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JPH0429723B2 - - Google Patents
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JPH0429723B2 - - Google Patents

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Publication number
JPH0429723B2
JPH0429723B2 JP59190056A JP19005684A JPH0429723B2 JP H0429723 B2 JPH0429723 B2 JP H0429723B2 JP 59190056 A JP59190056 A JP 59190056A JP 19005684 A JP19005684 A JP 19005684A JP H0429723 B2 JPH0429723 B2 JP H0429723B2
Authority
JP
Japan
Prior art keywords
melting
hot
time
current
molten metal
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
JP59190056A
Other languages
Japanese (ja)
Other versions
JPS6167725A (en
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
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Priority to JP19005684A priority Critical patent/JPS6167725A/en
Publication of JPS6167725A publication Critical patent/JPS6167725A/en
Publication of JPH0429723B2 publication Critical patent/JPH0429723B2/ja
Granted legal-status Critical Current

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  • Manufacture And Refinement Of Metals (AREA)

Description

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

産業上の利用分野 この発明は、Ti、Zr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。 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、いわゆるホツトトツプを行な
うものである。 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、ある一定時期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
に伴つ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。 しかしながら、溶解終了時に電源を切つた際の
溶湯プールが深ければ成分偏析、収縮孔は大きく
なる。そのため、溶解後期にはホツトトツプを実
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。 しかるに、現在一般に行なわれている溶解末期
に行なつているホツトトツプは、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
軽減されるに至つていない。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41−8321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。 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プール深さを徐々に
小さくして収縮孔の発生を防止するものである。 しかしながら、この場合にはホツトトツプ時間
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。 この発明は、かかる現状にかんがみ、ホツトト
ツプ開始までは高電流溶解を行ない、ホツトトツ
プ開始後は溶湯プールを徐々に浅くし、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。 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
のホツトトツプに際し、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。 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TAのホツトトツ
プを行なう従来法Aと、最初から溶解電流を一定
の減速係数で徐々に低減する減速溶解法Bを掲げ
た。 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IOで溶解し、ホツトトツ
プ開始時期になると、電流をI1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I2
で低下して時間T2の溶解を行なつて電源を切る
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。 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、ホツトトツプを数段階
(図面には2段階及び3段階を示した)にわたつ
て行なう溶解電流パターンを採用するものであ
る。 この際のホツトトツプの電流I1、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
よつて決定される。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、 I1=0.60〜0.80I0 I2=0.40〜0.60I0 I3=0.15〜0.40I0 が望ましいことを知つた。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 T1=20〜40分 T2≧20分(調整分を含む) 3段階の場合 T1=20〜40分 T2=20〜40分 T3≧10分(調整分を含む) が望ましい。 この発明におけるホツトトツプの実施は、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
切つた際の溶湯プール深さを極力浅くすること、
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。 更に、ホツトトツ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。 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788mm、長
さ6300mm、重量7200Kg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つて二重溶解
し、直径980mm、長さ2100mm、重量7150Kgの純チ
タン鋳塊を製造した。 この際、一次溶解はすべて同一条件で行ない、
二次溶解のホツトトツプ条件を第1図に示すよう
に変化させて製造した。すなわち、Aはホツトト
ツ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減速溶解
法、Cはこの発明の実施例である。なお、この
際、従来法Aのホツトトツプ時間(TA)は30分、
発明法Cのホツトトツプ時間(TC)は100分とし
た。又、同時に各鋳塊を二つに縦断し、偏析の著
しいFe、Oについて成分分布を調整すると共に、
生産性、表面品質の観察を行なつた。その結果を
第1表に示す。
INDUSTRIAL APPLICATION FIELD 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 Ti and Zr and their alloys. Conventional technology High melting point active metals are usually melted by vacuum arc melting, but this method involves constant melting with a constant electric current.
In the latter stage of melting, the melting current is reduced within a relatively short period of about 20 to 60 minutes, a so-called hot-top process. In the solidification of molten metal in consumable electrode vacuum arc melting, solidification from the bottom of the mold is predominant in the initial stage, but after a certain period of time, solidification from the mold wall becomes significantly large. At this time,
The depth of the molten metal pool is constant if the melting rate is constant, and 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, and solidification progresses from the bottom to the top. There is little component segregation and shrinkage pores. However, if the molten metal pool is deep when the power is turned off at the end of melting, component segregation and shrinkage pores will become larger. Therefore, hot-topping is carried out in the late stage of melting, but the homogeneity cannot be improved unless the current is properly controlled. However, the current hot-top process, 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, so component segregation and shrinkage pores are sufficiently reduced. It has not yet been achieved. Therefore, various methods have been devised in the past, and as a method for reducing the occurrence of shrinkage pores, for example, there is a method disclosed in Japanese Patent Publication No. 8321/1983 in which the melting current is gradually lowered by a constant deceleration coefficient from the initial stage of melting. 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 reducing the depth of the molten metal pool while preventing solidification from the upper surface of the molten metal pool. However, in this case, since the hot-top time is increased, the melting rate is reduced, productivity is deteriorated, and the surface quality of the ingot is also deteriorated. In view of the current situation, this invention performs high-current melting until the start of hot-topping, gradually makes the molten metal pool shallower after starting hot-topping, and maintains a state close to uniform solidification while supplying appropriate hot water, thereby improving homogeneity and surface quality. This paper proposes a vacuum arc melting method for high melting point active metals and their alloys to obtain excellent ingots. Means for Solving the Problems This invention is 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 at the hot top in the latter stage of melting, and each stage is maintained for a certain period of time. The gist is to hold the molten metal, gradually reduce the depth of the molten metal pool, and solidify in a state close to uniform solidification. 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, and for comparison, conventional method A involves hot-topping T A for a short time after steady melting, and decelerated melting method B, which gradually reduces the melting current with a constant deceleration coefficient from the beginning. was raised. In the method of the present invention, in a steady state, melting is performed with a steady current I O determined by the electrode and mold dimensions, and when the hot-top start time comes, the current is lowered to I 1 and melting is performed with this current for a time T 1 . Further, the current is reduced to I 2 and melted for a time T 2 and the power is turned off, or the current is further reduced to I 3 and melted for a time T 3 and the power is turned off. As mentioned above, this invention gradually makes the molten metal pool shallower, and in order to ensure the surface quality of the ingot while supplying the molten metal appropriately, the hot top is heated in several stages (stages 2 and 3 are shown in the drawing). This method employs a melting current pattern that is carried out over several periods. At this time, the hot-top currents I 1 , I 2 , and I 3 are
Determined by mold dimensions and material, i.e. level of added elements. As a result of various experiments from the viewpoint of component segregation, surface quality, productivity, etc., the inventors found that I 1 =0.60 to 0.80 I 0 I 2 = 0.40 to 0.60 I 0 I 3 = 0.15 to 0.40 I 0 are desirable. Also, the time varies depending on the dissolution situation, but according to the experimental results, in the case of 2 stages T 1 = 20 to 40 minutes T 2 ≧ 20 minutes (including adjustment) In the case of 3 stages T 1 = 20 to 40 minutes T 2 = 20 to 40 minutes T 3 ≧10 minutes (including adjustment) is desirable. The implementation of hot top in this invention is determined by taking into account 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 made as shallow as possible. to do,
By properly supplying molten metal during the process of lowering the current, a state close to uniform solidification is achieved. Furthermore, even if the molten metal pool is deep, as long as the molten metal is supplied properly, it can be assumed that there will be no segregation of components or formation of shrinkage pores. We should aim to improve the quality of life. Examples Example 1 Using a compact formed by a hydraulic press, a primary electrode of 788 mm in diameter, 6300 mm in length, and 7200 kg in weight was produced by plasma beam welding, and this was then melted into a secondary electrode using a consumable electrode type vacuum arc melting furnace. A pure titanium ingot with a diameter of 980 mm, a length of 2100 mm, and a weight of 7150 kg was produced by heavy melting. At this time, all primary melting was performed under the same conditions,
Production was carried out by changing the hot-top conditions for secondary melting as shown in FIG. That is, A is a conventional method with a short hot-top time, B is a deceleration melting method in which the melting current is reduced by a constant deceleration coefficient from the beginning to the end of melting, and C is an embodiment of the present invention. In this case, the hot-top time (T A ) of conventional method A is 30 minutes,
The hot-top time (T C ) of invention method C was 100 minutes. At the same time, each ingot was longitudinally cut into two, and the component distribution was adjusted for Fe and O, which were significantly segregated.
Productivity and surface quality were observed. The results are shown in Table 1.

【表】【table】

【表】 最大偏析値=最大分析値/目標値
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
(c図)を第2図に示す。 上記結果より、この発明法Cはホツトトツプ時
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、又長時間ホツトトツプを行なつた減
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。なお、第4図のマクロ写真は、上記各方法
A、B、Cにより製造された純チタン鋳塊トツプ
部の組織を示したものであるが、この写真によつ
ても、この発明法Cによるものは、他のA、Bの
ものに比べ均質であることがわかる。 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
6250mm、重量4860Kg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つて二重溶解
し、直径735mm、長さ2570mm、重量4830KgのTi−
6Al−4V合金を製造した。 この際、一次溶解はすべて同一条件で行ない、
二次溶解のホツトトツプ条件を第1図に示すよう
に変化させて、従来法Aのホツトトツプ時間は43
分、発明法Cは103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Al、V、Fe、
Oについて成分分布を調査すると共に、表面品質
の観察を行なつた。その結果を第2表に示す。
[Table] Maximum segregation value = Maximum analysis value / Target value Also, based on the above results, calculate the maximum variation from the target value (Figure a), the ingot surface quality index (Figure b), and the production efficiency (Figure c). Shown in Figure 2. From the above results, this invention method C has significantly improved component segregation compared to the conventional method A, which has a short hot-top time, and can obtain the same homogeneity as the decelerated melting method B, which has hot-topped for a long time. It can be seen that an ingot with excellent productivity and surface quality can be obtained. The macrophotograph in Figure 4 shows the structure of the top part of pure titanium ingots produced by each of the methods A, B, and C described above. It can be seen that the item is more homogeneous than the other items A and B. Example 2 Using a compact molded using a hydraulic press, a diameter of 560 mm and a length of 560 mm were obtained by plasma beam welding.
A primary electrode with a diameter of 6250 mm and a weight of 4860 Kg was prepared, and this was double melted using a consumable electrode type vacuum arc melting furnace.
A 6Al-4V alloy was produced. At this time, all primary melting was performed under the same conditions,
By changing the hot top conditions for secondary melting as shown in Figure 1, the hot top time for conventional method A was 43
minutes, and invention method C was set at 103 minutes. At the same time, each ingot was longitudinally cut into two to remove Al, V, Fe, which have problems with segregation.
The component distribution of O was investigated, and the surface quality was also observed. The results are shown in Table 2.

【表】【table】

【表】 ただし、目標値からの最大変動量及び最大偏析度は第
1表の注釈に同じ。
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
(C図)を第3図に示す。 上記結果より、この発明法Cは成分調整を行な
つていない従来法Aに比べ、成分偏析は著しく改
善されており、又長時間ホツトトツプを行なつた
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。 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
のホツトトツプにおいて、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。
[Table] However, the maximum variation from the target value and the maximum degree of segregation are the same as the notes in Table 1.
Furthermore, 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 C) are shown in Figure 3. From the above results, this invention method C has significantly improved component segregation compared to conventional method A in which component adjustment is not performed, and it also achieves homogeneity equivalent to slow dissolution method B, which uses hot top for a long time. At the same time,
It can be seen that an ingot with excellent productivity and surface quality can be obtained. Effects of the Invention This invention reduces the melting current in several stages at the hot top in the latter half of the final melting process when high melting point active metals and their alloys are melted in a vacuum arc, thereby solidifying the metal in a state close to uniform solidification. It is possible to obtain ingots with excellent homogeneity, surface quality, and productivity.

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

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
よる純チタン鋳塊トツプ部のマクロ組織を示す写
真である。 A…従来法、B…減速溶解法、C…発明法、I0
…定常溶解電流、I1…第1段階ホツトトツプ電
流、I2…第2段階ホツトトツプ電流、I3…第3段
階ホツトトツプ電流、T1…第1段階ホツトトツ
プ時間、T2…第2段階ホツトトツプ時間、T3
第3段階ホツトトツプ時間、TA…Aパターンで
の全ホツトトツプ時間、TB…Bパターンでの全
ホツトトツプ時間、TC…Cパターンでの全ホツ
トトツプ時間。
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. FIG. 4 is a photograph showing the macrostructure of the top part of the pure titanium ingot according to Example 1. A... Conventional method, B... Decelerated dissolution method, C... Invention method, I 0
...steady melting current, I 1 ... first stage hot top current, I 2 ... second stage hot top current, I 3 ... third stage hot top current, T 1 ... first stage hot top time, T 2 ... second stage hot top time, T3 ...
3rd stage hot top time, T A ... total hot top time in A pattern, T B ... total hot top time in B pattern, T C ... total hot top time in C pattern.

Claims (1)

【特許請求の範囲】[Claims] 1 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、溶解後期のホツトト
ツプに際し、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。
1. In the consumable electrode vacuum arc melting method for high melting point active metals and their alloys, the melting current is reduced in several stages at the hot top in the latter stage of melting, and each stage is held 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.
JP19005684A 1984-09-10 1984-09-10 Method for vacuum arc-melting active metal having high melting point and alloy thereof Granted JPS6167725A (en)

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 JPS6167725A (en) 1986-04-07
JPH0429723B2 true 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)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6396247B2 (en) * 2015-03-27 2018-09-26 株式会社神戸製鋼所 Ingot manufacturing method and manufacturing apparatus made of high melting point active metal alloy
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
JPS6167725A (en) 1986-04-07

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