JPS63127746A - Magnetic field generator for magnetic resonance diagnostic apparatus - Google Patents

Magnetic field generator for magnetic resonance diagnostic apparatus

Info

Publication number
JPS63127746A
JPS63127746A JP61272910A JP27291086A JPS63127746A JP S63127746 A JPS63127746 A JP S63127746A JP 61272910 A JP61272910 A JP 61272910A JP 27291086 A JP27291086 A JP 27291086A JP S63127746 A JPS63127746 A JP S63127746A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic field
permanent magnet
peripheral edge
diagnostic apparatus
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
JP61272910A
Other languages
Japanese (ja)
Inventor
武夫 金子
河本 宏美
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 JP61272910A priority Critical patent/JPS63127746A/en
Publication of JPS63127746A publication Critical patent/JPS63127746A/en
Pending legal-status Critical Current

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  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は磁気共鳴診断装置等において静磁場を形成する
のに用いる磁界発生装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Field of Industrial Application) The present invention relates to a magnetic field generating device used to generate a static magnetic field in a magnetic resonance diagnostic apparatus or the like.

(従来の技術) 一般にこの種の磁界発生装置は、第2図に示すように相
対向して配置した永久磁石1,1と、これら永久磁石1
.1の対向面に設けた磁極板2゜2と、前記永久磁石1
.1を磁気的に結合して磁気回路を形成するヨーク3と
からなり、前記磁極板2,2の間に磁界を発生させるよ
うになっている。
(Prior Art) Generally, this type of magnetic field generating device consists of permanent magnets 1, 1 arranged opposite to each other as shown in FIG.
.. 1 and the permanent magnet 1.
.. 1 and a yoke 3 that magnetically couples the magnetic pole plates 2 and 2 to form a magnetic circuit, and generates a magnetic field between the magnetic pole plates 2 and 2.

そしてこの種の装置においては、上下磁極板2゜2の間
にある空隙4内の磁界が均一になるようにする必要があ
ることから、従来は第2図又は第3図に示すように磁極
板2の対向面周縁部2Aを隆起せしめ、これによって磁
界分布の均一化を図っていた。
In this type of device, it is necessary to make the magnetic field in the air gap 4 between the upper and lower magnetic pole plates 2°2 uniform, so conventionally the magnetic poles are arranged as shown in Fig. 2 or 3. The peripheral edge 2A of the facing surface of the plate 2 is raised to make the magnetic field distribution uniform.

(発明が解決しようとする問題点) ところが上述のように磁極板2の対向面周縁862Aを
隆起せしめると、その隆起している分だけ中央部に比べ
て厚さが増すことになり、永久磁石からの磁束はこの増
加している分だけ中央部より余分に通らなければ空隙部
4に達することができず、このため空隙部4における周
縁部2Aに対応する部分の磁気1強度が減少してしまう
という問題がある。
(Problem to be Solved by the Invention) However, when the peripheral edge 862A of the facing surface of the magnetic pole plate 2 is raised as described above, the thickness increases by the raised area compared to the central part, and the permanent magnet The magnetic flux from the magnetic flux cannot reach the gap 4 unless it passes further from the center by this increased amount, and as a result, the magnetic flux 1 in the area corresponding to the peripheral edge 2A in the gap 4 decreases. There is a problem with putting it away.

この問題を解決するには、空隙部4におCブる周縁部2
Aに対応する部分についても必要磁界強度が得られるよ
うに、永久磁石1の量を多くすることが考えられるが、
この場合法のような問題がある。
To solve this problem, the peripheral edge 2 that extends into the cavity 4 must be
It is conceivable to increase the amount of permanent magnet 1 so that the required magnetic field strength can also be obtained for the part corresponding to A, but
In this case there are legal issues.

即ち、全ての磁束が前述の磁気回路を通れば良いが、磁
束は磁性体内は通りやすく非磁性体は通りづらい(磁気
抵抗が大ぎい)という性質があるため、磁界は永久磁石
のもつ強度だけではなく永久磁石の周囲に置かれたヨー
ク、及び[a極板等によっても大きな影響を受けること
となる。このため、相対向する磁石1からの磁束は、空
隙部4を介して他方の磁石1に向うものよりも第2図に
矢印Fで示すように、より近い位置にあるヨーク3に向
うものの方が多く、実際に空隙部4に発生する磁気強度
は磁石1の持つ磁界強度の30乃至40%程度でしかな
い。従って、空隙部4において必要磁界強度が得られる
ように永久磁石1の耐を多くした場合には、非常に磁界
ロスが大となって目標に対し1.7乃至1.6倍の永久
磁石量を設けなければいけないという問題が生じるので
ある。
In other words, all of the magnetic flux needs to pass through the magnetic circuit described above, but since magnetic flux has the property of passing easily through magnetic bodies and having difficulty passing through non-magnetic bodies (magnetic resistance is large), the magnetic field is limited to the strength of the permanent magnet. Instead, it is greatly influenced by the yoke placed around the permanent magnet, the a-pole plate, etc. Therefore, the magnetic flux from the opposing magnets 1 is directed toward the yoke 3 located closer, as shown by arrow F in FIG. 2, than toward the other magnet 1 via the gap 4. The magnetic strength actually generated in the gap 4 is only about 30 to 40% of the magnetic field strength of the magnet 1. Therefore, if the resistance of the permanent magnet 1 is increased to obtain the required magnetic field strength in the air gap 4, the magnetic field loss will be extremely large, and the amount of permanent magnets will be 1.7 to 1.6 times the target. The problem arises that it is necessary to provide a

本発明の目的は、以上のような従来装置における問題点
を解決し、空隙部にあける磁界分布をより一層均−にす
ることになる。
An object of the present invention is to solve the above-mentioned problems in the conventional device and to make the magnetic field distribution in the gap even more uniform.

[発明の構成] (問題点を解決するための手段) 上記目的を達成するため本発明は、永久磁石の対向面周
縁部を中央部より隆起せしめた構成とした。
[Structure of the Invention] (Means for Solving the Problems) In order to achieve the above object, the present invention has a structure in which the peripheral edge of the facing surface of the permanent magnet is raised from the center.

(作 用) 本発明は上記の構成としたので、次のように作用する。(for production) Since the present invention has the above configuration, it operates as follows.

即ち、磁極板の対向面周縁部を隆起せしめた場合であっ
ても、永久磁石の対向面周縁部が隆起しているので、結
果として磁極板の厚さは従来に比べて均等化されること
となる。従って、永久磁石からの磁束は磁極板の周縁部
においても中央部と同じだけの距離を通れば空隙部に達
するので、従来のように空隙部における周縁部に対応す
る部分の磁気強度が減少するということがなく、これに
よって磁界の均一化が図られることとなる。
In other words, even when the periphery of the opposing surface of the magnetic pole plate is raised, the periphery of the opposing surface of the permanent magnet is raised, and as a result, the thickness of the magnetic pole plate is made more uniform than in the past. becomes. Therefore, the magnetic flux from the permanent magnet reaches the gap after passing the same distance at the periphery of the magnetic pole plate as it does at the center, so the magnetic intensity in the gap corresponding to the periphery decreases as in the conventional case. Thereby, the magnetic field can be made uniform.

しかも、永久fa15の対向面周縁部を隆起させたこと
により、結果として永久磁石の対向面周縁部はヨークか
ら遠ざかることとなるので、従来に比べて磁気損失が少
なくなる。
Furthermore, by raising the peripheral edge of the facing surface of the permanent fa 15, the peripheral edge of the facing surface of the permanent magnet is moved away from the yoke, so that magnetic loss is reduced compared to the conventional case.

従って本発明によれば、永久磁石の強度を上げずに効率
良く均一な磁界分布を得ることができる。
Therefore, according to the present invention, it is possible to efficiently obtain a uniform magnetic field distribution without increasing the strength of the permanent magnet.

(実施例) 以下図示の実施例について説明する。(Example) The illustrated embodiment will be described below.

第1図は本発明に係る磁気共鳴診断装置用!i磁界発生
装置一実施例を示す概略正面図であり、第2図に示した
従来の装置と同様な部分については同一の符号を付しで
ある。即ち、3は従来と同様なヨークである。
Figure 1 is for a magnetic resonance diagnostic device according to the present invention! FIG. 2 is a schematic front view showing one embodiment of the i-magnetic field generating device, in which the same parts as in the conventional device shown in FIG. 2 are designated by the same reference numerals. That is, 3 is a yoke similar to the conventional one.

5.5は永久磁石であり、対応面周縁部5A。5.5 is a permanent magnet, and the corresponding surface periphery 5A.

5Aを隆起せしめ、これに応じて底部周縁も傾斜させて
全体的に同一の厚みとなるようにしている。
5A is raised, and the bottom peripheral edge is also inclined accordingly so that the thickness is the same overall.

6.6は磁極板であり、その対向周縁部6A。6.6 is a magnetic pole plate, and its opposing peripheral edge 6A.

6Aが前記永久磁石に沿って隆起しており、全体的に永
久磁石と相似形になるようにされている。
6A is raised along the permanent magnet, so that the overall shape is similar to that of the permanent magnet.

更に図示の永久磁石5.5は、ヨーク3との接合部にお
いて、その周縁部7が円環状に切除された状態となって
いるので、その切除部分にヨーク材(又は永久磁石材)
と同一の材質の円環部材が充填されている。
Furthermore, the illustrated permanent magnet 5.5 has its peripheral edge 7 cut out in an annular shape at the joint with the yoke 3, so a yoke material (or permanent magnet material) is applied to the cut portion.
It is filled with an annular member made of the same material.

以上のような磁界発生装置は次のような作用効果を奏す
る。
The magnetic field generating device as described above has the following effects.

■ 磁極板6.6の対向面周縁部6Aが図示のように隆
起していても、永久磁石5,5の対向面周縁部5Aが隆
起しているので、結果として磁極板6の厚さは従来に比
べて均等化される。従って、永久磁石5からの磁束は磁
極板6の周縁部6Aにおいても中央部と同じだけの距離
を通れば空隙部4に達するので、従来のように空隙部4
における周縁部に対応する部分の磁気強度が減少すると
いうことがなく、これによって磁界が均一化される。
■ Even if the periphery 6A of the facing surface of the magnetic pole plate 6.6 is raised as shown in the figure, the periphery 5A of the facing surface of the permanent magnets 5, 5 is raised, so as a result, the thickness of the magnetic pole plate 6 is Equalized compared to before. Therefore, the magnetic flux from the permanent magnet 5 reaches the gap 4 if it passes the same distance at the peripheral edge 6A of the magnetic pole plate 6 as it does at the center.
The magnetic strength of the portion corresponding to the peripheral edge of the magnetic field does not decrease, thereby making the magnetic field uniform.

■ 永久磁石の対向面周縁部5Aを隆起させたことによ
り、結果として永久磁石の対向面周縁部5Aはヨーク3
から遠ざかることとなるので、従来に比べて磁気損失が
少なくなる。即ち、従来に比べて永久磁石の対向面周縁
部5A間の距離(が短くなると同時に周縁部5Aからヨ
ーク3までの距離りが大となるので磁気損失は従来に比
べて著しく少なくなる。
■ By raising the peripheral edge 5A of the facing surface of the permanent magnet, as a result, the peripheral edge 5A of the facing surface of the permanent magnet is raised to the yoke 3.
Therefore, the magnetic loss is reduced compared to the conventional case. In other words, the distance between the peripheral edges 5A of the facing surfaces of the permanent magnets becomes shorter than in the past, and at the same time the distance from the peripheral edge 5A to the yoke 3 increases, so the magnetic loss is significantly reduced compared to the conventional.

■ 従って本実施例によれば、永久磁石の強度を上げず
に効率良く均一な磁界分布を得ることができる。
(2) Therefore, according to this embodiment, it is possible to efficiently obtain a uniform magnetic field distribution without increasing the strength of the permanent magnet.

以上本発明の一実施例について説明したが、本発明は上
記実施例に限定されるものではなく、本発明の要旨の範
囲内において適宜変形実施可能であることは言うまでも
ない。
Although one embodiment of the present invention has been described above, it goes without saying that the present invention is not limited to the above embodiment, and can be modified as appropriate within the scope of the gist of the present invention.

[発明の効果〕 以上詳述したように本発明によれば、永久磁石の強度を
上げずに効率良く均一な磁界分布を得ることができる。
[Effects of the Invention] As detailed above, according to the present invention, it is possible to efficiently obtain a uniform magnetic field distribution without increasing the strength of the permanent magnet.

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

第1図は本発明に係る磁気共鳴診断装置用磁界発生装置
の一実施例を示す概略正面図、第2図は従来装置の概略
正面図、第3図は他の従来例の部分正面図である。 3・・・ヨーク、4・・・空隙部、5・・・永久磁石、
5A・・・永久磁石周縁部、6・・・ra磁極板6A・
・・磁極板周縁部。
FIG. 1 is a schematic front view showing an embodiment of a magnetic field generating device for a magnetic resonance diagnostic apparatus according to the present invention, FIG. 2 is a schematic front view of a conventional device, and FIG. 3 is a partial front view of another conventional example. be. 3...Yoke, 4...Gap, 5...Permanent magnet,
5A... Permanent magnet periphery, 6... ra magnetic pole plate 6A.
...periphery of magnetic pole plate.

Claims (1)

【特許請求の範囲】[Claims] 相対向して配置した永久磁石と、これら永久磁石の対向
面に設けた磁極板と、前記永久磁石を磁気的に結合する
ヨークとからなり、前記磁極板間に磁界を発生させる磁
界発生装置において、前記永久磁石の対向面周縁部を中
央部より隆起せしめたことを特徴とする磁気共鳴診断装
置用磁界発生装置。
A magnetic field generating device that generates a magnetic field between the magnetic pole plates, comprising permanent magnets arranged opposite to each other, magnetic pole plates provided on opposing surfaces of these permanent magnets, and a yoke that magnetically couples the permanent magnets. . A magnetic field generating device for a magnetic resonance diagnostic apparatus, characterized in that a peripheral edge portion of the facing surface of the permanent magnet is raised from a central portion.
JP61272910A 1986-11-18 1986-11-18 Magnetic field generator for magnetic resonance diagnostic apparatus Pending JPS63127746A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61272910A JPS63127746A (en) 1986-11-18 1986-11-18 Magnetic field generator for magnetic resonance diagnostic apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61272910A JPS63127746A (en) 1986-11-18 1986-11-18 Magnetic field generator for magnetic resonance diagnostic apparatus

Publications (1)

Publication Number Publication Date
JPS63127746A true JPS63127746A (en) 1988-05-31

Family

ID=17520460

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61272910A Pending JPS63127746A (en) 1986-11-18 1986-11-18 Magnetic field generator for magnetic resonance diagnostic apparatus

Country Status (1)

Country Link
JP (1) JPS63127746A (en)

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