JPS6316604A - Coil equipment - Google Patents

Coil equipment

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Publication number
JPS6316604A
JPS6316604A JP61161188A JP16118886A JPS6316604A JP S6316604 A JPS6316604 A JP S6316604A JP 61161188 A JP61161188 A JP 61161188A JP 16118886 A JP16118886 A JP 16118886A JP S6316604 A JPS6316604 A JP S6316604A
Authority
JP
Japan
Prior art keywords
coil
coils
origin
circular
axis
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
JP61161188A
Other languages
Japanese (ja)
Inventor
Kotaro Hamashima
浜島 高太郎
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP61161188A priority Critical patent/JPS6316604A/en
Publication of JPS6316604A publication Critical patent/JPS6316604A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To eliminate anxiety of a patient and reduce the weight of a coil system and make the system compact by a method wherein circular coils are so arranged as to make an imaginery line connecting an origin of coordinates and the inside edge of the radial direction of the circular coil at the outermost side of the axial direction fall within the angle range of not less than about 34.5 deg. and not more than about 63.4 deg. from the center axis. CONSTITUTION:Circular coils 1, 1' and 2 are composed of a frame 3 and superconductors wound on the frame 3 and the coil 2 is provided at the middle part between the coils 1 and 1'. In this case, the coils 1, 1' and 2 are wound on the cylindrical frame 3 and the coils 1 and 1' are provided on both sides of the coil 2. An imaginery line L which connects the center of the coil 2, i.e. an origin 0 of coordinates and the inside edge 4 of the radial direction of the coil 1 at the outermost side along a Z-axis looking from the origin o is drawn and the angle theta between the imaginery line L and the Z-axis is defined. The coils 1 and 1' and the coil 2 are so arranged as to have an identical center axis and to be symmetrical with respect to the imaginery plane R and further the coils 1 and 1' are so arranged as to make the angle theta fall within the range of not less than about 34.5 deg. and of not more than about 63.4 deg..

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は、医療用M RI (Magnetic Re
sonanceTmag i ng )装置や、N M
 R−CT (Nuclear Hagne−tic 
Resonance−Computer Tomogr
aphy)装置などに用いるコイル装置に関する。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention is directed to medical MRI (Magnetic Reaction MRI).
sonanceTmag ing ) device, N M
R-CT (Nuclear Hagne-tic
Resonance-Computer Tomogr
This invention relates to a coil device used in aphy) devices and the like.

(従来の技術) 最近、医療用MRI装置や、NMR−CT装置では、X
12CT装置と異なった方法、すなわち、原子核の核磁
気共鳴現象を利用した方法で断層像が得られるようにな
り、実際の診断にも使用され始めている。この断層像を
鮮明にし、しかも、短時間で1最影するには、所定の空
間に高均一の分布磁界を発生させる必要がある。この場
合、分布磁界の均一度は診断対象によっても異なるが、
例えば1OcM球内で0.lppm  (1x10−7
)である装置も出現している。
(Prior art) Recently, in medical MRI equipment and NMR-CT equipment,
It has become possible to obtain tomographic images using a method different from that of the 12CT device, that is, a method that utilizes the nuclear magnetic resonance phenomenon of atomic nuclei, and it has begun to be used in actual diagnosis. In order to make this tomographic image clear and to obtain the best image in a short time, it is necessary to generate a highly uniform distributed magnetic field in a predetermined space. In this case, the uniformity of the distributed magnetic field varies depending on the diagnosis target, but
For example, 0.0 in a 1OcM sphere. lppm (1x10-7
) devices have also appeared.

ところで、この種の分布磁界を発生させるには、円形コ
イルが多く用いられるが、その中心軸をZ軸とした場合
、Z軸上の磁界82は次式のように展開して表わすこと
ができる。
By the way, circular coils are often used to generate this kind of distributed magnetic field, and if the central axis is the Z-axis, the magnetic field 82 on the Z-axis can be expressed by expanding as shown in the following equation. .

+ a 4 Z p+   ・・・・・・・・・(1)
a、=I−f   (Z  、  θ  )   ・・
・・・・(2)nCC ただし、 I 2円形コイルに流れる電流 z、:z軸方向の測定位置 Z :円形コイルの7方向の位置 θ :円形コイルのZ軸からの角度 である。
+ a 4 Z p+ ・・・・・・・・・(1)
a, = I-f (Z, θ)...
...(2) nCC However, I 2 Current z flowing through the circular coil: Measurement position Z in the z-axis direction: Position of the circular coil in 7 directions θ: Angle of the circular coil from the Z-axis.

ここで、Z=Oの仮想平面に関して1対の円形コイルを
対称に配置し、しかも、これらのコイル対に同じ方向の
電流を供給した場合の中心軸付近の磁界B7は次式のよ
うに偶関数で表わされる。
Here, when a pair of circular coils are arranged symmetrically with respect to the imaginary plane of Z=O, and current is supplied in the same direction to these coil pairs, the magnetic field B7 near the central axis is calculated by the following equation. Represented by a function.

8    ・・・・・・・・・(3) +a8Z、+ また、1対のコイルに限らず、多数のコイル対であって
も(3)式と同じ形で表現でき、係数a2nは次式のよ
うになる。
8 ・・・・・・・・・(3) +a8Z,+ Also, not only one pair of coils but also many coil pairs can be expressed in the same form as equation (3), and the coefficient a2n is expressed as the following equation become that way.

a =Σ ■、・f2n”’ci、θci)・(412
0、1 1==ま ただし、 M:コイル対数 である。
a = Σ ■,・f2n”'ci, θci)・(412
0, 1 1 = = square, M: coil logarithm.

ところで、上述した係数”2nは円形コイルに流れる電
流とコイルの配置との関数になっているため、これら2
つのパラメータを適切に選ぶことにより係数a2nを零
にすることができる。一方、係数a。は位置に関係しな
い定数項で、均一磁界の成分を表わし、上記n〜0の係
数a2nは逆に均一な磁界分布を乱す誤差成分を表わす
ことになる。
By the way, the coefficient "2n" mentioned above is a function of the current flowing through the circular coil and the arrangement of the coil, so these two
By appropriately selecting two parameters, the coefficient a2n can be made zero. On the other hand, the coefficient a. is a constant term that is not related to position and represents a component of a uniform magnetic field, and the coefficient a2n of n to 0 represents an error component that disturbs the uniform magnetic field distribution.

かくして、高均一な分布磁界を得るには、誤差成分を表
わす係数a2.(n≧1)を、できる限りnの高いとこ
ろまで零にする必要がある。
Thus, in order to obtain a highly uniform distributed magnetic field, the coefficient a2. (n≧1) must be reduced to zero as high as possible.

一方、次数が高くなるぼど係数a2oは、Z方向位置Z
Cの増大とともに急激に減少する傾向にあるため、コイ
ルの軸長を長くするほど、高次項の影響が少なくなって
高均一な分布磁界を実現し易いと言える。
On the other hand, the coefficient a2o with a higher degree is
Since C tends to decrease rapidly as C increases, it can be said that the longer the axial length of the coil, the less the influence of higher-order terms becomes, making it easier to realize a highly uniform distributed magnetic field.

かかる観点から高均一の分布磁界を得る従来のコイル装
置として公知文献、例えば、JOURN^L DEPI
IYSrQUE 8THINTERNATIONAL 
C0NFERENCE ONMAGNET TECII
NOLOGY、5EPTEHBER5Tll〜9T11
.1983GR[N0BLE (FRANCE)に示さ
れたものがある。
From this point of view, there are known documents as conventional coil devices that obtain a highly uniform distributed magnetic field, such as JOURN^L DEPI.
IYSrQUE 8THINTERNATIONAL
C0NFERENCE ONMAGNET TECII
NOLOGY, 5EPTEHBER5Tll~9T11
.. There is one shown in 1983GR [N0BLE (FRANCE).

このコイル装置は、Z−0の原点を含むように配置した
中心のコイルと、Z=0の仮想平面に対称に配置した1
対のコイルとで構成されている。
This coil device consists of a central coil arranged to include the origin of Z-0, and a coil arranged symmetrically to the imaginary plane of Z=0.
It consists of a pair of coils.

なお、原点を含むように配置した中心のコイルは、やは
り、Z=0の仮想平面に対称な形状になっているので、
このコイルもまた対をなしているものと推定され、結局
、Z=Oの仮想平面に対して2対のコイルが対称に配置
された構成になっていると推定される。そして、このコ
イル装置においては、ZIN1方向最外側端の円形コイ
ルの径方向内側の縁と原点とを結ぶ仮想線分がZ軸に対
して略30.8度になるようなコイル配置になっている
Note that the central coil placed to include the origin has a shape that is symmetrical to the imaginary plane of Z=0, so
It is estimated that these coils also form a pair, and in the end, it is estimated that the two pairs of coils are arranged symmetrically with respect to the imaginary plane of Z=O. In this coil device, the coil arrangement is such that the imaginary line segment connecting the radially inner edge of the outermost circular coil in the ZIN1 direction and the origin is approximately 30.8 degrees with respect to the Z axis. There is.

一般に、上述した仮想線分がZ軸となす角度をOとし、
θ−63.44度となるようにコイルを配置すると、い
わゆる、ヘルム・ホルツ型のコイル配置となって係数a
2=oとなることが知られている。
Generally, the angle that the above-mentioned virtual line segment makes with the Z axis is O,
If the coil is arranged so that θ is -63.44 degrees, it becomes a so-called Helm-Holtz type coil arrangement, and the coefficient a
It is known that 2=o.

しかし、上記従来のコイル装置のθが略30.8度にな
っている点を考慮すると、この装置はコイルの軸長を長
くして高次項の影響を除去して高均一の分布磁界を実現
したものと思われる。
However, considering that the θ of the conventional coil device mentioned above is approximately 30.8 degrees, this device increases the axial length of the coil to eliminate the influence of higher-order terms and achieves a highly uniform distributed magnetic field. It seems that it was done.

(発明が解決しようとする問題点) MRI装置では、円形コイルとして通常は超電導コイル
を用い、患者はこの超電導コイルの中心部における高均
一の磁界中にて診断を受けることになるので、コイルの
軸方向長さが短いほど患者に不安感を与えないで済む。
(Problems to be Solved by the Invention) In an MRI apparatus, a superconducting coil is usually used as the circular coil, and the patient is diagnosed in a highly uniform magnetic field at the center of the superconducting coil. The shorter the axial length, the less anxiety the patient will feel.

しかしながら、従来のコイル装置はコイルの軸方向長さ
が大きいために患者に不安感を与えるという問題点があ
った。
However, the conventional coil device has a problem in that the length of the coil in the axial direction is large, giving the patient a sense of anxiety.

また、従来のコイル装置では、コイルの軸方向長さが大
きいために、コイルのff1faが増えるという問題点
もあった。
Further, in the conventional coil device, since the length of the coil in the axial direction is large, there is also a problem that the ff1fa of the coil increases.

本発明は上記の問題点を解決するためになされたもので
、患者の不安感を払拭し1!?、史せて、コイル小爪を
著しく軽減することのできるコイル装置の提供を目的と
する。
The present invention was made to solve the above-mentioned problems, and eliminates patients' feelings of anxiety. ? The purpose of the present invention is to provide a coil device that can significantly reduce the occurrence of small coil claws.

〔発明の構成〕[Structure of the invention]

(問題点を解決するための手段) 本発明は、それぞれ中心軸が一致するように配置される
と共に、前記中心軸上に仮定した原点を合み且つこの中
心軸に垂直な仮想平面に対称に配置された複数の円形コ
イルを備えたコイル装置において、前記原点から見て軸
方向最外側端の前記円形コイルの径方向内側の縁と前記
原点とを結ぶ仮想線分が、前記中心軸に対して34.5
度以上、63.4度以下の角度範囲に収まるように前記
円形コイルを配置したことを特徴とするものである。
(Means for Solving the Problem) The present invention is arranged such that their central axes coincide with each other, and the assumed origin is aligned with the central axis and is symmetrical with respect to a virtual plane perpendicular to the central axis. In a coil device including a plurality of circular coils arranged, an imaginary line segment connecting the radially inner edge of the circular coil at the outermost end in the axial direction when viewed from the origin and the origin is relative to the central axis. te 34.5
The present invention is characterized in that the circular coils are arranged so as to fall within an angular range of 63.4 degrees or more.

(作 用) 一般に、中心軸が一致するように配置されると共に、中
心軸上に仮定した原点を含み且つこの中心軸に垂直な仮
想平面に対称に配置された複数の円形コイルを備えたコ
イル装置においては、軸方向外側端の径方向内側のコイ
ル縁と原点とを結ぶ仮想線分が中心軸に対してどのよう
な角度範囲にあるかによって分布磁界の均一度が異なる
他、上述した磁界の展開式中の係数a2nの符舅が反対
になったりする。
(Function) Generally, a coil is provided with a plurality of circular coils that are arranged so that their central axes coincide, that include an assumed origin on the central axis, and that are symmetrically arranged on a virtual plane perpendicular to the central axis. In the device, the uniformity of the distributed magnetic field differs depending on the angle range of the virtual line connecting the radially inner coil edge of the axially outer end and the origin with respect to the central axis. The sign of the coefficient a2n in the expansion equation may be reversed.

今、仮想線分がZ軸となす角をθとし、角度θを横軸、
磁界分布を乱す誤差を縦軸として両者の関係を表わすと
第2図のようになる。すなわち、角度θが34°のとき
誤差は約−5ppm  (ppmは誤差磁界/中心磁界
を106倍した値)で、角α0が35°のとき誤差は約
5 ppmであり、磁界の誤差はこの二点を結ぶ直線に
従って変化すること、および、角度θが34.5°の近
くで誤差が零になることが発明者等の実験により明らか
になっている。
Now, the angle that the virtual line segment makes with the Z axis is θ, and the angle θ is the horizontal axis,
The relationship between the two is shown in FIG. 2, with the vertical axis representing the error that disturbs the magnetic field distribution. In other words, when the angle θ is 34°, the error is approximately -5 ppm (ppm is the value obtained by multiplying the error magnetic field/center magnetic field by 106), and when the angle α0 is 35°, the error is approximately 5 ppm, and the error in the magnetic field is Experiments conducted by the inventors have revealed that the error changes along a straight line connecting two points, and that the error becomes zero when the angle θ is close to 34.5°.

したがって、角度Oを34.5°にすることが最良では
あるものの、少イ【りともこの角度以下にすることはコ
イルの軸方向長さを無駄に長くすることに他ならない。
Therefore, although it is best to set the angle O to 34.5°, making it at least less than this angle is nothing but an unnecessarily long axial length of the coil.

一方、角度θが63.4°を越えると、上述した係数a
2が負になって、コイルに供給する電流の方向を逆にす
る必要性が生じ、その分だけ線材のtが増大することに
なる。
On the other hand, when the angle θ exceeds 63.4°, the above-mentioned coefficient a
2 becomes negative, it becomes necessary to reverse the direction of the current supplied to the coil, and the t of the wire increases by that amount.

そこで、本発明は、角度θが略34.5°以上、63.
4°以下の角度範囲に収まるように円形コイルを配置す
ることにより、患者の不安感を払拭すると共に、コイル
重囲の軽減を図るようにしている。
Therefore, in the present invention, the angle θ is approximately 34.5° or more, 63.
By arranging the circular coils within an angular range of 4 degrees or less, the patient's sense of anxiety is eliminated and the coil surroundings are reduced.

(実施例) 第1図は本発明の一実施例の構成を示す縦断面図である
。同図において、円形コイル(以下、単にコイルと言う
)1.1’および2は、それぞれ超電導体を巻枠3上に
巻回したもので、このうち、コイル2はコイル1.1′
の中間に配置されている。
(Embodiment) FIG. 1 is a longitudinal sectional view showing the configuration of an embodiment of the present invention. In the same figure, circular coils (hereinafter simply referred to as coils) 1.1' and 2 are superconductors wound on a winding frame 3, and among these, coil 2 is a coil 1.1'.
is placed in the middle.

この場合、コイル1,1′および2は円筒状の巻枠3に
巻かれており、コイル1.1′はコイル2の両側に対称
に配置されている。
In this case, the coils 1, 1' and 2 are wound on a cylindrical bobbin 3, the coils 1.1' being arranged symmetrically on both sides of the coil 2.

今、巻枠3の中心軸、すなわら、コイル1゜1′および
2の中心軸を7、コイル2の中心、すなわち原点をOl
この原点Oを含み、ZIIlIlに重直な仮想平面をR
とする。また、原点0より見て、Z軸方向の最外側にJ
3けるコイル1の(¥方向内側の縁4と原点Oとを結ぶ
線分を仮想線分りとし、この仮想線分りとZ軸とのなす
角をθとづる。
Now, the central axis of winding frame 3, that is, the central axis of coils 1°1' and 2, is 7, and the center of coil 2, that is, the origin, is 7.
A virtual plane that includes this origin O and is perpendicular to ZIIlIl is R
shall be. Also, when viewed from the origin 0, there is a J on the outermost side in the Z-axis direction.
The line segment connecting the inner edge 4 of the coil 1 in the 3rd direction and the origin O is defined as an imaginary line segment, and the angle between this imaginary line segment and the Z-axis is defined as θ.

ここで、コイル1.1′および2はそれぞれ中心軸が一
致するように配置され、さらに、仮想平面Rに対称に配
置されている。また、角度θは略34.5′以上、63
.4度以下の範囲に収まるようにコイル1.1′が配置
されている。
Here, the coils 1.1' and 2 are arranged so that their central axes coincide with each other, and furthermore, they are arranged symmetrically about the virtual plane R. Also, the angle θ is approximately 34.5' or more, 63
.. The coil 1.1' is arranged so as to fall within a range of 4 degrees or less.

かかる構成により、原点Oを含む所定の空間5の磁界に
、負の誤差成分が含まれることを防止し、しか−b、上
記(4)式の関数fの符号の変化に対応して電流の向き
を逆にする必要性を除去している。
With this configuration, it is possible to prevent negative error components from being included in the magnetic field in the predetermined space 5 including the origin O, and it is possible to prevent the current from being included in the magnetic field in the predetermined space 5 including the origin O. Eliminating the need to reverse orientation.

この結果、コイルの軸方向長さを抑えて患者の不安感を
払拭すると共に、コイル重量のli’f減が図られてい
る。
As a result, the length of the coil in the axial direction is suppressed to eliminate the patient's sense of anxiety, and the weight of the coil is reduced.

なお、1−記実施例では3個のコイルを用いたが、多数
のコイルであっても、要は、中心軸を一致させて仮想平
面Rに対して対称に配置し、角度θが略34.5°以上
、63.4°以下の範囲に収まるように配置しておけば
、上jホしたと同様な効果が19られることは明らかで
ある。
Although three coils were used in Example 1-1, even if there are a large number of coils, the key is to align the central axes and arrange them symmetrically with respect to the virtual plane R, so that the angle θ is approximately 34. It is clear that the same effect as described above can be obtained by arranging the angle within the range of .5° or more and 63.4° or less.

第3図は本発明の他の実施例の構成を示す縦断面図であ
り、仮想、平面Rに対してコイル2、コイル6.6’ 
、コイル1.1′を対称に配置しているが、原点Oを囲
むように配置したコイル2の内径が最も小さく、原点O
より見てZ軸方向外側のコイルはど、その内径を犬ぎく
している。なお、この場合も角度θは略34.5°以上
、63.4°以下に収まるようなコイル形状とコイル配
置になっている。
FIG. 3 is a longitudinal cross-sectional view showing the configuration of another embodiment of the present invention, in which coil 2, coil 6.6'
, the coils 1 and 1' are arranged symmetrically, but the inner diameter of the coil 2, which is arranged so as to surround the origin O, is the smallest, and the inner diameter of the coil 2 that surrounds the origin O is the smallest.
If you look closely, the inner diameter of the outer coil in the Z-axis direction is narrower. In this case as well, the coil shape and coil arrangement are such that the angle θ is approximately 34.5° or more and 63.4° or less.

かかる構成によれば、中央部のコイルの内径を小さくし
た分だけ、さらに、litを軽減することができろ。
According to such a configuration, it is possible to further reduce the lit by reducing the inner diameter of the central coil.

次に、第4図は本発明のもう一つ他の実施例の構成を示
1縦斯面図である。同図において、コイル2、コイル6
.6′およびコイル1.1′は仮想平面Rに対して対称
に配置されているが、原点0を囲むように配置されたコ
イル2の内径が最も大きく、Z軸方向外側のコイルはど
、その内径が小さくなっている。なお、この場合も角度
θは略34.5′以上、63.4°以下に収まるような
コイル形状とコイル配置になっている。
Next, FIG. 4 is a longitudinal sectional view showing the structure of another embodiment of the present invention. In the same figure, coil 2, coil 6
.. 6' and coils 1.1' are arranged symmetrically with respect to the virtual plane R, but coil 2, which is arranged so as to surround the origin 0, has the largest inner diameter, and the outer coil in the Z-axis direction has the largest inner diameter. The inner diameter is smaller. In this case as well, the coil shape and coil arrangement are such that the angle θ is approximately 34.5' or more and 63.4° or less.

この]イル装置は、上記第1図に示したコイル装置と比
べて、Z軸方向外側のコイル1.1′の内径を小さくし
た分だけ中心のコイル2の内径を大きくした形になって
おり、コイルff1fflが同一であったとしても、患
者が置かれる周囲の空間が著しく拡げられ、これによっ
て患者の不安感を確実に除去することができる。
Compared to the coil device shown in Fig. 1 above, this coil device has a shape in which the inner diameter of the central coil 2 is increased by the smaller inner diameter of the outer coil 1.1' in the Z-axis direction. Even if the coils ff1ffl are the same, the surrounding space in which the patient is placed is significantly expanded, thereby reliably eliminating the patient's sense of anxiety.

なお、角度θが同じである場合、第1図および第3図に
それぞれ示したコイル装置に比べて、第4図に示したコ
イル装置の軸方向長さが最も短くなる。したがって、こ
の面でも患者の不安感を和らげることができる。
Note that when the angle θ is the same, the axial length of the coil device shown in FIG. 4 is the shortest compared to the coil devices shown in FIGS. 1 and 3, respectively. Therefore, in this aspect as well, the patient's anxiety can be alleviated.

〔発明の効果〕〔Effect of the invention〕

以上の説明によって明らかなように、この発明によれば
、軸方向外側端の円形コイルの径方向内側の縁と原点と
を結ぶ仮想線分が、中心軸に対して略34.5°以上、
63.4°以下の角度範囲に収まるように円形コイルを
配置したので、この装置を区療用MRI装首等に適用し
た場合に、患者に与える不安感を確実に除去し1.7る
と共に、コイル手足を軽減して、いわゆる、コンパクト
化しjりるという効果がある。
As is clear from the above description, according to the present invention, the virtual line segment connecting the radially inner edge of the circular coil at the axially outer end and the origin is approximately 34.5 degrees or more with respect to the central axis.
Since the circular coil is arranged within an angle range of 63.4 degrees or less, when this device is applied to MRI neck straps for medical treatment, it can reliably eliminate the feeling of anxiety caused to patients. This has the effect of reducing the number of coil limbs and making it more compact.

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

第1図は本発明の一実施例の縦断面図、第2図は本発明
の詳細な説明するために、円形コイルに接するように引
いた仮想線分のなす角度と磁界の誤差との関係を示す線
図、第3図は本発明の他の実施例の縦断面図、第4図は
本発明のもう一つ仙の実施例の縦断面図である。 1.1’ 、2.2’ 、6.6’ ・・・円形コイル
、3・・・巻枠、O・・・原点、Z・・・中心軸、R・
・・仮想平面、L・・・仮想線分。 出願人代理人  佐  藤  −雄 ち 1 図
FIG. 1 is a longitudinal cross-sectional view of an embodiment of the present invention, and FIG. 2 is a diagram showing the relationship between the angle formed by a virtual line segment drawn so as to be in contact with a circular coil and the error in the magnetic field, in order to explain the present invention in detail. FIG. 3 is a longitudinal cross-sectional view of another embodiment of the present invention, and FIG. 4 is a longitudinal cross-sectional view of another embodiment of the present invention. 1.1', 2.2', 6.6'...Circular coil, 3...Reeling frame, O...Origin, Z...Center axis, R...
...Virtual plane, L...Virtual line segment. Applicant's agent Yuchi Sato 1 Figure

Claims (1)

【特許請求の範囲】[Claims]  それぞれ中心軸が一致するように配置されると共に、
前記中心軸上に仮定した原点を含み且つこの中心軸に垂
直な仮想平面に対称に配置された複数の円形コイルを備
えたコイル装置において、前記原点から見て軸方向最外
側端の前記円形コイルの径方向内側の縁と前記原点とを
結ぶ仮想線分が、前記中心軸に対して略34.5度以上
、63.4度以下の角度範囲に収まるように前記円形コ
イルを配置したことを特徴とするコイル装置。
They are arranged so that their central axes coincide, and
In a coil device comprising a plurality of circular coils that include a hypothetical origin on the central axis and are arranged symmetrically on a virtual plane perpendicular to the central axis, the circular coil at the outermost end in the axial direction when viewed from the origin The circular coil is arranged such that a virtual line connecting the radially inner edge of the coil and the origin falls within an angle range of approximately 34.5 degrees or more and 63.4 degrees or less with respect to the central axis. Characteristic coil device.
JP61161188A 1986-07-09 1986-07-09 Coil equipment Pending JPS6316604A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61161188A JPS6316604A (en) 1986-07-09 1986-07-09 Coil equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61161188A JPS6316604A (en) 1986-07-09 1986-07-09 Coil equipment

Publications (1)

Publication Number Publication Date
JPS6316604A true JPS6316604A (en) 1988-01-23

Family

ID=15730259

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61161188A Pending JPS6316604A (en) 1986-07-09 1986-07-09 Coil equipment

Country Status (1)

Country Link
JP (1) JPS6316604A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5396208A (en) * 1990-06-08 1995-03-07 U.S. Philips Corporation Magnet system for magnetic resonance imaging
JP2008086582A (en) * 2006-10-03 2008-04-17 Hitachi Metals Ltd Magnetic field generator
JP2009216424A (en) * 2008-03-07 2009-09-24 Kobe Steel Ltd Magnet position measuring method and magnetic field measuring instrument

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61100644A (en) * 1984-10-24 1986-05-19 Hitachi Ltd Electromagnet for generating uniform magnetic field

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61100644A (en) * 1984-10-24 1986-05-19 Hitachi Ltd Electromagnet for generating uniform magnetic field

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5396208A (en) * 1990-06-08 1995-03-07 U.S. Philips Corporation Magnet system for magnetic resonance imaging
JP2008086582A (en) * 2006-10-03 2008-04-17 Hitachi Metals Ltd Magnetic field generator
JP2009216424A (en) * 2008-03-07 2009-09-24 Kobe Steel Ltd Magnet position measuring method and magnetic field measuring instrument

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