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JPH06249934A - Sample tube for NMR - Google Patents

Sample tube for NMR

Info

Publication number
JPH06249934A
JPH06249934A JP5061122A JP6112293A JPH06249934A JP H06249934 A JPH06249934 A JP H06249934A JP 5061122 A JP5061122 A JP 5061122A JP 6112293 A JP6112293 A JP 6112293A JP H06249934 A JPH06249934 A JP H06249934A
Authority
JP
Japan
Prior art keywords
sample
magnetic field
test tube
cavity
coil
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.)
Pending
Application number
JP5061122A
Other languages
Japanese (ja)
Inventor
Makoto Fujita
真 藤田
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 JP5061122A priority Critical patent/JPH06249934A/en
Publication of JPH06249934A publication Critical patent/JPH06249934A/en
Pending legal-status Critical Current

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  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

PURPOSE:To obtain NMR (nuclear magnetic resonance absorption analysis) spectrum with a high resolution using a small amount of sample by forming a spherical cavity within a cylinder which is inserted into a coil for analysis and then penetrating a capillary hole leading to the cavity from the upper edge along the center line of the cylinder. CONSTITUTION:A test tube 1 is a cylinder made of glass, a spherical cavity 3 is formed at the center part, and then a capillary hole 4 is penetrated to the cavity 3 along the axis of the cylinder from the upper edge. A coil 2 for analysis and the test tube 1 are placed in a static magnetic field H. A sample liquid solution S is allowed to flow from the capillary hole 4 to fill in the cavity 3 and no liquid solution S is filled into the capillary hole 4 itself. Since the test tube 1 is made of a diamagnetic material, no static magnetic field at the upper and lower both edge parts is disturbed due to the test tube itself when a constant magnetic substance is mixed for forming a nonmagnetic or a weak constant magnetism. When the outer diameter of the test tube 1 is made uniform and the test tube 1 is extended fully longer so that both edges completely leave the upper and lower both edges of the coil 2, even a slight flow of magnetic field at the upper and lower both edges of the test tube 1 does not reach the location of the sample, thus further reducing disturbance of the magnetic field.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はNMR(核磁気共鳴吸収
分析)用の試料管の改良に関する。
FIELD OF THE INVENTION The present invention relates to an improvement of a sample tube for NMR (nuclear magnetic resonance absorption analysis).

【0002】[0002]

【従来の技術】NMR用試料管は従来図2に示すように
試験管形をしており、これをNMR装置に挿入する。N
MR装置は試料管の管軸方向に強い静磁場Hを形成して
おり、試料管1はこの静磁内に置かれた分析用コイル2
内に挿入される。この場合一般に、試料溶液は空気とは
透磁率が異っているので、試料管内の試料溶液Sの上下
両端部では静磁場は乱れている。この静磁場の乱れが分
析用コイル2で囲まれた領域内にまで及んでいると、N
MRスペクトルの分解能が低下するため、試料溶液の上
下両端部を分析用コイルの上下端より更に上下外方に位
置させるようにしており、このため試料溶液は分析用コ
イルに囲まれた領域の体積以上の量を必要とし、微量試
料の分析は困難であった。また上述したように試料を余
分に用いて、上下両端の磁場の乱れた部分が分析用コイ
ルの領域の外に位置しているようにしても、分析用コイ
ル領域での試料溶液断面における磁場は均一にならない
ので、補正作業(シミング)が必要で、しかも試料溶液
断面の磁場の不均一の程度は試料溶液の透磁率によって
異っているため、試料毎にシミングをやり直す必要があ
って分析操作が面倒であった。
2. Description of the Related Art A conventional NMR sample tube has a test tube shape as shown in FIG. 2 and is inserted into an NMR apparatus. N
The MR device forms a strong static magnetic field H in the tube axis direction of the sample tube, and the sample tube 1 has an analysis coil 2 placed in this magnetostatic field.
Inserted inside. In this case, since the sample solution generally has a different magnetic permeability from that of air, the static magnetic field is disturbed at the upper and lower ends of the sample solution S in the sample tube. If the disturbance of the static magnetic field reaches the area surrounded by the analysis coil 2, N
Since the resolution of the MR spectrum is reduced, the upper and lower ends of the sample solution are positioned further up and down outside the upper and lower ends of the analysis coil. Therefore, the sample solution has a volume in the area surrounded by the analysis coil. The above amount was required, and it was difficult to analyze a trace amount sample. Further, as described above, even if the extra sample is used and the disturbed portions of the magnetic field at the upper and lower ends are located outside the area of the analysis coil, the magnetic field in the sample solution cross section in the analysis coil area is Since it is not uniform, correction work (shimming) is required, and the degree of non-uniformity of the magnetic field in the cross section of the sample solution differs depending on the magnetic permeability of the sample solution, so it is necessary to perform shimming again for each sample. Was troublesome.

【0003】[0003]

【発明が解決しようとする課題】本発明は小量の試料溶
液でも分解能が良く、試料毎にシミングをやり直す必要
もないようなNMR用試料管を提供しようとするもので
ある。
SUMMARY OF THE INVENTION The present invention is intended to provide an NMR sample tube which has a high resolving power even with a small amount of sample solution and does not need to perform shimming again for each sample.

【0004】[0004]

【課題を解決するための手段】分析用コイルに挿入され
る円柱体の中に球形(一般的には楕円体)の空洞を形成
し、円柱体の中心線に沿って上端からこの空洞に通じる
細管孔を貫入させて試料管とした。
A spherical (generally ellipsoidal) cavity is formed in a cylindrical body to be inserted into an analysis coil, and the cavity extends from the upper end along the centerline of the cylindrical body. The sample tube was made by penetrating the narrow tube hole.

【0005】[0005]

【作用】球体(一般には楕円体)を均一磁場内に置く
と、透磁率の如何に係りなく、その物体内は均一に磁化
され、物体外部の磁場は乱れても物体内の磁場は一様均
一なものとなる。楕円体の場合、楕円軸が外の一様な磁
場に対して傾いているときでも楕円体内の磁場は一様均
一なもので、唯物体内の磁場の方向が外部磁場と異った
ものとなる。本発明の場合、試料は楕円体の空洞内に満
され、空洞の楕円軸がNMR装置の静磁場と平行である
から、試料内には静磁場と同じ方向の均一磁場が形成さ
れており、試料内に磁場の乱れた場所がないから、空洞
は分析用コイル領域内に全体が入る大きさでよく、分析
用コイル領域の外まで試料溶液で満す必要がなくなり、
微量の試料でも分解能の高いNMRスペクトルを得るこ
とができ、試料内の磁場は均一であるから、試料毎にシ
ミングをやり直す必要がなくなる。
When a sphere (generally an ellipsoid) is placed in a uniform magnetic field, the inside of the body is magnetized uniformly regardless of the magnetic permeability, and the magnetic field inside the body is uniform even if the magnetic field outside the body is disturbed. It becomes uniform. In the case of an ellipsoid, even if the ellipse axis is inclined with respect to the outer uniform magnetic field, the magnetic field inside the ellipsoid is uniform, and the direction of the magnetic field inside the object is different from the external magnetic field. . In the case of the present invention, the sample is filled in the cavity of the ellipsoid, and the ellipse axis of the cavity is parallel to the static magnetic field of the NMR apparatus, so that a uniform magnetic field in the same direction as the static magnetic field is formed in the sample, Since there is no place where the magnetic field is disturbed in the sample, the size of the cavity can be entirely within the analysis coil area, and it is not necessary to fill the outside of the analysis coil area with the sample solution.
An NMR spectrum with high resolution can be obtained even with a small amount of sample, and since the magnetic field in the sample is uniform, it is not necessary to perform shimming again for each sample.

【0006】[0006]

【実施例】図1に本発明の一実施例のNMR用試料管を
示す。1が試料管でガラスで作られた円柱体であり、中
央部に球形の空洞3が形成してあり、上端から円柱体の
軸に沿って細管孔4が空洞3まで貫通させてある。2は
分析用コイルで、分析用コイルとこの試料管1とが静磁
場Hの中に置かれる。試料溶液Sは球形の空洞3内を充
満させるように細管孔4から注入される。細管孔4自体
には試料溶液を満さない。細管孔内まで試料溶液が入っ
ていると却って試料内の磁場の乱れが生じる。
EXAMPLE FIG. 1 shows an NMR sample tube according to an example of the present invention. Reference numeral 1 denotes a sample tube, which is a cylindrical body made of glass, in which a spherical cavity 3 is formed in the central portion, and a thin tube hole 4 is made to penetrate from the upper end to the cavity 3 along the axis of the cylindrical body. Reference numeral 2 is an analysis coil, and the analysis coil and the sample tube 1 are placed in a static magnetic field H. The sample solution S is injected from the capillary hole 4 so as to fill the inside of the spherical cavity 3. The capillary hole 4 itself is not filled with the sample solution. On the contrary, if the sample solution is filled into the narrow tube hole, the magnetic field in the sample is disturbed.

【0007】試料管1はガラス製であるが、ガラスは反
磁性材料であるので、常磁性物質を混入して非磁性或は
微弱な常磁性とすると試料管自体による上下両端部の静
磁界の乱れは非常に少なくなる。試料管を外径を一様に
して充分長くして、両端が分析用コイル2の上下両端か
ら充分離れているようにすれば試料管の上下両端部のわ
ずかな磁場の乱れも試料の所には及ばず分析用コイルの
領域では静磁界は均一とみなせるので、試料管の材料を
単に非磁性にするより、一層磁場の乱れは少くなる。ま
た上下両端を丸くしておくと、試料管全体が細長い楕円
体とみなせて都合がよい。なお上述実施例では空洞の形
は球であるが、前述したように楕円体の形であれば細長
くても偏平であってもよく、楕円軸の一つが静磁場の方
向と平行しておれば、空洞内の試料溶液中の磁場も静磁
場と平行で均一になっている。つまり球は楕円体の特殊
なものである。また試料管の透磁率を空気とほとんど同
じにすれば、試料管は図1のような外径一定の形でなく
てもよく、試料部のみをふくらませた細管の形でもよ
い。
The sample tube 1 is made of glass, but since glass is a diamagnetic material, if a paramagnetic substance is mixed into the sample tube to make it nonmagnetic or weakly paramagnetic, the static magnetic field at the upper and lower ends of the sample tube itself will be Disturbances are very small. If the outer diameter of the sample tube is made uniform and the length is sufficiently long so that both ends are sufficiently separated from the upper and lower ends of the analysis coil 2, even a slight disturbance of the magnetic field at the upper and lower ends of the sample tube will reach the sample. Since the static magnetic field can be regarded as uniform in the area of the analysis coil, the disturbance of the magnetic field is further reduced as compared with the case where the material of the sample tube is simply made non-magnetic. If both upper and lower ends are rounded, it is convenient that the entire sample tube can be regarded as an elongated ellipsoid. Although the shape of the cavity is a sphere in the above-mentioned embodiment, it may be elongated or flat as long as it is an ellipsoidal shape as described above, as long as one of the ellipse axes is parallel to the direction of the static magnetic field. The magnetic field in the sample solution in the cavity is also parallel and uniform with the static magnetic field. So the sphere is a special kind of ellipsoid. Further, if the magnetic permeability of the sample tube is almost the same as that of air, the sample tube does not have to have a shape with a constant outer diameter as shown in FIG. 1, but may have the shape of a thin tube in which only the sample portion is inflated.

【0008】[0008]

【発明の効果】本発明によれば、磁場の乱れている部分
が分析用コイルの領域に入らないようにするため多量の
試料を必要とすると云うようなことがなく、分析用コイ
ル領域内の小さな体積内を満すだけの試料の量で分析が
できるため、試料の無駄がなく、小量しか入手できない
試料の分析も可能となり、磁場の乱れの影響が全くない
から、小量の試料で分解能の良いNMRスペクトルを得
ることができ、試料毎のシミングの手間が不要となって
分析作業の能率が向上し、試料が小量ですむから、試料
の誘電率の違いによる分析用コイルの入力高周波に対す
る同調のずれが小さく、分析装置の取扱いも楽となる。
According to the present invention, a large amount of sample is not required in order to prevent the disturbed portion of the magnetic field from entering the area of the analysis coil. Since it is possible to analyze with a sample amount that fills a small volume, there is no waste of sample, and it is possible to analyze a sample that can be obtained only in a small amount. It is possible to obtain a high-resolution NMR spectrum, eliminating the need for shimming for each sample, improving the efficiency of analysis work, and reducing the amount of sample required. The deviation of tuning to high frequency is small, and the analyzer is easy to handle.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の一実施例の試料管の縦断側面図FIG. 1 is a vertical sectional side view of a sample tube according to an embodiment of the present invention.

【図2】従来例の試料管の側面図FIG. 2 is a side view of a conventional sample tube.

【符号の説明】[Explanation of symbols]

1 試料管 2 分析用コイル 3 空洞 4 細管孔 S 試料溶液 1 Sample tube 2 Coil for analysis 3 Cavity 4 Capillary hole S Sample solution

Claims (1)

【特許請求の範囲】[Claims] 試料を収納する部分を楕円体空洞とし、その一軸方向に
細長管を接続したことを特徴とするNMR用試料管。
An NMR sample tube characterized in that an ellipsoidal cavity is formed in a portion for accommodating a sample, and elongated tubes are connected in the uniaxial direction.
JP5061122A 1993-02-25 1993-02-25 Sample tube for NMR Pending JPH06249934A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5061122A JPH06249934A (en) 1993-02-25 1993-02-25 Sample tube for NMR

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5061122A JPH06249934A (en) 1993-02-25 1993-02-25 Sample tube for NMR

Publications (1)

Publication Number Publication Date
JPH06249934A true JPH06249934A (en) 1994-09-09

Family

ID=13161962

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5061122A Pending JPH06249934A (en) 1993-02-25 1993-02-25 Sample tube for NMR

Country Status (1)

Country Link
JP (1) JPH06249934A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7135865B2 (en) 2004-03-22 2006-11-14 Hitachi, Ltd. Nuclear magnetic resonance spectrometer and method for operation thereof
JP2008082751A (en) * 2006-09-26 2008-04-10 Hitachi Ltd NMR probe and NMR apparatus
EP1918731A1 (en) * 2006-11-04 2008-05-07 Bruker BioSpin AG Sample container for NMR measurements with homogenisation of sample volume by sample container boundaries
DE102011007167A1 (en) * 2011-04-11 2012-10-11 Bruker Biospin Ag NMR measuring arrangement with optimized sample container geometry and method for calculating the shape of the sample container

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7135865B2 (en) 2004-03-22 2006-11-14 Hitachi, Ltd. Nuclear magnetic resonance spectrometer and method for operation thereof
JP2008082751A (en) * 2006-09-26 2008-04-10 Hitachi Ltd NMR probe and NMR apparatus
EP1918731A1 (en) * 2006-11-04 2008-05-07 Bruker BioSpin AG Sample container for NMR measurements with homogenisation of sample volume by sample container boundaries
JP2008116458A (en) * 2006-11-04 2008-05-22 Bruker Biospin Ag Sample holder for NMR measurement that homogenizes the magnetic field in the sample volume by the boundary surface of the sample holder
US7656158B2 (en) 2006-11-04 2010-02-02 Bruker Biospin Ag Sample holder for NMR measurements with field homogenization in the sample volume by means of the bordering surfaces of the sample holder
DE102011007167A1 (en) * 2011-04-11 2012-10-11 Bruker Biospin Ag NMR measuring arrangement with optimized sample container geometry and method for calculating the shape of the sample container
US8912796B2 (en) 2011-04-11 2014-12-16 Bruker Biospin Ag NMR measuring configuration with optimized sample container geometry and method for calculating the shape of the sample container
DE102011007167B4 (en) * 2011-04-11 2016-05-19 Bruker Biospin Ag NMR measuring arrangement with optimized sample container geometry and method for calculating the shape of the sample container

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