Flashcards for Chapter 1: Crystal Structures of Metals

Chapter 1: Crystal Structures of Metals

Nature of Metals
  • Characteristics:

    • Metals are typically hard, tough, ductile, deformable, and conductive (thermal and electrical).

    • Conductivity hierarchy: Hardness: Polymer < Metal < Ceramic

    • Toughness: Ceramic < Metal < Polymer

    • Melting Point: Polymer < Metal < Ceramic

    • Thermal Conductivity: Ceramic < Polymer < Metal

    • Electrical Conductivity: Ceramic < Polymer < Metal

  • Atomic Arrangement:

    • The properties of metals are significantly influenced by the arrangement of atoms in three-dimensional space.

    • Certain metals exhibit soft-hard magnetic properties.

Atomic Structure
  • Components of Atoms:

    • Consists of a nucleus (positively charged, made of protons and neutrons) and electrons (negatively charged, orbiting around the nucleus).

    • Protons = Electrons in neutral atoms; different chemical elements have different proton counts.

  • Energy Levels:

    • Electron configurations across various energy levels contribute to different physical properties.

Electron Orbitals
  • Shapes of Electron Orbitals:

    • s subshell: Spherical density distribution

    • p subshell: Dumbbell-shaped

    • d and f orbitals: More complex shapes

  • Electron Probability:

    • Orbitals define the 3D regions where electrons are likely located, impacting bonding and material properties.

Free Electron Model
  • Electrons in metals are modeled as free-moving; they form a 'sea of electrons' that moves amongst fixed positive metal ions.

  • This electron behavior affects mechanical strength, ductility, thermal and electrical resistivity, and conductivity.

Crystal Structures of Metals
  • Crystal Lattice:

    • Comprised of unit cells that repeat to create a 3D structure, determining the physical arrangement of atoms.

  • Unit Cell:

    • Defined by principal axes (x, y, z) and characterized by 6 lattice parameters: lengths (a, b, c) and angles (α, β, γ).

    • For cubic structures: a = b = c and eta = eta = eta = 90^{ ext{o}}.

  • Calculation of Lattice Parameters:

    • Example of Iron (Fe): Given a = 0.287 ext{ nm}, the number of unit cells in 1 cm is calculated as follows:
      1 ext{ cm} = 10^{-2} ext{ m} = 3.48 imes 10^7 ext{ unit cells}.

Basic Crystal Structures
  • Types of Structures:

    • Body Centered Cubic (BCC)

    • Face Centered Cubic (FCC)

    • Hexagonal Close Packed (HCP)

  • Example Elements:

    • BCC: a-Fe, Cr, Mo, W

    • FCC: Al, Cu, Pb, Au, Ni

    • HCP: a-Ti, Zn, Mg, Cd

Atomic Packing Factor (APF)
  • Definition:

    • APF = rac{ ext{Total sphere volume}}{ ext{Total unit cell volume}}

  • FCC Example:

    • Total atom contribution: 1/8 at corners + 1/2 at faces = total 4 atoms.

    • ext{Volume calculations:}

    • Unit cell volume, V_c = a^3\

    • Total sphere volume for FCC, V_s = rac{4}{3}
      ho^3 ext{pi} \

    • APF Calculation: ext{APF} = 0.74.

Slip Systems and Plastic Deformation
  • Slip Plane:

    • A plane with a high density of atoms (low-index planes) facilitates easier atomic movement during stress applications.

  • Number of Slip Systems:

    • BCC: 12 slip systems (though not all active)

    • FCC: 12 active slip systems (high ductility)

    • HCP: 3 active slip systems (less ductile)

  • Ductility Significance:

    • Metals that can undergo significant plastic deformation without failing are considered safer for engineering applications.

Summary of Key Concepts
  • Crystal structures in metals primarily include BCC, FCC, and HCP, with FCC and HCP being close-packed structures.

  • Lattice configurations related to the number and arrangement of atoms directly influence the physical and mechanical attributes of the metal.

  • A higher number of active slip systems corresponds to greater ductility, making metals easier to deform without cracking.

References
  • Callister, W. D. Fundamental of Materials Science and Engineering/ an Interactive E. Text, 2001, John Wiley & Sons, Inc., New York.