ES195 Materials for Engineering Flashcards
5 “families” of materials
Metals/alloys (Gold, Steel, Cu alloys)
Ceramics (Alumina, Silicon carbide)
Polymers (Polyester, phenolic)
Glasses (soda glass, borosilicate)
Rubbers (Silicones, EVA)
Hybrids combine 2 or more e.g. GFRP, composites
Purpose of selection methodology
Material properties vary enormously
Multiple factors affect design choice
Function - loading, environment its in.
Commercial - availability of raw materials, required manufacturing volume
Environmental - impact of different materials e.g. embodied energy, pollutants
Three way relationship
Between properties, processing and structure
In manufacturing, we deliberately change
compositions and thermo-mechanically
process materials to change their
structure and properties
Material structures
Crystalline/polycrystallaline - long range order
Amorphous - short range order
Typical values for elastic modulus
Steel ≈ 200GPa
Al alloys ≈ 70 GPa
Ti alloys ≈ 110 Gpa
Ball and spring model of elasticity
Material in tension, bonds stretch and atoms move apart, vice versa for compression.
Also represents how spring gets narrower in the middle
εz = -νεy (poisons ratio)
Primary vs secondary bonds
Primary
Ionic, covalent, metallic
Secondary
Van Der walls (dipolar attraction between uncharged atoms)
Hydrogen - dipole attraction between bonded hydrogen and neighbouring ions
Structure of diff bonding types
Ionic - highly ordered, simple structure e.g. cubic. Stuff, strong and brittle
Covalent - highly ordered, often complex, stiff strong and brittle
Metallic - complex, alloying possible, variety of structures, moderate stiffness, variety of strength and ductility
Why covalent bonds easier to deform
Materials deform when defects propagate through them. Defects move easier along a line/simple plane. Easier in a cubic (ionic crystal) rather than a complex structure (covalent)
Directions denoted by
Square brackets
Crystalline structure
Atoms situated in repeated, periodic array over large distances, 3d pattern, each atom bonded to nearest neighbour
For those that do not crystallize, this long-range atomic order is absent; these non-crystalline
or amorphous materials
What type of materials from crystalline structure
All metals, many ceramics and certain polymers (under normal solidification conditions)
Atomic hard sphere model
Spheres representing nearest neighbour atoms touching each other
Lattice
“lattice” means a three-dimensional array of
points coinciding with atom positions (or
sphere centres).
Unit cell
The unit cell is the basic structural unit of the crystal structure.
Chosen to represent the
symmetry of the crystal structure,
wherein all the atom positions in the
crystal may be generated by
translations of the unit cell integral
distances along each of its edges
Atomic bonding in metallic crystal structures
Metallic and nondirectional, leads to relatively large numbers of nearest neighbours and dense atomic packings for most metallic crystal structures. Also in hard model, each sphere represents an ion
Derive a in terms of r, apf and coordination number for FCC and BCC
Also effective number of atoms hcp
FCC - a=2√2r APF 0.74 cn 12
BCC - a = 4√3r/3 APF 0.68 cn 8
effective atoms FCC 4 BCC 2
6 for hcp
Polymorphism and allotropy + examples
Polymorphism - metals/non metals having more than one crystal structure
Allotropy is when found in elemental solids
Carbon- graphite is stable polymorph, diamond under high pressure
Pure iron BCC at room temp, FCC at 912C
Equivalent directions
Spacing along each atom is same along direction
Grain boundary
Atomic mismatch within the region where two grains meet; this area, called a grain boundary
Grains have same lattice structure but may be oriented differently
Anisotropy
Properties of single crystals depending on direction in which measurement is taken from
For polycrystalline materials, each crystal grain is anisotropic, but when a specimen is taken the aggregate behaves isotropically
Sometimes grains have preferential crystallographic orientation - material is said to have a texture (aka fibre)
Crystalline defect
A lattice irregularity having one or more of its dimensions on the
order of an atomic diameter.