crystal structure of metal

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Crystal Structure of Metals

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Page 1: Crystal structure of metal

Crystal Structure of Metals

Page 2: Crystal structure of metal

WHY STUDY The Structure of Crystalline Solids?

The properties of some materials are directly related to their crystal structures. i.e. pure and undeformed magnesium and beryllium, having one crystal structure, are much more brittle (lower degrees of deformation) than are pure and undeformed metals such as gold and silver that have yet another crystal structure.

A knowledge of the crystal structure for iron helps us understand transformations that occur when steels are heat treated to improve their mechanical properties.

Furthermore, significant property differences exist between crystalline and noncrystalline materials

having the same composition.

Page 3: Crystal structure of metal

Learning Objective

Difference in atomic/molecular structure between crystalline and noncrystalline materials.

unit cells for face-centered cubic, body centered cubic, and hexagonal close-packed crystal structures.

Distinguish between single crystals and polycrystalline materials.

Define isotropy and anisotropy with respect to material properties.

ISSUES TO ADDRESS...

Page 4: Crystal structure of metal

A crystalline material is one in which the atoms are situated in an orderly, repeating pattern extending in all three dimension .i.e.Nacl ,CsF etc.crystalline solids depend on the crystal structure of the material, the manner in which atoms, ions, or molecules are spatially(three dimension) arranged.lattice is used in the context of crystal structures; in this sense lattice means a three-dimensional array of points coinciding with atom positions (or sphere centers).

Amorphous solid is one in which the atom are not situated in an orderly, repeating pattern. i.e. glass , rubber, plastic etc.Amorphous solid don’t have sharp melting point that is why particle of glass soften over temperature range.

Page 5: Crystal structure of metal

ENERGY AND PACKINGENERGY AND PACKING Energy

r

typical neighbor bond length

typical neighbor bond energy

• Non dense, random packing Energy

r

typical neighbor bond length

typical neighbor bond energy

Dense, regular-packed structures tend to have lower energy

Page 6: Crystal structure of metal

Crystalline solid

Amorphous solid

Page 7: Crystal structure of metal

The smallest repeating unit in a crystal is a unit cell.

Three-dimensional packing of unit cells produces the crystal lattice.

There are seven different unit cells:• Cubic: All three axes have same length and

intercept at right angles.

• Tetragonal: The three axes intercept at right angles, but one axis is longer or shorter than the other two equal axes.

• Hexagonal: Three of the four axes are in one plane, intercept at 120°, and are of the same length.

Page 8: Crystal structure of metal

• Trigonal(rhombohedral): Same axes as hexagonal, but angle lie b/w right angle to 120°.

• Orthorhombic: The three axes are of different lengths and are at right angles to each other.

Monoclinic: The three axes are of different lengths and two are at right angles to each other. The third axis is inclined.

Triclinic: All three axes are of different lengths and form oblique angles.

Page 9: Crystal structure of metal

CRYSTAL SYSTEMS

Page 10: Crystal structure of metal

Metallic Crystal StructuresThe atomic bonding in this group of materials

is metallic and thus non-directional in nature.For metals, using the hard-sphere model for the

crystal structure, each sphere represents an ion core.

There are three principle crystal structures for metals:

Body-center-cubic (BCC)Face-centered cubic (FCC) Hexagonal closed packed(HCP)

Page 11: Crystal structure of metal

• Coordination # = 8

--Note: All atoms are identical; the center atom is shaded differently only for ease of viewing.

BODY CENTERED CUBIC STRUCTURE

• Atoms touch each other along cube diagonals.

example: Cr, W, Fe (), Tantalum, Molybdenum

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

In BCC atoms located at all eight corners and a single atom at the cube center. This is called a body-centered cubic (BCC) crystal structure.

Page 12: Crystal structure of metal

ATOMIC PACKING FACTOR: BCC

Unit cell contains: 1 + 8 x 1/8 = 2 atoms/unit cell

Close-packed directions: length = 4R

= 3 a

APF = a3

4

3( 3a/4)32

atoms

unit cell atomvolume

unit cell

volume

• APF for a body-centered cubic structure = p3/8 = 0.68

aR

Page 13: Crystal structure of metal

FACE CENTERED CUBIC STRUCTURE (FCC)

--Note: All atoms are identical; the face-centered atoms are shaded differently only for ease of viewing.

Coordination # = 12

Atoms touch each other along face diagonals.

example: Al, Cu, Au, Pb, Ni, Pt, Ag

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

In FCC atoms located at each of the corners and the centers of all the cube faces. This is called the face-centered cubic (FCC) crystal structure.

Page 14: Crystal structure of metal

ATOMIC PACKING FACTOR: FCCClose-packed directions: length = 4R

= 2 a

Unit cell contains:

6 x 1/2 + 8 x 1/8

= 4 atoms/unit cell

a

2 a

APF =

4

3p ( 2 a/4 )34

atoms

unit cell atom

volume

a3

unit cell

volume

• APF for a face-centered cubic structure = 0.74

Page 15: Crystal structure of metal

A sites

B B

B

BB

B B

C sites

C C

CA

B

B sites

• ABCABC... Stacking Sequence• 2D Projection

• FCC Unit Cell

B B

B

BB

B B

B sites

C C

CA

C C

CA

AB

C

FCC Stacking Sequence

Page 16: Crystal structure of metal

Hexagonal Close-Packed Structure (HCP)• ABAB... Stacking Sequence

• 3D Projection • 2D Projection

c

a

A sites

B sites

A sitesBottom layer

Middle layer

Top layer

• Coordination # = 12

• APF = 0.74

• c/a = 1.633

6 atoms/unit cell

ex: Cd, Mg, Ti, Zn

Page 17: Crystal structure of metal

Close packed crystals

…ABCABCABC… packing[Face Centered Cubic (FCC)]

…ABABAB… packing[Hexagonal Close Packing (HCP)]

A plane

B plane

C plane

A plane

Page 18: Crystal structure of metal

COMPARISON OF CRYSTAL STRUCTURESCrystal structure coordination # packing factor close packed

directions

Body Centered Cubic (BCC) 8 0.68 body diagonal

Face Centered Cubic (FCC) 12 0.74 face diagonal

Hexagonal Close Pack (HCP) 12 0.74 hexagonal side

Page 19: Crystal structure of metal

SINGLE VS POLYCRYSTALS• Single Crystals

an object composed of randomly oriented crystals, formed by rapid solidification

A single crystal is formed by the growth of a crystal nucleus without secondary nucleation or impingement on other crystals.

• Polycrystals

-Properties vary with direction: anisotropic.-Example: the modulus

of elasticity (E) in BCC iron:

-Properties may/may not vary with direction.-If grains are randomly oriented: isotropic. (Epoly iron = 210 GPa)-If grains are textured, anisotropic.

E (diagonal) = 273 GPa

E (edge) = 125 GPa

200 mm

Page 20: Crystal structure of metal

Isotropic:Substances in which measured (physical)properties are independent of the direction of measurement are isotropic.

The substance in which physical properties are show variation with changing the direction . Such substance are called anisotropic.

ANISOTROPY:

A different chemical bonding in all directions is also a condition for anisotropy.

Page 21: Crystal structure of metal

SUMMARY• Atoms may assemble into crystalline, polycrystalline or amorphous structures.

• We can predict the density of a material, provided we know the atomic weight, atomic radius, and crystal geometry (e.g., FCC, BCC, HCP).

• Material properties generally vary with single crystal orientation (i.e., they are anisotropic), but properties are generally non-directional (i.e., they are isotropic) in polycrystals with randomly oriented grains.

Page 22: Crystal structure of metal