Defects in the regular geometrical arrangement of the atoms in a crystalline solid
Perfect crystal
An idealization, there is no such thing in nature
Defects
May be the results of crystal deformation, rapid cooling from high temperature, or high energy radiation striking the solid
Defects
Influence the mechanical, electrical, and optical behavior of the crystal
Types of crystal imperfections
Point defects
Line defects
Surface defects
Volume defects
Point defects
Lattice errors at isolated points, due to imperfect packing of atoms during crystallization or vibrations of atoms at high temperatures
Equilibrium concentration of point defects
n = N * exp(-Ed/kbT), where n is number of defects, N is number of atomic sites per mole, Ed is free energy required to form defects, kb is Boltzmann's constant, and T is absolute temperature
Vacancies
Simplest point defect, missing atom or vacant atomic site
Frenkel defect
Cation leaving its normal position and moving into an interstitial site
Schottky defect
Removing one cation and one anion from the interior of the crystal and placing them both at an external surface
Compositional defects
Impurity atoms during crystallization, occurring as substitutional or interstitial impurities
Electronic defects
Errors in charge distribution in solids, necessary for electrical conductivity and related phenomena
Line imperfections/dislocations
D defects around which some of the atoms are misaligned, responsible for ductility in materials
Edge dislocations
Vertical plane in the crystal doesn't extend from top to bottom, causing compression above and tension below the slip plane
Screw dislocations
Formed by shearstress, upper region of crystal shifted one atomic distance relative to bottom portion
Burgers vector
Magnitude and direction of lattice distortion associated with a dislocation, perpendicular to dislocation line in edge dislocations and parallel in screw dislocations
Surface imperfections
D defects arising from a change in the stacking of atomic planes on or across a boundary
External surface imperfections
Boundary where bonds do not extend beyond, surface atoms have higher energy
Separate crystals/grains of different orientation in a polycrystalline material, region of imperfect atomic packing
High angle grain boundaries
Orientation difference between neighboring grains is more than 10-15 degrees
Interfaces
Boundary between 2 crystals with different crystalline arrangements or compositions
Tilt boundaries
Low angle boundary with orientation difference less than 10 degrees, composed of edge dislocations
Twin boundaries
Atomic arrangement on one side is a mirror reflection of the other side, occur in pairs
Stacking defects
Fault arising from stacking one atomic plane out of sequence on another, while the lattice on either side is perfect
Volume imperfections
D imperfections like cracks or large vacancies/voids where clusters of atoms are missing
Technically important properties like mechanical strength, ductility, crystal growth, magnetic hysteresis, dielectric strength, and semiconductor conduction are greatly affected by crystal imperfections
Diffusion
The process by which atoms move in a material. Many reactions in solids and liquids are diffusion dependent.
Diffusion in solids
Atoms are not fixed at their position but constantly move (oscillate)
Diffusion is difficult in solids due to bonding and requires time, external energy to mobilize the atoms
Diffusion couple
Joining bars of two different metals together so that there is intimate contact between the two faces, then heating and cooling to observe interdiffusion
Interdiffusion
The process whereby atoms of one metal diffuse into another
Self-diffusion
Atoms within one material exchanging positions
Diffusion mechanisms
1. Vacancy diffusion
2. Interstitial diffusion
Vacancy diffusion
Involves the interchange of an atom from a normal lattice position to an adjacent vacant lattice site or vacancy
Diffusing atoms and vacancies exchange positions, so diffusion of atoms in one direction corresponds to motion of vacancies in the opposite direction
Interstitial diffusion
Atoms migrate from an interstitial position to a neighboring one that is empty
Found for interdiffusion of impurities like hydrogen, carbon, nitrogen, and oxygen which have atoms small enough to fit into interstitial positions
Host or substitutional impurity atoms rarely form interstitials and do not normally diffuse via this mechanism
Interstitial diffusion occurs much more rapidly than diffusion by the vacancy mode, since the interstitial atoms are smaller and more mobile
There are more empty interstitial positions than vacancies, so the probability of interstitial atomic movement is greater than for vacancy diffusion
Factors that influence diffusion
Diffusion mechanism (substitutional vs interstitial)
Temperature
Type of crystal structure of the host lattice
Type of crystal imperfections (diffusion faster along grain boundaries and dislocation lines)
Excess vacancies
Concentration of diffusing species
Steady-state diffusion
Diffusion that takes place at a constant rate, where the number of moles of particles crossing a given interface is constant with time
Unsteady-state (non-steady state) diffusion
Diffusion where the rate is a function of time, so the rate of change of concentration with distance varies with time