JPS6156947A - High frequency coil for nmr imaging apparatus - Google Patents

High frequency coil for nmr imaging apparatus

Info

Publication number
JPS6156947A
JPS6156947A JP59100206A JP10020684A JPS6156947A JP S6156947 A JPS6156947 A JP S6156947A JP 59100206 A JP59100206 A JP 59100206A JP 10020684 A JP10020684 A JP 10020684A JP S6156947 A JPS6156947 A JP S6156947A
Authority
JP
Japan
Prior art keywords
saddle
coils
parts
coil
shaped
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
JP59100206A
Other languages
Japanese (ja)
Inventor
Taiji Hashimoto
泰司 橋本
Kimiharu Shimizu
公治 清水
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 JP59100206A priority Critical patent/JPS6156947A/en
Publication of JPS6156947A publication Critical patent/JPS6156947A/en
Pending 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
    • G01R33/34046Volume type coils, e.g. bird-cage coils; Quadrature bird-cage coils; Circularly polarised coils
    • G01R33/34069Saddle coils
    • 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
    • G01R33/36Electrical details, e.g. matching or coupling of the coil to the receiver

Landscapes

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

Abstract

PURPOSE:To improve the upper limit of a high frequency to be used, by electrically connecting two saddle-type signal coils in parallel, and making the distances between the corresponding points and power feeding points on two parallel straight-line parts equal. CONSTITUTION:Two saddle-type coils 1 and 2 are formed by conducting wire parts ABCDEF and A'B'C'D'E'F'. The coils are symmetrically arranged so that the centers of curvatures of the arc parts on the corresponding sides agree. Thus a coil pair having the saddle type as a whole is constituted. The central angle of the arc parts of both coils 1 and 2 is made to be 120 deg.. The length of the straight line part is made to be twice the radius of curvature at the arc part. Cut parts AF and A'F' are provided at the centers of the arc parts on the same side. The conducting parts A and A' and F and F' are connected. Power is fed in parallel symmetrically through terminals 3 and 4, which are connected to the central points of the connecting lines. Thus the maximum frequency limit of the high frequency to be used can be increased.

Description

【発明の詳細な説明】 (イ)産業上の利用分野 本発明はNMRイメージング装置用高周波コイルに関す
る。
DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a high frequency coil for an NMR imaging device.

(ロ)従来技術 一般にコイル状に巻かれた導体線が純インダクタンス素
子として機能するためには、その直流抵抗成分が無視し
得る場合でも、供給される交流電流の波長に対して導体
線の長さが近似的に無視し得る程度に短かいことが必要
である。  ′ところで医療用NMRイメージング装置
では、直流磁場と、それに直交する高周波磁場中に被検
体としての人体または人体の一部を挿入する必要がある
が、人体の挿入、引出しを容易にするため、高周波磁場
用コイルおよびNMR信号検出用コイル(両者兼用の場
合もある)にはしばしば鞍型コイルが用いられる。しか
し、被検体が人体またはその一部であるため、コイルの
形状・寸法は理化学用NMR装置の場合にくらべて格段
に大きくならざるを得す、しかも1.一般的に云って信
号強度を上げるためにはNMR周波数をある程度まで高
くすること、即ち、使用高周波の波長を短かくすること
か望ましく、このことは冒頭に述べた波長とコイル導体
長との間に望まれる関係に矛盾する。
(b) Prior art In general, in order for a conductor wire wound into a coil to function as a pure inductance element, even if its DC resistance component can be ignored, the length of the conductor wire relative to the wavelength of the supplied alternating current must be It is necessary that the length be short enough to be approximately negligible. 'By the way, in medical NMR imaging equipment, it is necessary to insert a human body or a part of the human body as a subject into a DC magnetic field and a high-frequency magnetic field perpendicular to it. Saddle-shaped coils are often used as magnetic field coils and NMR signal detection coils (sometimes used for both). However, since the subject to be examined is a human body or a part thereof, the shape and dimensions of the coil must be much larger than those for physical and chemical NMR devices. Generally speaking, in order to increase the signal strength, it is desirable to increase the NMR frequency to a certain degree, that is, to shorten the wavelength of the high frequency used. conflict with the desired relationship.

実験ないし経験の示すところによれば導体長ば実用上、
波長の/20以下に保つことが必要で、これを超えると
、コイルのQ−値が著しく低下する。
Experiments and experience have shown that in practice, if the conductor is long,
It is necessary to keep it below /20 of the wavelength; if it exceeds this, the Q-value of the coil will drop significantly.

以上を、人体頭部イメージング用の鞍型コイルについて
考察する。この場合鞍型コイルの円弧状部の曲率半径は
最低15(!7+1は必要であり、一方、理論的に求め
られる鞍型コイルの理想形状によれば、その直線部の長
さは上記曲率半径の2倍々することが望ましい。従って
この鞍型コイル1個の導体長は123ffiとなるが、
NMR用高周波コイルとしては、このような鞍型コイル
2個から成る鞍型コイルのペアとして使用するので、両
コイルを直列に接続した場合、導体部総延長は2’4’
6cmに達する。これに対して波長の/20が246a
mになる周波数は6.1MH2J−算出される。従って
、:)   。。、9カ、j−よ、うつO’am=l 
tvt[JIW=1ルとする場合、NMR周波数は6・
IMHz以下に選ばなければならない。
The above will be considered regarding a saddle-shaped coil for human head imaging. In this case, the radius of curvature of the arcuate portion of the saddle-shaped coil must be at least 15 (!7+1); on the other hand, according to the theoretically determined ideal shape of the saddle-shaped coil, the length of the straight portion is the radius of curvature above Therefore, the conductor length of one saddle-shaped coil is 123ffi, but
The high-frequency coil for NMR is used as a pair of saddle-shaped coils consisting of two such saddle-shaped coils, so when both coils are connected in series, the total length of the conductor part is 2'4'.
Reaches 6cm. On the other hand, the wavelength /20 is 246a
The frequency that becomes m is calculated as 6.1MH2J. Therefore :). . , 9ka, j-yo, Utsu O'am=l
When tvt[JIW=1, the NMR frequency is 6.
Must be selected below IMHz.

このような欠点を幾分でも克服するために、第1図に示
すように鞍型コイルペアを構成する2つの鞍型シングル
コイル1および2を、それらかつくる磁場が加算的にな
るよう電流の向きを選んで、電気的に並列に接続構成し
た高周波コイルも提案されている。即ち、コイル導体部
と波長との関係が問題になるのは、電流路の長さが波長
に対して無視し得なくなると、導体各部における電流値
の時間変化に無視し得ないずれを生ずるため、つ捷り、
導体部に沿っての電流の位相差が無視できなくなるため
である。従って、両シングルコイルを並列接続すること
によって各シングルコイル毎に電流路の長さを考慮する
だけでよいことになれば、使用高周波の限界波長は倍に
なり、上記に例示した鞍型コイルペアの場合、並列接続
によりNMR周波数は12.2MH2まで高く選ぶこと
ができるようになる。               
        I々ころで、鞍型コイルペアにおいて
は、その中心部につくられる磁場は、その主要部が鞍型
コイル直線部を流れる電流によっており、円弧部の電流
による寄与は小さいにも拘らず、考慮すべき電流路の長
さには円弧部の長さも含まれているため、両シングルコ
イルの並列接続によっても、上述のように使用高周波周
波数の上限は、直列接続の場合の高々2倍にしかならな
い。
In order to overcome some of these drawbacks, as shown in Fig. 1, two saddle-shaped single coils 1 and 2 constituting a saddle-shaped coil pair are arranged so that the direction of the current is made additive. High-frequency coils have also been proposed in which the following are selected and configured to be electrically connected in parallel. In other words, the relationship between the coil conductor and the wavelength becomes a problem because when the length of the current path becomes negligible relative to the wavelength, a non-negligible deviation occurs in the time change of the current value in each part of the conductor. , shunting,
This is because the phase difference of the current along the conductor portion cannot be ignored. Therefore, if both single coils are connected in parallel, and it is only necessary to consider the length of the current path for each single coil, the limit wavelength of the high frequency used will be doubled, and the saddle-shaped coil pair illustrated above will be In this case, the parallel connection allows the NMR frequency to be selected as high as 12.2 MH2.
In a saddle-shaped coil pair, the magnetic field created at the center is mainly due to the current flowing through the straight section of the saddle-shaped coil, and although the contribution from the current in the arcuate section is small, it cannot be considered. Since the length of the current path includes the length of the arc, even if both single coils are connected in parallel, the upper limit of the high frequency that can be used is only twice as high as in the case of series connection, as described above. .

(ハ) 目的 本発明の目的は、従来技術に伴う上記のような欠点を排
除し、使用高周波周波数の上限をさらに高めた、NMR
装置用鞍型コイルペアを提供することにある。
(C) Purpose The purpose of the present invention is to eliminate the above-mentioned drawbacks associated with the prior art, and to develop an NMR system that further increases the upper limit of the usable high frequency.
An object of the present invention is to provide a saddle-shaped coil pair for a device.

に)構成 上記の目的を達成するため、本発明による鞍型コイルペ
アは、NMR装置用鞍型高周波コイル・ペアであって、
このコイルペアを構成する2つの鞍型シングルコイルが
電気的に互に並列接続されていることと、各鞍型シング
ルコイルにおける互に平行する2つの直線部上の対応す
る2点と当該鞍型シングルコイルへの給電点との間の距
離が等しくなっていることを特徴としている。
B) Structure To achieve the above object, the saddle-shaped coil pair according to the present invention is a saddle-shaped high-frequency coil pair for an NMR apparatus, which comprises:
The two saddle-shaped single coils constituting this coil pair are electrically connected to each other in parallel, and the two corresponding points on the two parallel straight sections of each saddle-shaped single coil are connected to the saddle-shaped single coil. It is characterized by the fact that the distance between the power supply point to the coil and the power supply point is the same.

(ホ)実施例 以下に本発明の実施例を図面に基づいて説明する。(e) Examples Embodiments of the present invention will be described below based on the drawings.

第2図は本発明実施例よりなる鞍型コイルペアの構成を
模式的に示した斜視図である。同図において2つの鞍型
コイル1および2はそれぞれ導線部ABCDEFおよび
AIB/ C/ D/ E7 F/より成り、それぞれ
の互に対応する側の円弧部の曲率中心が一致するよう互
に対称に配列されて全体の鞍型コイルペアを構成してい
る。両統型コイル1および2とも、円弧部の中心角は1
20°で、直線部の長さは円弧部曲率半径の倍に選ばれ
ている。また、両統型コイル1および2は、それぞれ、
同じ側の円弧部中央に切断AFおよびA’F’を有し、
AとA′およびFとF′が結ばれ、それぞれAとA′の
中点およびFとF′の中点に接続された端子3および4
より、共に対称的に並列給電されるようになっている。
FIG. 2 is a perspective view schematically showing the configuration of a saddle-shaped coil pair according to an embodiment of the present invention. In the same figure, two saddle-shaped coils 1 and 2 each consist of conductor parts ABCDEF and AIB/C/D/E7F/, and are arranged symmetrically so that the centers of curvature of the circular arc parts on the corresponding sides coincide with each other. They are arranged to form a whole saddle-shaped coil pair. For both type coils 1 and 2, the central angle of the arc part is 1
20°, and the length of the straight section is chosen to be twice the radius of curvature of the arc section. In addition, both type coils 1 and 2 are, respectively,
It has cutting AF and A'F' in the center of the arc part on the same side,
A and A' and F and F' are connected, and terminals 3 and 4 are connected to the midpoint of A and A' and the midpoint of F and F', respectively.
This allows them to be symmetrically fed in parallel.

このような鞍型コイルペアの構造により、各鞍型コイル
はその直線部に関して対称力位置に給電点を有すること
になるので、互に平行な2本の直線部上の対応する点に
おける電流の(絶対値の)間に位相差は生じない。しか
も、先に述べたように鞍型コイルペアの中心部につくら
れる磁場に関しては、事実上、直線部の電流によるもの
だけを考えればよいから、コイル導体部の長さと波長と
の関係は、鞍型コイル直線部の長さと波長との関係に置
換される。前述のような円弧部の中心角を120°、直
線部の長さを円弧部曲率半径の2倍とする理想形状の鞍
型コイルにおいては、円弧部の長さが鞍型コイル−周の
長さの約Aを占めるから、円弧部の長さを考慮する必要
がなくなることにより、使用高周波の最高周波数限界は
大幅に増大する。
Due to this structure of the saddle-shaped coil pair, each saddle-shaped coil has a feeding point at a symmetrical force position with respect to its straight section, so that the current (( There is no phase difference between the absolute values. Moreover, as mentioned earlier, regarding the magnetic field created at the center of the saddle-shaped coil pair, we only need to consider the magnetic field caused by the current in the straight section, so the relationship between the length of the coil conductor and the wavelength is similar to that of the saddle-shaped coil pair. It is replaced by the relationship between the length of the straight part of the type coil and the wavelength. In the ideally shaped saddle-shaped coil where the central angle of the arc part is 120° and the length of the straight part is twice the radius of curvature of the arc part as described above, the length of the arc part is equal to the length of the saddle-shaped coil - circumference. Since there is no need to consider the length of the arc portion, the maximum frequency limit of the high frequency used is greatly increased.

本発明はまた、第3図に示すように、各鞍型コイルの、
非給電側円弧部の中央にキャパシタンスKを挿入して実
施することもできる。とのキャパシタンスにの挿入によ
り鞍型コイルペア全体のイ、!     ンダクタンス
は第2図に示した実施例の場合より小さくなり、Q−値
が改善される。
The present invention also provides, as shown in FIG.
It is also possible to insert a capacitance K into the center of the non-power feeding side circular arc portion. By inserting into the capacitance of the entire saddle-shaped coil pair i,! The inductance is smaller than in the embodiment shown in FIG. 2, and the Q-value is improved.

本発明はさらに、第4図に示すような構造に変形実施す
ることもできる。本実施例は4個の短冊型コイルa+ 
 4+  5.  eで構成されており、鞍型コイルペ
アとは云えないが、コイル13および14の内側の辺が
第2図の鞍型コイル1の直線部に対応し、コイル15お
よび16の内側の辺が第2図の鞍型コイル2の直線部に
対応している。第4図においても、第2図の各部に対応
する個所には、第2図に用いたのと同じ記号、々いし番
号が付されている。
The present invention can also be modified into a structure as shown in FIG. In this example, four rectangular coils a+
4+ 5. Although it cannot be called a saddle-shaped coil pair, the inner sides of coils 13 and 14 correspond to the straight part of saddle-shaped coil 1 shown in FIG. This corresponds to the straight portion of the saddle-shaped coil 2 shown in FIG. In FIG. 4, the same symbols and numbers as used in FIG. 2 are given to the parts corresponding to the parts in FIG. 2.

(へ)効果 以上の説明から明らかなように、本発明によれば、外形
寸法を同じとすれば使用高周波の最高周波数限界を従来
の鞍型コイルペアの場合より格段に高く選ぶことができ
、捷だ、最高周波数限界を同じとすれば、鞍型コイルペ
アの形状を従来のもt↑ のより大きく段重することができる。
(F) Effect As is clear from the above explanation, according to the present invention, if the external dimensions are the same, the maximum frequency limit of the high frequency used can be selected to be much higher than in the case of the conventional saddle-shaped coil pair. However, if the maximum frequency limit is the same, the shape of the saddle-shaped coil pair can be made larger than that of the conventional t↑.

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

第1図は従来技術による鞍型コイルペアの斜視図である
。第2図は本発明実施例による鞍型コイルペアの斜視図
である。第3図は、本発゛明の他の実施例による鞍型コ
イルペアの斜視図である。第4図は磁場発生に関しては
第2図に示した鞍型コイルペアと同じ効果を有する変型
実施例の構成を示す。 1.2・・鞍型シングルコイル、 3.4・・電流供給端子、
FIG. 1 is a perspective view of a saddle-shaped coil pair according to the prior art. FIG. 2 is a perspective view of a saddle-shaped coil pair according to an embodiment of the present invention. FIG. 3 is a perspective view of a saddle-shaped coil pair according to another embodiment of the present invention. FIG. 4 shows a modified embodiment having the same effect as the saddle coil pair shown in FIG. 2 in terms of magnetic field generation. 1.2...Saddle type single coil, 3.4...Current supply terminal,

Claims (2)

【特許請求の範囲】[Claims] (1)NMR装置用鞍型高周波コイル・ペアであつて、
このコイルペアを構成する2つの鞍型シングルコイルが
電気的に互に並列接続されていることと、各鞍型シング
ルコイルにおける互に平行する2つの直線部上の対応す
る2点と当該鞍型シングルコイルへの給電点との間の距
離が等しくなつていることとを特徴とする、NMRイメ
ージング装置用高周波コイル。
(1) A pair of saddle-shaped high-frequency coils for NMR equipment,
The two saddle-shaped single coils constituting this coil pair are electrically connected to each other in parallel, and the two corresponding points on the two parallel straight sections of each saddle-shaped single coil are connected to the saddle-shaped single coil. A high-frequency coil for an NMR imaging device, characterized in that the distances between the coil and a power feeding point are equal.
(2)上記各鞍型シングル・コイル中の円弧状部の中央
にキャパシタンスが直列接続されていることを特徴とす
る、特許請求の範囲第1項記載の、NMRイメージング
装置用高周波コイル。
(2) A high-frequency coil for an NMR imaging apparatus according to claim 1, characterized in that a capacitance is connected in series at the center of the arc-shaped portion in each of the saddle-shaped single coils.
JP59100206A 1984-05-17 1984-05-17 High frequency coil for nmr imaging apparatus Pending JPS6156947A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59100206A JPS6156947A (en) 1984-05-17 1984-05-17 High frequency coil for nmr imaging apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59100206A JPS6156947A (en) 1984-05-17 1984-05-17 High frequency coil for nmr imaging apparatus

Publications (1)

Publication Number Publication Date
JPS6156947A true JPS6156947A (en) 1986-03-22

Family

ID=14267829

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59100206A Pending JPS6156947A (en) 1984-05-17 1984-05-17 High frequency coil for nmr imaging apparatus

Country Status (1)

Country Link
JP (1) JPS6156947A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01254155A (en) * 1988-04-05 1989-10-11 Hitachi Ltd Checking device using nuclearmagnetic resonance

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01254155A (en) * 1988-04-05 1989-10-11 Hitachi Ltd Checking device using nuclearmagnetic resonance

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