JPS63160315A - Gradient magnetic-field coil device for magnetic resonance imaging system - Google Patents

Gradient magnetic-field coil device for magnetic resonance imaging system

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Publication number
JPS63160315A
JPS63160315A JP61306484A JP30648486A JPS63160315A JP S63160315 A JPS63160315 A JP S63160315A JP 61306484 A JP61306484 A JP 61306484A JP 30648486 A JP30648486 A JP 30648486A JP S63160315 A JPS63160315 A JP S63160315A
Authority
JP
Japan
Prior art keywords
magnetic field
winding frame
field coil
gradient magnetic
resonance imaging
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
JP61306484A
Other languages
Japanese (ja)
Inventor
Moriaki Takechi
盛明 武智
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP61306484A priority Critical patent/JPS63160315A/en
Publication of JPS63160315A publication Critical patent/JPS63160315A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce the vibration of a spool and the noise sharply by fixing a ring-shaped rib made of a non-magnetic metal to the central part of the spool in the axial direction. CONSTITUTION:A ring-shaped rib made of a non-magnetic metal material such as stainless steel is fixed to the central part of a spool 8 in the Z-axis direction. Because Young's modulus of the metal material is high as compared with that of a non-metal material such as a resin-laminated material, it is possible to enhance the rigidity of the spool 8 against the deformation in the diametric direction. Accordingly, it is possible to reduce the vibration of the spool due to the electromagnetic force of a gradient magneticfield coil.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、磁気共鳴イメージノブ装置用傾斜磁場コイ
ル装置に関し、さらに詳しくいうと、静磁界発生用マグ
ネットの開口部に装着された巻枠と1巻枠に巻回されて
傾斜磁場を発生するコイルを備えた磁気共鳴イメージン
グ装置用傾斜磁場コイル装置に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a gradient magnetic field coil device for a magnetic resonance image knob device, and more specifically, to a gradient coil device for a magnetic resonance image knob device. The present invention relates to a gradient magnetic field coil device for a magnetic resonance imaging apparatus, which includes a coil wound around a single winding frame to generate a gradient magnetic field.

〔従来の技術〕[Conventional technology]

第≠図は従来の磁気共鳴イメージング装置のマグネット
部分を示したものである。同図において。
Figure ≠ shows the magnet part of a conventional magnetic resonance imaging device. In the same figure.

静磁場発生用マグネット(1)の開口部内側に巻枠に巻
回された傾斜磁場コイル(2)が配置名れている。
A gradient magnetic field coil (2) wound around a winding frame is arranged inside the opening of the static magnetic field generating magnet (1).

(3)はベッド装置、悴)は被験者を示す。第1図は従
来の傾斜磁場コイル(2)の構成を示し、同図において
、X軸方向傾斜磁場コイル(j)、y軸方向傾斜磁場コ
イル(4Lz軸方向傾斜磁場コイル(71が非導電性材
料でなる円筒状の巻枠rIr)に巻回、保持されている
(3) indicates the bed device, and (3) indicates the subject. Figure 1 shows the configuration of a conventional gradient magnetic field coil (2). It is wound and held in a cylindrical winding frame (rIr) made of material.

以上の構成による磁気共鳴イメージングには、マグネツ
h (1)によシ発生している空間的に均一な磁界K、
中心からの距離とともに線形に増加する傾斜磁界を重畳
させることが必要である。
For magnetic resonance imaging with the above configuration, a spatially uniform magnetic field K generated by the magnet h (1),
It is necessary to superimpose a gradient magnetic field that increases linearly with distance from the center.

第6図は、傾斜磁場コイルの発生する磁場の分布を示し
たものであシ、第を図(alは2軸方向傾斜磁場、第を
図(b)はχ軸方向傾斜磁場を示してbる。
Figure 6 shows the distribution of the magnetic field generated by the gradient magnetic field coils. Ru.

第6図(al において、2軸方向傾斜磁場コイル(7
)は。
In Figure 6 (al), the biaxial gradient magnetic field coil (7
)teeth.

軸中心0点に対称に円形コイルが配置名れてbる。A circular coil is arranged symmetrically around the 0 point of the axis center.

コイル対には互いに逆方向の電流(Ilが通電され。Currents (Il) in opposite directions are applied to the coil pair.

2軸方向の磁場(Hlが形成されるが、2軸に垂直な面
では磁場の強さは均一であシ、また2軸方向では逆極性
から正極性へと中心0点からの距離に比例して強さが直
線的に変化している。また、第6図(bl においては
、X軸方向傾斜磁場コイル(よ)は軸中心0点に対称に
≠個の鞍形コイルが配置名れている。コイルには図中矢
印の向きに電流(11が流され、2軸方向の磁場(用を
発生するが、磁場の強さはX座標に比例し、X軸に垂直
な面内では均一でろる。また、y軸方向傾斜磁場コイル
(6)は、X軸方向傾斜磁場コイル(jlを2軸のまわ
シにりσ回転することにより得られる。
A biaxial magnetic field (Hl is formed, but the strength of the magnetic field is uniform in the plane perpendicular to the two axes, and in the biaxial direction, it changes from reverse polarity to positive polarity in proportion to the distance from the center 0 point. In addition, in Figure 6 (bl), the X-axis gradient magnetic field coil (Y) has ≠ saddle-shaped coils arranged symmetrically around the 0 point of the axis center. A current (11) is passed through the coil in the direction of the arrow in the figure, generating a magnetic field in two axes, but the strength of the magnetic field is proportional to the X coordinate, and in the plane perpendicular to the X axis, The y-axis gradient magnetic field coil (6) is obtained by rotating the X-axis gradient magnetic field coil (jl) by σ around two axes.

磁気共鳴イメージング装置において、傾斜磁場コイルに
流される電流は、第7図(a)に示すようなパルス状の
波形をしている。このために傾斜磁場コイルには電流波
形と相似な波形の電磁機械力が発生する。コ゛イルで発
生した電磁機械力は1巻枠(f) K伝達され、巻枠(
r)に、第7図(blに示すような振動、騒音を発生さ
せる。
In a magnetic resonance imaging apparatus, a current passed through a gradient magnetic field coil has a pulse-like waveform as shown in FIG. 7(a). For this reason, an electromagnetic mechanical force having a waveform similar to the current waveform is generated in the gradient magnetic field coil. The electromagnetic mechanical force generated in the coil is transmitted to one winding frame (f) K, and the winding frame (
r), vibrations and noise as shown in FIG. 7 (bl) are generated.

傾斜磁場コイルは円筒状の巻枠(1) K固定されてい
るので、傾斜磁場コイルの振動、騒音を低減するには1
巻枠(J′)の剛性を高め1巻枠(rlの振動を低減す
ればよい6巻枠Trlの剛性を高めるには1巻枠材料と
してヤング率の高い金属材料を用いるのが効果的である
。しかし、傾斜磁場コイルは第7図(alに示すような
パルス状電流で駆動されるため。
Since the gradient magnetic field coil is fixed to a cylindrical winding frame (1) K, in order to reduce the vibration and noise of the gradient magnetic field coil,
It is effective to increase the rigidity of the winding frame (J') and reduce the vibration of the first winding frame (rl).In order to increase the rigidity of the sixth winding frame Trl, it is effective to use a metal material with a high Young's modulus as the first winding frame material. However, because the gradient magnetic field coil is driven by a pulsed current as shown in Fig. 7 (al).

巻枠(J′)に導電材料を使用すると、傾斜磁場コイル
の発生するパルス状磁場によって巻枠frlに渦電流が
鋳起され、傾斜磁場の空間分布および時間波形が変歪す
る。、また、鋼板などの磁性金属材料を巻枠(rlに使
用すると、マグネットの発生する静磁場分布をも変歪さ
せる。このため、傾斜磁場コイルの巻枠材料としては、
W脂積層品などの非導電材料が用いられている、 このような1円筒状巻枠(♂)の振動特性を調査の結果
1巻枠(J′)の固有振動モードは、第r図(alJb
l、(c)のような2軸方向の変形と、第り図(al、
(bl、(clのような径方向の変形との合成されたも
のとなる。そうして、径方向変形に基く振動モードは数
十■2の低周波から発生し1巻枠(、rlの振動騒音の
低減には径方向変形に基く振動の抑制が効果的であるこ
とが明らかとなった。
When a conductive material is used for the winding frame (J'), an eddy current is induced in the winding frame frl by the pulsed magnetic field generated by the gradient magnetic field coil, and the spatial distribution and temporal waveform of the gradient magnetic field are distorted. In addition, if a magnetic metal material such as a steel plate is used for the winding frame (rl), it will also distort the static magnetic field distribution generated by the magnet.For this reason, as a winding frame material for the gradient magnetic field coil,
As a result of investigating the vibration characteristics of such a single cylindrical winding frame (♂), in which a non-conductive material such as W fat laminate is used, the natural vibration mode of the first winding frame (J') is shown in Figure r ( alJb
Biaxial deformation as shown in (c) and (al,
It is a composite of radial deformation such as (bl, (cl).The vibration mode based on radial deformation is generated from several tens of 2 low frequencies, It has become clear that suppression of vibration based on radial deformation is effective in reducing vibration noise.

径方向変形に基く固有振動数αには次の関数がめる。The following function is included in the natural frequency α based on radial deformation.

ここに、(t、lは巻枠の厚さ、(D)は直径、(E)
は巻枠材料のヤング率、(ρ)は密度を表わす。
Here, (t, l is the thickness of the reel, (D) is the diameter, (E)
is the Young's modulus of the bobbin material, and (ρ) is the density.

したがって、径方向変形に基く固有振動数を高め、発生
する振動を低減するには1巻枠(lr)の板厚(tlを
厚くすればよいが1巻枠の価格0重量が増加する。
Therefore, in order to increase the natural frequency based on radial deformation and reduce the generated vibration, it is sufficient to increase the plate thickness (tl) of one winding frame (lr), but the price and weight of one winding frame increases.

〔発明が解決しようとする問題点3 以上のような従来の磁気共鳴装置用傾斜磁場コイル装置
では、コイルの励磁時に巻枠に大きな振動を発生し、振
動に伴って巻枠から騒音を発生し、巻枠の内側に位置す
る被験者に苦痛を与えるという問題点があった。また、
巻枠の振動を低減するためには非導電材料よりなる巻枠
の厚みを増加し、径方向変形に基く振動の低減を図るこ
とが考えられるが、そうすると、高価で9重量の大きな
巻枠が必要となるという問題点があった。
[Problem to be Solved by the Invention 3] In the conventional gradient magnetic field coil device for a magnetic resonance apparatus as described above, large vibrations are generated in the winding frame when the coil is excited, and noise is generated from the winding frame due to the vibration. However, there was a problem in that it caused pain to the subject located inside the reel. Also,
In order to reduce the vibration of the winding frame, it is possible to increase the thickness of the winding frame made of non-conductive material to reduce vibrations caused by radial deformation, but this would require an expensive and heavy winding frame. The problem was that it was necessary.

この発明は、上記のような問題点を解決するためになさ
れたもので、振動騒音を低減することができる磁気共鳴
イメージング装置用傾斜磁場コイル装置を得ることを目
的とする。
The present invention was made in order to solve the above-mentioned problems, and an object of the present invention is to obtain a gradient magnetic field coil device for a magnetic resonance imaging apparatus that can reduce vibration noise.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る磁気共鳴イメージング装置用傾斜磁場コ
イル装置は1巻枠の軸方向中心部に非磁性金属材料より
なる円環状リブが固着されている。
In the gradient magnetic field coil device for a magnetic resonance imaging apparatus according to the present invention, an annular rib made of a non-magnetic metal material is fixed to the axial center of one winding frame.

〔作 用〕[For production]

この発明においては、巻枠の軸方向中心部が非磁性金属
材料よυなる円環状リブな固着しているため1巻枠の径
方向変形に対する剛性が高く、径方向変形に基く振動、
騒音が著しく低減される。
In this invention, since the axial center of the winding frame is fixed to the annular rib made of non-magnetic metal material, the rigidity against radial deformation of the first winding frame is high, and the vibration caused by the radial deformation is high.
Noise is significantly reduced.

〔実施例〕〔Example〕

第1図はこの発明の一実施例を示し1図において、(り
)は巻枠(Ir)の2軸方向中心部に固着されたステン
レス鋼のような非磁性金属材料よりなる円環状リブであ
る。
FIG. 1 shows an embodiment of the present invention, and in FIG. 1, (ri) is an annular rib made of a non-magnetic metal material such as stainless steel fixed to the center of the winding frame (Ir) in the biaxial direction. be.

その他、第5図におけると同一符号は同一部分である。In addition, the same reference numerals as in FIG. 5 indicate the same parts.

以上の構成によシ、一般に、金属材料のヤング率は、樹
脂積層品などの非金属材料のヤング率に比べて高いので
1円環状リブ(り)を固着したことにより、巻枠(fl
の径方向変形に対する剛性を高めることができる。した
がって、傾斜磁場コイルの電磁力に基く巻枠振動を低減
することができる、円環状リブ(5F)は短絡環を形成
しているが、第1図のように、巻枠(I)の軸方向中心
位置に設けると。
According to the above structure, since the Young's modulus of metal materials is generally higher than that of non-metallic materials such as resin laminates, by fixing one annular rib, the winding frame (fl
The rigidity against radial deformation can be increased. Therefore, the annular rib (5F) forms a short-circuit ring that can reduce the vibration of the reel due to the electromagnetic force of the gradient magnetic field coil, but as shown in Fig. 1, the axis of the reel (I) When installed at the center of the direction.

対称配置名れる傾斜磁場コイルの中心位置にあることに
なるので、第6図fa1.(blかられかるように。
Since it is located at the center of the gradient magnetic field coil, which is called a symmetrical arrangement, it is shown in Fig. 6 fa1. (As you can see from bl.

円環状リブ(り)には傾斜磁場は鎖交しない。したがっ
て、渦電流の誘起によシ傾斜磁場を変歪させるおそれも
ない。
The gradient magnetic field does not interlink with the annular rib. Therefore, there is no fear that the gradient magnetic field will be distorted due to the induction of eddy currents.

以上のように1巻枠(1)の中央部に、樹脂積層品など
の非金属材料に比べてヤング率の高い金属材料よりなる
円環状リブ(り)を固着しているので1巻枠(r)の径
方向変形に対する剛性を高めることができ、コイル通電
時の振動騒音を著しく低減することができる。
As described above, the annular rib made of a metal material with a higher Young's modulus than non-metallic materials such as resin laminates is fixed to the center of the first reel frame (1). r) The rigidity against radial deformation can be increased, and vibration noise when the coil is energized can be significantly reduced.

第2図は他の実施例を示し、巻枠(J’)の軸方向中心
部に固着された円環状リブ(り)は、円周方向にコ分割
された非磁性金属材料よりなる円環状リブ部材(りa)
(りb)からなっている0円環状リブ部材(りa)(り
b)はボルト(10)で互いに締結されている。
FIG. 2 shows another embodiment, in which the annular rib fixed to the axial center of the winding frame (J') is an annular rib made of a non-magnetic metal material divided into co-parts in the circumferential direction. Rib member (ria)
The circular annular rib members (ria) and (rib) made up of (rib) are fastened to each other with bolts (10).

以上の構成になる傾斜磁場コイル巻枠(IIは1円環状
リブ(り)が円周方向に分割されたリブ部材(りa)(
りb)をボルト(10)で締結した構造になっているの
で1円環状リブ(り)が巻枠<Ir)の外周から容易に
装着でき、巻枠(lr)に強固に固着することができる
The gradient magnetic field coil winding frame with the above configuration (II is a rib member (ria) in which one annular rib (ri) is divided in the circumferential direction) (
Since the rib (b) is fastened with the bolt (10), the one-ring rib (ri) can be easily attached from the outer periphery of the winding frame <Ir), and can be firmly fixed to the winding frame (lr). can.

また、第3図は別の実施例を示し、巻枠(r)は。Further, FIG. 3 shows another embodiment, in which the winding frame (r) is.

軸方向にコ分割された巻枠部材(ra)(J’b)から
なっておシ、その中間に円環状リブ(り)がボルト(/
/)で固着されている。
It consists of a winding frame member (ra) (J'b) divided in the axial direction, and an annular rib (ri) in the middle of the frame member (ra) (J'b).
/) is fixed.

この構成による巻枠(lr)は、軸方向に2分割された
巻枠部材(fa)(r、b)が、軸方向中心に設けられ
た円環状リブ(り)とボルト(ll)によシ締結されて
いるので、径方向変形に対し高い剛性を有すると同時に
、各巻枠部材(ra)(rb、)の所要長が巻枠(r)
全長の約l/2に短縮されるため、安価に製作すること
ができるという利点がある。
The winding frame (lr) with this configuration has a winding frame member (fa) (r, b) divided into two parts in the axial direction, which is connected by an annular rib (ri) and a bolt (ll) provided at the center in the axial direction. Because they are fastened together, they have high rigidity against radial deformation, and at the same time, the required length of each reel member (ra) (rb,)
Since it is shortened to about 1/2 of the total length, it has the advantage that it can be manufactured at low cost.

〔発明の効果〕〔Effect of the invention〕

この発明は1以上の説明から明らかなように。 The invention will be apparent from one or more of the descriptions.

傾斜磁場コイルの巻枠の軸方向中心部に、非磁性金属材
料でなる円環状リブを固着したので、巻枠の径方向変形
に対する剛性が高められ、傾斜磁場コイルの電磁力に基
く巻枠の振動、騒音を著しく低減することができる。
An annular rib made of a non-magnetic metal material is fixed to the axial center of the winding frame of the gradient magnetic field coil, increasing the rigidity of the winding frame against radial deformation. Vibration and noise can be significantly reduced.

また、この円環状リブな巻枠の軸方向中心位置に配置し
たので、円環状リブには傾斜磁場が鎖交せず、円環状リ
ブに剛性の高い金属材料を使用しても、渦電流の誘起に
よる傾斜磁噛変歪のおそれがない。
In addition, since the annular rib is placed at the axial center of the winding frame, the gradient magnetic field does not interlink with the annular rib, and even if a highly rigid metal material is used for the annular rib, eddy currents will not occur. There is no risk of induced magnetic gradient distortion.

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

第1図はこの発明の一実施例斜視図、第2図は他の実施
例で、同図(alは正面図、(blは側面図、第3図は
別の実施例の正断面図、第≠図は従来の磁気共鳴イメー
ジング装置のマグネット部の一部切欠き斜視図、第5図
は従来の傾斜磁場゛コイル装置の斜視図、第6図は第よ
図のものの発生出場分布を示す模式図、第7図は第5図
のものにおける駆動電流および振動の波形線図、第r図
は第1図のものにおける巻枠の軸方向振動モードを示す
模式図、第2図は第よ図のものにおける巻枠の径方向振
動モードを示す模式図である。 (/1・−マグネット、(2)・・傾斜S場コイル、(
g)・・巻枠、(ra)、(tb)・・巻枠部材、(り
)φ・円環状リブ、(りa)、(りb)・・円環状リブ
部材。 なお、各図中、同一符号は同−又は相当部分を示す。 帛2図 (a)          (b) 9at9b:日yF’Y”−リブ靜材 8a、8b巻枠部オ 帛9図 X。
Fig. 1 is a perspective view of one embodiment of the present invention, Fig. 2 is another embodiment (al is a front view, (bl is a side view, Fig. 3 is a front sectional view of another embodiment, Figure ≠ is a partially cutaway perspective view of the magnet section of a conventional magnetic resonance imaging device, Figure 5 is a perspective view of a conventional gradient magnetic field coil device, and Figure 6 shows the generation distribution of the one in Figure 3. Schematic diagram: Figure 7 is a waveform diagram of drive current and vibration in the one shown in Figure 5; Figure R is a schematic diagram showing the axial vibration mode of the winding frame in the one shown in Figure 1; It is a schematic diagram showing the radial vibration mode of the winding frame in the figure. (/1 - magnet, (2)... gradient S field coil, (
g)... Winding frame, (ra), (tb)... Winding frame member, (ri) φ, annular rib, (ri a), (ri b)... annular rib member. In each figure, the same reference numerals indicate the same or corresponding parts. Folder 2 (a) (b) 9at9b: Day yF'Y"-rib protector 8a, 8b winding frame section Fig. 9X.

Claims (4)

【特許請求の範囲】[Claims] (1)静磁界発生用マグネットの開口部に装着された円
筒状の巻枠と、この巻枠に巻回保持された傾斜磁場コイ
ルと、前記巻枠の軸方向中心部に固着され非磁性金属材
料よりなる円環状リブとを備えてなる磁気共鳴イメージ
ング装置用傾斜磁場コイル装置。
(1) A cylindrical winding frame attached to the opening of a magnet for generating a static magnetic field, a gradient magnetic field coil wound and held on this winding frame, and a non-magnetic metal fixed to the axial center of the winding frame. A gradient magnetic field coil device for a magnetic resonance imaging device, comprising an annular rib made of a material.
(2)非磁性金属材料はステンレス鋼である特許請求の
範囲第1項記載の磁気共鳴イメージング装置用傾斜磁場
コイル装置。
(2) The gradient magnetic field coil device for a magnetic resonance imaging apparatus according to claim 1, wherein the nonmagnetic metal material is stainless steel.
(3)円環状リブが、円周方向に分割された円環状リブ
部材をボルトで締結してなる特許請求の範囲第1項記載
の磁気共鳴イメージング装置用傾斜磁場コイル装置。
(3) A gradient magnetic field coil device for a magnetic resonance imaging apparatus according to claim 1, wherein the annular rib is formed by fastening annular rib members divided in the circumferential direction with bolts.
(4)巻枠が、円環状リブをはさんで軸方向に配置名れ
た2つの巻枠部材からなる特許請求の範囲第1項記載の
磁気共鳴イメージング装置用傾斜磁場コイル装置。
(4) A gradient magnetic field coil device for a magnetic resonance imaging apparatus according to claim 1, wherein the winding frame comprises two winding frame members arranged in the axial direction with an annular rib sandwiched therebetween.
JP61306484A 1986-12-24 1986-12-24 Gradient magnetic-field coil device for magnetic resonance imaging system Pending JPS63160315A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61306484A JPS63160315A (en) 1986-12-24 1986-12-24 Gradient magnetic-field coil device for magnetic resonance imaging system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61306484A JPS63160315A (en) 1986-12-24 1986-12-24 Gradient magnetic-field coil device for magnetic resonance imaging system

Publications (1)

Publication Number Publication Date
JPS63160315A true JPS63160315A (en) 1988-07-04

Family

ID=17957575

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61306484A Pending JPS63160315A (en) 1986-12-24 1986-12-24 Gradient magnetic-field coil device for magnetic resonance imaging system

Country Status (1)

Country Link
JP (1) JPS63160315A (en)

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