Introduction Flashcards

1
Q

Define amorphous and crystalline solids.

A

Amorphous solids - Locally ordered but no long range order.

Crystalline solids - Periodic structure repeating over long distances.

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2
Q

Name the 9 important Bravais lattices and describe their differences.

A

Cubic (all edges the same length): Primative (P), Body (I) and Face (F)

Tetragonal (square base but different length): Primative(/simple) and Body

Orthorhombic (all different lengths): Primative, Body, Base-centered and Face

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3
Q

How do you calculate the density of a unit cell?

A

Find the side that defines the lattice parameter (where the atoms touch) and use the atomic radius to find the lattice parameter. Then find the volume.

Calculate the number of atoms in a cell and find the weight of the cell from the atomic mass. Density can then be found.

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4
Q

Draw each of the miller planes for (100) to (222) for all variations and give the distance between planes for each.

A
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5
Q

What is the difference between allotropy and polymorphism?

A

Allotropy is the ability of single atom to form more than one structure in a particular state (e.g. O2 and O3).

Polymorphism is the ability of a compound to form more than one crystal form.

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6
Q

What must be considered when using a metal/compound which has multiple allotropes?

A

How the volume of the lattice may change when changing between allotropes. The volume per atom of each form can be found to show the percentage volume change.

The properties of the structure will change as well. This is especially true for tin.

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7
Q

Describe the transition between β and α tin.

A

β tin is a BCT structure stable above 13 degrees and is a good metallic conductor, coordination 8.

α tin is stable below 13 degrees and is a non metallic insulator. The material fractures as the volume changes, coordination 4.

This is problem where tin is being used however the transition occurs over 100s of years.

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8
Q

What is the equation for Braggs law?

How is the difference between planes calculated?

What are systematic absences?

A

2d sinθ = nλ (n = 1 when using miller indices)

Cubic structures: d2 = a2/(h2 + k2 + l2) where h, k and l are the lattice parameters.

Orthorhombic structures: d-2 = h2/a2 + k2/b2 + l2/c2

If there is a layer of atoms between the planes which are being studied for diffraction then the diffaction angle expected will be absent (100 cancelled by 200).

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9
Q

What planes cause the first angles seen in the diffraction of the primitive, body and face cubic structures?

How does the angle of the diffraction change when the distance between planes increases?

A

PC: 100

BCC: 110

FCC: 111

When the distance between planes increases, the angle of diffraction angle becomes smaller.

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10
Q

Calculate the angle of diffraction for the planes of Na (BCC) from (100) to (200) and determine which are seen.

λ = 154 pm, a = 423 pm.

A

(100) θ = 10.488º not seen
(110) θ = 14.918º seen
(111) θ = 18.378º not seen (centre atom isn’t part of the plane)
(200) θ = 21.350º seen

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11
Q

Name and briefly describe the 8 types of defects and state their dimensionality.

A

Interstitial impurity (0D) - impurity between atoms in the lattice

Self interstitial (0D) - extra atom between atoms in the lattice

Vacancy (0D) - atom removed from the lattice

Substitutional impurity (0D) - atom substituted for an impurity

Group of impurities (1/2D) - multiple substitutional impurities grouped together

Edge dislocation (1D) - extra half plane of atoms added/removed

Vacancy dislocation loop (1/2D) - set of vacancies as a group

Interstitial dislocation loop (1/2D) - interstital atoms forming as a group between the lattice

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12
Q

Describe the two types of defect lines.

A

Edge - plane is correct when completing a square movement but start location is not the same as the end point.

Screw - Following the defect in a square takes you to the correct site, but in the incorrect plane.

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13
Q

Define grains and grain boundaries.

A

Grains - areas of well formed crystal

Grain boundaries - defects in a line between grains

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14
Q

Define Schottky and Frenkel defects for ionic lattices.

A

Schottky - ion and cation pair removed from lattice, the volume is the same but the density is reduced as mass is lost. 2 vacancies are formed.

Frenkel - An ion is moved to form an interstitial. Cation interstitials are much more common as anions are usually larger.

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15
Q

How do defects affect the lattice atoms surrounding it?

A

Vacancies cause the surrounding atoms to be pulled towards it. Intertitials push away surrounding atoms.

Edge dislocations stress the top and bottom in different ways:

Where an additional atom is present the atoms are compressed - they want to push outwards.

Where an atom is missing there is tension - the atoms want to pull inwards.

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16
Q

What is the equation for the number of defects?

What are the main steps towards its derivation?

A

nd = Ne-ε​d/kT

Where nd = number of defects, N = number of sites, εd = energy of defect

k = boltzmann constant, T = temperature

Using G = H - TS, some defects are preffered as entropy favours it.

H = ndεd and S = klnω where ω = the number of microstates which is found by pascals triangle and NCnd. We use the general formula for NCnd.

An approximation is used that is d(Aln(A))/dA = - 1 - lnA.

Assuming N>>nd gives the equation in the form we use.

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17
Q

What happens if 2 Burgers vectors in opposite directions meet?

A

They annihilate, leaving no defects.

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18
Q

Define an edge and a screw dislocation in terms of Burgers vectors.

A

Edge dislocation - Burgers vector perpendicular to dislocation/defect (all one plane)

Screw dislocation - Burgers vector is parallel to dislocation/defect (vectors cover one plane

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19
Q

How do dislocation lines minimse the lattice energy? Why does this occur?

A

They bring lines closer in together to try close the gaps the defects leave behind. Defects also repel each other if the compressions and tensions are on the same side. If they are on opposite sides then they will annihilate.

The elastic energy of a defect is proportional to the Burgers vector, b, squared so 2 seperate defects are better than 2 together.

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20
Q

What is the significance of defects for crystals?

A

For diamonds, defects occur naturally but when they are synthetically made there are very few. For lasers and electronics, perfect crystals are required.

21
Q

Define elastic and plastic deformation in terms of sheering a lattice.

A

Elastic - the bonds are stretched under the load but are not permanently deformed. The lattice appears to lean.

Plastic - bonds are broken and reformed as the planes slide across each other. The structure is permanently deformed.

During sheering, the vertical bonds lengthen until they are closer to the adjacent atom, at which point, the bonds will break and reform with the closer atom.

22
Q

Define the following in terms of stess and strain: ductile, brittle, toughness, stiffness and strength.

A

Ductile - the ability of a material to draw wires under strain

Brittle - materials that break under a small strain

Toughness - the ability to absorb energy before fracture, the area under a stress-strain curve

Stiffness - the ability to resist deformation

Strength - the ability to withstand a load

23
Q

Give full definitions of stress and strain, including equations.

A

Stress, σ = Force, F/Cross sectional area, A. Units are Nm-2.

Strain, ε = extension, x/original length, L. This is dimensionless.

These are also known as engineering or nominal stress and strain.

True stress uses the actual area which will change as the load is applied. True strain is defined as ln(actual length/original length).

24
Q

How does the diameter change when a material is under compression and tension?

A

Tension = reduction in diameter

Compression = increase in diameter

25
Q

Define a stress strain plot and sketch an example with each of the regions of the line described.

A

A strain is applied and the stress is measured.

O-A: Linear region, elastic/proportional, Hooke’s law obeyed

A-B: No longer linear but still elastic region, B marks the end of elasticity

C: Proof stress (aka. offset yield stress, 0.2 proof stress) is the point where if released, the material will be deformed by 0.2% strain

D: UTS - ultimate tensile strength/stress, maximum stress that can be taken

E: Fracture point/final instability point, where the material breaks

26
Q

How in the Young’s modulus defined? What are its units? What actually determines the Young’s modulus?

A

It is defined by Hooke’s law from the linear section of the stress-strain graph.

E = σε-1, units are Nm-2

The Young’s modulus is physically determined by the resistance to changing chemical bond length of adjacent atoms. This depends on the plane that material is being stretched as well as the atoms.

27
Q

Draw 3 rods that have been stretched until they break, one which is brittle, one which is ductile and one inbetween. Then draw a stress strain graph showing each material. Which material is the toughest?

A
28
Q

What is necking and when does it occur?

A

Necking is where the rod non-uniformally changes diameter, making a point where the rod breaks. This occurs at the UTS.

29
Q

How can the properties of a material be changed without altering the composition? What effects do these have?

A

Work-Hardening - heating and working with force gives a more brittle material with a higher UTS

Annealing - heating to a high temperature and letting the grains recrystalise, this makes the material more ductile and workable

30
Q

How can aluminiums compostion be changed to be significantly stronger?

A

Adding 4% by weight of copper to form Dural makes the material more brittle but means it can take a signifcantly higher stress. This is because CuAl2 precipitates forms especially at grain boundaries which adds resistance to the movements of the grains and dislocations.

31
Q

Draw a stress-strain graph for an elastic band with lines for the stretch and the release. Describe the cause and results of its shape.

A

Rubber is cross-linked so the polymers all tangle together when loose. When stretched they untangle and allign to the limit of the cross links. When you allign the elastic band you give the rubber energy as you give it a higher entropy so when it relaxes, there is an energy gain. This is represented by the area between the curves, called hysteresis, and is given out as heat during relaxation.

32
Q

Draw the stress-strain graph for a brittle polymer, a ductile polymer, a typical polymer and rubber.

A
33
Q

When drawing a polymer, explain why there is such a long drawing region.

A

The chains are extending with almost no resistance called cold-drawing, this is where the diameter will decrease linearly as more and more of the polymer chains are alligned.

34
Q

Aside from the Young’s modulus, what other elastic moduli are used? How can these be combined for measuring strain in 1 direction? What is a typical range of values for this?

A

When a material is put under tension, a transverse strain occurs in the perpendicular directions. Poisson’s ratio, ν, is the ratio of transverse strain over longitudinal strain.

ν = -εtl

If stress is applied in 3 directions, the strain in the x direction is:

εx = E-1x - νσy - νσz)

ν ≤ 0.5 and can even be negative in high tech materials used in trainers.

35
Q

Define specifc strength and give its units.

A

Specific strength is a materials strength (force per unit area) at failure, divided by the density. Units are N m kg-1 or the Yuri.

36
Q

How do we define how a material deforms?

A

A slip system needs to be defined which consists of a slip plane and a slip direction. During plastic deformation there tends to be only one slip system but at high temperatures and high stress others may occur. The slip doesn’t occur all at once, they glide through a system rather than moving all at once.

37
Q

What determines how easy a dislocation moves? Why do they only move in certain directions?

A

The ease of movement depends on the degree of distortion around the dislocation core. If the distortion is spread over a larger region, it is easier to move. Wide dislocations are common in ductile materials.

The energy of the dislocation is proportional to the burgers vector so the dislocation will only move over close packed planes.

38
Q

What are the slip planes and directions of an FCC and a BCC crystal? Why do they slip this way? How many slip systems are possible for each?

A

FCC: Slip along close packed plane {111} in the <110> direction, 12 possible systems as the dot product must be zero so there are negatives.

BCC: Slip along the nearest neighbours plane since there is no close packed plane which is {110} in the <111> direction. There is also 12 possible slip systems.

39
Q

How do you determine which slip system will slip when undergoing stress in a perticular direction? Show all the steps.

A

OILS rule: O (zero) I (intermediate) L (lowest) S (sign change)

For FCC: 1. Write tensile axis [U V W], [2 1 -4]

  1. Ignoring signs, identify the highest, intermediate and lowest number, [I L H]
  2. The slip direction is the < 1 1 0 > direction where the 0 is the intermediate position and the signs of the other 2 positions are kept the same, < 0 1 -1 >
  3. The slip plane is { 1 1 1 } with the signs of the highest and intermediate perserved but the lowest switched, { 1 -1 1 }

For BCC the same occurs but with the slip plane in steps 2 and 3 and the slip direction in step 4.

40
Q

Describe in terms of slip how carbon strengthans iron.

A

The carbon is a smaller atom which interupts the regular structure, this makes the material harder to slip. Low carbon steel (up to 0.3% carbon) is malleable and ductile but with lower tensile strength. High carbon steel (0.3 - 1.7%) carbon is much stronger and used for its higher tensile strength.

41
Q

What are the componants and units of a magnetic field?

A

A magnetic field is a vector field that points from south to north. The units are the Tesla (T) = kg s-2 A-1.

42
Q

Describe and give three examples of ferromagnetic materials.

A

Ferromagnetic materials have many domains which each have an alligned spin direction. In their equilibrium the domains point in random directions but when exposed to a magnetic field they all become alligned and become magnetic, and when the magnet is removed they stay magnetic. Soft materials lose magnetism over time but hard materials such as ferrite form permanent magnets when processed in magnetic fields.

The soft magnetic elements are iron, nickel and colbalt, hard materials include rare earth metals.

43
Q

Define ferro, antiferro and ferri.

A

Ferro: spin states alligned

Anti-Ferro: regular pattern of alternating spins

Ferri: can be weakly magnetised as alligning spin is favourable but has anti spin atoms often found where materials have different components

44
Q

Why do some magnets not retain their domain orientation?

A

Energy is stored in a magnetic field, known as magnetocrystalline energy. This makes the domains easier to align in specific directions in a crystal, but the boundaries are random.

45
Q

How does the induced magnetism in a material change when the applied field is increased? How does this depend on the axis the field is applied? Sketch a graph the situations.

A

Aligning in some directions is easier due to the domains in the material. But the boundaries are random.

46
Q

Draw a curve showing how the induced magnetisation changes in a material as a field is applied.

A
47
Q

How does applied magnetisim change when a field is turn off in soft and hard materials? Why is this important?

A
48
Q

What is the Curie temperature?

A

As temperature increases, the ablity to magnetise a material decreases. At the Curie temperature, no magnetism occurs even at high temperatures.