mle1101 ay1213 sem2 detailed tutorial solutions
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MLE1101AY12/13 Semester 2
Tutorial 1-6 Detailed Tutorial Solutions
Written by: Ms Kong Hui Zi :3
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Determinetheelectronconfigurationsforasiliconatom(Z=14)
andagermaniumatom(Z=32).
Explainwhythesetwoelementsdisplaysimilar characteristics.
Tutorial1Question2(ElectronicConfig.):
e configurationofSi(Z =14): 1s22s22p63s23p2
e configurationofGe (Z=32): 1s22s22p63s23p64s23d104p2
or 1s22s22p63s23p63d104s24p2
Bothelementshaveavalenceelectronstructureoftheformxs2xp2
wherex is3 forSiand4 forGe,
(bothbelongtoGp.4inPeriodictable)
soverysimilarcharacteristics.
5
1s
2s 2p
3s 3p 3d
4s 4p 4d 4f
5s 5p 5d 5f
6s 6p 6d
7s 7p
1s22s22p63s23p64s23d104p6
36electrons
In a commercial xray generato
(Cu) or tungsten (W) is expose
energy electrons. These electron
metal atoms. When the metal athey emit xrays of characteris
example, a tungsten atom st
may lose one of its K shell
another electron, probably from
into the vacant site in the K s
occurs in tungsten, a tungsten K
Tutorial1Question4(E
34 8
15
9
6.63 10 J s 3 10 m/s9.30 10 J
1m0.02138nm
10 nm
hcE
AtungstenK
xrayhasawavelength of0.02138nm.
Whatisitsenergy?Whatisitsfrequency?
Tutorial1Question4(Contd):
8
19
9
3.00 10 m/ s1.40 10 Hz
1m0.02138nm10 nm
c
7
[LNChap2p.6]
Tutorial1Question5(EDescribetheelectrontransferp
formationoftheioniccompoun
Electropositive : Li:1s22s1
Electronegative: O:1s22s22p4
Li++Li++O2 Li2O
Li LiO
++ + ++
[LN: Noble gas:s2p6 ,Metals:1 #of
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Tutorial1Question6(IonicBonding):IftheattractiveforcebetweenapairofSr2+ andO2 ionsis1.29x
108NandtheionicradiusoftheO2 ionis0.132nm,calculatethe
ionicradiusoftheSr2+ ion innanometers.
21 2
net a tt ract ive repulsive 2 1
04n
Z Z e nbF F F
a a
2192
1 20
12 2 2 80 attractive
10
2 2 1.6 10 C
4 4 8.85 10 C / N m 1.29 10 N
2.672 10 m 0.2672nm
Z Z ea
F
0 0 0.2672nm 0.132nm 0.135nma r R r a R9
o = Permeabilityoffreespace,b&nareconstants
[LNChap2p.2223]
Tutorial1Question7(CUseschematicdiagramstodepictt
ineachofthefollowingmaterials:
(b)C2H6 (ethane)
(c)C2H3Cl (VinylChloride)
#ofcovalentbonds # ofvalenceelectNo.ofvalenceelectrons: H:1 O:6
c.f. C2HCl3 (Chloroform
8O:1s22s22p4
Usetheconceptofsecondarybondstrengthtopredictwhichmemberofeachpairof
materialsbelowhasahigher meltingtemp.
Matls Typeof 2o bond Size Ans: m.p. (oC)
(a) C2H4 WeakVan der Waals Similar Lower 169C
C2H2F2 Permanent dipolefromhighly electrove F(EN=4.1)
Similar Higher 144or
165C
(b) H2O Permanentdipolew moreelectrove O(EN=3.5)
+HBonding
Similar Higher 0C
H2S Permanentdipolewithelectrove S(EN=2.4)
Similar Lower 85.5C
(c) C3H8 organicmoleculescomposedofcarbonand
hydrogen V.d.W. only
Smaller (orshorter)
moleculeLower 189.7C
C12H26 organicmoleculescomposedofcarbonand
hydrogen V.d.W. only
Largermolecule
canformalarger
numberofdipoles
Higher 9.6C
11
Tutorial1Question9(SecondaryBonds): SecondaryBondin
Aspecialcase:hydrogenbonding
(a) It occurs between molecules in which h
(F), oxygen (O) and nitrogen (N).
(b) For each HF, HO and HN bond, the si
other atom. Thus, the hydrogen end of th
bare proton, which is capable of a strong at
adjacent molecule.
H Cl H Clsecondarybonding
Fluctuating
dipole
Permanent
dipole+ +
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Chap.3Cyrstal Structure1. CrystalStructure,SpaceLattice,UnitCell,Amorphous
2. 14Bravais Lattices:Cubic,Tetragonal,Orthorhombic,Rhombohedral,Hexagonal,Monoclin
3.
4. AtomicPackingFactor Interplanar spacing
5. AtomsPositions
6. CrystallographicDirtn:Start&End,End start(orwalk),I
7. MillerIndices:Origin,Intercept,Inverse,Integer,Bracket,
8. VolumeDensity(g/cm3 ), PlanarDensity(Ctr),LinearAto
9. Polymorphismor
Allotropy
10. XRayDiffraction:
hkla d
2
2 2 2 2
2sin
4h k l
a
2 sinhkl
d
2
2
sin
sin
A
B
3
3
4
3n r
a A A
A
A
A
A
AB
B BC
CC
Stacking:ABAB
vs ABCABC
BCC 2atoms
CN=8
0.68
FCC 4atoms
CN=12
0.74
HCP 6atoms
CN=12
0.74
4 3R a 4 2R a 2 c
R aa
Massu.c./Volumeu.c. Equiv.#ofatomctr intersected
SelectedArea
Equiv.#ofat
S
Integer#ofwavelength BCC:h+k+l =even,FCC:(h,k,l)allevenorallodd
HCP(0001) FCC(111)
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Thed130 interplanar spacinginaBCCelementis0.1587nm.
(a) Whatisitslatticeconstanta?
(b) Whatistheatomicradiusoftheelement?
(c) Whatcouldthiselement be?
Tutorial2Question5:
2 2 2 2 2 2
0.1587 1 3 0 0.502hkla d h k l nm (a)
3 0.50234 3 0.2174
4 4
nmaR a R nm (b)
(c) Lattice
Constant
Crystalstructure
Atomicradius
Qn 5 Ans: 0.502 BCC 0.2174
Barium,Ba 0.5019 BCC 0.217
Lead,Pb 0.49502 FCC 0.175
Potassium, K 0.5344 BCC 0.238
Silicon,Si 0.54282 Diamond 0.1171
Question8:ThelatticeconstantforBCCtantalumat20
16.6g/cm3.Calculateavalueforitsatomic
3
Atominumber of atoms
mV a
3
7
216.6
0.33026 10 6.023 10
Atomic mass
180.08 /Atomic mass g mol
18 1 2
8 Number of atoms
Calculatetheplanaratomicdensityinatomspersquaremillimetreforthe
(111)crystalplaneinFCCgold,whichhasalatticeconstantof0.40788nm.
1 1sin
2 2Area of Triangle bh ab
21 3
2 2 sin 602 2
oArea of a a a
1 1
3 3 22 6Number of atoms
2
6
13 2
2 2
3 0.40788 10
1.39 10 /
Number of AtomsPlanar Density
Area mm
atoms mm
3
a a
(111)
Question9:
1
6
1
2
1
4
12 12
Number of atoms
62.33 10
Number of Linear Density
Length
ato
2 2
6
7
2
2 0.3039 10
4.3 10
Face diagonal a a a
mm
Calculate the linear atomic density in at
direction in BCC vanadium, which has a lat
Draw[110]inBCCunitcell
Question10:
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5
Cubic structure
XRD
2A
2BXRDpattern
0.75
0.5
3
4
2
4
2
2 2 2 2
2sin
4h k l
a 2 2 2
hkla d h k l
2 sinhkld
No. 2 sin sin21 38.60o 19.30o 0.3305 0.109
2 55.71o 27.86o 0.4672 0.218
Anxraydiffractometer (Wavelength ofth
recorderchartforanelementthathaseithe
showeddiffractionpeaksatthefollowing2
38.60,55.71,69.70,82.55,95.00and10
(a) Determinethecrystalstructureofthe
(b) Determinethelatticeconstantofthee
(c) Identifytheelement.
Question11(Contd):
(a)
2 2 2
0.15405
2sin 2sin 19.3
na h k l
(b)
2
2 2 2 2
2sin
4h k l
a
7
Anxraydiffractometer (Wavelength oftheincomingradiation=0.15405nm)
recorderchartforanelementthathaseithertheBCCortheFCCcrystalstructure
showeddiffractionpeaksatthefollowing2 angles:
38.60,55.71,69.70,82.55,95.00and107.67.
(a) Determinethecrystalstructureoftheelement.
(b) Determinethelatticeconstantoftheelement.
(c) Identifytheelement.
Question11(Contd):
Lattice Constant(nm) CrystalstructureQn 11Ans: 0.3296 BCC
Magnesium, Mg 0.32094 HCP
Niobium,Nb 0.33007 BCC
Tantalum,Ta 0.33026 BCC
Zirconium,Zr 0.32312 HCP
(0.30to0.34)(c)
Coordinates
x, y, z
(0, 1,0)
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Drawdirectionvectorsinunitcubesforthefollowingcubicdirections:
9
Question1:
111
113
121
110(a) (b) (c) (d)
y
x
z
(0,0,1)
(0,1,0)(0,0,0)x
(b)1. Start&Endpositions:
2. End start(orwalk):
3. Integer:
4. Sqr Bracket:
1, 1, 0 0, 0, 0 1, 1, 0
1 1 0
1 1 0
1 1 0
1 1 0
x
x
1, 0, 0 0,1, 0 1, 1, 0
x
Drawdirectionvectorsinunitcubesforth
Question1(Contd):
111
(a) (b
(d 121
(c)
y
x
z
1
3
11
Question2:
Whataretheindicesofthedirectionsshownintheunitcube:
(e)1. Start&Endpositions:
2. End start(orwalk):
3. Integer:
4. Sqr Bracket:
(1,1,0)
1,0,1
4
1,0,1
4
1 3
, 0,1 1,1, 0 , 1, 14 4
3
4, 1 4, 1 4 3, 4, 44
(1,1,0)
3 4 4
Question2(Contd):
Whataretheindicesofthedirectionsshow
(g)
11,0,
4
10,1,
2
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13
Question2(Contd):
Whataretheindicesofthedirectionsshownintheunitcubebelow:
Subtractingorigincoordinates
fromemergencecoordinates
(e)
(f)
(g)
(h)
x y z
Origin: 1 1 1
Intercept: 1 1
Inverse: 1 1 0
Integer: 1 1 0
Bracket:
x
Origin: 0
I nt ercept : 1
Inverse: 1
Integer: 1
Bracket: 1
1 1 0 h k Family
15
Question3:
(a)1. Origin
2. Intercept
3. Inverse
4. Integer
5. Bracket
x y z
Origin: 1 0 1
Intercept: 1
Inverse: 1 0 3
Integer: 1 0 3
Bracket: 1 0 3
y
x
z
x
13
(1,0,1)
WhataretheMillerindicesofthecubiccrystallographicplanesshownbelow:
Question3(Contd):
W
c
(0,0,0) x y
x
z
1 10
4 4
2 1 8 3 51
3 4 12 12
5 1 1 12 30
12 4 4 5 5
y ax b
a b b
a a
y x x
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17
Question3(Contd):
x
x
(0,0,0)
Top
view
xx y
x
z
3 30
4 4
1 3 4 9 51
3 4 12 12
5 3 3 12 90
12 4 4 5 5
y ax b
a b b
a a
y x x
(c) x y z
Origin: 0 1 0
Intercept:
Inverse: X 9 X 9 0 X 9
Integer: 5 12 0
Bracket: 5 12 0
3
4
4
3
9
55
9
(0,1,0)
Question3(Contd):
(b) x y z
Origin: 0 1 1
Intercept: 1 1
Invers e: 1 X2 1 X2 X2
Integer: 2 2 3
Bracket: 2 2 3
2
3
WhataretheMillerindicesofthecubic
crystallographicplanesshownbelow:
3
2
(d)
Orig
Inte
Inve
Inte
Brac
19
(a)
Question4:
y
x
z
DrawinunitcubesthecrystalplanesthathavethefollowingMillerindices:
111 213 121 102(a) (b) (c) (d)
(a) x y z
Origin: 0 1 1
Intercept:
Inverse: 1 1 1
Integer:
Bracket: 1 1 1
x(0,1,1)
y
x
z
x
x
x
x
Originat
(b)
Question4(Contd):
y
x
z
Drawinunitcubesthecrystalplanesthat
111 102(a) (b) (c)
(0,0,1)
y
x
z
x
x
x x
x
x
1
2
Originat
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21
(c)
Question4: DrawinunitcubesthecrystalplanesthathavethefollowingMillerindices:
111 213 121 102(a) (b) (c) (d)
(c) x y z
Origin: 0 1 1
Inverse: 1 1
Bracket: 1 2 1
1
2
y
x
z
(0,1,1)
y
x
z
x
x
1
2
x
x
x
(d)
y
x
z
(0,0,1)
y
x
z
x
x12 x
x
x
1
3
(d) x y z
Origin: 0 0 1
Inverse: 1
Bracket:
1
2
1
3
2 1 3
OriginatOriginat
1
1
x
y
Intercept:
x=1
y=1
Intercep
a1 a2 a31 1 1 1
23
x
xx
DrawthehexagonalcrystalplaneswhoseMillerBravais indicesare:
Question6:
1 0 1 1(a) (b) (c) 0 1 1 1 1 2 1 0
(a) a1 a2 a3 c
Origin: 0 0 0 0
Intercept:
Inverse: 1 1 1
Integer:
Bracket:
c
a1
a2
a3
a3
1 0 1 1
(b)
(c)
c
c
(b)
Orig
Inte
Inve
Inte
Brac
(c)
Orig
Inte
Inve
Inte
Brac
Question6(Contd): DrawthehMillerBrav
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DetermineMillerBravais indicesofthehexagonalcrystalplanesinthefigues below:
25
Question7(Contd):
(b) a1 a2 a3 c
Origin: 0 0 0 1
Intercept: 1 1 1
Inverse: 1 1 0 1
Integer: 1 1 0 1
Bracket: 1 1 0 1
(b) a1 a2 a3 c
Origin: 0 0 0 0
Intercept: 1 1 1
Inverse: 1 1 0 1
Integer: 1 1 0 1
Bracket: 1 1 0 1
c
a1
a1
a2
DetermineMillerBravais indicesofthehexag
c
Question7:
(c)
Origin
Interc
Invers
Intege
Bracke
27
AreaofCD=a 0cos 30
cV HC
a
a
60o
A
B
CArea of
cV HCP
Equilateral
Triangle
VolumeofHCPunitcell:
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Chap.4Solidification&Imperfections
12nN d
VG
r
2
*1. HomogeneousNucleation:
2. HeterogeneousNucleation:
3. Growth,GrainRefiner,GrainBoundaries(polycrystalline),
SingleCrystal Creepresistance
4. Substitutional solidsolution:Substi.Solvent,distort,Solubility ifdia.
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vacancy
1. 2.
3.
4. Diffusionrate:solid
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Calculate the number of atoms in a critically sized nucleus for the
homogeneous nucleation of pure iron. Assume T (undercooling) = 0.2 Tm.
Tutorial3Question1(Nucleation):
*
7 2
10
3
2 2
0.2
2 204 10 J/cm 1808K9.72 10 m
2098J/ cm 0.2 1808K
m m
f f m
T Tr
H T H T
3
3 10 27 34 4vol.ofcriticalsizednucleus * 9.72 10 m 3.85 10 m
3 3r x
For 1criticallysizednucleus,
LatentheatoffusionHf =2098J/cm3, Surfaceenergy=204107J/cm2,
MeltingtemperatureTm =1808K,latticeconstantBCCa=0.28664nm.
r*
3
Tutorial3Question1(Con
3 vol.of1unitcellofFe 0.28664 1a
29 329 3
Averagevolume/atom (includesspace
2.355 1 0 m1.178 1 0 m
2
vol.ofnucleus 3.85
Volume/atom 1.17
For1BCCFeunitcell,
NumberofAtoms
in1nucleus =
Calculate the number of atoms in a c
homogeneous nucleation of pure iron. AssumLatentheatoffusionHf =2098J/cm
3, Surfaceenergy
MeltingtemperatureTm =1808K,latticeconstantBCCa
h
x
y
Calculate the radius of the largest interstitial void in the BCC iron lattice. Theatomic radius of the iron atoms in this lattice is 0.124nm, and the largest
interstitial voids occur at etc., type positions.
Tutorial3Question2(Interstitial):
1 14 2, ,0
2 2
2 25
4 2 16
a ah a
h =RFe +Rvoid
ForBCCstructure,
void Fe 0.160nm 0.124nm 0.036nmR h R
RFe
Rvoid
5
4 0.124nm43 4 0.286nm
3 3
Ra R a
225 5
0.286nm 0.160nm16 16
h a
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[AdaptedfromMST5001LecturenotesChap2]
Interstitialsite inFCCunitcell(Extra)
7
Describe and illustrate the edge and screwt
What types ofstrain fields surround both typ
Tutorial3Question3(Disl
Line imperfection caused by an extra
half plane of atoms between two
normal planes of atoms.
Lin
up
to
sep
EdgeDislocation
Tension
Compression
Shea
Dislocationline
[AdaptedfromMST5001LecturenotesChap4]9
Dislocations:BurgersCircui
Edgedislocation
definesense
of
Dislocation
line
closedcircuitbyRHrule
vectorfromStarttoFinish Burgersvector
T
[AdaptedfromMST5001LecturenotesChap4]
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If there are 400 grains per square inch on a photomicrograph of a ceramic
material at 200x, what is the ASTM grainsize number of the material?
Tutorial3Question4(Grainsize):
[LNChap4p36]
2
2 2100
200400grains/inch 1600grains/inch
100x
xN
x
1 12 1600 2 ln1600 1 ln2 10.64 1 11.64n nN n n
[TBCD:Tutorials Grainsize.htmlorTBExample4.5]
11
a) Calculatetheequilibriumconcentration
purecopperat850oC.Assumethatthee
inpurecopperis1.00eV,constant C=1.
b) Whatisthevacancyfractionat800oC?
Tutorial3Question5(Vac
5
VacancyFraction= 1 exp8.6
2.02 10
vn
N(b)
a) Calculatetheequilibriumconcentrationofvacanciespercubicmeterin
purecopperat850oC.Assumethattheenergyofformationofavacancy
inpurecopperis1.00eV,constantC=1.
b) Whatisthevacancyfractionat800oC?
Tutorial3Question5(Contd):
(AtomicmassofCu=63.54g/mol;DensityofCu=8.96g/cm3;
Avogadrosconstant=6.02x1023 atoms/mol;Boltzmannsconstant=8.62x105 eV/K)
2328 3
3
3
3
8.96 6.023 10 atoms / mol8.49 10 /
. . 63.54g /mol1001
1
AN g xN x atoms mA M cm
cmm
28 3
5
24 3
1eV8.49 10 atoms/ m exp
8.62 10 e V / K 850 273
2.77 10 vacancies/ m
vnK
exp expv v v
v
n E EC n NC
N kT kT
13
WriteequationforFicks firstlawofdiffusion,
Tutorial3Question6(Fick
2
atomsInSIunitform,
m s
dCJ D
dx
where
J = Flux,netflowofatoms
D
=
Diffusitivity, Diffusion
Coefficien
= ConcentrationgradientdC
dx
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Consider the gas carburizing of a gear of 1018 steel (0.18 wt%) at 927oC.
Calculate the time necessary to increase the carbon content to 0.35 wt% at
0.40 mm below the surface of the gear. Assume the carbon content at the
surface to be 1.15 wt%. D (C in iron) at 927oC = 1.28x1011m2/s.
0 2
S X
S
C C xerf
C C Dt
55.90170.8247 erf
t
Co=0.18wt%
T=927oC
t=?Cx =0.35wt%
x=0.4x103 m
Cs=1.15wt%
D=1.28x1011 m2/s
3
11 2
1.15 0.35 0.4 10 m
1.15 0.18 2 1.28 10 m / s
xerf
x t
Tutorial3Question7(Diffusion):
3400
3400sec 56.67mins60
st
s
55.9017
0.9587t
15
z erf (z)
0.95 0.8209
z 0.8247
1 0.8427
1 0.8427 0.8247
1 0.95 0.8427 0.8209
0.9587
z
z
z erf (z)
0.95 0.8209z 0.8247
1 0.8427
17
The diffusivity of copper atoms in the alumi
600oC and 2.50x1015 m2/s at 400oC. Calcula
case in this temperature range. Given R = 8.3
0 exp
QD D
RT
13 2
15 2
7.5 10 /exp
8.314 / 2.5 10 /
m s Q
J mol K m s
3139.3 10 J/Q x
0
1
2
0
exp
exp
DD
D D
Tutorial3Question8(Diff
Thankyou!
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Chap.6Mechanical
cos cosr
0
F
A
i 0
0
l l
l
Ti
F
A 0i
0
ln lnTi
Al
l A
E
(12): 1
(3): 00
FCC
HCP
y ok
d
(Coldwork(loadr.t.)createmoredefects(dislocations,atomsmove
dislocationmovementhinderedby GB&otherdislocations,Anneal
(deform2000%,>0.5Tm+slowstrain+5m+strainsensitive(resistivity),GBsoften,grainsslideandelongated)
(
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ExplanatoryNotesforQn
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Engineering stressstraindatawereobtainedatthe
beginningofatensiletest0.2%Cplaincarbonsteel.
(a) Plottheengineeringstressstraincurve
(b) Determinethe0.2percentoffsetyieldstress
(c) Determinethetensileelasticmodulus
Tutorial4Question1( ): (k psi) (in./in.)0 0
15 0.0005
30 0.001
40 0.0015
50 0.0020
60 0.0035
66 0.004
70 0.006
72 0.008
0
10
20
30
40
50
60
70
80
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009
Engineering
Stress
(1000
psi)
EngineeringStrain(in./in.)
(a)
0.2%( =0.002)yieldstress
=66x103 psi
3
7
30 10 psi
0.001
3.0 10 psi
xE
(b)
(c) [LNChap6p89]
2
A 0.505in.diameter aluminum alloy test
diameter of the bar is 0.490 in. at this load,
(a) the engineering stress and strain and (b)
22
2
0
2
2
0.505
0.200
i2 4
0.4900.189in
4i
d
A r
A
Assumenovolumechange, 0 0 i iA l A l
32
0
25000lb125 10 psi
0.200in
fFx
A
32
25000lb133 10 psi
0.189in
f
T
i
Fx
A
(a)
(b)
Question2(Tensile):
Units: psi:poundforcepersquareinch
a) Why do pure FCC metals like Ag and Cu have low values of critical resolved
shear stress c?
b) What is believed to be responsible for the high values ofc for HCP titanium?
For FCC metals like Ag and Cu, slip takes place on the closepacked {111}
o ctahedral pla nes an d i n the close p ac ked dire ctions .
Lower shear stress is required for slip to occur in densely packed planes.
The high c values associated with HCP titanium is attributed to the mixedcovalent and metallic bonding with the atomic lattice structure.
[TB Chap6 p237]
Question3(CriticalResolvedShearStress):
4
110
[TBChap6p236]
Slipsystem:Thesystem(plane+direction)i
HighestPlanardensity,HighestLineardensi
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111
111
111
111
110
101
011
1 1 2 2 3 3cos
, cos90 0o
u v u v u v u v u v
If perpendi cul ar u v u v
110
101
011
110
101
011
1 2 3u u u u
1 2 3v v v v
110
101
011
7
2 2 21 2 3u u u u
A stress of 75 MPa is applied in the [001] d
(a) the resolved shear stress acting on the
shear stress acting on the sli p s(111)[110]
Question4(Schmids Law
(a)
isbtw &SlipDirtF
isbtw &NormalofSlipPlaneF
cos 54.73
a
a
45Facediagonal
cos cos 75cos45 cos54.7 30.6MPar
Question4(Contd):
9
A stress of 75 MPa is applied in the [001] direction on an FCC single crystal. Calculate
(a) the resolved shear stress acting on the slip system and (b) the resolved
shear stress acting on the sli p system.
(111)[101]
(111)[110]
(b)
cos cos 75cosr
Question4(Contd):A stress of 75 MPa is applied in the [001] d
(a) the resolved shear stress acting on the
shear stress acting on the sli p s(111)[110]
asi
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A 70% Cu 30% Zn brass wire is cold drawn 20 percent to a diameter of 2.80 mm. The
wire is then further colddrawn to a diameter of 2.45 mm. Definition of cold reduction is
given as:
changeincrosssectionalarea%coldreduction 100% 100%
originalcrosssectionalarea
o i
o
A Ax
A
a) Calculate the total percent cold work that the wire undergoes.
b) Estimate the wires tensile, yield strengths and elongation from figure (a) in the
appendix
2 2
1
2
1
2 2 21 1
1
2.80mm
2 220% 100%
2
0.20 7.84mm
3.13 mm
d
d
d d
d
2 2
2
Total%coldwork
3.13mm 2.45mm
2 2100%
3.13mm
2
38.75%
(a)
Question5(ColdWork):
11Figure (a): % Cold work v
work is expressedas a p
For Cold Work 39%,
TensileStrength 76kpsi
YieldStrength 64kpsi
ksi:1000psi
Elongation 7%
Question5(ColdWork):
A 70% Cu 30% Zn brass wire is cold draw
wire is then further colddrawn to a diamet
given as:
a) Calculate the total percent cold work t
b) Estimate the wires tensile, yield stren
appendix
Derivetheleverrulefortheamountinweightpercentofeachphaseintwophase
regionsof abinaryphasediagram.Useaphasediagraminwhichtwoelementsare
completelysolubleineachother. Isomorphous
1L SX X
0 L
S
S L
w w LOX
w w LS
S o
L
S L
w w OSX
w w LS
X:weightfraction
Total B = B in Liquid + B in Solid
Similarly,
0
0
0
0
1
L L S S
S L S S
L S L S S
L S S L
w X w X w
w X w X w
w w X w X w
w w X w w
Question6(LeverRule):
13
0 53 45
58 45
LS
S L
w wX
w w
58 53
58 45
S oL
S L
w wX
w w
0
5 845 58
13 13
17. 3 3 5.7 53 %
L L S Sw X w X w
wt N i
ExtraSlideonLeverRule
0
1 30 0 ,
53 %58 %
45 %
o
S
L
At T C
w wt Ni w wt Ni
w wt Ni
p/s: Tielineisusedin2phaseregiononly
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Ag=88wt%
T=1000oC
Consider the binary eutectic coppersilver phase diagram. Make phase analyses of an
88 wt% Ag 12 wt% Cu alloy at the temperatures (a) 1000oC, (b) 800oC, (c) 780oC + T,(d) 780oC T. T is assumed to be less than 1oC. In the phase analyses, include:(i) The phases present; (ii) The chemical compositions of the phases; (iii) The amounts
of each phase; (iv) Sketch the microstructure by using 2cmdiameter circular fields.
wt% cm
10 1.25
8 1
Question7(PhaseDiagram):
15
(a)T =1000oC
(i)Phasespresent: Liqu
(ii)Compositionofphase: 88wt
(iii)Amountofeachphase:
T=1000oC
wt%ofliquidphase 100%
T=800oC
(b)T = 800oC
(i)Phasespresent: Liquid Beta(ii)Compositionofphase: 78wt%Ag 93wt% Ag
(iii)Amountofeachphase: (iv)Micro
structure
Ag=88wt%
93 88wt%ofliquidphase 100% 33.3%
93 78
88 78
wt%ofbetaphase 100% 66.7%93 78
17
(b)
9378
L
(c)T = 780oC+T
(i)Phasespresent: Liqu
(ii)Compositionofphase: 71.9w
(iii)Amountofeachphase:
A
91.2 88wt%ofliquidphase 10
91.2 71.9
88 71.9wt%ofbetaphase 100
91.2 71.9
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(d)T = 780oC T
(i)Phasespresent: Alpha Beta
(ii)Compositionofphase: 7.9wt%Ag 91.2wt% Ag
(iii)Amountofeachphase: (iv)Microstructure
Ag=88wt%
T=780oC T, T
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Os=30wt%
T=2665oC +T
(c)T = 2665oC+T
(i)Phasespresent: Liquid Beta
(ii)Compositionofphase: 23wt%Os 61.5wt% Os
(iii)Amountofeachphase: (iv)Microstructure
61.5 30wt%ofliquidphase 100% 81.8%
61.5 23
30 23wt%ofbetaphase 100% 18.2%
61.5 23
23Ni=
T=1517oC T
Consider an Fe 4.2 wt% Ni alloy that is s
the amount of phase and phase, respectT to less than 1oC.
Question9(Peritectic):
Ni=4.2wt%
T=1517oC T
4.2 4wt%of phase 100% 66.7%
4.3 4
4.3 4.2wt%of phase 100% 33.3%4.3 4
Peritectic:L+
RH
side:
L
+
LHside:L+L
25
L[LNChap7p15]
Eutectic L +Eutectoid +
Peritectic +L
Peritectoid +
Monotectic L1 +L2
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Martensite:
Metastable phaseconsisting
ofsupersaturatedsolid
solutionofCinBCCorBCC
tetragonaliron.
Causedbyrapidcoolingof
austeniticsteelintoroom
temperature(quenching).
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Pearlite(layered +Fe3C)
Bainite(nonlayered
Pearlite)
Ms
MfMartensite (bct)
250oC
550o
C
+Fe3C
+Fe3C
723oC
IsothermalTransformationDiagramofEutectoid pla
(0.8wt%C)
Time (s
ForTutorial5Question2
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Chap.8MetallicAlloys1. Eutectoid(0.8wt%C,ifnothyper/hypo pro ) AusteniteFCC (at723o
FerriteBCC0.02wt%C+ Cementite/IronCarbideFe3C6.67wt%C
2. Martensite:
Quench to
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Chap.9Polymers1. Polymerization:Chain:freeradical,Stepwise:Condensationbyproduct,N
2.
3. Vinyl,Vinylidene,zigzag,entangled,secondarybondsbtwchains,550n
Copolymers(random,alternating,block,graft)
4. Thermoplastics:PE:CH2=CH2,HD:littlebranching,chainsclosepack,incc
PVC: CH2=CHCl,strongstrengthstrongdipole,brittleCl steric hindrancer
PP:CH2=CHCH3 ,CH3restrictrotationincstrengthhardnessstabilitydec f
PS:CH2=CH ,bulky,rigid,inflexible,brittle,dimensionstable
PTFE:
CF2=CF2,
small
regular
F
dense,
strong
dipole
chemical
resistance
hi
5. Thermosetting:covalentbondnetworke.g.Phenolics rigidstablecreepc
6. Elastomers (Rubbers): Vulcanizationcrosslinking isoprenegreatdimensio
7. SolidificationofThermoplastics:
8. DeformationofThermoplastics:
9. Effectsof
Temperature:
10. StrengtheningofThermoplastics:incmolecularwt.(notmuchincbeyond
crystallinity (effectivepacking),pendant(hinderchainslippage),polar(m
MolecularmassofpolymerDP=
Massof
amer
i i
m
i
f MM
f
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Ferrite
Cementite
orIron
carbide
Eutectoid
Pearlite
Hypo Eutectoid Hyper
0.8wt%C
+Fe3C
Proeutectoid Fe3C+Pearlite
Proeutectoid +Pearlite
Pearlite
A hypoeutectiod plaincarbon steel was slow
carbon concentration (in wt%) in the carbon
723C T? (Hint: see microstructure)
Ferrite
Auste
x
5.9wt%
Tutorial5Question1:
Draw timetemperature cooling paths for a 1080 steel on an isothermal transformation
diagram that will produce the following microstructures. Start with the steels in the
austenitic condition at time = 0 and 850C.
(f)100
%
lower
bainite
1080Steel 0.8wt%C Eutectoidcomposition
P
B
Ms
Mf
(a) 100%martensite
(c)100%finepearlite +Fe
3C
(e)100%upperbainite
Time (s)
Question2:
+Fe3C
Ms
Mf
(b)50%mar
+50%coars
(d) 50%martensite
+50%upperbainite
+Fe3C
+Fe3C
Question2(Contd):
1% 1
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CentralLibraryRBR (2hrs)
Callnumber: TA403Smi 2009
Whatisthemicrostructureproducedafterau
Doesanaustempered steelneedtobetempe
After austempering, a eutectoid plaincarb
Subsequent tempering is not necessary sidistortion and impact energy values comp
with a marquenched and tempered steel.
A
[TBFig.9.34]
Question3:
reheatMartensite atmartensite
Martempering:Tempering:
QuenchAustensite to>Ms,
Holdtill
Tuniform,
then
slow
cool,
finalTempering
Temperedmartensite
Impactenergy>tempered
(Waterquench+Temper) (Marquenching +temper)
[TBFig.9.29] [TBFig.9.33]
Describethefourdecompositionstructurest
whenasupersaturatedsolidsolutionofanA
Supersaturated solid solution (FCGP1 zones: consist of segregated regions in th
few atoms thick (0.4 to 0.6nm) and
in diameter.
They form on the {100} cubic plane
straining the lattice tetragonally
with the matrix.
GP2 zones ( phase): approximately 1 to 4nm thick an
diameter.
These zones are also coherent wit
and have a tetragonal structure.
[TBp.407409]
Question4:
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Supersaturated solid solution (FCC)GP1 zonesGP2 zones ( phase) phase: nucleates heterogeneously and is incoherent with the
matrix.
This phase has a tetragonal structure with a thicknessof 10 to 150nm.
phase (CuAl2): an incoherent equilibrium phase having the
composition CuAl2.
This phase, which forms from or directly from thematrix, has a BCT structure.
[PhaseTransformationsinMetalsandAlloysbyD.A.PorterandK.E.Eastering,p297]
Question4(Contd):Describethefourdecompositionstructuresthatcanbedeveloped
whenasupersaturatedsolidsolutionofanAl4%Cualloyisaged.
Extra:
Determine the mole fraction of polyvinyl chlo
having a molecular weight of 11,000 g/mol and
avav
MW (polymer) 11,000g/mMW (mer)
DP 150
av PVC PVC PVAc PVAc PMW (mer) MW MW f f f
PVCMW 3H 2C 1Cl
3 1 2 1 2 1 35.5
62.5g/ mol
PVAcMW
6 1
86.0g
PVC PVAc0.539 0.461f f
Question5:
Howisitpossibleforapolymerchainsuchasapolyethyleneonetokeepgrowing
spontaneouslyduringpolymerization?
The polymer chains in chain polymerization keep growing spontaneously because the
energy of the chemical system is lowered by the chain polymerization process; the
total energy of newly created polymers is lower than the total energy of the
monomers that have reacted to form them.
Monomerschemicallyreactwitheach
othertoproducelinearpolymersand
asmallmoleculeofbyproduct
[LNChap9p5,6,11]
heat
Question7:
1 . ChainPolymerization:
2. Stepwise
Polymerization
(Condensation):
Explainhowdoestheamountofcrystallin
(a)density,(b)tensilestrength
(a) Density increases, due to increase of t
(b) Tensile strength increases, due to str
between the polymer chains that are p
Question8:
Amorphous
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How much sulphur must be added to 70g of butadiene rubber to cross link 3.0 percent of
the mers? (Assume all sulphur is used to crosslink the mers and that only one sulphur
atom is involved in each crosslinking bond.)
polybutadieneMW
6H 4C 54g/mol
NumberofofmolesofButadiene
70g = 1.2963
54g /mol
Vulcanization
3NumberofofmolesofSulphur= NumberofofmolesofButadiene
100
MassofSulphur=0.03 1.2963mol 32g/mol=1.24g
Question6:(lecturehasntcovered)
How does the presence of a methyl group
polymer chain affect the glass transition temp
polyethylene?
Thesubstitutionofhydrogenatomswithmeth
increasesthebondstrengthsbyrestrictingthe
Consequently,polypropylenehasahigherglas
[MaterialsScienceandEngineering:AnIntroduction
Callister 7th edn.p.501 CLRBRTA403Cal2007]
Question9:(lecturehasntcovered)
Polyethylene
[MaterialsScience
andEngineering:An
Introduction,byW.D.
Callister 7th edn.
p.548]
CentralLibraryRBR
Callnumber:
TA403Cal2007
Extra:FactorsthataffectGlassTransitionTemperatureTg :
[MaterialsScienceandEngineering:AnIntrod
For noncrystalline thermoplastic:
The liquid, upon solidification, changes to a superco
liquid that is in the solid state, which is rubbery or f
leathery, at temperature below TmAs the temperature decreases, the polymer shows a
decrease in specific volume until the temperature r
Below Tg, the polymer becomes glassy and brittle.
For partly crystalline polymer:
Its specific volume drop abruptlyat Tm , due to more
Extra:CharacteristicchangesduringGlassTra
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Chap.10CeramicsOx
. , , , ,
2. AXStructure( +chargebalance):
3. FCCInterstitialsites:Octahedral Tetrahedral vs HCP
r
R
0.410.2250.155
CN=4
ZnS
4. CsCl,NaCl,ZnS,Antifluorite,CaF2
FCC:4atoms4octahed 8tetrahed
HCP:6atoms6octahed 12tetrahed
5. Corundum(Al2O3):6O2 formFCCwithAl3+ at4among6octahed
Li2ONa2O UO2NuclearFuel
emptyoctohed 3 2 2a r R
2 2a r R
3
4
ar R
3Graphite:3sp2formcovalentlayer,1pelectronbond btwlayers ,Spinel (
6. Silicates(SiO42):tetrahedralislandchain/ring(2corners)
2,
7. MaterialspreparationFormDryingSinteringVitrification
~w S con_ ox e
. 2 3, 3 4, , 2
9. Toughness: ZrO2 9mol%MgO cubictetragona IC fK Y a
10. Glasses: Structure,Composition, TemperedGlas
* expoQ
RT
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[BookbyCallister CLRBRTA403Cal2007]
2
3a
3
4
a
Tutorial6Questi
Calculatethecriticalradius
Calculatethedensity ingramspercubiccentimetreofCsI,whichhastheCsCl structure.
IonicradiiareCs+ =0.165nmandI =0.220nm.
3 2a r R
Question2:
8
20.165nm 0.220nm
3
0.445n m 4.45 10 cm
a
22ll132.9
g / mol 126.9
g /mol
un tcell 23 23 .
6.02x10 ions/ mol 6.02x10 ion/ mol
223
3 38
4.32 1 0 g4.90g/cm
4.45 10 cm
m mdensity
v a
4
Calculate the planar densitie
(111) and (110) planes for (a)
Ionic radii are Co2+ = 0.082nm
2
(a)CoO
Question3:
2
0.0820.621
0.132
r o
r O
0.414 0.732r
R
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2
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Ce O2 4Ce4+ 8O2
Question4:Calculate the linear density of Ce4+ and O2 in ions per nm2
in the [111] and [110] directions for CeO2,
which has the calcium fluorite (CaF2) structure.
Ionic radii are Ce4+ = 0.102nm and O2 = 0.132nm.
4 2Ce O
3
4
40.102 0.132 0.540nm
3
a r R
a
4 24 2
L
12 Ce 2O
1Ce 2O2111
10
4 23a 3 0.540nm
1.07Ce 2.14O /nm
44
4L
12 1 Ce
2Ce2110 2.62Ce / nm
2a 2 0.540nm
CaF2
4Ca2+ formsFCC
8F occupytetrahedral
Antifluorite
e.g.Na2O,
Li2O
What causes the lack of plasticity in crystalline
ceramics?
Thelackofplasticity incrystallineceramics
is attributed to their Ionic and Covalent
Question5:
chemicalbonds.
InCovalentlybondedceramics,thebondingbetweenatomsis
specific anddirectional.
Specific:betweenthese2atoms,
Directional:must
be
of
certain
angle 1
2
3
4
5
67
1
2
3
4
5
6
7
[TBChap11p611613]
Therefore,theywillundergobrittle
fracturesascovalentbondsare
brokenwithoutsubsequentreformation.(unlikeinmetallicmaterials)
1 2 3 4 5 6 1 2 3 4 5 612
For Ioniccrystals,theslipofoneplaneofions
involvesionsofdifferentchintocontact,andthusattrac
Question5(Cont
repu s ve orcesmay epro
Forexample,intheNaCltyp
Sliponthe{110}familyofpslipplanesremainattracted
Incontrast,sliponthe{100
samechargeswillrepeleac Hence,therearelimitedsli
lackofplasticity inionically
Polycrystalline ioniccerami
cannotcontinueacrossthe
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(110)
(100)
110
(100)
[010]
(110)
impossible
14
possible
Explain the plastic deform
solids such as NaCl and MgO
What is the preferred slip sy
Question6:
Fo r some sin glecry
compressive stresses at
prior to fracture because
other.
These slip planes, wh
110typ ca y pre er t e
How do (a) porosity and (b) grain size affect the tensile strength of ceramic
materials?
a) Porosity: [LNChap10p24]
Question7:
Pores serve as stress concentration points and induce cracks at lower
threshold values.
They decrease the effective crosssectional area for load distribution as
well.
Consequently, as the porosity of a ceramic material increases, the material
tensile strength decreases.
b Grain Size:
For a porosityfree ceramic, the flaw size, and thus the strength, is solely a
function of grain size
The finer the grain size, the smaller the flaws and the greater the ceramic
tensile strength.
16
s
(surfacedefects, void
[LNlastyear]
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