Le titane et ses alliages sont très largement étudiés en raison de leur grande utilisation dans l'industrie chimique, les implants médicaux et les industries aérospatiales. Vu le rôle important dans la déformation plastique, le maclage a été largement étudié dans les métaux hexagonaux L'état de contrainte locale peut être modifié par maclage, ce qui influence les modes séquentiels de déformation tels que le glissement, le maclage et le maclage secondaire Ainsi, il existe une demande urgente pour comprendre le mécanisme associé à la déformation induite par maclage, utile pour le développement de modèles prédictifs qui peuvent décrire les événements ultérieurs induits par maclage, ainsi que leurs corrélations avec les microstructures. Dans ce travail, l'analyse cristallographique de la sélection de variantes de macles et des jonctions macle-macle (TTJ= twin-twin junction) est appliquée sur du titane commercialement pur. Un nouveau mécanisme de maclage séquentiel, où les macles {101̅2} sont stimulées par des jonctions macle {112̅1}-macle, est observée par EBSD quasi in situ. Un autre mécanisme de maclage séquentiel a été trouvé lorsque le maclage de compression {112̅2} contient une macle d'extension {101̅2} près des joints de grain à forte désorientation. L'accommodation est utilisée pour déterminer le variant de macle séquentiel lorsque le facteur de Schmid classique (SF) n'est pas suffisant. En outre, une analyse détaillée des 425 macles secondaires {101̅2} détectées dans les macles {11 2̅ 2} primaires révèle que les deux variants de macles qui présentent une désorientation spécifique par rapport aux grains parents sont les plus fréquentes. Il est possible de justifier la prévalence des macles secondaires avec un mécanisme de nucléation aidée par les dislocations prismatiques. Lorsqu'il est complété par une analyse SF généralisée, le critère peut prédire avec précision la sélection entre deux variants dans le groupe des macles secondaires les plus fréquentes. Lorsque plusieurs variants de macles sont actifs dans le même grain, des interactions macle-macle peuvent se produire. Les jonctions macle {112̅2}-macle peuvent être divisés en trois types selon la cristallographie des macles {112̅2}. Une analyse statistique de ces interfaces révèle qu'un seul type est le plus fréquent tandis que les autres types sont rarement activés. La fréquence des TTJ peut être évaluée en utilisant une analyse SF généralisée. Il en ressort que les interfaces macle-macle (TTB= twin-twin boundary) ne se forment que d’un côté de la macle. Concernant la formation de TTBs basée sur les interactions des dislocations de macle, les dislocations d'interface dans les TTBs observées ont une énergie de ligne inférieure à celles des TTB non observées. Une opération similaire est appliquée à l'analyse de {112̅1} TTJs / Titanium and its alloys have been extensively investigated due to their wide application in chemical industry, medical implants and aerospace industries. As a significant role in plastic deformation, twinning has been widely studied in hexagonal metals. The local stress state may be modified by twinning, which influences sequential plastic deformation modes such as slips, twinning and secondary twinning. Thus, there is also an urgent demand for understanding the mechanism associated with the twinning-induced deformation, which is useful for the development of predictive capabilities that can describe twinning and twinning-induced sequential events, and their correlations with microstructures. In this work, crystallographic analysis of twin variant selection and twin-twin junctions is applied in commercially pure titanium. A new sequential twinning mechanism that {101̅2} twins are stimulated by the {112̅1} twin-twin junctions (TTJs) is observed by quasi in-situ EBSD. Another sequential twinning mechanism that a {112̅2} compression twin adjoins a {10 1̅ 2} extension twin is found at high angle grain boundaries. Displacement gradient accommodation is used to determine the sequential twin variant while the classical Schmid factor (SF) is not sufficient. Besides, a detailed analysis of the detected 425 {101̅2} double twins inside primary {112̅2} twins reveals that the double twin variants that exhibit specific misorientation with respect to the parent grains are the most frequent. The prevalence of double twins is possible to justify with the prismatic-dislocation mediated nucleation mechanism. When complemented with an apparent SF analysis, the criterion can accurately predict the selection between two variants within the group of the popular double twins. When multiple twin variants are active in the same grain, twin-twin interactions may happen. {112̅2} TTJs can be divided into three types according to the crystallography of {112̅2} twins. A statistical analysis of {112̅2} TTJs reveals that one type is the most popular while other types are rarely activated. The frequency of TTJs can be evaluated by using an apparent SF analysis. The interesting finding is that twin-twin boundaries (TTBs) form in one side of the incoming twin as a TTJ forms. Corresponding to the formation of TTBs based on the interactions of twinning dislocations, interface dislocations in the observed TTBs have lower line energy than those in the un-observed TTBs. Similar operation is applied to the analysis of {112̅1} TTJs

This thesis aims to reveal the correlation between stress corrosion cracking propagation behavior and Schmid and Taylor factor mismatch using EBSD analysis. <div><br></div><div>Chloride induced stress corrosion cracking (CISCC) is one of the most vulnerable weaknesses for the widely used austenitic stainless steel in many industries. The complex nature of CISCC involves mechanical, electrochemical, and microstructural perspectives. The objective of this thesis is to assess CISCC phenomenon in austenitic stainless steel from the mechanical and crystallographic perspective, specifically on the effect of local strain and stress and anisotropic plastic deformation. Austenitic stainless steel 304L test coupons are bent in four-point bending fixtures to obtain tensile stress for CISCC, followed by corrosion experiment in boiling magnesium chloride solution. Stress state of the sample is evaluated by finite element analysis (FEA) and X-ray Diffraction Crystallography (XRD) prior corrosion test. Cross section of the cracked region are analyzed with Electron Backscatter Diffraction (EBSD) to analyze the relationship between CISCC behaviors and crystallographic features in the sample. Schmid factor and Taylor factor are used to quantitatively evaluate CISCC initiation and propagation behavior. It is learned that in polycrystalline FCC stainless steel, mismatch of Schmid factor and Taylor factor values in adjacent grains along crack path governs CISCC propagation susceptibility and path selection. Crack propagation factor competition model is proposed based on observations from EBSD maps, incorporating Schmid factor and Taylor factor mismatch, electrochemical condition of crack tip, and anisotropic properties. <br></div>

In the present work, deformation behavior, texture and microstructure evolution of commercially pure titanium (CP Ti) are investigated by electron backscattered diffraction (EBSD) after compression tests at elevated temperatures. By analysing work hardening rate vs. flow stress, the deformation behaviour can be divided into three groups, viz. three-stage work hardening, two-stage work hardening and flow softening. A new deformation condition map is presented, dividing the deformation behavior of CP Ti into three distinct zones which can be separated by two distinct values of the Zener-Hollomon parameter. The deformed microstructures reveal that dynamic recovery is the dominant deformation mechanism for CP Ti during hot working. It is the first time that the Schmid factor and pole figures are used to analyse how the individual slip systems activate and how their activities evolve under various deformation conditions. Two constitutive equations are proposed in this work, one is for single peak dynamic recrystallization (DRX), the other is specially for CP Ti deformed during hot working. After the hot compression tests, some stress-strain curves show a single peak, leading to the motivation of setting up a DRX model. However, the examinations of EBSD maps and metallography evidently show that the deformation mechanism is dynamic recovery rather than DRX. Then, the second model is set up. The influence of the deformation conditions on grain size, texture and deformation twinning is systematically investigated. The results show that {10-12} twinning only occurs at the early stage of deformation. As the strain increases, the {10-12} twinning is suppressed while {10- 11} twinning appears. Three peaks are found in the misorientation frequency-distribution corresponding to basal fiber texture, {10-11} and {10-12} twinning, respectively. A logZ-value of 13 is found to be critical for both the onset of {10-11} compressive twinning and the break point for the subgrain size. The presence of {10-11} twinning is the key factor for effectively reducing the deformed grain size. The percentage of low angle grain boundaries decreases with increasing Z-parameter, falling into a region separated by two parallel lines with a common slope and 10% displacement. After deformation, three texture components can be found, one close to the compression direction, CD, one 10~30° to CD and another 45° to CD. / QC 20100819