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UNIT I:CRYSTAL   STRUCTURE ,[object Object],[object Object],[object Object],[object Object],[object Object]
Crystal Structure matter
Gases ,[object Object],[object Object],Crystal Structure
Liquids and Liquid Crystals ,[object Object],[object Object],Crystal Structure Liquid crystals have mobile molecules, but a type of long range order can exist; the molecules have a permanent dipole. Applying an electric field rotates the dipole and establishes order within the collection of molecule s. + - + - + - + - + - + - + -
Crytals ,[object Object],[object Object],[object Object],[object Object],Crystal Structure
Crystal Structure SOLID MATERIALS CRYSTALLINE POLYCRYSTALLINE AMORPHOUS (Non-crystalline) Single Crystal
Types of Solids ,[object Object],[object Object],[object Object],Crystal Structure
Crystalline Solid ,[object Object],[object Object],Crystal Structure
Crystalline Solid Crystal Structure Single Crystal Single Pyrite Crystal Amorphous Solid ,[object Object]
Polycrystalline Solid Crystal Structure Polycrystalline Pyrite  form (Grain) ,[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object]
CRYSTAL LATTICE Crystal Structure What is crystal  ( space ) lattice? In crystallography, only the geometrical properties of the crystal   are of interest, therefore one  replaces each atom by a geometrical   point located at the equilibrium position of that atom. Platinum Platinum surface Crystal lattice and  structure of  Platinum ( scanning tunneling microscope )
[object Object],[object Object],[object Object],Crystal Structure Crystal Lattice α a b C B E D O A y x
Crystal Structure ,[object Object],Crystal Structure Crystal =  Crystal Lattice  + Basis Structure
A two-dimensional Bravais lattice with different choices for the basis
Basis [Motif] Crystal Structure E H b) Crystal lattice obtained by identifying  all the atoms  in (a) a) Situation of atoms at the corners of regular hexagons ,[object Object],O A C B F b G D x y a α a b C B E D O A y x
Crystal structure ,[object Object],[object Object],[object Object],Crystal Structure Crystal = Crystal Lattice  + Basis Structure
Crystal Structure Crystal Lattice Bravais Lattice (BL) Non-Bravais Lattice (non-BL) ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Translational Lattice Vectors – 2 D ,[object Object],[object Object],[object Object],[object Object],[object Object],Crystal Structure P Point D(n1, n2) = ( 0 ,2)   Point F (n1, n2) = (0,-1)
[object Object],[object Object],Lattice Vectors – 2 D Crystal Structure
Crystal Structure Lattice Vectors – 3D   An ideal  three dimensional  crystal  is described by 3 fundamental translation vectors  a, b  and  c .  If there is a lattice point represented by the position vector R , there is then  also a lattice point represented  by the position vector where  u ,  v  and  w   are arbitrary integers .        R =  u   a +  v   b +  w   c    
Unit Cell in 2D ,[object Object],Crystal Structure 2D-Crystal Unit Cell S S a b S S S S S S S S S S S S S
Unit Cell in 2D ,[object Object],Crystal Structure 2D-Crystal The choice of  unit cell  is not unique . a b S S S S
2D  Unit Cell  example -(NaCl) Crystal Structure We define  lattice points  ; these are points with  identical environments
Choice of origin is arbitrary  - lattice points need not be atoms -  but  unit cell size should always be the same . Crystal Structure
This is also a unit cell -  it doesn’t matter if you start from Na or Cl Crystal Structure
- or if you don’t start from an atom Crystal Structure
This is  NOT a unit cell  even though they are all the same -  empty space is not allowed ! Crystal Structure
Unit Cell in 3D Crystal Structure
Crystal Structure Unit Cell in 3D
Three common Unit Cell in 3D  Crystal Structure
[object Object],[object Object],[object Object],Crystal Structure Unit Cell
[object Object],[object Object],3D – 14 BRAVAIS LATTICES  AND THE  SEVEN CRYSTAL SYSTEM Crystal Structure TYPICAL CRYSTAL STRUCTURES
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Crystal Structure
Coordinatıon Number  ,[object Object],[object Object],Crystal Structure ,[object Object],[object Object],[object Object]
Atomic Packing Factor ,[object Object]
Crystal Structure 1-CUBIC CRYSTAL SYSTEM ,[object Object],[object Object],[object Object],a- Simple Cubic (SC) a b c
Atomic Radius for SC ,[object Object],[object Object],[object Object],[object Object],[object Object],a
Atomic Packing Factor of SC Crystal Structure
[object Object],[object Object],[object Object]
b-Body Centered Cubic (BCC) Crystal Structure a b c ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
b-Body Centered Cubic (BCC) Crystal Structure ,[object Object],[object Object],[object Object],[object Object],a b c
Atomic Radius for BCC unit cell r =a x (3) 1/2 /4
Crystal Structure Atomic Packing Factor of BCC 2 (0,433a)
[object Object],[object Object]
c- Face Centered Cubic (FCC) ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Crystal Structure Many of common metals (Cu,Ni,Pb..etc) crystallize in FCC structure.
Atomic Radius for FCC  r = a x (2) 1/2 /4
Crystal Structure 4 (0 . 353a) Atomic Packing Factor of FCC FCC 0 . 74
Crystal Structure Atoms   Shared Between: Each atom counts: corner 8 cells 1/8 face centre 2 cells 1/2 body centre 1 cell 1 lattice type cell contents P 1  [=8 x 1/8] I 2  [=(8 x 1/8) + (1 x 1)] F 4  [=(8 x 1/8) + (6 x 1/2)] Unit cell contents Counting the number of atoms  within  the unit cell

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Unit i-crystal structure

  • 1.
  • 3.
  • 4.
  • 5.
  • 6. Crystal Structure SOLID MATERIALS CRYSTALLINE POLYCRYSTALLINE AMORPHOUS (Non-crystalline) Single Crystal
  • 7.
  • 8.
  • 9.
  • 10.
  • 11.
  • 12. CRYSTAL LATTICE Crystal Structure What is crystal ( space ) lattice? In crystallography, only the geometrical properties of the crystal are of interest, therefore one replaces each atom by a geometrical point located at the equilibrium position of that atom. Platinum Platinum surface Crystal lattice and structure of Platinum ( scanning tunneling microscope )
  • 13.
  • 14.
  • 15. A two-dimensional Bravais lattice with different choices for the basis
  • 16.
  • 17.
  • 18.
  • 19.
  • 20.
  • 21. Crystal Structure Lattice Vectors – 3D An ideal three dimensional crystal is described by 3 fundamental translation vectors a, b and c . If there is a lattice point represented by the position vector R , there is then also a lattice point represented by the position vector where u , v and w are arbitrary integers .   R = u a + v b + w c    
  • 22.
  • 23.
  • 24. 2D Unit Cell example -(NaCl) Crystal Structure We define lattice points ; these are points with identical environments
  • 25. Choice of origin is arbitrary - lattice points need not be atoms - but unit cell size should always be the same . Crystal Structure
  • 26. This is also a unit cell - it doesn’t matter if you start from Na or Cl Crystal Structure
  • 27. - or if you don’t start from an atom Crystal Structure
  • 28. This is NOT a unit cell even though they are all the same - empty space is not allowed ! Crystal Structure
  • 29. Unit Cell in 3D Crystal Structure
  • 31. Three common Unit Cell in 3D Crystal Structure
  • 32.
  • 33.
  • 34.
  • 36.
  • 37.
  • 38.
  • 39.
  • 40. Atomic Packing Factor of SC Crystal Structure
  • 41.
  • 42.
  • 43.
  • 44. Atomic Radius for BCC unit cell r =a x (3) 1/2 /4
  • 45. Crystal Structure Atomic Packing Factor of BCC 2 (0,433a)
  • 46.
  • 47.
  • 48.
  • 49. Atomic Radius for FCC r = a x (2) 1/2 /4
  • 50. Crystal Structure 4 (0 . 353a) Atomic Packing Factor of FCC FCC 0 . 74
  • 51. Crystal Structure Atoms Shared Between: Each atom counts: corner 8 cells 1/8 face centre 2 cells 1/2 body centre 1 cell 1 lattice type cell contents P 1 [=8 x 1/8] I 2 [=(8 x 1/8) + (1 x 1)] F 4 [=(8 x 1/8) + (6 x 1/2)] Unit cell contents Counting the number of atoms within the unit cell