Week 2 Flashcards

1
Q

Define crystalline

A

atoms are situated in a repeating or periodic array over large atomic distances; maintain long-range atomic order

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2
Q

Define Crystal Structure

A

properties of crystallin solids depend on crystal structure; manner in which atoms, ions or molecules are spatially arranged

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3
Q

Define Unit Cell

A

small repeat entities; basic structural unit or building block of the crystal structure and defines the crystal structure by virtue of its geometry and the atom positions within

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4
Q

Define Lattice

A

3-D array of points coinciding with atom positions (or sphere centers)

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5
Q

How many crystal systems are there and name them

A
Cubic
Tetragonal 
Orthorhombic
Rhombohedral
Hexagonal
Monoclinic
Triclinic
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6
Q

The 14 Crystal (Bravais) Lattices

A

Simple Cubic, body-centered cubic, Face-centered cubic, simple tetragonal, body-centered tetragonal, simple orthorhombic, body-centered orthorhombic, face-centered orthorhombic, rhombohedral, hexagonal, simple monoclinic, base-centered monoclinic, triclinic

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7
Q

What is the Coordination Number

A

Number of adjacent ions/atoms surrounding a reference ion/atom

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8
Q

Atomic Packing Factor

A

volume of atoms in a unit cell divided by the total unit cell volume

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9
Q

Most common crystal structure for elemental metals at room temp

A

Face centered cubic
Body centered cubic
Hexagonal Close Packed

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10
Q

How to calculate theoretical density

A

[nA] / VcNa
n = # of atoms associated with each cell (atoms)
A = atomic weight (g/mol)
Vc = volume fo unit cell (cm^3)
Na = Avogardro’s number (6.022 x 10^23 atoms/mol)

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11
Q

What is polymorphism

A

Having more than one crystal structure

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12
Q

What is Allotropy

A

When polymorphism exists in elemental solids

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13
Q

Lattice Position Coordinates

A

to specify a particular point within a unit cell
x, y, and z(right-handed)

  • axes not mutually perpendicular for hexagonal, rhombohedral, monoclinic and triclinic
  • a, b, and c (unit cell lengths)
  • p, q and r (fractional lengths)
  • point coordinate = (q,r,s)
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14
Q

Steps to get cyrstallographic directions

A
  1. construct x,y,z
  2. coordinates of two points (x1,y1,z1 and x2,y2,z2)
  3. normalize coordinate differences (x2 - x1)/a, …
  4. multiply/divide by n with common factor to reduce to smallest integer values
  5. represented as [uvw]; u = n(x2-x1)/2; v=n(y2-y1)/b; w=n(z2-z1)/c
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15
Q

What are crystallographically equivalent points

A

points where spacing of atoms along each direction is same

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16
Q

Directions in Hexagonal Crystals

A
U = n(a''1-a'1)/a
V = n(a''2-a'2)/a
W = n(z''-z')/a
[UVW] to [uvtw]
u = (1/3)(2U - V)
v = (1/3)(2V - U)
t = -(u+v)
w = W
17
Q

Crystallographic Planes

A
  1. If plane passes through origin, construct another parallel plane or establish new origin
  2. Plane either intersects or parallels each of the three axes; origin is the intersection of each of axes (A,B,C)
  3. Reciprocals are normalized and multiple by respective a, b, and c lattice parameters
  4. If required, change to smallest integers by multiplications or division by common factor
  5. Integer indices (hkl) enclosed within parentheses

h = na/A ; k = nb/B ; l = nc/C

18
Q

Linear Density (equation)

A

of atoms entered on direction vector divided by length of direction vector

19
Q

Planar Density (equation)

A

of atoms centered on plane divided by area of plane

20
Q

What are single crystals

A
  • when the repeated arrangement of atoms is perfect and extends throughout the material without interruption
  • all unit cells interlock in the same way and have same orientation (flat surfaces)
  • exist naturally and can be produced
  • applications: electronic microcircuits, semiconductors
21
Q

Polycrystalline Materials

A
  • composed of a collection of many small crystals(grains)
  • small crystals form at various positions
  • grains grow by successive addition
  • extremities of adjacent grain impinge on one another
  • atomic mismatch within region where two grains meet (grain boundary)
22
Q

Ceramics

A
  • wide variety of chemical composition is reflected in crystalline structures
  • ionic packing factor rather than atomic packing factor
23
Q

Polymers

A
  • most commercial plastics are to a large degree noncrystalline
  • chain-like structure of long polymeric molecules
  • long-chain molecules folds back and forth on itself
24
Q

Anisotropy

A

Directionality of properties due to variance of atomic/ionic spacing with crystallographic direction

25
Q

Isotropic

A

materials in which measured properties are independent of the direction of measurement

26
Q

Diffraction and when does it occur

A
  • scattering of radiation by regular array of scattering centers

Occurs when obstacles:

  1. are capable of scattering the wave
  2. have spacings that are comparable in magnitude to the wavelength
27
Q

What is Bragg’s equation

A

n(wavelength) = 2d(hkl) sin(pheta)

n = difference in path length between adjacent beams (whole number)
d = spacing between adjacent crystal planes
pheta = Bragg angle (2pheta: diffraction angle)
28
Q

Semiconductor structure

A

diamond cubic structure

29
Q

Noncrystalline solids

A
  • solids that lack a systematic and regular arrangement of atoms over relatively large atomic distances (amorphous)
  • depends on the ease with which a random atomic structure in the liquid can transform to an ordered state during solidification
  • formation favoured by rapid cooling through freezing temp