JPS585950A - X-ray tube - Google Patents
X-ray tubeInfo
- Publication number
- JPS585950A JPS585950A JP56102417A JP10241781A JPS585950A JP S585950 A JPS585950 A JP S585950A JP 56102417 A JP56102417 A JP 56102417A JP 10241781 A JP10241781 A JP 10241781A JP S585950 A JPS585950 A JP S585950A
- Authority
- JP
- Japan
- Prior art keywords
- anode
- metal layer
- heavy
- ray
- conversion
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J35/00—X-ray tubes
- H01J35/02—Details
- H01J35/04—Electrodes ; Mutual position thereof; Constructional adaptations therefor
- H01J35/08—Anodes; Anti cathodes
- H01J35/10—Rotary anodes; Arrangements for rotating anodes; Cooling rotary anodes
Abstract
Description
【発明の詳細な説明】
本発明はxlIm撮影鋏置に装いられるXH管の改良に
関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement of the XH tube installed in the xlIm imaging scissors device.
xII管の一つに回転陽極構造の回転陽極X線管がある
。このX@管は第1図(a)の如く円錐台形状を成しそ
の円魅斜面部分にX線変換用の変換層、例えばタングス
テン等の重金属にょる層鵡
を形成した陽極PをモータMの回転8に固定し、また陽
極Pの円鍾向の一部に対向させて定位置に陽極Kl配設
すると共にこれらをガラス等の筐体Tで覆りた構成とな
っており、陽極Pt回転させつつ第1図(b) o如く
陰極により電子e¥を放出させて陽極Pの対向面に衝突
させる仁とによ〕、陽極Pのこの電子衝突点(これがX
ls焦点となる)よりxst−放出させるものである。One type of xII tube is a rotating anode X-ray tube with a rotating anode structure. This X@ tube has a truncated conical shape as shown in Fig. 1 (a), and a conversion layer for X-ray conversion, for example, a layer of heavy metal such as tungsten, is formed on the rounded slope part of the anode P. The anode Kl is fixed at the rotation 8 of the anode P, and the anode Kl is disposed at a fixed position facing a part of the anode P in the circular direction, and these are covered with a housing T made of glass or the like. While rotating, the electron e is emitted by the cathode and collided with the opposite surface of the anode P as shown in Fig. 1(b).
xst- is emitted from the ls focal point).
電子eが衝突することにより陽極Pの諌衝突点は赤熱さ
れることになるが、陽極Pは回転されるために一点のみ
加熱されることは防止できるから、これによって陽極P
の溶解を抑え、X*連続曝射會可能としてiる。陽極P
上の電子衝突点であるX41焦点は実際の焦点面積が1
1と比較的大であっても円錐台形の円節斜面に焦点が形
成され、この焦点よ)陽極Pの半径方向にX@Xrが曝
射される九め、実効焦点は九と小さくなり、この実効焦
点!、の面積のX−ビームとなりてX線は外部へ放出さ
れる。The colliding point of the anode P becomes red-hot due to the collision of the electrons e, but since the anode P is rotated, heating at only one point can be prevented.
It is possible to suppress the dissolution of X* and to enable continuous exposure. Anode P
The actual focal area of the X41 focal point, which is the electron collision point above, is 1
Even if it is relatively large (1), a focal point is formed on the circular nodal slope of the truncated cone, and when X@Xr is irradiated in the radial direction of the anode P (this focal point), the effective focal point becomes as small as 9. This effective focus! The X-rays become an X-beam with an area of , and are emitted to the outside.
ところで、このようなXil管を用いて一豐ルスx*t
一連続的に曝射する場合1即ち、一定の時間間隔で間欠
的にxIIを曝射する場合、従来はX線管の管電圧中管
電流を開閉させたb、X線管として三極形のものを用い
、そのグリッド電位を制御するなどしてX線管のオンオ
フ制御を行なうことによ〕実施するが、Xll1I管に
は高電圧の管電圧が印加されることから、スイッチング
は高電圧を対象とする制御となシ、従ってスイッチング
素子として四極真空管(テトロード管)尋を用いなけれ
ばならないのでその制御回路も複雑となる欠点があった
。By the way, using such a Xil tube,
In the case of continuous irradiation 1, that is, in the case of intermittently emitting This is carried out by controlling the grid potential of the X-ray tube to turn on and off the X-ray tube. Therefore, a tetrode vacuum tube must be used as a switching element, which has the disadvantage that the control circuit is complicated.
ところが、CT(コンビエータ・トモグラヒイ)用X線
装置中成いは循環器系の検査に供するシネ撮影用X線装
置、或いはXm透視像をディジタルデータから得るディ
ジタルラジオグラフィ装置、心血管X@装置、関欠罎射
形としてX線被曝量を抑えるようにしたX線低減化装置
等には連続ノ譬ルスx*t−必要とする場合が多くな〕
、特に画像をrイゾタル・データとして得るものの場合
には画質の改良のために/ヤルス暢と締量の安定した/
4ルスXll1iが必要となる。However, X-ray equipment for CT (combinatorial tomography), cine X-ray equipment for examination of the circulatory system, digital radiography equipment that obtains Xm fluoroscopic images from digital data, cardiovascular X@ equipment, X-ray reduction equipment, etc. designed to suppress the amount of X-ray exposure as a radiation pattern often requires a continuous nollus x*t.]
In order to improve the image quality, especially when the image is obtained as isotal data, it is necessary to improve the image quality and stabilize the image quality.
4rus Xll1i is required.
しかしながら、従来のようにパルスx!i曝射の制御に
管電圧、管電流をスイッチング方式をを供給するための
電源ケーブルの持つ浮遊容量のために電荷が残留するな
どの原因で、制御特性が変動し、X線の/譬ルス幅中x
!1線量の変動を抑えることが困難であり九。However, as in the past, pulse x! i) The control characteristics fluctuate due to residual charges due to the stray capacitance of the power cable used to supply the tube voltage and tube current switching system for controlling the irradiation. Width medium x
! 9. It is difficult to suppress fluctuations in one dose.
本発明は上記事情に鑑みて成されたもので、回転陽極の
焦点形成面にあるx11変換用の変換層例えば重金属層
を陽極の回転方向に不連続に形成し、この重金属層の途
切れる部分ではX線変換が成されないようにするととに
よ)、制御回路等が全く不要でしかも/ぜルス幅や線量
の安定し九X線パルスを発生することができるようにし
ixawt−提供することを目的とする。The present invention has been made in view of the above circumstances, and a conversion layer for x11 conversion, such as a heavy metal layer, on the focal point forming surface of a rotating anode is formed discontinuously in the rotation direction of the anode, and at the discontinuous part of the heavy metal layer. The purpose is to provide an ixawt system that can generate nine X-ray pulses with stable pulse width and dose without requiring any control circuits (by preventing X-ray conversion from occurring). shall be.
以下、本発明の一実施例について第2図を参照しながら
説明する。An embodiment of the present invention will be described below with reference to FIG.
本発明は電子ビームを衝突させることによシその電子の
持つエネルギt−x*に変換する回転陽極に着目し、こ
の回転陽極の有するXMl変換のための変換層例えば重
金属層を不連続にすることKよって重金属層の途切れる
部分ではX線変換(高電圧tX線エネルギに変換)が成
されず従って回転陽極の回転速度と焦点の面積を°考慮
して所望のΔルス幅とすべく適宜重金属部と非重金属部
の領域を設定しておくことによシ、陽極の回転とともに
陰極からの放出電子が重金属部から非重金属部へそして
再び重金属部へと衝突位置が移シ変ることになり、陽極
の回転と陽極Pの構造としては円蝕台形状の非重金属部
に対向する軌跡上に位置させて2 J 、 J J’で
示すようKこの重金属層721kl)抜くようにした3
7.第2図(b) (、)に14.114’、11.J
IS’21で示すようにたて溝状に複数本(1本でも曳
い)の溝を規則的に形成してその部分の重金属層321
−1jJ)除くようにすれば良い。The present invention focuses on a rotating anode that converts the energy of electrons into t-x* by colliding with an electron beam, and makes the conversion layer for XMl conversion, such as a heavy metal layer, of this rotating anode discontinuous. Therefore, X-ray conversion (conversion into high-voltage tX-ray energy) is not performed at the discontinuous part of the heavy metal layer, and therefore, the heavy metal is appropriately adjusted to obtain the desired Δlux width, taking into account the rotation speed of the rotating anode and the area of the focal point. By setting the area between the metal part and the non-heavy metal part, the collision position of the electrons emitted from the cathode will change from the heavy metal part to the non-heavy metal part and then back to the heavy metal part as the anode rotates. The rotation of the anode and the structure of the anode P were such that it was positioned on a locus facing the non-heavy metal part in the shape of a truncated concavity, and the heavy metal layer (721kl) was removed as shown by 2J, JJ'.
7. Figure 2(b) (,) shows 14.114', 11. J
As shown in IS'21, a plurality of vertical grooves (even one groove) are formed regularly and the heavy metal layer 321 is formed in that portion.
-1jJ) can be removed.
また、溝等を形成しなくとも重金属層、が不連続になる
ように仁の重金属層を基台21上に構成するよう圧した
り、場合によりては貫通孔としても曳い。In addition, even if grooves or the like are not formed, the heavy metal layer may be pressed so as to be discontinuous on the base 21, or may be formed as a through hole in some cases.
このような構造の回転陽極PI第1図のxII管XTの
陽極Pとして用いれば上述したように陽極Pt−回転さ
せつつ電子V−ムを放出するだけで良質の安定したX
* 14ルスが得られる。If the rotating anode PI having such a structure is used as the anode P of the
* 14 Rus obtained.
そのため、従来のように管電圧中管電流の開閉などの電
気的な制御のための制御回路が全く不要となり、従って
X線発生装置としては整流回路だけで済み、負荷変動に
対する保護回路やサージ防止のためO対策が不要となり
安価となる利点もある。Therefore, there is no need for a control circuit for electrical control such as opening and closing of tube voltage and tube current as in the past.Therefore, the X-ray generator only needs a rectifier circuit, and a protection circuit for load fluctuations and surge prevention. Therefore, there is an advantage that O countermeasures are not required and the cost is reduced.
また% X4!1iliiが安定する結果、例えばCT
装置やディジタル・2ジオダツフイ等の装置において画
像の安定や装置の信頼性が向上する。Also, as a result of stabilizing %X4!1ilii, for example, CT
The stability of images and the reliability of devices are improved in devices such as digital and 2-geo Datsufi devices.
このように回転陽極のX線焦点形成面にあるXll1!
変換用の重金属層を陽極の回転方向に適宜の間隔をもっ
て除去した構成とじ%X!I焦点がこの不連続となる重
金属層によって断続形成されるようにしたことKより、
X線管′は電源を供給すればノ譬ルス状のXMとしてX
@曝射を行なうから、巣に陽極の重金属層の分布状11
t−変更するだけで所望のパルス幅のX線14ルスを規
則的に曝射でき、しかもパルス幅は陽極の構造と回転速
度で決定されるため、ノタルスX@曝射制御のための回
路が全く不要で装置が安価となり、しか4浮遊容量など
電気的な影響は全く受けないからパルス幅やX線線量も
安定する他、このパルスX線により得られた被写体透過
X線の検出値は高精度となシ、高画質の儂が得られる等
、安価で構造簡易且つ容易に高品位のxstqルスを得
ることのできるXa管を提供することができる。In this way, Xll1! on the X-ray focus forming surface of the rotating anode!
A structure in which the heavy metal layer for conversion is removed at appropriate intervals in the rotational direction of the anode %X! Since the I focal point is formed intermittently by this discontinuous heavy metal layer,
When the X-ray tube' is supplied with power, it emits X as a nollus-like
@ Because of the irradiation, the distribution of the heavy metal layer of the anode on the nest 11
X-rays with the desired pulse width can be regularly irradiated by simply changing the t-t, and since the pulse width is determined by the structure and rotation speed of the anode, the Notarus X@ exposure control circuit is It is not necessary at all, making the equipment cheaper, and since it is completely unaffected by electrical influences such as stray capacitance, the pulse width and X-ray dose are stable, and the detected value of the X-rays transmitted through the object obtained by this pulsed X-ray is high. It is possible to provide an Xa tube that is inexpensive, has a simple structure, and can easily obtain high-quality xstq pulses with high accuracy and high image quality.
尚、本発明は上記し且つ図面に示す実施例に限定するこ
となくその要旨を変更しない範囲内で適宜変形して実施
し得るものであ)、例えば回転陽極の回転数は用途によ
)一般に20〜40回転/秒であるが近時はより高速の
ものが多くなってきているので、焦点形成面の重金属除
去部Fi轟然回転体の動釣合を考慮して配買されるにビ
デオテーゾレコー〆・へνPの釣合手法を応用して製作
することかで′!ゐ他、また陽極の材料としてはタング
ステンの他、炭素やセラミック醇も使用できることは勿
論である。It should be noted that the present invention is not limited to the embodiments described above and shown in the drawings, and can be implemented with appropriate modifications within the scope of the gist thereof.) For example, the rotation speed of the rotating anode may vary depending on the application) The rotation speed is 20 to 40 revolutions per second, but recently there are many faster speeds, so it is necessary to consider the dynamic balance of the heavy metal removal part Fi on the focal point forming surface and to consider the dynamic balance of the rotating body. By applying the νP balancing method to the record, it can be produced! In addition to tungsten, it is of course possible to use carbon or ceramic porcelain as the material for the anode.
第1図(a)if従来の回転陽極形のXmWを示す図、
第1図(b) Hその陽極と陰極及び焦点の関係を示す
図、第2図(a) (b)(、)杜本発明によるX線管
の回転陽極の形状を示す斜視図である。
21・・・基台、22・・・重金属層、xs、is’r
x4+x4’*xs、xs’、zs’・・・重金属層の
除去部分。
出願人代理人 弁理士 鈴 江 武 彦矛1
(a)
]
(a) (b)
(b)
?b
(C)
5FIG. 1(a) If a diagram showing XmW of a conventional rotating anode type,
FIG. 1(b) is a diagram showing the relationship between the anode, cathode, and focal point, and FIG. 2(a) is a perspective view showing the shape of the rotating anode of the X-ray tube according to the present invention. 21... Base, 22... Heavy metal layer, xs, is'r
x4+x4'*xs, xs', zs'...Removed portion of heavy metal layer. Applicant's agent Patent attorney Takehiko Suzue 1 (a) ] (a) (b) (b) ? b (C) 5
Claims (1)
た変換層に衝突させてX線曝射する*iit回転形とし
たX@管において、前記陽極は前記変換層の少なくとも
前記電子摘突位置を不連続とし、これにょ〕曝射X *
’t ”ルス化することを特徴とするX線管。In a rotary X@ tube, the electron tX-ray conversion material emitted from the cathode collides with a formed conversion layer to irradiate X-rays, and the anode is located at least at the electron extraction position of the conversion layer. is discontinuous, and this] exposure X *
An X-ray tube characterized by 't' russification.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56102417A JPS585950A (en) | 1981-07-01 | 1981-07-01 | X-ray tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56102417A JPS585950A (en) | 1981-07-01 | 1981-07-01 | X-ray tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS585950A true JPS585950A (en) | 1983-01-13 |
Family
ID=14326865
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP56102417A Pending JPS585950A (en) | 1981-07-01 | 1981-07-01 | X-ray tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS585950A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2013076598A1 (en) * | 2011-11-23 | 2013-05-30 | Koninklijke Philips Electronics N.V. | Periodic modulation of the x-ray intensity |
GB2517671A (en) * | 2013-03-15 | 2015-03-04 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target and rotary vacuum seal |
JP2015532427A (en) * | 2012-10-12 | 2015-11-09 | コーニンクレッカ フィリップス エヌ ヴェKoninklijke Philips N.V. | X-ray imaging apparatus and method |
-
1981
- 1981-07-01 JP JP56102417A patent/JPS585950A/en active Pending
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2013076598A1 (en) * | 2011-11-23 | 2013-05-30 | Koninklijke Philips Electronics N.V. | Periodic modulation of the x-ray intensity |
JP2015503190A (en) * | 2011-11-23 | 2015-01-29 | コーニンクレッカ フィリップス エヌ ヴェ | Periodic modulation of X-ray intensity |
US9870892B2 (en) | 2011-11-23 | 2018-01-16 | Koninklijke Philips N.V. | Periodic modulation of the X-ray intensity |
JP2015532427A (en) * | 2012-10-12 | 2015-11-09 | コーニンクレッカ フィリップス エヌ ヴェKoninklijke Philips N.V. | X-ray imaging apparatus and method |
GB2517671A (en) * | 2013-03-15 | 2015-03-04 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target and rotary vacuum seal |
US9941090B2 (en) | 2013-03-15 | 2018-04-10 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, and rotary vacuum seal |
US9947501B2 (en) | 2013-03-15 | 2018-04-17 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target, and rotary vacuum seal |
US9966217B2 (en) | 2013-03-15 | 2018-05-08 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target, and rotary vacuum seal |
US10008357B2 (en) | 2013-03-15 | 2018-06-26 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target, and rotary vacuum seal |
US10020157B2 (en) | 2013-03-15 | 2018-07-10 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target, and rotary vacuum seal |
US10096446B2 (en) | 2013-03-15 | 2018-10-09 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target, and rotary vacuum seal |
US10102997B2 (en) | 2013-03-15 | 2018-10-16 | Nikon Metrology Nv | X-ray source, high-voltage generator, electron beam gun, rotary target assembly, rotary target, and rotary vacuum seal |
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