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* * * Introduction and point groups Stereographic projections Low symmetry systems Space groups Deformation and texture Interfaces, orientation relationships Martensitic transformations * * * * * * Materials, transformation temperatures & strength * * * Olson and Hartman, 1982 * * * Olson and Hartman, 1982 * * * Olson and Hartman, 1982 * * * Martensite can form at very low temperatures. Martensite can grow very rapidly. No composition change during transformation. Diffusionless transformation? * * * Shape of martensite ? * * * * * * Irrational: why? * * * * * * Orientation relationships: irrational * * * athermal transformation * * * q Creation of a bi-crystal cut and rotate by angle q about axis normal to diagram * * * * * * Glissile interface * * * * * * Glissile interface cannot contain more than one set of dislocations. Martensitic transformation only possible if the deformation which changes the parent into the product leaves one line undistorted and unrotated, i.e. an invariant-line. Deformation is an invariant-line strain. * * * * * * * * * * * * * * * * * * c r d s 1 Christian, 1957 * * * * * * body-centred cubic cubic close-packed * * * (a) BAIN STRAIN (c) Body-centered tetragonal austenite (d) Body-centered cubic martensite a a a 1 2 3 b 3 b 1 b 2 (b) * * * * * * [100] [001] o a a' b b' o b' b a,a' (a) (b) * * * * * * * * * * * * transformation twins (Wayman) * * * hexagonal close-packed cubic close-packed * * * * * * Brooks, Loretto and Smallman, 1979 * * * * * * a g Carbon Concentration Free Energy a x x x ag ga * * * * * *
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