crystal system

25
CRYSTAL SYSTEM 1 CRYSTAL SYSTEM 1 Representator: MD. MOHYMENUL ISLAM ID: PH 12004 3 rd YEAR 1 st SEMESTER DEPT. OF PHYSICS MBSTU

Upload: mohymenul-islam

Post on 12-Apr-2017

80 views

Category:

Science


0 download

TRANSCRIPT

Page 1: Crystal system

CRYSTAL SYSTEM1

CRYSTAL SYSTEM1

Representator:MD. MOHYMENUL ISLAMID: PH 120043rd YEAR 1st SEMESTERDEPT. OF PHYSICSMBSTU

Page 2: Crystal system

CrystalTranslational VectorCrystal StructureCrystal LatticeUnit cellLattice ConstantSymmetry OperationPacking FactorMiller IndicesInter-planar Spacing

CRYSTAL SYSTEM2

Page 3: Crystal system

3CRYSTAL SYSTEM

SOLID MATERIALS

CRYSTALLINE

Single Crystal

POLYCRYSTALLINE

AMORPHOUS(Non-crystalline)

A crystal is a solid in which atoms are arranged in some regular repetition pattern in all directions.

CrystalCrystals (at a given temperature, pressure, and volume) have stronger bonds between molecules and atoms than liquids. It’s require more energy to break the bonds.

Page 4: Crystal system

Crystalline material is a material comprised of one or many crystals. Ex:Diamond,quartz,mica etc. Amorphous have order only within a few atomic or molecular dimensions. Ex: Glass,plastics,rubbers.Polycrystallne is a material made up of an aggregate of many small single crystals (also called crystallites or grains).Ex:Metals and ceramics.

CRYSTAL SYSTEM 4

*Crystal Types

Single Pyrite Crystal

AmorphousSolid

Polycrystalline Pyrite form

(Grain)

Page 5: Crystal system

CRYSTAL SYSTEM5

* Difference between crystalline & non-crystalline

1.Long range order.

2.Fixed melting point.

3.Atoms or molecules are periodically arranged.

1.Short range order.

2.No fixed melting point. 3.Atoms or molecules are randomly arranged.

Crystalline Non-crystalline

CRYSTAL SYSTEM

5

Page 6: Crystal system

CRYSTAL SYSTEM6

Translational Lattice Vectors

A lattice translation operation is defined by the displacement of a crystal by a crystal translation vector.

Rn = n1 a + n2 b

This is translational symmetry.

The vectors a, b are known as lattice vectors and (n1, n2) is a pair of integers whose values depend on the lattice point.

P

Point D(n1, n2) = (0,2)

Page 7: Crystal system

CRYSTAL SYSTEM7

*Crystal Structure*A CRYSTAL STRUCTURE is a periodic arrangement of atoms in the crystal that can be described by a LATTICE

Lattice: A 3D translationally periodic arrangement of points in space.Basis: A group of atoms associated with each lattice point to represent crystal structure.

Page 8: Crystal system

CRYSTAL SYSTEM8

Bravais Lattice (BL) All atoms are of the same kind All lattice points are equivalent

Non-Bravais Lattice (non-BL)

Bravais Lattice Non-Bravais Lattice

Page 9: Crystal system

UNIT CELL The smallest component of the crystal which

when stacked together with pure translational repetition reproduces the whole crystal.

CRYSTAL SYSTEM9

Sa

b

S

S

S

S

S

S

S

S

S

S

S

S

S

S

Page 10: Crystal system

CRYSTAL SYSTEM 10

THREE COMMON UNİT CELL İN 3D • Primitive (P) unit cells contain only a single lattice point.• Internal (I) unit cell contains an atom in the body center.• Face (F) unit cell contains atoms in the all faces of the planes composing the cell.

Page 11: Crystal system

CRYS

TAL

SYST

EM

11

CRYS

TAL

SYST

EM

11

Crystal Structure 11

Unit cell exist in only seven shapes

Page 12: Crystal system

The numbers a,b,c specifying the size of a unit cell (in fact, conventional unit cell) are called its lattice constant

For cubic lattice, the lattice constant,

12

Where, ρ=density of the latticen= number of particles M= molecular weight of the crystal NA =Avogadro number

a=(nM/NAρ)1/3

Page 13: Crystal system

CRYSTAL SYSTEM13

Symmetry Operation: A symmetry operations is one which leaves the crystal unchanged such as translation, rotation, reflection or inversion.

5-fold symmetry:

Symmetry Operations

N-fold axes with n=5 or n>6 does not occur in crystals

Adjacent spaces must be completely filled (no gaps, no overlaps).

Page 14: Crystal system

14CRYSTAL SYSTEM

*Atomic Packing Factor*Atomic Packing Factor (APF) is defined as the volume of atoms in the unit cell divided by the volume of the unit cell.

Page 15: Crystal system

Simple Cubic Structure (SC)Close-packed directions are cube edges.

• Coordination = 6 (nearest neighbors)

a = 2r, r = a/2Atomic Radius, r=0.5a

a

Page 16: Crystal system

Atomic Packing Factor (APF):SC

• APF = 0.52, That means the percentage of packing is 52%

APF = a3

43p (0.5a) 31

atomsunit cell

atomvolume

unit cellvolume

APF = Volume of atoms in unit cell*

Volume of unit cell*assume hard spheres

close-packed directions

a

R=0.5a

Number of lattice point 8 x 1/8 = 1 atom/unit cell

Page 17: Crystal system

Body Centered Cubic Structure (BCC)

• Coordination # = 8

• Atoms touch each other along cube diagonals.

Ex: Cr, Fe , Molybdenum

2 atoms/unit cell: 1 center + 8 corners x 1/8

Atomic Radius ,r =a x (3)1/2/4

Page 18: Crystal system

Atomic Packing Factor: BCC

a

APF =

43p ( 3a/4)32

atomsunit cell atom

volume

a3unit cellvolume

length = 4R =Close-packed directions:

3 aaR

a 2

a 3

• APF for a body-centered cubic structure = 0.68

Page 19: Crystal system

Face Centered Cubic Structure (FCC)

• Coordination = 12

• Atoms touch each other along face diagonals.

Ex: Al, Cu, Ni,Ag

4 atoms/unit cell: 6 face x 1/2 + 8 corners x 1/8

Atomic Radius ,r = a x (2)1/2/4

Page 20: Crystal system

Atomic Packing Factor: FCC

APF =

43p ( 2a/4)34

atomsunit cell atom

volume

a3unit cellvolume

Close-packed directions: length = 4R = 2 a

Number of lattice point : 6 x 1/2 + 8 x 1/8 = 4 atoms/unit cell

a

2 a

• APF for a face-centered cubic structure = 0.74

Page 21: Crystal system

Miller Indices• Miller Indices is a group of smallest integers which represent a direction or a plane.

To determine Miller indices of a plane, take the following steps:

1) Determine the intercepts of the plane along each of the three crystallographic directions2) Take the reciprocals of the intercepts3) If fractions result, multiply each by the denominator of the smallest fraction.

Page 22: Crystal system

CRYSTAL SYSTEM22

(233)

Page 23: Crystal system

CRYSTAL SYSTEM23

Inter-planar Spacing For orthorhombic, tetragonal and cubic

unit cells (the axes are all mutually perpendicular), the inter-planar spacing is given by:

h, k, l = Miller indicesa, b, c = unit cell dimensions

222 lkh

adhkl

• For cube a = b = c than

Page 24: Crystal system

24

REFERENCES

Sourcewww.Google.comhttp://en.wikipedia.orgSolid State Physics & Electronics

By R.K. PURI” Solid State Physics ” By R.L.

SINGHALSeventh Revised & Enlarged Edition-2003

CRYSTAL SYSTEM

Page 25: Crystal system

CRYS

TAL

SYST

EM

25