Научная статья на тему 'Исследование неравновесных фаз, образующихся при сварке взрывом титана и алюминия'

Исследование неравновесных фаз, образующихся при сварке взрывом титана и алюминия Текст научной статьи по специальности «Технологии материалов»

CC BY
260
46
i Надоели баннеры? Вы всегда можете отключить рекламу.
Ключевые слова
СВАРКА ВЗРЫВОМ / МАССОПЕРЕНОС / МЕХАНОХИМИЯ / ИНТЕРМЕТАЛЛИДНЫЕ ФАЗЫ / КРИВИЗНА КРИСТАЛЛИЧЕСКОЙ РЕШЕТКИ / EXPLOSION WELDING / MASS TRANSFER / MECHANOCHEMISTRY / INTERMETALLIC PHASES / THE CURVATURE OF THE CRYSTAL LATTICE

Аннотация научной статьи по технологиям материалов, автор научной работы — Носков Ф.М., Квеглис Л.И., Мали В.И., Лесков М.Б., Захарова Е.В.

Представлено исследование физико-химических процессов, происходящих в зоне контакта титана и алюминия при совместной пластической деформации, вызванной сваркой взрывом. Один из наиболее эффективных путей решения задач материаловедения заключается в разработке композиционных материалов. Важным достоинством материалов, используемых в летательных аппаратах, является их малая плотность, обеспечивающая возможность получать в итоге композиты с высоким уровнем удельной прочности. Данное исследование способствует разработке композитных материалов на основе Ti-Al, которые могут быть использованы для изготовления лопаток газовых турбин, пустотелых и ребристых сварных конструкций для авиационной промышленности. Сварка взрывом представляет собой высокоэнергетический технологический процесс, позволяющий с высоким качеством соединять разнородные металлические материалы, в том числе различные комбинации материалов, используемых для композитов металл-интерметаллид. Система Ti-Al исследована достаточно широко, однако остается ряд неясных вопросов, а именно, какие интерметаллидные фазы могут образоваться при сварке взрывом. Условия образования ряда интерметаллидных фаз Ti-Al: Al5Ti2, Al11Ti5, Al2Ti, AlTi3, Al3Ti, среди которых в рамках одной формульной единицы могут быть реализованы различные типы структур (стабильные, метастабильные, виртуальные). В процессе механохимических реакций в зоне контакта титана и алюминия при сварке взрывом формируются неравновесные интерметаллические фазы: Al2Ti, Al5Ti3, Ti3,3Al. Для исследования структуры переходных зон полученных образцов использовали сканирующий электронный микроскоп JEOL 6390LV. Фазовый анализ проводили на рентгеновском дифрактометре фирмы Bruker в излучении меди. Показано, что массоперенос титана в алюминий происходит направленными потоками атомных кластеров со скоростью не менее 35 м/с. В зоне контакта Ti и Al формируются интерметаллические фазы в процессе механохимических реакций, протекающих на интерфейсе. Процессы структурообразования при сварке взрывом объясняются с позиций аномально быстрого направленного массопереноса в условиях напряжений, создающих кривизну кристаллической решетки.

i Надоели баннеры? Вы всегда можете отключить рекламу.
iНе можете найти то, что вам нужно? Попробуйте сервис подбора литературы.
i Надоели баннеры? Вы всегда можете отключить рекламу.

STUDIES OF NONEQUILIBRIUM PHASES FORMED AT EXPLOSION WELDING OF TITANIUM AND ALUMINUM

The work is devoted to the study of physical and chemical processes occurring in the contact zone of titanium and aluminum at the joint plastic deformation caused by explosion welding. One of the most effective ways to solve problems of materials science is the development of composite materials. An important advantage of the materials used in aircraft, is their low density, providing the possibility to receive the result composites with high specific strength. This study supports the development of composite materials based on Ti-Al, which can be used for the manufacture of gas turbine blades, and ribbed hollow weldments for the aircraft industry. Explosion welding is a high-energy process, allowing high quality joining dissimilar metal materials including various combinations of materials used for the composite metal-intermetallic compound. Ti-Al system was studied extensively enough, but there remain a number of unclear issues, namely which can form intermetallic phases with the explosion welding. conditions for the formation of a number of intermetallic phases Ti-Al: Al5Ti2, Al11Ti5, Al2Ti, AlTi3, Al3Ti, including in the framework of one formula unit of different types of structures (stable and metastable, virtual) can be implemented. During the mechano-chemical reactions in the contact zone between titanium and aluminum are formed during explosion welding nonequilibrium intermetallic phases: Al2Ti, Al5Ti3, Ti3.3Al. To study the transition zones of the samples structure used a scanning electron microscope JEOL 6390LV. The phase analysis was performed on the X-ray diffractometer company “Bruker” in the emission of copper. It is shown that the mass transfer titanium aluminum atomic clusters directional flow at a rate of at least 35 m / s occurs. Intermetallic phases formed in the contact zone during mechanochemical reactions occurring at the interface of Ti and Al. Processes of structure formation under explosion welding are explained from the standpoint of an abnormally rapid directional mass transfer under conditions of stress, creating a lattice curvature.

Текст научной работы на тему «Исследование неравновесных фаз, образующихся при сварке взрывом титана и алюминия»

UDK 621.771

Sibirskii Gosudarstvennyi Aerokosmicheskii Universitet imeni Akademika M. F. Reshetneva. Vestnik Vol. 18, No. 1, P. 205-210

STUDIES OF NONEQUILIBRIUM PHASES FORMED AT EXPLOSION WELDING OF TITANIUM AND ALUMINUM

F. M. Noskov 1, L. I. Kveglis 1, V. I. Mali 2, M. B. Leskov E. V. Zakharova 1

1 Siberian Federal University 79g, Svobodny Av., Krasnoyarsk, 660041, Russian Federation

2 Institute of Hydrodynamics them. Lavrenteva SB RAS 15, Lavrentiev Av., Novosibirsk, 630090, Russian Federation E-mail: leskovmb@gmail.com

The work is devoted to the study of physical and chemical processes occurring in the contact zone of titanium and aluminum at the joint plastic deformation caused by explosion welding. One of the most effective ways to solve problems of materials science is the development of composite materials. An important advantage of the materials used in aircraft, is their low density, providing the possibility to receive the result composites with high specific strength. This study supports the development of composite materials based on Ti—Al, which can be used for the manufacture of gas turbine blades, and ribbed hollow weldments for the aircraft industry.

Explosion welding is a high-energy process, allowing high quality joining dissimilar metal materials including various combinations of materials used for the composite metal-intermetallic compound.

Ti-Al system was studied extensively enough, but there remain a number of unclear issues, namely which can form intermetallic phases with the explosion welding. conditions for the formation of a number of intermetallic phases Ti-Al: Al5Ti2, AluTi5, Al2Ti, AlTi3, Al3Ti, including in the framework of one formula unit of different types of structures (stable and metastable, virtual) can be implemented. During the mechano-chemical reactions in the contact zone between titanium and aluminum are formed during explosion welding nonequilibrium intermetallic phases: Al2Ti, Al5Ti3, Ti33Al.

To study the transition zones of the samples structure used a scanning electron microscope JEOL 6390LV. The phase analysis was performed on the X-ray diffractometer company "Bruker" in the emission of copper.

It is shown that the mass transfer titanium aluminum atomic clusters directional flow at a rate of at least 35 m / s occurs. Intermetallic phases formed in the contact zone during mechanochemical reactions occurring at the interface of Ti and Al. Processes of structure formation under explosion welding are explained from the standpoint of an abnormally rapid directional mass transfer under conditions of stress, creating a lattice curvature.

Keywords: explosion welding, mass transfer, Mechanochemistry, intermetallic phases, the curvature of the crystal lattice.

Вестник СибГАУ Том 18, № 1. С. 205-210

ИССЛЕДОВАНИЕ НЕРАВНОВЕСНЫХ ФАЗ, ОБРАЗУЮЩИХСЯ ПРИ СВАРКЕ ВЗРЫВОМ ТИТАНА И АЛЮМИНИЯ

Ф. М. Носков \ Л. И. Квеглис \ В. И. Мали 2, М. Б. Лесков Е. В. Захарова 1

1 Сибирский федеральный университет Российская Федерация, 660041, г. Красноярск, просп. Свободный, 79г

2 Институт гидродинамики имени Лаврентьева СО РАН Российская Федерация, 630090, г. Новосибирск, просп. Лаврентьева, 15 E-mail: leskovmb@gmail.com

Представлено исследование физико-химических процессов, происходящих в зоне контакта титана и алюминия при совместной пластической деформации, вызванной сваркой взрывом. Один из наиболее эффективных путей решения задач материаловедения заключается в разработке композиционных материалов. Важным достоинством материалов, используемых в летательных аппаратах, является их малая плотность, обеспечивающая возможность получать в итоге композиты с высоким уровнем удельной прочности. Данное исследование способствует разработке композитных материалов на основе Ti-Al, которые могут быть использованы для изготовления лопаток газовых турбин, пустотелых и ребристых сварных конструкций для авиационной промышленности.

Сварка взрывом представляет собой высокоэнергетический технологический процесс, позволяющий с высоким качеством соединять разнородные металлические материалы, в том числе различные комбинации материалов, используемых для композитов металл-интерметаллид.

Система Т1—Л1 исследована достаточно широко, однако остается ряд неясных вопросов, а именно, какие интерметаллидные фазы могут образоваться при сварке взрывом. Условия образования ряда интерметаллид-ных фаз Т1-Л1: Л15Т12, Л1иТ15, Л12Т1, ЛШ3, Л13Т1, среди которых в рамках одной формульной единицы могут быть реализованы различные типы структур (стабильные, метастабильные, виртуальные). В процессе меха-нохимических реакций в зоне контакта титана и алюминия при сварке взрывом формируются неравновесные интерметаллические фазы: Л12Т1, Л15Т13, Т133Л1.

Для исследования структуры переходных зон полученных образцов использовали сканирующий электронный микроскоп №0Ь 6390ЬУ. Фазовый анализ проводили на рентгеновском дифрактометре фирмы Бгиквг в излучении меди.

Показано, что массоперенос титана в алюминий происходит направленными потоками атомных кластеров со скоростью не менее 35 м/с. В зоне контакта Т1 и Л1 формируются интерметаллические фазы в процессе механохимических реакций, протекающих на интерфейсе. Процессы структурообразования при сварке взрывом объясняются с позиций аномально быстрого направленного массопереноса в условиях напряжений, создающих кривизну кристаллической решетки.

Ключевые слова: сварка взрывом, массоперенос, механохимия, интерметаллидные фазы, кривизна кристаллической решетки.

Introduction. In aviation and space there is an urgent need to provide a strong, light and wear-resistant designs. One of the most effective ways to solve problems of materials science is the development of composite materials. An important advantage of the materials used in aircraft, their low density, providing the possibility to receive the result composites with high specific strength. For example in [1; 2] developed composite materials based on Ti-Al, Ni-Al, which can be used for the manufacture of gas turbine blades, and ribbed hollow weldments for the aircraft industry. It is known that titanium and aluminum, can react with each other to form intermetallic compounds such as TiAl3, characterized by high hardness and friability. It is known [2] that the formation of intermetallic compounds leads to a drastic reduction of mechanical characteristics of welded structures. However, in [3], the specific rigidity Ti-TiAl3 twice the specific rigidity steel. In [4] a detailed study of the structure and properties of multilayered composite Ti-Al, produced by explosion welding. It is shown that intermetallic compound TiAl3 greatly improves the mechanical properties of the composite. In [5] states that the operation of the intermetallic alloys based on Ti-Al at temperatures below 600 °C is ineffective in connection with the destruction of the fragile material. Heating in the range from 600 °C to 750 °C contributes to a sharp increase in ductility intermetallics while maintaining its strength. This allows their use in the aerospace industry.

In recent years, explosive welding has proved to be an effective method of creating a multi-layered composite materials. explosion welding is a high-energy process, allowing high quality joining dissimilar metal materials including various combinations of materials used for the composite metal - intermetallic laminated (MIL) [4]. Pressure developed during the explosion welding, providing excellent contact between the surfaces of the welded metal. The cumulative flow generated during the welding process, cleans the plate from the oxide films and impurities that could reduce the rate of solid-phase processes [6]. Subsequent annealing is proposed as an alternative method of creating a multi-layer metal -

intermetallic laminated (MIL) [4]. Annealing may be conducted at temperatures above and below the melting point of aluminum, local melting can occur due to the exothermic nature of the reaction between Al and Ti [7].

Currently, solid-state processes that may occur during the plastic deformation actively studied [3-9]. Mechanical impact can initiate mechanochemical reactions occurring at high speeds during the passage of plastic deformation waves [10]. The possibility of formation of intermetallic compounds due to the energy expended on the plastic deformation of the metal heat affected zone [11].

The ultra-high pressure and shear strain can increase the mass transfer rate by 15 orders of magnitude compared to the conventional diffusion [12; 13]. The usual mechanisms of a new phase with the emergence and growth of embryos in plastic deformation wave can not work because of the short duration of the process. For the formation of new phases in the static experiments, the time required several seconds or more. In the waves of plastic deformation of these processes will be completed within the order of 10-5-10-7 c [14]. In practice, particle sizes of the new phase can reach several tenths of a millimeter and more [14]. The study of the processes occurring in the metal contact zone with intense dynamic loads, is of considerable interest for the production of composite materials with new properties.

Ti-Al system was studied extensively enough, but there remain a number of unclear issues, namely which can form intermetallic phases with the explosion welding. In [15] identified a number of conditions for the formation of intermetallic phases Ti-Al: Al5Ti2, AlnTi5, Al2Ti, AlTi3, Al3Ti, including in the framework of one formula unit of different types of structures (stable and metastable, virtual) can be implemented.

Objective. To investigate the products of solid state reactions, occurring in the contact zone of titanium and aluminum at the joint plastic deformation caused by explosion welding.

Methods of experiment. Samples of the composite obtained by explosion welding multilayer stack wafers

commercially pure titanium VT1-0 (IMI125) and A5 (ENAW-1050A) thick aluminum 0.5 and 1 mm, respectively. Package 11 of alternating titanium and aluminum plates 12 are welded one explosion of the explosive charge ammonite 6GV as described in [16]. The thickness of the explosive was 45 mm, is made up of plates dimensions 80*80 mm. Detonation velocity estimated at 3600 m / s collision angles were set by 24o (upper plate) to 6,2o (for the lower plate). We studied the structure of the transition zone in the cross-sectional plane (perpendicular to the layers of aluminum and titanium) and aluminum contact area structure and titanium after mechanical separation of the layers of the composite.

To study the transition zones of the samples structure used a scanning electron microscope JEOL 6390LV. The phase analysis was performed on the X-ray diffractometer company "Bruker" in the emission of copper.

Experimental results. Fig. 1 shows image of the contact area in the transverse cut plane aluminum and titanium obtained by X-ray microanalysis. We see what happened titanium penetration into aluminum, and the process is not a continuous front of the diffusion zone, was the formation of discrete particles at a considerable depth of the contact zone.

Aluminium also penetrates into the titanium, but in much smaller quantity than titanium in aluminum. Study of energy dispersive spectra (fig. 1), and X-ray diffraction spectra revealed that the aluminum to titanium from 10 to 70 microns in depth, formed intermetallic compound. Assuming that the distance that penetrates the titanium in aluminum is about 70 micrometers (fig. 1, a), and the reaction time is about 2 microseconds, then a simple calculation shows that the rate of mass transfer of titanium in aluminum is not less than 35 m / from. According to [17; 18], the coefficient of mutual diffusion of titanium and aluminum at a temperature of 1,123 K is about 10-16 m2 / s, from the viewpoint of diffusion rate is 8.10 m / s. Therefore, in this experiment, the mass transfer titanium in aluminum (significantly at temperatures below 1000 K), at least eight orders of magnitude higher than the rate of diffusion. Similar results were obtained with other materials in the paper [19].

By method scanning electron microscopy and energy dispersive analysis was investigated the area contact aluminum and titanium after mechanical separation of the layers of the composite. Image of the surface of the titanium band gap in the X-ray of titanium and aluminum are shown in fig. 2, a and b, respectively.

Ti Ka1

IOOmi:«

IUiB *

b

Fig. 1. Study contact zone Ti-Al: a - the image obtained in the scanning electron microscope mode in microanalysis X-ray of titanium; b - Energy-spectrum square area shown in fig. 1, a

ж xjß

Я . _ .

&

4L v

Ж

b

Fig. 2. Image Ti surface area in contact with the Al in the resulting SEM microanalysis mode in: a - X-ray of titanium; b - X-ray of aluminum

a

a

Fig. 3. X-ray diffraction spectra of the titanium surface (on the top) and aluminum (bottom) phase and reflexes: Al2Ti (diamonds), Al5Ti3 (squares), Ti33Al (circles)

On the surface of titanium fig. 2, a you can see the dark specks - aluminum, and fig. 2, b light specks correspond to aluminum. Since the location of these inclusions in fig. 2, a and fig. 2, b substantially coincide, a coincidence indicates good adhesion of aluminum to titanium in the resulting samples. The concentration of aluminum in the inclusions on the surface of the titanium layer can be up to 20 at. %.

X-ray diffraction spectra from the surface of the titanium and aluminum layers after their separation are shown in fig. 3. On the surface of the titanium layer revealed the presence of intermetallic compounds and Al2Ti Ti3.3Al. On the surface of the aluminum layer revealed the presence of intermetallic compounds and Al2Ti Al5Ti3.

The phase Al2Ti existing in a very narrow concentration range presents at diagram of phase equilibria Al-Ti [20]. This phase is formed by explosion welding. Based on the state diagram, you can expect to see Ti3Al phase having a wide field of existence, however, is not found in our experiment this phase. Phase Al5Ti3 and Ti3.3Al absent in the diagram of phase equilibria, but are present in the samples welded by explosion. Thus due to explosion welding we discovered the occurrence of non-equilibrium phases.

The discussion of the results. Mass transfer during explosion welding can be caused by gradients of stress, which are significantly higher than the yield strength of the material. Any excess of the yield stress gives rise to a wave of plastic deformation [12]. The waves of plastic deformation, according V. E. Panin theory, can create significant non-diffusion fluxes of mass propagating over long distances with the speed of sound in the material. An example of such speed of mass transfer is given in [21].

If explosion welding, significant curvature of crystalline lattice is appearing in the local contact zone of welded blanks [22; 23]. In the context of the local curvature of the crystalline lattice, in areas of increased

interatomic distances special structural states are exist, which increase the degrees of freedom in a deformable solid. In [24] such states were called interatomic bifurcation structural states (IBSS). Due to occurrence in deformed metal IBSS possible to implement the directional mass transfer proceeding at a speed of switching of interatomic bonds, which in some cases can reach sound velocity in the metal [25]. The redistribution of atoms at the interface of the two materials may accelerate the formation of new phases, noted in [16].

Conclusion:

1. In the process of mechanochemical reaction at the contact zone of titanium and aluminum at explosion welding nonequilibrium intermetallic phases are formed: Al2Ti, Al5Ti3, Ti3.3Al.

2. During explosion welding mass transfer occurs by penetration flows of titanium atoms over distances of up to 70 microns from the interface at a rate of at least 35 m / s.

3. Processes of structure formation under explosion welding can be explained from the position of the crystal lattice curvature which appears in the conditions of stress gradient and leads to abnormally rapid directional mass transfer.

Acknowledgments. The authors thank A. K. Abkaryana (Siberian Federal University, Krasnoyarsk) and A. D. Gre-chanik (IRGETAS, Ust-Kamenogorsk) for help with the experiment.

Благодарности. Авторы благодарят А. К. Абкаряна (Сибирский федеральный университет, г. Красноярск) и А. Д. Гречаника (ШГЕТАС, г. Усть-Каменогорск) за помощь в эксперименте.

References

1. Badamshin I. Kh., Kusova O. I. [The temperature dependence of the elastic modulus and intermetallic TiAl Ni3Al - the main alloy components of gas turbine blades]. Vestnik UGATU. 2012, Vol. 16, No. 5(50), P. 4143 (In Russ.).

2. Ponomarev D. V., Gadalov V. N., Bashurin A. V., Mastikhin E. Yu. [Diffusion welding of titanium-aluminum laminate panels]. Vestnik VGTU. 2008, Vol. 4, No. 10, P. 40-43 (In Russ.).

3. Vecchio K. S. Synthetic multifunctional metallic-intermetallic laminate composites. JOM. 2005, Vol. 57(3), P. 25-31. DOI: 10.1007/s11837-005-0229-4.

4. Bataev I. A., Bataev A. A., Mali V. I., Pavliukova D. V. Structural and mechanical properties of metallic-intermetallic laminate composites produced by explosive welding and annealing. Materials & Design. 2012, Vol. 35, P. 225-234. DOI: http://dx.doi.org/10.1016/ j.matdes.2011.09.030.

5. Gus'kov M. S. Sozdanie vysokoprochnogo kom-pozitsionnogo materiala titan - alyuminiy s perfo-rirovannym intermetallicheskim sloem i oksido-kerami-cheskim pokrytiem. Diss. kand. tekh. nauk [Creating high-titanium composite material - a perforated aluminum intermetallic layer and ceramic oxide coating. Cand. eng. sci. diss.]. Penza, 2015. 151 p.

6. Deribas A. A. Fizika uprochneniya i svarki vzryvom [Physics hardening and explosion welding]. Novosibirsk, Nauka Publ., 1980, P. 188.

7. Harach D. J., Vecchio K. S. Microstructure evolution in metal-intermetallic laminate (MIL) composites synthesized by reactive foil sintering in air. Metal Mater Trans. 2001, Vol. 32A, P. 1493-505. DOI: 10.1007/s11661-001-0237-0.

8. Bychkov V. M., Selivanov A. S. [Study of weldability of heat-resistant nickel alloy EP742 by linear friction welding]. Vestnik UGATU. 2012, Vol. 16, No. 7(52), P. 112-116 (In Russ.).

9. Kuz'min S. V., Lysak V. I., Rybin V. V., Peev A. P. [Features of plastic deformation of the metal heat-affected zone at explosion welding of dissimilar metals]. Izvestiya VolgGTU. 2010, Vol. 5, No. 4, P. 4-11 (In Russ.).

10. Panin V. E., Grinjaev Ju. V. [Physical Meso-mechanics - a new paradigm at the intersection of physics and mechanics of solids]. Fiz. mezomeh. 2003, Vol. 6, No. 4, P. 9-36 (In Russ.).

11. Zel'dovich Ja. B. Fizika udarnykh voln i vysoko-temperaturnykh gidrodinamicheskikh yavleniy [Physics of Shock Waves and High-Temperature Hydrodynamic Phenomena]. Mosocw, Fizmatlit Publ., 2008, 656 p.

12. Panin V. E., Egorushkin V. E. Curvature. Solitons as generalized structural wave carriers of plastic deformation and fracture. Physical Mesomechanics. 2013, Vol. 16, Iss. 4, P. 267-286. DOI: 10.1134/S1029959913040012.

13. Enikolopov E. S. [Effect of high pressure on the chemical shift reaction]. Mezhdunarodnyy simpozium po khimicheskoy fizike. Sbornik materialov [International Symposium on Chemical Physics. The collection of materials]. Chernogolovka, Izd. Otdela himicheskoy fiziki Publ., 1981, P. 83 (In Russ.).

14. Dremin A. N., Breusov O. N. Processes Occurring in Solids Under the Action of Powerful Shock Waves. RUSS CHEM REV. 1968, Vol. 37, No. 5, P. 392-402. DOI: 10.1070/RC1968v037n05ABEH001643.

15. Ghosh G., Asta M. First-principles calculation of structural energetics of Al-TM (TM = Ti, Zr, Hf) intermetallics. Acta Materialia. 2005, Vol. 53, P. 32253252. DOI: 10.1016/j.actamat.2005.03.028.

16. Mali V. I., Pavliukova D. V., Bataev I. A., Bataev A. A., Smirnov A. A., Yrtsev P. S., Bazarkina V. V. Formation of the intermetallic layers in Ti-Al multilayer composites. Advanced Materials Research. 2011, Vol. 311313, P. 236-239. DOI 10.4028/www. scientific. net/ AMR. 311-313.236.

17. Bokshtejn B. S. Diffuziya v metallah [Diffusion in Metals]. Moscow, Metallurgiya Publ.,1978, 248 p. (In Russ.).

18. Larikov L. N., Isajchev V. I. Struktura i svoystva metallov i splavov. Diffuziya v metallakh i splavakh [Structure and properties of metals and alloys. Diffusion in metals and alloys.]. Kiev, Naukova dumka Publ., 1987, 510 p. (In Russ.).

19. Zvorykin L. O. Osobennosti massoperenosa v metallah i splavah pri prohozhdenii udarnyh voln. Avtoref. dokt. tekh. nauk [Features of the mass transfer in metals and alloys during the passage of shock waves. Doct. Diss.]. Kiev, Institut metallofiziki AN Ukrainy Publ., 1994, 240 p. (In Russ.).

20. Ljakishev N. P. Diagrammy sostoyaniya dvoynykh metallicheskikh system [The diagrams of binary metallic systems]. Moscow, Mashinostroenie Publ., 1996, Vol. 3, 992 p.

21. Markidonov A. V., Starostenkov M. D., Soskov A. A., Poletaev G. M. Molecular dynamics study of structural transformations of cylindrical nanopores in gold under thermal activation conditions and under the action of acoustic and shock waves. Physics of the Solid State. 2015, Vol. 57, No. 8, P. 1551-1554. DOI: 10.1134/ S106378341508017X.

22. Meng X., Yanshu F., Xiaoshu Z. Quantitative characterization of morphology of explosive welding interfaces based on fractal theory. Explosion and Shock Waves. 2016, Vol. 36, Iss. 1, P. 50-56. DOI: 10.11883/ 1001-1455(2016)01-0050-07.

23. Greenberg B. A., Ivanov M. A., Inozemtsev A. V., Kuz'min S. V., Lysak V. I., Vlasova A. M., Pushkin M. S. Interface relief upon explosion welding: Splashes and waves. Physics of Metals and Metallography. 2015, Vol. 116, Iss. 4, P. 367-377. DOI: 10.1134/S0031918 X15040079.

24. Panin V. E., Panin A. V., Elsukova T. F., Popko-va Yu. F. Fundamental Role of Crystal Structure Curvature in Plasticity and Strength of Solids. Phys. Mesomech. 2015, Vol. 18, No. 2, P. 89-99. DOI: 10.1134/ S1029959915020010.

25. Abylkalykova R. B., Kveglis L. I., Kalitova A. A., Noskov F. M. Abnormally Fast Migration of Substance at Shock Loadings. Advanced Materials Research. 2014, Vol. 871, P. 231-234. DOI: 10.4028/www.scientific.net/ AMR.871.231.

Библиографические ссылки

1. Бадамшин И. Х., Кусова О. И. Температурная зависимость модуля упругости интерметаллидов TiAl и Ni3Al - основных компонентов сплавов лопаток газовых турбин // Вестник УГАТУ. 2012. Т. 16, № 5(50). С. 41-43.

2. Диффузионная сварка слоистых титано-алюминевых панелей / Д. В. Пономарев [и др.] // Вестник ВГТУ. 2008. Т. 4, № 10. С. 40-43.

3. Vecchio K. S. Synthetic multifunctional metallic-intermetallic laminate composites // JOM 2005. Vol. 57(3). P. 25-31. DOI: 10.1007/s11837-005-0229-4.

4. Structural and mechanical properties of metallic-intermetallic laminate composites produced by explosive welding and annealing / I. A. Bataev [et al.] // Materials & Design. 2012. Vol. 35. P. 225-234. DOI: http://dx.doi. org/10.1016/j.matdes.2011.09.030.

5. Гуськов М. С. Создание высокопрочного композиционного материала «титан-алюминий» с перфорированным интерметаллическим слоем и оксидо-керамическим покрытием : дис. ... канд. техн. наук / Пензенский государственный университет. Пенза, 2015. 151 с.

6. Дерибас А. А. Физика упрочнения и сварки взрывом. Новосибирск : Наука. 1980. 188 c.

7. Harach D. J., Vecchio K. S. Microstructure evolution in metal-intermetallic laminate (MIL) composites synthesized by reactive foil sintering in air // Metal Mater Trans. 2001. Vol. 32A. P. 1493-505. DOI: 10.1007/ s11661-001-0237-0.

8. Бычков В. М., Селиванов А. С. Исследование свариваемости жаропрочного никелевого сплава ЭП742 методом линейной сварки трением // Вестник УГАТУ. 2012. Т. 16, № 7(52). С. 112-116.

9. Особенности пластической деформации металла околошовной зоны при сварке взрывом разнородных металлов / С. В. Кузьмин [и др.] // Известия ВолгГТУ. 2010. Т. 5, № 4. С. 4-11.

10. Панин В. Е., Гриняев Ю. В. Физическая мезо-механика - новая парадигма на стыке физики и механики деформируемого твердого тела // Физическая мезомеханика. 2003. Т. 6, No. 4. С. 9-36.

11. Зельдович Я. Б. Физика ударных волн и высокотемпературных гидродинамических явлений. М. : Физматлит, 2008. 656 с.

iНе можете найти то, что вам нужно? Попробуйте сервис подбора литературы.

12. Panin V. E., Egorushkin V. E. Curvature. Solitons as generalized structural wave carriers of plastic deformation and fracture // Physical Mesomechanics. 2013. Vol. 16, iss. 4. P. 267-286. DOI: 10.1134/ S1029959913040012.

13. Ениколопов Е. С. Влияние высокого давления со сдвигом на химические реакции // Международный симпозиум по химической физике : сб. материалов. Черноголовка : Изд-во Отдела химической физики, 1981. С. 83.

14. Dremin A. N., Breusov O. N. Processes Occurring in Solids Under the Action of Powerful Shock Waves //

RUSS CHEM REV. 1968. Vol. 37, № 5. P. 392-402. DOI: 10.1070/RC1968v037n05ABEH001643.

15. Ghosh G., Asta M. First-principles calculation of structural energetics of Al-TM (TM = Ti, Zr, Hf) intermetallics // Acta Materialia. 2005. Vol. 53. Р. 32253252. DOI: 10.1016/j.actamat.2005.03.028.

16. Formation of the intermetallic layers in Ti-Al multilayer composites / V. I. Mali [et al.] // Advanced Materials Research. 2011. Vol. 311-313. P. 236-239. DOI 10.4028/www.scientific.net/AMR.311-313.236.

17. Бокштейн Б. С. Диффузия в металлах. М. : Металлургия,1978. 248 с.

18. Лариков Л. Н., Исайчев В. И. Структура и свойства металлов и сплавов. Диффузия в металлах и сплавах. Киев : Наукова думка, 1987. 510 c.

19. Зворыкин Л. О. Особенности массопереноса в металлах и сплавах при прохождении ударных волн : автореф. дис. ... д-ра техн. наук. Киев : Ин-т металлофизики АН Украины, 1994. 240 с.

20. Лякишев Н. П. Диаграммы состояния двойных металлических систем : справ. В 3 т. М. : Машиностроение, 1996. 992 с.

21. Molecular dynamics study of structural transformations of cylindrical nanopores in gold under thermal activation conditions and under the action of acoustic and shock waves / A. V. Markidonov [et al.] // Physics of the Solid State. 2015. Т. 57, № 8. P. 15511554. DOI: 10.1134/S106378341508017X.

22. Meng X., Yanshu F., Xiaoshu Z. Quantitative characterization of morphology of explosive welding interfaces based on fractal theory // Explosion and Shock Waves. 2016. Vol. 36, iss. 1. P. 50-56. DOI: 10.11883/ 1001-1455(2016)01-0050-07.

23. Interface relief upon explosion welding: Splashes and waves / B. A. Greenberg [et al.] // Physics of Metals and Metallography. 2015. Vol. 116, iss. 4. P. 367-377. DOI: 10.1134/S0031918X15040079.

24. Fundamental Role of Crystal Structure Curvature in Plasticity and Strength of Solids / V. E. Panin [et al.] // Phys. Mesomech. 2015. Vol. 18, No. 2. P. 89-99. DOI: 10.1134/S1029959915020010.

25. Abnormally Fast Migration of Substance at Shock Loadings / R. B. Abylkalykova [et al.] // Advanced Materials Research. 2014. Vol. 871. P. 231-234. DOI: 10.4028/www.scientific.net /AMR.871.231.

© Noskov F. M., Kveglis L. I., Mali V. I., Leskov M. B., Zakharova E. V., 2017

i Надоели баннеры? Вы всегда можете отключить рекламу.