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Published byElinor Craig Modified over 8 years ago
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Crystal Structure and Crystallography of Materials
Chapter 2: Defect Structure in FCC, HCP, and BCC
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A B C Structure Visualization in Projection: (110) Projection of FCC
[111] [001] [110] {111} Planes A B C Stacking sequence of FCC ; A B C A B C A B C …..
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Perfect Dislocation and Shockley Partial Dislocation in FCC:
Have to understand dislocation both perfect and partial Perfect Dislocation 1/2 [110] type Shockley Partial Dislocation 1/6 [112] type [112] a/2[112] a/2[110] a/6[112] C A B C A A B A
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Shockley Partial Dislocation:
Moving atom from B → C position A B C
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A B C A B C A B C A A B C A C A B C A B A B C A C B C A B C
Shockley Partial Dislocation: A B C A B C A B C A A B C A C A B C A B Stacking fault (one layer missing) → intrinsic stacking fault Locally HCP form A B C A C B C A B C Intrinsic stacking fault Extrinsic stacking fault ▼ A B
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Shockley Partial Dislocation:
B C B→C C→A A→B [111] [110] projection B
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A B A B A B A B A B A B A B A B A A B A B C A C A C A C A C A C A C
Phase Transformation from HCP to FCC: A B A B A B A B A B A B A B A B A A B A B C A C A C A C A C A C A C A B A B C A B C B C B C B C B C B A B A B C A B C A B A B A B A B A A B A B C A B C A B C A C A C A C A B A B C A B C A B C A B C B C B
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A B C A B C A B C A B C A B C A B C A B C
Twin Structure Formation: A B C A B C A B C A B C A B C A B C A B C A B C A B C A B C A C B A B C A B C A B C A B C A B C A B C A C A B C A B C A B C A A B C A B C A B C A C B C A B C A B C A B A B C A B C A B C A C B A C A B C A B C A A B C A B C A B C A C B A C B C A B C A B A B C A B C A B C A C B A C B A B C A B C Shockley partials on consecutive closed packed planes.
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Twin Structure Formation:
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Twin Structure Formation:
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Twin Structure Formation:
Fig. 3 Image simulations of Si-{111}-twin structures: (a) relaxation using empirical MD with the TS potential and atoms according to Fig.2, (b) non-relaxed twin, (c) ab-initio relaxed twin (T), (d) C-layer outside the twin, (e) half layer C-occupation, (f) double layer C-occupation, (g) random C-substitution (R) from Fig. 1.
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Grain Boundary Structure:
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Grain Boundary Structure: Coincident Site Lattice (CSL)
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Grain Boundary Structure: Coincident Site Lattice (CSL)
Shown is the calculated (0oK) energy for symmetric tilt boundaries in Al produced by rotating around a <100> axis (left) or a <110> axis (right). We see that the energies are lower, indeed, in low S orientations, but that it is hard to assign precise numbers or trends. Identical S values with different energies correspond to identical grain orientation relationships, but different habit planes of the grain boundary.
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Grain Boundary Structure in Colloidal Particle Self-Assembly
V I D G
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Grain Boundary Structure in Graphene:
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Cation-Anion radius ratio
Interstitial Sites in Close-Packed Structure: Geometry Coordination # Cation-Anion radius ratio 2 3 4 6 8 <
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Interstitial Sites in FCC Structure:
Octahedral sites: 4 Tetrahedral sites: 8
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Interstitial Sites in HCP Structure:
Tetrahedral sites ; 4 (0,0,3/8) (0,0,5/8) (1/3,2/3,1/8) (1/3,2/3,7/8)
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(2/3,1/3,1/4) (2/3,1/3,3/4) Interstitial Sites in HCP Structure:
Octahedral sites ; 2 A site B site C site (2/3,1/3,1/4) (2/3,1/3,3/4)
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Interstitial Sites in BCC Structure:
3 octa octa = octa
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4/2 tetra x 6 = 12 tetra Interstitial Sites in BCC Structure: a r+ri
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Phase Transformation (Allotropic Phase Transformation)
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