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1. There have no two-phases area in diffusion area, every layer is single-phases 2. Phase's interface moves according to parabola law 3. Phase's width
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Discrepancies between theory and practice in Deformation. 1. Morphology of the surface in deformation. 2. The great difference between theoretical and actual strength of single crystals (. >>)
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By cottrell atmosphere model, we can explain the sharp yielding phenomenon
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Back stress exerted by obstacle on leading dislocation. (It is supposed to be a short-range-force.) nrbdx =tpbdx dx virtual displacement
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5.16 Dislocation in FCC crystals Perfect dislocation b =na, +nb. +nC
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山西师范大学:《材料科学基础》课程教学大纲(材料化学专业)
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5. 8 The Stress Around a Dislocation 1. Screw dislocation: Displacement:
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Edge dislocation 1. Slip (glide) Dislocation motion vs. atom movement. Direction:l⊥讠 Plane:lb(l× Dislocation motion vs. crystal movement. → crystal movement→(dislocation motion)
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1. Classification y Ideal or perfect crystal real or defect crystal According to dimension o point defect: vacancies, interstitial atoms s line defect dislocation planar defect: stacking fault o volume defect mosaic structure
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1. The cause of rotation: Due to constraints, or boundary conditions imposed on the crystal. ll. The rule of rotation:
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