Chapter 4: Crystal Structure Flashcards

1
Q

Structure of materials

A

Arrangement of atoms in a material to minimize bond energy.

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2
Q

Short ranged order (SRO)

A

Regular and predictable arrangement of atoms over a short distance. Based on the coordination number of atoms.

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3
Q

Short ranged order (SRO) examples

A

amorphous materials (wax, glass, liquids)

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4
Q

Long ranged order (LRO)

A

Regular and predictable arrangement of atoms over infinitely great distances.

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5
Q

Long ranged order (LRO) examples

A

Crystalline solids, tempered chocolate

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6
Q

Crystalline materials

A

3D structures where the material is arranged regularly. (SRO & LRO)

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7
Q

Amorphous materials

A

Solids that are non-crystalline

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8
Q

Metallic structures

A

Crystalline

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9
Q

Ceramic structures

A

Crystalline and/or amorphous

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10
Q

Polymer structures

A

Amorphous and/or partially crystalline

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11
Q

Semiconductor structures

A

Crystalline

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12
Q

Composite structures

A

Crystalline and amorphous

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13
Q

Unit cell

A

Smallest indivisible group of atoms of a substance that has the overall symmetry of a crystal. A group of unit cells is a LRO crystal structure.

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14
Q

Mass density

A

Representation of the amount of mass (or the number of particles) of a substance.

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15
Q

Mass density formula

A

p = (nM)/(VNa)

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16
Q

Lattice parameters

A

Edge length of a unit cell

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17
Q

Lattice

A

3D network of points

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18
Q

Crystal basis

A

Repeating unit centered on lattice points

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19
Q

Bravis lattice

A

Array of discrete points with an arrangement and orientation that look exactly the same from any of the discrete points. Each point has the same surroundings

20
Q

Atomic packing factor

A

APF = (Volume of atoms in unit cell) / (Volume of unit cell)

21
Q

Simple cubic (SC) structure

A

Quarter atoms at each corner, 2 atoms in the unit cell. CN = 6, a = 2r, APF = 0.52

22
Q

Linear packing factor

A

LPF = (length of vector covered by atom) / (length of vector)

23
Q

Face centered cubic (FCC) structure

A

Quarter atoms in each corner, half atoms on each face, 4 atoms in the unit cell. CN = 12, a = 2sqrt(2)r, APF = 0.74. Close packed bravis lattice with sequence ABCABC

24
Q

Planar packing factor

A

PPF = (area covered by atoms) / (area of atom)

25
Q

Body centered cubic (BCC) structure

A

Quarter atoms in each corner, 1 atom in the center, 3 atoms in the unit cell. CN = 8, a = 4/sqrt(3)r, APF = 0.68. Bravis lattice.

26
Q

Hexagonal close packed (HCP) structure

A

7 close packed atoms on alternating layers with 3 atoms in the hollows, 6 atoms in the unit cell. CN = 12, a = 2r, APF = 0.74. Close packed with sequence ABAB

27
Q

Packing sequence and ductility

A

The closer packed atoms are, the more ductile the material. FCC is more ductile than HCP since slip is possible in every direction.

28
Q

Miller indices

A

Way to describe points, lines, planes in 3D space using h, k, l. Negative numbers are written with bars above them.

29
Q

Directions

A

Written without commas inside square brackets. Families use pointed brackets.

30
Q

Points

A

Written with commas and no brackets. Range from 0 to 1.

31
Q

Planes

A

Written without commas inside brackets. Families use curly brackets and rely on spacing

32
Q

Crystal defects

A

Control diffusion and plasticity. Eliminated to reduce total energy.

33
Q

Point defects

A

Crystal disturbances at a single point.

34
Q

Vacancies

A

Empty lattice sites that occur spontaneously.

35
Q

Vacancy ratio

A

Nv/Nt = e^(-Q/RT)

36
Q

Solute atoms

A

Atoms dissolved into the crystal lattice to remove vacancies, forms a solid solution.

37
Q

Substitutional solute atoms

A

Atoms replace the solute on the lattice site due to being a similar size/electronegativity.
EX: nickel in gold

38
Q

Interstitial solute atoms

A

Small atoms go in between lattice atoms.
EX: Carbon in steel

39
Q

Atomic vibrations

A

Atoms vibrate about their lattice positions at 10^13Hz and release the extra energy responsible for thermal activation.

40
Q

Line defects/dislocations

A

Atom planes are distorted so that half planes end inside the crystal. Motion produces slip and plastic deformation.

41
Q

Interfacial defects

A

Phase and orientation changes between grain boundaries

42
Q

Volume defects

A

Void formation at grain boundaries

43
Q

Bregg’s law

A

Describes the interaction of x-rays and crystal lattices.

44
Q

Bregg’s law formula

A

nλ = 2d(hkl)sinθ

45
Q

Interplanar spacing formula

A

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

46
Q

X-Ray diffraction

A

Used to determine crystal structure. Crystalline structures have many diffraction angles while amorphous ones have few.