MEC207 Metals Lecture 4 Notes
Review of Lecture 3
- Briefly looked at metal powder processing routes, their applicability, advantages, disadvantages and future developments.
Properties
- Material properties are influenced by atomic arrangement and microstructure.
- Defining properties is essential.
Microstructure
- Microstructure varies at different scales as shown in the example of Aluminium alloy 2024.
- Examples include:
- Single crystal (0.4 nm)
- Grain (100 μm)
Scale and Length
- Scale and length are crucial in materials science.
- Understanding atomic scale phenomena helps in comprehending micro or macroscale behavior.
Mechanical Properties
- Mechanical properties describe a metal's response to applied force.
- Important mechanical properties:
- Stiffness
- Strength
- Ductility
- Hardness
- Toughness
- Fatigue
- Creep
- Except for stiffness, these properties are sensitive to composition, microstructure, and temperature.
- Strength and toughness will be discussed later.
Bonding
- Properties related to bond energy.
Types of Bonding
- Primary:
- Secondary:
- Primary bonds are strong, resulting from transfer or sharing of outer orbital electrons.
- Secondary bonds are weak.
Bond Energy Curve
- Dependence of potential energy on atomic spacing.
- Long-range attraction versus short-range repulsion.
- Superposition of attractive and repulsive potentials.
- The bond-energy curve determines engineering properties:
- Melting temperature
- Elastic modulus (stiffness)
- Thermal expansion coefficient
- Potential Energy E
- ED is the dissociation energy.
- Attractive energy E<em>A, Repulsive energy E</em>R, Net energy EN.
Bonding Types and Properties
- Ionic:
- High melting point.
- Examples: NaCl, MgO.
- Covalent:
- High melting point.
- Examples: Si, C(diamond).
- Metallic:
- Variable melting point.
- Examples: Al, Fe, W, Hg
- Van der Waals:
- Low melting point.
- Example: Ar.
- Hydrogen:
- Low melting point.
- Examples: NH<em>3, H</em>2O
Melting Point vs Binding Energy
- The graph shows the relationship between melting point (K) and binding energy (kJ/mol).
Thermal Expansivity
- Thermal expansion results from changes in average separation between atoms or molecules.
- As temperature increases, the amplitude of molecular vibrations increases, causing expansion.
Coefficient of Linear Expansion
- α is the coefficient of linear expansion and depends on the material.
- Area and volume expansion also occur.
Coefficient of Thermal Expansion Values
- Examples:
- Steels: ~12 x 10−6/°C
- Aluminium Alloys: ~23 x 10−6/°C
- Copper Alloys: ~18 x 10−6/°C
- Magnesium Alloys: ~26 x 10−6/°C
- Titanium Alloys: ~9 x 10−6/°C
- Tungsten: ~4.5 x 10−6/°C
Thermal Expansion and Bonding Energy
- The graph illustrates how the coefficient of thermal expansion relates to bonding energy (kJ/mol).
Thermal Expansion Example
- DAOB-D Length 61.7m, AA2618, α = 24 x 10-6/ °C, ΔT 180°C
- Δl = α(T<em>1−T</em>i) = 61.7 x 24 x 10−6 x 180 = 0.267m
Elastic Modulus
- Different materials have different elastic modulus values. Material E/MN/m2
- Examples:
- Rubber: 1
- Polythene/nylon: 400
- Plywood: 7 000
Stiffness
- Bond energy only partially explains differences in stiffness because there is another factor that needs to be considered.
Atomic Packing
- Packing of atoms in metals contributes to macroscopic stiffness.
- Simple cubic packing.
- Close-packed directions.
- Close packed atoms (2D plane) (many engineering metals).
3D Close-Packed Structures
- Plane A, Plane B, Plane C
Close-Packed Hexagonal (c.p.h.) Structure
- The stacking sequence ABAB… corresponds to the close-packed hexagonal structure (e.g. Mg, Zn, Ti).
Face-Centred Cubic (f.c.c.) Structure
- The stacking sequence ABCABC… corresponds to the face-centred cubic structure (e.g. Al, Cu, Ni, Fe-y).
Atomic Arrangement and Crystallographic Structure
- Atomic arrangement influences crystallographic structure.
Simple Cubic Structure
- Close packed directions are cube edges
- Lattice parameter = a = 2R
- Co-ordination number = 6
- 1 atom/unit cell: 8 corners x 1/8
- Rare due to low packing density, Only Polonium (Po) has this structure; No "metals" have this structure.
Face Centred Cubic Structure (fcc)
- Atoms touch each other along face diagonals. e.g: Al, Cu, Au, Pb, Ni, Pt, Ag, Pd
- Lattice parameter = a = 22R
- Co-ordination number = 12
- 4 atoms/unit cell: 6 face x 1/2 + 8 corners x 1/8
Body Centred Cubic Structure (BCC)
- BCC is not a close packed structure
- Atoms touch each other along cube diagonals. e.g. Cr, W, Fe (a), Ta, Mo
- Lattice parameter = a = 4R/3
- Co-ordination number = 8.
- 2 atoms/unit cell: 1 centre + 8 corners x 1/8
- Close-packed directions: length = 4R = 3a
Importance of Atomic Arrangement
- Atomic arrangements of atoms and ions determine the microstructure and properties of a material.
- Controls tensile behavior, fracture behavior, and density.
- Materials with similar atomic arrangements behave similarly when loaded.
- Crystal structure can cause anisotropy in properties.
Polymorphism & Allotropy
- Polymorphism: a material may have more than one crystal structure (i.e. BCC, FCC & HCP).
- A material that shows polymorphism exists in more than one type of space lattice in the solid state.
- Allotropy: Polymorphic change is reversible with temperature or pressure.
- The prevailing crystal structure depends on both temperature and external pressure.
- Iron can exist in more than one crystal structure.
- Changes are reversible.
- Different allotropes are designated with Greek letters.
- Low temperature iron is BCC (ALPHA iron, α-Fe).
- At 912°C, α-Fe changes to GAMMA iron (γ-Fe) which is FCC (causes contraction).
- At 1394°C, γ-Fe reverts to the BCC form (DELTA iron, δ-Fe) stable up to the melting point of iron (1538°C).
- Upon cooling, the reverse changes occur.
Polymorphism in Tin
- White (β) tin converts to Gray (α) tin upon cooling with substantial volume change.
Next Lecture
- Link between atomic arrangement and properties.