BME - lecture 2
Basic Materials Engineering Course Notes
Overview
Instructor: Łukasz Kołodziejczyk, Prof. TUL
Institution: Politechnika Łódzka, Institute of Materials Science & Engineering
Email: lukasz.kolodziejczyk@p.lodz.pl
1. Crystalline Solids
A. Structure of Crystalline Solids
Imperfections in Solids
Defects in materials that can influence physical properties.
Dislocations and Strengthening Mechanisms
A focus on how dislocation dynamics can affect material strength.
2. Short-Range Order (SRO) vs. Long-Range Order (LRO)
A. Short-Range Order (SRO)
Found in monoatomic gases or plasma in types of light.
Atoms or ions lack orderly arrangement and randomly fill available space.
Related to amorphous materials (e.g., liquid crystals).
B. Long-Range Order (LRO)
Seen in materials like metals, alloys, ceramics, semiconductors, and some polymers.
Atoms or ions maintain a repetitive, grid-like pattern in three dimensions.
Characterized by an orderly arrangement extending over a length scale of greater than 100 nm.
3. Single Crystal vs. Polycrystalline Materials
Single Crystal Material: Contains only one crystal; properties depend on chemical composition and directional characteristics.
Polycrystalline Material: Composed of multiple crystal grains with different orientations.
Grain Boundaries are regions of misalignment between adjacent crystals.
Properties depend on the characteristics of both the grains and grain boundaries.
4. Amorphous Materials
Defined as materials that exhibit only a short-range order.
Form when the kinetics of manufacturing do not allow periodic arrangements.
Examples: Glass, certain polymers, colloidal gels.
Unique properties arise from their irregular atomic arrangements.
5. Basic Crystallography Terms
A. Lattice
A collection of points in a periodic arrangement, where each point has identical surroundings.
Can be 1D, 2D, or 3D.
B. Motif (Basis)
Group of one or more atoms associated with each lattice point.
C. Crystal Structure
Formed by combining the lattice and motif.
D. Unit Cell
The smallest subdivision of a lattice that retains lattice characteristics; can be stacked to create the whole lattice.
6. Bravais Lattices
There are seven unique crystal systems for three-dimensional space filling:
Cubic
Tetragonal
Orthorhombic
Rhombohedral (Trigonal)
Hexagonal
Monoclinic
Triclinic
There are 14 distinct arrangements known as Bravais lattices.
7. Lattice Parameters
Describe the size and shape of the unit cell:
Dimensions of the sides of the unit cell
Angles between the sides.
8. Metallic Crystal Structures
A. Common Metallic Structures
Most metals are found in three crystal structures: FCC (Face-Centered Cubic), BCC (Body-Centered Cubic), and HCP (Hexagonal Close-Packed).
B. Examples of Metallic Crystals
Aluminum (FCC), Atomic Radius: 0.1431 nm
Molybdenum (BCC), Atomic Radius: 0.1363 nm
Cadmium (HCP), Atomic Radius: 0.1490 nm
Nickel (FCC), Atomic Radius: 0.1246 nm
Chromium (BCC), Atomic Radius: 0.1249 nm
Platinum (FCC), Atomic Radius: 0.1387 nm
Cobalt (HCP), Atomic Radius: 0.1253 nm
Silver (FCC), Atomic Radius: 0.1445 nm
Copper (FCC), Atomic Radius: 0.1278 nm
Tantalum (BCC), Atomic Radius: 0.1430 nm
Gold (FCC), Atomic Radius: 0.1442 nm
Titanium (α) (HCP), Atomic Radius: 0.1445 nm
Iron (α) (BCC), Atomic Radius: 0.1241 nm
Tungsten (BCC), Atomic Radius: 0.1371 nm
Lead (FCC), Atomic Radius: 0.1750 nm
Zinc (HCP), Atomic Radius: 0.1332 nm
9. Number of Atoms per Unit Cell
Each unit cell's definition includes specific numbers of lattice points, with identifiable positions:
Corner atoms
Body-centered atoms
Face-centered atoms
Each corner point can be shared by multiple unit cells.
A. Calculation Formula
N = Ni + rac{Nf}{2} + rac{N_c}{8}
Where:
$N_i$ = number of interior atoms
$N_f$ = number of face atoms
$N_c$ = number of corner atoms
$X$ = 8 for cubic and 6 for hexagonal forms.
10. Allotropic or Polymorphic Transformations
Materials having more than one crystal structure are categorized as allotropic or polymorphic.
This applies to both pure elements and compounds.
11. Isotropic and Anisotropic Behavior
A. Definitions
Isotropic Material: Properties are identical in all directions.
Anisotropic Material: Properties depend on the crystallographic direction measured.
B. General Trends
Most polycrystalline materials display isotropic properties.
Single crystals or oriented grains exhibit anisotropic mechanical, optical, magnetic, and dielectric properties.
12. Imperfections in Atomic and Ionic Arrangements
Engineered materials contain defects which impact properties:
Point Defects
Line Defects (Dislocations)
Surface Defects
13. Point Defects
Localized disruptions in the crystal structure.
Three significant types include:
Vacancy: An atom or ion missing from its normal site.
Interstitial Atom: An extra atom inserted into vacant positions in the crystal.
Substitutional Atom: An atom replaced by a different type.
A. Impurities and Dopants
Impurities: Naturally present elements or compounds.
Dopants: Elements added intentionally in known concentrations for beneficial effects.
14. Vacancies
Defined as when an atom or ion is absent.
Produce increased randomness, raising entropy and boosting thermodynamic stability.
A. Formation
of vacancies can occur during phase transitions, such as melting or solidification, which allow materials to adapt to changing environmental conditions.
15. Interstitial Defects
Form when an extra atom is inserted into a normally unoccupied crystal position.
They hinder dislocation movement, thereby enhancing material strength.
Their concentration stays relatively steady regardless of temperature changes.
16. Substitutional Defects
Arise from replacing one atom with a different type in the lattice.
May alter surrounding interatomic distances, often enhancing the material's strength.
17. Dislocations
Line imperfections formed during solidification or plastic deformation.
Crucial for understanding deformation and strength in materials, especially metals.
A. Types of Dislocations
Screw Dislocation
Edge Dislocation
Mixed Dislocation
18. Edge Dislocations
Conceptualized by cutting a perfect crystal and filling a space with an extra atomic plane.
A. Burgers Vector
The Burgers vector ($ extbf{b}$) indicates displacement created by an edge dislocation, and is perpendicular to the edge dislocation line.
19. Screw Dislocations
Formed by skewing a crystal, creating a displacement indicated by the Burgers vector ( extbf{b}) parallel to the dislocation's axis.
20. Mixed Dislocations
Characteristics of both edge and screw dislocations, with a Burgers vector neither perpendicular nor parallel.
21. Surface Defects
Defects that separate areas with different structures or orientations:
Interfacial Defects
External Surfaces
Grain Boundaries
Phase Boundaries
Twin Boundaries
Stacking Faults
22. Dislocations and Strengthening Mechanisms
Understanding these mechanisms is essential for designing properties such as strength and toughness in metals and composites.
23. Plastic Deformation vs. Dislocation Motion
Plastic deformation involves the movement of numerous dislocations.
The process of deformation termed slip occurs along slip planes.
24. Analogy with Caterpillar
The motion of dislocations can be likened to a caterpillar moving.
25. Formation of a Step
Illustrated by the motion of edge and screw dislocations with respect to applied shear stress ($ au$).
26. Dislocation Density
Refers to the number of dislocations per unit area or volume of a material.
A. Expression
Measured in millimeters of dislocation per cubic millimeter or equivalent to dislocations per square millimeter.
Values include:
Carefully solidified metals: approx. $10^3$ dislocations/mm$^3$
Heavily deformed metals: $10^9$ to $10^{10}$ dislocations/mm$^3$
Deformed metals post-heat treatment: $10^5$ to $10^6$ dislocations/mm$^3$
Ceramic materials: $10^2$ to $10^4$ dislocations/mm$^3$
Silicon single crystals: $0.1$ to $1$ dislocations/mm$^3$
27. Case Study: Dislocation Interactions
Focus on dislocation annihilation in a perfect crystal structure.
28. Slip Systems
Dislocations have preferred planes for movement due to atomic arrangements.
A. Definitions
Slip Plane: Plane with highest atomic packing density.
Slip Direction: Direction along the plane that is most densely packed with atoms.
29. Conclusion
On a microscopic level, plastic deformation corresponds to the MOTION OF DISLOCATIONS in reaction to applied shear stress.