Materials yapa yapa Flashcards

(70 cards)

1
Q

3 points about metals

A

(metallic bonding)
– Strong, high modulus, ductile
– High thermal and electrical conductivity
– Crystalline, opaque, reflective

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2
Q

3 points on polymers (plastics)

A

(covalent and van der Waals bonding)
– Soft, ductile, low strength, low modulus, low density
– Thermal and electrical insulators
– Optically translucent or transparent

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3
Q

Ceramics

A

(ionic and covalent bonding)
– Metallic/non-metallic element compounds (oxides, carbides, etc.)
– Brittle, crystalline or amorphous, high Temp
– Strong, high modulus
– Electrically and thermally insulating

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4
Q

elastic deformation

A

returns to original shape

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5
Q

plastic deformation

A

– structure retains some
permanent deformation
– many structures involve both
elastic and plastic responses

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6
Q

Tensile test

A

how does it work

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7
Q

Draw a stress strain curve for ceramics, metals and polymers

A
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8
Q

draw a tensile test diagram, engineering stress vs engineering strain

A
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9
Q

Name all stages of tensile test

A
  • initial elastic region
  • non linear elastic region
  • yield stress
  • plastic deformation
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10
Q

Describe Initial Elastic region

A

recoverable (O - A)
– Linear Elastic
* Stress is directly proportional to strain
* When the force is removed the specimen returns to it’s original undeformed
shape
– Hooke’s Law

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11
Q

Where does yield stress occur

A

Material Yields at B
– Yield stress σy (yield strength) - The stress at which the onset of
plastic deformation occurs

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12
Q

Where does plastic deformation occur (and describe it etc)

A

Plastic Deformation after B
– Plastic deformation is not recoverable and it is permanent
– When the load is removed the specimen does not return to its
original undeformed shape. The material becomes damaged
– Work hardening – occurs during plastic deformation

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13
Q

Define toughness

A

TOUGHNESS – the amount of
energy a material can absorb
before it undergoes fracture

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14
Q

Poisson’s Ratio

A

as ratio of lateral (contraction) strain to
axial (extension) strain
𝑃𝑜𝑖𝑠𝑠𝑜𝑛 𝑅𝑎𝑡𝑖𝑜 = 𝜈 = − 𝑙𝑎𝑡𝑒𝑟𝑎𝑙 𝑠𝑡𝑟𝑎𝑖𝑛/𝑎𝑥𝑖𝑎𝑙 𝑠𝑡𝑟𝑎𝑖𝑛 = − ∆𝑑/𝑑 // ∆𝐿/𝐿

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15
Q

Shear Stress

A

shear stress (τ) acts tangential to the surface of a material element

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16
Q

Shear Modulus

A

shear modulus (G) is described in terms of ratio of shear stress
(τ) to the corresponding shear strain (γ)

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17
Q

Elastic isotropic material properties E, υ and G are not
independent and may be related to one another by,

A

𝐸 = 2(1 + 𝜐) 𝐺

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18
Q

Torsion

A

Angle of twist

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19
Q

Stiffness

A

resistance to elastic deformation

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20
Q

Yield strength

A

ability to resist plastic deformation

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21
Q

ductile

A

large plastic strain before fracture

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22
Q

brittle

A

low plastic strain before fracture

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23
Q

hardness

A

ability to resist localized plastic deformation

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24
Q

Formula for true stress related to engineering stress

A

σ true
= σ eng (1 + ε eng)

ε true
= ln (1 + ε eng)

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25
Atomics bonding- what happens to atoms during elastic deformation?
– Atoms are stretched/separated but bonds are not broken – Atoms return to original position on removal of load
26
Name the primary vs secondary bonding types
Primary (Chemical): Strong – Ionic (Ceramics) – Covalent (Polymers) – Metallic * Secondary (Physical): Weak – van der Waals – Hydrogen
27
Ionic Bonding
Transfer of electron(s) takes place between atoms 2Na + Cl2 → 2NaCl – High melting and boiling points
28
Covalent Bonding
Covalent bonding - Outer electrons (valence) are shared between atoms weaker than Ionic Bond – Polymers are primarily bonded together through covalent bonds
29
Metallic Bonding
Metallic bonding – Outer (valence) electron not bound to any particular atom * Drift throughout entire structure – Negative electron cloud – Positive ion cores * Typically high bond strength – Plastic deformation ability (unlike brittle ionic bonds) * Free electrons – High thermal and electrical conductivity
30
Crystalline Materials
A material in which the atoms are situated in a repeating or periodic array over large atomic distances * Upon solidification, the atoms will position themselves in a repetitive three-dimensional pattern * Each atom is bonded to its nearest neighbour atoms * All metals, many ceramics and certain polymers form crystalline structures * Many material properties depend on crystal structure * Structure of crystal minimises energy
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Unit cell
Smallest repeat structure is called the
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Three types of metallic bonding for crystal structures
Three common types for metal – Body Centred Cubic – Face Centred Cubic – Hexagonal Close Packed
33
Is lattice structure seen in metals?
Lattice structure typically not seen in metallic materials due to inefficient packing sequence... Polonium is only example
34
Face Centered Cubic (FCC)
atom at each corner + single atom in each cube face Metals include aluminium, copper, gold, lead, nickel and silver * Readily undergo plastic deformation * Configuration allows atoms to slip past each other easily
35
Body Centered Cubic (BCC)
atom at each corner + single atom in each cube Materials include lithium, alpha-iron and tungsten * Tend to be harder and less malleable Atomic Packing Factor = 𝑽 𝒂𝒕𝒐𝒎𝒔 // 𝑽 𝒖𝒏𝒊𝒕 𝒄𝒆𝒍𝒍
36
Face centered Cubic - atoms and coordination number
4 atoms 12 coordination number
37
Body centered Cubic - atoms and coordination number
2 atoms 8 coordination number
38
Simple Cubic - atoms and coordination number
atoms 1 coordination 6
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Hexagonal Close Packed
Metals include Ti, Mg, Zn * Closed Packed but with much fewer slip planes * Normally brittle / low ductility
40
Anisotropy
Anisotropy — Property value depends on crystallographic direction of measurement If grains textured (e.g., deformed grains have preferential crystallographic orientation): properties anisotropic.
41
Isotropy
properties homogenous if grains randomly oriented: properties isotropic
42
Lattice Parameters
The unit cell geometry is completely defined in terms of six parameters: the three edge lengths a, b, and c, and the three interaxial angles α, β, and γ
43
Three point indices , lattice coordinate position
Coordinate specifications are possible using three point indices: q, r, and s * These indices are fractional multiples of a, b, and c unit cell lengths – q is some fractional length of a along the x axis, – r is some fractional length of b along the y axis, – s is some fractional length of c along the z axis example
44
Crystallographic Directions
A crystallographic direction is defined as a line directed between two points, or a vector – x, y, z coordinate system in unit cell corner – determine coordinates of two points on the direction vector (xi , y i , zi ) – determine length by subtracting coordinates (head – tail) – normalize by dividing by their respective lattice parameters * Convert to smallest integer * They are expressed in square brackets [u v w]
45
Slip
sliding displacement along a plane
46
Slip System
= slip plane and slip direction Slip occurs on densely or close-packed planes, in close-packed directions – Lower shear stress/energy is required for slip to occur in close-packed planes and in close-packed directions
47
Which is more packed, FCC or BCC?
No truly close packed planes like FCC so BCC less packed BCC ductile, but typically less so than FCC
48
HCP are the planes close packed and what are the slip systems like?
Closed-packed but with much fewer slip systems (typically 3 or 6) – HCP metals tend to be quite brittle, with low ductility
49
Schmid's Law
Show that the Resolved Shear Stress (RSS) (t R) on a slip plane in the slip direction is given by, t R = σ cosλ cosf (Schmid’s Law)
50
Critical RSS
Slip will occur The shear stress for initiating slip in different materials – This is a material property – Slip will happen on the plane with highest RSS ( tR ) * For a single crystal – the engineering stress ( σ) required to cause slip depends on angle of slip plane to loading * Engineering yield stress may therefore vary for a single crystal depending on the loading direction
51
Slip Stress for Polycrystalline Materials
Each crystal oriented differently to nominal loading – Slip directions/planes are therefore randomly oriented
52
Crystal Lattice
Periodic arrangement of atoms
53
defect
disrupts the order of the lattice
54
Name the 3 types of lattice imperfections
Point Line planar
55
Name the 3 types of Point defects
vacancy self interstitial substitutional
56
Point defect
* Point Defects – any defect that affects a few neighbouring atoms or lattice points
57
Interstitial atom (Point Defect)
Interstitial atom – A point defect where a smaller atom fits in between other atoms in the crystal lattice – Can be an Impurity or intentional alloying element – Induce minor stress-field on the lattice
58
Point Defect - Substitutional
Substitutional atom – A point defect where an impurity atom substitutes for a host atom – Induce stress-field on the lattice
59
Alloys
Solid solutions where one metal type is dissolved within another to enhance mechanical properties
60
Point defect- vacancy
A location in a crystal lattice where an atom is missing Induce stress-field on the lattice
61
Line Defects- name the three types of dislocation
Edge dislocation – Line defect where an extra half-plane of atoms exists in crystal lattice – Screw Dislocation – Line defect, where path spirals around a dislocation line penetrating otherwise parallel planes – Mixed Dislocations – Edge + Screw defects
62
Edge Dislocation
Edge dislocation – Line defect where an extra half-plane of atoms exists in crystal lattice
63
Screw dislocation
– Screw Dislocation – Line defect, where path spirals around a dislocation line penetrating otherwise parallel planes Screw dislocations occur when the lattice itself is sheared such that there is a misalignment of the atoms * Dislocation line is the edge, or where this misalignment begins
64
Mixed dislocation
– Mixed Dislocations – Edge + Screw defects
65
Dislocation - line defects
linear defect around which some of the atoms are misaligned dislocation density influences strength and increases with applied stress
66
Line defects - Burgers vector
Magnitude of dislocation given by the Burgers Vector, b – Draw loop around defect – Repeat the loop steps in a perfect crystal – b is the vector required to close the loop * b is always perpendicular to dislocation line for edge dislocations – Magnitude of lattice distortion
67
Dislocation Density
Dislocation Density = Total dislocation line length per unit volume – Highly deformed metal – cold worked (rolling, drawing etc.): – Means there has been significant amount of plastic deformation
68
Why are dislocations highest in metals??
The number of dislocations is highest in metals * Atoms easily move to another position with dislocation movement * Motion of dislocations is easiest because metals have non-directional bonding and close-packed directions * Covalent – directional, angular bonding – need to break bond * Ionic – charged ions don’t want to change position
69
Grain Boundaries
Grain Boundaries are planar defects  a 2D interface between adjacent grains (single crystals) in a polycrystalline material * Most common type of “planar” defect * Characteristics can strengthen or weaken a material * Grains randomly oriented * Each grain has it’s defined crystal structure, i.e. FCC, etc
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