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:
    • Ionic
    • Covalent
    • Metallic
  • Secondary:
    • Van der Waals
    • Hydrogen
  • 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
    • EDE_D is the dissociation energy.
  • Attractive energy E<em>AE<em>A, Repulsive energy E</em>RE</em>R, Net energy ENE_N.

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>3NH<em>3, H</em>2OH</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\alpha 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 106/°C10^{-6}/°C
    • Aluminium Alloys: ~23 x 106/°C10^{-6}/°C
    • Copper Alloys: ~18 x 106/°C10^{-6}/°C
    • Magnesium Alloys: ~26 x 106/°C10^{-6}/°C
    • Titanium Alloys: ~9 x 106/°C10^{-6}/°C
    • Tungsten: ~4.5 x 106/°C10^{-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\alpha = 24 x 10-6/ °C, Δ\DeltaT 180°C
  • Δ\Deltal = α\alpha(T<em>1T</em>iT<em>1-T</em>i) = 61.7 x 24 x 10610^{-6} x 180 = 0.267m

Elastic Modulus

  • Different materials have different elastic modulus values. Material E/MN/m2m^2
  • 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
    • ABCABC…
    • ABABAB…
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 = 222\sqrt{2}R
  • 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\sqrt{3}
  • Co-ordination number = 8.
  • 2 atoms/unit cell: 1 centre + 8 corners x 1/8
  • Close-packed directions: length = 4R = 3\sqrt{3}a

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.

Allotropic Forms of Iron

  • 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\alpha-Fe).
  • At 912°C, α\alpha-Fe changes to GAMMA iron (γ\gamma-Fe) which is FCC (causes contraction).
  • At 1394°C, γ\gamma-Fe reverts to the BCC form (DELTA iron, δ\delta-Fe) stable up to the melting point of iron (1538°C).
  • Upon cooling, the reverse changes occur.
Polymorphism in Tin
  • White (β\beta) tin converts to Gray (α\alpha) tin upon cooling with substantial volume change.

Next Lecture

  • Link between atomic arrangement and properties.