All Study Guides Crystallography Unit 4
💎 Crystallography Unit 4 – Crystal Structures and PackingCrystal structures and packing are fundamental concepts in crystallography, exploring how atoms arrange in solids. This unit covers crystal systems, unit cells, symmetry operations, and close packing. Understanding these principles is crucial for predicting and manipulating material properties.
The study delves into Miller indices for describing crystal planes, various types of crystal defects, and practical applications in materials science. X-ray diffraction, electron microscopy, and crystal engineering techniques are explored, highlighting the importance of crystallography in modern technology and research.
Fundamental Concepts
Crystallography studies the arrangement of atoms in crystalline solids
Crystals exhibit long-range order and periodic atomic arrangements
Unit cells are the smallest repeating units that make up a crystal structure
Lattice points represent the locations of atoms or groups of atoms in a crystal
Symmetry plays a crucial role in determining the properties of crystals
Translational symmetry involves the repetition of a unit cell in three dimensions
Point symmetry includes operations such as rotation, reflection, and inversion
Rotation symmetry occurs when a crystal appears unchanged after rotation around an axis
Reflection symmetry exists when a crystal remains unchanged upon reflection across a plane
Types of Crystal Systems
There are seven distinct crystal systems based on the symmetry and shape of the unit cell
Triclinic system has the lowest symmetry with no restrictions on cell parameters
Monoclinic system has one angle (β) not equal to 90° and a ≠ b ≠ c
Orthorhombic system has all angles equal to 90° and a ≠ b ≠ c
Tetragonal system has all angles equal to 90° and a = b ≠ c
Tetragonal crystals often exhibit unique optical and electrical properties
Trigonal (Rhombohedral) system has all angles equal and a = b = c
Hexagonal system has all angles equal to 90°, a = b ≠ c, and γ = 120°
Graphite and many ceramics crystallize in the hexagonal system
Cubic system has the highest symmetry with all angles equal to 90° and a = b = c
Examples of cubic crystals include sodium chloride (NaCl) and diamond
Unit Cells and Lattice Points
A unit cell is the smallest repeating unit that can generate the entire crystal structure through translation
Lattice points are mathematical points representing the locations of atoms or groups of atoms
Primitive unit cells contain only one lattice point, typically at the cell corners
Non-primitive unit cells may have additional lattice points at cell faces or inside the cell
The Bravais lattices describe the 14 unique lattice types based on the seven crystal systems
Cubic system has three Bravais lattices: simple cubic, body-centered cubic, and face-centered cubic
Hexagonal system has one Bravais lattice: hexagonal close-packed
Unit cell parameters (a, b, c, α, β, γ) define the size and shape of the unit cell
Coordination number represents the number of nearest neighbors for each atom in a crystal structure
Symmetry Operations and Elements
Symmetry operations are transformations that leave a crystal unchanged in appearance
Symmetry elements are geometric entities (points, lines, or planes) about which symmetry operations are performed
Identity operation (E) leaves the crystal unchanged and is present in all crystal systems
Rotation axes (1, 2, 3, 4, 6) describe the number of times a crystal can be rotated to coincide with itself
Two-fold rotation axis (2) requires a 180° rotation to achieve self-coincidence
Six-fold rotation axis (6) requires a 60° rotation to achieve self-coincidence
Mirror planes (m) reflect the crystal across a plane, resulting in an identical structure
Inversion centers (i) transform each point (x, y, z) to (-x, -y, -z) through the center of symmetry
Rotoinversion axes combine rotation and inversion operations
Screw axes combine rotation and translation operations
21 screw axis involves a 180° rotation followed by a translation of 1/2 the unit cell length
Close Packing and Coordination Numbers
Close packing describes the most efficient arrangement of atoms in a crystal structure
Hexagonal close packing (HCP) and cubic close packing (CCP) are common close-packed structures
HCP has an ABABAB... stacking sequence of close-packed planes
CCP, also known as face-centered cubic (FCC), has an ABCABCABC... stacking sequence
Coordination number (CN) is the number of nearest neighbors for each atom in a crystal structure
In close-packed structures (HCP and CCP), the coordination number is 12
Octahedral voids in close-packed structures have a coordination number of 6
Tetrahedral voids in close-packed structures have a coordination number of 4
Interstitial sites are empty spaces between atoms where smaller atoms can be accommodated
Octahedral sites are larger and can accommodate larger interstitial atoms compared to tetrahedral sites
Miller Indices and Crystal Planes
Miller indices (hkl) are used to describe the orientation of crystal planes and directions
Crystal planes are denoted by integers h, k, and l, which are the reciprocals of the intercepts on the x, y, and z axes, respectively
(100) plane intersects the x-axis at 1 and is parallel to the y and z axes
(111) plane intersects all three axes at 1
Directions in crystals are denoted by [uvw], where u, v, and w are the components of the direction vector
[100] direction is parallel to the x-axis
[111] direction passes through the opposite corners of the unit cell
Planes and directions with the same symmetry are denoted by {hkl} and , respectively
Miller indices are crucial for understanding the arrangement of atoms and predicting crystal properties
Crystal Defects and Imperfections
Real crystals contain various types of defects and imperfections that deviate from the perfect periodic arrangement
Point defects are localized defects involving one or a few atoms
Vacancies are empty lattice sites where atoms are missing
Interstitials are atoms occupying non-lattice sites between regular atoms
Substitutional defects occur when an atom is replaced by an atom of a different type
Line defects, or dislocations, are irregularities along a line in the crystal structure
Edge dislocations are caused by the insertion or removal of an extra half-plane of atoms
Screw dislocations result from the displacement of atoms in a spiral manner around the dislocation line
Planar defects involve irregularities in the stacking sequence of atomic planes
Stacking faults occur when the regular stacking sequence is disrupted
Twin boundaries separate two mirror-image regions of the crystal
Grain boundaries are interfaces between crystallites (grains) with different orientations in polycrystalline materials
Defects can significantly influence the mechanical, electrical, and optical properties of crystals
Practical Applications in Materials Science
Crystallography plays a vital role in understanding and designing materials with desired properties
X-ray diffraction (XRD) is a powerful technique for determining crystal structures and identifying phases
Bragg's law (n λ = 2 d sin θ nλ = 2d \sin θ nλ = 2 d sin θ ) relates the wavelength of X-rays to the interplanar spacing and diffraction angle
XRD patterns provide information about lattice parameters, crystal symmetry, and phase composition
Electron microscopy techniques (SEM, TEM) enable the visualization of crystal structures and defects at high resolutions
Structure-property relationships link the atomic arrangement to macroscopic material properties
Mechanical properties (strength, ductility) are influenced by the presence and motion of dislocations
Electrical properties (conductivity, semiconductivity) depend on the electronic band structure determined by the crystal structure
Crystal engineering involves the design and synthesis of functional materials with tailored properties
Pharmaceutical compounds can be engineered to have desired solubility and bioavailability
Metal-organic frameworks (MOFs) are crystalline materials with tunable porosity for gas storage and catalysis applications
Epitaxial growth techniques enable the fabrication of single-crystal thin films for electronic and optoelectronic devices
Molecular beam epitaxy (MBE) allows precise control over the growth of semiconductor heterostructures
Pulsed laser deposition (PLD) is used to grow complex oxide thin films with specific crystal orientations