JPS6167725A - Method for vacuum arc-melting active metal having high melting point and alloy thereof - Google Patents
Method for vacuum arc-melting active metal having high melting point and alloy thereofInfo
- Publication number
- JPS6167725A JPS6167725A JP19005684A JP19005684A JPS6167725A JP S6167725 A JPS6167725 A JP S6167725A JP 19005684 A JP19005684 A JP 19005684A JP 19005684 A JP19005684 A JP 19005684A JP S6167725 A JPS6167725 A JP S6167725A
- Authority
- JP
- Japan
- Prior art keywords
- melting
- molten metal
- hot top
- stage
- vacuum arc
- 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.)
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- Manufacture And Refinement Of Metals (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
この発明は、Ti5Zr等の高融点活性金属及びその合
金の真空アーク溶解において、均質性のすぐれた鋳塊を
得るための真空アーク溶解方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to a vacuum arc melting method for obtaining an ingot with excellent homogeneity in vacuum arc melting of high melting point active metals such as Ti5Zr and their alloys.
従来の技術
高融点活性金属は通常真空アーク溶解して溶製されるが
、その方法は一定の電流で定常溶解し、溶解後期に20
〜60分程度の比較的短時間内で溶解電流を減少させる
、いわゆるホットトップを行なうものである。Conventional technology High melting point active metals are usually melted by vacuum arc melting, but this method involves constant melting with a constant current, and in the late stage of melting, 20
This is a so-called hot top process in which the melting current is reduced within a relatively short period of about 60 minutes.
消耗電極式真空アーク溶解における溶融金属の凝固は、
初期においては鋳型底面からの凝固が支配的であるが、
ある一定時刻を過ぎると鋳型壁面からの凝固が著しく大
きくなる。この時期では、溶湯プールの深さは溶解速度
が一定であれば一定となり、凝固は下方から順次上方へ
進行し、それに伴って消耗電極より給湯されるので、残
留部分は比較的に均一化され、中心部での成分偏析、収
縮孔の発生は少ない。Solidification of molten metal in consumable electrode vacuum arc melting is
In the initial stage, solidification from the bottom of the mold is dominant;
After a certain period of time, the amount of solidification from the mold wall increases significantly. At this stage, the depth of the molten metal pool is constant if the melting rate is constant, solidification progresses sequentially from the bottom to the top, and as the metal is supplied from the consumable electrode, the remaining portion is relatively uniform. , component segregation and shrinkage pores in the center are small.
しかしながら、溶解終了時に電源を切った際の溶湯プー
ルが深ければ成分偏析、収縮孔は太き(なる。そのため
、溶解後期にはホットトップを実施するが、この際電流
を適正に制御しなければ均質性を改善することはできな
い。However, if the molten metal pool is deep when the power is turned off at the end of melting, the components will be segregated and the shrinkage pores will be thick.Therefore, a hot top is carried out in the late stage of melting, but the current must be properly controlled at this time. Homogeneity cannot be improved.
しかるに、現在一般に行なわれている溶解末期に行なっ
ているホットトップは、時間が比較的短かく、溶湯プー
ルが、まだかなり深い状態で溶解を終了しているため、
成分偏析、収縮孔共に十分軽減されるに至っていない。However, the current hot top method, which is generally carried out at the final stage of melting, takes a relatively short time and finishes melting while the molten metal pool is still quite deep.
Both component segregation and shrinkage pores have not been sufficiently reduced.
そこで、従来より種々の工夫がなされており、収縮孔の
発生を低減させる方法として、例えば特公昭41−83
21号に溶解初期より溶解電流を一定の減速係数により
徐々に低下させる方法がある。Therefore, various efforts have been made to reduce the occurrence of shrinkage holes.
No. 21 has a method in which the melting current is gradually lowered by a constant deceleration coefficient from the early stage of melting.
発明が解決しようとする問題点
上記収縮孔発生の低減方法は、溶湯プールの上面からの
凝固を防ぎつつ溶湯ブール深さを徐々に小さくして収縮
孔の発生を防止するものである。Problems to be Solved by the Invention The above method for reducing the occurrence of shrinkage holes is to prevent the occurrence of shrinkage holes by gradually decreasing the depth of the molten metal boule while preventing solidification from the upper surface of the molten metal pool.
しかしながら、この場合にはホットトップ時間を長くす
るために、溶解速度が小さくなり、生産性が悪化し、又
鋳塊の表面品質も低下する。However, in this case, since the hot top time is increased, the melting rate becomes low, productivity deteriorates, and the surface quality of the ingot also deteriorates.
この発明は、かかる現状にかんがみ、ホットトップ開始
までは高電流溶解を行ない、ホットトップ開始後は溶湯
プールを徐々に浅<シ、適正な給湯を行ないながら均一
凝固に近い状態にして、均質性、表面品質のすぐれた鋳
塊を得るための高融点活性金属及びその合金の真空アー
ク溶解方法を提案するものである。In view of the current situation, this invention performs high current melting until the hot top starts, and after the hot top starts, the molten metal pool is gradually shallowed and the molten metal is appropriately supplied to a state close to uniform solidification, thereby achieving homogeneity. This paper proposes a vacuum arc melting method for high melting point active metals and their alloys to obtain ingots with excellent surface quality.
問題点を解決するための手段
この発明は、高融点活性金属及びその合金の消耗電極式
真空アーク溶解方法において、溶解後期のホラ))ツブ
に際し、溶解電流を数段階で減少し、それぞれの段階に
一定時間保持して、溶湯プール深さを徐々に小さくし、
均一凝固に近い状態で凝固せしめることを要旨とする。Means for Solving the Problems This invention provides a consumable electrode type vacuum arc melting method for high melting point active metals and their alloys, in which the melting current is reduced in several stages during the final stage of melting. The depth of the molten metal pool is gradually reduced by holding it for a certain period of time.
The gist is to solidify in a state close to uniform solidification.
作 用
次に、この発明の詳細を第1図に基いて説明する。この
発明の実施による方法をCに示し、比較のため、定常溶
解の後に短時間T^のホットトップを行なう従来法Aと
、最初から溶解電流を一定の嫉速係数で徐々に低減する
減速溶解法Bを掲げた。Operation Next, the details of this invention will be explained based on FIG. 1. A method according to the present invention is shown in C. For comparison, conventional method A involves hot top for a short period of time T^ after steady melting, and deceleration melting in which the melting current is gradually reduced with a constant speed coefficient from the beginning. Law B was proposed.
この発明の方法は、定常状態では電極、鋳型寸法で決定
される定常電流I。で溶解し、ホットトップ開始時期に
なると、電流を■、まで低下させ、この電流で時間T1
だけ溶解する。さらに、電流■2まで低下して時間T、
の溶解を行なって電源を切るか、又はさらにI3の電流
に低減し、時間T3だけ溶解し電源を切る。In the method of the present invention, in a steady state, a steady current I is determined by the electrode and mold dimensions. When it is time to start the hot top, the current is reduced to ■, and at this current the time T1
only dissolves. Furthermore, the current decreases to ■2 for a time T,
Either the current is melted and the power is turned off, or the current is further reduced to I3, the current is melted for a time T3, and the power is turned off.
上記のごとく、この発明は溶湯プールを徐々に浅くし、
かつ適正な給湯を行ないつつ、鋳塊の表面品質を確保す
るため、ホットトップを数段階(図面には2段階及び3
段階を示した)にわたって行なう溶解電流パターンを採
用するものである。As mentioned above, this invention gradually makes the molten metal pool shallower,
In order to ensure the surface quality of the ingot while supplying appropriate hot water, the hot top is installed in several stages (the drawing shows two stages and three stages).
This method employs a dissolution current pattern that occurs over a period of time (as shown in the figure).
この際のホットトップの電流!7、I2、I3 は電
極、鋳型寸法、及び材質すなわち添加元素のレベルによ
って決定される。発明者らは成分偏析、表面品質、生産
性等から種々実験した結果、I、=0.60〜0.80
I。The current of the hot top at this time! 7, I2, and I3 are determined by the electrode, mold dimensions, and material, i.e., the level of added elements. The inventors conducted various experiments on component segregation, surface quality, productivity, etc., and found that I, = 0.60 to 0.80.
I.
y、−0,40〜0.60I。y, −0.40 to 0.60I.
l3=0.15〜0,40I0
が望ましいことを知った。又、時間は溶解状況により変
るが、実験の結果では、
2段階の場合
T、=20〜40分
子、220分(調整分を含む)
3段階の場合
T、=20〜40分
子2=20〜40分
子、510分(調整分を含む)
が望ましい。I learned that l3=0.15 to 0.40I0 is desirable. Also, the time varies depending on the dissolution situation, but according to the experimental results, in the case of 2 steps, T = 20 to 40 molecules, 220 minutes (including adjustment), and in the case of 3 steps, T = 20 to 40 molecules, 2 = 20 ~ 40 molecules, 510 minutes (including adjustment) is desirable.
この発明におけるホラ)l−ツブの実施は、電流を低下
する際に、溶湯プールの深さ、保有熱、及び溶解状況を
考慮して定めたものであり、電源を切った際の溶湯プー
ル深さを極力浅(すること、電流を低下させる過程で溶
湯を適正に給湯させることなどにより、均一凝固に近い
状態を現出させるものである。In this invention, the implementation of the molten metal tube is determined by taking into consideration the depth of the molten metal pool, retained heat, and melting situation when reducing the current, and the depth of the molten metal pool when the power is turned off is By keeping the molten metal as shallow as possible and by properly feeding the molten metal during the process of lowering the current, a state close to uniform solidification is achieved.
更に、ホットトップ開始するまでの経過は、溶湯プール
が深くても適正な給湯が行なわれておれば成分偏析、収
縮孔の生成はないと考えてよいので、高電流溶解をして
表面品質、生産性の向上を図るべきである。Furthermore, even if the molten metal pool is deep, as long as the molten metal is supplied properly, there will be no segregation of components or formation of shrinkage pores. We should aim to improve productivity.
実 施 例
実施例1
油圧プレスにより成型されたコンパクトを用いて、プラ
ズマビーム溶接により、直径788 mlA、長さ63
00羽、電縫7200 kgの一次電極を作製し、これ
を消耗電極式真空アーク溶解炉を使って二重溶解し、直
径980all、長さ2100 u71、重量7150
kpの純千タン鋳塊を製造した。Examples Example 1 Using a compact molded by a hydraulic press, a diameter of 788 mlA and a length of 63 mm was made by plasma beam welding.
A primary electrode of 00 wires and 7200 kg of electric resistance welding was made, and this was double melted using a consumable electrode type vacuum arc melting furnace, and a diameter of 980all, a length of 2100 u71, and a weight of 7150 was made.
KP pure 1,000 tan ingot was produced.
この際、−次溶解はすべて同一条件で行ない、二次溶解
のホットトップ条件を第1図に示すように変化させて製
造した。すなわち、Aはホットトップ時間の短い従来法
、Bは溶解初期より終了まで一定減速係数で溶解電流を
低減させる城速溶解法、Cはこの発明の実施例である。At this time, the secondary melting was all carried out under the same conditions, and the hot top conditions for the secondary melting were varied as shown in FIG. That is, A is a conventional method with a short hot top time, B is a fast melting method in which the melting current is reduced by a constant deceleration coefficient from the beginning of melting to the end, and C is an embodiment of the present invention.
なお、この際、従来法Aのホットトップ時間(TA)は
30分、発明法Cのホットトップ時間(Tc)は100
分とした。In this case, the hot top time (TA) of conventional method A is 30 minutes, and the hot top time (Tc) of inventive method C is 100 minutes.
It was a minute.
又、同時に各鋳塊を二つに縦断し、偏析の著しいFe、
Oについ−C成分分布を1.1整すると共に、生産性、
表面品質の観察を行なった。その結果を第1表に示す。At the same time, each ingot was longitudinally cut into two, and Fe, which had significant segregation, was cut into two.
In addition to adjusting the -C component distribution for O to 1.1, productivity,
Observations of surface quality were made. The results are shown in Table 1.
(以F余白)
1’JQ−
1″ ″′1
又、上記結果に基いて、目標値からの最大変動1a(a
図)、鋳塊表面品質指数(b図)、生産能率CC図)を
第2図に示す。(Hereinafter F margin) 1'JQ- 1'''''1 Also, based on the above results, the maximum variation from the target value 1a (a
Fig. 2 shows the ingot surface quality index (Fig. b), and production efficiency (CC Fig.).
上記結果より、この発明法Cはホットトップ時間の短い
従来法Aに比べ、成分偏析は著しく改善されており、又
長時間ホットトップを行なった誠速溶解法Bと同等の均
質性が得られると共に、生産性、表面品質の優れた鋳塊
が得られることがわかる。なお、第4図のマクロ写真は
、上記各方法A、B、CによりdA造された純チタン鋳
塊トップ部の組織を示したものであるが、この写真によ
っても、この発明法Cによるものは、他のA、Hのもの
に比べ均質であることがわかる。From the above results, this invention method C has significantly improved component segregation compared to the conventional method A, which uses a short hot top time, and can obtain the same homogeneity as the straight melting method B, which uses a long hot top time. It can be seen that an ingot with excellent productivity and surface quality can be obtained. The macro photograph in Fig. 4 shows the structure of the top part of pure titanium ingots produced by each method A, B, and C described above. It can be seen that this is more homogeneous than the other A and H.
実施例2
油圧プレスにより成型されたコンパクトを用いてプラズ
マビーム溶接により直径560mm、長さ625011
M、重量4860吟の一次′市極を作製し、これを消耗
電極式真空アーク溶解炉を使って二重溶解し、直径73
5朋、長さ2570朋、重量48301c7のTi−6
AI?−4V合金ヲ製造シタ。Example 2 Using a compact molded by a hydraulic press, a diameter of 560 mm and a length of 625011 was made by plasma beam welding.
M, the weight of 4860 gin was produced, and this was double melted using a consumable electrode type vacuum arc melting furnace, and the diameter was 73.
Ti-6 of 5 mm, length 2570 mm, weight 48301 c7
AI? -4V alloy manufacturing site.
この際、−次溶解はすべて同一条件で行ない、二次溶解
のホットトップ条件を第1図に示すように変化させて、
従来法人のホットトップ時間は43分、発明法Cは10
3分とした。又、同時に各鋳塊を二つに縦断し、偏析に
問題のあるA4、V、Fe。At this time, all secondary melting was performed under the same conditions, and the hot top conditions for secondary melting were changed as shown in Figure 1.
Conventional corporate hot top time is 43 minutes, invention method C is 10 minutes
It was set to 3 minutes. At the same time, each ingot is longitudinally cut into two, and A4, V, and Fe, which have segregation problems.
Oについて成分分布を稠査すると共に、表面品質の観察
を行なった。その結果を第2表に示す。The component distribution of O was investigated, and the surface quality was also observed. The results are shown in Table 2.
(以下余白)
又、上記結果に基いて、目標値からの最大変動量(a図
)、鋳塊表面品質指数(b図)、生産能率(0図)を第
3図に示す。(See the margins below) Also, based on the above results, the maximum variation from the target value (Figure a), the ingot surface quality index (Figure B), and the production efficiency (Figure 0) are shown in Figure 3.
」ユ記結果より、この発明法Cは成分調整を行なってい
ない従来法Aに比べ、成分偏析は著しく改善されており
、又長時間ホットトップを行なった減速溶解法Bと同等
の均質性が得られると共に、生産性、表面品質の優れた
鋳塊が得られることがわかる。The results show that the invented method C has significantly improved component segregation compared to the conventional method A, which does not adjust the components, and has the same homogeneity as the slow dissolution method B, which uses a hot top for a long time. It can be seen that an ingot with excellent productivity and surface quality can be obtained.
発 明 の 効 果
この発明は、高融点活性金属及びその合金を真空アーク
溶解する際、最終溶解における溶解後期のホットトップ
において、溶解電流を数段階で減少して、均一凝固に近
い状態で凝固せしめるため、均質性、表面品質、生産性
の優れた鋳塊を得ることができる。Effects of the Invention This invention, when performing vacuum arc melting of high-melting point active metals and their alloys, reduces the melting current in several stages at the hot top in the latter half of final melting to solidify in a state close to uniform solidification. As a result, an ingot with excellent homogeneity, surface quality, and productivity can be obtained.
第1図は消耗電極式真空アーク溶解における二次溶解電
流パターンを示す線図、第2図は実施例1において、第
3図は実施例2において、それぞれ鋳塊の均質性、表面
品質、生産性に及ぼす溶解パターンの影響を示す図表、
第4図は実施例1による純ナタン鋳塊トップ部のマクロ
組織を示す写真である。
A・・・従来法、B・・・ン威速溶解法、C・・・発明
法、Io・・・定常溶解電流、11・・・第1段階ホッ
トトップ電流、T2・・・第2段階ホットトップ電流、
T3・・・第3段階ホットトップ′「f流、T1・・・
第1段階ホットトップ時間、T2・・・第2段階ホット
トップ時間、T3・・・第3段階ホットトップ時間、T
A・・・ Aパターンでの全ホットトップ時間、TB・
・・Bパターンでの全ホットトップ時間、Tc・・・C
パターンでの全ホットトップ時間。Figure 1 is a diagram showing the secondary melting current pattern in consumable electrode type vacuum arc melting, Figure 2 is a diagram showing the ingot homogeneity, surface quality, and production in Example 1, and Figure 3 is in Example 2. Diagram showing the effect of dissolution pattern on
FIG. 4 is a photograph showing the macrostructure of the top part of the pure natan ingot according to Example 1. A: Conventional method, B: Rapid melting method, C: Invention method, Io: Steady melting current, 11: 1st stage hot top current, T2: 2nd stage hot top current,
T3... 3rd stage hot top 'F style, T1...
1st stage hot top time, T2... 2nd stage hot top time, T3... 3rd stage hot top time, T
A... Total hot top time in A pattern, TB.
...Total hot top time in pattern B, Tc...C
All hot top time in the pattern.
Claims (1)
解方法において、溶解後期のホットトップに際し、溶解
電流を数段階で減少させ、それぞれの段階に一定時間保
持して、溶湯プール深さを徐々に小さくし、均一凝固に
近い状態で凝固せしめることを特徴とする高融点活性金
属及びその合金の真空アーク溶解方法。In the consumable electrode vacuum arc melting method for high melting point active metals and their alloys, during the hot top in the late melting stage, the melting current is reduced in several stages and held at each stage for a certain period of time to gradually increase the depth of the molten metal pool. A vacuum arc melting method for high melting point active metals and their alloys, which is characterized by reducing the size and solidifying in a state close to uniform solidification.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19005684A JPS6167725A (en) | 1984-09-10 | 1984-09-10 | Method for vacuum arc-melting active metal having high melting point and alloy thereof |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19005684A JPS6167725A (en) | 1984-09-10 | 1984-09-10 | Method for vacuum arc-melting active metal having high melting point and alloy thereof |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6167725A true JPS6167725A (en) | 1986-04-07 |
JPH0429723B2 JPH0429723B2 (en) | 1992-05-19 |
Family
ID=16251605
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19005684A Granted JPS6167725A (en) | 1984-09-10 | 1984-09-10 | Method for vacuum arc-melting active metal having high melting point and alloy thereof |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6167725A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2016185562A (en) * | 2015-03-27 | 2016-10-27 | 株式会社神戸製鋼所 | Method and apparatus for manufacturing ingot comprising alloy of high melting point active metal |
JP2022076856A (en) * | 2020-11-10 | 2022-05-20 | 株式会社神戸製鋼所 | Ingot of pure titanium or titanium alloy |
-
1984
- 1984-09-10 JP JP19005684A patent/JPS6167725A/en active Granted
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2016185562A (en) * | 2015-03-27 | 2016-10-27 | 株式会社神戸製鋼所 | Method and apparatus for manufacturing ingot comprising alloy of high melting point active metal |
JP2022076856A (en) * | 2020-11-10 | 2022-05-20 | 株式会社神戸製鋼所 | Ingot of pure titanium or titanium alloy |
Also Published As
Publication number | Publication date |
---|---|
JPH0429723B2 (en) | 1992-05-19 |
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