Martensite in Steels - Department of Materials Science and Metallurgy
Martensite in Steels - Department of Materials Science and Metallurgy
Martensite in Steels - Department of Materials Science and Metallurgy
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egion is similarly deflected though the scratch rema<strong>in</strong>s connected at the α ′ /γ <strong>in</strong>terface. Theseobservations, <strong>and</strong> others, confirm that the measured shape deformation is an <strong>in</strong>variant–planestra<strong>in</strong> (Fig. 3e–g) with a large shear component (≃ 0.22) <strong>and</strong> a small dilatational stra<strong>in</strong> (≃ 0.03)directed normal to the habit plane.Fig. 3: (a, b) Step caused by the passage <strong>of</strong> a slip dislocation. (c, d) Manyslip dislocations, caus<strong>in</strong>g a macroscopic shear. (e) An <strong>in</strong>variant–plane stra<strong>in</strong>with a uniaxial dilatation. (f) An <strong>in</strong>variant–plane stra<strong>in</strong> which is a simpleshear. (g) An <strong>in</strong>variant–plane stra<strong>in</strong> which is the comb<strong>in</strong>ed effect <strong>of</strong> a uniaxialdilatation <strong>and</strong> a simple shear.Ba<strong>in</strong> Stra<strong>in</strong>We now consider the nature <strong>of</strong> the stra<strong>in</strong> necessary to transform the c.c.p. lattice <strong>of</strong> γ<strong>in</strong>to the b.c.c. lattice <strong>of</strong> α ′ . Such a stra<strong>in</strong> was proposed by Ba<strong>in</strong> <strong>in</strong> 1924 <strong>and</strong> hence is known6