Pure vanadium and titanium for low activation alloys

The refining processes of vanadium and titanium from metal and gas impurities by physical methods in vacuum are considered. The effectiveness of using electron-beam melting, zone recrystallization and electrotransport for purification of these metals is shown. Vanadium and titanium in a purity of...

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Datum:2016
Hauptverfasser: Pylypenko, M.M., Lavrinenko, S.D.
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Veröffentlicht: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2016
Schriftenreihe:Вопросы атомной науки и техники
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spelling nasplib_isofts_kiev_ua-123456789-1154042025-02-09T17:46:34Z Pure vanadium and titanium for low activation alloys Чистые ванадий и титан для малоактивируемых сплавов Чисті ванадій і титан для малоактивованих сплавів Pylypenko, M.M. Lavrinenko, S.D. Материалы реакторов на тепловых и быстрых нейтронах The refining processes of vanadium and titanium from metal and gas impurities by physical methods in vacuum are considered. The effectiveness of using electron-beam melting, zone recrystallization and electrotransport for purification of these metals is shown. Vanadium and titanium in a purity of more than 99.99% have been produced. Рассмотрены процессы рафинирования ванадия и титана от металлических и газовых примесей физическими методами в вакууме. Показана эффективность использования электронно-лучевой плавки, зонной рекристаллизации и электропереноса для очистки этих металлов. Получены образцы титана и ванадия чистотой более 99,99 мас.%. Розглянуто процеси рафінування ванадію і титану від металевих і газових домішок фізичними методами у вакуумі. Показана ефективність використання електронно-променевої плавки, зонної рекристалізації і електропереносу для очищення цих металів. Отримано зразки титану і ванадію чистотою понад 99,99 мас.%. 2016 Article Pure vanadium and titanium for low activation alloys / M.M. Pylypenko, S.D. Lavrinenko // Вопросы атомной науки и техники. — 2016. — № 4. — С. 49-53. — Бібліогр.: 11 назв. — англ. 1562-6016 https://nasplib.isofts.kiev.ua/handle/123456789/115404 669.054; 669.292; 669.295 en Вопросы атомной науки и техники application/pdf Національний науковий центр «Харківський фізико-технічний інститут» НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Материалы реакторов на тепловых и быстрых нейтронах
Материалы реакторов на тепловых и быстрых нейтронах
spellingShingle Материалы реакторов на тепловых и быстрых нейтронах
Материалы реакторов на тепловых и быстрых нейтронах
Pylypenko, M.M.
Lavrinenko, S.D.
Pure vanadium and titanium for low activation alloys
Вопросы атомной науки и техники
description The refining processes of vanadium and titanium from metal and gas impurities by physical methods in vacuum are considered. The effectiveness of using electron-beam melting, zone recrystallization and electrotransport for purification of these metals is shown. Vanadium and titanium in a purity of more than 99.99% have been produced.
format Article
author Pylypenko, M.M.
Lavrinenko, S.D.
author_facet Pylypenko, M.M.
Lavrinenko, S.D.
author_sort Pylypenko, M.M.
title Pure vanadium and titanium for low activation alloys
title_short Pure vanadium and titanium for low activation alloys
title_full Pure vanadium and titanium for low activation alloys
title_fullStr Pure vanadium and titanium for low activation alloys
title_full_unstemmed Pure vanadium and titanium for low activation alloys
title_sort pure vanadium and titanium for low activation alloys
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
publishDate 2016
topic_facet Материалы реакторов на тепловых и быстрых нейтронах
url https://nasplib.isofts.kiev.ua/handle/123456789/115404
citation_txt Pure vanadium and titanium for low activation alloys / M.M. Pylypenko, S.D. Lavrinenko // Вопросы атомной науки и техники. — 2016. — № 4. — С. 49-53. — Бібліогр.: 11 назв. — англ.
series Вопросы атомной науки и техники
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fulltext ISSN 1562-6016. ВАНТ. 2016. №4(104) 49 UDC 669.054; 669.292; 669.295 PURE VANADIUM AND TITANIUM FOR LOW ACTIVATION ALLOYS M.M. Pylypenko 1 , S.D. Lavrinenko 1,2 1 National Science Center “Kharkov Institute of Physics and Technology”, Kharkov, Ukraine E-mail: mpylypenko@kipt.kharkov.ua; 2 V.N. Karazin Kharkov National University, Kharkov, Ukraine The refining processes of vanadium and titanium from metal and gas impurities by physical methods in vacuum are considered. The effectiveness of using electron-beam melting, zone recrystallization and electrotransport for purification of these metals is shown. Vanadium and titanium in a purity of more than 99.99% have been produced. INTRODUCTION Modern tendencies of development of reactor technologies are aimed to further increase reliable and safe operation of power units and to provide efficiency and competitiveness of nuclear power. This requires an increase in power density, power of units, increasing the duration of campaigns, more efficient fuel burning, including by improving the quality of construction materials [1-4]. The progress achieved in the field of nuclear physics, reactor physics and reactor materials in recent years, led to the development of a number of advanced nuclear energy systems [1]. These projects have advantages in economy, security, reliability and non- proliferation of nuclear materials. New structural materials must be pure. We know that high levels of impurities and gases in steels and alloys significantly worsen their mechanical, corrosion and radiation properties and, therefore, limit their use in operating and designing reactors. Use of high-purity metals as initial components of new structural materials will provide desired properties in the resulting products [5, 6]. Vanadium, titanium and chromium are metallic elements which are necessary components to produce low-activity alloys for nuclear energy of present and future. Vanadium alloys are considered as a promising candidate structural material for fusion and fast-fission reactors applications because of their attractive properties such as superior high temperature thermal and physical properties, good resistance against neutron irradiation and low neutron activation level. It is well known that increased level of interstitial impurities such as C, N, O would result in loss of workability, weldability and irradiation resistance [78]. On the other hand, increased level of undesirable elements such as Co, Nb, Ag, Mo, Al, Na, Ni, Cu, Fe etc. would dominate the activation level of vanadium alloys which would substantially influence not only the recycling aspects of used reactor materials but also the waste management aspects of them. The required impurity levels for hands-on recycling of the low-activity vanadium alloys are around the magnitude concentrations of 0.01, 0.1, 0.01, 10, 0.5 and 30 wppm, respectively, for the elements Co, Nb, Ag, Mo, Cu, Ni and Al based on the neutron irradiation fluence of 15 (MW∙year)/m 2 [7]. Impurities increase the strength of titanium, also greatly reduces it ductility, but interstitial impurities such as H, O, N, and C have the strongest negative action on properties of titanium. Titanium entirely loses its ability to plastic deformation and becomes brittle if it contains 0.003, 0.02, and 0.7 wt.% hydrogen, nitrogen and oxygen, respectively. Under neutron irradiation the embrittlement of titanium alloys increases with increasing contents of oxygen, nitrogen and hydrogen in the alloy. The activation level of vanadium alloys will be depending on impurity contents in alloys. So obtaining of high-purity components (vanadium and titanium) for low-activity alloys is relevant today. 1. METHODS AND TECHNOLOGIES FOR REFINING OF METALS To obtain pure metals at different stages of refining, the various chemical and physico-chemical methods are used, but usually the refining process comprises of physical methods – distillation, zone recrystallization, electrotransport and various combinations thereof. These methods are mainly physical processes: evaporation and condensation, crystallization, diffusion and electromigration, etc. The advantages of these methods over the others are the ability to yield high purity material, and the final product is obtained in a compact form including single crystals with a perfect crystal structure. Electron beam melting (EBM) of metals is performed on an ultra-high vacuum installation. To pump installation, the two hetero-ion pumps were used with a pumping speed of 5000 l/s each, and the titanium sublimation pump was applied also. Application of such a system of vacuum pumping allows to get an ultimate vacuum in the installation 1.7∙10 -6 Pa [9]. In the spectrum of the residual gas in installation were absent heavy hydrocarbons. Refining of metals was carried out in vacuum (1…5)·10 -5 Pa. Refining was conducted in the regime: heating ⇒ melting ⇒ excerpt of metal in molten state ⇒ crystallization ⇒ pulling ingot. Zone recrystallization with an electron-beam heating is carried out, as a rule, in installations with combined pumping systems [9]. Diffusion pumps are equipped with sorption and condensation traps; sorption, cryogenic and ion-sorption pumps are used to give “oil- free” ultrahigh vacuum. Electron-beam zone recrystallization was carried out in vacuum mailto:mpylypenko@kipt.kharkov.ua 50 ISSN 1562-6016. ВАНТ. 2016. №4(104) 1·10 -6 …1·10 -5 Pa. Choice of pumping system for different methods of refining was determined mainly by degree of interaction of metals with residual gases of the vacuum environment under refining conditions. 2. RESULTS AND DISCUSSION Results of physical methods of refining of vanadium and titanium which are important components for the production of low-activity alloys for nuclear power are given below. The metals differing by initial degree of purity and method of preparation were used to research the purification processes. 2.1. Vanadium The initial materials used for research: rods of technical vanadium, electrolytic vanadium VEL-1 and vanadium, which was received by iodide refining (IV). Studies have shown that carrying out EBM of electrolytic vanadium reduces the metallic impurities, for example, chromium concentration was reduced by two orders of magnitude, as well as potassium concentration was reduced by about 75 times; but no reduction of silicon concentration. Carrying out electron beam melting of vanadium in vacuum 5·10 -4 Pa allowed to increase the purity of metal up to 99.95 wt.%. The impurity concentrations of that vanadium are given in Table 1. Carrying out zone melting can effectively remove impurities of aluminum, iron, nickel, copper and chromium. Silicon is slightly removed while impurities of refractory metals (tungsten, molybdenum, tantalum and niobium) accumulated during long recrystallization of vanadium [10]. Table 2 compares the effectiveness of purification of technical vanadium rods by EBM methods and zone melting (ZM). ZM of vanadium is carried out at a speed of 4 cm/hour. The data in Table 2 show that ZM is more effective method for purification of vanadium samples than EBM. Silicon content in a technical metal is high, and it is the limiting impurity for ZM process. Table 1 The impurity contents of vanadium, ppm Metal Al Fe Si Cu Cr Na K Mn Ni Cl P O Initial 120 70 17 100 850 3 130 1.5 8 42 70 590…800 After EBM 11 10 17 18 7 0.4 1.7 0.11 5 4 0.5 160…200 Table 2 The content of impurities in the technical vanadium after EBM and ZM Type of metal Content of impurities, ppm Fe Cr Cu Mo Si Mg Al Initial 1000 30 5 60 1500 16 200 After EBM in vacuum 5·10 -4 Pа 200 < 30 2.4 40 1500 5 20 After ZM in vacuum 2·10 -5 Pа 17 < 30 < 1.4 20 1300 < 0.5 < 10 For the study of ZM process IV was also used. The content of impurities in the IV after one pass of ZM is given in Table 3. The distribution of the relative residual resistivity (RRR = R (300 K)/R (4.2 K)) and microhardness of vanadium along the sample are shown in Fig. 1. High efficiency of this method with respect to reduce concentration of gas-forming impurities was proved by study of thermal desorption of the initial samples and after refining. The dependence of total pressure on heating of vanadium samples in the temperature range 25…800 °C is given in Fig. 2. The degassing intensity for the sample after refining is five times less than for initial metal. The mass-spectra of gases released from vanadium sample during the thermal desorption are correspond to H2O, CO, N2, CO2 etc. The highest intensity of degassing took place in the temperature range 300…600 °C, peaking at about 500 °C [11]. Fig. 1. Distribution of RRR (1) and microhardness (2) along the length of the sample of IV after one pass of molteng zone ISSN 1562-6016. ВАНТ. 2016. №4(104) 51 Table 3 The content of impurities in the IV after ZM Type of metal Content of impurities, ppm Fe Cu Mo Mn Si Mg Al Initial 920 9 13 6 40 1.5 80 After ZM initial end of sample 150 4.8 16 1 40 <1 <10 last end of sample 600 11 12 2 37 <1 <10 Fig. 2. The dependence of total pressure of vapors on heating of vanadium before (1) and after refining (2) in temperature range 25…800 °C The results of metallographic measurements of vanadium samples before and after EBM under vacuum are given in Fig. 3. The initial samples of compacted powders were in tablets form. Refined sample has a relatively large grain with size of about 380 m, which can be observed visually (see Fig. 3,b). The grains are equiaxial, the grain boundaries are clean. The microhardness of the initial vanadium is Hμ = 1090 MPa, after electron-beam melting Hμ = 1440 MPa. Increasing the microhardness of vanadium after EBM can be explained by the fact that the initial samples of compacted powders were produced from flakes of electrolytic vanadium. Consequently, these samples have a higher porosity and, correspondingly, less microhardness value. a b Fig. 3. Obtained samples of vanadium (a) and their microstructure (b) The most pure vanadium was obtained using method of electrotransport or electromigration on wire samples produced from metal after double EBM of electrolytic powder vanadium. Solid state electrotransport is another technique useful particularly in the removal of interstitial impurities such as H, O, N, and C from refractory metals and has met with unprecedented success. Studies have shown that interstitial impurities are migrated to the cathode side of the vanadium sample when passing a constant electric current of high density, 52 ISSN 1562-6016. ВАНТ. 2016. №4(104) i.e. effective charge of these impurities is positive. From the numerical solution of the equation for electrotransport follows that at 1650 °C for 200 hours at a current density of approximately 5·10 3 А/cm 2 the electrotransport will result in a significant reduction of oxygen, nitrogen and carbon. It is experimentally shown that under the above conditions the RRR of vanadium samples after purification by electrotransport increases from 50 up to 1600. The chemical composition of high- purity vanadium with RRR = 1200 and purity more than 99.99% wt.%, which was obtained by electrotransport, is as follows (mass spectral method, at.%): Na < 1.0·10 -5 ; K – 1.0·10 -5 ; Ca – 4.0·10 -5 ; Cu – 5.0·10 -5 ; Mg < 1.0·10 -5 ; Zn < 9.0·10 -5 ; Al – 9.0·10 -5 ; Si – 2.0·10 -3 ; Ti – 4.0·10 -5 ; P – 1.0·10 -4 ; As – 3.0·10 -5 ; S < 4.0·10 -5 ; Mn < 1.0·10 -5 ; Fe – 2.0·10 -5 ; Cl – 7.0·10 -5 ; Nb – 4.0·10 -5 ; Cr – 1.0·10 -3 ; F – 1.0·10 -3 ; Ni – 3.0·10 -5 ; Ga – 3.0·10 -5 ; Zr – < 5.0·10 -5 ; Mo – 2.0·10 -5 ; C < 1.0·10 -2 ; N2 < 1.0·10 -2 ; O2 < 9.0·10 -3 . Analysis results indicates that for a higher degree of purification of vanadium it is necessary to use combination of different refining methods which would allow remove impurities such as silicon, refractory metals, carbon, nitrogen, oxygen from vanadium. Vacuum distillation of vanadium, which can reduce silicon content in the metal more than ten times as well as impurities of refractory metals, is worth exploring. 2.2. Titanium Titanium sponge TG-90 and titanium produced by iodide refining (ITi) were used as starting materials for purification by electron-beam melting. EBM of titanium sponge was carried out in two stages. In the first step the pieces of titanium sponge were heated to a high temperature and melted. Gaseous impurities intensively removed from the metal during heating and melting. During a second stage the obtained ingots were melted by drip melt method. Titanium ingots with diameter of 150 mm and 99.99 wt.% purity were produced by EBM method. The content of impurities in titanium after EBM is given in Table 4. Analysis of the results of experimental melting of titanium sponge TG-90 showed that the hydrogen content of titanium after EBM decreased by 4.5 times compared to the initial concentration and the concentration of O and N was significantly decreased. The impurity content in the produced titanium ingots decreased much more than required by the standards for titanium. Table 4 The content of impurities in titanium, ppm Type of metal Al V Fe Si Ni O N H Initial sponge TG-90 100 3 500 100 400 400 200 72 After EBM 7 1.5 400 5 50 70 15 16 More pure titanium was obtained after EBM of the initial iodide titanium. Impurity contents in the ITi after two electron-beam remelting are as follows: Al – 8.0·10 -1 ; P – 1.0; S – 8.0; K – 6.0·10 -1 ; Ca – 2.0; V – 3.0; Cr – 3.0; Mn < 9.0·10 -1 ; Fe – 15; Ni – 50; Cu – 3.0; Zn – 2.0; As – 8.0; Sn < 8.0 ppm. It should be noted that EBМ of titanium favorably affects to the vacuum conditions of the installation due to the good getter abilities of titanium layers deposited on the chamber walls owing to evaporation at EBM [2]. CONCLUSIONS Regularities refining of vanadium and titanium were investigated; it has allowed reaching a higher level of purity metals by applying methods of electron-beam melting, zone recrystallization and electrotransport in vacuum. These methods had demonstrated high efficiency of purification of vanadium and titanium from interstitial impurities and majority of metallic impurities. Vanadium and titanium in a purity of more than 99.99 % have been produced. Suggested methods for obtaining high-purity metals have created the necessary prerequisites for their use in improving existing and producing new structural materials. REFERENCES 1. A technology roadmap for generation IV nuclear energy systems, issued by U.S. DOE nuclear energy research advisory committee and the Generation IV international forum (GIF - 002-00). Washington, 2002, 91 р. 2. S.D. Lavrynenko, M.M. Pylypenko. Pure Metals for Nuclear Power // SMC Bulletin. 2015, v. 6, N 1, p. 19-24. 3. V.N. Voyevodin. Actual problems of scientific and technical support of safe operation and development of the nuclear power complex of Ukraine // Herald of the National Academy of Sciences of Ukraine. 2014, N 8, c. 25-32. 4. V.N. Voyevodin, I.M. Neklyudov. Evolution of the Structure Phase State and Radiation Resistance of Structural Materials. Kiev: “Naukova dumka”, 2006, 375 p. 5. V.M. Azhazha, S.D. Lavrynenko, M.M. Pyly- penko. Pure and super pure metals in atomic energy // PAST. Series “Vacuum, Pure Materials, Superconductors”. 2007, N 4, p. 3-12. 6. M.M. Pylypenko. The role of high-purity metals in the creation of new materials for structural elements NPP // PAST. Series “Vacuum, Pure Materials, Superconductors”. 2008, N 1, p. 10-17. 7. Y. Wu, T. Muroga, Q. Huang, et al. Effect of impurities on low activation characteristic of V-4Cr-4Ti alloy // J. Nucl. Mater. 2002, v. 307-311, p. 1026-1030. 8. I.M. Neklyudov, V.M. Azhazha, G.P. Kovtun, M.M. Pylypenko. Impact on the quality of purity materials for nuclear and thermonuclear energy // Proceedings of the IV International Conference “Quality Strategy in Industry and Education” (May ISSN 1562-6016. ВАНТ. 2016. №4(104) 53 30  June 6, 2008, Varna, Bulgaria). Dnepropetrovsk, Varna, 2008, v. 1, p. 416-420. 9. G.F. Tihinsky, G.P. Kovtun, V.M. Azhazha. Obtaining of ultrapure rare metals. M.: “Metallurgy”, 1986, 160 p. 10. V.M. Azhazha, P.N. Vyugov, S.D. Lavrynenko, M.M. Pylypenko. Electron-beam zone melting of vanadium, niobium and tantalum // Special metallurgy: yesterday, today and tomorrow. Kiev: “Politekhnica”, 2002, p. 220-225. 11. Y.P. Bobrov, A.E. Dmitrenko, D.V. Koblik, et al. Electron-beam melting of vanadium // PAST. Series “Vacuum, Pure Materials, Superconductors”. 2014, N 1, p. 27-31. Статья поступила в редакцию 01.06.2016 г. ЧИСТЫЕ ВАНАДИЙ И ТИТАН ДЛЯ МАЛОАКТИВИРУЕМЫХ СПЛАВОВ Н.Н. Пилипенко, С.Д. Лавриненко Рассмотрены процессы рафинирования ванадия и титана от металлических и газовых примесей физическими методами в вакууме. Показана эффективность использования электронно-лучевой плавки, зонной рекристаллизации и электропереноса для очистки этих металлов. Получены образцы титана и ванадия чистотой более 99,99 мас.%. ЧИСТІ ВАНАДІЙ І ТИТАН ДЛЯ МАЛОАКТИВОВАНИХ СПЛАВІВ М.М. Пилипенко, С.Д. Лавриненко Розглянуто процеси рафінування ванадію і титану від металевих і газових домішок фізичними методами у вакуумі. Показана ефективність використання електронно-променевої плавки, зонної рекристалізації і електропереносу для очищення цих металів. Отримано зразки титану і ванадію чистотою понад 99,99 мас.%.