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Crystal structure of metal


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Crystal structure of metal

  1. 1. 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.
  2. 2. 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.
  3. 3. A crystalline material is one in which the atoms are situatedin an orderly, repeating pattern extending in all threedimension .i.e.Nacl ,CsF etc.crystalline solids depend on the crystal structure of thematerial, the manner in which atoms, ions, or molecules arespatially(three dimension) arranged.lattice is used in the context of crystal structures; in thissense lattice means a three-dimensional array of pointscoinciding with atom positions (or sphere centers).Amorphous solid is one in which the atom are not situatedin an orderly, repeating pattern. i.e. glass , rubber, plastic etc.Amorphous solid don’t have sharp melting point that iswhy particle of glass soften over temperature range.
  4. 4. ENERGY AND PACKING  ENERGY AND PACKING • Non dense, random packingDense, regular-packed structures tend to have lower energy
  5. 5. Crystalline solid Amorphous solid
  6. 6.  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.
  7. 7. • 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.
  9. 9. 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)
  10. 10. 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.
  11. 11. 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
  12. 12. 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.
  13. 13. 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
  14. 14. 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
  15. 15. Hexagonal Close-Packed Structure (HCP)• ABAB... Stacking Sequence• 3D Projection • 2D Projection A sites Top layerc 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
  16. 16. Close packed crystals A plane B plane C plane A plane …ABCABCABC… packing …ABABAB… packing[Face Centered Cubic (FCC)] [Hexagonal Close Packing (HCP)]
  17. 17. COMPARISON OF CRYSTALSTRUCTURESCrystal structure coordination # packing factor close packed directionsBody Centered Cubic (BCC) 8 0.68 body diagonalFace Centered Cubic (FCC) 12 0.74 face diagonalHexagonal Close Pack (HCP)12 0.74 hexagonal side
  18. 18. 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.
  19. 19. Isotropic:Substances in which measured (physical)properties are independentof 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.
  20. 20. 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.