JPS5960950A - X-ray tube device of rotary anode type - Google Patents

X-ray tube device of rotary anode type

Info

Publication number
JPS5960950A
JPS5960950A JP17187282A JP17187282A JPS5960950A JP S5960950 A JPS5960950 A JP S5960950A JP 17187282 A JP17187282 A JP 17187282A JP 17187282 A JP17187282 A JP 17187282A JP S5960950 A JPS5960950 A JP S5960950A
Authority
JP
Japan
Prior art keywords
magnetic
cylindrical body
rotating anode
rotary anode
axial direction
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
JP17187282A
Other languages
Japanese (ja)
Inventor
Hajime Sudo
肇 須藤
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 JP17187282A priority Critical patent/JPS5960950A/en
Publication of JPS5960950A publication Critical patent/JPS5960950A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J35/00X-ray tubes
    • H01J35/02Details
    • H01J35/04Electrodes ; Mutual position thereof; Constructional adaptations therefor
    • H01J35/08Anodes; Anti cathodes
    • H01J35/10Rotary anodes; Arrangements for rotating anodes; Cooling rotary anodes
    • H01J35/101Arrangements for rotating anodes, e.g. supporting means, means for greasing, means for sealing the axle or means for shielding or protecting the driving
    • H01J35/1017Bearings for rotating anodes
    • H01J35/103Magnetic bearings

Abstract

PURPOSE:To enable a rotary anode to be rotated without contact by supporting it radially and axially while allowing the magnetic fluxes of permanent magnets installed outside a case to pas inside cylinders which are made of a high permeability material and installed at different levels in the axial direction of the rotary anode. CONSTITUTION:A rotary anode 3 is provided with cylinders 16a and 16b which are made of a high permeability material and located at different levels in the axial direction. Inside the cylinders 16 and 16b, coils 34, 35 and 39 which cause the magnetic fluxes of annular permanent magnets 26 and 28, placed outside a vacuum case 1 corresponding to the cylinders 16a and 16b and attached to a magnetic pole 38, to pass through both a magnetic gap producing radially supporting force and magnetic gap producing axially supporting force arranged in series so as to obtain magnetic attraction and which regulate these magnetic fluxes, are installed. In addition, a driving motor 18 and displacement detectors 42 and 43 are installed, thereby constituting an X-ray tube device. As a result, the rotary anode 3 can be rotated without contact by magnetically supporting it axially and radially in a stable manner.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、回転陽極型X線管装置に係り、特に、真空容
器外に設fitさねた磁気力供給源によって回転陽極側
を完全非接触に支承させようにしたX線層・装置の改良
に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a rotating anode type X-ray tube device, and in particular, to a rotating anode type X-ray tube device in which the rotating anode side is completely non-contacted by a magnetic force supply source installed outside the vacuum vessel. This invention relates to improvements in X-ray layers and equipment that support the

〔発明の技術的背−以〕[Technical background of the invention]

X線管装置を構造的に分類すると固定陽極型と、回転陽
極型とに大別される。このうち、回転陽極型は、陽極が
回転しているので、陽極に加わる熱負荷の実効面積を大
Aくでき、これによって、1し1間的な大資荀に酬える
ことができる利点をωhえている。
Structurally, X-ray tube devices are roughly divided into fixed anode types and rotating anode types. Among these, the rotating anode type has the advantage that since the anode is rotating, the effective area of the heat load applied to the anode can be increased to a large area, and this allows for a temporary large investment. ωh is getting better.

ところで、回転陽極型のXA、+l!管装置にあって、
陽極を大負荷から保護するには、陽極をでき得る限シ高
速回転させる必鼎がある。このように、陽極を高速回転
させるに際して、回転部を機械的軸受で支承させた場合
には、通常は、高々、毎分1.8万回転程度が限界であ
る。また、機械的軸受を用いた場合には、℃時間に規定
回転数まで上昇させようとすると、大電力を心労とする
ばかりか、軸受の寿命が著しく短かくなる欠点がある。
By the way, the rotating anode type XA, +l! In the pipe equipment,
In order to protect the anode from heavy loads, it is necessary to rotate the anode as fast as possible. As described above, when the anode is rotated at a high speed and the rotating part is supported by a mechanical bearing, the rotation speed is usually at most about 18,000 rotations per minute. Further, when a mechanical bearing is used, if an attempt is made to increase the rotational speed to a specified level within a time period of 0.degree. C., it not only requires a large amount of power, but also has the disadvantage that the life of the bearing is significantly shortened.

さらに、機械的な接触による騒音が大きいので1基原用
として用いるには不向きである。
Furthermore, the noise caused by mechanical contact is large, making it unsuitable for use as a single base.

そこで、このような不具合を解消するために、最近では
、回転陽極を、真空容器外から供給される磁気力で完全
非接触に支承させるようにしたものが提案されている。
In order to solve this problem, recently it has been proposed to support the rotating anode in a completely non-contact manner using magnetic force supplied from outside the vacuum container.

すなわち、この磁気支承型の装FYは、回転陽極同軸的
に高透磁率材製の筒体を取り付けるとともに真空容器外
に上記筒体に対して磁気支承力を作用させるに必要な磁
気力を供給するだめの永久磁石および電磁石を配置して
上記筒体を軸方向、半径方向共に完全非接触に支承する
ようにしている。
In other words, in this magnetic bearing type installation FY, a cylinder made of a high magnetic permeability material is attached coaxially to the rotating anode, and the magnetic force necessary to apply a magnetic bearing force to the cylinder outside the vacuum vessel is supplied. Additional permanent magnets and electromagnets are arranged to support the cylinder in both the axial and radial directions in a completely non-contact manner.

このように、回転部を磁気力で支承するようにした回転
1(リイ1fij型XIi、Iil ’i’+装置2−
1にあっては、真空容器内において回転部が、いわゆる
浮いている形態となるので、摩」::1によるエネルギ
の損失が存在せず、機械的1i1i1受で支持されたも
のに較べて許容回転数を大幅に向上させることができ、
しかも低油イ’i’成力で親り↓゛回転数域で短時間に
上昇させることができる。:1 /、−1!(空答器内
に摩1tJ小諒]が4在していないので1j:W :F
Jjの心自己がなく・しかも% ’jm f?lI:全
体を大幅((長寿命化させるととがてきる。
In this way, the rotation 1 (Li 1fij type XIi, Iil 'i' + device 2-
1, the rotating part is in a so-called floating form within the vacuum container, so there is no loss of energy due to friction, and it is more permissible than that supported by a mechanical 1i1i1 support. The rotation speed can be significantly increased,
Moreover, the low oil pressure makes it easy to increase the engine speed in the ↓゛ rotation speed range in a short time. :1 /, -1! (There are no 4 words in the blank answer box, so 1j:W :F)
Jj's heart has no self and %'jm f? lI: Significantly increases the overall lifespan.

〔背景技術の問題点〕[Problems with background technology]

しかしながら、従来の回転陽柿型X線管装置にあっては
次のような問題があった。すなわち回転部を磁気力によ
って支承するには、軸方向の磁気支承力と半径方向の磁
気支承力とを作用させる必要があるが、従来装置では、
磁気支承力に供される永久も6石から出た418束を、
軸方向支承用磁路と半径方向支承用磁路との2つの並列
的な磁路に分配供給するようにしている。このため、磁
気抵抗の大きい力の磁路に十分な磁束を供給することが
できず、この結果、軸方向或いは半径方向+1=に磁気
剛性の大きな支承が行なえず、これが原因して結果的に
消費電力の少ない支承ができない問題があった。寸だ磁
気剛性を充分に上げることが出来ずあらゆる方向の外力
に対して充分に対抗し得ることは円錐であった。
However, the conventional rotating persimmon type X-ray tube apparatus has the following problems. In other words, in order to support the rotating part by magnetic force, it is necessary to apply an axial magnetic bearing force and a radial magnetic bearing force, but with conventional devices,
The 418 bundles from Eikyoku are subjected to magnetic bearing force,
It is distributed and supplied to two parallel magnetic paths: an axial support magnetic path and a radial support magnetic path. For this reason, it is not possible to supply sufficient magnetic flux to the magnetic path with large magnetic resistance, and as a result, it is not possible to provide support with large magnetic rigidity in the axial direction or radial direction. There was a problem in that it was not possible to provide a bearing with low power consumption. It was a cone that could not sufficiently increase the magnetic rigidity and could sufficiently resist external forces in all directions.

〔発明の目的〕[Purpose of the invention]

本発明は、このような事情に鑑みてなされたもので、そ
の目的とするところは、永久磁石を主たる磁気力供給源
として用い回転陽極側を軸方向ならびに半径方向に大き
な磁気剛性で磁気支承させることができ、もって、少な
い消費電力で全ての方向に安定した磁気支承を実現でき
る回転陽極型X線管装置を提供することにある。
The present invention has been made in view of the above circumstances, and its purpose is to magnetically support the rotating anode side with large magnetic rigidity in the axial and radial directions using a permanent magnet as the main magnetic force supply source. An object of the present invention is to provide a rotating anode type X-ray tube device that can achieve stable magnetic support in all directions with low power consumption.

〔発明の概要〕[Summary of the invention]

本発明に係るX線管装置は、内部に陰極と回転陽極とを
収容してガる真空容器内に上記回転陽極と同軸的Kかつ
上記回転陽極に連結して高透磁率材製の筒体を軸方向に
複数設けている。
The X-ray tube device according to the present invention includes a cylindrical body made of a high magnetic permeability material, which is coaxial with the rotating anode and connected to the rotating anode in a vacuum container housing a cathode and a rotating anode therein. A plurality of are provided in the axial direction.

ヤして、前記真空容器外に前記各筒体と嵌合する関係に
11911方向に着磁された環状永久磁石が上記筒体と
同敬配置l・・°さノLる。これら環状永久磁石の両1
/+#fにはこれら両Miiaにそtl、ぞれ磁気的に
接続され、それぞれで上記4p状永久イb石の一1fi
lAから出たb’Q束を刈1応する前記節体内に佃1カ
向に通過させて他喘に戻す経路で案内するとともに上記
筒体の軸方向の長さとの関連において−カと上記筒体と
の間に半径り向の磁気的吸引力を、他方と子記t゛;〕
体との間に軸方向成分をもった磁気的吸引力をそれぞれ
作用させる一対の磁極が配置6゛さり、さらに、上記各
磁極を」1過するHk’を東を割切jし得るようにコイ
ルが装着されでいる。
Then, an annular permanent magnet magnetized in the 11911 direction is disposed outside the vacuum container so as to fit into each of the cylindrical bodies, and is arranged in the same direction as the cylindrical bodies. Both of these annular permanent magnets
/+#f is magnetically connected to both Miia, and each has one of the 4P-shaped permanent stones.
The b'Q bundle coming out of lA is passed through the corresponding segmental body in one direction and guided along the path to return to the other segment, and in relation to the axial length of the cylinder, -f and the above. A radial magnetic attraction force is applied between the cylindrical body and the other side.
A pair of magnetic poles each exerting a magnetic attractive force with an axial component between the magnetic pole and the body are arranged 6゛, and furthermore, it is arranged so that Hk' passing through each of the above magnetic poles can be divided in the east. The coil is installed.

〔発明の効架・〕[Efficacy of invention]

上記A’:B成であると、各永久イム石から出た磁束は
、永久磁石〜一方の磁極〜対応するf3tJ記筒体〜他
方の磁極〜永久磁石の経路で〕fする。したがって、一
方の磁極と筒体との間に存在する磁気ギャップおよび他
方の磁極と筒体との間に存在する磁気ギャップは永久イ
遊石に対して直列となる。このプこめ、2つの磁気ギャ
ップを通る磁束は2つの磁気ギャップの磁気抵抗の和に
よっヤ決定される。前述の如く、筒体の軸方向長さとの
関連において一方の磁極と筒体との間には半径方向の磁
気的吸引力が作用し、他方のliD 極と筒体との間に
は軸方向成分をもったIJ口気気的吸引力作用するよう
に設定されているので、これら半径方向の磁気的吸引プ
ハつまり半径方向支承力と、11J1方向の磁気的吸引
力、つまh +ilb方向支承力とは、従来装置のよう
に何れか一方が極端に小さく力るよう々ことはなく、バ
ランスした値となる。したがって、永久磁石から出た磁
束を有効に利用して、回転陽極側全りクロカ向、半径方
向共に大きな磁気剛性で支承させることができる。この
だめ、従来装置とは違って磁気支承に豊する電力消費を
十分に小さな伯に抑えることができる。
When the above A':B composition is established, the magnetic flux emitted from each permanent imite is 〕f along the path from the permanent magnet to one magnetic pole to the corresponding f3tJ cylinder to the other magnetic pole to the permanent magnet. Therefore, the magnetic gap existing between one magnetic pole and the cylinder and the magnetic gap existing between the other magnetic pole and the cylinder are in series with the permanent gemstone. In this case, the magnetic flux passing through the two magnetic gaps is determined by the sum of the magnetic reluctances of the two magnetic gaps. As mentioned above, in relation to the axial length of the cylinder, a radial magnetic attractive force acts between one magnetic pole and the cylinder, and an axial magnetic attraction force acts between the other pole and the cylinder. Since the IJ port is set to act as a pneumatic attraction force with components, these radial magnetic attraction forces, that is, the radial support force, the magnetic attraction force in the 11J1 direction, and the support force in the 11J1 direction and the 11J1 direction support force. This means that unlike conventional devices, one side does not apply an extremely small force, and the force is balanced. Therefore, by effectively utilizing the magnetic flux emitted from the permanent magnet, the entire rotary anode side can be supported with large magnetic rigidity in both the circular direction and the radial direction. Therefore, unlike conventional devices, the power consumption of the magnetic bearing can be suppressed to a sufficiently small amount.

〔発明のちト施例〕[Example after invention]

以下、本発明の実施例を図面を参照しながら説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図において、図中1は絶e茨材で筒状に形成された
真空容器であシ、この真空容器I内の図中上部には陰4
!y、 2と、ブことえは円板状に形成でれ7’?回転
1%極3とが図中上]方向に九り間対向して自装置され
て因る。
In FIG. 1, numeral 1 in the figure is a vacuum container formed in a cylindrical shape from elongated thorn material.
! y, 2 and B Kokoe are formed into a disk shape 7'? The rotating 1% pole 3 is mounted opposite to the upper direction in the figure.

陰極2にtま内部に■1示し7なめフ・fラメントが装
着さizでいる。そして、上記陰極2は真空容器1の図
中土壁中央部を気密に貫通して設けられブと導体4の先
嬬部に固定されている。
Inside the cathode 2, a 7-fold filament is attached. The cathode 2 is provided airtightly penetrating the central portion of the earthen wall of the vacuum vessel 1 in the figure, and is fixed to the tip of the conductor 4.

回転1シリ極3は、その図中上面周辺部が、常に陰極2
と対向する関係に配置1シイされており、上記周辺部上
面は外周縁に近づくにしたがって所望のX線を得るのに
必要なテーパ面に形成されている。そして回転陽Qi 
3 /Ii後述するところの回転子11によって支持さ
れている。
Rotation 1 silicon electrode 3 has a peripheral part of its upper surface always connected to cathode 2.
The upper surface of the peripheral portion is formed into a tapered surface necessary to obtain the desired X-rays as it approaches the outer peripheral edge. And rotating positive Qi
3/Ii It is supported by a rotor 11 which will be described later.

しかして、前記真空容器Iの壁部で前記回転陽極3の図
中下面に対向する部分には、この部分全上記回転陽極3
の側へ向けて有底筒状に凹没させた凹没壁5が形成され
ており、さらに上記凹没壁5の、−わゆる底壁中央部に
は、上記中央部を上記凹没壁5と同心的に回転陽極側と
は反対側へ向けて凹没させた内側凹没壁6が形成されて
いる。そして、上記凹没壁5とその外側に位1〆1′す
る筒状の11で部7との間に形成された筒状空間8訃よ
、び前記内側凹没壁6内に回転子1ノが回転自在に収容
されている。
Therefore, on the wall of the vacuum chamber I, the entire portion of the rotary anode 3 facing the lower surface of the rotary anode 3 in the drawing is
A recessed wall 5 recessed in the shape of a cylinder with a bottom is formed toward the side of the recessed wall 5, and furthermore, at a central portion of the recessed wall 5, which is called a bottom wall, the central portion is connected to the recessed wall. An inner recessed wall 6 is formed concentrically with the rotary anode 5 and recessed toward the side opposite to the rotating anode side. A cylindrical space 8 is formed between the recessed wall 5 and a cylindrical portion 7 located outside the recessed wall 5, and a rotor 1 is disposed within the inner recessed wall 6. is rotatably housed.

回転子11は犬きく分けて、前記回転陽極3と同軸的に
配設され図中上端部が上記回転陽極3の図中下面中央部
に連結されるとともに図中下端仰1が前記内側凹没壁6
で囲まれた空洞内に嵌入したj−n11j+性の補助軸
12と、図中上端部が輿状絶鉱椙13を介して補助軸1
2に接続されるとともに[?21中下端(nilが前記
筒状空間8内に嵌入した筒状の回転子本体14とで構成
されている。回転子本体14は、外径がFJiJ記壁部
7の内径より小さく、また内径がiiJ記凹没壁5の外
径より大きい寸法に非砲性材または常磁性材で形−成さ
れた筒状の支持枠15と、この支持枠15の内fi1面
に軸方向17Il:2段構成に形成された環状τN11
6IL、16bと、この穢状篩16 a 、 16b内
に装着された高透磁本材製の筒体12a。
The rotor 11 is divided into two parts and arranged coaxially with the rotary anode 3, and the upper end in the figure is connected to the center of the lower surface of the rotary anode 3 in the figure, and the lower end 1 in the figure is connected to the inner recess. wall 6
The j-n11j+ auxiliary shaft 12 fitted into the cavity surrounded by
2 and is connected to [? 21 is composed of a cylindrical rotor main body 14 fitted into the cylindrical space 8. The rotor main body 14 has an outer diameter smaller than the inner diameter of the wall portion 7, A cylindrical support frame 15 made of a non-gun-like material or a paramagnetic material and having a dimension larger than the outer diameter of the recessed wall 5, and an axial direction 17Il:2 on the inner surface of this support frame 15. Annular τN11 formed in a step configuration
6IL, 16b, and a cylindrical body 12a made of a highly permeable main material mounted inside the sieves 16a, 16b.

17bと、上記支持枠15のたとえば外周面中央部に固
定さ1したモータI8のローフ1gとで構成されている
。才た、前記内側1凹没壁6の内ωiには、非常時新・
だけ前記補助軸12を機械的に支持する1紬受211L
、21bが、・塁時は、上記補助軸12に対して非接触
に設けである。さらに、補助+iQl+ 72の1ン1
中下端面にはビン22が突設してあり%とのビン22に
対向する位16にI’ll 接触板23が配設され、こ
れら接触板23とビン22とで陽恰’ili IAi導
入装罫が構成されている。そして、上6ピ接1.リミ板
23に:i:、内仰I凹没壁6のいわゆる底1・&を気
密に1.N7通した導電棒24の先端に接続されている
17b, and a loaf 1g of a motor I8 fixed to, for example, the center of the outer peripheral surface of the support frame 15. In the inside ωi of the inside 1 recessed wall 6, there is an emergency new
1 pongee support 211L that mechanically supports the auxiliary shaft 12
, 21b are provided in a non-contact manner with respect to the auxiliary shaft 12 when on base. In addition, auxiliary + iQl + 72 1 n 1
A bottle 22 is protruded from the middle and lower end surface, and a contact plate 23 is provided at a position 16 opposite to the bottle 22. The binding is configured. And upper 6 pins 1. To the limit plate 23: i:, the so-called bottom 1 & of the inward I recessed wall 6 is airtightly 1. It is connected to the tip of a conductive rod 24 passed through N7.

しかして、前記凹没壁5で囲まれた78間内には@1図
中上方から下方に亘って環状磁極材25、図示極性に1
110方向に’12 イ「Hされた:2’J状永久Jo
b石26、環状磁極材27、図示極性に軸方向に着磁さ
れた現状永久磁石28および現状磁棲旧29が同+li
t的に、かつ稍層状薦に挿小さり、ている。環状磁極材
25.29は、それぞれ上記環状永久磁石の外径とほぼ
等しい外径の環状部3θ、3ノと、この環状部30 、
 、? Jの外周i?+−1に第2図にも示すようにた
とえば90度の開き角をもって一体的に突設された磁極
32a。
Therefore, within the space 78 surrounded by the recessed wall 5, there is an annular magnetic pole material 25 extending from the top to the bottom in the drawing.
'12 in the 110 direction 'H': 2' J-shaped permanent Jo
The b stone 26, the annular magnetic pole material 27, the current permanent magnet 28 which is axially magnetized with the illustrated polarity, and the current magnetic magnet 29 are the same as +li.
It is very small and has a slightly thinner layer. The annular magnetic pole members 25 and 29 each have an annular portion 3θ, 3n having an outer diameter approximately equal to the outer diameter of the annular permanent magnet, and an annular portion 30,
,? The outer circumference of J? As shown in FIG. 2, a magnetic pole 32a integrally protrudes from +-1 with an opening angle of, for example, 90 degrees.

32 b + J 2c 、32d bよび33aL3
3b 。
32 b + J 2c , 32d b and 33aL3
3b.

ssc 、5sa(但し、33bおよび33dは図示せ
ず。)とで構成されている。そして、上記各磁極の外周
には半径方向安定化f’!i制御川のコイ用34a、3
4b 、34c 、34dおよび358゜35b  、
35c  、35d(但し、35bおよび、? 5 d
は図示せず。)がそり、それ装着されている。一方、前
記環状磁極材27は、内外径が前記環状永久磁石26.
28のそれとほぼ等しい筒状部37と、この筒状部37
の外周面に一体的に突設されたリング状磁極部38とで
構成されている。そして、上記筒状部37の両端外周に
は、軸方向安定化制御用コイル39 a + 39bが
それぞれ装着されている。なお、前記筒体17a 、 
17bの軸方向の長さは、磁極s 2a〜32 d (
33a〜33d)と磁極部38との間の距t’iil:
 、1ニジ長く設定されており、tた、筒体17aと1
7bとの間の軸方向の間隔は磁極部38の軸方向の厚み
より若干狭い関係に設定されている。
ssc, 5sa (however, 33b and 33d are not shown). The outer periphery of each magnetic pole is provided with radial stabilization f'! i control river carp 34a, 3
4b, 34c, 34d and 358°35b,
35c, 35d (however, 35b and ?5d
is not shown. ) is mounted on the sled. On the other hand, the annular magnetic pole material 27 has an inner and outer diameter equal to that of the annular permanent magnet 26.
A cylindrical portion 37 approximately equal to that of 28, and this cylindrical portion 37
The ring-shaped magnetic pole part 38 is integrally provided on the outer circumferential surface of the magnetic pole part 38. Axial stabilization control coils 39 a + 39 b are attached to the outer periphery of both ends of the cylindrical portion 37, respectively. Note that the cylindrical body 17a,
The axial length of 17b is the magnetic poles s 2a to 32 d (
33a to 33d) and the magnetic pole part 38:
, is set to be one length longer, and the cylinder bodies 17a and 1
7b is set to be slightly narrower than the axial thickness of the magnetic pole portion 38.

しかして、前記真空容器1の壁部7の外側には、上記壁
部7との間に所宗の間隙4oをあけて非磁性イ」又は常
磁性相で有底筒状に形成された筒体41が” 9fJさ
れている。そして、上記間隙40内の図中上部および下
部で前記磁極、32a〜32dおよび33a〜33dの
各磁極面に対向する位値近傍には第2図に示すように前
記回転子本体14の軸方向と偵ダする方向の変位をt見
出する変位検出器42が設けてあり、さら如軸方向忽′
位を検出する変位検出器43も設けである。また、上記
空間40内の前記ロータ19に対向する缶1i2にはモ
ータ18のステータ20が取シ伺けられている。そして
、上記ステータ2θの電機子巻線は図示しないモータ駆
動用電源に接続され、また各変位検出器42および43
の出力端は回転子安定化制御装fα51に接続されてい
る。」−配回転子安定化flt1.制御装置511′i
、実際には、半径方向の安定化をNするものと、軸方向
の安定fヒを1・!するものとで構成されており、さら
に、両者共に位い’ jJl、正安定北側■11方式を
実Lj1.するものとカバランス友シメ化flj制御方
式を実TM1するものとで捕成さルている。今、半径方
向のカバランスに′定化fii1.I御方式を実現する
ものの1つをJllJ、り出して示すと、jlJ”x 
1図に示すように対向′J−る位1、i′に存在する先
位検出器42の出力を岐ノ[ゑ・位相処i!i!装置1
ζi52、信号増幅1J置53、パワー増幅装置54ν
こ力え、この)eワー増幅装jr’j 54で上記変位
検出器間に位1ζtする半径方向安定化H11]御用の
コイルに、磁気ギャップ長の変化を位相補償及びGa1
n補償した信号を処理した、電υ1tを磁気ギャップ長
か九I加する方向に位16゛するものにはm束をjl加
させる向きに供=t、、tた磁気ギヤツノ°長かみ−少
する方向に位iaするものにはbu 9iL ?減少6
ぜる向きに供給するようにしている。軸方向変位検出器
43の出力も同じ原理で処理芒えLる。なお、第1しく
中45はX線透過窓を示している。
Therefore, on the outside of the wall 7 of the vacuum container 1, a bottomed cylindrical cylinder of non-magnetic or paramagnetic phase is provided with a gap 4o between the wall 7 and the wall 7. The body 41 has a diameter of 9fJ.The upper and lower parts of the gap 40, in the vicinity of the positions facing each of the magnetic poles 32a to 32d and 33a to 33d, are arranged as shown in FIG. A displacement detector 42 is provided for detecting the displacement of the rotor main body 14 in the axial direction and in the rectangular direction.
A displacement detector 43 for detecting the position is also provided. Further, the stator 20 of the motor 18 is inserted into the can 1i2 facing the rotor 19 in the space 40. The armature winding of the stator 2θ is connected to a motor drive power source (not shown), and each displacement detector 42 and 43
The output terminal of is connected to the rotor stabilization control device fα51. ”-allocation rotor stabilization flt1. Control device 511'i
, in fact, the radial stabilization is N and the axial stability f is 1.! Furthermore, both of them are located at the position 'jJl, and the positive stable north side ■11 method is set to the actual Lj1. The control method is comprised of one that performs the TM1 control method and one that performs the actual TM1 control method. Now, for the radial coverage fii1. One of the things that realizes the I control method is JllJ.
As shown in FIG. 1, the output of the preceding detector 42 located at the opposite position 1, i' is divided into two parts. i! Device 1
ζi52, signal amplification 1J position 53, power amplification device 54ν
Radial stabilization H11 which increases the position of 1ζt between the displacement detectors with this) e-war amplifier jr'j 54] Phase compensation and Ga1
In the case where the n-compensated signal is processed and the electric current υ1t is increased by 16° in the direction of adding 9I to the magnetic gap length, the magnetic gear horn is applied in the direction of adding m flux to jl = t, , t. bu 9iL for those who are located in the direction of decrease 6
I try to feed it in the opposite direction. The output of the axial displacement detector 43 is also processed using the same principle. Note that the first center 45 indicates an X-ray transmitting window.

このような構成であると、永久磁石26゜28から出た
磁束の“、第4図に/I!It: !−矢印で示す経路
X、、X2を;[jlって磁気支承に供される〇すなわ
ぢ1永久磁石26から出lヒ磁束は、環状bi、4極利
27の磁極バl538から回1;5ユ子1)に設けられ
た筒体77aの端面部に入り、この筒体17a内をld
l方向に通行した後、環状磁極材25の磁極32h〜3
2dに入り、上記束状磁極材25’i−介]7で永久磁
石26に戻る経1)1≦を通る。したかって、磁イヅ部
38と筒体17aの端面部との間には、軸方向成分を含
んだ磁気的吸引力、つ−まり廟1方向支承力〃・作用し
、ま/r磁極32 a 〜32 dと筒(4= 27 
aとの間には半径方向の磁気的吸引力、つまり半径方同
支承力が作用することになる。そして、lIル極部38
と筒体17gの端面部との間の磁気ギャップおよび磁極
32a〜32dと筒体17&との間の磁気ギャップは永
久磁石26VC対して直列に介在していることになるの
で、上述した軸方向支承力と半径方向支承力とは倒れか
一方が極端に小さくなることは力り、適正な値に設定出
来る。経路X2についても同様である。したがって、回
転子11は永久磁石26.28から供給された磁束によ
って回転軸方向および半径方向共に大きな支承力で支承
されることになる。なおと(D (!: t= %前述
した回転子安定化制御装散51によって、上記磁気的支
承力が回転子に加わる外力とつり合う杼に回転子の位U
4或いは電流が調節される。
With such a configuration, the magnetic flux emitted from the permanent magnet 26゜28 in Fig. 4 /I!It: ! The magnetic flux emitted from the permanent magnet 26 enters the end face of the cylinder 77a provided at the cylindrical body 77a from the magnetic pole bar 1538 of the annular bi, quadrupole 27. ld inside the cylinder 17a
After passing in the l direction, the magnetic poles 32h to 3 of the annular magnetic pole material 25
2d, and returns to the permanent magnet 26 at the bundled magnetic pole material 25'i-]7, passing through 1) 1≦. Therefore, between the magnetic pole part 38 and the end face part of the cylindrical body 17a, a magnetic attraction force including an axial component, that is, a one-way support force, acts, and the magnetic pole 32 a ~32 d and cylinder (4 = 27
A radial magnetic attraction force, that is, a radial support force acts between the a and the a. And lI le pole part 38
The magnetic gap between the cylindrical body 17g and the end face of the cylindrical body 17g and the magnetic gap between the magnetic poles 32a to 32d and the cylindrical body 17& are interposed in series with the permanent magnet 26VC. The force and the radial bearing force can be set to an appropriate value, since either one of them can become extremely small. The same applies to route X2. Therefore, the rotor 11 is supported by the magnetic flux supplied from the permanent magnets 26, 28 with a large supporting force both in the rotation axis direction and in the radial direction. Naoto (D (!: t=%) The rotor stabilization control device 51 described above causes the rotor to be placed in the shuttle where the magnetic bearing force balances the external force applied to the rotor.
4 or the current is adjusted.

したがって、同転子111rr、’、上記磁気的支承力
によって完全に非接触状態、つ−を如浮き上った状態に
支承づれる。この状態でモータ18のステータ2(7に
電蝕を接続すると、そのロータJ9が回転し、これに伴
なってiiJ記ロータ19のl1li! sされでいる
回転子11が回転を開始する。
Therefore, the trochanter 111rr,' is supported in a completely non-contact state and in a floating state due to the above-mentioned magnetic support force. When electrolytic corrosion is connected to the stator 2 (7) of the motor 18 in this state, the rotor J9 rotates, and the rotor 11 of the rotor 19 starts rotating accordingly.

したがって、回転陽極3も回転をu[]始する。そして
、回転子11が規定回転数に至った時点で軸方向安定化
制御用コイル39a、39bに信+!Fを与え、回転子
の位16を軸方向に強制的にずらすことによって陽vf
電流導入装f6゛を作動させると、回転陽極3と陰極2
との間は電位差が犬きくなシ、陰=I′l1m 、?で
発生した11□1子が回転陽極3に衝突し、こitによ
ってX 糺、J Pが第1図中矢印Pて示すように放出
される。Lまたがって、ここに回転陽極型のX線管装置
ト)゛としての機能が発揮されることになる。そして、
X?tE4非照射皓Cては、コイル39 a、 39 
bの伺勢を厚゛除するとともにモータ電(・媛を(−や
l1Jiする。このとき、回転子11は高1′L梁中に
完全非(べ触で支承されているから、几−]、゛による
回転数の減衰は無く、又、この詩カバランス安九“制御
方式を採用すれば磁気支承力?:1 、はとんど永久1
i’J石26.28によるもので、+5るフ、:め、消
費する電力の非常に少さい状態で回転を常時維]−する
ことが可能となり嘱したがって、任意の時に、最小の待
ち時間でX線を細りすることができる。
Therefore, the rotating anode 3 also starts rotating u[]. Then, when the rotor 11 reaches the specified rotation speed, a signal is sent to the axial stabilization control coils 39a and 39b! By giving F and forcibly shifting the rotor position 16 in the axial direction, the positive vf
When the current introducing device f6 is activated, the rotating anode 3 and cathode 2
There is a large potential difference between , Yin = I'l1m, ? The 11□1 particles generated in this collision collide with the rotating anode 3, and X and J P are ejected as shown by the arrow P in FIG. Astride the L, the function of a rotating anode type X-ray tube device is exerted here. and,
X? tE4 non-irradiation coil 39 a, 39
At the same time, reduce the bias of the motor b. ], There is no attenuation of the rotation speed due to ゛, and if you adopt this Kabalance Ankyu "control method, the magnetic bearing force?: 1, is almost permanent 1
Due to the i'J stone 26.28, it is possible to constantly maintain the rotation with very little power consumption.Therefore, at any given time, the minimum waiting time can narrow down the X-rays.

このように、永久磁石から出た<ra束を、半径方向支
承力を作用させるだめの磁気ギャップと軸方向支承力を
作用さぜるための磁気ギヤングとを直列に介して通過さ
せるようにしているので永久磁石から出た磁束を、適正
な値で半径方向支承および軸方向支承に有効に利用でき
、結局、前述した効果が得られる。
In this way, the <ra flux emitted from the permanent magnet is made to pass in series through the magnetic gap for applying the radial bearing force and the magnetic gearing for applying the axial bearing force. Therefore, the magnetic flux emitted from the permanent magnet can be effectively used for radial support and axial support at an appropriate value, and as a result, the above-mentioned effects can be obtained.

なお、本発明は上述しブこ実施例に限定さ?するもので
はない。すなわち、上述した実施例では、1つの環状磁
極材27で2つの磁極を兼fi1させているが、これは
別々に設けてもよい。壕だ、永久磁石26.28の内佃
に回転子を住僧゛させているが、この関係を逆にしても
伺ら支障は々い。寸だ、実施例においては冷却手段が省
略されているが真空容器外から冷却するようにしてもよ
い。また、磁気支承要素を軸方向に24fl設けている
が3組以上設けてもよい。
It should be noted that the present invention is not limited to the above-mentioned embodiments. It's not something you do. That is, in the embodiment described above, one annular magnetic pole material 27 serves as two magnetic poles, but they may be provided separately. The rotor is housed in the inner part of the permanent magnet 26.28, but even if this relationship was reversed, there would be many problems. Although the cooling means is omitted in the embodiment, cooling may be provided from outside the vacuum container. Moreover, although 24 fl of magnetic bearing elements are provided in the axial direction, three or more sets may be provided.

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

第1図は本発明の一実施例に係るX線管装置の要部縦訂
[面図、第2図は同装置を第1図1におけるA−A線に
沿って切断し矢印方向に見た断面間、第3図は同装置σ
゛を第11ン1におけるB−B絢に沿って切断し矢印方
向に見た1)1拍j図、第4図は回装僅′における41
8束の通過経路を説明するだめの図である。 1・・・真空容器、2・・・陰極、3・・・回転陽極、
5・・・凹没壁、11・・・回転子、14・・・回転子
本体、J 7 a l I 7 b・f5を体、18 
・・・モータ、26゜28・・・永久磁石。 出納1人代理人  弁理士 鈴 江 武 彦第2図 第3図 第4図 35a(35b、35c、35d)
FIG. 1 is a vertically sectional view of the main parts of an X-ray tube device according to an embodiment of the present invention, and FIG. Figure 3 shows the same device σ
1) 1 beat j diagram cut along the B-B thread in the 11th section 1 and seen in the direction of the arrow, Figure 4 shows the 41
It is a diagram for explaining the passage paths of eight bundles. 1... Vacuum vessel, 2... Cathode, 3... Rotating anode,
5... Concave wall, 11... Rotor, 14... Rotor body, J 7 a l I 7 b/f5 body, 18
...Motor, 26°28...Permanent magnet. 35a (35b, 35c, 35d)

Claims (1)

【特許請求の範囲】[Claims] 真空容器内に陰極と回転陽極とを離間対向させて配置す
るとともに上記真空容器外に設けられた磁気力供給源に
よって上記回転陽極側を完全非接触状態に磁気支承する
ようにした回転陽極形x#iI管装置において、前記回
転陽極に同軸的に軸方向に複数連結し設けられた高透磁
率材製の筒体と、前記真空容器外に前記も筒体と嵌合す
る関係に配置さハ、るとともに軸方向に着磁された上記
筒体と同数のJAJ状永久磁石と、これら環状永久磁石
の両端にそれぞれ磁気的に接続され、それぞれで上記環
状永久磁石の一端から出た磁束を対応する前記筒体内に
軸方向に)Jfl遇させて他端に戻す経路で案内すると
ともに上記筒体の軸方向の長さとの関連において一方と
上記筒体との間に半径方向の磁気的吸引力を、他方と上
記筒体との間に軸方向成分をもった磁気的吸引力をそれ
ぞれ作用させる一対の71’;j極と、これら磁極を辿
過する磁束を制御し得るように装着された代数のコイル
とをJ4、I#fi して々ることを特徴とする回転陽
極型X線管装置。
A rotating anode type x in which a cathode and a rotating anode are placed in a vacuum container so as to be spaced apart and facing each other, and the rotating anode side is magnetically supported in a completely non-contact state by a magnetic force supply source provided outside the vacuum container. #i In the II tube device, a plurality of cylindrical bodies made of a high magnetic permeability material are provided and coaxially connected to the rotating anode in the axial direction, and a cylindrical body is arranged outside the vacuum vessel in a relationship to fit with the cylindrical bodies. , and the same number of JAJ-shaped permanent magnets as the cylindrical body magnetized in the axial direction, and magnetically connected to both ends of these annular permanent magnets, each corresponding to the magnetic flux emitted from one end of the annular permanent magnet. (in the axial direction) into the cylindrical body and guided along a path returning to the other end, and a radial magnetic attraction force is generated between one cylindrical body and the cylindrical body in relation to the axial length of the cylindrical body. and a pair of 71';j poles that apply a magnetic attraction force with an axial component between the other and the cylindrical body, respectively, and a pair of poles 71'; A rotating anode type X-ray tube device characterized by having an algebraic coil and a J4, I#fi.
JP17187282A 1982-09-30 1982-09-30 X-ray tube device of rotary anode type Pending JPS5960950A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17187282A JPS5960950A (en) 1982-09-30 1982-09-30 X-ray tube device of rotary anode type

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17187282A JPS5960950A (en) 1982-09-30 1982-09-30 X-ray tube device of rotary anode type

Publications (1)

Publication Number Publication Date
JPS5960950A true JPS5960950A (en) 1984-04-07

Family

ID=15931351

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17187282A Pending JPS5960950A (en) 1982-09-30 1982-09-30 X-ray tube device of rotary anode type

Country Status (1)

Country Link
JP (1) JPS5960950A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2632451A1 (en) * 1988-06-06 1989-12-08 Mecanique Magnetique Sa X-ray tube with rotating anode mounted on a magnetic suspension
CN105666370A (en) * 2016-03-31 2016-06-15 金华职业技术学院 Aerial positioning device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2632451A1 (en) * 1988-06-06 1989-12-08 Mecanique Magnetique Sa X-ray tube with rotating anode mounted on a magnetic suspension
CN105666370A (en) * 2016-03-31 2016-06-15 金华职业技术学院 Aerial positioning device

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