrical pipe as shown in Fig. 2, but if it acts as an electromagnetic barrier between the arc coil parts of the mutual coils, it may be a cylindrical pipe as shown in Fig. 3 (al). You can also prepare a vibrator split in half and use it with the two halves facing each other, or use the
A disc-shaped one as shown in 1 may also be used.
シールド環としては、導電材料や金属、高分子材料等を
用いることができ、これらの材料を使ったフィルム状の
プリント板や、ガラス、セラミックに蒸着したもの、箔
状板をガラス、セラミック基材に張り付けたものでもよ
い。As the shield ring, conductive materials, metals, polymer materials, etc. can be used, and film-like printed boards made of these materials, those deposited on glass or ceramic, or foil-like plates made of glass or ceramic substrates can be used. It may also be attached to.
以上の説明から明らかなように、本発明によれば、観測
用コイルと照射/ロック用コイルとの間でアークコイル
部に起因する電磁結合を遮断するため、両コイル共にサ
ンプルに近接して配置できる。その結果、それぞれのコ
イルでのNMR共鳴信号の感度を高め、測定効率の向上
を図ることができる。特に、従来のNMR用コイルでは
、コイル相互間の!磁結合により共振波が数多く発生す
るため、目的とする共振波の発生エネルギーを吸収する
場合が多く、また、検出空間外の空間にある物質の信号
をピンクアップし、スペクトラムの裾の広がりが大きく
していた。しかし本発明によれば、シールド環を設け、
不要な共振波の減少を図ると共に、検出空間外からの信
号のピンクアップを遮断するので、上記のような従来の
NMR用コイルによる問題が解消し、測定感度や測定効
率の向上を図ることができる。As is clear from the above description, according to the present invention, in order to cut off electromagnetic coupling caused by the arc coil between the observation coil and the irradiation/locking coil, both coils are placed close to the sample. can. As a result, the sensitivity of the NMR resonance signal in each coil can be increased, and measurement efficiency can be improved. In particular, in conventional NMR coils, between the coils! Since many resonant waves are generated due to magnetic coupling, the generated energy of the desired resonant wave is often absorbed, and the signals of substances in the space outside the detection space are pinked up, causing the tail of the spectrum to widen significantly. Was. However, according to the present invention, a shield ring is provided,
In addition to reducing unnecessary resonance waves, it also blocks the pink-up of signals from outside the detection space, which eliminates the problems with conventional NMR coils and improves measurement sensitivity and efficiency. can.
第1図は本発明に係るNMR用コイルの1実施例を示す
図、第2図は本発明に係るN M R用コイルの回路図
、第3図はシールド環の他の実施例を示す図、第4図は
NMR用コイルの構成例を示す図、第5図は従来のNM
R用コイルの形状例を示す図である。
1と3・・・ボビン、2・・・シールド環、4と5・・
・コイル。
出 願 人 日本電子株式会社
第1図
(い (C)第2図
第3図
(α)
Cb)
第4図FIG. 1 is a diagram showing one embodiment of the NMR coil according to the present invention, FIG. 2 is a circuit diagram of the NMR coil according to the present invention, and FIG. 3 is a diagram showing another embodiment of the shield ring. , Fig. 4 shows an example of the configuration of an NMR coil, and Fig. 5 shows a conventional NM coil.
It is a figure which shows the example of a shape of the coil for R. 1 and 3...bobbin, 2...shield ring, 4 and 5...
·coil. Applicant: JEOL Ltd. Figure 1 (C) Figure 2 Figure 3 (α) Cb) Figure 4
Claims (1)
クコイル部と紬に平行な輪方向コイル部とにより構成さ
れる2組のコイルを同心円筒上に配置してなるNMR用
コイルにおいて、前記2組のコイルのアークコイル部間
にシールド環を挟み込むように配置したことを特徴とす
るNMR用コイル。An NMR coil in which two sets of coils each consisting of an arc-shaped arc coil part and a circular coil part parallel to the pongee are arranged on a concentric cylinder on the outer periphery of a cylindrical space in which a sample is loaded. An NMR coil characterized in that a shield ring is placed between the arc coil portions of the two sets of coils.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61190278A JPH0652298B2 (en) | 1986-08-13 | 1986-08-13 | NMR coil |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61190278A JPH0652298B2 (en) | 1986-08-13 | 1986-08-13 | NMR coil |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6345549A true JPS6345549A (en) | 1988-02-26 |
JPH0652298B2 JPH0652298B2 (en) | 1994-07-06 |
Family
ID=16255501
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61190278A Expired - Fee Related JPH0652298B2 (en) | 1986-08-13 | 1986-08-13 | NMR coil |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0652298B2 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4924184A (en) * | 1988-04-11 | 1990-05-08 | Mitsubishi Denki Kabushiki Kaisha | Magnetic resonance apparatus |
JP2002085373A (en) * | 2000-09-14 | 2002-03-26 | Ge Medical Systems Global Technology Co Llc | Method for inhibiting electromagnetic coupling between coils, orthogonal coil, mri device and method of making orthogonal coil |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60177249A (en) * | 1983-12-16 | 1985-09-11 | ゼネラル・エレクトリツク・カンパニイ | Nmr device |
-
1986
- 1986-08-13 JP JP61190278A patent/JPH0652298B2/en not_active Expired - Fee Related
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60177249A (en) * | 1983-12-16 | 1985-09-11 | ゼネラル・エレクトリツク・カンパニイ | Nmr device |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4924184A (en) * | 1988-04-11 | 1990-05-08 | Mitsubishi Denki Kabushiki Kaisha | Magnetic resonance apparatus |
JP2002085373A (en) * | 2000-09-14 | 2002-03-26 | Ge Medical Systems Global Technology Co Llc | Method for inhibiting electromagnetic coupling between coils, orthogonal coil, mri device and method of making orthogonal coil |
Also Published As
Publication number | Publication date |
---|---|
JPH0652298B2 (en) | 1994-07-06 |
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Legal Events
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