3.14/3.40j/22.71j recap basic crystallography and miller indices

13
Ting-Yun Huang, 2012/09/18 Page 1 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices Ting-Yun Huang 2012 Sep. 18 th

Upload: kenton

Post on 16-Jan-2016

37 views

Category:

Documents


0 download

DESCRIPTION

3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices. Ting-Yun Huang 2012 Sep. 18 th. Outline. Basic Structures Cubic: FCC/BCC HCP Miller Indices From 3D to 4D: Miller indices for hexagonal crystals From 3D to 2D: Stereographic Projection Zone axis. BCC/FCC /HCP. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Ting-Yun Huang, 2012/09/18Page 1

3.14/3.40J/22.71J Recap

Basic Crystallography and Miller Indices

Ting-Yun Huang

2012 Sep. 18th

Page 2: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Outline• Basic Structures

– Cubic: FCC/BCC

– HCP

• Miller Indices

– From 3D to 4D: Miller indices for hexagonal crystals

– From 3D to 2D: Stereographic Projection

– Zone axis

Ting-Yun Huang, 2012/09/18Page 2

Page 3: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

BASIC STRUCTURESBCC/FCC /HCP

Ting-Yun Huang, 2012/09/18Page 3

Page 4: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Basic Structures: BCC

• Coordination number = 8

• Number of atoms in unit cell = 2

• α-Fe(room temperature) , δ-Fe(high T), β-Ti(high T), Zr (high T)

Ting-Yun Huang, 2012/09/18Page 4

Page 5: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Basic Structures: FCC• Coordination number =

12

• Number of atoms in unit cell = 4

• Closest packing

– ABCABC packing

• γ-Fe, Cu, Ag, Au, Al, Ni, Pb, Pt

Ting-Yun Huang, 2012/09/18Page 5

Page 6: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Basic Structures: HCP

•Coordination number = 12

•Number of atoms in unit cell = 2(*)

•Closest packing

– ABAB packing

•Mg, Zn, α-Ti, Be, Cd, Zr (low T)

Ting-Yun Huang, 2012/09/18Page 6

Page 7: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

MILLER INDICESNotations/Hexagonal Systems/Stereographic Projection

Presentation Author, 2003Page 7

Page 8: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Miller Indices-Notations• Directions

– Specific Direction: [u1 u2 u3]

– Family of Directions: <u1 u2 u3>

• Planes

– Reciprocal of the intercepts

– Specific Plane: (u1 u2 u3)

– Family of Planes: {u1 u2 u3}

Ting-Yun Huang, 2012/09/18Page 8

Page 9: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

From 3D to 4D-

Miller indices for HCP structures• Constraints:

– [u1u2u3v]→u1a1+u2a2+u3a3+vc

– u1+u2+u3 = 0

• Redundant coordinate system which is not orthogonal

• But we can still perform inner product.

Ting-Yun Huang, 2012/09/18Page 9

Page 10: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

From 3D to 2D-Stereographic Projection

Ting-Yun Huang, 2012/09/18Page 10

Page 11: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Zone axis

In this TEM diffraction, the structure

is FCC and the zone axis is [112].

The (11-1) and (2-20) plane have the

same zone axis [112].

Presentation Author, 2003Page 11

_(111) _

(220)

Page 12: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

From 3D to 2D-Stereographic Projection

Ting-Yun Huang, 2012/09/18Page 12

Page 13: 3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices

Thank you!

Ting-Yun Huang, 2012/09/18Page 13