Lecture 3 and 4 Flashcards

1
Q

Density is linked to

A

atomic weight - but is not always the case

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

As increase temperature density does what and why

A

the density decreases as atoms;
amplitude of vibration increases
atoms gets further apart as it would require more energy to stay at the same distance and vibrate with greater amplitude see lennord jones
same mass for larger volume therefore lower density
thermal expansion

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

At certain temperature some materials undergo

A

a phase change ie FCC to BCC different structure

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

what can happen in a phase change

A

change in density
magnetic properties alter
a lot of mechanical properties
at certain temperature property you are relying on may disappear due to phase change

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

BCC

A

body centered cubic atoms touch across internal diagonal not a close packed system atoms all corners one in the middle not a stable structure

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

FCC

A

face centered cubic close packed structure based on layers of atoms, atoms touch across diagonal of face packing sequence ACB ACB ACB

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

Most materials are

A

crystalline structure (not are but focus on crystalline atm)

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

crystalline structures can be descirbed as

A

regular array of atoms can be described as unit cells which is a basic building block to make the whole structure

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

lattice spacing

A

a - length width and depth of unit cell (volume of unit cell = a^3)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

sharing of atoms between unit cells meaning

A

if you had a unit cell of simple cubic structure at each corner was an atom then each atom would be shared with 8 other unit cells therefore an eighth of that atom would be inside the unit cell
total atoms in unit cell = 1/8 * 8 = 1

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

What can we tell from unit cell of an atom

A

everything dont care about the number of unit cells as it just makes the crystal larger repeat of the same unit cell can characterize the crystal by characterizing the unit cell

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

atomic packing fraction

A

number of particles x volume of particle (4/3pi r^3) / volume of unit cell

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

method for finding APF

A

find lattice structure in terms of radius of atoms (see what plane atoms touching on)
find volume of unit cell in terms of radius of atom
find number of atoms in unit cell (remember some shared)
insert into APF equation, radius cancels giving %

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

simple cubic structure

A

one atom at each corner of cube

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

What does the APF tell you

A

% of unit cell filled with atomic volume

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

HCP

A

hexagonal close packed close packed structure based on layers of atoms packing structure AB AB AB

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

number of atoms in FCC unit cell

A

1/2 * 6 + 1/8 * 8 = 4

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

types of materials FCC

A

aluminium copper

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

FCC close packed plane

A

(1 1 1)

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

FCC a in terms of r equation

A

a^2 + a^2 = (4R)^2
a^2 = 8R^2
a= 2root2 * R

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

perfect dislocation is where

A

atom crystal moved but maintained the structure of the crystal - hoped from one to the other

22
Q

HCP materials

A

cobalt alpha titanium

23
Q

HCP structure unit cell

A

hexagonal prism each face is a place A and A with the B layer in the middle unit cell is a third of this structure

24
Q

HCP unit cell

A

2 atoms per unit cell V = (root3 * a^2 *c)/2

where c is the distance between two layers of the same structure ie A and A

25
BCC
not a close packed system atoms all corners one in the middle not a stable structure
26
BCC materials
alpha iron
27
Some materials will have different properties in
different directions - easy to split in one direction hard in another direction
28
miller indices are
a way of describing a crystals orientation
29
miller indices used to describe
planes
30
brackets for planes groups of planes | directions and groups of directions
(planes) {collection of planes} [directions] | goes x y z
31
what is a plance
a surface of a cube, due to symmetry will be the same as another surface this is how we group together (1 0 0) same as (0 1 0) (0 0 1) therefore group {1 0 0} or {0 1 0} where it cuts the axis that we put the point same crystal structure no difference in information from plane mechanically respond the same
32
diagram if (1 1 1) plane and (2 1 0)
see powerpoint
33
miller indices equation
``` lattice constant (a) / distance at which it cuts as fraction of a ie a/a = 1 a/infinity = 0 ie parallel to this axis a/ 0.5 a = 2 ```
34
how to do negative in miller indices
put bar over top of number
35
miller indices directions vs planes
the plane and direction with same miller indices will perpendicular to each other take start point of direction as origin and indices with respect to that
36
direction in miller indices is
how far it travels in a certain direction
37
(1 1 1) plane for FCC
is close packed plane as its plane in which atoms are in contact with each other slip plane
38
orientation of stresses defined in
similar way to miller indicies x axis is 1 y axis is 2 z axis is 3
39
normal stress
acting out of surface
40
shear stress
acting parallel to surface
41
stress notation
sigma ij where i is the plane and j is the direction the force acts
42
how many components of stress on a cube
9 but gets cut down to 6 unique ones as you cannot generate stress on one surface of cube without having equal and opposite on other side
43
each surface has what kind of stresses on it
2 shear and one normal (first number will all be the same if on the same plane, the normal the number will be the same, the shear stresses will be the other two directions)
44
1 0 0 plane also known as
x plane or yz plane
45
how are shear stresses written
with a tau instead of a sigma
46
what the three normal stresses and 3 shearing stresses
sigma 11 sigma 22 sigma 33 | tau 12 tau 13 and tau 23 these cover all forces due to equal and opposite reactions
47
show that there are only 3 unique shear stresses and state why
see powerpoint due to equal and opposite and static equilibrium - material will push back in opposite direction therefore tau 13 = tau 31 tau 23 = tau 32 tau 12 = tau 21
48
why can we cancel the z stresses
as we often work in 2 dimensions as forces in third are negligible (walls and thin plates) interested in stresses in surface not thickness
49
shear is rotating clockwise this is
positive if anticlockwise motion it is negative
50
normal is tension this is
positive if compression it is negative
51
in static equilibrium stresses are balanced shear stresses are
complimentary (see powerpoint)