Introduction Flashcards
Define amorphous and crystalline solids.
Amorphous solids - Locally ordered but no long range order.
Crystalline solids - Periodic structure repeating over long distances.
Name the 9 important Bravais lattices and describe their differences.
Cubic (all edges the same length): Primative (P), Body (I) and Face (F)
Tetragonal (square base but different length): Primative(/simple) and Body
Orthorhombic (all different lengths): Primative, Body, Base-centered and Face
How do you calculate the density of a unit cell?
Find the side that defines the lattice parameter (where the atoms touch) and use the atomic radius to find the lattice parameter. Then find the volume.
Calculate the number of atoms in a cell and find the weight of the cell from the atomic mass. Density can then be found.
Draw each of the miller planes for (100) to (222) for all variations and give the distance between planes for each.
What is the difference between allotropy and polymorphism?
Allotropy is the ability of single atom to form more than one structure in a particular state (e.g. O2 and O3).
Polymorphism is the ability of a compound to form more than one crystal form.
What must be considered when using a metal/compound which has multiple allotropes?
How the volume of the lattice may change when changing between allotropes. The volume per atom of each form can be found to show the percentage volume change.
The properties of the structure will change as well. This is especially true for tin.
Describe the transition between β and α tin.
β tin is a BCT structure stable above 13 degrees and is a good metallic conductor, coordination 8.
α tin is stable below 13 degrees and is a non metallic insulator. The material fractures as the volume changes, coordination 4.
This is problem where tin is being used however the transition occurs over 100s of years.
What is the equation for Braggs law?
How is the difference between planes calculated?
What are systematic absences?
2d sinθ = nλ (n = 1 when using miller indices)
Cubic structures: d2 = a2/(h2 + k2 + l2) where h, k and l are the lattice parameters.
Orthorhombic structures: d-2 = h2/a2 + k2/b2 + l2/c2
If there is a layer of atoms between the planes which are being studied for diffraction then the diffaction angle expected will be absent (100 cancelled by 200).
What planes cause the first angles seen in the diffraction of the primitive, body and face cubic structures?
How does the angle of the diffraction change when the distance between planes increases?
PC: 100
BCC: 110
FCC: 111
When the distance between planes increases, the angle of diffraction angle becomes smaller.
Calculate the angle of diffraction for the planes of Na (BCC) from (100) to (200) and determine which are seen.
λ = 154 pm, a = 423 pm.
(100) θ = 10.488º not seen
(110) θ = 14.918º seen
(111) θ = 18.378º not seen (centre atom isn’t part of the plane)
(200) θ = 21.350º seen
Name and briefly describe the 8 types of defects and state their dimensionality.
Interstitial impurity (0D) - impurity between atoms in the lattice
Self interstitial (0D) - extra atom between atoms in the lattice
Vacancy (0D) - atom removed from the lattice
Substitutional impurity (0D) - atom substituted for an impurity
Group of impurities (1/2D) - multiple substitutional impurities grouped together
Edge dislocation (1D) - extra half plane of atoms added/removed
Vacancy dislocation loop (1/2D) - set of vacancies as a group
Interstitial dislocation loop (1/2D) - interstital atoms forming as a group between the lattice
Describe the two types of defect lines.
Edge - plane is correct when completing a square movement but start location is not the same as the end point.
Screw - Following the defect in a square takes you to the correct site, but in the incorrect plane.
Define grains and grain boundaries.
Grains - areas of well formed crystal
Grain boundaries - defects in a line between grains
Define Schottky and Frenkel defects for ionic lattices.
Schottky - ion and cation pair removed from lattice, the volume is the same but the density is reduced as mass is lost. 2 vacancies are formed.
Frenkel - An ion is moved to form an interstitial. Cation interstitials are much more common as anions are usually larger.
How do defects affect the lattice atoms surrounding it?
Vacancies cause the surrounding atoms to be pulled towards it. Intertitials push away surrounding atoms.
Edge dislocations stress the top and bottom in different ways:
Where an additional atom is present the atoms are compressed - they want to push outwards.
Where an atom is missing there is tension - the atoms want to pull inwards.
What is the equation for the number of defects?
What are the main steps towards its derivation?
nd = Ne-εd/kT
Where nd = number of defects, N = number of sites, εd = energy of defect
k = boltzmann constant, T = temperature
Using G = H - TS, some defects are preffered as entropy favours it.
H = ndεd and S = klnω where ω = the number of microstates which is found by pascals triangle and NCnd. We use the general formula for NCnd.
An approximation is used that is d(Aln(A))/dA = - 1 - lnA.
Assuming N>>nd gives the equation in the form we use.
What happens if 2 Burgers vectors in opposite directions meet?
They annihilate, leaving no defects.
Define an edge and a screw dislocation in terms of Burgers vectors.
Edge dislocation - Burgers vector perpendicular to dislocation/defect (all one plane)
Screw dislocation - Burgers vector is parallel to dislocation/defect (vectors cover one plane
How do dislocation lines minimse the lattice energy? Why does this occur?
They bring lines closer in together to try close the gaps the defects leave behind. Defects also repel each other if the compressions and tensions are on the same side. If they are on opposite sides then they will annihilate.
The elastic energy of a defect is proportional to the Burgers vector, b, squared so 2 seperate defects are better than 2 together.