Presentation is loading. Please wait.

Presentation is loading. Please wait.

Paul Sundaram University of Puerto Rico at Mayaguez

Similar presentations


Presentation on theme: "Paul Sundaram University of Puerto Rico at Mayaguez"— Presentation transcript:

1 Paul Sundaram University of Puerto Rico at Mayaguez
Cubic systems Paul Sundaram University of Puerto Rico at Mayaguez

2 Review Seven crystal systems Fourteen Bravais lattices
4/15/2017 Review Seven crystal systems Fourteen Bravais lattices Cubic and Hexagonal systems: 90% of all metals have a cubic or hexagonal structure

3 Cubic system characteristics
Unit cell a=b=c, a= b = g =90˚ Face diagonal and body diagonal Number of atoms per unit cell Coordination number:number of nearest neighbor atoms Close-packed structures Atomic Packing Factor (APF) APF=(vol.of atoms in unit cell)/(vol. of unit cell) Atom positions, crystallographic directions and crystallographic planes (Miller indices) Planar atomic density & linear atomic density

4 Some concepts Number of atoms per unit cell
Corner atom = 1/8 per unit cell Body centered atom = 1 Face centered atom = 1/2 Body diagonal= Face diagonal=

5 Simple cubic(P)

6 Simple cubic

7 Simple cubic

8 Body centered cubic(I)

9 Real picture

10 Body centered cubic

11 Body centered cubic

12 Face centered cubic(F)

13 Real picture

14 Face centered cubic

15 Face centered cubic *Highest packing possible in real structures

16 Questions

17 Atomic Positions Z (1/2,1/2,1) (0,1,1) (0,0,1) (1/2,1/2,1/2)
(1/2,0,1/2) Y (0,0,0) X

18 Crystallographic directions
Concept of a vector & components R R cos(90-f) f R cos(f)

19 Examples Components X:a cos 90=0 Y:a cos 90=0 Z:a cos 0=a
Miller index:[001] Examples Components X:a cos 90=0 Y:a cos 0=a Z:a cos 90=0 Miller index:[010] Components X:a cos 0=a Y:a cos 90=0 Z:a cos 90=0 Miller index:[100] Components X:a cos 90=0 Y:a cos 0=a Z:a cos 90=0 Miller index:[010] Family <100> <010> <001>

20 Examples Components X: 0 Y: a Z: a Miller index:[011] Components X: a

21 Examples Components X: 0 Y: -a Z: -a Miller index:[0 1 1] Components
Family <110> <011> <101>

22 Examples Components X: -a Y: -a Z: -a Miller index:[111] Components
Family <111>

23 Crystallographic planes
1.Intersections with X,Y,Z axes   1 2. Take the inverse 1/ 1/ 1/1 Miller index(0 0 1) Z How to determine indices of plane 1.Intersections with X,Y,Z axes 1   2. Take the inverse 1/1 1/ 1/ Miller index(1 0 0) Y X 1.Intersections with X,Y,Z axes  1  2. Take the inverse 1/ 1/1 1/ Miller index(0 1 0) Family {100}

24 Example 1 1  1/1 1/1 1/  Miller index(1 1 0) Z
How to determine indices of plane 1.Intersections with X,Y,Z axes 1 1  2. Take the inverse 1/1 1/1 1/  Miller index(1 1 0) Y X Family {110}

25 Example 1 1 1 1/1 1/1 1/1 Miller index(1 1 1) Z
How to determine indices of plane 1.Intersections with X,Y,Z axes 1 1 1 2. Take the inverse 1/1 1/1 1/1 Miller index(1 1 1) Y X Family {111}

26 Examples Components X: 1/2 Y: 1/2 Z: 1 [1/2 1/2 1] [112] Components
[-1 1 1/2] [2 2 1] Components X: -1 Y: -1/2 Z: 1/2 [-1 -1/2 1/2] [2 1 1]

27 Examples Intersections -1,-1,1/2 Inverse Intersections -1 -1 2
(1 1 2) Intersections 1/2,1,1/2 Inverse 2 1 2 (212) Intersections 1/6,-1/2,1/3 Inverse (6 2 3) Intersections -1/2,1/2,1 Inverse -2 2 1 (2 2 1)


Download ppt "Paul Sundaram University of Puerto Rico at Mayaguez"

Similar presentations


Ads by Google