Influence of Annealing on NiTi Shape Memory Alloy Subjected to Severe Plastic

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    Inuence of annealing on NiTi shape memory alloy subjected to severe plasticdeformation

    Shuyong Jiang a,*, Yanqiu Zhang a, Lihong Zhao a, Yufeng Zheng b

    a Industrial Training Centre, Harbin Engineering University, Harbin 150001, Chinab Center for Biomedical Materials and Engineering, Harbin Engineering University, Harbin 150001, China

    a r t i c l e i n f o

    Article history:

    Received 13 February 2012

    Received in revised form

    30 April 2012

    Accepted 19 July 2012

    Available online 10 October 2012

    Keywords:

    A. Nanostructured intermetallics

    B. Martensitic transformations

    B. Shape-memory effects

    C. Heat treatment

    C. Plastic forming, cold

    a b s t r a c t

    The amorphous phase with the retained nanocrystalline phase, the deformation bands and the amor-

    phous bands coexist due to inhomogeneous plastic deformation in nickeletitanium shape memory alloy

    (NiTi SMA) subjected to severe plastic deformation (SPD) based on local canning compression. Trans-

    mission electron microscopy, X-ray diffraction and differential scanning calorimetry are used to inves-

    tigate microstructural evolution and phase transformation of NiTi sample subjected to SPD in the case of

    annealing for 2 h at 300 C, 450 C and 600 C, respectively. Annealing at 300 C and 450 C leads to

    nanocrystallization of amorphous NiTi sample, while annealing at 600 C results in the coarse-grained

    NiTi sample, where the (001) martensite compound twins are found. The precipitation phases such as

    Ni4Ti3 and Ni3Ti are suppressed in NiTi sample formed as a result of crystallization of the amorphous

    structure and thus occur more easily in the deformation bands in the case of annealing. Martensitic

    phase transformation is inuenced by the grain size and is suppressed with the decrease in the nano-

    crystalline grain size.

    2012 Elsevier Ltd. All rights reserved.

    1. Introduction

    Nickeletitanium shape memory alloy (NiTi SMA) is widely

    used in engineering elds due to its shape-memory effect as well

    as superelasticity [1]. Cold working plays an important role in

    engineering application of NiTi SMA and has a signicant inu-

    ence on shape-memory effect as well as superelasticity of NiTi

    SMA. In general, cold plastic deformation leads to a high density

    of dislocations in NiTi SMA, which makes a contribution to

    superelasticity of NiTi SMA [2e4]. However, severe plastic

    deformation (SPD) based on cold working is able to lead to

    nanocrystallization or amorphization of NiTi SMA. So far, plenty

    of work with respect to SPD of NiTi SMA in the case of cold

    working has been done over the last decade by means of high-pressure torsion (HPT) [5,6], cold rolling [7,8], cold drawing

    [9,10] and surface mechanical attrition treatment (SMAT)[11,12].

    SPD of NiTi SMA followed by subsequently appropriate heat

    treatment contributes to improving the mechanical properties

    and the functional properties of NiTi SMA, such as high ultimate

    strength and high elongation at the elevated temperatures [13]

    and perfect superelasticity [14,15], which is attributed to

    nanocrystallization of amorphous NiTi SMA prepared by SPD in

    the case of annealing. Many researchers investigated crystalliza-

    tion mechanism of amorphous NiTi SMA subjected to SPD and

    phase transformation behaviour of NiTi SMA after crystallization.

    Waitz et al. [16,17] induced nanocrystallization of an amorphous

    NiTi SMA based on HPT in the case of annealing and found that

    martensitic phase transformation is suppressed with decreasing

    the nanocrystalline grain size and phase transformation behav-

    iour is closely related to the nanocrystalline grain size. Peter-

    lechner et al. [18] studied relaxation and crystallization kinetics

    of amorphous NiTi SMA made by repeated cold rolling and

    revealed that nucleation and growth of the crystalline phase is

    based on mixed nucleation or nucleation with a decreasing rate

    as well as three-dimensional growth. Srivastava et al. [19]investigated the inuence of the different annealing tempera-

    tures on crystallization of amorphous bands of cold-rolled

    NiTi SMA and demonstrated that annealing for 30 min at or

    above 350C leads to crystallization of the amorphous regions

    and the grain size increases with the increase in the annealing

    temperature.

    In the present study, local canning compression was used in

    order to lead to SPD of NiTi SMA, and subsequently the inuence of

    annealing on microstructural evolution, precipitation and phase

    transformation of NiTi samples subjected to SPD was investigated

    systematically.* Corresponding author. Tel.: 86 139 36266338; fax: 86 451 82519952.

    E-mail address:[email protected](S. Jiang).

    Contents lists available at SciVerse ScienceDirect

    Intermetallics

    j o u r n a l h o m e p a g e : w w w . e l s e v i e r .c o m / l o c a t e / i n t e r m e t

    0966-9795/$e see front matter 2012 Elsevier Ltd. All rights reserved.

    http://dx.doi.org/10.1016/j.intermet.2012.07.025

    Intermetallics 32 (2013) 344e351

    mailto:[email protected]://www.sciencedirect.com/science/journal/09669795http://www.elsevier.com/locate/intermethttp://dx.doi.org/10.1016/j.intermet.2012.07.025http://dx.doi.org/10.1016/j.intermet.2012.07.025http://dx.doi.org/10.1016/j.intermet.2012.07.025http://dx.doi.org/10.1016/j.intermet.2012.07.025http://dx.doi.org/10.1016/j.intermet.2012.07.025http://dx.doi.org/10.1016/j.intermet.2012.07.025http://www.elsevier.com/locate/intermethttp://www.sciencedirect.com/science/journal/09669795mailto:[email protected]
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    2. Materials and methods

    As-received NiTi alloy with a nominal composition of Ni50.9Ti49.1(at.%) was prepared by means of vacuum induction melting

    method, and then was rolled at 800 C and nally was drawn to

    NiTi bar with the diameter of 12 mm. The transformation temper-

    atures of NiTi bar are as follows: Ms 27.2C, Mf41.7

    C,

    As 17.3C,Af4.1

    C. Therefore, microstructure of as-received

    NiTi bar possesses a typical B2 austenite structure at room

    temperature. NiTi samples with the diameter of 4 mm and the

    height of 6 mm were cut from the NiTi bar by means of electro-

    discharge machining (EDM) and then were locally inserted into

    the low carbon steel cans with the inner diameter of 4 mm, the wall

    thickness of 3 mm and the height of 3 mm. The locally canned NiTi

    samples were placed between the top anvil and the bottom one of

    INSTRON-5500R universal testing machine and then were

    compressed at the reduction in height by 75% at the strain rate of

    0.05 s1 at room temperature. The compressed NiTi samples were

    annealed for 2 h at 300 C, 450C and 600C, respectively, and

    subsequently were cooled to room temperature at the atmosphere.

    Microstructural evolution of NiTi samples subjected to SPD and

    subsequent NiTi samples subjected to annealing was investigated

    by means of transmission electron microscope (TEM). Foils for TEMobservation were mechanically ground to 70 mm and then thinned

    by twin-jet polishing in an electrolyte consisting of 6% HClO4, 34%

    C4H10O and 60% CH3OH by volume fraction. TEM observations were

    conducted on a FEI TECNAI G2 F30 microscope with a side-entry

    and double-tilt specimen stage with angular range of40 at an

    accelerating voltage of 300 kV.

    In order to further understand the phase structures of NiTi

    samples subjected to annealing, X-ray diffraction (XRD) was carried

    out using a Philips XPert Pro diffractometer with CuKaradiation at

    ambient temperature. The samples were scanned over 2q ranging

    from 10 to 100 by continuous scanning with tube voltage of 40 kV

    and tube current of 40 mA.

    Differential scanning calorimeter (DSC) was used in order to

    obtain the transformation temperatures of NiTi samples subjected

    to annealing in the temperature range from 100C to 100C at

    the heating and cooling rates of 10 C/min.

    3. Results

    3.1. NiTi sample subjected to SPD under local canning compression

    Fig.1 demonstrates the schematic diagram of deformation mode

    of NiTi sample under local canning compression and the corre-

    sponding TEM photographs taken from the different deformation

    zones of NiTi sample subjected to SPD. Fig. 1(a) shows the sche-

    matic diagram of deformation mode of NiTi sample subjected to

    SPD based on local canning compression. It can be seen from

    Fig. 1(a) that NiTi sample is caused to be in a three-dimensional

    compressive stress state during plastic deformation. In order to

    better understand deformation mechanism of NiTi sample under

    local canning compression, the continuous deformation process

    can be divided into two stages, namely intermediate deformation

    degree by 50% and nal deformation degree by 75%. When NiTi

    sample is subjected to reduction in height by 50%, it is completely

    compressed into the steel can, which undergoes radial and

    Fig. 1. Schematic diagram of deformation mode of NiTi sample under local canning compression and the corresponding TEM photographs taken from the different deformation

    zones. (a) Schematic diagram of deformation mode showing NiTi s ample subjected to SPD; (b) dark-eld image showing nanocrystalline phase embedded in the amorphous matrix;

    (c) bright-

    eld image showing the presence of amorphous bands; and (d) bright-

    eld image showing the presence of deformation bands.

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    tangential elongation strain without axial compression strain. Both

    NiTi sample and the steel can are subjected to radial and tangential

    elongation strain as well as axial compression strain in the case of

    reduction in height by 75%. Furthermore, the plastic deformation

    zones of NiTi sample under local canning compression consist of

    the principal deformation zone, the intermediate deformation zone

    and the minimum deformation zone. It can be found that inho-

    mogeneous plastic deformation leads to the different microstruc-

    tural morphologies in NiTi sample subjected to SPD. TEM bright-

    eld image of NiTi sample in the principal deformation zone is

    indicative of the presence of an almost complete amorphous phase,

    in which the retained nanocrystalline phase is embedded in the

    amorphous matrix, as shown inFig. 1(b). However, the amorphous

    bands and the deformation bands occur in the plastic deformation

    zones other than the principal deformation zone, as shown in

    Fig. 1(c) and (d), respectively.

    3.2. Nanocrystallization of amorphous NiTi sample subjected to

    annealing

    Figs. 2 and 3 demonstrate TEM photographs of NiTi samples

    subjected to SPD after annealing for 2 h at 300C and 450 C,

    respectively. NiTi samples subjected to SPD before annealingbelong to an almost complete amorphous phase, in which a small

    amount of nanocrystalline phase is embedded in the amorphous

    matrix. It can be seen fromFigs. 2 and 3 that annealing at 300 C

    and 450C for 2 h leads to nanocrystallization of amorphous NiTi

    samples. Furthermore, the nanocrystalline grain size increases

    with the increase in the annealing temperature. The size distri-

    bution of the nanocrystalline grains was measured by means of

    extra TEM bright and dark images, in which the diameter of the

    nanocrystalline grain in the selected area can be obtained by

    combining DigitalMicrograph software with equal perimeter

    method. The mean grain size in the diameter can be calculated

    according to the selected 200 grains. In the case of annealing at

    300 C, the mean grain size is about 12 nm in the diameter, but in

    the case of annealing at 450C, the mean grain size is about50 nm in the diameter.

    3.3. Twinning of amorphous NiTi samples subjected to annealing

    Fig. 4 indicates microstructural morphologies of NiTi sample

    subjected to SPD after annealing at 600 C for 2 h. It can be found

    from Fig. 4 that NiTi sample subjected to SPD is completely

    crystallized after annealing at 600C for 2 h and is characterized by

    the coarsegrains rather than the nonacrystalline grains. In addition,

    there exist plenty of annealing twins in the coarse-grained NiTi

    sample. The corresponding selected area electron diffraction

    patterns (SAEDPs) reveal that the annealing twins belong to (001)

    martensite compound twins.

    3.4. Microstructural evolution of amorphous bands after annealing

    There exist a lot of amorphousbands in NiTi sample subjectedto

    SPD.Fig. 5illustrates microstructural evolution of the amorphous

    bands after annealing for 2 h at 300 C and 450C, respectively. It

    can be seen fromFig. 5that a lot of nanocrystalline grains arise in

    the amorphous bands of NiTi sample subjected to SPD. In terms of

    annealing at 300 C, the dislocation defects remain between the

    amorphous bands since thermal driving force is insufcient to

    eliminate them. However, the amorphous bands in NiTi sample

    after annealing at 600C for 2 h is unable to be found.

    3.5. Microstructural evolution of deformation bands after annealing

    There exist a lot of deformation bands in NiTi sample subjected

    to SPD due to inhomogeneous plastic deformation under local

    canning compression. The deformation bands are attributed to

    a consequence of dislocation slip. Fig. 6 indicates that the micro-

    structures of the deformation bands in NiTi sample subjected to

    SPD after annealing at 300 C and 450C, respectively. It can be

    seen from Fig. 6 that annealing at the twotemperatures is unable to

    lead to complete elimination of the deformation bands and a lot of

    ne precipitation phases occur in the deformation bands after

    annealing. Furthermore, as compared to annealing at 450C, the

    deformation bands of NiTi sample in the case of annealing at 300C

    are more apparent since thermal driving force is more insufcient.

    However, the deformation bands in NiTi sample after annealing at

    600 C for 2 h have been completely eliminated by means of

    thermal driving force.

    3.6. XRD curves of annealed NiTi samples

    Fig. 7 indicates XRD curves of NiTi samples subjected to SPD

    after annealing at 300 C, 450 and 600 C, respectively. NiTi

    sample annealed at 300 C is mainly composed of B2 austenite

    phase with a small amount of Ni4Ti3 precipitationphase. In the case

    of annealing at 450C, NiTi sample consists of B2 austenite phase,

    Fig. 2. TEM photographs of NiTi sample subjected to SPD after annealing at 300

    C. (a) Bright-

    eld image; and (b) dark-

    eld image.

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    samples for DSC test are located in the principal deformation zone

    and thus are obtained by means of crystallization of the amorphousNiTi phase. It can be found fromFig. 8that NiTi sample annealed at

    300 C shows no phase transformation, while NiTi samples

    annealed at 450C and 600 C exhibit martensitic phase trans-

    formation. Furthermore, as compared to as-received NiTi sample,

    martensitic phase transformation temperatures are enhanced for

    NiTi samples subjected to SPD as well as subsequent annealing.

    4. Discussion

    Inhomogeneous plastic deformation is unavoidable during SPD of

    NiTi alloy under local canning compression at room temperature. An

    almost complete amorphous matrix with a small amount of nano-

    crystalline phase occurs in the principal deformation zone of NiTi

    sample. In the plastic deformation zones other than the principaldeformation zone, there exist a lot of deformation bands in which

    there are plenty of crystal defects, such as dislocations, stacking

    faults, and twins. At the low annealing temperatures of 300 C and

    450C, some crystal defects can be eliminated by means of static

    recovery, but the deformation bands are unable to be removed

    completely due to insufcient thermal driving force. In the case of

    annealing at 600C, the occurrence of static recrysallization leads to

    complete elimination of the deformation bands. However, the

    amorphous NiTi sample caused by SPD belongs to the metastablephase and possesses the low thermal stability[16]. For example, the

    fully amorphous NiTi sample after being subjected to high-pressure

    torsion (HPT) exhibits partial nanocrystallization along with the

    extremely small grains of 10e20 nm even at room temperature,

    while the complete nanocrystallization with homogeneous nano-

    crystalline structure of 20e30 nm is performed in the case of

    annealing at 200 C for 2 h[13]. In the present study, the complete

    crystallization of the amorphous NiTi sample is obtained by

    annealing for 2 h at 300 C, 450C and 600 C, respectively, while

    the grain size increases with the increase in the annealing temper-

    ature. In particular, the complete nanocrystallization is obtained in

    the case of annealing at 300 C and 450C, respectively. Physical

    mechanism of crystallization with respect to the amorphous NiTi

    sample obtained by SPD can be outlined as nucleation and growth ofthe grains in the amorphous matrix, in which the retained nano-

    crystalline debriscanrstly act as the heterogeneous nucleation sites

    [16]. The nucleation rate and the growth rate during crystallization

    play the critical roles in determining the nal grain size. In general,

    the fast nucleation rate and the slow growth rate contribute to

    obtaining the ne grains. In the present work, the annealing

    temperature is considered as the only variable. Therefore, the grain

    Fig. 5. TEM photographs of amorphous bands in NiTi samples subjected to SPD after annealing at different temperatures: (a) 300 C; and (b) 450 C.

    Fig. 6. TEM photographs of deformation bands in NiTi samples subjected to SPD after annealing at different temperatures: (a) 300

    C; and (b) 450

    C.

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    size after crystallization depends on the growth rate of the grains,

    while the elevated annealing temperature leads to increasing the

    growth rate and thus results in the occurrence of the coarser grains.

    As a result, in the case of annealing at 600 C, the faster growth rate

    leads to rapid growth of the grains in a certain time, so the coarse-

    grained NiTi sample occurs.

    Furthermore, annealing has an inuence on not only micro-

    structural evolution, but also precipitation process of NiTi sample

    subjected to SPD. It can be seen from XRD curves in Fig. 7 that

    annealingat 300C leads toonly Ni4Ti3 precipitate and annealing at

    600 C leads to only Ni3Ti precipitate, while Ni4Ti3precipitate and

    Ni3Ti precipitate coexist in the case of annealing at 450C. It can be

    Fig. 7. XRD curves of NiTi samples subjected to SPD after annealing at different temperatures: (a) 300 C; (b) 450 C; and (c) 600 C.

    Fig. 8. DSC curves of NiTi samples subjected to SPD after annealing at different temperatures: (a) 300

    C; (b) 450

    C; and (c) 600

    C.

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    found that SPD results in the occurrence of Ni 3Ti precipitate at the

    lower temperature and leads to the decrease of the highest

    temperature at which Ni4Ti3 precipitate occurs. In general, there are

    three precipitation phases including Ni4Ti3, Ni3Ti2and Ni3Ti in Ni-

    rich NiTi SMA after annealing, which depends on annealing

    temperature and annealing time. Ni4Ti3 phase occurs at the lower

    annealing temperature and the shorter annealing time, and Ni3Ti

    phase arises at the higher annealing temperature and the longer

    annealing time, while Ni3Ti2 phase appears at intermediate

    annealing temperature and time [1]. Therefore, both Ni4Ti3 and

    Ni3Ti2 are the metastable phases, while Ni3Ti is the equilibrium

    phase. In the present work, no Ni3Ti2 phase is found at the three

    annealing temperatures. In addition, TEM observations reveal that

    no precipitation phases are found in NiTi specimens derived from

    crystallization of amorphous phase. Accordingly, the precipitation

    phases occur in the deformation bands of NiTi sample after

    annealing. The grain size seems to have a considerable effect on

    nucleation and growth of Ni4Ti3 precipitate. For instance, Ni4Ti3precipitate shall be suppressed in the nanocrystalline NiTi sample

    obtained by crystallization of the amorphous phase after HPT[20].

    Therefore, in the present study, annealing at 300 C and 450C

    leads to nanocrystallization of amorphous NiTi sample and conse-

    quently the precipitation phases shall be suppressed since thenanocrystalline grains impede the formation of the self-

    accommodation. However, no precipitation phases are found in

    the coarse-grained NiTi sample formed as a result of crystallization

    of the amorphousstructure by means of annealing at 600C, which

    shall be further investigated in the future work.

    It can be seen from the previous experimental results that the

    grain size has a considerable inuence on martensitic phase

    transformation of NiTi sample. Annealing at 300 C leads to the

    nanocrystalline NiTi sample with the smallest mean grain size of

    about 12 nm, where martensitic phase transformation is

    completely suppressed. Annealing at 450C results in further

    increase of the grain size of the nanocrystalline NiTi sample, where

    the mean grain size is about 50 nm, while the largest grain size is

    about 90 nm. Therefore, in the nanocrystalline NiTi sample ob-tained in the case of annealing at 450 C, martensitic phase trans-

    formation takes place in the largernanocrystalline grains, butis still

    suppressed in the smaller nanocrystalline grains. However,

    annealing at 600C leads to the coarse-grained NiTi sample of

    which the grain size is greater than 200 nm. Martensitic phase

    transformation occurs more easily in the coarser grains. Accord-

    ingly, it can be concluded that martensitic phase transformation is

    suppressed with the decrease in the nanocrystalline grain size.

    Similar conclusions were reported in the nanocrystalline NiTi

    sample derived from crystallization of the amorphous structure in

    the case of HPT and subsequent annealing [16]. Suppression of

    martensitic phase transformation in the nanocrystalline NiTi

    sample is possible to be attributed to the presence of elastic strains,

    lattice defects or crystal renement[7,16]. In the present study, theelastic strains and the lattice defects shall be almost eliminated in

    the nanocrystalline NiTi sample resulting from crystallization of the

    amorphous phase in the case of annealing, so grain renement as

    well as the corresponding constraint by the grain boundaries plays

    an important role in suppressing martensitic phase transformation

    based on self-accommodation of the martensitic variants. As

    compared to the nanocrystalline NiTi sample, martensite is able to

    nucleate at the dislocation tangles and near the grain boundaries in

    the coarse-grained NiTi sample, which contributes to the occur-

    rence of martensitic phase transformation.

    Furthermore, the (001) compound twins are observed during

    transformation of B2 austenite to B190 martensite in the coarse-

    grained NiTi sample formed as a consequence of annealing at

    600

    C. It is well known that f111gtype I twin, h011i type II twin

    and (001) compound twin are frequently found in martensitic

    phase transformation of NiTi alloy in the case of heat treatment.

    f111g type I twin and h011i type II twin comply with the

    phenomenological crystallographic theory and thus belong to

    a lattice invariant shear[21e23]. However, (001) compound twin

    does not give a solution to the phenomenological crystallographic

    theory and cannot be a lattice invariant shear, so it is recognized as

    a deformation twin[24e26]. In the present study, the other two

    twin modes except the (001) compound twin are not found. Only

    (001) compound twins are observed in the nanocrystalline NiTi

    sample formed as a result of crystallization of the amorphous

    structure by HPT and subsequent annealing[16,17]. It is proposed

    that in NiTi sample obtained by crystallization of the amorphous

    phase, the (001) compound twin occurs more frequently instead of

    f111gtype I twin and h011i type II twin. The lattice distortion along

    with the dislocation defects frequently occurs in NiTi sample with

    the coarse grains derived from crystallization of the amorphous

    phase and thus contributes to the occurrence of the (001)

    martensite compound twins. In particular, the formation of the

    twins should be more susceptible to taking place at the grain

    boundaries.

    5. Conclusions

    (1) SPDof NiTi samplebased on local canning compressionleads to

    the complicated microstructural morphologies, including

    deformation bands, amorphous bands and amorphous phase in

    which the retained nanocrystalline phase is embedded in the

    amorphous matrix.

    (2) Annealing at 300 C and 450 C leads to nanocrystallization of

    amorphous NiTi sample, but is unable to result in complete

    elimination of deformation bands and amorphous bands.

    Annealing at 600 C results in complete crystallization of NiTi

    sample subjected to SPD, where deformation bands and

    amorphous bands are not able to be detected. The (001)

    compound twins are found during transformation of B2

    austenite to B190 martensite in the coarse-grained NiTi sampleformed as a consequence of annealing at 600 C.

    (3) The precipitation phases are suppressed in NiTi sample formed

    as a result of crystallization of amorphous structure in the case

    of annealing at 300 C, 450 C and 600 C, respectively. The

    precipitation phases occur more easily in the deformation

    bands of NiTi sample after annealing. SPD results in the

    occurrence of Ni3Ti precipitate at the lower temperature and

    leads to the decrease of the highest temperature at which

    Ni4Ti3precipitate occurs.

    (4) The grain size has a considerable inuence on martensitic

    phase transformation of NiTi sample. Grain renement plays an

    important role in suppressing martensitic phase trans-

    formation. Martensitic phase transformation is suppressed

    with the decrease in the nanocrystalline grain size.

    Acknowledgements

    The work was nancially supported by National Natural Science

    Foundation of China (No. 51071056) and the Fundamental Research

    Funds for the Central Universities of China (No. HEUCFR1132 and

    No. HEUCF121712).

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