JPH04154029A - X-ray image tube - Google Patents

X-ray image tube

Info

Publication number
JPH04154029A
JPH04154029A JP27767590A JP27767590A JPH04154029A JP H04154029 A JPH04154029 A JP H04154029A JP 27767590 A JP27767590 A JP 27767590A JP 27767590 A JP27767590 A JP 27767590A JP H04154029 A JPH04154029 A JP H04154029A
Authority
JP
Japan
Prior art keywords
input window
curvature
radius
ray image
curvature radius
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
JP27767590A
Other languages
Japanese (ja)
Inventor
Keiichi Saito
啓一 斉藤
Satoru Sano
哲 佐野
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 JP27767590A priority Critical patent/JPH04154029A/en
Publication of JPH04154029A publication Critical patent/JPH04154029A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a required structure without unnecessarily enlarging the thickness of a plate and a meridian curvature radius of an input window by making the peripheral part of the meridian curvature radius smaller than the central part so as to improve intensity of the input window. CONSTITUTION:The peripheral part 10b of the curvature radius of an input window 10 connected airtight to the open end of a bottomed cylindrical envelope main body 2, in the direction of meridian is defined smaller than the center part 10a. Namely, Rc>Re is satisfied, where Rc is the curvature radius in the center part 10a of the input window 10, and Re is the curvature radius in the peripheral part 10b. The intensity of the input window is thus improved. A required structure is thus obtained without unnecessarily enlarging the plate thickness of the input window 10 and a meridian curvature radius, and the reliability and performance of a product can be improved, while the size and the weight thereof can be reduced.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) この発明はX線イメージ管に係り、特にその真空外囲器
の入力窓の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) This invention relates to an X-ray image tube, and more particularly to an improvement in the input window of its vacuum envelope.

(従来の技術) 従来、X線イメージ管は第5図に示すように構成され、
真空外囲器1は金属あるいはガラスよりなる有底筒状の
外囲器本体2と、その開口端に気密接合された入力窓3
とからなっている。この場合、入力窓3はその子午線方
向の曲率半径が中央部も周辺部も同等に形成されている
。つまり、曲率半径は全面に亘って等しい。
(Prior Art) Conventionally, an X-ray image tube is configured as shown in FIG.
The vacuum envelope 1 includes a bottomed cylindrical envelope body 2 made of metal or glass, and an input window 3 hermetically sealed to the open end of the envelope body 2.
It consists of In this case, the input window 3 is formed so that the radius of curvature in the meridian direction is the same at both the center and the periphery. In other words, the radius of curvature is the same over the entire surface.

このような真空外囲器1内の入力側には、入力窓3に対
向して入力面4が配設されている。一方、真空外囲器1
内の出力側には、陽極5が配設されると共に出力面6が
形成され、更に真空外囲器1内の側壁に沿って集束電極
7.8が配設されている。
On the input side of such a vacuum envelope 1, an input surface 4 is arranged opposite to the input window 3. On the other hand, vacuum envelope 1
On the output side of the vacuum envelope 1, an anode 5 is arranged and an output surface 6 is formed, and a focusing electrode 7.8 is arranged along the side wall of the vacuum envelope 1.

動作時には、X線発生器から放射されたX線は被写体(
図示せず)を透過して入力面4に達し、この入力面4か
ら出た光電子が集束電極7.8及び陽極5により集束・
加速されて出力面6を励起し、この出力面6には輝度増
強された光出力像が再現される。
During operation, the X-rays emitted from the X-ray generator strike the object (
(not shown) and reach the input surface 4, and the photoelectrons emitted from the input surface 4 are focused by the focusing electrode 7.8 and the anode 5.
The acceleration excites the output surface 6, on which a light output image with enhanced brightness is reproduced.

ところで、この種のX線イメージ管は、その製造工程に
おいて信頼性を高めるため、外囲器本体2と入力窓3と
の真空気密を保つ必要が生じる。
By the way, in order to improve the reliability of this type of X-ray image tube in its manufacturing process, it is necessary to maintain vacuum tightness between the envelope body 2 and the input window 3.

この真空気密は例えば溶接であったり、圧接であったり
するが、入力窓3はX線透過率、入力窓材によるX線の
散乱を極力少なくし、且つ真空外囲器1としての強度を
十分に有するように検討されなければならない。
This vacuum sealing is achieved by welding or pressure welding, for example, but the input window 3 is designed to minimize X-ray transmittance and scattering of X-rays by the input window material, and to provide sufficient strength as the vacuum envelope 1. should be considered to ensure that the

(発明が解決しようとする課題) 真空外囲器1として入力窓3の構造を考えるとき、強度
の点に着目すると球面が良いことは言うまでもない。而
も、子午線方向の曲率半径は小さくし、板厚は厚くし、
材質としては純アルミニウム金属よりアルミニウム系合
金の方が強く、更に例えばステンレス系合金の方がより
強いことは言うまでもない。
(Problem to be Solved by the Invention) When considering the structure of the input window 3 as the vacuum envelope 1, it goes without saying that a spherical surface is better from the viewpoint of strength. However, the radius of curvature in the meridian direction should be small, the plate thickness should be thick,
As for the material, it goes without saying that an aluminum alloy is stronger than pure aluminum metal, and furthermore, for example, a stainless steel alloy is even stronger.

しかし、X線透過率は板厚を薄くした方が良く、材質も
原子番号の小さいものを選ぶのが良い。更に、X線イメ
ージ管の小形化という点では、第6図に示したように子
午線曲率半径の小さい入力窓9よりも子午線曲率半径の
大きい入力窓3の方が良い。このように、入力窓はお互
いに相反する性質を共に満足するような構造を十分考慮
する必要がある。
However, for X-ray transmittance, it is better to make the plate thinner, and it is better to select a material with a small atomic number. Furthermore, in terms of downsizing the X-ray image tube, the input window 3 having a large meridional curvature radius is better than the input window 9 having a small meridional curvature radius as shown in FIG. In this way, it is necessary to carefully consider the structure of the input window that satisfies the mutually contradictory properties.

この発明は、入力窓が十分な強度を保ちつつ、X線透過
率か高く、且つ低散乱にして小形であり、製品としての
信頼性を向上させたX線イメージ管を提供することを目
的とする。
An object of the present invention is to provide an X-ray image tube that has an input window that maintains sufficient strength, has high X-ray transmittance, has low scattering, is compact, and has improved reliability as a product. do.

[発明の構成コ (課題を解決するための手段) この発明は、有底筒状の外囲器本体の開口端(こ気密接
合された人力窓は、子午線方向の曲率半径が中央部より
周辺部の方が小さく設定されたX線イメージ管である。
[Structure of the Invention (Means for Solving the Problems) This invention provides a manual window which is airtightly connected to the open end of a bottomed cylindrical envelope main body, so that the radius of curvature in the meridian direction is larger than the center part. This is an X-ray image tube with a smaller size.

(作 用) この発明によれば、入力窓の板厚や子午線曲率半径を不
必要に大きくすることなく、必要な構造を得ることが出
来、製品の信頼性及び性能力(向上し、小形・軽量化を
図ることが出来る。
(Function) According to the present invention, the required structure can be obtained without unnecessarily increasing the board thickness or meridional curvature radius of the input window, and the reliability and performance of the product are improved. Weight reduction can be achieved.

(実施例) 以下、図面を参照して、この発明の一実施例を詳細に説
明する。
(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings.

この発明によるX線イメージ管は第1図1こ示すように
構成され、従来例(第5図)と同一箇所1こは同一符号
を付すことにすると、有底筒状の外囲器本体2の開口端
には入力窓10がTIG溶接、あるいは圧接などにより
気密接合されて、真空外囲器11が形成されている。
The X-ray image tube according to the present invention is constructed as shown in FIG. An input window 10 is hermetically sealed to the open end of the vacuum envelope 11 by TIG welding or pressure welding, thereby forming a vacuum envelope 11.

この場合、人力窓10はその子午線方向の曲率半径が、
中央部10gより周辺部10bの方が小さく設定されて
いる。即ち、入力窓10の中央部10aでの曲率半径を
Re、周辺部10bでの曲率半径をReとすれば、 Rc>Re の関係を満足するように設定されている訳である。
In this case, the radius of curvature of the human powered window 10 in the meridian direction is
The peripheral portion 10b is set smaller than the central portion 10g. That is, if the radius of curvature at the central portion 10a of the input window 10 is Re, and the radius of curvature at the peripheral portion 10b is Re, the setting is made to satisfy the relationship Rc>Re.

ここで、入力窓10の材料として、例えばアルミニウム
を用いるとガラスを用いた場合と比べて、入力窓10の
板厚を小さくすることが出来る。例えばガラスを用いた
場合は3mmの厚さが必要であったのに対し、アルミニ
ウムを用いた場合は1mmの厚さで済ますことが出来る
。その結果、X線透過率を向上させ、入力窓10による
X線の散乱を減少させることが出来、X線イメージ管の
性能を著しく向上させることが出来る。
Here, if aluminum is used as the material for the input window 10, the thickness of the input window 10 can be made smaller than when glass is used. For example, when glass is used, a thickness of 3 mm is required, whereas when aluminum is used, a thickness of 1 mm is sufficient. As a result, the X-ray transmittance can be improved and the scattering of X-rays by the input window 10 can be reduced, and the performance of the X-ray image tube can be significantly improved.

更に、アルミニウムで作られた入力窓10は、その構造
を放射線源側に凸型に出来るため、X線イメージ管の大
きさを最小限にすることが出来る。
Furthermore, since the input window 10 made of aluminum can have a convex structure toward the radiation source side, the size of the X-ray image tube can be minimized.

例えば、第2図に示すように、もし凹型の人力窓(例え
ばチタニウム製)12を用いた場合は、X線イメージ管
の大きさは凸型の入力窓10を用いた場合のX線イメー
ジ管に比べて寸法Aだけ大きくなってしまうという欠点
がある。
For example, as shown in FIG. 2, if a concave input window 12 (made of titanium, for example) is used, the size of the X-ray image tube will be the same as that of the X-ray image tube when a convex input window 10 is used. The disadvantage is that the dimension A is larger than that of .

しかし、例えば直径35cmの入力視野を有するX線イ
メージ管の入力窓には約2トンもの大気圧がかかる。
However, for example, approximately 2 tons of atmospheric pressure is applied to the input window of an X-ray image tube having an input field of view of 35 cm in diameter.

又、X線イメージ管の排気・加温脱ガス工程においては
、およそ250℃で行なわれるため、入力窓の強度は更
に弱くなってしまう。このため、人力窓の子午線方向の
曲率半径や板厚を十分検討する必要がある。
Furthermore, since the evacuation/heating and degassing process of the X-ray image tube is carried out at approximately 250° C., the strength of the input window is further weakened. For this reason, it is necessary to carefully consider the radius of curvature in the meridian direction and the plate thickness of the manual window.

そこで今、第3図に示されるように、入力窓の任意の点
Pにおいてpという外圧が作用する時、子午線方向の応
力を01、円周方向の応力をσ2、入力窓の板厚をt1
点Pにおける子午線方向の曲率半径をrl、点Pにおけ
る子午線に垂直な方向の曲率半径を「2とすれば、 σI/ r 1 + a 2 / r 2−1) / 
tという関係が成立する。入力窓の曲率半径か全て等し
い場合は、f 、 m j 2であるのてσ−pr2/
2tとなるが、曲率半径を入力窓の周辺部において小さ
くした場合は、σt−pr+/2tとなる。ここで、こ
の発明におけるrl<r2の関係を考えると、σ1〈σ
となり、入力窓にかかる応力を小さくすることが出来る
Now, as shown in Fig. 3, when an external pressure p acts at any point P on the input window, the stress in the meridian direction is 01, the stress in the circumferential direction is σ2, and the plate thickness of the input window is t1.
If the radius of curvature in the meridian direction at point P is rl, and the radius of curvature in the direction perpendicular to the meridian at point P is 2, then σI/ r 1 + a 2 / r 2-1) /
The relationship t holds true. If the radii of curvature of the input windows are all equal, then f and m j 2, so σ-pr2/
2t, but if the radius of curvature is made smaller around the input window, it becomes σt-pr+/2t. Here, considering the relationship rl<r2 in this invention, σ1<σ
Therefore, the stress applied to the input window can be reduced.

但し、半径方向の変曲位置(子午線曲率半径位置)は、
X線イメージ管の管種に応じ、σ1σ2.p、*が一定
でないので、−律には定められない。
However, the radial inflection position (meridian curvature radius position) is
Depending on the type of X-ray image tube, σ1σ2. Since p and * are not constant, it cannot be determined by the law.

尚、子午線方向の曲率半径の変化の仕方は、第4図の線
aで示されるように、中心部の曲率半径とそれより小さ
い曲率半径をある点で連続且つ微分可能になるようにつ
なげたり、同図の線すで示されるように、中心部から周
辺部まで徐々に曲率半径を小さくしていったり、同図の
線Cで示されるように、成る一定の割合で曲率半径を変
化させても良い。
The way the radius of curvature changes in the meridian direction is to connect the radius of curvature at the center and the radius of curvature smaller than that in a continuous and differentiable manner at a certain point, as shown by line a in Figure 4. , the radius of curvature is gradually reduced from the center to the periphery, as shown by the lines in the same figure, or the radius of curvature is changed at a constant rate, as shown by the line C in the figure. It's okay.

[発明の効果コ 以上説明したようにこの発明によれば、入力窓は、その
子午線曲率半径が中央部より周辺部の方か小さいので、
人力窓の強度か向上し、入力窓の板厚や子午線曲率半径
を不必要に太き(することなく、必要な構造か得られる
[Effects of the Invention] As explained above, according to the present invention, the meridional curvature radius of the input window is smaller at the periphery than at the center.
The strength of the manual window is improved, and the required structure can be obtained without making the input window's thickness or radius of meridian curvature unnecessarily thick.

その結果、製品の信頼性及び性能を向上することが出来
る。又、最小限の大きさで製造することがa来、小形化
及び軽量化が図られる。
As a result, product reliability and performance can be improved. Furthermore, since it can be manufactured to a minimum size, it can be made smaller and lighter.

【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に係るX線イメージ管を示
す縦断面図、第2図は入力窓が凸型の場合と凹型の場合
を比較した縦断面図、第3図は入力窓の強度について説
明する斜視図、第4図は子午線方向の曲率半径の変化の
仕方と入力窓の位置との関係を示す図、第5図は従来の
X線イメージ管を示す縦断面図、第6図は入力窓の子午
線方向の曲率半径が大きい場合と小さい場合のX線イメ
ージ管を示す縦断面図である。 人力窓、 ・・・入力窓の中心部、 b・・・入力窓の周辺部、 ・・・真空外囲器、
FIG. 1 is a vertical cross-sectional view showing an X-ray image tube according to an embodiment of the present invention, FIG. 2 is a vertical cross-sectional view comparing cases where the input window is convex and concave, and FIG. 3 is a vertical cross-sectional view showing the input window. FIG. 4 is a perspective view illustrating the intensity of curvature in the meridian direction, FIG. FIG. 6 is a longitudinal sectional view showing an X-ray image tube in which the input window has a large radius of curvature in the meridian direction and a small radius of curvature in the meridian direction. Manual window, ... Center of input window, b ... Periphery of input window, ... Vacuum envelope,

Claims (1)

【特許請求の範囲】 有底筒状の外囲器本体の開口端に入力窓が気密接合され
てなる真空外囲器を備えたX線イメージ管において、 上記入力窓は、子午線方向の曲率半径が中央部より周辺
部の方が小さいことを特徴とするX線イメージ管。
[Claims] In an X-ray image tube equipped with a vacuum envelope in which an input window is hermetically sealed to the open end of a bottomed cylindrical envelope body, the input window has a radius of curvature in the meridian direction. An X-ray image tube characterized in that the area is smaller at the periphery than at the center.
JP27767590A 1990-10-18 1990-10-18 X-ray image tube Pending JPH04154029A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP27767590A JPH04154029A (en) 1990-10-18 1990-10-18 X-ray image tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP27767590A JPH04154029A (en) 1990-10-18 1990-10-18 X-ray image tube

Publications (1)

Publication Number Publication Date
JPH04154029A true JPH04154029A (en) 1992-05-27

Family

ID=17586740

Family Applications (1)

Application Number Title Priority Date Filing Date
JP27767590A Pending JPH04154029A (en) 1990-10-18 1990-10-18 X-ray image tube

Country Status (1)

Country Link
JP (1) JPH04154029A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0653772A1 (en) * 1993-10-29 1995-05-17 Kabushiki Kaisha Toshiba Radiation image intensifier and method of manufacturing the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0653772A1 (en) * 1993-10-29 1995-05-17 Kabushiki Kaisha Toshiba Radiation image intensifier and method of manufacturing the same

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