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FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: [email protected]
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FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: [email protected].

Dec 21, 2015

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Page 1: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

FE ReviewMaterials Science and Structure of

Matter

Jeffrey W. Fergus

Materials Engineering

Office: 281 Wilmore

Phone: 844-3405

email: [email protected]

Page 2: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Organization from 1996-7 Review Manual(same topics in 2004 review manual)

• Crystallography• Materials Testing• Metallurgy

Page 3: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Crystallography

• Crystal structure– atoms/unit cell– packing factor– coordination number

• Atomic bonding• Radioactive decay

Page 4: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Bravais Lattice

Crystal System Centering

a

b

c

P: Primitive: (x,y,z)

I: Body-centered: (x,y,z); (x+½,y+½,z+½)

C: Base-centered: (x,y,z); (x+½,y+½,z)

F: Face-centered: (x,y,z); (x+½,y+½,z) (x+½,y,z+½); (x,y+½,z+½)

(x,y,z): Fractional coordinates - proportion of axis length, not absolute distanct

Centering must apply to all atoms in unit cell.

Page 5: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Bravais Lattices (14)

Crystal System

Parameters Primitive (Simple)

Body-Centered

Face-Centered

Base-Centered

Cubic abc

X X X

Tetragonal abc

X X

Orthorhombic abc

X X X X

Rhombohedral abc

X

Hexagonal abc

X

Monoclinic abc

X X

Triclinic abc

X

Page 6: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Atoms Per Unit Cell

• Corners - shared by eight unit cells (x 1/8)– (0,0,0)=(1,0,0)=(0,1,0)=(0,0,1)=(1,1,0

)=(1,0,1)=(0,1,1)=(1,1,1)

• Edges - shared by four unit cells (x 1/4)– (0,0,½)= (1,0,½)= (0,1,½)= (1,1,½)

• Faces - shared by two unit cells (x 1/2)– (½,½,0)= (½,½,1)

Page 7: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Common Metal Structures

• Face-Centered Cubic (FCC)– 8 corners x 1/8 + 6 faces x 1/2 – 1 + 3 = 4 atoms/u.c.

• Body-Centered Cubic (BCC)– 8 corners x 1/8 + 1 center – 1 + 1 = 2 atoms/u.c.

• Hexagonal Close-Packed (HCP)– 8 corners x 1/8 + 1 middle – 1 + 1 = 2 atoms/u.c.– 12 hex. Corner x 1/6 +2 face x 1/2 + 3

middle = 6 atoms/u.c.

Page 8: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Packing Factor

• Fraction of space occupied by atoms• For FCC

• For BCC

cba

rFP i

334

..

a

ar

raraa2

44diagonalface 22

740

23

24

443

334

3

334

.r

a

r.F.P

raraaa3

44diagonalbody 322

680

83

34

223

334

3

334

.r

a

r.F.P

Page 9: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Density

volumemass

.c.uvolume

moleatom

molemass

.c.uatom

Density

338249158

1052393106020

71584

cm

g.

cmx.moleatom

x.

moleg

..c.u

atom

Density

For nickel:- Atomic weight = 58.71 g/mole- Lattice parameter = 3.5239 Å=3.5239 x 10-8 cm- Avogrado’s No. = 6.02 x 1023 = 0.602 x 1024 = atoms/mole

Page 10: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Close Packed (CN=12)

Highest packing density for same sized spheresFCC and HCP structures

Page 11: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Cube Center (CN=8)

Same atoms: BCCDifferent atoms: CsCl

Page 12: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Octahedral Site (CN=6)

In FCC:- Center (½,½,½)- Edges (0,0,½),(0,½,0),(½,0,0)- 4 per unit cell- All filled - NaCl structure

8-sided shape

Page 13: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Tetrahedral Site (CN=4)In FCC:- Divide cell into 8 boxes - center of small box- (¼,¼,¼),(¾,¼,¼),(¼,¾,¼),(¾,¾,¼)(¼,¼, ¾)(¾,¼, ¾),(¼,¾, ¾)(¾,¾, ¾)-8 per unit cell-All filled - CaF2 structure; half-filled - ZnS

4-sided shape

Page 14: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Radius Ratio Rules

Critical Radius for CN 8 = 0.732

Critical Radius for CN 6 = 0.414

Critical Radius for CN 4 = 0.225

CN 8

CN 6

CN 4

CN 3planar

Critical radius is size of atom which just fits in siteDefine minimum for bonding (i.e. atoms must touch to bond)

Page 15: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Close Packed Plane

A BA BA C

HCP: ABABABABABABABABFCC: ABCABCABCABCABCSame packing density (0.74)Same coordination (CN=12)

Page 16: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Miller Indices

Planes

Directions

(hkl)

{hkl}

[hkl]

<hkl>

specific

family

specific

family

A family of planes includes all planes which are equivalent by symmetry - depends on crystal system. - For cubic: (110),(011) and (101) are all {110} - For tetragonal: (011) and (101) are {101}

but (110) is not (ca)

- No commas- No fractions- Negative indicated by bar overnumber

Page 17: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Miller Indices - Directions

ba

c

1

1/4

1/2

-1/3

1/2-1

x1

y1/4

z1/2 (x 4)

214

x1/2

y-1

z-1/3 (x 6)

263

Page 18: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Miller Indices - Planes

41

21

ba

c

41

21

ba

c

x1/44

y0

z-1/2-2

204

interceptreciprocal

Page 19: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Miller Indices - Planes

31

21

ba

c

41

31

21

ba

c

41

x1/44

y-1/3-3

z-1/2-2

234

interceptreciprocal

Page 20: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Atomic Bonding

• Covalent– sharing electrons– strong– directional

• Ionic– trading of elecrons– electrostatic attraction or

ions– strong– non-directional

• Metallic– metal ions in sea or

electrons– moderately strong

– non-directional

• Secondary– Van der Waals– H-bonding

– electrostatic attraction of electric dipole (local charge distribution

– weak

Page 21: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Radioactive Decay

• Loss of electrons/protons/neutrons– alpha - 2 protons / two neutrons (i.e He nucleus)– beta - electrons– gamma - energy

• Exponential decay

t

expNN o

22 2

121

21

21

ln

tln

N

Nln

texpNNN

o

ooo

21

21

69302t

t.expN

tlnt

expNN oo half life

amount

original amount

time

time constant

Page 22: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Material Testing

• Stress-strain relationships– engineering stress and strain– stress-strain curve

• Testing methods– tensile test– endurance test– impact test

Page 23: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Stress

AFNormal

AFShear

Tension: >0 Compression: <0

F F FA A A

Page 24: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Strain

oo

o

ll

lll

Strain tan

ha

strain Shear

lol lo l h

a

Page 25: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Tensile Test

lengthwidth

thickness

Control length (l)

Measure force (F) with load cell

oo

o

ll

lll

Strain

twF

AF

Stress

Reduced section used to limit portion of sample undergoing deformation

Page 26: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Stress-Strain Curve

Str

ess

Strain

Ultimate Tensile Strength

Yield Point

Slope = E (Young’s Modulus)

Percent Elongation(total plastic deformation)

Elastic Limit

Proportionality Limit

Force decreases due to necking

Page 27: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

0.2% Offset Yield Strength

Str

ess

Strain0.2% strain

0.2% offsetyield strength

Page 28: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

True/Engineering Stress/Strain

iT A

F

oE A

Foo

oE l

llll

i

o

l

l o

iT l

lln

ldl

1 ET ln

EET 1ooii lAlA

Engineering(initial dimensions)

True(instantaneous

dimensions)

Usingand

Stress Strain

Page 29: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

True/Engineering Stress/StrainS

tres

s

Strain

True

Engineering

True stress does not decrease

Decrease in engineering stress due to decreased load required in the reduces cross-sectional area of the neck.

Page 30: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Strain Hardening

Str

ess

Strain

Onset of plastic deformation after

reloading

Plastic deformation require larger load after defomation.Sample dimensions are decreased, so stress is even higher

Page 31: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Bending Test

Four-point Three-point

LL/2

h

w

By summing moment in cantilever beam

22

3

wh

FLmax

FF/2F/2

Tension at bottom, compression at top

Page 32: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Hardness

• Resistance to plastic deformation• Related to yield strength• Most common indentation test

– make indentation– measure size or depth of indentation– macro- and micro- tests

• Scales: Rockwell, Brinell, Vickers, Knoop

Page 33: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Impact

hi

hf

Fracture energy = mghi -mghf

Charpy V-notch

Toughness: combination of strength and ductility - energy for fracture

Page 34: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Ductile-Brittle Failure

• Ductile– Plastic deformation– cup-cone / fibrous

fracture surface

• Brittle– little or no plastic

deformation– cleaved fracture

surface

Temperature

Fra

ctu

re E

ner

gy

Ductile-Brittle Transition Tempeature

(DBTT)

Page 35: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Creep / Stress Relaxation

• Load below yield strength - elastic deformation only• Over long time plastic deformation occurs• Requires diffusion, so usually a high-temperature

process

• Activation energy, Q (or EA)

kTE

expARTQ

expA Aratecreep

Page 36: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Creep /Stress Relaxation

Creep

FF

FF

time

fixed strain

Stress Relaxation

fixed load

time

Permanent deformation

Page 37: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Fatigue

Number of Cycles to Failure

Str

ess

Fatigue Limit(ferrous metals)

Repeated application of load - number of cycles, rather than time important.

max

min

ave

max

min

0

0

Page 38: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Metallurgy

• Corrosion• Diffusion• Phase Diagrams

– lever rule

– Fe-Fe3C diagram

– Gibb’s phase rule

• Thermal processing

Page 39: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Corrosion Resistance

• Thermodynamics vs. Kinetics– Thermodynamics - stable phases– Kinetic - rate to form stable phases

• Active vs. Passive– Active: reaction products ions or gas - non protective– Passive: reaction products - protective layer

• Corrosion resistance– Inert (noble): gold, platinum– Passivation: aluminum oxide (alumina) on aluminum,

chromia on stainless steel

Page 40: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Electrode Potential

• Tendency of metal to give up electron• Oxidation (anode)

– M = M2+ + 2e- (loss electrons)

• Reduction (cathode)– M2+ + 2e- = M (gain electrons)

• LEO (loss electrons oxidation) goes GER (gain electrons reduction)

Page 41: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Corrosion Reactions• Oxidation - metal (anode)

– M = M2+ + 2e-

• Reduction - in solution (cathode)– 2H+ + 2e- = H2

– 2H+ + ½O2 + 2e- = H2O

– H2O + ½O2 + 2e- = 2OH-

• Overall Reactions– M + 2H+ =M2+ + H2

– M + 2H+ + ½O2 = M2+ + H2O

– M + H2O + ½O2 = M2+ + 2OH- = M(OH)2

Page 42: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Galvanic Corrosion / Protection

• At joint between dissimiliar metals– reaction rate of active metal increases– reaction of less active metal decreases

• Galvanic corrosion– high corrosion rate at galvanic couple

• presence of Cu increase the local corrosion rate of Fe

• Galvanic protection– Galvanized steel

• presence of Zn decreases the local corrosion rate of Fe

– Galvanic protection• Mg or Zn connected to Fe decrease corrosion rate

Page 43: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Waterline Corrosion

• Oxygen concentration in water leads to variation in local corrosion rates

Higher corrosion rate near oxygen access

Rings of rust left from water drops

Rust just below water surface

Page 44: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Diffusion

• Atoms moving within solid state• Required defects (e.g. vacancies)• Diffusion thermally activated• Diffusion constant follows Ahrrenius relationship

kTE

expDRTQ

expDD Aoo

Gas constant

Boltzman’s constant Temperature

Activation Energy

Page 45: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Steady-State Diffusion

• Fick’s first law (1-D)• J = flux (amount/area/time)• For steady state

xC

DJ

xC

DJ

C

x

sm

massmm

mass

sm

J2

32

Page 46: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Phase Equilibria

• Gibb’s Phase Rule• P + F = C + 2 (Police Force = Cops + 2)

– P = number of phases– F = degrees of freedom– C = number of components (undivided units)– 2: Temperature and Pressure

• One-component system– F = 1 + 2 - P = 3 - P

• Two-component system– F = 2 + 2 - P = 4 - P

• Two-component system at constant pressure– F = 2 + 1 - P = 3 - P

“2” becomes “1” at constant pressure

Page 47: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Pressure-Temperature Diagram

water

ice

watervapor

Temperature

Pre

ssu

re

Single-phase area: can change T and P indepenently

(F=2)

Two-phase line: Change T (P) require specific change in P (T)

(F=1)

Three-phase point: One occurs at specific T and P (triple point)

(F=0)

One component: H2OIf formation of H2 and O2 were considered there would be two

components (H and O)

Page 48: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Phase Diagrams

L

(pure B, neglibible

solubility of A)

L

L

L

Composition (%B)

Te

mp

era

ture

Two-component @ constant pressure

Three-phase - horizontal line

EutecticL 2 solids ( + )

PeritecticL +solid () solid ()

Eutectoidsolid () 2 solids ( + )

BA

Page 49: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Lever Law• Phase diagram give compositions of phases

– two-phase boundaries in 2-phase mixture

• Mass balance generate lever law

L

S

Composition (%B)A B

Te

mp

era

ture

LiquidComp.

(XL)

SolidComp. (XS)

AlloyComp.(Xalloy)

SL

alloyL

XX

XXsolid%

SL

Salloy

XX

XXliquid%

Opposite arm over total length

Right arm for solid

Left arm for liquid

Page 50: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

70 wt% Pb -30 wt% SnA ssessed P b-Sn phase diagram.

256°C

12.8 wt% Sn

First solid

%)Pb(Sn%..)liq(Sn%.)Pb(Sn%.)alloy(Sn%

Sn%..liq% 3031886131830

861

At 183.1°C

%)Pb(Sn%..)eut(Sn%.)alloy(Sn%.)eut(Sn%.

Sn%.Pb.prim% 70318861

30861318

Page 51: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

70 wt% Pb -30 wt% SnA ssessed P b-Sn phase diagram.

256°C

12.8 wt% Sn

First solid

%)Pb(Sn%..)liq(Sn%.)Pb(Sn%.)alloy(Sn%

Sn%.% 1531889731830

897

At 182.9°C

%)Pb(Sn%..)liq(Sn%.)alloy(Sn%.)liq(Sn%.

Sn%.phasePb% 85318897

30897318

Page 52: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Microconstituents

%)Pb(Sn%..)liq(Sn%.)Pb(Sn%.)alloy(Sn%

Sn%.L% 3031886131830

861

%)Pb(Sn%..)eut(Sn%.)alloy(Sn%.)eut(Sn%.

Sn%.Pb.% 70318861

30861318Prim

%)Pb(Sn%..)liq(Sn%.)Pb(Sn%..)eut(Sn%.

Sn%.% .eutin 55318897318861

897

%)Pb(Sn%..)liq(Sn%..)eut(Sn%..)liq(Sn%.

Sn%.Pb% .eutin 45318897861897

318

Eutectic Microsconstituent ((Pb)+Sn)

Primary Pb

Phases in Eutectic Microsconstituent

Page 53: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

A ssessed F e-C phase diagram .

Fe-Fe3C Phase Diagram

Austenite

Ferrite

Cementite

Pearlite (ferrite + cementite)%C = 0.77%

HypereutectoidHypoeutectoid

Cast Irons

Steels

Page 54: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Time-Temperature-Transformation (TTT) Diagram

fs

ps

bs

ms

mf

pf

bf

727°C

800°C

200°C

100°C

KeyMain symbolf = ferritep = pearliteb = bainitec = cementite (Fe3C)Subscriptss = startf = finish

Tem

per

atu

re

Log Time

Decomposition of Austenite at fixed temperature

Martensiteathermal (diffusionless)

Pearlite: High Tempslow nucleation

Bainite: Diffusion slow

for pearlite

Coarse pearlite

Fine pearlite

Page 55: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Quench / Hardenability / Tempering

• Quench - rapidly cool– in steel: cool fast enough to Ms to prevent pearlite / bainite

formation

• Hardenability– ease of forming martensite in steels– alloying elements inhibit pearlite / bainite formation, promote

martensite formation

• Tempering of steels– reheating martensite to form transition carbides– improve toughness

Page 56: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Cold Working• Plastic deformation creates dislocations, which

increases strength / decreases ductility• Reduction in Area used to quantify degree of cold

working%

AAfA

RA%CW%i

i 100

%lw

lwlwRA%

ii

ffii 100

%lll

RA%i

fi 100

if wwfor

%d

dd%

d

dd

RA%

i

fi

i

fi

100100

4

442

22

2

22

Page 57: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Cold Worked Properties

0

100

200

300

400

500

600

0 10 20 30 40 50 60 70 80

Percent Cold Work

Str

ess

(MP

a)

0

2

4

6

8

10

12

14

16

Percen

t Elo

ng

ation

Yield StrengthTensile StrengthPercent Elongation

Page 58: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Balancing Strength / Ductility

0

100

200

300

400

500

600

0 10 20 30 40 50 60 70 80

Percent Cold Work

Str

ess

(MP

a)

0

5

10

15

20

25

30

35

Percen

t Elo

ng

ation

Yield Strength

Tensile Strength

Percent Elongation

Sy > 310 MParequires

%CW > 22%Elongation > 10%

requires%CW < 31%

Both Propertiesrequires

22% < %CW < 31%

Page 59: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Balancing Strength / Toughness

100

150

200

250

300

350

400

450

500

550

600

0 10 20 30 40 50 60 70Percent Cold Work

Str

es

s (

MP

a)

0

5

10

15

20

25

30

35

40

45

50Yield Strength

Tensile Strength

Fracture Toughness Fra

ctu

re To

ug

hn

es

s (K

Ic ) (MP

a m

0.5)

y = 250 MPa13% CW

KIc = 16 MPa m0.5

39% CW

31% CWSy = 364 MPa

KIc = 22 MPa m0.5

Sy > 250 MPaand

Kic > 16 Mpa m½

requires 13% < %CW < 39%

Examplefor 31% CW

Sy = 364 MPaKic = 22 Mpa m½

Page 60: FE Review Materials Science and Structure of Matter Jeffrey W. Fergus Materials Engineering Office: 281 Wilmore Phone: 844-3405 email: jwfergus@eng.auburn.edu.

Cold Work / Anneal / Hot Work• Annealing can eliminate effect of cold work

– recovery - stress relief, little change in properties– recrystallization - elimination of dislocations, decrease in

strength, increase in ductility– grain growth - increase in grain size, decreases both

strength and ductility

• Hot working– deforming at high enough temperature for immediate

recrystallization– list cold-working and annealing at the same time– no increase in strength– used for large deformation– poor surface finish - oxidation– After hot working, cold working used to increase strength

and improve surface finish