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JPH0426178B2 - - Google Patents
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JPH0426178B2 - - Google Patents

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Publication number
JPH0426178B2
JPH0426178B2 JP62265296A JP26529687A JPH0426178B2 JP H0426178 B2 JPH0426178 B2 JP H0426178B2 JP 62265296 A JP62265296 A JP 62265296A JP 26529687 A JP26529687 A JP 26529687A JP H0426178 B2 JPH0426178 B2 JP H0426178B2
Authority
JP
Japan
Prior art keywords
brazing
heat storage
alloy layer
storage material
bonding
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 - Lifetime
Application number
JP62265296A
Other languages
Japanese (ja)
Other versions
JPH01109647A (en
Inventor
Yukio Takabayashi
Seiji Yabe
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.)
Tokyo Tungsten Co Ltd
Original Assignee
Tokyo Tungsten Co Ltd
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 Tokyo Tungsten Co Ltd filed Critical Tokyo Tungsten Co Ltd
Priority to JP26529687A priority Critical patent/JPH01109647A/en
Publication of JPH01109647A publication Critical patent/JPH01109647A/en
Publication of JPH0426178B2 publication Critical patent/JPH0426178B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】[Detailed description of the invention]

[産業上の利用分野] 本発明は、X線管用回転陽極とその製造方法に
関し、特に高負荷用のX線管用回転陽極とその製
造方法に関する。 [従来の技術] 一般に、X線管用回転陽極(以下、ターゲツト
と呼ぶ)は、その特性としては、高負荷に耐え、
且つ、高融点であることが要求される。そこで、
従来は、Re−W/Mo張り合わせ材料がX線管用
ターゲツトとして用いられている。さらに、ター
ゲツトの特性を向上させた高負荷用のターゲツト
として用いるために、ターゲツト自身を大型化
(大径化、厚板化)して、ターゲツトの蓄熱容量
を大きくする方法が採用されている。 しかしながら、金属からなるターゲツトの大型
化は、一方で、熱容量を増大させることができる
ものの、ターゲツト自身の質量をも増大させるこ
とになり、このため、高速回転中の回転機構に
種々の不都合を生じさせ、また、定常回転数に到
達するまでの時間を長くしてしまう等の問題があ
つた。 そこで、近年は、熱容量が大きく、且つ、軽量
であるグラフアイトを蓄熱材として用いて、Re
−W/Moを張り合わせ材料のMo側に、蓄熱材
をろう付けにより接合して組合わせた構造の高負
荷用のターゲツトが研究されている。 一般にグラフアイトと高融点金属との結合に用
いられる従来のろう材には、特開昭61−111979号
公報に記載されるように、Ti−Cu−Ni、Ti−Cu
−Si、Ti−78Ag−22Cu、Fe−36〜45Ni−Ti、
35Au−35Ni−30Moや、或いはMo−Co、Zr−
Ti等が用いられていた。 [発明が解決しようとする問題点] ところが、上述の成分からなるろう材を用いた
従来の高負荷用のX線管用のターゲツトは、ろう
付け工程中又は実際に使用される高真空中の高温
(1200℃)状態においては、蓄熱材とろう材との
境界、即ち、ろう付け部付近の温度が、1000〜
1200℃の高温になると、グラフアイトとろう材と
の境界に、ろう材成分による金属炭化物が生成し
てしまう欠点がある。 すなわち、金属炭化物は、一般に硬くて脆弱で
あるばかりでなく、生成時に体積変化が生じるた
め、Re−W/Mo張り合わせ材料と蓄熱材との間
に剥離が生じ、耐熱性及び耐衝撃性を低減させ、
抗析力の殆どない実用に耐えないターゲツトにし
てしまうという問題があつた。 そこで、本発明の目的は、上記欠点に鑑み、金
属炭化物の生じない高負荷用のX線管用回転陽極
とその製造法を提供することである。 [問題点を解決するための手段] 本発明によれば、Mo又はMo合金層にW又は
W合金層を張り合わせて形成された張り合わせ材
料と、クラフアイトを含む蓄熱材と、前記張り合
わせ材料のうちのMo又はMo合金層と前記蓄熱
材との間に介在する5〜30重量%Ru−Pdからな
るろう材とを有し、前記張り合わせ材料と蓄熱材
とは、前記ろう材を介して接合されていることを
特徴とするX線管用回転陽極が得られる。 さらに、本発明によれば、Mo又はMo合金層
にW又はW合金層を張り合わせて形成された張り
合わせ材料と、クラフアイトを含む蓄熱材と5〜
30重量%Ru−Pdからなるろう材とを準備する準
備工程と、前記張り合わせ材料のうちのMo又は
Mo合金層と前記畜熱材との間に、前記ろう材を
介在させて、真空中で、荷重を加えながら加熱
し、前記ろう材を溶解させた後冷却するろう付け
工程とを有することを特徴とするX線管用回転陽
極の製造方法が得られる。 即に、本発明は、W又は、W合金(Re−W、
ThO2−W、Ru−W、、ZrO2−W等)とMo又は
Mo合金(Hf−Mo、ZrO2−Mo、A12O3−Mo、
CO−Mo等)とからなる張り合わせ材料のMo側
に、グラフアイトを含む蓄熱材をろう付けする場
合に、そのろう材としてRu−Pdを使用するもの
である。これは、ろう材が剥離の原因となる炭化
物を生成せず、また、溶解したろう材はグラフア
イトに良く溶解し、いわゆる混合層が形成される
ため、良好な接合強度を発揮し、一方、Mo側と
の濡れ性も非常に良く、均一なろう付けが可能だ
からである。しかも、ろう材によるガス成分(特
に、水素ガス)を吸収するゲツター効果が発揮さ
れることにより、X線管内部の微量ガス成分を吸
収し、より高真空にするように作用して、結果的
に、耐電圧性に優れたX線管を形成することにな
る。 また、RuとPdとからなるろう材の化学組成
は、Ruが5〜30重量%残部Pdであり、最も好ま
しくはRuが20重量%残部であり、この数値限定
をしたのは、純パラジウムろう材及びRuが重量
で30%を越え残部Pdの化学組成のろう材は、ヒ
ートサイクル試験においてグラフアイト部分が破
断を生ずる為で、また、好ましくは、Ruが5〜
20重量%残部Pdとしたのは、純パラジウムろう
材及びRuが重量30%を越え残部Pdの化学組成の
うちのろう材は、接合部の高温抗折力が弱いから
である。 [実施例] 本発明の実施例について図面を参照して説明す
る。 まず、第1図に示すX線管用回転陽極(ターゲ
ツト)は、断面台形で中空の円錐形状のMo層1
と、このMo層1の母線がなす傾斜面上に張り合
わせた5%Re−W合金層2とからなる外径125
mm、中心部厚さ8mmの張り合わせ材料3と、この
張り合わせ材料3のうちのMo層1の底面に、Ru
−Pdからなるろう材4を介して接合された外径
120mm、厚さ15mmの高純度、高密度のグラフアイ
トからなる蓄熱材5とから構成されている。 次に、製造方法について、説明する。 まず、準備工程において、断面台形で中空の円
錐形状のMo層と5%Re−W合金層2とを張り合
わせ、上述した製品形状に成形した外径125mm、
中心部厚さ8mmの張り合わせ材料3と、外径120
mm、厚さ15mmの高純度、高密度のグラフアイトか
らなる蓄熱材5と、35gの粉末状又は箔状のRu
−Pdからなるろう材4とを準備する。尚、張り
合わせ材料3のうちのMo層1の外周に、ろう付
け時に蓄熱材5のずれを防止する枠6を取り付け
る。 次に、ろう付け工程において、この張り合わせ
材料3のうちのMo層1の底面と蓄熱材5との間
に、ろう材4を35g(0.3〜0.4g/cm2)挟み込
み、10-5Torr以下の高真空に維持された真空炉
内に入れる。真空炉内で、300〜500g/cm2の荷重
をかけながら、ろう材の融点1550〜1750℃以上の
温度に加熱し、ろう材を溶解させてろう材4を形
成し、5〜30分保持する。その後、高真空を維持
しながら室温まで冷却する。このとき、ろう材層
の厚さは0.1〜0.2mmとなり、はみ出したろう材は
切削等で除去し、完成品とする。 ここで、このターゲツトのうち、蓄熱材5をろ
う材4との境界、すわなち、ろう付け部をX線回
折法により分析したところ、剥離等の原因になる
金属炭化物の生成は見られなかつた。 また、ろう付け部の接合強度を評価するため
に、張り合わせ材料3と蓄熱材5との接合部、す
なわち、ろう材4を中心に集中荷重を加える抗折
力試験をおこなつた。 その方法が第2図及び第3図を参照して説明さ
れる。第2図は、本発明の実施例に係る高温抗折
試験の試験片を、第3図は、高温試験機を示す。
まず、モリブデンとグラフアイトとの張り合わせ
材から、モリブデン7とグラフアイト8材の接合
部分9を中心にして、長さ30mm、幅(w)5mm、
厚さ(t)1mmの第2乃至第5の試験片10,1
0……を得た。次に、第3図に示すように、各試
験片10,10,……を順次試験機に硬質棒材1
1,12を支持端としてセツトした。この状態
で、ろう付け部9に集中した荷重(L)を硬質棒材1
3を介して加えた。支持端に置かれた硬質棒材1
1,12の水平距離(スパンd)は20mmで、抗折
力(F)は、荷重(L)を段階的に調節することにより、
1/10Kg/mm2の位まで測定可能である。 真空度10-5Torr以下の炉中で、上記試験片を
1200℃、10分間加熱し、試験片10,10,…
…、破断の最少荷重(Lmin)を測定し抗折力(F)
を次の計算式を用いて計算した。その結果を表1
に示す。 F=2/3×Lmin×d/w×t2 ここで、wは試験片の幅5mm、tは試験片の厚
さ1mm、dはスパン20mm、Lminは破断時の最小
荷重である。 次に、ヒートサイクル試験について述べる。 水素中にて、タングステン板の通電加熱体15
の上に、上記抗折試験片と同一形状のろう付け試
験片を置き、次の条件にて電流の通電、遮断をく
り返し、ろう付け部9の破断の有無を確認した。 加熱温度1100〜1300℃、昇温時間30秒 昇温時間30秒、サイクル10回 その結果を表1に示す。あわせて、同条件でな
された、比較例第1、第6の試験片についても併
記する。
[Industrial Application Field] The present invention relates to a rotating anode for an X-ray tube and a method for manufacturing the same, and particularly to a rotating anode for a high-load X-ray tube and a method for manufacturing the same. [Prior Art] In general, a rotating anode for an X-ray tube (hereinafter referred to as a target) has the characteristics of being able to withstand high loads,
Moreover, it is required to have a high melting point. Therefore,
Conventionally, Re-W/Mo laminate materials have been used as targets for X-ray tubes. Furthermore, in order to use the target as a high-load target with improved target characteristics, a method has been adopted in which the target itself is made larger (larger diameter, thicker plate) to increase the heat storage capacity of the target. However, while increasing the size of a metal target can increase its heat capacity, it also increases the mass of the target itself, which causes various inconveniences to the rotating mechanism during high-speed rotation. In addition, there was a problem that the time required to reach a steady rotational speed was increased. Therefore, in recent years, graphite, which has a large heat capacity and is lightweight, has been used as a heat storage material.
- A high-load target with a structure in which W/Mo is combined with a heat storage material bonded to the Mo side of the laminated material by brazing is being researched. Conventional brazing fillers generally used for bonding graphite and high-melting point metals include Ti-Cu-Ni, Ti-Cu
-Si, Ti-78Ag-22Cu, Fe-36~45Ni-Ti,
35Au−35Ni−30Mo, or Mo−Co, Zr−
Ti etc. were used. [Problems to be Solved by the Invention] However, the conventional targets for high-load X-ray tubes using brazing filler metals made of the above-mentioned components cannot be used at high temperatures during the brazing process or in the high vacuum in which they are actually used. (1200℃), the temperature near the boundary between the heat storage material and the brazing material, that is, the brazing area, is 1000℃
At high temperatures of 1,200°C, metal carbides from the brazing filler metal components are formed at the boundary between the graphite and the brazing filler metal. In other words, metal carbides are not only hard and brittle in general, but also change in volume during formation, which causes separation between the Re-W/Mo laminate material and the heat storage material, reducing heat resistance and impact resistance. let me,
There was a problem in that the target had almost no resistance and was not suitable for practical use. SUMMARY OF THE INVENTION In view of the above drawbacks, an object of the present invention is to provide a rotating anode for a high-load X-ray tube that does not generate metal carbides, and a method for manufacturing the same. [Means for Solving the Problems] According to the present invention, a bonding material formed by bonding a W or W alloy layer to a Mo or Mo alloy layer, a heat storage material containing craftite, and one of the bonding materials A brazing material made of 5 to 30% by weight Ru-Pd is interposed between the Mo or Mo alloy layer and the heat storage material, and the bonding material and the heat storage material are joined via the brazing material. A rotating anode for an X-ray tube is obtained. Furthermore, according to the present invention, a bonding material formed by bonding a W or W alloy layer to a Mo or Mo alloy layer, and a heat storage material containing kraftite.
A preparation process of preparing a brazing material consisting of 30% by weight Ru-Pd, and a brazing material consisting of 30% by weight of Ru-Pd, and
a brazing step in which the brazing material is interposed between the Mo alloy layer and the heat storage material, heating is performed in a vacuum while applying a load, and the brazing material is melted and then cooled. A method for producing a characteristic rotating anode for an X-ray tube is obtained. Specifically, the present invention provides W or a W alloy (Re-W,
ThO 2 -W, Ru-W, ZrO 2 -W, etc.) and Mo or
Mo alloy (Hf−Mo, ZrO 2 −Mo, A 12 O 3 −Mo,
Ru-Pd is used as a brazing material when a heat storage material containing graphite is brazed to the Mo side of a bonding material made of (CO--Mo, etc.). This is because the brazing filler metal does not generate carbides that can cause peeling, and the melted brazing filler metal dissolves well in graphite, forming a so-called mixed layer, so it exhibits good bonding strength. This is because it has very good wettability with the Mo side, allowing uniform brazing. Moreover, the getter effect of absorbing gas components (especially hydrogen gas) by the brazing material absorbs trace gas components inside the X-ray tube, working to create a higher vacuum, resulting in In addition, an X-ray tube with excellent voltage resistance is formed. In addition, the chemical composition of the brazing filler metal consisting of Ru and Pd is 5 to 30% by weight of Ru with the balance being Pd, and most preferably Ru with the balance being 20% by weight. This is because a brazing filler metal with a chemical composition in which Ru exceeds 30% by weight and the remainder is Pd will cause breakage in the graphite portion in a heat cycle test.
The reason for setting the balance Pd to 20% by weight is that pure palladium brazing filler metals and brazing filler metals with a chemical composition in which Ru exceeds 30% by weight and the balance Pd has a weak high-temperature transverse rupture strength at the joint. [Example] An example of the present invention will be described with reference to the drawings. First, the rotating anode (target) for an X-ray tube shown in Fig. 1 consists of a hollow conical Mo layer 1 with a trapezoidal cross section.
and the 5% Re-W alloy layer 2 laminated on the inclined surface formed by the generatrix of this Mo layer 1.
A bonded material 3 with a thickness of 8 mm at the center and Ru on the bottom surface of the Mo layer 1 of this bonded material 3.
−Outer diameter joined via brazing filler metal 4 made of Pd
It is composed of a heat storage material 5 made of high-purity, high-density graphite with a length of 120 mm and a thickness of 15 mm. Next, the manufacturing method will be explained. First, in the preparation process, a hollow cone-shaped Mo layer with a trapezoidal cross section and a 5% Re-W alloy layer 2 were laminated together and formed into the above-mentioned product shape with an outer diameter of 125 mm.
Laminated material 3 with center thickness 8mm and outer diameter 120
Thermal storage material 5 made of high-purity, high-density graphite with a thickness of 15 mm and 35 g of powdered or foil Ru
- Prepare a brazing filler metal 4 made of Pd. A frame 6 is attached to the outer periphery of the Mo layer 1 of the bonding material 3 to prevent the heat storage material 5 from shifting during brazing. Next, in the brazing process, 35 g (0.3 to 0.4 g/cm 2 ) of brazing material 4 is sandwiched between the bottom surface of the Mo layer 1 of this bonding material 3 and the heat storage material 5, and the amount is 10 -5 Torr or less. Place it in a vacuum furnace maintained at a high vacuum. In a vacuum furnace, while applying a load of 300 to 500 g/ cm2 , heat to a temperature above the melting point of the brazing material of 1550 to 1750°C to melt the brazing material to form the brazing material 4, and hold for 5 to 30 minutes. do. Thereafter, it is cooled to room temperature while maintaining a high vacuum. At this time, the thickness of the brazing material layer is 0.1 to 0.2 mm, and the protruding brazing material is removed by cutting or the like to form a finished product. Of these targets, when the boundary between the heat storage material 5 and the brazing material 4, that is, the brazed part, was analyzed by X-ray diffraction, no formation of metal carbides that could cause peeling etc. was observed. Ta. In addition, in order to evaluate the bonding strength of the brazed portion, a transverse rupture strength test was conducted in which a concentrated load was applied to the bonded portion between the laminate material 3 and the heat storage material 5, that is, the brazing material 4. The method will be explained with reference to FIGS. 2 and 3. FIG. 2 shows a test piece for a high-temperature bending test according to an example of the present invention, and FIG. 3 shows a high-temperature testing machine.
First, from the laminated material of molybdenum and graphite, the length is 30 mm, the width (w) is 5 mm, and the joint part 9 of molybdenum 7 and graphite 8 is the center.
Second to fifth test pieces 10,1 with a thickness (t) of 1 mm
I got 0... Next, as shown in Fig. 3, each test piece 10, 10, . . .
1 and 12 were set as supporting ends. In this state, the load (L) concentrated on the brazed part 9 is applied to the hard bar 1.
Added via 3. Rigid bar 1 placed on the support end
The horizontal distance (span d) of 1 and 12 is 20 mm, and the transverse rupture force (F) can be adjusted by adjusting the load (L) in stages.
It is possible to measure up to 1/10Kg/ mm2 . The above test piece was placed in a furnace with a vacuum level of 10 -5 Torr or less.
Heating at 1200℃ for 10 minutes, test pieces 10, 10,...
..., measure the minimum load at break (Lmin) and calculate the transverse rupture force (F)
was calculated using the following formula. Table 1 shows the results.
Shown below. F=2/3×Lmin×d/w×t 2 where w is the width of the test piece 5 mm, t is the thickness of the test piece 1 mm, d is the span 20 mm, and Lmin is the minimum load at breakage. Next, a heat cycle test will be described. In hydrogen, tungsten plate electrically heated body 15
A brazed test piece having the same shape as the above bending test piece was placed on top of the test piece, and the presence or absence of breakage of the brazed portion 9 was confirmed by repeatedly turning on and cutting off the current under the following conditions. Heating temperature: 1100 to 1300°C, heating time: 30 seconds, heating time: 30 seconds, cycle: 10 times The results are shown in Table 1. In addition, the first and sixth comparative example test pieces, which were made under the same conditions, are also described.

【表】 ここで、ヒートサイクル試験欄の○印は、破断
無しを示す。 表1から、Ru5〜20重量%、残部Pdの化学組
成のろう材を使用したものは、殆ど抗折力のない
従来のターゲツトに比べ高温抗折力(F)が大きく、
かつヒートサイクル試験においても破断が無い。 一方、室温における抗折試験の結果、表1の化
学組成のろう材を使用した試験片10は、全て、
ろう付部9で破断せず、グラフアイト母材8で遮
断し、母材8より大きな接合強度を有することが
確認された。 [発明の効果] 以上の説明のとおり、本発明によれば、剥離の
原因となる金属炭化物を生成せず、また、グラフ
アイトに良く溶解して良好な接合強度を発揮し、
一方、Mo側との濡れ性も非常に良く、均一なろ
う付けが可能なため、常温はもとより高温での接
合強度が優れており、さらに、高温での温度変化
に対しても破断されない、X線管用回転陽極が得
られる。さらに、本発明によれば、ガス成分(特
に、水素ガス)を吸吸するゲツター効果を有し、
X線管内部の微量ガス成分を吸収し、より高真空
にするように作用する耐電圧性に優れたX線管用
回転陽極が得られる。
[Table] Here, the mark ○ in the heat cycle test column indicates no breakage. From Table 1, it can be seen that those using a brazing filler metal with a chemical composition of 5 to 20% by weight of Ru and the balance Pd have a higher high-temperature transverse rupture strength (F) than conventional targets that have almost no transverse rupture strength.
Moreover, there was no breakage in the heat cycle test. On the other hand, as a result of the bending test at room temperature, all of the test pieces 10 using the brazing filler metal with the chemical composition shown in Table 1 had
It was confirmed that the bond did not break at the brazed portion 9, was blocked by the graphite base material 8, and had a bonding strength greater than that of the base material 8. [Effects of the Invention] As explained above, according to the present invention, metal carbides that cause peeling are not generated, and the metal carbide dissolves well in graphite and exhibits good bonding strength.
On the other hand, it has very good wettability with the Mo side and enables uniform brazing, so the bonding strength is excellent not only at room temperature but also at high temperatures. A rotating anode for wire tubes is obtained. Furthermore, according to the present invention, it has a Getter effect that absorbs gas components (particularly hydrogen gas),
A rotating anode for an X-ray tube with excellent voltage resistance that absorbs trace gas components inside the X-ray tube and acts to create a higher vacuum can be obtained.

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

第1図は、本発明の一実施例に係るX線管用回
転陽極を示す断面図、第2図は、本発明の効果を
確認するために使用される高温抗折試験片を示す
図、第3図は、第2図に示された試験片を試験す
る高温抗折試験機を示す図第4図は、第2図の試
験片のヒートサイクル試験を説明するための図で
ある。 図中1はMo層、2はRe−W合金層、3は張り
合わせ材料、4はろう材、5は蓄熱材、6は枠、
9はろう付接合部、10は試験片である。
FIG. 1 is a sectional view showing a rotating anode for an X-ray tube according to an embodiment of the present invention, FIG. 2 is a view showing a high temperature bending test piece used to confirm the effects of the present invention, and FIG. FIG. 3 is a diagram showing a high temperature bending tester for testing the test piece shown in FIG. 2. FIG. 4 is a diagram for explaining a heat cycle test of the test piece shown in FIG. In the figure, 1 is a Mo layer, 2 is a Re-W alloy layer, 3 is a bonding material, 4 is a brazing material, 5 is a heat storage material, 6 is a frame,
9 is a brazed joint, and 10 is a test piece.

Claims (1)

【特許請求の範囲】 1 Mo又はMo合金層にW又はW合金層を張り
合わせて形成された張り合わせ材料と、グラフア
イトを含む蓄熱材と、5〜30重量%Ru−Pdから
なるろう材とを有し、前記ろう材を、前記張り合
わせ材料のうちのMo又はMo合金層と前記蓄畜
熱材との間に介在させて、前記張り合わせ材料と
蓄熱材とを接合したことを特徴とするX線管用回
転陽極。 2 Mo又はMo合金層にW又はW合金層を張り
合わせて形成された張り合わせ材料と、グラフア
イトを含む蓄熱材と、5〜30重量%Ru−Pdから
なるろう材とを準備する準備工程と、前記張り合
わせ材料のうちのMo又はMo合金層と前記蓄熱
材との間に前記ろう材を介在させて、真空中で、
荷重を加えながら加熱し、前記ろう材を溶解させ
た後冷却させるろう付け工程とを有することを特
徴とするX線管用回転陽極の製造方法。
[Claims] 1. A lamination material formed by laminating a W or W alloy layer on a Mo or Mo alloy layer, a heat storage material containing graphite, and a brazing material consisting of 5 to 30% by weight Ru-Pd. X-rays, characterized in that the brazing material is interposed between the Mo or Mo alloy layer of the laminated material and the heat storage material to bond the laminated material and the heat storage material. Rotating anode for pipes. 2. A preparation step of preparing a bonding material formed by bonding a W or W alloy layer to a Mo or Mo alloy layer, a heat storage material containing graphite, and a brazing material consisting of 5 to 30% by weight Ru-Pd; In a vacuum, the brazing material is interposed between the Mo or Mo alloy layer of the laminated material and the heat storage material,
A method for manufacturing a rotating anode for an X-ray tube, comprising a brazing step of heating while applying a load, melting the brazing material, and then cooling.
JP26529687A 1987-10-22 1987-10-22 Rotary anode for x-ray tube and its manufacture Granted JPH01109647A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26529687A JPH01109647A (en) 1987-10-22 1987-10-22 Rotary anode for x-ray tube and its manufacture

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26529687A JPH01109647A (en) 1987-10-22 1987-10-22 Rotary anode for x-ray tube and its manufacture

Publications (2)

Publication Number Publication Date
JPH01109647A JPH01109647A (en) 1989-04-26
JPH0426178B2 true JPH0426178B2 (en) 1992-05-06

Family

ID=17415233

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26529687A Granted JPH01109647A (en) 1987-10-22 1987-10-22 Rotary anode for x-ray tube and its manufacture

Country Status (1)

Country Link
JP (1) JPH01109647A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3052240B2 (en) * 1998-02-27 2000-06-12 東京タングステン株式会社 Rotating anode for X-ray tube and method for producing the same
DE10319549B3 (en) * 2003-04-30 2004-12-23 Siemens Ag Rotating anode X-ray tube has a transition part for connecting a shaft to a lid
US7508916B2 (en) * 2006-12-08 2009-03-24 General Electric Company Convectively cooled x-ray tube target and method of making same
CN108453413A (en) * 2018-03-30 2018-08-28 西安瑞鑫科金属材料有限责任公司 A kind of palladium ruthenium binary alloy brazing material

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4073426A (en) * 1977-04-18 1978-02-14 General Electric Company Method for joining an anode target comprising tungsten to a graphite substrate
US4119879A (en) * 1977-04-18 1978-10-10 General Electric Company Graphite disc assembly for a rotating x-ray anode tube
DE3226858A1 (en) * 1982-07-17 1984-01-19 Philips Patentverwaltung Gmbh, 2000 Hamburg TURNING ANODE TUBE TUBES

Also Published As

Publication number Publication date
JPH01109647A (en) 1989-04-26

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