Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles

The uniaxial and hydrostatic deformations of martensitic structure B19’ of NiTi shape memory alloy are studied using first-principles calculations. The bulk and Young’s moduli and the theoretical strength under uniaxial tension and hydrostatic loading are computed from crystal response to applied de...

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Published in:Проблемы прочности
Date:2008
Main Authors: Sestak, P., Cerny, M., Pokluda, J.
Format: Article
Language:English
Published: Інститут проблем міцності ім. Г.С. Писаренко НАН України 2008
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/48236
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Cite this:Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles / P. Sestak, M. Cerny, J. Pokluda // Проблемы прочности. — 2008. — № 1. — С. 20-23. — Бібліогр.: 7 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Sestak, P.
Cerny, M.
Pokluda, J.
author_facet Sestak, P.
Cerny, M.
Pokluda, J.
citation_txt Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles / P. Sestak, M. Cerny, J. Pokluda // Проблемы прочности. — 2008. — № 1. — С. 20-23. — Бібліогр.: 7 назв. — англ.
collection DSpace DC
container_title Проблемы прочности
description The uniaxial and hydrostatic deformations of martensitic structure B19’ of NiTi shape memory alloy are studied using first-principles calculations. The bulk and Young’s moduli and the theoretical strength under uniaxial tension and hydrostatic loading are computed from crystal response to applied deformations. The behavior of angle β of the B 19’ structure was investigated along the whole deformation path. The computed values of Young’s moduli are compared with available experimental results. The results obtained complement and extend the already known characteristics of NiTi alloy. Проведено исследование одноосной и гидростатической деформаций мартенситной структуры B19’ сплава с памятью формы NiTi по методу расчетов ab initio. Величины объемного модуля упругости, модуля Юнга и теоретической прочности при одноосном растяжении и гидростатическом нагружении рассчитаны по реакции кристалла на приложенные деформации. Изучен характер изменения угла β структуры B19’ по всей траектории деформации. Выполнено сопоставление расчетных значений модуля Юнга с имеющимися экспериментальными результатами. Полученная информация дополняет и расширяет уже известные данные о характеристиках сплава NiTi.
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fulltext UDC 539. 4 E la s t ic P r o p e r t ie s o f B 1 9 ’ S tr u c tu r e o f N iT i A l lo y u n d e r U n ia x ia l a n d H y d r o s ta t ic L o a d in g f r o m F ir s t P r in c ip le s P . S estak ,1a M . C ern y ,1b and J . P o k lu d a 1c 1 Institute o f Physical Engineering, Faculty o f Mechanical Engineering, Brno University o f Technology, Brno, Czech Republic a sestak@kn.vutbr.cz, b cerny.m@fme.vutbr.cz, c pokluda@fme.vutbr.cz The uniaxial and hydrostatic deformations o f martensitic structure B 19’ o f NiTi shape memory alloy are studied using first-principles calculations. The bulk and Young’s moduli and the theoretical strength under uniaxial tension and hydrostatic loading are computed from crystal response to applied deformations. The behavior o f angle 5 o f the B 19’ structure was investigated along the whole deformation path. The computed values o f Young’s moduli are compared with available experim ental results. The results obtained com plem ent and extend the already known characteristics o f NiTi alloy. K eyw o rd s : N iT i, B 1 9 ’, shape m em ory alloy, first principles, ab-initio, elastic properties, theoretical strength, uniaxial and hydrostatic deformation. In trod uction . The shape m em ory alloys (SM A ) are important materials for many industrial as w e ll as m edical applications ow ing to their shape m em ory effect. This effect is connected w ith a transformation betw een martensitic and austenitic structure, w hich can be started by an external pressure or temperature. There are several types o f the transformations, depending on a particular alloy. The nickel-titanium alloy is one o f the m ost important types o f SM A. It is w idely used in m edicine (stents, bone im plants, etc.). The N iT i alloy can transform from the m onoclin ic B 1 9 ’ (m artensitic) to cubic B 2 (austenitic) structure and v ice versa. A n extensive overview o f a current state o f the art can be found in the paper b y Otsuka and Ren [1]. The aim o f this work is to com pute the Young E and bulk B m oduli and the theoretical strengths under uniaxial and hydrostatic (isotropic) loading. The Young m odulus has been com puted for three crystallographic directions (E [100], E [010], and E [001]) parallel to prim itive translation vectors (r1, r2 , and ^ ) show n in Fig. 1. The dependence o f the 5 angle (betw een r1 and r 3 vectors) on the applied uniaxial deform ation has been also investigated. [Û10] N r„ -- rx [1ÛQ] Fig. 1. The martensitic structure (B19’) o f NiTi alloy with marked crystallographic directions. © P. SESTÂK, M. CERNŸ, J. POKLUDA, 2008 20 ISSN 0556-171X. Проблемы прочности, 2008, № 1 mailto:sestak@kn.vutbr.cz mailto:cerny.m@fme.vutbr.cz mailto:pokluda@fme.vutbr.cz Elastic Properties o f B 1 9 ’ Structure o f NiTi Alloy E lectron ic S tru ctu re C om pu tations. A ll quantities o f interest are com puted from the total energy E total o f the system at hand as a function o f an appropriate deform ation and from the H ellm an-Feynm an stress tensor The total energies and stresses w ere com puted b y the A binit program code. A binit is a great tool for electronic structure calculations developed by the team o f Prof. X avier G onze at the U niversity Catholique de Louvain [2, 3], w hich is distributed under the G N U General Public L icense. Another additional package including pseudo-potentials [4] together w ith its generators, manuals, tutorials, exam ples, etc. is available at [5]. The calculations w ere perform ed using G G A norm -conserving pseudo-potentials and the cu to ff energy w as set to 1000 eV for com putations o f elastic m oduli and 800 eV for theoretical strength evaluation. The solution w as considered to be self-consistent w hen the energy difference o f three consequent iterations becam e sm aller than 0.1 f ie V for com putation o f elastic properties and 1.0 i e V for the theoretical strength. During the uniaxial deform ation the structure m ust be relaxed in order to a llow the Poisson contraction. The relaxations w ere m ade by an external procedure utilizing the Hellm an-Feynm an stress tensor [6 ] com puted by the A binit code. C om p u tation o f E la stic M od u li and T h eoretica l S trength . The Y oung’s m odulus can be com puted as 1 d E total E = V 0 “ i 2- , (1) where £ is the relative uniaxial deform ation, £ = a /a 0 — L Sim ilarly, the uniaxial stress can be evaluated as _ uni 1 d E total V0 d£ (2 ) The bulk m odulus and the hydrostatic stress were calculated according to the relations 1 d Etotal B = (3) and a hyd = ± ^ to to L , V0 dv (4) where v is the relative volum e v = V0 / V — I Both stresses approach their m axim a at the points o f inflection o f E totai ( e ) or E totai ( v ) dependences. I f no other instability appears before reaching the points, their m axim um values specify the corresponding theoretical strength values o id . R esu lts. The experim ental and ab-initio values o f prim itive translation vectors and angle o f the B 1 9 ’ structure are displayed in Table 1. The ab-initio results predict slightly larger values than those found in experim ent. This overestim ating o f translation vectors is a typical effect o f G G A pseudopotential type but the related errors are sm aller than 5%. Table 2 contains the com puted values o f the Y oung’s and bulk m oduli o f the martensitic B 1 9 ’ and austenitic B2 structures. A s can be seen, the Y oung’s m oduli o f B 1 9 ’ are higher than those o f the austenitic B2 structure for all the directions studied. These results are in contrast w ith experim ental and finite elem ent m ethod (FEM ) values, w hich predict the Y oung’s m odulus o f martensite to about one-third to one-half o f that o f austenite [7]. This can be explained by the fact that the experim ental data were m easured on polycrystalline sam ples at finite temperatures, w hereas the atom istic m odel does not allow ISSN 0556-171X. npoôëeubi npounocmu, 2008, № 1 21 P. Sestdk, M. Cerny, and J. Pokluda for any shear deformation o f martensite variants, and describes a hom ogeneous deformation o f a single crystal at the absolute zero temperature. On the other hand, the bulk m odulus for the B 1 9 ’ structure is low er than that for the B 2 structure. Table 3 contains values o f the theoretical strength for all applied deform ations. T a b l e 1 The Experimental [1] and Ab-Initio Crystallographic Data for B19’ Structure Parameter Experimental Ab initio ao , A 2.889 3.007 ^ , A 4.120 4.121 c^ A 4.622 4.813 5 , deg 96.8 100.6 V , A 3 54.63 58.61 T a b l e 2 The Elastic Moduli o f the B19’ and B2 Structures, as Obtained from Present Ab-Initio Calculations along with Experimental [7] Results Structure\moduli E [100], GPa E [010], GPa E [001], GPa B , GPa B 19’ (ab-initio) 96 124 126 137 B2 (ab-initio) 72 72 72 155 B2 (FEM) 69 69 69 - T a b l e 3 Computed Values o f the Theoretical Strength of the B19’ and B2 Structures Structure\theoretical strength a d [100], GPa a uf [010], GPa a uf [001], GPa aP,Ga B19’ (ab-initio) 19.0 27.5 20.7 22.1 B2 (ab-initio) - - - 24.0 - 0.1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 1.2 1.3 Relative deform ation Fig. 2. The angle 5 as a function o f applied deformation. The detail o f the range close to the nondeformed state is depicted at the bottom right. Under an applied deform ation, the angle 5 changes as a result o f the relaxation procedure. The dependence o f the 5 angle on the applied deform ation is show n in Fig. 2. 22 ISSN 0556-171X. npo6neMbi npouHocmu, 2008, № 1 Elastic Properties o f B 1 9 ’ Structure o f NiTi Alloy The points related to the theoretical strength are also marked (the inflection point in the dependence E total ( e ) resp. E total ( v ) by dashed vertical lines. One can see that the angle i grow s for all the deform ation paths except for the [010] direction. N ote that the [010] direction is perpendicular to vectors ri and r 3 ; therefore, the decrease in the i angle during the [01 0 ] deform ation is to be expected. C onclusions. The uniaxial and hydrostatic deform ation o f martensitic structure B 1 9 ’ o f N iT i shape m em ory alloy w as studied using first-principles calculations. The results o f com putations o f Y oung’s and bulk m oduli are as follow s: E [100] = 96 GPa, E [010] = 124 GPa, E [001] = 126 GPa, and B = 137 GPa. During the uniaxial and hydrostatic deform ation the theoretical strengths w ere com puted for all cases o f applied deformations: a u f [100] = 19.0 GPa, a u f [010] = 27.5 GPa, a u f [001] = 20 .7 GPa, and a h f = 22.1 GPa. The Young m oduli o f B 1 9 ’ are higher than those o f the austenitic B 2 structure for all the directions studied and the bulk m odulus for the B 1 9 ’ structure is low er than that for the B2 structure. The angle i grow s for all deform ation paths except for the [010] direction. Acknowledgments. This research was supported by research projects GA 106/05/H008 and MSM 0021630518. 1. K. Otsuka and X. Ren, Prog. Mater. Sci., 50, 511 (2005). 2. X. Gonze, J.-M. Beuken, R. Caracas, et al., Comp. Mater. Sci., 25, 478 (2002). 3. X. Gonze, G.-M. Rignanese, M. Verstraete, et al., Zeit. Kristallogr., 220, 558 (2005). 4. M. Fuchs and M. Scheffler, Comp. Phys. Communicat., 119, 67 (1999). 5. http://www.abinit.org 6. D. R. Hamann, X. Wu, K. M. Rabe, and D. Vanderbilt, Phys. Rev. B, 71 (2005). 7. X. M. Wang and Z. F. Yue, Comp. Mater. S ci, 39, 697 (2007). Received 28. 06. 2007 ISSN 0556-171X. n poôëeu u npouHocmu, 2008, № 1 23 http://www.abinit.org
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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
issn 0556-171X
language English
last_indexed 2025-12-07T18:39:33Z
publishDate 2008
publisher Інститут проблем міцності ім. Г.С. Писаренко НАН України
record_format dspace
spelling Sestak, P.
Cerny, M.
Pokluda, J.
2013-08-17T10:46:29Z
2013-08-17T10:46:29Z
2008
Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles / P. Sestak, M. Cerny, J. Pokluda // Проблемы прочности. — 2008. — № 1. — С. 20-23. — Бібліогр.: 7 назв. — англ.
0556-171X
https://nasplib.isofts.kiev.ua/handle/123456789/48236
539. 4
The uniaxial and hydrostatic deformations of martensitic structure B19’ of NiTi shape memory alloy are studied using first-principles calculations. The bulk and Young’s moduli and the theoretical strength under uniaxial tension and hydrostatic loading are computed from crystal response to applied deformations. The behavior of angle β of the B 19’ structure was investigated along the whole deformation path. The computed values of Young’s moduli are compared with available experimental results. The results obtained complement and extend the already known characteristics of NiTi alloy.
Проведено исследование одноосной и гидростатической деформаций мартенситной структуры B19’ сплава с памятью формы NiTi по методу расчетов ab initio. Величины объемного модуля упругости, модуля Юнга и теоретической прочности при одноосном растяжении и гидростатическом нагружении рассчитаны по реакции кристалла на приложенные деформации. Изучен характер изменения угла β структуры B19’ по всей траектории деформации. Выполнено сопоставление расчетных значений модуля Юнга с имеющимися экспериментальными результатами. Полученная информация дополняет и расширяет уже известные данные о характеристиках сплава NiTi.
en
Інститут проблем міцності ім. Г.С. Писаренко НАН України
Проблемы прочности
Научно-технический раздел
Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles
Исследование упругих свойств структуры B19’ сплава NiTi при одноосном и гидростатическом нагружении при использовании метода ab initio
Article
published earlier
spellingShingle Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles
Sestak, P.
Cerny, M.
Pokluda, J.
Научно-технический раздел
title Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles
title_alt Исследование упругих свойств структуры B19’ сплава NiTi при одноосном и гидростатическом нагружении при использовании метода ab initio
title_full Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles
title_fullStr Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles
title_full_unstemmed Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles
title_short Elastic properties of B19’ structure of NiTi alloy under uniaxial and hydrostatic loading from first principles
title_sort elastic properties of b19’ structure of niti alloy under uniaxial and hydrostatic loading from first principles
topic Научно-технический раздел
topic_facet Научно-технический раздел
url https://nasplib.isofts.kiev.ua/handle/123456789/48236
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