JPH0246003Y2 - - Google Patents
Info
- Publication number
- JPH0246003Y2 JPH0246003Y2 JP1741885U JP1741885U JPH0246003Y2 JP H0246003 Y2 JPH0246003 Y2 JP H0246003Y2 JP 1741885 U JP1741885 U JP 1741885U JP 1741885 U JP1741885 U JP 1741885U JP H0246003 Y2 JPH0246003 Y2 JP H0246003Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- magnetic
- magnetic pole
- permanent magnet
- air 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
Links
- 230000007246 mechanism Effects 0.000 claims description 7
- 229910052761 rare earth metal Inorganic materials 0.000 description 4
- 230000003068 static effect Effects 0.000 description 3
- 238000012423 maintenance Methods 0.000 description 2
- 150000002910 rare earth metals Chemical class 0.000 description 2
- 229910000859 α-Fe Inorganic materials 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 238000005481 NMR spectroscopy Methods 0.000 description 1
- 229910052779 Neodymium Inorganic materials 0.000 description 1
- 229910052777 Praseodymium Inorganic materials 0.000 description 1
- 229910052772 Samarium Inorganic materials 0.000 description 1
- 229910000828 alnico Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 229910017052 cobalt Inorganic materials 0.000 description 1
- 239000010941 cobalt Substances 0.000 description 1
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 1
- 239000002826 coolant Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 239000000498 cooling water Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- RKTYLMNFRDHKIL-UHFFFAOYSA-N copper;5,10,15,20-tetraphenylporphyrin-22,24-diide Chemical compound [Cu+2].C1=CC(C(=C2C=CC([N-]2)=C(C=2C=CC=CC=2)C=2C=CC(N=2)=C(C=2C=CC=CC=2)C2=CC=C3[N-]2)C=2C=CC=CC=2)=NC1=C3C1=CC=CC=C1 RKTYLMNFRDHKIL-UHFFFAOYSA-N 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 238000003325 tomography Methods 0.000 description 1
Landscapes
- Magnetic Resonance Imaging Apparatus (AREA)
- Control Of Electrical Variables (AREA)
Description
【考案の詳細な説明】
利用産業分野
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 description of the invention] Industrial field of application 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 a magnetic field generator using
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 wire made of copper or aluminum wrapped in a cylindrical shape, and superconducting magnets that use special conducting wire 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
あり、汎用されるには至つていない。 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 small and generating a strong magnetic field, but it requires the use of expensive liquid helium or the like as a coolant. There is a problem that the running cost as well as the so-called initial cost is extremely high, so it has not been widely used.
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なく、漏洩磁界の少
ない永久磁石を使用するNMR−CT用磁気回路
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 has previously proposed a magnetic circuit for NMR-CT that uses permanent magnets with a magnetic field strength equal to or higher than that of the above-mentioned normal conduction magnets, consumes no power, and has a small leakage magnetic field. A magnetic field generating device for magnetically coupling a magnetic pole piece and at least one permanent magnet with a yoke to generate a magnetic field in the air gap, characterized in that an annular protrusion is provided on each opposing surface of the magnetic pole piece. Proposed a generator (patent application 1982-
No. 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、上記磁界発生装置を設計する際に、
永久磁石の磁気特性、各種構成部品の形状に基づ
いた解析により、最も効率のよい磁気回路を設計
するが、磁気特性のばらつき、各構成部品の寸法
精度のばらつき等により、設計どおりの磁界を高
精度で得るのが困難であり、また、保守管理上、
設計値どおりの磁界を維持するのが困難となる問
題があり、該磁界発生装置の組立時あるいは組立
後に、磁界調整の必要があつた。 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, when designing the above magnetic field generator,
The most efficient magnetic circuit is designed through analysis based on the magnetic properties of permanent magnets and the shapes of various component parts, but due to variations in magnetic properties and dimensional accuracy of each component, it is difficult to increase the magnetic field as designed. It is difficult to obtain accuracy, and in terms of maintenance management,
There is a problem in that it is difficult to maintain the magnetic field as designed, and it is necessary to adjust the magnetic field during or after assembly of the magnetic field generator.
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が得ら
れ、保守管理に際しても均一かつ安定な磁界を得
るために、磁界調整可能な磁気回路を有する磁界
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 been developed to obtain 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, and to provide a uniform and stable magnetic field even during maintenance management. In order to obtain a magnetic field, the object is a magnetic field generating device having a magnetic circuit capable of adjusting the magnetic field.
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、かつ磁界均一度の調整が可能な磁気回路を
目的に種々検討した結果、磁気回路において少な
くとも一方の磁極片を対向する磁極片の対向平面
と平行方向に僅かに移動させることにより、磁気
回路空隙内の磁界均一度が著しく向上し、特に、
磁極片の対向平面と平向方向に高精度で均一な磁
界域が拡大され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 that can also adjust the degree of magnetic field uniformity. By slightly moving the magnetic pole pieces in a direction parallel to the opposing plane, the magnetic field uniformity within the magnetic circuit air gap is significantly improved.
It was discovered that a highly accurate and uniform magnetic field area is expanded in the direction parallel to the opposing plane of the magnetic pole pieces.
すなわち、この考案は、空隙を形成して対向す
る一対の磁極片と、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、一対の磁極片対向面の平
行方向に、相対的に磁極片を平行移動可能となし
た磁界調整機構を有することを特徴とする磁界発
生装置である。 That is, this invention provides a magnetic field generating device that magnetically couples a pair of magnetic pole pieces facing each other with an air gap and at least one permanent magnet using a yoke, and generates a magnetic field in the air gap. This is a magnetic field generating device characterized by having a magnetic field adjusting mechanism that can relatively move the magnetic pole pieces in parallel in a direction parallel to opposing surfaces.
磁気回路は、少なくとも1の永久磁石を用い
て、空隙を介して対向させた磁極片を継鉄で磁気
的に結合すればいかなる構成も利用でき、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、磁極片形状を適宜選
定することが望ましい。 Any configuration can be used for the magnetic circuit as long as at least one permanent magnet is used and magnetic pole pieces that are opposed to each other with an air gap are magnetically coupled with a yoke. It is desirable to appropriately select the shape of the magnetic pole piece depending on the size and size of the required air gap.
また、空隙を介して対向する磁極片面に環状突
起を設けた磁気回路とするのもよく、磁極面平面
の周縁部や任意の個所に断面三角形や台形の突起
とする等種々形状の突起が採用でき、また、環状
突起の中央に凸状突起を連続、非連続で設けるの
もよい。 It is also good to have a magnetic circuit with an annular protrusion on one side of the magnetic poles facing each other with an air gap in between.Protrusions of various shapes, such as protrusions with a triangular or trapezoidal cross section, can be used on the periphery of the plane of the magnetic pole face or at any desired location. It is also possible to provide convex protrusions in the center of the annular protrusion, either continuously or discontinuously.
磁界調整機構は、相対的に磁極片を平行移動さ
せるもので、実施例に示す如く、対向する磁極片
を磁気的に結合しかつ空隙を形成保持する継鉄側
面に、非磁性ボルトを複数本配置して、ボルトの
侵入度合に応じて移動量が変化する構成など、磁
気回路構成に応じて種々の調整機構が採用できる
が、調整機構を組込んだ磁気回路における各磁極
片への影響が、磁気的に等価であることが望まし
く、永久磁石の磁気特性、形状寸法、継鉄の形状
寸法及び空隙の大きさ等に応じて適宜選定するこ
とが望ましい。 The magnetic field adjustment mechanism relatively moves the magnetic pole pieces in parallel, and as shown in the example, a plurality of non-magnetic bolts are attached to the side of the yoke that magnetically couples the opposing magnetic pole pieces and holds them by forming a gap. Various adjustment mechanisms can be adopted depending on the magnetic circuit configuration, such as a configuration in which the amount of movement changes depending on the degree of penetration of the bolt, but the influence on each magnetic pole piece in the magnetic circuit incorporating the adjustment mechanism , are preferably magnetically equivalent, and are desirably selected appropriately depending on the magnetic properties and dimensions of the permanent magnet, the dimensions of the yoke, the size of the air gap, etc.
また、磁極片の相対的な平行移動量は、必要以
上に大きくなると調整機構が大型化、複雑化する
だけでなく、磁気的バランスがくずれる要因とな
るなど種々の問題を生じるため、磁極片外径に対
して、2%以下の平行移動量が好ましい。 In addition, if the amount of relative parallel movement of the magnetic pole pieces becomes larger than necessary, it will not only make the adjustment mechanism larger and more complicated, but also cause various problems such as causing a loss of magnetic balance. The amount of parallel movement is preferably 2% or less with respect to the diameter.
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、1〜5KG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 5 kg by using the following permanent magnet, and 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、すぐれた性能を得られ、さらに、この永久磁
石の磁気特性が特に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
ことができる性質を有効に利用できる。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 this permanent magnet, it is possible to downsize the device and obtain excellent performance.Furthermore, the magnetic properties of this permanent magnet make it possible to achieve a significantly high maximum energy product by cooling it to below 0°C. You can effectively utilize the properties you can obtain.
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図と第2図はこの考案によるNMR−CT
に用いる磁気回路の縦断正面図と横断側面図であ
る。Disclosure of the invention based on drawings Figures 1 and 2 are NMR-CT based on this invention.
FIG. 2 is a vertical front view and a cross-sectional side view of a magnetic circuit used in the present invention.
第1図と第2図に示す磁気回路は、一対のFe
−B−R系永久磁石1,1の各々の一方端に磁極
片2を固着して対向させ、永久磁石1の他方端
を、円筒体からなりその円周部の一部を開口した
形状の継鉄3で結合し、磁極片2間の空隙4内
に、静磁界を発生させる構成であり、一対の磁極
片2,2には、その対向面の周縁の内側に、所定
の内径、高さからなる断面略台形の環状突起5を
突設した構成であり、Fe−B−R系永久磁石1,
1は同一方向に磁化してある。 The magnetic circuit shown in Figures 1 and 2 consists of a pair of Fe
- A magnetic pole piece 2 is fixed to one end of each of the B-R permanent magnets 1, 1, and the other end of the permanent magnet 1 is made of a cylindrical body with a part of its circumference open. They are connected by a yoke 3 and are configured to generate a static magnetic field in the air gap 4 between the magnetic pole pieces 2.The pair of magnetic pole pieces 2, 2 have a predetermined inner diameter and height on the inside of the periphery of their opposing surfaces. Fe-B-R permanent magnet 1,
1 are magnetized in the same direction.
さらに、各磁極片2の外周部に対向する位置の
継鉄3には、120゜間隔で3箇所に、それぞれ継鉄
3外周面から中心に向つて螺着された非磁性の移
動量調節ボルト6が配置してあり、各移動量調整
ボルト6の螺合進退によつて、各磁極片2が、一
対の磁極片対向面の平行方向に、相対的に磁極片
2を平行移動可能に構成してある。 Furthermore, on the yoke 3 located opposite the outer periphery of each magnetic pole piece 2, there are non-magnetic movement adjustment bolts screwed in three places at 120° intervals from the outer periphery of the yoke 3 toward the center. 6 are arranged, and each magnetic pole piece 2 is configured to be able to move relatively in parallel in the parallel direction of the pair of opposing surfaces of the magnetic pole pieces by screwing the movement adjustment bolts 6 back and forth. It has been done.
上記構成において、例えば、一方の磁極片2の
位置は固定し、他方の磁極片2の位置を3本の移
動量調整ボルト6の螺合進退によつて移動させ、
一対の磁極片2の対向中心線を僅かにずらせる
と、空隙4内は特に、水平方向に極めて高い均一
度を有する静磁界が得られる。 In the above configuration, for example, the position of one magnetic pole piece 2 is fixed, and the position of the other magnetic pole piece 2 is moved by screwing the three movement adjustment bolts 6 back and forth,
By slightly shifting the opposed center lines of the pair of magnetic pole pieces 2, a static magnetic field having extremely high uniformity in the horizontal direction can be obtained within the air gap 4.
ちなみに、第1図、第2図に示した構成の
NMR−CT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
ない、移動量調節ボルトによる磁界調整を行なつ
たところ、上記の構成からなるNMR−CTと同
様構成で上記の磁界調整機構を有しない磁気回路
と比較すると、3軸方向の150ppm以下の均一磁
界範囲が、15%拡大した。 By the way, the configuration shown in Figures 1 and 2
An Fe-B-R permanent magnet with a maximum energy product of 35 MGOe was used in the NMR-CT, and the opposing distance of the magnetic pole pieces was set to 600 mm, and the magnetic field was adjusted using the travel adjustment bolt. As a result, when compared with a magnetic circuit having the same configuration as the NMR-CT described above but without the magnetic field adjustment mechanism described above, the range of a uniform magnetic field of 150 ppm or less in three axial directions was expanded by 15%.
第1図と第2図はこの考案による磁界発生装置
に用いる磁気回路の縦断正面図と横断側面図であ
る。
1……Fe−B−R系永久磁石、2……磁極片、
3……継鉄、4……空隙、5……環状突起、6…
…移動量調節ボルト。
1 and 2 are a vertical front view and a cross-sectional side view of a magnetic circuit used in a magnetic field generating device according to this invention. 1... Fe-BR-based permanent magnet, 2... Magnetic pole piece,
3...Yoke, 4...Gap, 5...Annular protrusion, 6...
...Travel adjustment bolt.
Claims (1)
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、
一対の磁極片対向面の平行方向に、相対的に磁極
片を平行移動可能となした磁界調整機構を有する
ことを特徴とする磁界発生装置。 A magnetic field generating device that magnetically couples a pair of magnetic pole pieces facing each other with an air gap and at least one permanent magnet using a yoke to generate a magnetic field in the air gap,
A magnetic field generating device characterized by having a magnetic field adjustment mechanism capable of relatively moving a magnetic pole piece in parallel in a direction parallel to a pair of opposing surfaces of the magnetic pole pieces.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1741885U JPH0246003Y2 (en) | 1985-02-09 | 1985-02-09 | |
| EP85302389A EP0161782B1 (en) | 1984-04-11 | 1985-04-04 | Magnetic field generating device for nmr-ct |
| US06/719,820 US4672346A (en) | 1984-04-11 | 1985-04-04 | Magnetic field generating device for NMR-CT |
| DE8585302389T DE3566185D1 (en) | 1984-04-11 | 1985-04-04 | Magnetic field generating device for nmr-ct |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1741885U JPH0246003Y2 (en) | 1985-02-09 | 1985-02-09 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61134011U JPS61134011U (en) | 1986-08-21 |
| JPH0246003Y2 true JPH0246003Y2 (en) | 1990-12-05 |
Family
ID=30505100
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1741885U Expired JPH0246003Y2 (en) | 1984-04-11 | 1985-02-09 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0246003Y2 (en) |
-
1985
- 1985-02-09 JP JP1741885U patent/JPH0246003Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61134011U (en) | 1986-08-21 |
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