Chapter 3 Flashcards

1
Q

Unit cell

A

fundamental repeating structure that is found in all crystalline structures

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2
Q

lattice parameters

A

a - define a unit cell’s size and shape

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3
Q

unit cell shapes

A
  1. cubic
  2. tetragonal
  3. orthorhombic
  4. rhombohedral
  5. hexagonal
  6. monoclinic
  7. triclinic
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4
Q

Bravais lattices

A

expands number of lattices to 14 because you have to take into account location of atoms

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5
Q

BCC Lattice definition

A

body centered cubic - atoms at corner of cell and one in the middle - a = 4R/sqrt(3)

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6
Q

bcc lattice characteristics

A

at room temp is quite open so not in lowest energy state

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7
Q

bcc lattice number of atoms

A

of interior atoms = 1
# of corner atoms = 8 * 1/8 = 1
total = 2

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8
Q

fcc lattice definition

A

face centered cubic - atoms at corners and centered on each cube face - a = 2Rsqrt(2)

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9
Q

fcc lattice number of atoms

A

of face-centered atoms = 6*1/2 = 3

of corner atoms = 8 *1/8 = 1
total = 4

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10
Q

hcp definition

A

hexagonal close packed - two hexagons with atoms at each corner and one in the faces’ centered stacked on top of each other with three interior atoms - a/c = 1.63333 (a = edge length of hexagon, c = height of prism)

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11
Q

hcp number of atoms

A

of corner atoms = 12 * 1/6 = 2
# of face atoms = 2 * 1/2 = 1
# of interior atoms = 3
total = 6

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12
Q

theoretical density of a material

A

rho = nA/V(c)N(a)
n = number of atoms in a unit cell
N(a) = Avogadro’s number
A = atomic weight
V(c) = volume of cell

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13
Q

Miller - Bravais

A

four axis system for representing hcp - a1, a2, a3, evenly spaced axis in xy plane and z is same - [uvtw] - can convert from [UVT] using formulas

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14
Q

crystal planes rules

A
  1. pick origin
  2. determine intercepts of plane with respect to the axis
  3. take inverse numbers of intercepts
  4. make these numbers integers
  5. these are your (h k l) indices
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15
Q

important notes for crystal plane indices

A

no intercept - infinity (1/infinity = 0)
-1 = 1 bar (1 with line above it)

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16
Q

crystal directions for cubic crystals

A

n is usually 1
use starting point and end point
since unit cell, a=b=c=1

17
Q

APF

A

atomic packing factor
volume of atoms - use sphere formula (4piR^3/3) and number of atoms
volume of cell - use ‘a’ parameter and formula of cube volume

18
Q

LD

A

linear density - number of atoms per unit length whose centers lie on the direction vector - must take into account proportion of atoms in that unit cell

19
Q

PD

A

planar density - number of atoms per unit length on a plane

20
Q

the higher the density, the more likely _______

A

it is for electrons and atoms to interact with each other - (111) plane is more active than (100) for fcc

21
Q

fcc pattern

22
Q

hcp pattern

23
Q

what are the most important planes

A

highest density planes or close packed planes

24
Q

x-ray diffraction principle

A

like skipping rocks, if the speed (energy) and direction (angle) are right then we diffract the incoming x-ray beam

25
Q

bragg’s law

A

nlamda = 2d*sin(theta)
n is usually 1
d is spacing between planes

26
Q

spacing between planes for cubic

A

d = a/sqrt(h^2+k^2+l^2)

27
Q

allowed reflections for BCC

A

h+k+l must be even

28
Q

allowed reflections for FCC

A

h,k,l must all be even or all be odd