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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.
Learning Objective
  ISSUES TO ADDRESS...
 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.
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.
ENERGY AND PACKING
  ENERGY AND PACKING




 • Non dense, random packing




Dense, regular-packed structures tend to have lower energy
Crystalline solid   Amorphous solid
 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.
• 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.
CRYSTAL SYSTEMS
Metallic Crystal Structures
 The 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)
BODY CENTERED CUBIC STRUCTURE
   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.
          example: Cr, W, Fe (), Tantalum, Molybdenum
                                                  • Coordination # = 8




    2 atoms/unit cell: 1 center + 8 corners x 1/8
  • Atoms touch each other along cube diagonals.
--Note: All atoms are identical; the center atom is shaded
  differently only for ease of viewing.
ATOMIC PACKING FACTOR: BCC



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



 • APF for a body-centered cubic structure = p3/8 = 0.68
FACE CENTERED CUBIC STRUCTURE (FCC)
    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.
    example: Al, Cu, Au, Pb, Ni, Pt, Ag
                                             Coordination # = 12




   4 atoms/unit cell: 6 face x 1/2 + 8 corners x 1/8
   Atoms touch each other along face diagonals.

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


  2a                                         Unit cell contains:
                                                 6 x 1/2 + 8 x 1/8
                                              = 4 atoms/unit cell
   a
                  atoms
                                      4                              volume
                 unit cell        4       p ( 2 a/4 ) 3
                                      3                               atom
                        APF =
                                                            volume
                                            a3
                                                            unit cell
  • APF for a face-centered cubic structure = 0.74
FCC Stacking Sequence
• ABCABC... Stacking Sequence
• 2D Projection
                              B         B
                                    C
                      A
        A sites           B         B       B
                              C         C
        B sites                 B       B
        C sites


                                              A
• FCC Unit Cell                              B
                                            C
Hexagonal Close-Packed Structure                       (HCP)
• ABAB... Stacking Sequence
• 3D Projection                     • 2D Projection


                        A sites
                                                 Top   layer
c                       B sites
                                                 Middle layer

                     A sites
                                                 Bottom layer
            a
• Coordination # = 12
                                  6 atoms/unit cell
    • APF = 0.74
                                  ex: Cd, Mg, Ti, Zn
    • c/a = 1.633
Close packed crystals




                              A plane
                              B plane


                               C plane

                                A plane

  …ABCABCABC… packing                          …ABABAB… packing
[Face Centered Cubic (FCC)]              [Hexagonal Close Packing (HCP)]
COMPARISON OF CRYSTAL
STRUCTURES
Crystal 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
SINGLE VS POLYCRYSTALS
    • Single Crystals
   A single crystal is formed by the growth of a
   crystal nucleus without secondary
   nucleation or impingement on other
   crystals.
    -Properties vary with
     direction: anisotropic.
    -Example: the modulus
     of elasticity (E) in BCC iron:                200 mm

     • Polycrystals
  an object composed of randomly oriented cr
  ystals, formed by rapid solidification
-Properties may/may not vary with direction.
-If grains are randomly oriented: isotropic.
 (Epoly iron = 210 GPa)
-If grains are textured, anisotropic.
Isotropic:
Substances in which measured (physical)properties are independent
of the direction of measurement are isotropic.

  ANISOTROPY:
  The substance in which physical properties are show variation
  with changing the direction . Such substance are called
  anisotropic.
 A different chemical bonding in all directions is also a
 condition for anisotropy.
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.
Crystal structure of metal

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Crystal structure of metal

  • 1.
  • 2. 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.
  • 3. Learning Objective ISSUES TO ADDRESS...  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.
  • 4. 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.
  • 5. ENERGY AND PACKING  ENERGY AND PACKING • Non dense, random packing Dense, regular-packed structures tend to have lower energy
  • 6. Crystalline solid Amorphous solid
  • 7.  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.
  • 8. • 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.
  • 10. Metallic Crystal Structures  The 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)
  • 11. BODY CENTERED CUBIC STRUCTURE 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. example: Cr, W, Fe (), Tantalum, Molybdenum • Coordination # = 8 2 atoms/unit cell: 1 center + 8 corners x 1/8 • Atoms touch each other along cube diagonals. --Note: All atoms are identical; the center atom is shaded differently only for ease of viewing.
  • 12. ATOMIC PACKING FACTOR: BCC R a Unit cell contains: 1 + 8 x 1/8 = 2 atoms/unit cell • APF for a body-centered cubic structure = p3/8 = 0.68
  • 13. FACE CENTERED CUBIC STRUCTURE (FCC) 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. example: Al, Cu, Au, Pb, Ni, Pt, Ag Coordination # = 12 4 atoms/unit cell: 6 face x 1/2 + 8 corners x 1/8 Atoms touch each other along face diagonals. --Note: All atoms are identical; the face-centered atoms are shaded differently only for ease of viewing.
  • 14. ATOMIC PACKING FACTOR: FCC 2a Unit cell contains: 6 x 1/2 + 8 x 1/8 = 4 atoms/unit cell a atoms 4 volume unit cell 4 p ( 2 a/4 ) 3 3 atom APF = volume a3 unit cell • APF for a face-centered cubic structure = 0.74
  • 15. FCC Stacking Sequence • ABCABC... Stacking Sequence • 2D Projection B B C A A sites B B B C C B sites B B C sites A • FCC Unit Cell B C
  • 16. Hexagonal Close-Packed Structure (HCP) • ABAB... Stacking Sequence • 3D Projection • 2D Projection A sites Top layer c B sites Middle layer A sites Bottom layer a • Coordination # = 12 6 atoms/unit cell • APF = 0.74 ex: Cd, Mg, Ti, Zn • c/a = 1.633
  • 17. Close packed crystals A plane B plane C plane A plane …ABCABCABC… packing …ABABAB… packing [Face Centered Cubic (FCC)] [Hexagonal Close Packing (HCP)]
  • 18. COMPARISON OF CRYSTAL STRUCTURES Crystal 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
  • 19. SINGLE VS POLYCRYSTALS • Single Crystals A single crystal is formed by the growth of a crystal nucleus without secondary nucleation or impingement on other crystals. -Properties vary with direction: anisotropic. -Example: the modulus of elasticity (E) in BCC iron: 200 mm • Polycrystals an object composed of randomly oriented cr ystals, formed by rapid solidification -Properties may/may not vary with direction. -If grains are randomly oriented: isotropic. (Epoly iron = 210 GPa) -If grains are textured, anisotropic.
  • 20. Isotropic: Substances in which measured (physical)properties are independent of the direction of measurement are isotropic. ANISOTROPY: The substance in which physical properties are show variation with changing the direction . Such substance are called anisotropic. A different chemical bonding in all directions is also a condition for anisotropy.
  • 21. 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.