Exam review
Materials Moments:
Rich W.—Cooking Surfaces
Vanessa P. & Shelby R.—Flat Irons
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Viewer Mail
Dear Prof, You said that this clicker trial is not going to count against our grades in the class, but it seems like it is counting against my grade.
A: Once students have had the chance to confirm that they are using their clickers correctly, I will remove the trial scores. (By the end of this week.)
Viewer Mail
Dear Dr. Scarbrough, I wasn't able to input an answer for a question. My iclicker2 turned off after inactivity. Please give us a few seconds so that we have time to turn on our clickers again.
A: Whenever you are delayed with your clicker, during my countdown, just raise your hand or shout (nicely) “Wait!” and I will gladly wait a few moments for you.
Today clickers count toward your grade
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Family of Directions: <1 1 0>
Unit cube
1= [1 1 0]
4
3
1
2
5
5 = [1 1 0]
4 = [1 1 0]
2 = 3= [1 1 0]
y
x
z
p_pg44
- Structurally equivalent
- Atomic packing is equivalent
Family of Directions: <1 1 0>
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p_pg44.jpg
f07_03_pg54
[a1 a2 a3 z]
Vector:
[1 0 0 1]
Hexagonal
Crystallographic directions
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f07_03_pg54.jpg
Other Directions
[ 1 1 0]
[ 1 0 2]
[ 1 1 1]
[ 2 1 1]
[ 2 1 1]
[ 0 0 1]
[ 1 0 1]
Section 3.10
Crystallographic Planes:
Miller Indices
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Crystallographic Planes
Steps to finding Miller indices:
1) Translate plane away from origin or axis
2) Find length of planar intercept:
(x = a; y = b; z = c)
3) Take reciprocal of a, b, c
4) Find smallest equivalent integer set
5) Notation: (h k l)
Examples
1
2
3
z
x
y
Families of Planes:
All parallel planes are equivalent
Families of Planes
(100)
(010)
(001)
{100}
{010}
{001}
Family of Planes MI: (X Y Z)
Structurally equivalent planes: {X Y Z}
Hexagonal Crystallographic planes:
The basal plane
Other Planes:
( 1 2 3)
(0 0 1)
(0 1 1)
(1 1 2)
(2 0 1)
(1 0 1)
Notation Summary
Solved Examples posted on Canvas:
Files>Assignments, Homework, Extra Credit
Packing and Close-packed Planes
Close-packed Xl Structures
- FCC & HCP—APF = .74
- Most efficient packing
for equal-sized spheres.
- BCC—APF = .68
- Not as efficient
BCC: Which is the closest-packed plane?
z
z
A)
B)
C)
D)
z
x
y
y
x
z
y
x
y
x
Figs. 3.11, 3.12
f10_03_pg58
(110) plane packing
- FCC
- BCC
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f10_03_pg58.jpg
Different Packing…
So What?
Packing along planes:
- Strongly affects deformation
- Atoms can slip past each other on tightly packed planes (plastic deformation).
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f11_03_pg59.jpg
Figs. 3.11, 3.12
f10_03_pg58
(110) plane packing
- FCC
- BCC
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f10_03_pg58.jpg
SEM {100} planes
SEM single cadmium crystal deforming by dislocation slip on {100} planes.
Sections 3.13-3.15
Single Crystals
Polycrystalline Materials
Anisotropy
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Terms
- Crystalline
- Crystal structure
- Crystal lattice
- Single crystal
- Polycrystalline
Crystal lattice:
http://chemed.chem.wisc.edu/chempaths/GenChem-Textbook/Lattices-and-Unit-Cells-837.html
Unit Cell
Crystal Lattice
Long-range 3-D representation of a crystal
Specific location for each atom
Single Crystals
Crystal structure repeats perfectly over large atomic distance
Galena (Lead ore)
Polycrystalline materials
Many small crystals grow together
Polycrystalline materials
Extremely small crystals grow together.
Fig. 3.18
f17_03_pg65
Polycrystalline grain growth
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f17_03_pg65.jpg
Polycrystalline CaC03 (Calcite)
Thin Section
Anisotropy
Properties dependent on
crystallographic direction
Isotropy
Properties independent of crystallographic direction.
Polycrystalline copper (SEM)
SiO2 Thin section
Isotropy
Properties independent of crystallographic direction.
Thin section of schist
Anisotropy
- Properties differ according to direction.
- Atomic structure influential.
Random orientations of anisotropic material
yield isotropic behavior
Polycrystalline Calcite
Metal Thread Anisotropy
Section 3.17
Non-Crystalline Solids
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Non-Crystalline Solids
- Amorphous—without ordered form.
- Formed by rapid cooling from a melt
Non-crystalline solids
www.msm.cam.ac.uk
Hand sample of fractured glass
SEM of fractured glass
Glass: SiO2
(Glassy texture)
Fig. 3.23
f22_03_pg71
Crystalline SiO2
Non-Crystalline SiO2
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f22_03_pg71.jpg
Ancillary Materials
Notation Summary
- Crystallographic directions:
- Vectors: [x y z]
- Families: <x y z>
- Crystallographic planes:
- Planes: (h k l)
- Family of planes: {h k l}
Terms
- Crystalline—regular repeating order over a long atomic distance
- Crystal structure–shape of atomic arrangement
- Crystal lattice–more specific–specified location expected for each atom or molecule.
- Single crystal–Crystal structure repeats perfectly over large atomic distance.
- Polycrystalline–Crystalline material having more than one crystal or grain.
Crystal lattice
The organization of atoms—allows for a specific place for every molecule or atom in the solid.
- Crystal Structure–more general—how atoms
(or ions, or molecules)
are spatially arranged.
- Crystal structures are unique to each material.
Crystallographic Planes
- All parallel planes are equivalent.
- Steps to finding Miller indices:
1) Translate plane away from origin or axis
2) Find length of planar intercept:
(x = a; y = b; z = c)
3) Take reciprocal of a, b, c
4) Find smallest equivalent integer set
5) Notation: (h k l)
Metallic xl Structures
Face-Centered Cubic (FCC)
Cu, Al, Ag, Au, Pb, Ni, Pt
Body-Centered Cubic (BCC)
Na, Fe, Cr, Mo, W
Hexagonal Close-Packed (HCP)
Ti, Zn, Cd, Co, Mg