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Module 3: The structure of crystalline solids

  • Fundamental Concepts

    • Atoms in crystalline solids are positioned in orderly and repeated patterns that are in contrast to the random and disordered atomic distribution found in noncrystalline or amorphous materials

  • Unit cells

    • Crystal structures are specified in terms of parallelepiped units cells, which are characterized by geometry and atom positions within

  • Metallic crystal structures

    • Most common metals exist in at least one of three relatively simple crystal structures:

      • Face-centered cubic (FCC), which has a cubic unit cell

        Image shows 3 representations of the face-centered cubic crystal structure. The fist image shows atoms in a unit cell represented by halves or quarters of spheres arranged in a cube. The second image shows circles connected by lines forming a cube with additional circles in the center of each cube face. The third image shows a larger cube of spheres with a small cube highlighted to indicate a unit cell.
      • Body-centered cubic (BCC), which also has cubic unit cell

        Image shows 3 different representations of a body-centered cubic crystal structure.
      • Hexagonal close-packed, which has a unit cell of hexagonal symmetry

        Image shows 2 different representations for the hexagonal close-packed crystal structure.
    • Two features of a crystal structure are

      • Coordination number - the number of nearest-neighbor atoms

      • Atomic packing factor - the fraction of solid sphere volume in the unit cell

  • Density computations

    • The theoretical density of a metal is a function of the number of equivalent atoms per unit cell, the atomic weight, unit cell volume, and Avogadro’s number

  • Polymorphism and allotropy

    • polymorphism is when a specific material can have more than one crystal structure. Allotropy is polymorphism for elemental solids

  • Crystal systems

    • used to classify crystal structures on the basis of unit cell geometry

    • unit cell edge lengths and interaxial angles

    • there are seven crystal systems: cubic, tetragonal, hexagonal, orthorhombic, rhombohedral (trigonal), monoclinic, and triclinic

  • Point coordinates

    • crystallographic points, directions, and planes are specified in terms of indexing schemes

    • The basis for the determination of each index is a coordinate axis system defined by the unit cell for the particular crystal structure

  • Crystallographic directions

    • the location of a point within a unit cell is specified using coordinated that are fractional multiples of the cell edge lengths

    • directional indices are computed in terms of differences between vector head and tail coordinates

  • Crystallographic planes

    • for hexagonal unit cells, a four-index scheme for both directions and planes is found to be more convenient. Directions may be determined using

  • Linear and planar densities

    • crystallographic directional and planar equivalencies are related to atomic linear and planar densities, respectively

    • for a given crystal structure, planes having identical atomic packing yet different Miller indices belong to the same family

  • Close-packed crystal structures

    • both FCC and HCP crystal structures may be generated by the stacking of close-packed planes of atoms on top of one another. with this scheme A, B, and C denote possible atom positions on a close-packed plane

      • the stacking sequence for HCP is ABABAB…

      • the stacking sequence for FCC is ABCABCABC…

  • Single crystals

    • single crystals are materials in which the atomic order extends uninterrupted over the entirety of the specimen; under some circumstances, single crystals may have flat faces and regular geometric shapes

  • Polycrystalline materials

    • the vast majority of crystalline solids

    • composed of many small crystals or grains having different crystallographic orientations

    • a grain boundary is the boundary region separating two grains where there is some atomic mismatch

  • Anisotropy

    • anisotropy is the directionality dependence of properties

    • for isotropic materials, properties are independent of the direction of measurement

  • X-ray diffraction: determination of crystal structures

    • X-ray diffractometry is used for crystal structure and interplanar spacing determinations. A beam of x-rays directed on a crystalline material may experience diffraction (constructive interference) as a result of its interaction with a series of parallel atomic planes.

    • Bragg's law specifies the condition for diffraction of x-rays

  • Noncrystalline solids

    • Noncrystalline solid materials lack a systematic and regular arrangement of atoms or ions over relatively large distances (on an atomic scale). Sometimes the term amorphous is also used to describe these materials.

  • List of symbols

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Module 3: The structure of crystalline solids

  • Fundamental Concepts

    • Atoms in crystalline solids are positioned in orderly and repeated patterns that are in contrast to the random and disordered atomic distribution found in noncrystalline or amorphous materials

  • Unit cells

    • Crystal structures are specified in terms of parallelepiped units cells, which are characterized by geometry and atom positions within

  • Metallic crystal structures

    • Most common metals exist in at least one of three relatively simple crystal structures:

      • Face-centered cubic (FCC), which has a cubic unit cell

        Image shows 3 representations of the face-centered cubic crystal structure. The fist image shows atoms in a unit cell represented by halves or quarters of spheres arranged in a cube. The second image shows circles connected by lines forming a cube with additional circles in the center of each cube face. The third image shows a larger cube of spheres with a small cube highlighted to indicate a unit cell.
      • Body-centered cubic (BCC), which also has cubic unit cell

        Image shows 3 different representations of a body-centered cubic crystal structure.
      • Hexagonal close-packed, which has a unit cell of hexagonal symmetry

        Image shows 2 different representations for the hexagonal close-packed crystal structure.
    • Two features of a crystal structure are

      • Coordination number - the number of nearest-neighbor atoms

      • Atomic packing factor - the fraction of solid sphere volume in the unit cell

  • Density computations

    • The theoretical density of a metal is a function of the number of equivalent atoms per unit cell, the atomic weight, unit cell volume, and Avogadro’s number

  • Polymorphism and allotropy

    • polymorphism is when a specific material can have more than one crystal structure. Allotropy is polymorphism for elemental solids

  • Crystal systems

    • used to classify crystal structures on the basis of unit cell geometry

    • unit cell edge lengths and interaxial angles

    • there are seven crystal systems: cubic, tetragonal, hexagonal, orthorhombic, rhombohedral (trigonal), monoclinic, and triclinic

  • Point coordinates

    • crystallographic points, directions, and planes are specified in terms of indexing schemes

    • The basis for the determination of each index is a coordinate axis system defined by the unit cell for the particular crystal structure

  • Crystallographic directions

    • the location of a point within a unit cell is specified using coordinated that are fractional multiples of the cell edge lengths

    • directional indices are computed in terms of differences between vector head and tail coordinates

  • Crystallographic planes

    • for hexagonal unit cells, a four-index scheme for both directions and planes is found to be more convenient. Directions may be determined using

  • Linear and planar densities

    • crystallographic directional and planar equivalencies are related to atomic linear and planar densities, respectively

    • for a given crystal structure, planes having identical atomic packing yet different Miller indices belong to the same family

  • Close-packed crystal structures

    • both FCC and HCP crystal structures may be generated by the stacking of close-packed planes of atoms on top of one another. with this scheme A, B, and C denote possible atom positions on a close-packed plane

      • the stacking sequence for HCP is ABABAB…

      • the stacking sequence for FCC is ABCABCABC…

  • Single crystals

    • single crystals are materials in which the atomic order extends uninterrupted over the entirety of the specimen; under some circumstances, single crystals may have flat faces and regular geometric shapes

  • Polycrystalline materials

    • the vast majority of crystalline solids

    • composed of many small crystals or grains having different crystallographic orientations

    • a grain boundary is the boundary region separating two grains where there is some atomic mismatch

  • Anisotropy

    • anisotropy is the directionality dependence of properties

    • for isotropic materials, properties are independent of the direction of measurement

  • X-ray diffraction: determination of crystal structures

    • X-ray diffractometry is used for crystal structure and interplanar spacing determinations. A beam of x-rays directed on a crystalline material may experience diffraction (constructive interference) as a result of its interaction with a series of parallel atomic planes.

    • Bragg's law specifies the condition for diffraction of x-rays

  • Noncrystalline solids

    • Noncrystalline solid materials lack a systematic and regular arrangement of atoms or ions over relatively large distances (on an atomic scale). Sometimes the term amorphous is also used to describe these materials.

  • List of symbols

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