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Crystal Structure and Crystallography of Materials

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Presentation on theme: "Crystal Structure and Crystallography of Materials"— Presentation transcript:

1 Crystal Structure and Crystallography of Materials
Chapter 2: Defect Structure in FCC, HCP, and BCC

2 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 …..

3 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

4 Shockley Partial Dislocation:
Moving atom from B → C position A B C

5 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

6 Shockley Partial Dislocation:
B C B→C C→A A→B [111] [110] projection B

7 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

8 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.

9 Twin Structure Formation:

10 Twin Structure Formation:

11 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.

12 Grain Boundary Structure:

13 Grain Boundary Structure: Coincident Site Lattice (CSL)

14 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.

15 Grain Boundary Structure in Colloidal Particle Self-Assembly
V I D G

16 Grain Boundary Structure in Graphene:

17 Cation-Anion radius ratio
Interstitial Sites in Close-Packed Structure: Geometry Coordination # Cation-Anion radius ratio 2 3 4 6 8 <

18 Interstitial Sites in FCC Structure:
Octahedral sites: 4 Tetrahedral sites: 8

19 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)

20 (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)

21 Interstitial Sites in BCC Structure:
3 octa octa = octa

22 4/2 tetra x 6 = 12 tetra Interstitial Sites in BCC Structure: a r+ri

23 Phase Transformation (Allotropic Phase Transformation)


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