JPH0246002Y2 - - Google Patents
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- Publication number
- JPH0246002Y2 JPH0246002Y2 JP16813884U JP16813884U JPH0246002Y2 JP H0246002 Y2 JPH0246002 Y2 JP H0246002Y2 JP 16813884 U JP16813884 U JP 16813884U JP 16813884 U JP16813884 U JP 16813884U JP H0246002 Y2 JPH0246002 Y2 JP H0246002Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- magnetic
- air gap
- magnetic pole
- permanent magnets
- 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
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- Magnetic Resonance Imaging Apparatus (AREA)
Description
【考案の詳細な説明】
産業分野
この考案は、対象物の断面イメージを得て組織
の性質まで描き出すことのできる医療用核磁気共
鳴断層装置(以下、NMR−CTという)に用い
られる永久磁石を使用した磁界発生装置に係り、
大きな空隙内に強力かつ高精度で均一な静磁界を
発生する磁界発生装置に関する。[Detailed explanation of the invention] Industrial field This invention is a permanent magnet used in medical nuclear magnetic resonance tomography (hereinafter referred to as NMR-CT), which can obtain cross-sectional images of objects and depict the properties of tissues. Regarding the magnetic field generator used,
This invention relates to a magnetic field generating device that generates a strong, highly accurate, and uniform static magnetic field within a large air gap.
背景技術
NMR−CTは、人体の一部または全部を1〜
10KGの強力な磁界を形成する空隙内に挿入して
所要の断層イメージを得るため、この磁界が強力
かつ10-4以下の精度で一様で安定していることが
要求され、NMR−CT用の磁界発生装置として
は、銅またはアルミニウムからなる導線を円筒状
に巻着した常伝導磁石あるいは、特殊な導線を用
い、絶対零度付近の温度に冷却して使用する超伝
導磁石が知られている。BACKGROUND ART
In order to obtain the desired tomographic image by inserting the device into an air gap that generates a strong magnetic field of 10 KG, this magnetic field must be strong, uniform, and stable with an accuracy of 10 -4 or less. Known magnetic field generators include normal conducting magnets made of conductive wires made of copper or aluminum wrapped around them in a cylindrical shape, and superconducting magnets that use special conducting wires cooled to a temperature close to absolute zero. .
前者は構造上安価であるが十分な強力磁界を発
生させるためには、膨大な電力と冷却水が必要で
あり、ランニングコストが高く、コイルが作る漏
洩磁界は使用用途によつては悪影響の要因となる
等の問題があり、一方、後者の超伝導磁石は、電
力の消費が少なく小型で強力な磁界を発生し得る
利点があるが、冷媒として高価な液体ヘリウム等
の使用が不可欠であり、いわゆるイニシヤルコス
トとともにランニングコストも著しく高い問題が
ある。 The former is structurally inexpensive, but it requires a huge amount of electricity and cooling water to generate a sufficiently strong magnetic field, resulting in high running costs, and the leakage magnetic field created by the coil can be a negative factor depending on the application. On the other hand, the latter type of superconducting magnet has the advantage of consuming less power and being compact and capable of generating a strong magnetic field, but it requires the use of expensive liquid helium or the like as a coolant. There is a problem in that not only the so-called initial cost but also the running cost is extremely high.
本出願人は、先に、磁界強度が上記の常伝導磁
石と同等以上で電力の消費も少なく、漏洩磁界の
少ない永久磁石回路として、空隙を形成して対向
する磁極片と、少なくとも1の永久磁石とを継鉄
で磁気的結合し該空隙に磁界を発生させる磁界発
生装置において、上記磁極片の対向面の各々に環
状突起を設けたことを特徴とする磁界発生装置を
提案(特願昭58−196785号)した。 The present applicant previously developed a permanent magnet circuit that has a magnetic field strength equal to or higher than that of the above-mentioned normal conduction magnet, consumes less power, and has a small leakage magnetic field. A magnetic field generating device is proposed in which a magnet is magnetically coupled with a yoke to generate a magnetic field in the air gap, and the magnetic field generating device is characterized in that annular protrusions are provided on each of the opposing surfaces of the magnetic pole pieces. 58-196785).
上記の磁界発生装置によつて、空隙に発生する
磁界の均一精度を著しく向上させることができ
た。しかし、第3図に示す如く、一対の永久磁石
10の各々の一方端に磁極片11を固着して対向
させ、他方端を継鉄12で結合し、磁極片11間
の空隙13内に、静磁界を発生させる構成であ
り、一対の磁極片11には、その対向面の周縁
に、所定の内径、高さからなる断面略台形の環状
突起を突設した構成において、磁極からの磁束は
空隙外に漏洩しやすく、空隙中心垂直線上では、
磁極面に近い程磁界強度が高くなる性質があるた
め、通常使用磁界空間、例えば、半径200mm以上
の球形空間で所要の高い均一磁界を得るために
は、磁極間距離や磁極面積を大きくするなど、使
用磁界空間の10倍以上の空隙を要し、磁気回路の
小形化ができないという問題を有していた。 With the above magnetic field generating device, it was possible to significantly improve the uniformity accuracy of the magnetic field generated in the air gap. However, as shown in FIG. 3, the magnetic pole pieces 11 are fixed to one end of each of a pair of permanent magnets 10 and are opposed to each other, and the other ends are connected with a yoke 12, and in the air gap 13 between the magnetic pole pieces 11, This configuration generates a static magnetic field, and in a configuration in which a pair of magnetic pole pieces 11 has an annular protrusion projecting from the periphery of their opposing surfaces with a substantially trapezoidal cross section having a predetermined inner diameter and height, the magnetic flux from the magnetic poles is It is easy to leak outside the gap, and on the vertical line at the center of the gap,
Since the magnetic field strength tends to be higher as it gets closer to the magnetic pole surface, in order to obtain the required high uniform magnetic field in a normally used magnetic field space, for example, a spherical space with a radius of 200 mm or more, it is necessary to increase the distance between the magnetic poles and the magnetic pole area. However, there was a problem in that it required an air gap ten times larger than the magnetic field space used, and the magnetic circuit could not be made smaller.
考案の目的
この考案は、かかる現状に鑑み、強力な磁界が
得られる永久磁石を使用した磁界発生装置の空隙
において、高精度で均一かつ安定な磁界のより一
層の拡大を計つた磁気回路を有する磁界発生装置
を目的とし、永久磁石からの磁束の漏洩を防止
し、永久磁石量を低減して小型軽量化が達成でき
る磁界発生装置を目的としている。Purpose of the invention In view of the current situation, this invention has a magnetic circuit that further expands a highly accurate, uniform, and stable magnetic field in the air gap of a magnetic field generator using permanent magnets that can generate a strong magnetic field. The objective is a magnetic field generator that can prevent leakage of magnetic flux from permanent magnets, reduce the amount of permanent magnets, and achieve a reduction in size and weight.
考案の構成と効果
この考案は、高精度で均一かつ安定な磁界が得
られ、かつ漏洩磁束の少ない磁気回路を目的に
種々検討した結果、永久磁石と磁極片とで包囲さ
れる空隙の開口軸方向に配置されている板状磁極
片の厚みを中央部で薄くすることにより、漏洩磁
束が減少し、磁気回路空隙内の磁界均一度が著し
く向上し、高精度で均一な磁界域を拡大できるこ
とを知見したものである。Structure and effect of the invention This invention was developed as a result of various studies aimed at creating a magnetic circuit that can obtain a highly accurate, uniform, and stable magnetic field and has low magnetic flux leakage. By reducing the thickness of the plate-shaped magnetic pole pieces arranged in the direction at the center, leakage magnetic flux is reduced, the magnetic field uniformity within the magnetic circuit air gap is significantly improved, and a highly accurate and uniform magnetic field area can be expanded. This is what we discovered.
すなわち、この考案は、同方向に磁化された一
対の永久磁石を空隙を介して並列配置し、一対の
永久磁石において一対端面に板状磁極片を着設
し、該空隙を一軸方向に開口させて永久磁石と磁
極片で包囲した磁気回路に構成し、該板状磁極片
の前記軸方向における中心側を外方よりも薄肉と
したことを特徴とする磁界発生装置である。 That is, in this invention, a pair of permanent magnets magnetized in the same direction are arranged in parallel with an air gap between them, plate-shaped magnetic pole pieces are attached to a pair of end faces of the pair of permanent magnets, and the air gap is opened in a uniaxial direction. The present invention is a magnetic field generating device characterized in that the magnetic circuit is formed into a magnetic circuit surrounded by a permanent magnet and a magnetic pole piece, and the central side of the plate-shaped magnetic pole piece in the axial direction is made thinner than the outer side.
板状磁極片は、空隙の開口方向における中央部
を外方よりも薄肉とするが、空隙中心部に、発生
磁束を収束せしめる構成であれば、外方の厚肉部
位置や形状及び中央薄肉部との接続面形状などは
種々の形状が採用でき、永久磁石の磁気特性、形
状寸法、継鉄の形状寸法及び所要空隙の大きさ等
に応じて、板状磁極片形状を適宜選定することが
望ましい。 The plate-shaped magnetic pole piece has a thinner wall at the center in the opening direction of the air gap than at the outside, but if the configuration is such that the generated magnetic flux is converged at the center of the air gap, the position and shape of the outer thick part and the thin center wall can be changed. Various shapes can be adopted for the shape of the connection surface with the part, and the shape of the plate-like pole piece should be selected appropriately depending on the magnetic properties and dimensions of the permanent magnet, the shape and dimensions of the yoke, the size of the required air gap, etc. is desirable.
この考案による磁界発生装置は、下記の永久磁
石を使用することにより、1〜10KGの強磁界を
形成できる装置として、10ton以下の重量ですみ、
フエライト磁石を使用する磁界発生装置の100ton
以上に比べて著しい小型軽量化が達成できる。 The magnetic field generating device according to this invention is a device that can generate a strong magnetic field of 1 to 10 kg by using the following permanent magnet, and it weighs less than 10 tons.
100ton of magnetic field generator using ferrite magnet
Compared to the above, a significant reduction in size and weight can be achieved.
考案に用いる永久磁石
この考案の磁界発生装置に用いる永久磁石は、
フエライト磁石、アルニコ系磁石、希土類コバル
ト系磁石が使用できるが、先に出願人が提案し
た、高価なSmやCoを含有しない新しい高性能永
久磁石としてFe−B−R系(RはYを含む希土
類元素のうち少なくとも1種)永久磁石(特願昭
57−145072号)は、その最大エネルギー積が大き
いだけでなく、残留磁束密度(Br)の温度係数
が、0.07%/゜C〜0.15%/゜Cなる温度特性を
有するため、この永久磁石を上記のNMR−CT
に適用することにより、装置の小形化が達成で
き、すぐれた性能が得られ、さらに、この永久磁
石の磁気特性は、特に0゜C以下に冷却して使用す
ることにより、著しく高い最大エネルギー積を得
ることができ、有効利用できる。Permanent magnet used in the invention The permanent magnet used in the magnetic field generator of this invention is
Ferrite magnets, alnico magnets, and rare earth cobalt magnets can be used, but the applicant has previously proposed a new high-performance permanent magnet that does not contain expensive Sm or Co. At least one kind of rare earth element) Permanent magnet (Special application)
57-145072) not only has a large maximum energy product, but also has a temperature coefficient of residual magnetic flux density (Br) of 0.07%/°C to 0.15%/°C. The above NMR-CT
By applying it to a permanent magnet, it is possible to achieve a smaller device size and obtain excellent performance.Furthermore, the magnetic properties of this permanent magnet can be used especially when cooled to below 0°C, resulting in an extremely high maximum energy product. can be obtained and used effectively.
上記のFe−B−R系永久磁石は、R(但しRは
Yを含む希土類元素のうち少なくとも1種)8原
子%〜30原子%、B2原子%〜28原子%、Fe42原
子%〜90原子%を主成分とし、主相が正方晶相か
らなる永久磁石であり、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25MGOe以上の極めて高いエネ
ルギー積を示す、すぐれた永久磁石である。 The above Fe-BR-based permanent magnet has R (where R is at least one kind of rare earth elements including Y) 8 at% to 30 at%, B2 at% to 28 at%, Fe42 at% to 90 at%. It is a permanent magnet whose main phase is a tetragonal phase, and R is a light rare earth that is abundant in resources, mainly Nd and Pr.
It is an excellent permanent magnet that has extremely high energy product of over 25MGOe as its main component.
図面に基づく考案の開示
第1図はこの考案による磁界発生装置を示す正
面図と側面説明図である。第2図はこの考案によ
る板状磁極片の他実施例を示す断面説明図であ
る。Disclosure of the invention based on drawings FIG. 1 is a front view and a side explanatory view showing a magnetic field generating device according to this invention. FIG. 2 is an explanatory cross-sectional view showing another embodiment of the plate-shaped magnetic pole piece according to this invention.
第1図に示す磁気回路は、直方体からなる一対
のFe−B−R系永久磁石1,1を、長手方向の
主面を所定間隔で対抗させて並列配置し、空隙2
を形成し、このFe−B−R系永久磁石1,1の
上下の端面に板状磁極片3,3を貼着して、永久
磁石1の長手方向に開口が設けられ、空隙2が永
久磁石1と板状磁極片3とで包囲されている。 The magnetic circuit shown in FIG. 1 consists of a pair of rectangular parallelepiped Fe-B-R permanent magnets 1, 1 arranged in parallel with their longitudinal main surfaces facing each other at a predetermined interval.
The plate-shaped magnetic pole pieces 3, 3 are attached to the upper and lower end surfaces of the Fe-B-R permanent magnets 1, 1, and an opening is provided in the longitudinal direction of the permanent magnet 1, and the air gap 2 is permanently It is surrounded by a magnet 1 and a plate-shaped pole piece 3.
板状磁極片3は、空隙2の開口方向に厚肉の外
方部4、薄肉の中央部5、厚肉の外方部4に形成
され、外方部4から中央部5へは傾斜面6が形成
してある。また、Fe−B−R系永久磁石1,1
は同一の上下方向に磁化してある。 The plate-shaped magnetic pole piece 3 is formed into a thick outer part 4, a thin central part 5, and a thick outer part 4 in the opening direction of the air gap 2, and has an inclined surface from the outer part 4 to the central part 5. 6 is formed. In addition, Fe-BR permanent magnets 1, 1
are magnetized in the same vertical direction.
上記構成において、板状磁極片3,3から発生
する磁束は、Fe−B−R系永久磁石1,1の磁
化方向と同一方向に収束されて磁界形成するた
め、漏洩磁束が減少し、空隙2内は極めて高い均
一度を有する静磁界が得られる。 In the above configuration, the magnetic flux generated from the plate-shaped magnetic pole pieces 3, 3 is converged in the same direction as the magnetization direction of the Fe-BR permanent magnets 1, 1 to form a magnetic field, so that the leakage magnetic flux is reduced and the air gap 2, a static magnetic field with extremely high uniformity can be obtained.
また、板状磁極片は第1図の形状のほか、第2
図a図に示すように、中央部5を凹部湾曲面7で
形成することにより、厚肉の外方部4を構成する
のもよく、また、b図に示す如く、第1図に示し
た磁極片と同様に構成し、厚肉の外方部4の位置
を磁極片端部より中央部へ寄せた配置とするのも
よい。 In addition to the shape shown in Fig. 1, the plate-shaped magnetic pole piece has the shape shown in Fig.
As shown in Figure a, the thick outer part 4 may be constructed by forming the central part 5 with a concave curved surface 7. It is also preferable to have the same structure as the magnetic pole piece, with the thick outer portion 4 being placed closer to the center than the end of the magnetic pole piece.
ちなみに、第1図に示した構成のNMR−CT
装置に、最大エネルギー積35MGOeの特性を有
するFe−B−R系永久磁石を用い、磁極片の対
向距離として、600mmを設定して組立を行なつた
ところ、空隙中央部での磁界強度は4KGであつ
た。これと同程度の均一磁界範囲及び磁界強度を
有する第3図に示すNMR−CT装置を作製して
装置重量を比較したところ、本考案装置は20%の
軽量化が達成できた。 By the way, NMR-CT with the configuration shown in Figure 1
When assembling the device using Fe-B-R permanent magnets with a maximum energy product of 35 MGOe and setting the facing distance of the magnetic pole pieces to 600 mm, the magnetic field strength at the center of the air gap was 4 KG. It was hot. When an NMR-CT apparatus shown in FIG. 3 having a uniform magnetic field range and magnetic field strength comparable to this was fabricated and the weight of the apparatus was compared, it was found that the apparatus of the present invention was able to achieve a 20% weight reduction.
第1図はこの考案による磁界発生装置を示す正
面図と側面説明図である。第2図はこの考案によ
る板状磁極片の他実施例を示す断面説明図であ
る。第3図は磁界発生装置の縦断説明図である。
1……Fe−B−R系永久磁石、2……空隙、
3……板状磁極片、4……外方部、5……中央
部、6……傾斜面、7……湾曲面、10……永久
磁石、11……磁極片、12……継鉄、13……
空隙。
FIG. 1 is a front view and a side view showing a magnetic field generating device according to this invention. FIG. 2 is an explanatory cross-sectional view showing another embodiment of the plate-shaped magnetic pole piece according to this invention. FIG. 3 is a longitudinal sectional view of the magnetic field generator. 1... Fe-B-R permanent magnet, 2... Air gap,
3... Plate magnetic pole piece, 4... Outer part, 5... Central part, 6... Inclined surface, 7... Curved surface, 10... Permanent magnet, 11... Magnetic pole piece, 12... Yoke , 13...
void.
Claims (1)
して並列配置し、一対の永久磁石において一対端
面に板状磁極片を着設し、該空隙を一軸方向に開
口させて永久磁石と磁極片で包囲した磁気回路に
構成し、該板状磁極片の前記軸方向における中心
側を外方よりも薄肉としたことを特徴とする磁界
発生装置。 A pair of permanent magnets magnetized in the same direction are arranged in parallel with an air gap between them, plate-shaped magnetic pole pieces are attached to a pair of end faces of the pair of permanent magnets, and the air gap is opened in a uniaxial direction to connect the permanent magnets and the magnetic pole pieces. 1. A magnetic field generating device comprising a magnetic circuit surrounded by a magnetic field, wherein the central side of the plate-shaped magnetic pole piece in the axial direction is thinner than the outer side.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16813884U JPH0246002Y2 (en) | 1984-11-06 | 1984-11-06 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16813884U JPH0246002Y2 (en) | 1984-11-06 | 1984-11-06 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6182608U JPS6182608U (en) | 1986-05-31 |
| JPH0246002Y2 true JPH0246002Y2 (en) | 1990-12-05 |
Family
ID=30725918
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16813884U Expired JPH0246002Y2 (en) | 1984-11-06 | 1984-11-06 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0246002Y2 (en) |
-
1984
- 1984-11-06 JP JP16813884U patent/JPH0246002Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6182608U (en) | 1986-05-31 |
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