JPS6213008A - Uniform magnetic field generator - Google Patents

Uniform magnetic field generator

Info

Publication number
JPS6213008A
JPS6213008A JP60152816A JP15281685A JPS6213008A JP S6213008 A JPS6213008 A JP S6213008A JP 60152816 A JP60152816 A JP 60152816A JP 15281685 A JP15281685 A JP 15281685A JP S6213008 A JPS6213008 A JP S6213008A
Authority
JP
Japan
Prior art keywords
coil
coils
magnetic field
uniform magnetic
turns
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
JP60152816A
Other languages
Japanese (ja)
Inventor
Takahisa Nishikawa
西川 隆久
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 JP60152816A priority Critical patent/JPS6213008A/en
Publication of JPS6213008A publication Critical patent/JPS6213008A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To compose a magnet having a short axial direction by deciding the ratio of radii of inner, intermediate and outer coils to a distance from the central position, and the ratio of the numbers of windings of the inner, intermediate and outer coils to the prescribed values. CONSTITUTION:Three coil pairs composed of two coils having equal number of windings disposed on a central axis are disposed symmetrically to the central position. When the radii of inner coils 1, 2 of three coil pairs having substantially equal radii of the center of the sections of the coils are 0.5 and the number of windings of the inner coils is N1, the radii of the intermediate coils 3, 4 and the outer coils 5, 6 fall within 0.5+ or -0.05. The distances between the inner, intermediate and outer coils and the central position A fall respectively 0.0510+ or -0.0080, 0.2018+ or -0.0200, 0.5304+ or -0.0400, and the numbers of the windings of the intermediate and outer coils fall respectively within N1X(1.902+ or -0.200), N1X(5.258+ or -0.600).

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は、均一磁界発生装置に関し、例えばNMRCT
装置に用いられるものである。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a uniform magnetic field generator, for example, NMRCT.
It is used for equipment.

〈従来の技術〉 従来、高均一磁場を発生させる超電導マグネットにおけ
る線材の巻き方は、第2図に示すソレノイドコイル方式
あるいは第3図に示すソレノイドコイルとノツチコイル
の組み合わせ方式がとられていた。
<Prior Art> Conventionally, the method of winding a wire in a superconducting magnet that generates a highly uniform magnetic field has been the solenoid coil method shown in FIG. 2 or the combination method of a solenoid coil and a notch coil shown in FIG. 3.

〈発明が解決しようとする問題点〉 上述の磁界発生装置の欠点は、高均一磁場を得るために
は軸方向(Z方向)に長いマグネットになってしまうこ
とである。
<Problems to be Solved by the Invention> A drawback of the above-described magnetic field generator is that in order to obtain a highly uniform magnetic field, the magnet becomes long in the axial direction (Z direction).

このため、この超電導マグネットを用いたNMRCT装
置においては、人間が入る内ボアーが奥の深い穴になり
、患者に恐怖感を与えるとともに、アンテナの設置その
他の点で取り扱いにくいものになっていた。また、コイ
ルの線材も大量に必要とし、線材が高価であることから
、NMRCT装置のコストが高くなるという問題点を有
していた。
For this reason, in an NMRCT device using this superconducting magnet, the inner bore into which a person enters is a deep hole, which gives a sense of fear to the patient and makes it difficult to handle in terms of antenna installation and other aspects. Further, since a large amount of coil wire is required and the wire is expensive, there is a problem in that the cost of the NMRCT apparatus increases.

〈問題点を解決する為の手段〉 本発明の均一磁界発生装置は、中心軸上に配置した巻数
が等しい2個のコイルから構成されるコイル対を3対中
心位置に関し対称に配置した磁界発生装置であって、各
々のコイルの断面中心半径が略同一である上記3対のコ
イル対の内コイルの上記半径を0.5とし、この内コイ
ルの巻数をN1としたときに、上記3対のコイル対の中
コイルと外コイルの上記半径が0.5±0.05の範囲
にあり、上記内コイル、中コイル並びに外コイルと上記
中心位置との間の距離が各々0.0510±0.008
0.0.2018±0.0200.0.5304±0.
0400の範囲にあり、上記中コイルと外コイルの巻数
が各々N、+ x (1,902±0.200 ) 、
 NI X (5,258±0.600 ”)の範囲に
あることを特徴としている。
<Means for Solving the Problems> The uniform magnetic field generating device of the present invention generates a magnetic field by arranging three pairs of coils, each consisting of two coils having the same number of turns arranged on the central axis, symmetrically with respect to the center position. In the apparatus, when the radius of the coil among the three coil pairs is set to 0.5 and the number of turns of the inner coil is set to N1, the three pairs of coils have substantially the same cross-sectional center radius. The radius of the middle coil and outer coil of the coil pair is in the range of 0.5±0.05, and the distance between the inner coil, middle coil, and outer coil and the center position is 0.0510±0, respectively. .008
0.0.2018±0.0200.0.5304±0.
0400, and the number of turns of the middle coil and outer coil is N, + x (1,902±0.200), respectively.
It is characterized by being in the range of NI x (5,258±0.600'').

〈実施例〉 以下、本発明の一実施例について説明する。<Example> An embodiment of the present invention will be described below.

第1図は均一磁界発生装置のマグネットの断面構成を示
す。2個の内コイル1.2からなる内コイル対と、2個
の中コイル3.4からなる中コイル対と、2個の外コイ
ル5.6からなる外コイル対の3対のコイル対が、支持
部材7により軸Zlに同軸状に且つ均一磁界発生装置の
中心位置Aについて対称に配置される。内コイル1.2
は中心位置AからZ軸方向に左右に距離d1の位置にそ
れぞれ配置され、中コイル3.4は中心位NAからZ軸
方向に左右に距離d2の位置にそれぞれ配置され、外コ
イル5.6は中心位置AからZ軸方向に左右に距離d3
の位置にそれぞれ配置される。
FIG. 1 shows a cross-sectional configuration of a magnet of a uniform magnetic field generator. There are three coil pairs: an inner coil pair consisting of two inner coils 1.2, a middle coil pair consisting of two middle coils 3.4, and an outer coil pair consisting of two outer coils 5.6. , are arranged coaxially with the axis Zl by the support member 7 and symmetrically about the center position A of the uniform magnetic field generator. Inner coil 1.2
are arranged at distances d1 left and right in the Z-axis direction from the center position A, middle coils 3.4 are arranged at distances d2 left and right in the Z-axis direction from the center position NA, and outer coils 5.6 is the distance d3 left and right in the Z-axis direction from the center position A.
are placed at the respective positions.

距Md2は距離d1より大であり、距Mdaは距離d2
より大である。コイル1.、 2. 3. 4.、 5
゜6の断面中心半径はa、内コイル1.2の巻数はNl
、中コイル3,4の巻数はN2.外コイル5゜6の巻数
はN3である。
Distance Md2 is greater than distance d1, and distance Mda is greater than distance d2.
It's bigger. Coil 1. , 2. 3. 4. , 5
The center radius of the cross section of °6 is a, and the number of turns of the inner coil 1.2 is Nl
, the number of turns of the middle coils 3 and 4 is N2. The number of turns of the outer coil 5°6 is N3.

この磁界発生装置で均一な磁界とは、Z軸での均一性が
高い磁界である。それ故、Z軸上の磁界の強さH(Zl
をZの巾の級数として、H(Zl=fo+f2 Z2+
f4Z’ +f6 Z6 +・・・−(ll と表したとき(コイル配置は対称であるからZの奇数束
の項は現れない)、係数f2.f4.f5・・・がほぼ
零となるようにする必要がある。本発明においては、f
2およびf4を概略零となるようにし、f6が最も小さ
な値を待つようにすることにより、Zが充分小さい範囲
で均一な磁界を実現する。
A uniform magnetic field in this magnetic field generator is a magnetic field with high uniformity in the Z axis. Therefore, the magnetic field strength H (Zl
As a series of the width of Z, H(Zl=fo+f2 Z2+
When expressed as f4Z' +f6 Z6 +...-(ll (the coil arrangement is symmetrical, the odd bundle term of Z does not appear), so that the coefficients f2.f4.f5... are almost zero. In the present invention, f
By setting 2 and f4 to approximately zero and waiting for the smallest value of f6, a uniform magnetic field is realized in a sufficiently small range of Z.

内コイル対を構成するコイル1,2によりZ軸上に発生
する磁場H(d+、NI、Z)は、中コイル対を構成す
るコイル3.4によりZ軸上に発生する磁場H(d2.
N2.Z)は、外コイル対を構成するコイル5.6によ
りZ軸上に発生する磁場H(da、Na、Z)は、で表
わされる。
The magnetic field H (d+, NI, Z) generated on the Z-axis by coils 1 and 2 forming the inner coil pair is equal to the magnetic field H (d2.
N2. Z) is a magnetic field H (da, Na, Z) generated on the Z axis by the coil 5.6 forming the outer coil pair.

したがって、各々のコイルが2軸上に発生する磁界の強
さを総合すると、H(Zlは次式のようになる。
Therefore, when the strength of the magnetic field generated by each coil on the two axes is combined, H(Zl is as shown in the following equation.

(2)式をティラー展開して(11式を得る。この場合
、係数fn (n=0.2,4,6.=)は、次式で求
められる。
Equation (2) is expanded by Tiller to obtain Equation 11. In this case, the coefficient fn (n=0.2, 4, 6.=) is determined by the following equation.

nj   dz” 合のZ=0における値である。nj dz” This is the value at Z=0.

上述の均一な磁界を実現する条件は次のように書くこと
ができる。
The conditions for realizing the above-mentioned uniform magnetic field can be written as follows.

が最小となること  °°°−θJ +41. (51,+6)の条件を満たすように定数a
+dl+d2.da、N! 、N2.Naを定めること
により、均一な磁界を得る。
is the minimum °°°−θJ +41. Constant a so as to satisfy the condition (51, +6)
+dl+d2. Da, N! , N2. By determining Na, a uniform magnetic field can be obtained.

この6コイル方式の場合、Z軸上の磁場は、H(z)c
(H(d+ 、N1.Z)+H(dz、N2.Z)+H
(da、Na、Z)で表わすことができる。したがって
、Z軸上のいくつかの点をサンプルポイントとしてパラ
メータd+ 、N+ 、dz、N2.da、Naを種々
変えることにより、Z軸上の中心位置Aに近いサンプル
ポイントで均一な磁界となるパラメータd1゜N1.d
z、N2.da、Naを見出すことができる。
In the case of this 6-coil system, the magnetic field on the Z axis is H(z)c
(H(d+,N1.Z)+H(dz,N2.Z)+H
It can be expressed as (da, Na, Z). Therefore, some points on the Z axis are taken as sample points and the parameters d+, N+, dz, N2 . By varying da and Na, the parameters d1°N1. d
z, N2. da, Na can be found.

均一磁界を得るために上述の方法により求めたパラメー
タの比率は、次のとおりである。内コイル1.2の断面
中心半径aを0.5とし、この内コイル1.2の巻数を
N1とすると、中コイル3゜4と外コイル5,6の断面
中心部半径が0.5±0.05の範囲にあり、内コイル
1,2.中コイル3. 4並びに外コイル5,6と中心
位置Aとの間の距離dl、d2.daが各々0.051
0±0.0080.0.2018±0.0200.0.
5304±0.0400の範囲にあり、中コイル3,4
と外コイル5,6の巻数N2.N3が各N+ X (1
,902±0.200 ) 、 N+ X (5,25
8±o、eoo >の範囲にある。この場合、あるパラ
メーターを少し変化させると他のパラメータの最適値も
少しづつ変化するので、上述のようにある程度の範囲を
定めている。
The ratios of the parameters determined by the above method to obtain a uniform magnetic field are as follows. If the cross-sectional center radius a of the inner coil 1.2 is 0.5 and the number of turns of the inner coil 1.2 is N1, then the cross-sectional center radius of the middle coil 3°4 and the outer coils 5 and 6 is 0.5±. It is in the range of 0.05, and the inner coils 1, 2 . Medium coil 3. 4 and the distances dl, d2 . between the outer coils 5, 6 and the center position A. da is 0.051 each
0±0.0080.0.2018±0.0200.0.
5304±0.0400, medium coil 3,4
and the number of turns N2 of the outer coils 5 and 6. N3 is each N+X (1
,902±0.200), N+X(5,25
It is in the range of 8±o, eoo>. In this case, if a certain parameter is slightly changed, the optimum values of other parameters will also change little by little, so a certain range is defined as described above.

このように、コイル1,2,3,4,5.6の断面中心
半径aと中心位置Aとの間の距離dIta2.a3との
比率およびコイル1,2の巻数N1とコイル3,4の巻
数N2およびコイル5,6の巻数N3との比率を定める
と、Z軸上で均一な磁界が得られる。上述のようにパラ
メータを設定して計算シミュレーションを行った結果、
中心位買入から半径25cmの球状空間の内部で磁場の
均一度は60ppmであった。
In this way, the distance dIta2 . A3 and the ratio between the number of turns N1 of the coils 1 and 2, the number of turns N2 of the coils 3 and 4, and the number of turns N3 of the coils 5 and 6 are determined to obtain a uniform magnetic field on the Z-axis. As a result of setting the parameters as described above and performing a calculation simulation,
The uniformity of the magnetic field was 60 ppm inside a spherical space with a radius of 25 cm from the center point.

なお、第1図に示すコイルの断面形状は正方形であるが
、これは長方形又は円形等であってもよいことは言うま
でもない。
Although the cross-sectional shape of the coil shown in FIG. 1 is square, it goes without saying that it may be rectangular or circular.

〈発明の効果〉 以上説明したように、本発明においては、内コイル、中
コイル並びに外コイルの半径と中心位置からの距離との
比率および内コイル、中コイル並びに外コイルの巻数比
を所定値に定めたことにより、軸方向に短いマグネット
を構成することができ、同半径の従来のマグネットに比
べて約3/4に小さくすることができるとともに、線材
も従来の約3/4程度に減らすことができるので、コス
トダウンが達成できる。さらに、このマグネットを超電
導マグネットに適用した場合、小型化できることから周
囲からの放射熱の吸収が少なくなり、運転に要するエネ
ルギーを少なくすることができる。さらに、このマグネ
ットを用いたNMRCT装置においては、人間が入る内
ボアーが浅くなり、患者に恐怖感を与えることがない。
<Effects of the Invention> As explained above, in the present invention, the ratio of the radius of the inner coil, middle coil, and outer coil to the distance from the center position and the turn ratio of the inner coil, middle coil, and outer coil are set to predetermined values. By setting this, it is possible to construct a magnet that is short in the axial direction, making it about 3/4 smaller than a conventional magnet with the same radius, and also reducing the wire material to about 3/4 of the conventional magnet. As a result, cost reduction can be achieved. Furthermore, when this magnet is applied to a superconducting magnet, it can be miniaturized, which reduces the absorption of radiant heat from the surroundings and reduces the energy required for operation. Furthermore, in the NMRCT apparatus using this magnet, the inner bore into which a person enters is shallow, so that the patient does not feel scared.

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

第1図は本発明実施例の概略断面構成を示す図、第2図
と第3図は従来例の断面構成を示す図である。 1.2・・・内コイル 3.4・・・中コイル 5.6・・・外コイル A・・・中心位置 a・・・断面中心半径 dl、a2.d3・・・距離 特許出願人  株式会社島津製作所 代 理 人  弁理士  西1)新 第1回 第2UiJ         第3図 −−−一−→2 −−一→2
FIG. 1 is a diagram showing a schematic cross-sectional configuration of an embodiment of the present invention, and FIGS. 2 and 3 are diagrams showing a cross-sectional configuration of a conventional example. 1.2... Inner coil 3.4... Middle coil 5.6... Outer coil A... Center position a... Section center radius dl, a2. d3... Distance patent applicant Shimadzu Corporation Representative Patent attorney Nishi 1) New 1st 2nd UiJ Figure 3 ---1-→2 --1-→2

Claims (1)

【特許請求の範囲】[Claims]  中心軸上に配置した巻数が等しい2個のコイルから構
成されるコイル対を3対中心位置に関し対称に配置した
磁界発生装置であって、各々のコイルの断面中心半径が
略同一である上記3対のコイル対の内コイルの上記半径
を0.5とし、この内コイルの巻数をN_1としたとき
に、上記3対のコイル対の中コイルと外コイルの上記半
径が0.5±0.05の範囲にあり、上記内コイル、中
コイル並びに外コイルと上記中心位置との間の距離が各
々0.0510±0.0080、0.2018±0.0
200、0.5304±0.0400の範囲にあり、上
記中コイルと外コイルの巻数が各々N_1×(1.90
2±0.200)、Ni×(5.258±0.600)
の範囲にあることを特徴とする均一磁界発生装置。
3. A magnetic field generating device in which three pairs of coils each consisting of two coils having the same number of turns arranged on a central axis are arranged symmetrically with respect to the center position, and the cross-sectional center radius of each coil is approximately the same. When the radius of the inner coil of the pair of coils is 0.5 and the number of turns of the inner coil is N_1, the radius of the inner coil and outer coil of the three coil pairs is 0.5±0. 05, and the distances between the inner coil, middle coil, and outer coil and the center position are 0.0510±0.0080 and 0.2018±0.0, respectively.
200, 0.5304±0.0400, and the number of turns of the middle coil and outer coil are each N_1×(1.90
2±0.200), Ni×(5.258±0.600)
A uniform magnetic field generator characterized in that the magnetic field is within the range of .
JP60152816A 1985-07-10 1985-07-10 Uniform magnetic field generator Pending JPS6213008A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60152816A JPS6213008A (en) 1985-07-10 1985-07-10 Uniform magnetic field generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60152816A JPS6213008A (en) 1985-07-10 1985-07-10 Uniform magnetic field generator

Publications (1)

Publication Number Publication Date
JPS6213008A true JPS6213008A (en) 1987-01-21

Family

ID=15548782

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60152816A Pending JPS6213008A (en) 1985-07-10 1985-07-10 Uniform magnetic field generator

Country Status (1)

Country Link
JP (1) JPS6213008A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6822451B2 (en) 2002-07-31 2004-11-23 Ge Medical Systems Global Technology Company Llc Non-coupling magnetic sheilding coil
JP2007180344A (en) * 2005-12-28 2007-07-12 Nec Tokin Corp Magnetic field generating coil
JP2008141209A (en) * 2007-12-20 2008-06-19 Mitsubishi Electric Corp Superconducting magnet device
US7553783B2 (en) 2003-12-01 2009-06-30 Uni-Charm Corporation Cleaning sheet
US7735180B2 (en) 2004-06-03 2010-06-15 Uni-Charm Corporation Cleaning sheet

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6822451B2 (en) 2002-07-31 2004-11-23 Ge Medical Systems Global Technology Company Llc Non-coupling magnetic sheilding coil
US7553783B2 (en) 2003-12-01 2009-06-30 Uni-Charm Corporation Cleaning sheet
US7735180B2 (en) 2004-06-03 2010-06-15 Uni-Charm Corporation Cleaning sheet
JP2007180344A (en) * 2005-12-28 2007-07-12 Nec Tokin Corp Magnetic field generating coil
JP2008141209A (en) * 2007-12-20 2008-06-19 Mitsubishi Electric Corp Superconducting magnet device

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