5 looking inside materials determining atomic and molecular dimensions

68
5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions o Explain how an STM, AFM and SEM work o Determine resolution, magnification and atomic dimensions from microscope data o Estimate molecular size from experimental data

Upload: tulia

Post on 24-Feb-2016

43 views

Category:

Documents


0 download

DESCRIPTION

5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions. Explain how an STM, AFM and SEM work Determine resolution, magnification and atomic dimensions from microscope data Estimate molecular size from experimental data. Space shuttle tile SEM 2000x. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

5 LOOKING INSIDE MATERIALSDetermining atomic and molecular dimensions

o Explain how an STM, AFM and SEM work

o Determine resolution, magnification and atomic dimensions from microscope data

o Estimate molecular size from experimental data

Page 2: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Cotton wool SEM 150x Space shuttle tile SEM 2000x

Page 3: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Looking inside glasses

cracks

human scale

fracture strength

flow

stiffnessthermal conduction

semiconductionoptical

Si Si

1 m

1 mm

1 m

1 nm

1 pm

random atomic packing

atoms

Source: MF Ashby and HR Shercliff, Cambridge University Engineering Department.

cell wall fibre composite

human scale

Looking inside woods

thermal

strengthstiffness

strengthstiffnessthermal

strengthstiffnessthermal

1 m

1 mm

1 m

1 nm

1 pm

cellular structure

cellulose fibres

Source: MF Ashby and HR Shercliff, Cambridge University Engineering Department.

cellulose molecules

Page 4: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

human scale

Looking inside metals and ceramics

stiffnesselectricalopticalthermal

yield strength(metals)

yield strength(metals)

fracturestrength(ceramics)

XXXX

crack

1 m

1 mm

1 m

1 nm

1 pm

precipitatesarrays of dislocations

alloying element

dislocation

atoms and electronsSource: MF Ashby and HR Shercliff, Cambridge University Engineering Department.

human scale

Looking inside polymers

electrical

stiffnessthermaloptical

flow

strength

XXX X

H

C

H

H

C H

C

H

H

C

H

H

C

H

H

C

C

H

H

C

H

H

C

H

H

C

H

C

C

C

1 m

1 mm

1 m

1 nm

1 pm

craze

tangled molecules

molecules

atoms

Source: MF Ashby and HR Shercliff, Cambridge University Engineering Department.

Page 5: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions
Page 6: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

World’s smallest advertisement: STM of xenon atoms

Page 7: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

STM of iron on copper

Page 8: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

STM of iron on copper: “The atomic corral”

Page 9: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Making the corral

Page 10: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

STM of metal surface showing instrumentally-induced distortion of atom shapes

Page 11: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

AFM

Page 12: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions
Page 13: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

AFM image of gold 111

Page 14: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

AFM of rhodium screw dislocations

Page 15: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Say hallo to “carbon monoxide man” (STM image)

Page 16: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

AFM of DNA strand

Page 17: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

SEM

Page 18: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

SEM of fruit fly head. Be afraid........... Be very afraid..........

Page 19: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

SEM of solar spider Will he catch the fruit fly?

Page 20: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

SEM of ant

Page 21: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

SEM of snowflake

Page 22: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Fracture behaviour

o Learn how to calculate fracture energy

o Distinguish between strength and toughness in terms of fracture behaviour of materials

o Explain why metals are tough

Page 23: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Energy stored in stretched materialEnergy stored = area under graph

= ½ x F x e

= ½ x (k x e) x e

= ½ x k x e2

Page 24: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Intensive measurement of stored energy

Energy stored per unit volume in elastic region

Evol = ½ x stress x strain

Generally:

Evol = area under stress strain graph

Page 25: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Fracture energy and tensile strength

tensileforce

tensileforce

cross-sectionalarea

energy of increasedlattice vibration

energy offlying fragments

energy to createvoids in material

energy to createnew surface area

energy of soundin material

energy to move atomsaround (e.g. slip)

Large fracture energy = tough Large tensile strength = strong

fracture energy =total energy used to fracture

specimen cross-sectional area

tensile strength =breaking force

specimen cross-sectional area

Page 26: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions
Page 27: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions
Page 28: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

strongbrittle

strongtough

weakbrittle

weaktough

glass bonenylonwood

1 10 100 1000 10000 100000

WEAK

fracture energy / J m–2

STRONG

TOUGH

10

1

100

1000

BRITTLE

brick stone

high tensilesteel

mildsteel

epoxy resinpolyester

Strong and tough

Page 29: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Cracks and stress

Material is bent,upper surfacestretchedlower surfacecompressed.

h

Crack deflectstensile stress.Stressconcentratedbelow crack.

with a crack

Contours ofequal tensilestress. Largeststress nearsurface.

no cracks

Page 30: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Under tensile stress, cracks propagate through materials.

very small areaat tip of crack:stress verylarge here

bond between atomsat tip highly stressed bond breaks

next bond is stressed

Page 31: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Fracture surfaces in metals

Which shows ductile fracture, and which shows brittle fracture?

Page 32: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Fracture of CFRP in a tennis racquet

Page 33: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

ductile metal flows, crack blunted

Stopping cracks propagating

Metals resist cracking because they are ductile. Cracks are broadened and blunted. They do not propagate.

Metals are tough because they are ductile

Metals

stress stress stress stress

high stress stress reduced

Page 34: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Bone mechanical properties

• Density 1500 kg m-3

• Young’s modulus 17 GPa

• Strength (compressive) 180 MPa(tensile) 150 MPa

Page 35: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Composite materials

• Know the meaning of the term composite material

• For a range of composite materials (ferroconcrete, bone, CFRP etc.), explain how creating a composite can improve on the properties of the individual components

Starter: Give 2 reasons why metals have a largeplastic region and undergo ductile fracture.

Now give 2 reasons why glasses undergo brittle fracture with no plastic region.

Page 36: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Starter answers

Metals undergo ductile fracture because:1. Regular structure allows

planes of atoms to slip over each other (and allow dislocations , which we shall meet later, to move)

2. Non-directional metallic bonding allows metal to change shape in the region of highest stress, without fracturing.

Glasses undergo brittle fracture because:1. The bonding is highly

directional between ions, and can only respond to stresses by bond-breaking

2. The amorphous (random) nature of the glass’s structure does not allow planes of atoms to slip over each other, as there are no definable, ordered planes of atoms as in a metal.

Page 37: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Fibre-reinforced materials use a matrix to share stress amongst many strong fibres. The matrix also protects the fibresfrom cracks forming.

Fibre-reinforcement

Fibre-reinforced materials are tough because cracks can't propagate through the soft matrix

one fibre breaks, stress takenup by other fibres

strong fibre

stress stress stress stress

soft matrixsticks to fibres

Page 38: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Composite materials• Investigate properties of composite materials based on ice

Starter: Q1. Write 2 column headings, STEEL and CONCRETE.

Q2. Assign each of the following properties to the correct material. Some may be used for both, some not at all.TOUGH STIFF STRONG IN COMPRESSION HARD BRITTLE DENSE STRONG IN TENSION SOFT HIGH FRACTURE ENERGY LOW FRACTURE ENERGY

Q3. Show, on a 2-D strength against toughness plot, where concrete and steel would lie.

Q4. Explain why concrete might be unsuitable for the beams of a road bridge.Q5. Explain why steel on its own might be unsuitable for the same application.Q6. How might you exploit the properties of both materials to solve the problem?

Page 39: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions
Page 40: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Metal microstructures• Research and illustrate the

various atomic-scale features of metals

• Explain their effect on the properties of metals

Starter: Brainstorm all of the properties of a typical metal. How does the atomic structure and bonding in a metal account for these properties?

Page 41: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Metal microstructural featuresMetals are normally polycrystalline. Research the meaning ofthis term. What affects the size of crystal grains in a polycrystalline material?

Research, illustrate and explain the effect of the following microstructural features:GRAIN BOUNDARIESDISLOCATIONSVACANCIESINTERSTITIALSSUBSTITUTIONAL IMPURITIES

Page 42: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Modifying properties of metals

Research each of the following methods of treating metals.

• Describe what is involved in the treatment process.• State how the mechanical properties of the metal are

altered.• Explain in terms of the metal microstructure why the

properties are altered.

ALLOYINGWORK HARDENINGANNEALINGTEMPERING AND QUENCHING

Page 43: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions
Page 44: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Grain boundaries

Page 45: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

A dislocation: an incomplete row of atoms

Page 46: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Vacancies, interstitials and substitutional impurities

Page 47: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Metal microstructures

• Explain the effects that micro structural features have on the properties of metals

Page 48: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Shaping and slippingAtoms in gold are in a regular array: a crystal lattice. To shape the metal, onelayer must be made to slide over another.

To slip, layer ofatoms mustmove as a whole

Layer hasmoved oneatomic spacing

Atoms canmove oneby one

All atoms move:layer moves

Dislocationreachesedge ofcrystal

atommoves

dislocationmoves

One atommoves:dislocationmoves

in both a layer has slipped by one atomic spacing

dislocation

Page 49: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

dislocation free to move: slip occurs easily

Pure crystal Alloy

alloy atom pins dislocation: slip is more difficult

dislocation pinneddislocation

Alloys are generally less ductile than pure metals

Page 50: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Questions on modifying the properties of metals

1. Draw diagrams to illustrate the following:(a) the pinning of a dislocation by a foreign atom(b) a large substitutional impurity atom in a crystal(c) an interstitial atom 2. What common effect(s) on the metal’s properties do all of the

modifications described in Q1 have? 3. How can excessive work hardening of a metal be reduced? 4. A metal contains large crystal grains. How could you change the crystal

grain size to create smaller grains? 5. Now try Questions 70X from Folio Views

Page 51: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Heat treatment of steel

• Investigate and explain how various heat treatments of steel can affect its properties

Page 52: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Stiffness and elasticity

• Explain stiffness and elasticity in metals, ceramics and polymers

Starter: The stress-strain graph for rubber is shown on the right. Rubber shows very elastic behaviour. Explain how you can tell this from the graph.

What would the stress-strain graph for a typical metal look like if you stressed it until you were in the plastic region, then took the load away?

Page 53: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Ceramics versus metals

Ceramics have rigid structures

Covalent structures

example: silica (also diamond, carborundum)

Covalent bonds share electrons between neighbouratoms. These bonds are directional: they lock atomsin place, like scaffolding.

The bonds are strong: silica is stiff

Atoms are linked in a rigid giant structure

oxygen atom

joins to others

silicon atom

The atoms cannot slip: silica is hard and brittle

Page 54: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Metals have non-directional bonds

Metallic structures

example: gold

Atoms in metals are ionised. The free electronsmove between the ions. The negative charge of theelectrons 'glues' the ions together. But the ions caneasily change places.

The bonds are strong: metals are stiff

The ions can slip: metals are ductile and tough

Ions are held together, but can move

negativeelectron 'glue'

gold ion

++ + + + + +

+ + + + + + +

+ + + + + + +

+ + + + + + +

Page 55: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Ionic structures

example: common salt

chlorine ion

sodium ion

Ionic bonds pass electrons from one atom to another.Because like charges repel and unlike charges attract,the charged ions hold each other in place.

The bonds are strong: salt crystals are stiff

The ions cannot slip: salt crystals are hard and brittle

Ions are linked in a rigid giant structure

+

+

+

+–

– –

– –

Page 56: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Summary

Ceramics covalent or ionic

Metals

strong, rigid scaffolding,stiff, hard, brittle

mobile strong electron glue,stiff, ductile, tough

Page 57: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Explaining stiffness and elasticity

Metals

++ + + + + +

+ + + + + + +

+ + + + + + +

+ + + + + + +

a metal is an array ofpositive ions bondedby negative electron'glue'

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

+

stretching has to pull bonds apart

Elastic extensibility ~ 0.1% Young modulus~1011 — 1012 Pa

Stretching a metal stretches bonds — but not much.

gaps open up a little

Page 58: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Explaining stiffness and elasticity

Polythene

polythene is along flexiblechain moleculewhich folds up

bondrotates

stretching can rotate some bonds,making the folded chain longer

Young modulus~108 — 109 Pa

chains arefolded

bondrotates

Stretching polythene rotates bonds

Elastic extensibility ~ 1%

Page 59: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Explaining stiffness and elasticity

Stiffer polymers

Young modulus~1010 Pa

Young modulus~109 — 1010 Pa

Polystyrene hasbenzene ringssticking out sideways.They make chainrotations difficult.

Bakelite hasmassively cross-linked chains. Thecross-links stopthe chains fromunfolding.

Polystyrene Bakelite – a thermoset

Page 60: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Explaining plasticity

polythene strip 10 mm 100 mm thin crystalline strip ‘pulled outof’ wider region

Polythene is semi-crystalline. Think of polytheneas like cooked spaghetti. In amorphous regionsthe chains fold randomly. In crystalline regionsthe chains line up.

When stretched plastically, the chains slip pasteach other. More of the material has lined-upchains. More of it is crystalline.

Plastic extensibility > 100%

Polythene‘neck’

crystalline amorphous new crystallineregion

Page 61: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Rubber

Rubber stretches and contracts by chains uncoiling and coiling up again. Rubber is elastic, not plastic.

In stretched rubber, the chain bonds rotate, and chainsfollow straighter paths between cross-links. When let go,the chains fold up again and the rubber contracts.

In unstretched rubber, chains meander randomlybetween sulphur cross-links.

sulphur cross-linkssulphur cross-links

Elastic extensibility > 100%

Page 62: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Comparisons of materials of different classes(metals, ceramics, polymers) See p112-114 and the summary table on p118. Q1. Give an example of a material with (a) giant covalent structure; (b) an ionic structure; (c) metallic structure Q2. Explain why ceramics, salts and metals are all stiff, butonly metals are ductile and tough Q3. Why are polymers generally much less stiff than metals? Q4. How can some polymers be made stiffer? Q5. Why does rubber get stiffer the more it is stretched?

Page 63: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Electrical conductivity

• Investigate and explain the temperature dependence of the conductivity in metals, semiconductors and insulators

Page 64: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

• copper.swf• nichrome.swf

temperature / K

200 400 600 800

logarithmicscale

silicon

108

alloy

Conduction by metals and semiconductors

104

1

10–4

10–8

pure m eta l

Page 65: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Metal and alloy

200 400 600 800temperature / K

10

5

0

linearscale

Observation Metals conduct very well.

Explanation All the atoms in the metal are ionised. The ‘spare’ electrons arefree to move.

Explanation No more electrons become free to move. Moving electrons scatterfrom the vibrating lattice – so move a little less freely as the temperature risesand lattice vibrations increase (impurities and defects also reduce the conductivity).

Observation The conductivity of a metal decreases a little as it gets warmer.

‘soup’ of freeelectrons

all atoms ionised

++ + + + + +

+ + + + + + +

+ + + + + + +

+ + + + + + +

alloy

pure m eta l

temperature / K

200 400 600 800

logarithmicscale

silicon

108

alloy

104

1

10–4

10–3

pure metal

Page 66: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

temperature / K

silicon

300 350

10

5

0

Silicon(part of temperature range only)

Observation Seminconductors conduct much less well than metals, muchmore than insulators.

Explanation O nly a few (1 in 1012) a tom s are ion ised. There are only these fewelectrons free to m ove.

Observation The conductivity of a pure semiconductor increases dramaticallyas it gets warmer.

Explanation A t h igher tem peratu res, m ore atom s becom e ion ised . Theconductiv ity increases because there are m ore charge carriers free to m ove.E ffects o f extra la ttice v ibra tions are m uch sm aller.

linearscale

rare freeelectrons

+occasionalatoms ionised

+

temperature / K

200 400 600 800

logarithmicscale

silicon

108

alloy

104

1

10–4

10–8

pure metal

Page 67: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions

Chapter 5 consolidation

Q1. Sketch stress-strain graphs for low-carbon and high-carbon steels on the same set of axes.

Q2. Describe in words the differences between low- and high-carbon steels referring to stiffness, strength, ductility etc.

Q3. Explain the differences in terms of how the added carbon atoms are incorporated into the structure and the effects this has.

Q3. Complete the glossary exercise on material properties

Page 68: 5 LOOKING INSIDE MATERIALS Determining atomic and molecular dimensions