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JPH0821498B2 - Magnetic field generator for MRI - Google Patents
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JPH0821498B2 - Magnetic field generator for MRI - Google Patents

Magnetic field generator for MRI

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Publication number
JPH0821498B2
JPH0821498B2 JP2004685A JP468590A JPH0821498B2 JP H0821498 B2 JPH0821498 B2 JP H0821498B2 JP 2004685 A JP2004685 A JP 2004685A JP 468590 A JP468590 A JP 468590A JP H0821498 B2 JPH0821498 B2 JP H0821498B2
Authority
JP
Japan
Prior art keywords
magnetic field
permanent magnet
field generator
magnet
gap
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.)
Expired - Lifetime
Application number
JP2004685A
Other languages
Japanese (ja)
Other versions
JPH03209803A (en
Inventor
秀也 桜井
雅昭 青木
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.)
Proterial Ltd
Original Assignee
Sumitomo Special Metals Co Ltd
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Application filed by Sumitomo Special Metals Co Ltd filed Critical Sumitomo Special Metals Co Ltd
Priority to JP2004685A priority Critical patent/JPH0821498B2/en
Publication of JPH03209803A publication Critical patent/JPH03209803A/en
Publication of JPH0821498B2 publication Critical patent/JPH0821498B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 利用産業分野 この発明は、医療用核磁気共鳴断層撮影装置等に用い
られる永久磁石を使用した磁界発生装置の改良に係り、
空隙を形成して対向する一対の単数または複数の磁石セ
グメントからなる永久磁石構成体において、構成体の所
要位置または所要位置の磁石セグメントの空隙方向すな
わち磁化方向の高さを変えて配列し、磁極片を用いずに
均一磁界を発生させ、渦電流発生の減少、軽量化を図っ
た磁界発生装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to improvement of a magnetic field generator using a permanent magnet used in a nuclear magnetic resonance tomography apparatus for medical use,
In a permanent magnet structure comprising a pair of one or more magnet segments facing each other with a gap formed, the magnetic poles are arranged by changing the height of the magnet segment at the required position or at the required position in the void direction, that is, the magnetizing direction. The present invention relates to a magnetic field generator that generates a uniform magnetic field without using a piece to reduce eddy current generation and reduce weight.

背景技術 医療用核磁気共鳴断層撮影装置(以下MRIという)
は、強力な磁界を形成する磁界発生装置の空隙内に、被
検者の一部または全部を挿入して、対象物の断層イメー
ジを得てその組織の性質まで描き出すことができる装置
である。
BACKGROUND ART Medical Magnetic Resonance Tomography (hereinafter referred to as MRI)
Is a device that can insert a part or all of a subject into a void of a magnetic field generator that forms a strong magnetic field, obtain a tomographic image of an object, and depict the properties of the tissue.

上記MRI用の磁界発生装置において、空隙は被検者の
一部または全部が挿入できるだけの広さが必要であり、
かつ鮮明な断層イメージを得るために、通常、空隙内の
撮像視野内には、0.05〜1.5Tでかつ1×10-4以下の精度
を有する安定した強力な均一磁界を形成することが要求
される。
In the above-mentioned magnetic field generator for MRI, the space needs to be wide enough to allow insertion of a part or all of the subject,
In order to obtain a clear tomographic image, it is usually required to form a stable and strong uniform magnetic field with an accuracy of 0.05 to 1.5T and 1 × 10 -4 or less in the imaging field of view in the void. It

MRIに用いる磁界発生装置として、第9図に示す如
く、Fe−B−R系磁石を用いた一対の永久磁石構成体
(1)(1)の各々の一方端に磁極片(2)(2)を固
着して対向させ、他方端を板状継鉄(4)(5)、さら
にこれらを4本の柱状継鉄(6)にて連結し、磁極片
(2)(2)間の空隙(7)内に、静磁界を発生させる
構成が知られている。
As a magnetic field generator used for MRI, as shown in FIG. 9, magnetic pole pieces (2) (2) (2) (2) are provided on one end of each of a pair of permanent magnet constituents (1) (1) using Fe-BR magnets. ) Are fixed and made to face each other, and the other end is connected by plate yokes (4) and (5), and these are further connected by four columnar yokes (6) to form a gap between the pole pieces (2) and (2). A configuration for generating a static magnetic field in (7) is known.

例えば、上記構成において、より安定した均一磁界を
形成するため、磁極片の対向面の各々の周縁部に環状突
起(3)を設け、あるいはさらに磁極片の対向面の各々
の中央部に凸状突起(8)を設けた磁界発生装置が提案
(実開昭60−166110号公報)されている。
For example, in the above structure, in order to form a more stable and uniform magnetic field, an annular protrusion (3) is provided on each peripheral edge of the facing surface of the pole piece, or a convex shape is formed on each central portion of the facing surface of the pole piece. A magnetic field generator provided with a protrusion (8) has been proposed (Japanese Utility Model Laid-Open No. 60-166110).

かかる磁界発生装置では、永久磁石の対向面に磁極片
を設けることにより、均一磁界を得ているが、この構成
では磁極片側面からの漏洩が大きくなり、空隙中の磁界
強度が低下する問題がある。また、磁極片は磁界発生装
置の全重量の10%程度を占めるため、軽量化の妨げにも
なっていた。
In such a magnetic field generator, a magnetic pole piece is provided on the opposing surface of the permanent magnet to obtain a uniform magnetic field. However, with this configuration, leakage from the side surface of the magnetic pole piece becomes large, and the magnetic field strength in the air gap decreases. is there. Further, since the magnetic pole pieces occupy about 10% of the total weight of the magnetic field generator, it has been an obstacle to weight reduction.

一方、空隙内の位置情報を得るために、パルス電流を
印加することによって短時間で所望方向に傾斜した磁界
を発生する傾斜磁界コイル、すなわち、通常X、Y、Z
の3方向に対応する3組のコイル群を各磁極片の近傍に
配置するが、傾斜磁界コイルにより渦電流が発生し、傾
斜磁界が所定の強度に達するのに多くの時間を要する問
題がある。
On the other hand, in order to obtain position information in the air gap, a gradient magnetic field coil that generates a magnetic field inclined in a desired direction in a short time by applying a pulse current, that is, usually X, Y, Z
The three sets of coil groups corresponding to the three directions are arranged near each magnetic pole piece, but there is a problem that an eddy current is generated by the gradient magnetic field coil and it takes a lot of time for the gradient magnetic field to reach a predetermined strength. .

発明の目的 この発明は、上記現状に鑑み提案するもので、磁極片
を用いずに渦電流発生の減少並びに軽量化を図り、かつ
磁極片を用いた構成と同等以上の均一磁界が得られるM
RI用磁界発生装置の提供を目的としている。
SUMMARY OF THE INVENTION The present invention has been proposed in view of the above circumstances, and it is possible to reduce the generation of eddy current and reduce the weight without using a magnetic pole piece, and to obtain a uniform magnetic field equal to or higher than that of a configuration using a magnetic pole piece.
The purpose is to provide a magnetic field generator for RI.

発明の概要 この発明は、MRI用磁界発生装置において、磁極片を
使用することなく、所要空隙内に高精度の均一磁界を発
生する構成を目的に種々検討した結果、配列した複数の
永久磁石の磁化方向長さを部分的に調整するとことによ
り、均一磁界が得られ上記目的を達成できることを知見
しこの発明を完成したものである。
SUMMARY OF THE INVENTION The present invention has variously studied in order to generate a highly accurate uniform magnetic field in a required air gap in a magnetic field generator for MRI without using magnetic pole pieces. The present invention has been completed by finding that a uniform magnetic field can be obtained and the above-mentioned object can be achieved by partially adjusting the length in the magnetization direction.

すなわち、この発明は、 空隙を形成して対向し単数または複数の磁石セグメン
トからなる一対の永久磁石構成体を継鉄で磁気的結合
し、該空隙に磁界を発生させるMRI用磁界発生装置にお
いて、 永久磁石構成体の所要位置または所要位置の磁石セグ
メントが、その磁化方向長さを変えて配列され、該空隙
に均一磁界を発生させることを特徴とするMRI用磁界発
生装置である。
That is, the present invention relates to a magnetic field generator for MRI that magnetically couples a pair of permanent magnet constructs, which are opposed to each other with a gap and are composed of a single or a plurality of magnet segments, by a yoke to generate a magnetic field in the gap. The magnetic field generator for MRI is characterized in that a required position or a magnet segment at a required position of the permanent magnet structure is arranged by changing its magnetization direction length to generate a uniform magnetic field in the gap.

詳述すると、この発明は、前記構成のMRI用磁界発生
装置において、 永久磁石構成体を形成する磁石セグメントが単数の場
合、所要位置の磁石の磁化方向長さを変えるか、あるい
は磁石セグメントが複数の場合、所要の位置の磁石セグ
メントの磁化方向長さを変えて配列され、該空隙に均一
磁界を発生させることを特徴とする。
More specifically, according to the present invention, in the magnetic field generator for MRI having the above-mentioned structure, when the number of the magnet segments forming the permanent magnet structure is single, the magnetizing direction length of the magnet at the required position is changed, or the plurality of magnet segments are provided. In this case, the magnet segments are arranged at different positions with different lengths in the magnetization direction, and a uniform magnetic field is generated in the gap.

さらに、この発明は、永久磁石の磁化方向長さ(空隙
方向高さ)を変えるほか、磁石長さ、磁石幅、磁気特
性、磁石材質のうち、少なくとも1つを変え該空隙に均
一に磁界を発生させることを特徴とする。
Further, according to the present invention, in addition to changing the length of the permanent magnet in the magnetization direction (height in the air gap direction), at least one of the magnet length, magnet width, magnetic characteristics, and magnet material is changed so that a magnetic field is evenly applied to the air gap. It is characterized by generating.

発明の構成 この発明において、磁気回路は、空隙を形成して対向
する一対の永久磁石構成体を継鉄で磁気的結合した構成
であれば、継鉄、永久磁石構成体の磁石形状,寸法、配
列方法などはいかなる構成であってもよく、所要空隙の
大きさ等に応じて、永久磁石構成体の磁気特性、形状寸
法、継鉄の形状寸法等を適宜言選定することが望まし
い。
Configuration of the Invention In the present invention, the magnetic circuit is a configuration in which a pair of permanent magnet constituents facing each other with a gap formed therein are magnetically coupled with a yoke, and the yoke, the magnet shape and dimensions of the permanent magnet constituent, The arrangement method or the like may be any configuration, and it is desirable to appropriately select and select the magnetic characteristics, the shape size, the yoke shape size, etc. of the permanent magnet structure according to the size of the required voids and the like.

この発明は、永久磁石構成体の空隙対向面に磁極片を
設けることなく、所要の空隙に均一磁界を発生させるた
め、複数の永久磁石の磁化方向長さ(空隙方向高さ)を
変えて配列し永久磁石構成体を形成したことを特徴とし
ており、基本的な技術思想は、例えば、同一寸法、特性
の永久磁石で所定の永久磁石構成体を形成し、発生した
所要の空隙内の磁界強度分布を解析し、所要箇所の永久
磁石の磁化方向長さすなわち空隙方向の磁石高さを変
え、該空隙内が均一磁界となるように調整して永久磁石
を配列することにある。
According to the present invention, in order to generate a uniform magnetic field in a required air gap without providing pole pieces on the air gap facing surface of the permanent magnet structure, the magnetizing direction lengths (height in the air gap direction) of the plurality of permanent magnets are arrayed. The basic technical idea is, for example, that a predetermined permanent magnet structure is formed with permanent magnets of the same size and characteristics, and the generated magnetic field strength in the required air gap. This is to analyze the distribution, change the magnetization direction length of the permanent magnets at the required locations, that is, the magnet height in the air gap direction, and adjust the magnets so that a uniform magnetic field is formed in the air gaps.

さらに、この発明において、空隙を形成して対向する
一対の永久磁石構成体は、前述の如く任意の形状を取る
ことができ、この永久磁石構成体を形成する複数の永久
磁石は、前述の如く、永久磁石の磁化方向長さ、すなわ
ち空隙方向の磁石高さを変えるほか、磁石長さ、磁石
幅、磁気特性、磁石材質を変えてもよく、これら磁石を
種々のパターンで配列することができる。
Further, in the present invention, the pair of permanent magnet constituents that form a gap and are opposed to each other can have any shape as described above, and the plurality of permanent magnets forming this permanent magnet constituent are as described above. In addition to changing the magnetizing direction length of the permanent magnet, that is, the magnet height in the air gap direction, the magnet length, magnet width, magnetic characteristics, and magnet material may be changed, and these magnets can be arranged in various patterns. .

この発明は、単数または複数の磁石セグメントからな
る一対の永久磁石構成体の所要位置または所要位置の磁
石セグメントが、その磁化方向長さを変えて配列され、
該空隙に均一磁界を発生させることを特徴とするが、磁
化方向長さを変えて配列する寸法、あるいは永久磁石の
形状、配列パターン等は、軽量化、磁界均一度の向上な
どの主目的や、装置の種々の用途の違い等により、後述
する実施例に示す如く、所要空隙内の磁界強度、均一度
などの解析方法の選択が行われ、かつ前記解析結果と磁
石高さを変える位置や磁石セグメントの選定及び変更量
との具体的関係や、好ましい構成が変わるため、各条件
に応じて、磁石セグメント、磁石の磁化方向長さ等を適
宜選定する必要がある。
According to the present invention, a required position or a required position of a pair of permanent magnet constructions composed of a single or a plurality of magnet segments is arranged by changing its magnetizing direction length.
It is characterized in that a uniform magnetic field is generated in the air gap. However, the dimensions for changing the length in the magnetizing direction, the shape of the permanent magnet, the arrangement pattern, etc. are the main objectives such as weight reduction and improvement of magnetic field uniformity. Depending on various uses of the apparatus, the analysis method such as the magnetic field strength in the required air gap and the homogeneity is selected as shown in the examples described later, and the position of changing the analysis result and the magnet height can be selected. Since the specific relationship with the selection and change amount of the magnet segment and the preferable configuration are changed, it is necessary to appropriately select the magnet segment, the length of the magnetizing direction of the magnet, etc. according to each condition.

かかる磁気回路に用いる単数または複数の磁石セグメ
ントからなる磁石構成体の永久磁石は、フェライト磁
石、アルニコ系磁石、希土類コバルト系磁石が使用でき
るが、特に、RとしてNdやPrを中心とする資源的に豊富
な軽希土類を用い、B、Feを主成分として30MGOe以上の
極めて高いエネルギー積を示す、Fe−B−R系永久磁石
を使用することにより、著しく小型化することができ
る。
Ferrite magnets, alnico magnets, and rare earth cobalt magnets can be used as the permanent magnets of the magnet structure composed of one or a plurality of magnet segments used in such a magnetic circuit. By using abundant light rare earths and using Fe-BR permanent magnets containing B and Fe as the main components and having an extremely high energy product of 30 MGOe or more, the size can be significantly reduced.

図面に基づく発明の開示 第1図a,bはこの発明による磁界発生装置の永久磁石
構成体(下側)を示す説明図である。
Disclosure of the Invention Based on the Drawings FIGS. 1A and 1B are explanatory views showing a permanent magnet structure (lower side) of a magnetic field generator according to the present invention.

第2図aは磁極片のない磁界発生装置の縦断説明図で
あり、同b図は横断説明図である。
FIG. 2a is a vertical cross-sectional explanatory view of a magnetic field generator having no pole piece, and FIG. 2b is a cross-sectional explanatory view thereof.

第3図は磁界発生装置の球体空間内の磁界を測定する
方法を示す空隙の斜視説明図である。
FIG. 3 is a perspective explanatory view of a gap showing a method for measuring a magnetic field in a spherical space of a magnetic field generator.

第4図a〜dはこの発明の永久磁石構成体(上側)の
所要セグメントの磁化方向高さを変化させた例を示す説
明図である。
4A to 4D are explanatory views showing an example in which the magnetization direction height of the required segment of the permanent magnet structure (upper side) of the present invention is changed.

第5図、第6図は第3図の球体空間内のP1〜P7の磁界
不均一度を示すグラフであり、第5図は第9図の従来磁
界発生装置において磁極片を除去した場合、第6図は第
4図a〜dの永久磁石構成体の場合を示す。
5 and 6 are graphs showing the magnetic field inhomogeneities of P 1 to P 7 in the spherical space of FIG. 3, and FIG. 5 shows the conventional magnetic field generator of FIG. 9 with pole pieces removed. In this case, FIG. 6 shows the case of the permanent magnet construction of FIGS.

第7図は第1図aの実施例における球体空間内のP1
P7の磁界不均一度を示すグラフである。
FIG. 7 shows P 1 -in the spherical space in the embodiment of FIG. 1a.
7 is a graph showing the magnetic field inhomogeneity of P 7 .

第8図は最適化したこの発明の永久磁石構成体(上
側)の一実施例を示す説明図である。
FIG. 8 is an explanatory view showing one embodiment of the optimized permanent magnet structure (upper side) of the present invention.

装置構成 ここでは、第2図に示す如く、前述した第9図に示す
磁界発生装置の構成から磁極片(2)(2)を除き、Fe
−B−R系磁石を用いた一対の永久磁石構成体(1)
(1)を対向させ、他方端を長方形の板状継鉄(4)
(5)、さらにこれらを四隅を配設した4本の柱状継鉄
(6)にて連結し、永久磁石構成体(1)(1)間の空
隙(7)内に、静磁界を発生させる構成からなる磁界発
生装置に、この発明を適用した例を説明する。
Device Configuration Here, as shown in FIG. 2, the magnetic pole pieces (2) and (2) are removed from the configuration of the magnetic field generator shown in FIG.
-A pair of permanent magnet components using a B-R magnet (1)
(1) face each other and the other end has a rectangular plate yoke (4)
(5) Further, these are connected by four columnar yokes (6) having four corners, and a static magnetic field is generated in the space (7) between the permanent magnet constructs (1) and (1). An example in which the present invention is applied to a magnetic field generator having a configuration will be described.

まず、永久磁石構成体(1)を、同一寸法、特性の多
数の永久磁石で所定パターンで円盤状に形成し、あるい
は該構成に形成したと想定し、空隙(7)内に発生した
磁界状況、強度分布等を解析する。
First, assuming that the permanent magnet structure (1) is formed into a disk shape in a predetermined pattern with a large number of permanent magnets having the same size and characteristics, or is formed in this structure, the magnetic field state generated in the air gap (7). , Analyze intensity distribution, etc.

解析方法 解析方法には、有限要素法、境界要素法等の種々の解
析方法が採用できる。また、最近化手法としては、線形
計画法等の数理計画法が用いられるが、ここでは有限要
素法と線形計画法を併用する場合を説明する。
Analysis Method Various analysis methods such as a finite element method and a boundary element method can be adopted as the analysis method. Further, as the modernization method, a mathematical programming method such as a linear programming method is used. Here, a case where the finite element method and the linear programming method are used together will be described.

磁界発生装置空隙(7)内の磁界状況を有限要素法に
て調べる。
The state of the magnetic field in the magnetic field generator gap (7) is examined by the finite element method.

また、上記構成からなる磁界発生装置の空隙(7)に
おいて、その中心(O)から所定半径rの球体空間を設
定し、第3図に示す如く、当該球体の所要数の水平面、
ここでは7つの水平面(P1〜P7)で横断面し、さらに各
水平面(P1〜P7)と球体空間との交差円周上を、Z軸を
中心に所要角度で等分割した複数点での磁界強度を計算
し、各水平面(P1〜P7)の該円周上の磁界強度のばらつ
きを調べる。
Further, in the air gap (7) of the magnetic field generator having the above structure, a spherical space having a predetermined radius r is set from the center (O), and as shown in FIG. 3, a required number of horizontal planes of the spherical body,
Here, the cross section is taken along seven horizontal planes (P 1 to P 7 ), and the crossing circle between each horizontal plane (P 1 to P 7 ) and the spherical space is equally divided at the required angle around the Z axis. The magnetic field strength at the point is calculated, and the variation of the magnetic field strength on the circumference of each horizontal plane (P 1 to P 7 ) is examined.

次に、永久磁石構成体(1)(1)を構成する多数の
磁石セグメントの各々の磁化方向長さが、水平面(P1
P7)の該円周上の磁界強度に与える影響と調べる。
Next, the magnetization direction length of each of the multiple magnet segments forming the permanent magnet structure (1) (1) is determined by the horizontal plane (P 1 ~
The effect of P 7 ) on the magnetic field strength on the circumference is investigated.

第2図に示す如く磁極片を除き、永久磁石構成体
(1)(1)の空隙対向面が平坦な場合、すなわち、各
磁石セグメントの磁化方向高さが全て等しい場合の水平
面(P1〜P7)の該円周上の磁界強度を測定したところ、
第5図に示す如く、磁界強度の不均一の割合を空隙中心
の磁界強度からのずれ(%)で示すとおり、水平面(P1
〜P7)の磁界強度が著しく不均一である。
As shown in FIG. 2, except for the pole pieces, when the surfaces of the permanent magnet constituents (1) and (1) that face the air gap are flat, that is, when the magnetizing direction heights of all the magnet segments are all equal (P 1 ~ When the magnetic field strength on the circumference of P 7 ) was measured,
As shown in FIG. 5, as indicating the percentage of non-uniformity of the magnetic field intensity in the deviation from magnetic field strength of the gap center (%), horizontal (P 1
The magnetic field strength of ~ P 7 ) is extremely uneven.

そこで、第4図a〜dに示す如く磁化方向高さを低く
した磁石セグメントの位置を、永久磁石構成体(1)の
中心から順次外側へ移動させた場合の水平面(P1〜P7
の該円周上の磁界強度に与える影響を調べると、第6図
に示す如き結果を得る。
Therefore, as shown in FIGS. 4a to 4d, the positions of the magnet segments whose magnetizing heights are lowered are moved horizontally from the center of the permanent magnet structure (1) to the outside (P 1 to P 7 ).
When the effect of the above on the magnetic field strength on the circumference is examined, the results shown in FIG. 6 are obtained.

このように磁石セグメントの位置、その磁化方向高さ
の変化量について、水平面(P1〜P7)の該円周上の磁界
強度に与える影響を調べて、最適な磁石セグメントを選
定しこれを重ね合わせることにより、水平面(P1〜P7
の磁界強度が一定になる。
In this way, the effect of the position of the magnet segment and the amount of change in the magnetization direction height on the magnetic field strength on the circumference of the horizontal plane (P 1 to P 7 ) is examined, and the optimum magnet segment is selected and Horizontal planes (P 1 to P 7 ) by overlapping
The magnetic field strength of becomes constant.

さらに同様に、磁石セグメントの最適化を全領域に拡
大してゆき、最適な磁石セグメントを重ね合わせること
により均一磁界を得ることができるが、試行錯誤では多
大の工程を要するので、ここでは最適化手法のひとつで
ある線形計画法により、各磁石セグメントの磁化方向高
さを決定した。
Similarly, the optimization of the magnet segments can be expanded to the whole area, and a uniform magnetic field can be obtained by overlapping the optimal magnet segments, but trial and error requires a large number of steps, so optimization here is performed. The height of the magnetization direction of each magnet segment was determined by linear programming, which is one of the methods.

かかる解析に基づき、空隙(7)内の磁界強度の強弱
などに応じて、永久磁石構成体(1)(1)の多数の永
久磁石のうち、所要永久磁石の磁化方向長さを選定し、
例えば、第1図aに示す如く変化させて配列することに
より、第7図に示す如く、均一磁界を得ることができ
る。
Based on this analysis, the magnetization direction length of the required permanent magnet is selected from among the many permanent magnets of the permanent magnet structure (1) (1) in accordance with the strength of the magnetic field in the air gap (7),
For example, a uniform magnetic field can be obtained as shown in FIG. 7 by changing and arranging as shown in FIG.

第1図aに示す永久磁石構成体(1)は、板状継鉄
(5)上に種々の磁化方向長さの異なる永久磁石を配列
しているが、第1図bに示す如く、板状継鉄(5)表面
に凹凸を設けて、同様に永久磁石を配列し永久磁石構成
体(1)の空隙(7)対向面を平坦面としても同様の効
果が得られる。
In the permanent magnet structure (1) shown in FIG. 1a, various permanent magnets having different lengths in the magnetization direction are arranged on the plate yoke (5), but as shown in FIG. The same effect can be obtained by providing irregularities on the surface of the magnetic yoke (5), arranging permanent magnets in the same manner, and making the surface of the permanent magnet constituting body (1) facing the void (7) a flat surface.

さらに、磁石重量の軽減を目的に、前述した解析方法
により、各磁石セグメントの磁化方向高さの最適化を図
ったところ、各磁石セグメントを。第8図に示す如く、
特に周縁部の磁化方向を長くして環状の突起を形成する
とともに、中央部の所定位置の磁化方向を変化させて配
列することにより、より高精度の均一磁界を得ることが
でき、一層の軽量化が達成できた。
Furthermore, in order to reduce the weight of the magnets, the height of the magnetization direction of each magnet segment was optimized by the above-mentioned analysis method. As shown in FIG.
In particular, by increasing the magnetizing direction at the peripheral edge to form an annular protrusion and changing the magnetizing direction at a predetermined position in the center to arrange the magnets, a more accurate uniform magnetic field can be obtained, and the weight is further reduced. Was achieved.

実 施 例 常温時の(BH)maxが35MGOeを示すFe−B−R系永久
磁石を用い、直径300mm、高さ3.0mmの凸状突起と、外径
1100mm、内径900mm、高さ80mmの環状突起を有する磁極
片を配置し、磁極片の対向距離を500mmに設定した第9
図に示す従来の磁界発生装置において、空隙内の中心か
ら半径200mm以内の磁界均一度を測定したところ、50ppm
であった。
Practical example Using a Fe-BR permanent magnet with a (BH) max of 35 MGOe at room temperature, a convex protrusion with a diameter of 300 mm and a height of 3.0 mm and an outer diameter
9th with the pole piece having an annular projection of 1100mm, inner diameter 900mm, and height 80mm arranged and the facing distance of the pole piece set to 500mm
In the conventional magnetic field generator shown in the figure, the magnetic field uniformity within a radius of 200 mm from the center of the air gap was measured and found to be 50 ppm.
Met.

上記従来の磁界発生装置において、磁極片を除去し、
前述した解析方法を適用して永久磁石構成体の各永久磁
石の磁化方向長さの最適化を図り、永久磁石構成体対向
距離を500mmに設定し、第8図に示す永久磁石構成体を
有するこの発明による磁界発生装置を作製した。
In the above conventional magnetic field generator, the pole piece is removed,
The above-mentioned analysis method is applied to optimize the magnetization direction length of each permanent magnet of the permanent magnet structure, the facing distance of the permanent magnet structure is set to 500 mm, and the permanent magnet structure shown in FIG. 8 is provided. A magnetic field generator according to the present invention was produced.

この発明による磁界発生装置の空隙内の中心から半径
200mm以内の磁界均一度を測定したところ、従来装置と
同等であり、磁極片を使用しないことから磁石重量で10
%以上の軽量化が達成でき、装置全体としても軽量化が
可能になった。
The radius from the center in the air gap of the magnetic field generator according to the present invention
When the magnetic field homogeneity within 200 mm was measured, it was the same as that of the conventional device.
%, A weight reduction of more than 10% has been achieved, and it has become possible to reduce the weight of the entire device.

発明の効果 この発明による磁界発生装置は、磁極片を用いずに磁
化方向長さの異なる永久磁石を配列することにより、磁
極片を用いた構成と同等以上の均一磁界が得られ、ま
た、磁極片を用いないので渦電流の発生が抑えられ、さ
らに、軽量化を図ることができる。
Effects of the Invention In the magnetic field generator according to the present invention, by arranging permanent magnets having different lengths in the magnetization direction without using the magnetic pole pieces, a uniform magnetic field equal to or more than that of the configuration using the magnetic pole pieces can be obtained. Since no piece is used, generation of eddy current is suppressed, and further weight reduction can be achieved.

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

第1図a,bはこの発明による磁界発生装置の永久磁石構
成体(下側)を示す説明図である。 第2図aは磁極片のない磁界発生装置の縦断説明図であ
り、同b図は横断説明図である。 第3図は磁界発生装置の球体空間内の磁界を測定する方
法を示す空隙の斜視説明図である。 第4図a〜dはこの発明の永久磁石構成体(上側)の所
要セグメントの磁化方向高さを変化させた例を示す説明
図である。 第5図、第6図は第3図の球体空間内のP1〜P7の磁界不
均一度を示すグラフであり、第5図は第9図の従来磁界
発生装置において磁極片を除去した場合、第6図は第4
図a〜dの永久磁石構成体の場合を示す。 第7図は第1図aの実施例における球体空間内のP1〜P7
の磁界不均一度を示すグラフである。 第8図は最適化したこの発明の永久磁石構成体(上側)
の一実施例を示す説明図である。 第9図aは従来の磁界発生装置の縦断説明図であり、同
b図は横断説明図である。 1……永久磁石構成体、2……磁極片、 3……環状突起部、4,5……板状継鉄、6……柱状継
鉄、 7……空隙、8……凸状突起。
1A and 1B are explanatory views showing a permanent magnet structure (lower side) of a magnetic field generator according to the present invention. FIG. 2a is a vertical cross-sectional explanatory view of a magnetic field generator having no pole piece, and FIG. 2b is a cross-sectional explanatory view thereof. FIG. 3 is a perspective explanatory view of a gap showing a method for measuring a magnetic field in a spherical space of a magnetic field generator. 4A to 4D are explanatory views showing an example in which the magnetization direction height of the required segment of the permanent magnet structure (upper side) of the present invention is changed. 5 and 6 are graphs showing the magnetic field inhomogeneities of P 1 to P 7 in the spherical space of FIG. 3, and FIG. 5 shows the conventional magnetic field generator of FIG. 9 with pole pieces removed. In this case, FIG. 6 is the fourth
The case of the permanent magnet construction of FIGS. FIG. 7 shows P 1 to P 7 in the spherical space in the embodiment of FIG. 1a.
3 is a graph showing the magnetic field non-uniformity of FIG. FIG. 8 shows an optimized permanent magnet structure of the present invention (upper side).
It is explanatory drawing which shows one Example. FIG. 9A is a vertical cross-sectional explanatory view of a conventional magnetic field generator, and FIG. 9B is a cross-sectional explanatory view thereof. 1 ... Permanent magnet structure, 2 ... Pole piece, 3 ... Annular protrusion, 4,5 ... Plate yoke, 6 ... Column yoke, 7 ... Void, 8 ... Convex projection.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】空隙を形成して対向し単数または複数の磁
石セグメントからなる一対の永久磁石構成体を継鉄で磁
気的結合し、該空隙に磁界を発生させるMRI用磁界発生
装置において、 永久磁石構成体の所要位置または所要位置の磁石セグメ
ントが、その磁化方向長さを変えて配列され、該空隙に
均一磁界を発生させることを特徴とするMRI用磁界発生
装置。
1. A magnetic field generator for MRI for magnetically coupling a pair of permanent magnet constituents, which are opposed to each other with a gap and are composed of a single or a plurality of magnet segments, by a yoke to generate a magnetic field in the gap. A magnetic field generator for MRI, characterized in that required positions of a magnet structure or magnet segments at required positions are arranged with varying lengths in the direction of magnetization thereof to generate a uniform magnetic field in the gap.
JP2004685A 1990-01-12 1990-01-12 Magnetic field generator for MRI Expired - Lifetime JPH0821498B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2004685A JPH0821498B2 (en) 1990-01-12 1990-01-12 Magnetic field generator for MRI

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2004685A JPH0821498B2 (en) 1990-01-12 1990-01-12 Magnetic field generator for MRI

Publications (2)

Publication Number Publication Date
JPH03209803A JPH03209803A (en) 1991-09-12
JPH0821498B2 true JPH0821498B2 (en) 1996-03-04

Family

ID=11590749

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2004685A Expired - Lifetime JPH0821498B2 (en) 1990-01-12 1990-01-12 Magnetic field generator for MRI

Country Status (1)

Country Link
JP (1) JPH0821498B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040189123A1 (en) 2001-08-24 2004-09-30 Peter Nusser Magnetically hard object and method for adjusting the direction and position of a magnetic vector

Also Published As

Publication number Publication date
JPH03209803A (en) 1991-09-12

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