Materials Science Lecture #3
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Materials Science
Lecture #3
Prof. David W. Steuerman
September 16, 2009
Topics: More Defects
Types of Solids
Packing of Spheres
Department of Chemistry
University of Victoria
Crystals and Defects
Last Time: 0-D Defects, Diffusion,…
Au
Cu
Antisite Schottky Defect
Real crystals have defects.
Screw Dislocation
Last Time: 1-D Defects
Hard to see - think spiral ham
3
Dislocation Density
Definition: ρd = ld/V units of cm-2
total dislocation length per unit volume
Typical #’s: 108 to 1010 cm-2 for metals
10 to 105 cm-2 for semiconductors
Why the disparity?
4
2-Dimensional Defects
Grain Boundary: separation of regions with the same
crystal structure but different orientations
Grain Boundaries in Iron
5
Comment on Magnets
Magnetic Domains: separation of regions with the same
crystal structure and orientation but
different magnetic orientations
Crystal with no
structural defects
6
Comment on Magnets
Magnetic Domains: separation of regions with the same
crystal structure and orientation, but
different magnetic orientations
Disorder in
electron spin
7
3-Dimensional Defects
Precipitates or Agglomerates: More of a concern in more
complex materials with multiple constituents.
3-D Aggregate of Atoms
8
3-Dimensional Defects
Example: High Resolution Transmission Electron Microscopy
of Nb-doped SrTiO3
http://www.iwe.rwth‐aachen.de/emrl/r_p_1.html 9
Classification of Defects
Zero - Dimensional One - Dimensional
- Intrinsic/native point defects - Dislocation
- Impurity atoms - Disinclination
Two - Dimensional Three - Dimensional
- Stacking Faults, - Precipitates
- Grain boundaries, twin boundaries - Inclusions
- Domain walls (magnetic) - Agglomerates of point defects
10
What holds solids together?
4 Fundamental Forces:
Range (m) Relative Magnitude
Strong 10-15 1
Electromagnetic ∞ 10-2
Weak 10-18 10-6
Gravitational ∞ 10-36
Electromagnetic interactions govern molecules and materials.
Classification of Solids
Ionic Van der Waals
Covalent Metallic
Ionic Bonding
‐ + 2 Isolated Ions
−e 2
−e 2
F= V=
4πε o r 2
4πε o r
− e2 (1.60 × 10−19 C ) 2
V= =
4πε o r 4π (8.85 × 10−12 F × m −1 )(0.236 × 10−9 m)
= - 9.75 x 10-19 J
Potential Energy for a
= - 6.10 eV single NaCl molecule
Reminder: Work, Forces, and Potential
Concept: V ( r ) = − ∫ F ( r )dr From Introductory Physics
Conservative Force - Work done by a force on a particle is only
dependent upon the initial and final position.
rf
W = − ∫ F ( r )dr = −V f + Vi
ri
rf
ΔE = −W = − ∫ F ( r )dr
ri
r Rearrange
V ( r ) = − ∫ F ( r )dr F ( r ) = − dVdrr )
(
∞
At ∞ potential is 0.
Ionic Bonding Continued
Consider 1D Array ‐ + ‐ + ‐ + ‐ +
of Ions:
Consider 3D Array How many next
of Ions: nearest neighbors?
e2
E = −6 ×
4πε o ao 6 nearest neighbors of Na
e2 12 next nearest
E = +12 ×
4πε o ao 2 neighbors of Cl
e2 8 nearest neighbors of Na
E = −8 ×
4πε o ao 3
Ionic Bonding
Consider 3D Array
of Ions:
e2 ⎡ 12 8 ⎤
E= × ⎢6 − + .......⎥
4πε o ao ⎣ 2 3 ⎦
Convergent Infinite Series
e2 e2
E = −M d = −1.748
4πε o ao 4πε o ao
Madelung Constant
Van der Waals Interactions
Van der Waals Forces: interaction of dipoles
3 Categories:
Can you name them and
dipole-dipole
give an example of each?
dipole-induced dipole
induced dipole-induced dipole
Recall from Electrostatics:
Coulombic Potentials scale as 1/R
Dipole Potentials scale as 1/R2
Lennard-Jones Potential
Model applies to interacting pairs of neutral atoms or molecules.
r
Short Range:
Repulsion – Pauli Exclusion Principle
Long Range:
Attraction – Van der Waals forces – multipole contributions
Lennard-Jones Potential
Attractive Term
V ao V ( r ) = −( Bao )6 + ( Aao )12
r r
Repulsion Term
Metallic Bonding
+ + + +
-
- -
+ + + +
-
+ - + + +
- Metal atoms readily give up electrons
- These “free” electrons are treated as an electron gas
- Electrons delocalized over entire crystal
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