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Chapter 3: The Structure of Crystalline Solids
Issues to Address
Atoms and Solid Structures: Focus on how atoms assemble into solid structures, particularly metals.
Density and Structure: Explore how the density of a material relates to its structure.
Variation in Material Properties: Discuss when material properties may vary with the sample's orientation.
Outline of Chapter 3
Fundamental Concepts
Unit Cells
Metallic Crystal Structure
Density and Polymorphism
Crystal Systems
Point Coordinates, Crystallographic Planes, and Directions
Linear and Planar Densities
Crystalline and Nanocrystalline Materials
Energy and Packing
Types of Packing:
Non-Dense, Random Packing: Atoms arranged randomly.
Dense Regular Packing: Atoms arranged regularly, leading to lower energy configurations.
Atomic and Crystal Structure
Atomic Structure: Refers to the number of protons and neutrons in the nucleus and the arrangement of electrons.
Crystal Structure: Pertains to the arrangement of atoms, ions, or molecules in crystalline materials.
Materials and Packing
Crystalline Materials:
Atoms pack in periodic, three-dimensional arrays.
Examples: Metals, many ceramics, some polymers.
Non-Crystalline Materials:
Atoms lack periodic packing.
Typical in complex structures and materials cooled rapidly (e.g., amorphous SiO2).
Unit Cell
Definition: The smallest repeating structural unit of a crystalline solid.
Characteristics:
Defines the symmetry of a crystal structure.
Atoms in the crystal can be generated by translations of the unit cell.
Models: Hard-sphere model, reduced-sphere model.
Lattice
Lattice Definition: A three-dimensional array of points corresponding to atomic positions.
Lattice Points: Can contain atoms, molecules, or ions.
Metallic Crystals
Dense Packing:
Typically consist of one element, leading to similar atomic radii.
Metallic bonding is directional and lacks many restrictions compared to ionic or covalent bonds.
Common Crystal Structures: Simple cubic (SC), body-centered cubic (BCC), face-centered cubic (FCC), hexagonal close-packed (HCP).
Simple Cubic Structure (SC)
Coordination Number (C.N.): 6 nearest neighbors.
Density: Rare due to poor packing; an example is polonium (Po).
Body Centered Cubic Structure (BCC)
Coordination Number: 8, with close-packed directions along cube diagonals.
APF (Atomic Packing Factor): 0.68.
Face Centered Cubic Structure (FCC)
Coordination Number: 12, with close-packed directions along face diagonals.
APF: 0.74, includes 4 atoms per unit cell.
Hexagonal Close-Packed Structure (HCP)
Coordination Number: 12, with ABAB stacking sequence.
APF: 0.74.
Alloys and Compounds
Similar Structures: Often have close-packed structures.
Example: Sodium chloride (NaCl).
Theoretical Density
Density Calculation:
Example of Copper: Theoretical density ( Cu = 8.89 g/cm³) compared with actual density ( Cu = 8.94 g/cm³).
Material Classes and Densities
Metals: Close-packing and large atomic mass.
Ceramics: Less dense packing and lighter elements.
Polymers: Poor packing and lighter elements (C, H, O).
Composites: Intermediate density values.
Single Crystals vs. Polycrystals
Single Crystals: Anisotropic properties (vary with direction).
Polycrystals: Isotropic properties if grains are randomly oriented, or anisotropic if textured.
Allotropy and Polymorphism
Allotropy: The ability of an element to exist in multiple crystal structures (e.g., iron).
Example: Iron transitions between bcc and fcc.
Polymorphism: Occurs when compounds exhibit multiple crystalline forms (e.g., carbon).
Crystal Systems
Seven Crystal Systems: Based on geometrical properties of the unit cell.
Cubic: a = b = c; α = β = γ = 90°
Tetragonal: a = b ≠ c; α = β = γ = 90°
Orthorhombic: a ≠ b ≠ c; α = β = γ = 90°
Rhombohedral: a = b = c; α = β = γ ≠ 90°
Hexagonal: a = b ≠ c; α = β = 90°, γ = 120°
Monoclinic: a ≠ b ≠ c; α = γ = 90°; β ≠ 90°
Triclinic: a ≠ b ≠ c; α ≠ β ≠ γ.
Point Coordinates and Crystallographic Directions
Point Coordinates: Specified using fractional lengths of unit cell dimensions.
Crystallographic Directions: Defined by vectors enclosed in square brackets (e.g., [uvw]).
Crystallographic Planes
Defined by Miller indices (hkl) except in the hexagonal system.
Family of planes represented as sets (e.g., {100}).
X-Ray Diffraction (XRD)
XRD Basics: Utilizes the diffraction of X-rays through crystal planes to determine structure.
Bragg's Law: Relates the angle of diffraction to interplanar spacing and wavelength.
Summary
Materials can form crystalline or amorphous structures, and their density can be predicted based on atomic properties and geometry.
Material properties exhibit anisotropic behavior in single crystals but may be isotropic in polycrystalline materials with random orientation.