The demand for compact, efficient and high performance electronic devices and sensor systems has become one of the primary driving force for rapid advancement in miniaturization of current technology. However, the attempt to push the limits of component length scales into the nano regime is being challenged by possibly unconventional laws of physics. One of the key design parameters for good performance of any system is its structural stability, defined by the strength of a material. The strength of a material is defined as its resistance to plastic (or permanent) deformation. In conventional metals plastic deformation is carried by the migration of lattice defects such as vacancies and dislocations. The barriers to the motion of these defects provide strength to metals, leading to an inverse power law scaling with inter barrier spacing, l  = Bl q where represents the nominal strength, B is a measure for strengthening capability of barriers and q represents the order of strengthening. The well known Hall Petch relation (q=0.5) expresses this effect for grain boundary strengthening, where grain boundaries (GBs) obstruct motion of dislocations during plastic deformation. Extensive research over past few decades has shown that grain size strengthening may be limited by GB mediated deformation processes in nanocrsytalline (nc) metals with grain sizes of ≤ 20 nm. The strength of nanocrsytalline metals saturates, or in some cases decreases, with a reduction in grain size. Molecular dynamic simulations have provided some indication of atomic scale activities that dominate deformation in nc metals. Although it is difficult to experimentally monitor the atomistic processes, in situ mechanical tests in synchrotron facilities have captured some mesoscopic features of deformation in nanocrsytalline metals. For instance, experiments have shown that the typically extended elastic plastic transition during deformation of nanocrsytalline metals could be classified into two regimes. For initial stages of deformation, in the microplastic regime, the width of various diffracting peaks decreases suggesting the dominance of processes leading to structural relaxation. However, at later stages of deformation, in a manner similar to conventional metals, the diffraction peak widths increased signifying the increasing importance of deformation processes that involve an accumulation of defects. It is well known that thermal annealing also causes relaxation of materials and during high temperature deformation continuous relaxation of stress concentrations could retard premature failure of metals. As the ductility in nanocrsytalline metals is limited to 3-5%, with very limited strain hardening, the processes of structural relaxation are very important. Thus, there is a fundamental need to understand the nature of structural relaxation during microplastic deformation in nanocrystals. It is well known that character of grain boundaries plays an important role in material properties. As the grain boundary area per unit volume varies inversely with grain size, nanocrsytalline metals contain a significant amount of grain boundary area. Moreover, due to small grain sizes, conventional Frank Read sources cannot operate for nucleating dislocations. Dislocations in nc metals are nucleated from GBs, traverse grains and gets absorbed in other GBs. The small volume of grains further restricts dislocation interactions. Thus, dislocation nucleation, propagation and absorption become possible rate controlling mechanisms in nc metals. Molecular dynamic simulations of nanocrsytalline and bicrystalline samples have shown that grain boundary structure could significantly affect these mechanisms. Simulations have shown further that apart from dislocation plasticity other grain boundary mediated process like GB sliding and GB diffusion become important with decreasing grain size. These processes are also influenced by GB character. Thus, it is important to understand the role of GB character in deformation of nc metals. On one hand where the structural need for high strength has encouraged reduction of internal microstructural length scales, miniaturization has also encouraged reduction in external length scale of device components. In modern electronic and sensor devices a typical component size varies from a few hundred microns to few tens of nanometer. Several studies have shown that free surfaces could reduce the constraints on deforming grains. With decreasing sample dimensions, the free surface to volume ratio increases and the internal microstructural length scale may become comparable to the external sample size. An increasing contribution from these two geometrical parameters can introduce external size effects in mechanical properties of materials. In the past, most of the external size effects have been attributed to strain gradient plasticity and deformation source starvation. However, a different external size effect has been observed during uniaxial test of polycrystalline metals where the strength of materials was found to deviate from their bulk values at smaller sample sizes. While most studies have shown a weakening effect, there have also been a few observations of strengthening with a reduction in sample size. In most studies, the external sample size was kept constant and the internal grain size was varied by thermal annealing to produce samples with different external to internal size ratios. As the mechanical properties of metals are sensitive to the internal length scales it is difficult to explicitly follow the external size effect during these experiments. Moreover, compared to internal size effects mechanistic understanding of external size effect is limited, and systematic experimental efforts are required for proper characterization of these effects. The present investigation was undertaken to improve the scientific understanding of internal and external length effects on mechanical properties of nanocrystalline and coarse grained (~16 – 140 µm) polycrystalline nickel. For studying the internal size effects free standing nanocrystalline nickel samples with ~30 nm grain size and two different textures were synthesized using galvanostatic pulsed electrodeposition technique from Watts and Sulfamate baths. The nanocrsytalline deposits from a Watts bath showed a strong <100> fiber texture (NiS) while deposits from a Sulfamate bath were relatively weak textured (NiW), with s and w representing strong and weak texture, respectively. In situ mechanical tests at the PSI synchrotron facility in Switzerland were used to understand the nature of relaxation processes during thermal annealing and deformation of nc metals. The diffraction peak analysis showed that thermal annealing at 423 K of strong textured deposits caused a significant reduction in root mean square strain with limited grain growth. Furthermore, no residual strains developed, suggesting a homogenous distribution of relaxation processes during thermal annealing. In contrast, during deformation, structural relaxation was highly biased due to dislocation activities. The grains contributing to <200> diffraction peak transverse to loading axis showed early yielding and faster relaxation during deformation. The inhomogeneous nature of deformation was also reflected in development of transverse tensile residual stresses in the <200> grains. These experiments showed that relaxation processes during thermal annealing and deformation differ in their respective length scales. Nanocrsytalline deposits with two different textures were also deformed under synchrotron to access the role of GB character. As direct quantification of GB character distribution is difficult in nc metals, texture was taken as a qualitative representative for GB character. Previous studies have shown that the fraction of low angle boundaries increases with increasing sharpness of texture in fiber textured materials. Thus, the two textured deposits represented materials with two different low angle GB fractions. In situ tests showed that during the initial stages of microplastic deformation dislocation mechanisms were favored in strongly textured NiS. The transversely oriented <200> grains showed early yielding, which caused a redistribution of stress among other grain families. However, for weakly textured NiW deposits, smaller length scale atomic activities preceded dislocation activities. All the grains supported larger elastic strains at lower stresses suggesting significant plastic activity at GB regions. At higher stresses transversely oriented <220> grains yielded plastically and transferred elastic loads to <200> grains. Thus, the nature of plastic deformation was observed to depend on the distribution of GB character. For understanding the external size effects on mechanical properties polycrystalline nickel samples with grain sizes of 16, 51 and 140 µm were tested uniaxially at various sample thicknesses. Three different deformation regimes were identified based on the thickness of the samples. At higher thicknesses, in regime I, no significant variation of flow strength was observed. Flow strengths in regime II, at intermediate thicknesses, showed a strengthening effect with a reduction in thickness. However at lower thicknesses in regime III, a weakening trend was observed with decreasing thickness. The cross over from strengthening to weakening was observed to depend on grain size and applied strain. Detailed microstructural analysis with electron back scattered diffraction (EBSD) imaging showed that intragranular lattice rotation increases with a reduction in sample thickness. As lattice rotations may be considered to be accommodated by geometrically necessary dislocations, a semi empirical phenomenological model based on strain gradient plasticity was developed to understand the mechanics of external size effect during uniaxial test of polycrystalline samples. Further application of the model to the present experimental results showed that the characteristic length for strain gradient decreased with increasing grain size and applied strain.

Commercially available polycrystalline Ni (Ni200; grain size: 32 μm) and electrodeposited nanocrystalline Ni (grain size: 57 nm), Ni-2.6%Fe (grain size: 25 nm) and Ni-8.5%Fe (grain size: 20 nm) were analyzed for the phenomena of stress-induced heat generation and strain localization during plastic deformation at room temperature (i.e. 250C). Tensile specimens according to ASTM E8 standard dimensions were tested at strain rates of 10-2/s and 10-1/s, respectively, to record the amount of heat dissipated and the change of localized strain using a high resolution infrared (IR) detector and digital image correlation (DIC) camera, respectively. Results have shown that the maximum temperatures that were recorded in nanocrystalline Ni and Ni-Fe alloys were at least 300C lower than the onset temperatures for subgrain coalescence previously measured through differential scanning calorimetry. It can be concluded that thermally activated grain growth during tensile testing of nanocrystalline Ni and Ni-Fe alloys is not likely to occur.

Commercially available polycrystalline Ni (Ni200; grain size: 32 μm) and electrodeposited nanocrystalline Ni (grain size: 57 nm), Ni-2.6%Fe (grain size: 25 nm) and Ni-8.5%Fe (grain size: 20 nm) were analyzed for the phenomena of stress-induced heat generation and strain localization during plastic deformation at room temperature (i.e. 250C). Tensile specimens according to ASTM E8 standard dimensions were tested at strain rates of 10-2/s and 10-1/s, respectively, to record the amount of heat dissipated and the change of localized strain using a high resolution infrared (IR) detector and digital image correlation (DIC) camera, respectively. Results have shown that the maximum temperatures that were recorded in nanocrystalline Ni and Ni-Fe alloys were at least 300C lower than the onset temperatures for subgrain coalescence previously measured through differential scanning calorimetry. It can be concluded that thermally activated grain growth during tensile testing of nanocrystalline Ni and Ni-Fe alloys is not likely to occur.

Les alliages à base Nickel polycristallins sont largement utilisés pour les pièces aéronautiques soumises à des sollicitations extrêmes en service. Des objectifs toujours plus ambitieux en termes de rendement énergétique des moteurs d’avions ont conduit les constructeurs à augmenter leur température de fonctionnement. Les nuances utilisées jusqu’alors dans les parties chaudes, tels que l’Inconel 718, n’ont pas une tenue mécanique suffisante à ces températures. Le René 65 est un nouvel alliage à microstructure γ-γ’ élaboré spécifiquement pour ces applications. Il a été retenu par Safran Aircraft Engines comme constituant des disques de turbine basse pression du nouveau turboréacteur LEAP. Pour garantir la bonne tenue des disques, une microstructure fine et homogène est requise. Le procédé de forgeage de ces pièces est une séquence d’étapes de déformation à chaud et de traitements thermiques, durant lesquelles la microstructure évolue. Si les phénomènes physiques gouvernant les évolutions microstructurales sont connus, leurs mécanismes exacts et leurs cinétiques varient d’un alliage à l’autre.Des essais de déformation à chaud ont été réalisés en laboratoire dans différentes conditions de température, vitesse et taux de déformation représentatifs des procédés industriels. L’étude précise des mécanismes de recristallisation dynamique, ainsi que de leurs cinétiques, constitue la première partie de ce travail. La caractérisation fine des microstructures déformées a permis de mettre en évidence un nouveau mécanisme de recristallisation, dit de recristallisation en hétéroépitaxie, qui se superpose aux autres mécanismes conventionnels. L’interaction entre ces différents mécanismes ainsi que leurs cinétiques relatives ont été établies dans une vaste gamme de conditions de déformation. Il est démontré que ce mécanisme de recristallisation s'applique également à d'autres alliages γ-γ’. La deuxième partie de l’étude est consacrée à la stabilité des microstructures déformées lors de leur exposition à haute température. L'alliage René 65, comme d’autres alliages à base Nickel, est sensible à un phénomène indésirable dit de croissance sélective de grains. Ses conditions de déclenchement ont été déterminées, de manière à délimiter une fenêtre de forgeage critique. Les mécanismes microstructuraux à l’origine de ce phénomène ont été discutés, ainsi que la possibilité d’une solution préventive. / Polycrystalline Nickel-based alloys are widely used as components for rotative parts of jet engines submitted to extreme conditions. Endlessly increasing objectives in terms of energy efficiency have led the engine manufacturers to increase their service temperature. As a consequence, Inconel 718 and similar alloys -that were used until now- cannot withstand such severe conditions anymore, and lack mechanical resistance at the increased temperature. René 65 is a new γ-γ’ superalloy which has been designed specifically for that purpose by General Electric. It has been selected by Safran Aircraft Engines as the material for low-pressure turbine disks in the new LEAP engine. To reach the desired mechanical properties, a fine and homogeneous microstructure is required. The forging process is a complex sequence which involves various hot deformation stages and thermal treatments, during which the microstructure evolves. Although the underlying mechanisms governing the microstructure evolutions are quite known, their specific mechanism and kinetics may vary depending on the alloy.Interrupted compression tests were conducted at laboratory scale under thermomechanical conditions (temperature, strain and strain rate) in accordance with the industrial process. In the first part, the focus is placed on the dynamic recrystallization mechanisms. Accurate characterization of the deformed microstructures has enabled to highlight a new recrystallization mechanism which superimposes with more conventional ones. It was named heteroepitaxial recrystallization. The interactions between those mechanisms as well as their relative kinetics have been established in a wide range of deformation conditions. . It is demonstrated that this mechanism occurs in other γ-γ’ Nickel-based alloys. The second part of the study is dedicated to the stability of deformed microstructures when exposed to high temperature thermal treatments. René 65, as many other Nickel-based alloys, is subjected to the undesirable phenomenon of selective grain growth, which leads to very heterogeneous microstructures containing abnormally large grains in a fine matrix. Critical deformation conditions leading to heterogeneous microstructures during subsequent annealing have been determined in an aim to identify the critical forging window which should be avoided. The microstructural mechanisms responsible of this phenomenon have been investigated, and the possibility of a preventive solution is discussed.

Les microfils métalliques polycristallins produits par étirage à froid présentent une résistance mécanique significative en faisant des candidats idéaux pour les renforts de composites. Des études antérieures sur des fils de nickel polycristallin pur ont montré une dépendance importante par rapport à la taille de la limite d'élasticité et de la résistance à la traction, ainsi que de la ductilité.Le but de cette étude est de comprendre cet effet de la taille dans les microfils de nickel pur polycristallin par analyse de diffraction des rayons X in-situ (DRX) et simulations de la plasticité cristalline par éléments finis (CPFE). Des essais de traction monotone et cyclique in-situ sous rayonnement synchrotron ont été réalisés sur des microfils de diamètres allant de 100 à 40 μm. Les fils étirés à 100 micromètres obtenus dans le commerce présentent une architecture cœur-coquille avec une texture de fibre <111> dominante dans le cœur et une texture à double fibre hétérogène <111> et <100> dans la coquille. La réduction de la taille de l'échantillon par polissage électrolytique conduit à des fils ayant une microstructure homogène, tandis que la réduction de la taille de l'échantillon par un étirage à froid supplémentaire conduit à des fils avec une texture plus intense tout en conservant l'architecture cœur-coquille.La limite d'élasticité et la résistance à la traction des fils électropolis augmentent avec la diminution du diamètre, tandis que la ductilité diminue avec la réduction du diamètre. Dans le cas des fils étirés à froid, on observe que la limite d'élasticité et la résistance à la traction, ainsi que la ductilité, augmentent avec la diminution du diamètre. L'analyse DRX indique une plasticité successive des familles de grains sous iso-déformation. Nous avons observé que le gradient de la texture du microfil active des mécanismes de déformation qui ne sont pas observés pour les microfils à texture homogène. Pour comprendre l'influence de différents paramètres microstructuraux, notamment l'influence de la texture cristallographique, une microstructure représentative 3D a été générée et des simulations CPFE ont été réalisées. Le comportement simulé moyen des différentes familles de grains (<111>, <100>) concorde bien avec les résultats expérimentaux. La simulation CPFE indique une hétérogénéité du champ de contrainte à travers la microstructure en présence d'un gradient de texture cristallographique.Nous montrons que la micro-texture (texture simple ou double texture) et leur dispersion spatiale (homogène ou architecturée) peuvent être utilisées comme stratégie de conception pour obtenir une microstructure optimale en fonction de l’ensemble désiré de propriétés mécaniques. / Polycrystalline metallic microwires produced by cold-drawing exhibit significant mechanical strength that make them ideal candidates for reinforcement of composites. Previous studies on polycrystalline pure nickel wires have indicated a significant size dependence of their yield and tensile strength as well as their ductility. The aim of this study is to understand these size effects by in-situ X-ray diffraction (XRD) analysis and crystal plasticity finite element (CPFE) simulations. In-situ monotonous and cyclic tensile tests under synchrotron radiation were carried on microwires with diameters ranging from 100 to 40 µm. The commercially obtained 100µm as-drawn wires exhibit a core-shell architecture with <111> fiber texture dominant in core and heterogeneous dual fiber texture <111> and <100> in the shell. Reduction of specimen size by electropolishing leads to wires having a homogeneous microstructure, whereas reduction of specimen size by further cold drawing leads to wires with a sharper texture while retaining the core-shell architecture.The yield and tensile strength of the electropolished wires increase with decreasing diameter, whereas the ductility decrease with decreasing diameter. In the case of cold-drawn wires, the yield and tensile strength, and also the ductility was observed to increase with decreasing diameter. The XRD analysis indicates successive yielding of grain families under iso-strain condition. The gradient in the texture of the microwire was seen to activate deformation mechanisms which are not seen for microwires with homogeneous texture. To understand the influence of different microstructural parameters, and notably the influence of crystallographic texture, 3D representative microstructure was generated and CPFE simulations were carried out. The simulated average behavior of different grain families (<111>, <100>) agrees well with the experimental results. The CPFE simulations indicate heterogeneity in stress field across the microstructure in the presence of a gradient in crystallographic texture.We show that the microstructure engineering of micro-texture components (single- or dual-texture) and their spatial spread (homogenous or architectured) can be used as design guidelines for obtaining optimal microstructure in accordance with desired set of mechanical properties.

L'objectif de cette thèse est de mettre en évidence l'influence de la microstructure initiale sur le glissement intergranulaire lors du fluage à haute température d'un superalliage polycristallin à base de nickel. Dans ce but, plusieurs microstructures sont obtenues à partir de la microstructure de référence de l'alliage NR6, par application de traitements thermiques spécifiques. L'influence des paramètres microstructuraux sur les déformations locales est ensuite étudiée à l'aide d'une technique de microextensométrie couplée à une analyse par diffraction des électrons rétrodiffusés. Il est ainsi possible de relier microstructure, déformations locales et comportement macroscopique en fluage. Pour la microstructure de référence de l'alliage NR6, la déformation opère principalement par cisaillement des phases γ et γ'. Ce mécanisme est favorable au glissement intergranulaire. L'absence de précipités tertiaires de phase γ' favorise le contournement des précipités secondaires par les dislocations. Ceci permet de réduire le glissement intergranulaire mais est également néfaste pour la résistance à la déformation de l'alliage. La présence de joints de grains dentelés augmente la résistance au glissement intergranulaire mais diminue la résistance à la déformation intragranulaire en favorisant le contournement des précipités. Ainsi la résistance globale à la déformation n'est pas affectée. Enfin, l'augmentation de la taille de grains n'a d'influence ni sur les mécanismes de déformation mis en jeu ni sur l'amplitude du glissement. Cependant, la fraction moins élevée de joints de grains induit une diminution de la contribution du glissement intergranulaire à la déformation globale. / The aim of this study is to highlight the influence of initial microstructure on grain boundary sliding during high-temperature creep of a polycrystalline nickel-based superalloy. To reach this goal, several microstructures are produced from the reference microstructure of NR6 alloy by adequate heat treatments. The influence of microstructural parameters on local deformations is then studied thanks to a microextensometry technique coupled with an electron back-scattered diffraction analysis. It thereby enables linking microstructure, local deformations and macroscopic creep behaviour. In the case of NR6 alloy reference microstructure, deformation occurs mainly by γ and γ' phases cutting by dislocations. This mechanism is grain boundary sliding-favourable. The absence of tertiary γ' phase precipitates promotes secondary precipitates bypassing by dislocations. This results in a reduction of grain boundary sliding but is also harmful to the alloy creep resistance. Grain boundary serration improves grain boundary sliding resistance but diminishes intragranular deformation resistance by favouring precipitate bypassing. Then global deformation resistance is not changed. Finally, grain size increase has influence neither on activated deformation mechanisms nor on sliding amplitude. However, the decrease of grain boundary fraction leads to a reduction of grain boundary sliding contribution to overall strain.

Plastic deformation of metals and alloys are invariably accompanied by the development of texture. The origin of texture is attributed to the deformation micro-mechanisms associated with processing. The face-centered cubic (FCC) metals and alloys are known to exhibit two distinct types of textures when subjected to large strain rolling deformation, namely, (i) Cu-type texture, commonly seen in high/medium stacking fault energy (SFE) materials, (ii) Bs-type texture in low SFE materials. The circumstances that could result in the formation of Bs-type texture in low SFE materials still remains an open question and no definite mechanism has been uniquely agreed upon. Apart from the SFE, grain size could also influence the deformation mechanism and hence the deformation texture. It is well known that in materials with grain sizes less than 100 nm (referred to as nano-crystalline materials), the microstructures contain large fraction of grain boundaries. This subsequently introduces a variety of deformation mechanisms in the microstructure involving grain boundary-mediated processes such as grain boundary sliding and grain rotation, in addition to slip and twinning. A clear understanding of texture evolution in nano-crystalline materials, particularly at large strains, is a topic that remains largely unexplored. The present work is an attempt to address the aforementioned issues pertaining to the evolution of deformation texture, namely, (i) the effect of SFE and (ii) the effect of grain size, in FCC metals and alloys. Nickel-cobalt alloys are chosen as the model system for the present investigation. The addition of cobalt to nickel leads to a systematic reduction of SFE as a function of cobalt content. In this thesis, three alloys of Ni-Co system have been considered, namely, nickel – 20 wt.% cobalt, nickel – 40 wt.% cobalt and nickel – 60 wt.% cobalt. For a comparison, pure nickel has also been subjected to similar study. Chapter 1 of the thesis presents a detailed survey of literature pertaining to the evolution of rolling textures in FCC metals and alloys, and chapter 2 includes the details of the experimental techniques and characterization procedures, which are commonly employed for the entire work. Chapter 3 addresses the effect of stacking fault energy on the evolution of rolling texture. The materials subjected to study in this chapter are microcrystalline Ni-Co alloys. The texture evolution in Ni-20Co is very similar to pure Ni, and a characteristic Cu-type rolling texture is observed. The evolution of texture in these materials is primarily attributed to the intense dislocation activity throughout the deformation stages. In Ni-40Co, a medium SFE material, the rolling texture was predominantly Cu-type up to a strain of ε = 3 (95% thickness reduction). However, beyond this strain level, namely at ε = 4 (98%), the texture gets transformed to Bs-type with orientations maxima predominantly close to Goss ({110} <001>) position. Simultaneously, the Cu component which was dominant until 95% reduction has completely disappeared. The analysis of microstructures indicate that deformation is mostly accommodated by dislocation slip up to 95%, however, at ε > 3, Cu-type shear bands get initiated, preferably in the Cu-oriented ({112} <111>) grains. The sub-grains within the shear bands show preferred orientation towards Goss, which indicates that the Cu component should have undergone transformation and resulted in high fraction of Goss component. In Ni-60Co alloy, Bs-type texture forms in the early stages of deformation (ε ~ 0.5) itself and further deformation results in strengthening of the texture with an important difference that the maximum in orientation distribution has been observed at a location close to Goss component, rather than at exact Bs-location. The development of Bs-type texture is accompanied by the complete absence of Cu and S components. Extensive EBSD analyses show that the deformation twinning gets initiated beyond 10% reduction and was found extensively in most of the grains up to 50% reduction. At higher strains, tendency for twinning ceases and extensive shear banding is observed. A non-random distribution of orientations close to Goss orientation was found within the shear bands. The near-Goss component in the Ni-60Co alloy can be explained on the basis of deformation twinning and shear banding. Thus, a reasonable understanding of the deformation texture transition in the extreme SFE range has been developed. In chapter 4, the effect of fine grain size on the evolution of rolling texture has been addressed. Nanocrystalline (nc) nickel-cobalt alloys with a mean grain size of ~20 nm have been prepared by pulse electro-deposition method. For a comparison, nc Nickel (without cobalt) with similar grain size has also been deposited. For all the materials, a weakening of the initial fiber texture is observed in the early stage of room temperature rolling (ε ~ 0.22). A combination of equiaxed grain microstructure and texture weakening suggests grain boundary sliding as an operative mechanism in the early stage of rolling. At large strain (ε = 1.2), Ni-20Co develops a Cu-type texture with high fractions of S and Cu components, similar to pure Ni. The texture evolution in Ni-40Co and Ni-60Co alloys is more towards Bs-type. However, the texture maximum occurs at a location 10° away from the Goss. The evolution of Cu and S components in nc Ni-60Co alloy takes place simultaneously along with the α-fiber components during rolling. Microstructural investigation by TEM indicates deformation twinning to be more active in all the materials up to 40% reduction. However, no correlation could be drawn between the texture evolution and the density of twins. The deformation of nc Ni-20Co alloy, is also accompanied by significant grain growth at all the stages of rolling. The increase in grain size, subsequently, renders the texture to be of Cu-type. However, Ni-40Co and Ni-60Co alloys show high grain stability. The absence of strain heterogeneities such as shear bands, and the lack of significant fraction of deformation twins indicate that the observed Bs-type texture could be due to planar slip. The increase in deformation beyond 70% reduction caused a modest reduction in the intensity of deformation texture. The microstructural observation indicates the occurrence of restoration mechanisms such as recovery/ recrystallization at large strains. The overall findings of the investigation have been summarized in chapter 5. The deformation mechanism maps relating stacking fault energy with amount of strain and with grain size are proposed for micro- and nano- crystalline materials respectively.