2012
DOI: 10.1016/j.scriptamat.2011.11.036
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In situ TEM study of dislocation slip in a metastable β titanium alloy

Abstract: Dislocation slip is investigated in a metastable  titanium alloy with the Ti-23Nb-0.7Ta-2Zr-0.4Si composition (at. %) by in situ straining experiments in a transmission electron microscope (TEM). Moving dislocations have a/2<111> Burgers vectors and glide in {110}, {112} or {123} planes. The mobility of screw dislocations is lowered by punctual defects and the existence of a stable and sessile core configuration that has to recombine in order to allow dislocations to glide.

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Cited by 76 publications
(39 citation statements)
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“…9). This domain thus corresponds to the plastic domain wherein dislocation slip and twinning are mainly operating in this alloy [7] and more generally in this alloy family [5,[36][37][38]. As the SIM transformation is not fully reversible from 2% of applied strain (Fig.…”
Section: Correlation Between Sxrd Results and Tensile Curvesmentioning
confidence: 89%
“…9). This domain thus corresponds to the plastic domain wherein dislocation slip and twinning are mainly operating in this alloy [7] and more generally in this alloy family [5,[36][37][38]. As the SIM transformation is not fully reversible from 2% of applied strain (Fig.…”
Section: Correlation Between Sxrd Results and Tensile Curvesmentioning
confidence: 89%
“…The dislocation slip has been investigated in b-titanium alloy using TEM analysis [16]. The dislocations with Burgers vector b = a/2h111i are observed to glide on the {110}, {112}, and {123} planes similar to bcc metals, and the deformation is largely governed by the motion of screw segments.…”
Section: Discussion Of the Resultsmentioning
confidence: 99%
“…In order to achieve high transformation strains, it is desirable to minimize plastic strain accumulating through austenite slip. The slip in bTi-based alloys occur on {110}h111i system similar to bcc metals [16,37], and we are interested in obtaining the energy barriers (GSFE) required to nucleate a h111i dislocation on {110} plane. The GSFE can be obtained by rigidly shearing one half of the crystal relative to the other half on the {110} plane along h111i direction by displacement of u = nb, where b is the magnitude of the Burgers vector of the slip dislocation and n is the parameter ranging from 0 to 1 [29].…”
Section: Generalized Stacking Fault Energy and Austenite Slipmentioning
confidence: 99%
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