MODULE 2 Flashcards

1
Q

is one in which the atoms are situated in a repeating or periodic array over large atomic distances—that is, long-range order exists, such that upon solidification, the atoms
will position themselves in a repetitive three-dimensional pattern, in which each atom is bonded
to its nearest neighbor atoms.

A

Crystalline material

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

-do not crystallize and the long-range atomic order is absent.

A

Non-crystalline/Amorphous Material

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

the manner in which atoms, ions, or molecules are spatially arranged.

A

Crystal structure

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

where spheres representing nearest-neighbor atoms touch one
another.

A

Atomic hard-sphere model

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

means a three-dimensional array of points coinciding with atom positions (or
sphere centers).

A

Lattice

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

small groups of atoms form a repetitive pattern.

A

UNIT CELLS

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

are parallelepipeds or prisms having three sets of parallel faces; one is drawn within the
aggregate of spheres which in this case happens to be a cube.

A

UNIT CELLS

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

is the 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.

A

UNIT CELLS

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

What are three of the simple crystal strcutures found in metals?

A
  1. face-centered cubic,
  2. body centered cubic, and
  3. hexagonal close-packed.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

The crystal structure found for many metals has a unit cell of cubic geometry, with atoms
located at each of the corners and the centers of all the cube faces.

A

face-centered cubic,

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

the cube edge length a and the atomic radius R are related through of a fCC is

A

a = 2R√2

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

Numbers of atoms per unit cell in FCC can be calculated using

A

N = Ni +Nf/2+Nc/8

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

each atom has the same number of nearest-neighbor or touching atoms

A

coordination number

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

What is the coordination number of FCC?

A

12

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

is the sum of the sphere volumes of all atoms within a unit cell (assuming the atomic hard-sphere model) divided by the unit cell volume—that is,

A

Atomic packing factor (APF)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Equation of APF

A

volume of atoms in a unit cell/Total unit cell volume

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
17
Q

Another common metallic crystal structure also has a cubic unit cell with atoms located at
all eight corners and a single atom at the cube center.

A

body-centered cubic
(BCC) crystal structure.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
18
Q

Center and corner atoms touch one another along cube diagonals, and unit cell length a
and atomic radius R are related through

A

a =4R√3

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
19
Q

Number of atoms in FCC?

A

4

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
20
Q

NUMBER OF ATOMS IN BCC?

A

2

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
21
Q

coordination number for bcc?

A

8

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
22
Q

BCC atom packing factor

A

0.68

23
Q

FCC atom packing factor

A

0.74

24
Q

It is also possible to have a unit cell that consists of atoms situated only at the corners of a cube.

A

simple cubic (SC) crystal structure;

25
Q

The only simple-cubic element is

A

polonium,

26
Q

The top and bottom faces of the unit cell consist of six atoms that form regular hexagons and
surround a single atom in the center.

A

The Hexagonal Close-Packed Crystal Structure

27
Q

In order to compute the number of atoms per unit cell for the HCP crystal structure,

A

N = Ni +Nf/2+Nc/6

28
Q

number of atoms of hexagonal is?

A

6

29
Q

FCC Unit Cell Volume

A

16R3√2

30
Q

THEORETICAL DENSITY COMPUTATION

A

ρ =nA/(Vc xNa)

31
Q

when the periodic and repeated arrangement of atoms is perfect or extends throughout the entirety of the specimen without interruption,

A

single crystal.

32
Q

Most crystalline solids are composed of a collection of many small crystals or grains;

A

polycrystalline.

33
Q

Also, there exists some atomic mismatch within the region
where two grains meet; this area,

A

grain boundary.

34
Q

It lack a systematic and regular
arrangement of atoms over relatively large atomic distances.

A

noncrystalline solids

35
Q

meaning of amorphous?

A

“without form”

36
Q

The simplest of the point defects is

A

vacancy,

37
Q

The equilibrium number of vacancies Ny for a given quantity of material (usually per meter cubed) depends on and increases with temperature according to

A

Nv = N exp(−Qv/kt)

38
Q

The
value of k is

A

1.38 × 10−23 J/atom∙K, or 8.62 × 10−5
eV/atom∙K

39
Q

is an atom from the crystal that is crowded into an interstitial
site

A

self-interstitial

40
Q

small void space that under ordinary circumstances is not occupied.

A

interstitial site

41
Q

is the element or compound that is present in the greatest amount; on occasion,

A

Solvent

42
Q

used to denote an element or compound present in a minor concentration.

A

Solute

43
Q

is a linear or one-dimensional defect around which some of the atoms are misaligned.

A

dislocation

44
Q

it is a linear defect that centers on the line that is defined along the end of the extra
half-plane of atoms.

A

edge dislocation;

45
Q

being formed by a shear stress that is applied to produce the distortion shown in Figure, the upper front region of the crystal is shifted one atomic distance to the right relative
to the bottom portion.

A

screw dislocation,

46
Q

are boundaries that have two dimensions and normally separate
regions of the materials that have different crystal structures and/or crystallographic orientations.

A

Interfacial defects

47
Q

Within the boundary region, which is probably just several atom distances wide, there is some
atomic mismatch in a transition from the crystalline orientation of one grain to that of an adjacent
one.

A

grain boundary

48
Q

Surface atoms are not bonded to the maximum number of nearest neighbors and are
therefore in a higher energy state than the atoms at interior positions.

A

External Surfaces

49
Q

exist in multiphase materials, in which a different phase exists on each
side of the boundary; furthermore, each of the constituent phases has its own distinctive physical
and/or chemical characteristics.

A

Phase boundaries

50
Q

is a special type of grain boundary across which there is a specific mirror
lattice symmetry; that is, atoms on one side of the boundary are located in mirror image positions
to those of the atoms on the other side

A

twin boundary

51
Q

are defects in 3-dimensions. These include pores,
cracks, foreign inclusions and other phases.

A

BULK OR VOLUME DEFECTS

52
Q

Most dislocations found in crystalline materials are probably neither pure edge nor pure
screw but exhibit components of both types; these are termed

A

mixed dislocations

53
Q

The magnitude and direction of the lattice distortion associated with a dislocation are
expressed in terms

A

a Burgers vector