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Unit5
1
EngineeringMaterials
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ModernEngineeringMaterials
Metallicgla
sses
Nano-phasematerials
Ceramics
Bio-materials
Shapem
emoryalloysan
d
Syntheticmaterials
2
oernengn
eerngmaerasare
,wc
are
preparedbyg
roupingonekindofmaterialwiththeother.
1.
Metalmixed
withpolymer.
2.
Ceramicmixedwithmetals.
Itwasfoundthattheresultantm
aterialswithpeculiarpropertieswhich
varieswithrespecttothesize,shapeandthenatureofmixture.
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ME
TALLICGLASSES
ME
TALLICGLASSES
ME
TALLICGLASSES
ME
TALLICGLASSES
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MetallicGlasses
Modernengineeringmaterials
withhighstreng
th,goodmagnetic
propertiesandbettercorrosionresistance.
Metalsaresolids,whichexhibitscrystallineproperty,
malleability(flexible),duc
tility(abilitytodeformunderstress)etc.
Glass
esaresolidsinth
eamorphousforminwhichtheatoms
4
a
rrangementarenotpero
canteyarerreguar.
Theyare
transparent,brittle(breakable),n
on-magneticinn
ature.
SotheMetallicglassessharethepropertiesofb
othmetalsandg
lasses.
Metallicglassesarestrong,ductile,malleable,o
paqueandamorphous.
Theyhavego
odmagneticpropertiesandhighcorrosionresista
nce.
Metallicglass
=Amorphousmetal
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Tempe
ratureatwhich
theliquidlikeatomicconfigur
ationcan
befrozeninto
asolidisknow
nasglasstransitiontemperature.
Glass
transitiontemperatureform
etallicalloys
isabout
20Cto300C
.
GlasstransitionTemperatu
re(Tg)
TypesofMetallicGlass
es
5
Metallicglassesareoftwotypes.T
heyare
i.Metal-Metalloidglasses:
(Fe,Co,Ni)-
(B,Si,C,P
)
ii.Met
al-Metalglass
es:
(Ni
-Nb,Mg-
Zn,Cu-
Zr,Hf-Vaalloys)
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i.
Twin
rollersystem
Moltenalloyispassedthroughtw
orollersrotatin
gin
oppositedirections.
ii.Melt
spinningsystem-Quench
in
P
roductiono
fMetallicG
lasses
6
Moltenalloyjetim
pingesonafas
trotatingroller.
iii.Melt
extractionsystem
Fa
stmovingrollersweepsoffmoltendropletinto
astrip
fromasolidrod.
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"Quenching"isatechniq
ueusedtoform
metallicglasses.
Quenching
meansrapidcooling.
Actuallya
tomsofanymaterialsmovefre
elyinaliquidstate.
Atomscan
bearranedr
eularlwhenaliuidiscoole
dslowl.
MeltS
pinning
Principle
7
Instead,whenaliquidisquenched,
therewillbeanirregular
pattern,w
hichresultsintheformationofmetallicgla
sses.
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F
abricationProcedure
Ameltspinn
erconsistsofadiscmadeupofcopper.
Discisrotatedatahighspee
d-50m/s.
Aproperlysuper-heatedmoltenalloyisejected
underpress
ure(heliumorargon)through
afine
nozzleatthe
bottomofarefractorytubeontothe
spinningdisc.
8
Ejectedmelt
iscooledatafa
sterratewithth
ehelpofrotating
cooledcopp
erdisc.
Thus,aglass
yalloyribbons
tartsgettingformedovertherollerdisc.
Alloyismeltedbyinductio
nheating.
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PropertiesofMetallicGlasses
(a)Metallic
glasseshaveTetrahedralCloselyPacked(TCP)structure
ratherthanhexagonalc
loselypacked(HCP)structure.
(b)Theydo
nothaveanyc
rystaldefectssuchasgrainbou
ndaries,
dislocations,etc.
StructuralProperties
9
Mechanical(o
r)GeneralProperties
(a)Themetallicglassesare
verystrongin
nature.
(b)Theyha
vehighcorrosionresistance.
(c)Theypo
ssessmalleability,ductilityetc.
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MagneticProperties
(a)Theyexhibithighsaturationmagnetisation.
(b)
Metallicglassesaresoftmagneticmat
erials
sotheycanbe
easilymagnetised&demagnetised.
(c)
Theyhaveverynarrow
hysteresisloop
.
Sothehystersislossesarealmostneglig
ible.
10
d)
Theyexhibitverylowhysteresislossand
hencetransformercorelossisveryless.
(e)Theyhavehighmagneticpermeabilityand
exhibitferromagnetism.
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4.ElectricalProperties
(a)Metallic
glasseshavehighelectricalresistance(100
-cm).
(b)Highele
ctricalresistivityleadstoveryloweddycurrentlosses.
(c)Atlowte
mperature,res
istivityisminimum,
belowwh
ichit
variesasalo
garithmicfunctionoftemperature.
(d)Atverylowtemperatur
e,thermalexpansionco-efficientis
11
negave.
5)Metallicg
lassesareamorphousmetalal
loyswhichhavenolong
rangeatomicorder.
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Ap
plicationsofMetallicGlasses
1.
Metallicglassesareusedintaperecorderhe
ads,coresofhig
hpower
transformersandmagnetic
shields,sincemetallicglassespossesslow
magneticloss,highpermeability,saturation
magnetization
andlow
coercivity.
2.
Theyhave
higherworkability.Theycan
beeasilybent
without
12
.
.
3.
Metallicglasseshavehigh
electricalresistancewithnearlyzero
temperaturecoefficientof
resistance.Hencetheyareused
tomake
accurate
standard
resistances,computer
memories,
magnet
resistance
sensors
and
cryo-thermome
ters
(low
tem
perature
measuringthermometer).
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4.
Metallicglassesareveryusefulintheprodu
ctionofvery
highmagneticfields.
5.
Sincethey
arenotaffectedbynuclearradia
tion,theyareuse
d
inmakingcontainersfor
radioactivew
astedisposal.
6.
Sincethehaveverhihc
orrosionresistanceCrandP
13
basedmeta
llicglassesareusedinmarinecab
les,innersurface
ofreactor
vessels,orthopaedicalimplantsa
ndsurgicalclips.
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mart
Materials
mart
Materials
mart
Materials
mart
Materials
14
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Analloy
isapartial
orcompletesolidsolutionof
oneorm
oreelementsinametall
icmatrix.
Completesolidsolutionalloysgive
singlesolidphase
microstru
cture.
Alloy
15
Partialsolidsolutionsgivetwoormorephasesw
hich
arehomogeneousindistributiondepe
ndingonheat
treatmen
t.
Alloying
onemetalwithothermetal(s)ornonmetal(s)
oftenenhancesitsproperties.
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Physicalproperties
sucha
sdensity,reac
tivity,young's
modulus,and
electrical
andthermalc
onductivityof
analloymaynotdiffergreatly
fromthoseofitselements.
Engineeringproper
ties
suchastensilestrengthandshearstrengthmaybe
16
susanay
rom
oseo
e
consuenma
eras.
Steelisametalalloywhosemajorcompon
entis
ironwithca
rboncontentbetween0.02%a
nd2.14%
bymass.
Forexample,steelisstrongerthaniron,itsprimaryelement.
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Brassisa
nalloymadef
romcopperan
dzinc.
Bronzeusedforbearing
s,statues,orn
amentsandch
urch
bells,isanalloyofcopp
erandtin.
17
1.Unlikepuremetals,mostalloyso
nothaveasingle
meltingpoint.
2.Instea
d,theyhavea
meltingran
geinwhichth
e
materialisamixture
ofsolidandliquidphases.
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SSSShape
hape
hape
hapeMMMMemo
ry
emo
ry
emo
ry
emo
ryAAAAlloy(SMA),
lloy(SMA),
lloy(SMA),
lloy(SMA),
ametal
that"remembersitsgeom
etry
18
Sma
rtMetal
Sma
rtMetal
Sma
rtMetal
Sma
rtMetal(or)(or)(or)
(or)MemoryAlloy
MemoryAlloy
MemoryAlloy
MemoryAlloy,,,,
Intellig
entMaterials
Intellig
entMaterials
Intellig
entMaterials
Intellig
entMaterials(or)SmartAlloy,
(or)SmartAlloy,
(or)SmartAlloy,
(or)SmartAlloy,
MuscleWire
MuscleWire
MuscleWire
MuscleWire(or)
(or)
(or)
(or)ActiveMaterials
ActiveMaterials
ActiveMaterials
ActiveMaterials
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S
hapeMemo
ryAlloys(S
MAs)
Shapememoryal
loysarespecia
ltypeofalloyswhich
afterbein
gdeformed
canrememberandrecovertheir
originalshapewhensubjectedtothe
appropriateth
ermal
procedure
(Heating/Coo
ling).
19
Theabilityofthemetallicalloystoretaintheiroriginal
shapewhe
nheating/co
oling.
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1.Co
pper-Aluminiu
m-Nickel(AlNiCo)
2.Co
pper-Zinc-Alu
minum-Nickel
and
3.Nickel-Titanium
(NiTi)alloys.
Threemaintypeso
fshapemem
oryalloys
SMA'sca
nalsobeused
byalloying
20
ExamplesofSMAs
a.Au-Cd
alloy
b.
Ti-Nialloy
c.Mn-Cua
lloy
d.Ni-Mn
-Gaalloy
e.Cu-Al-Niallo
y.
Z
inc,Copper,Gold,Mangan
eseandIron.
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T
ransformationTemper
ature(Tt)
Shapereco
veryprocess
occursnotatasingletem
perature,
ratheritoccursoverarangeoftemperature.(60-1450K)
TherangeoftemperatureatwhichtheSMAswitche
sfrom
new
shape
toitsorigin
alshapeisc
alledTransfo
rmation
Temperatu
re(or)Memo
ryTransferTemperature.
21
BelowTt,SMAcanbebe
ntintovariousshapes.
AboveTt,SMAreturnst
oitsoriginalshape.
Thischangeinshapewasmainlycausedduetothechangein
crystalstructure(phase)
withinthem
aterials,due
tothe
rearrangementofato
mswithinitse
lf.
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(i)Martensite
Martensite
,namedafterthe
Germ
an
Solidcrystallinestructure
mostcomm
onlyreferstoaveryhard
formofste
elcrystallinestructure.
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Martensite
isaninterstitialsupersolutionofcarb
onin
-ironanditcrystallize
sintotwinned
structure.
Ithaspla
teletstructure
.
Martensite
istherelative
lysoftandeasilydeformed
phaseof
shaemem
oralloswh
icexistsatlo
wertemer
atures.
Martensites
tructurehavet
woforms
a)Twinnedmartensite
beforeloadingand
b)
Deform
edmartensite
afterloading
.
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(ii)
Austenite
Austenite(orgammaphaseiron)isa
metallicnon-magnetic
allotropeof
ironorasolidsolutionofiron,withan
solidsolutionofiro
n
.
Itisnamed
afterSirWilliamChandler
Roberts-A
usten(1843-1902).
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Austeniteisthesolidso
lutionofcar
bon
andothera
lloyingelementsing-ironandit
crystallizes
intocubicstr
ucture.
Ihasneedlelikestructure.
26
Austenite
isthestrongerphaseofsh
ape
memorya
lloyswhicho
ccursathigher
tempera
tures.
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M
artensite
A
ustenite
Alp
haphaseiron
in
Cry
stallinestructure
Gamm
aphaseironin
Cubicstructure
Plateletstructure
Needlelikestructur
e.
otaneasy
deformedphas
e
Stro
ngerphase
Low
ertemperatures
Highertemperature
s
Twinn
edmartensitebeforeloading
Deformedmartensiteafterloading
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Char
acteristics
SMA'sarem
etalswhichex
hibittwouniqueproperties
1.
ShapeMem
oryEffect
2.
Pseudoelas
ticity(or)Sup
erelasticity
withou
tchangeintem
perature
wtchangeintemperature
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ShapeM
emoryEffe
ct
Thephenom
enoninwhich
theshapemem
oryalloyapparently
deformed
atlowertemp
andreturns
toitsoriginalshape
(formershape)whenheate
dtohighertemp".
When
temperature
is
29
decreased,
phasetransfo
rmation
take
place
from
austenite
to
twinnedmartensite.
i.e.,amicroco
nstituent
transformationtakesplace
fromthe
AustenitetoMartensite.
1
2
3
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Duringthisstatethe
twinned
martensite
phasewillhavesame
sizeasthatofaustenitep
hase.
Whenloadisappliedtothe
3
1
30
,
deformed
martensitephase.
Whenthe
materialisheatedit
will
go
from
deformed
martensite
to
austenite
form
andthecyc
lecontinues.
2
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Pseu
do-elasticity(or)Super
Elasticity
a)Pseudo-elasticityoccursin
shapeme
moryalloysw
henthe
alloyisc
ompletelycomposed
ofausten
ite(temperatu
reis
31
.
b)Unliketheshapememoryeffect,
pseudo-el
asticityoccurs
without
achangein
tempera
ture.
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Themartensiticphase
isgenerated
bystressin
gthe
metalintheaustenitic
stateandthis
martensiteph
aseis
capableof
largestrains.
With
the
removal
of
the
load
,the
mart
ensite
transformsbackinto
theaustenite
phaseandresumes
Pseu
do-elasticity
32
itsoriginalshape.
(Process
similartopre
ssing
arubberorspring).
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H
ysteresis
Onhe
ating-Transfo
rmMartensi
tetoAustenite.
Thedifferencebetweenthetransitionte
mperaturesupon
heatingand
coolingisca
lledHysteresis.
The
difference
between
the
33
temperatureatwhichthematerial
is50%transformedtoaus
tenite
upon
hea
ting
and
50%
transformed
tomartensite
upon
cooling.
Differenceca
nbeupto20-30C.
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34
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Effects
ofSMA
(i)One-wa
yshapememo
ryalloy
(ii)Two-wayshapememo
ryalloy
(i)One-waySMA:
Whenthematerialiscoole
dbelow
35
themartensiteends(Mf)temperature.
Thenthereexistsomemino
rchangeandwillremainin
martensitefo
rmalone.
Thus,thoughthereissomechangeinits
temperature,theSMA
remainsinthesamephaseandthistyp
eofmaterial
iscalled
onewayshapememoryalloy.
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Ifthetemperatureisincreasedthen
themartensite
becomesa
usteniteandifthetemperat
ureisdecrea
sedit
reversesitsstate.
(ii)Two-w
aySMA:
36
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Applica
tionsofSMAs
1)
Firesafetyvalve
2)
Antennawires
3)
Toysan
dnovelties
7)Blood-clotfilter
8)Cryofith
ydrauliccouplings
9)Circuitedgeconnector
37
yega
ssrames
5)
Coffeepotthermostats
6)
Helicopterblades
orrectterreguart
esnteet
11)Artificialhip-joints,bone-plates
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Advantagesof
shapememo
ryalloys
Simp
licity,compactnessandsafety
mechanism.
Bio
compatibility.
Diversefieldsofap
plication,clean
,silent,sparkf
ree
wor
kingcondition
.
Goo
dmechanicalproperties.(stro
ng,corrosionr
esistant)
38
Degrad
ationpoorfatigueproperties.
Expensive.
Lowenergyefficiency.
Limitedbandwidthduetoheatingandcoolingrestrictions.
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Mo
dernE
nineerin
Mo
dernE
nineerin
Mo
dernE
nineerin
Mo
dernE
nineerin
39
Mat
erials
Mat
erials
Mat
erials
Mat
erials
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Nano-Ph
aseMaterials
Nanoscien
ceisthestudyofthefundamentalprinciplesofmolecules
andstructu
reswithatleastonedimensionsintherangeabout109m
to107m(1to100nm).
Atomsareextremelysmallandthediameterofasingleatomscanvary
from0.1to
0.5nanometersd
ependingonthetypeofelements
(nanometer
is109m).
40
molecules
(or)atomsdonot
moveawayfrom
eachother.
Allmaterialsarecomposedofgrains,whichinturncomprisem
ayatoms
Nanomaterialswheninpow
derform(calledn
anopowder)havegrain
sizesinthe
orderof1-100nm.
ex:ZnO,Cu-Fealloy,N
i,Pd,Pt,etc.
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Innanom
aterialsthemajorityoftheatomsa
relocatedonthe
surface
ofthepa
rticlesandhence
theatomsareofadifferentenvironment.
Nanomaterialshaveincreasedsurfacearea
ofthesubstance
with
highsurfaceareashaveen
hancedchemical,mechanicalopticaland
magnetic
properties.
41
Nanotech
nologyisafieldofappliedscience
focusedonthed
esign,
synthesis,characterizatio
nandapplicationofmaterialsand
devices
onthenanoscale.
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ClassificationofNa
nostructured
materials
Classificationbasedonthenumberof
dimension
sliewithinthen
anometerrange.
(1)Zerodimensionalnanostructure(0D
)
Ex:atoms
42
(2)Onedimensionalnan
ostructure(1D)
Ex:atomclusters
Multilayeredmaterialwithlayerofthicknessin
thenanometerrange-1D.
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ClassificationofNa
nostructured
materials
(3)Twodimensionalnanostructure(2D)
Ex:Nanotube.
Layersinthenanometerthicknessrange-2D
.
43
(4)Three
dimensionalna
nostructure(3D
)
Ex:
Quantumwell.
Materialwiththreedimension
alequiaxednano
size
grain.
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Quantum
wells,Quantumwiresand
Quantumdo
ts
Whensize
ofamaterial-reduced-
bulkormacro
scopicsize-verysmallsize
P
ropertiesremainsame
Sizedropsbelow100nm
Drasticchanges
inpropertiescanoccur.
If1D-reduced-
nanorange-
44
w
hiletheothertwodimensions
r
emainlargeresultingstructure.
If2D-reduced-nanorange-
oneremainslarge-resulting
s
tructure.
S
izereductioninw
hichallthree
d
imensionsleadstolownanometer
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Fabrica
tionmet
hods
45
Itresultsduetobuildingblock
ssuch
asatomsandm
oleculesandassemble
them
into
larger
nanostructured
material.
Itresultsduetobreakin
gdownof
largep
iecesofbulkm
aterialto
generatetherequiredfor
m.
Bottom-upapproach
Top-downappr
oach
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a.Milling
b.
Lithographics
c.
Machining
1.
Vaporp
hasedepositionm
ethods
a.C
hemicalvapordeposition
Bottom-upapproa
ch
Top-downapproa
ch
46
b.Physicalvaporde
position
2.
.Plasm
aassisteddepo
sitionprocess
3.
Molecularbeamepitaxy(MBE)
4.
Metalo
rganicvaporphaseepitaxy(MOVPE)
5.
Liquid
phaseprocesses
a.C
olloidalmethod
b.Sol-gelmethod
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Top-down
processesstarts
withlargescaleobjectandgradually
reducesitsdimensions.
Thetop-do
wnapproachesaresimpler.
Top-down
approach
47
Methodsu
sedtoproduce
nanostructuredm
aterialsunderto
p-down
approacha
regivenbelow.
a.
Milling
b.
Lithographics
c.
Machinin
g
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1)
Itisalsok
nownasMechanicalalloyingorMechanicalattrition.
2)
Itisasolidstateprocess.
3)
Highenergyballmillingcaninducestructuralchangesand
chemica
lreactionsatroomtemperature.
Itconsistsofstainlesssteelrotatingdrumwithhardsteelortungsten
HighEner
gyBallMillin
g
Procedure:
TopDownapproach
48
carbideballsinsideit.
Thecontain
erispurgedand
argonisintroducedtoprevent
unwanted
reactionsuchasoxidation.
Millingisca
rriedoutatroom
temperatureforu
pto150hours.
Powdermaterialsarecrushedmechanicallyintherotatingdr
umbythe
hardballs.Thisrepeateddeformationcancause
largereduction
singrain
sizeinthepow
derparticles.
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Atoms,mole
culesandevennanoparticlesthemselvescanbeu
sedasthe
buildingblocksforthecreationoflarger
nanostructurewithrequired
properties.
Bychanging
thesizeoftheb
uildingblocksan
dcontrollingtheirassembly
andarrangementitisposs
ibletochangethepropertiesofthe
nanostructuredmaterial.
Bottom-upapproach
50
,
,
andmoleculesintothelarger
nanostructureiscarriedoutbyas
equenceof
chemicalreactionscontrolledbycatalysts.
Thisisave
rypowerfulapp
roachofcreatingidenticalstructureswith
atomicprecision.
1.VaporPha
seDepositionmethods(CVD)
2.Plasmaassisteddepositionprocess
3.Molecular
BeamEpitaxy(MBE)
4.Me
talorganicvapourph
aseepitaxy
5.Liquidphaseprocesses
a.Colloidalmethod
b.Sol-gelmethod
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CVDinvolvestheflowofagaswithdiffusedre
actantsoverahot
substrate
surface.
Gasthatcarriesthereactantsis
calledthecarriergas.
Whilethegasflowsoverthehotsolidsurface,theheatenergyprovokes
chemicalreact
ionsofthereac
tantsthatform
film
duringandafterthe
reactions.
Bottom-Upapproach
ChemicalVaporDeposition(CVD)
51
.
Thinfilmofd
esiredcompositioncanthusbecr
eatedoverthesurfaceofthe
substrate.
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Resistanceheaterseithersurroundthechambe
rorliedirectlyu
nderthe
susceptorth
atholdsthesubstrates.
InCVDmethodcarbonnanotubesaregrownfromthedecompo
sitionof
hydrocarbonsattemperatu
rerangeof500to1200C.
Theyaregrownonsubstrate
ssuchascarbon
,quartzandsilic
onoron
floatingfin
ecatalystparticleslikeCO,Fe,N
ifromhydrocarbonssuch
Bottom-Upapproach
52
Growthof
nanostructurescanoccureitherintheheatingzon
ebefore
oraftertheheatingzone.
Thegrowthprocesstakesab
out30minutes.TheflowofH2ga
sis
maintainedat200ml/minut
es.Inertgasisusedtocoolthereactor.
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Pla
sma-assisted
depositionprocess
Sputtering
isaprocessinwh
ichenergetic
ionsknockatomsormoleculesfromatarget
thatactason
eelectrodeand
subsequently
depositthemon
asubstratethatisactingasan
anotherelectrode.
Bottom
-Upapproach
Thematerialtobedepositedse
rvesasa
cathode(target)andthesubstrateon
53
whichthematerialtobedepositedserves
asananode.
Thetargetandthesubstrateface
eachother
inthesputteringchamber.
Afterevacuat
ionofthechamber
aninertgas
argonisintro
ducedandservesa
sthe
mediuminw
hichtheelectrical
dischargeis
initiatedand
maintained.
Theuseofplasmai.e.,ionisedgasduringvapourdepositionisfound
toyield
highpurityfinalmaterialrelative
tothePVDandCV
Dtechniques.
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Whendcv
oltageoffewkilovoltsisapplieda
ndadjustedbetw
eenthe
electrodes
avisibleglowdischargeisinitiatedandmaintained.
Nowthefreeelectronswill
beacceleratedb
ytheelectricfieldand
gainsuffic
ientenergytoioniseargonatoms.
ResultingpositiveionsAr+
inthedischargestrikethecathodeand
physicallyejectorsputter
targetatomsthr
oughmomentum
transfer
tothem.
Bottom-Upapproach
54
eseaom
spass
roug
e
scargean
eposon
esusrae
withgrow
ingfilm.
Inadditiontothegrowthsp
eciesotherpartic
leslikeneutrala
toms,
electrons
andnegativeionsunderelectricfieldwillalsobom
bardand
interactwiththesurfaceo
fthesubstrateorgrownfilm.
Forthede
positionofinsula
tingfilmsanalte
rnateelectricfieldof
frequency13.56MHzisappliedtoproduceplasmabetween
the
electrodes
.
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Multipletargetscanberotatedsoastoproduceamultilayeredcoating
onthesubstrate.
Thesputte
redfilmconsistsofsmallergrainswithbetteradh
esionto
thesubstrate.
Byintrod
ucingamagneticfieldnearthetargetinthesputtering
process,thedepositionratecanbeincrease
dto1mm/minuteand
alsoitpre
ventsthesubstrateheatingduetosecondaryelectron
Bottom-Upapproach
55
.
Suchsputteringprocesswithprocesswithm
agneticfieldiscalled
magnetronsputtering.
Reactivegaseshavealsobeenintroducedintothechamberto
form
compound
filmswhichareknownasreactivesputtering.
Therearedifferenttypesplasma-assisteddepositiontechniques.
a).DCsputtering,
b).R
Fsputtering
c).Reactive
sputtering.
d).DCmagnetronsputtering
e).RFmagnetronsputtering.
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Sol-g
elMethod
Itisaversatileindustrialap
proachforfabric
atingnanomaterials.
Itisasolutio
nphasesyntheticroutetoproduc
ehighlypureorganic
orinorganic
materialsthathavehomogeneousparticleandporesizesas
wellasdensi
ties.
Thismethod
affordseasycontroloverthestoichiometryandhomogeneity
thatconventionalmethodslac
k.
Thistechni
ueallowsustochanethecomo
sitionandstructureof
Bottom-Upapproach
56
materialsonthenanometer
scale.
Itsbenefitsincludetheconvenienceoflow-tem
peraturepreparationusing
generalandinexpensivelabo
ratoryequipment.
Oneoftheimportantfeatures
ofthetechniqueisitsabilitytoproduce
materialsin
differentforms,suchaspowders,films,fibresofnanosize
andfreestandingpiecesofm
aterialscalledm
onoliths.
Scientistsha
veusedthistechniquetoproducetheworldslightest
materialsandsomeoftheto
ughestceramics
.
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Thismethodisbasedonthephasetransform
ationofasolution
obtainedfr
ommetallicalko
xidesororgano-
metallicprecursors.
Solutionco
ntainingparticles
insuspensionispolymerizedatlow
temperatu
retoformawet
gel.
Wetgelisthendensifiedthroughthermalan
nealingtogetthe
productslikeaglass,polycrystalsoradrygel.
Typicallythisinvolvesahyd
rolysisreactionfollowedbycond
ensation
Bottom-Upapproach
57
.
Tetraethylorthosilicate(TEOS)(Si(OC2H5)4)
+etha
nol(C2H5OH)
SiO2+otherproducts
Polymergel
soformedisa3Dskeltonsurroundinginterconnectedpores
andthiscan
bedriedandshrunktoformarigidsolidform.
Transforma
tiontogelisachievedbychangingthepHorthe
concentrationofthesolution
.
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Supercriticaldryingprocessremovestheliquidphasefrom
thegel
andproducesalow-densit
y3Dporusmate
rialcalledAERO
GEL.
Aerogelsdensitiesaretypicallybetween1-
20%thatofthebulk
material.
Whenthe
gelisdriedslow
lyinafluidevap
orationprocess,
the
gelsoriginalnetworkcollapses,whichcreatesahighdensity
material
knownas
aXEROGEL.
-
Bottom-Upapproach
58
.
Themethodstartswithaso
lutionconsisting
ofmetalcompou
ndssuch
asmetal
alkoxidesandacetylacetonatesas
sourceofoxides,wateras
hydrolys
isagent,alcoholassolventandacidorbasecatalyst.
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Sol-g
elmethod
Bottom-Upapproach
59
Tetraethylortho
silicate(TEOS)(Si(OC2H5)4)
+ethanol(C2H5OH)
SiO2+otherproducts
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Bottom-Upapproach
Itistheprocessinw
hichchemical
reactionsoccur
inaelectrolytes
olutionbythe
applicationofvo
ltage.
This
process
is
known
as
electroplating.
Electro
deposition
processrequiresan
electricallyconducting
substrate.
Electrodeposition
+
-
cd
Te
Electrolyt
------------------------
------------------------
------------------------
------------------------
------------------------
------------------------
------------------------
------------------------
60
strong,uniforma
ndstrong.
Intheelectrop
latingprocessthesubstrateisplacedinaliquidsolution
(electrolyte).W
henanelectricalpotentialisappliedbetweenacon
ducting
areaonthesub
strateandacounterelectrode(usuallyplatinum)inth
eliquid,
achemicalprocesstakesplace
resultinginthe
formationofa
layerof
materialonth
esubstrateandusuallysomegas
generationatthe
opposite
electrode.
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Electrod
epositionisbasicallyclassifiedinto
a)
Anodicelectrodepositio
n
and
b)
Cathodicelectrodeposition.
InanAnodicProcess,ametalanode
iselectrochemically
oxidizedinthepresenceofoth
erionsinsolutio
n,whichthenreact
togetherand
depositonthean
ode.
Bottom-Upapproach
61
Ina
Cathodicprocesscomponents
aredepositedontothe
cathodefrom
solutionprecursors.
Ex:
Cd2++2e
Cd
HTeO2++4e+3H+
Te+2H2O
Cd2++Te2
CdTe
Ex:
C
C
+2e
Cd2++Te2
Cd
Te
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PropertiesofNanoParticles
Physicalproperties
i.
Sincethesizeoftheparticleisveryless-interparticlespa
cingis
verylessinnanomaterials.
ii.
Becauseo
fitsverylesssize
,thesenanomate
rialscannotbefu
rther
dividedintosmallparticles
anditdoesnotha
veanydislocationinit.
Thuswec
ansaythattheyh
avehighstreng
thandsuperhardness. 62
iii.
Themeltingpointofnanomaterialswillb
everyless.
i.
Thehardnessofnanophasematerialsisduetothephase
transform
ation,stressrelief,densityandgra
inboundaries.
ii.
Theyex
hibitsuperplasticbehaviour.
Mechanicalproperties
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Magnetic
properties
i.
Innano-materialsalarge
numberofatomswillbepresen
tatthe
surface.Theseatomswillhaveless-co-ord
inationnumberandhence
posseslo
calmagneticmomentwithinthem
selves.
ii.
Duetolargemagneticmomentthesenano-materialsexhibits
spontaneousmagnetisa
tionatsmallersizes.
iii.Ferro-magneticandantiferromagneticmultilayernano-mate
rialshas
63
antagnetoesstanceeect.
iv.Thenanomaterialsshows
variationintheirmagneticpro
perty,
whentheychangefrombu
lkstatetocluster(nanoparticle)s
tate.
M
aterials
Bulkstate
Nanophase
state
1
Iron,Ni,Cobalt
F
erromagnetic
Superparam
agnetic
2
Na,K
F
erromagnetic
Ferromagnetic
3
C
r
An
tiferromagnetic
FrustratedPara
magnetic.
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Electricalpropertie
s
i.
Theen
ergybandsinthesematerialswillbeverynarrow.
ii.
Theionizationpotentia
lisfoundtobehigher.
iii.Whenthenanomaterials
arepreparedfrom
bulkmaterials,they
havemorelocaliedmolecularbands.
64
iv.
Nano-materialsarecapa
bleofstoringhydrogenatoms.
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Application
sofNano-Particles
a)Sincethey
arestronger,lighteretc.,theyareusedtomakehard
metals.
b
Smartma
neticfluidsareusedinvaccumsealsmaneticsear
ators
(i)MechanicalEngineering
65
etc.,
c)UsedinG
iantMagnetoRe
sistance(GMR)
spinvalves.
d)Nano-ME
MS(Micro-Ele
ctroMechanicalSystems)areused
in
ICs,Opticalswitches,Pressuresensors,Masssensorsetc.
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(ii)
Electrical,ElectronicsandCommunic
ation
Engineeri
ng
a)Orderlyassemblednanomater
ialsareusedasqu
antumelectronic
devices
andphotoniccrystals.
b)Theyareuse
dassensingelem
ents.
c)Especiallyth
emolecularnanomaterialsareusedtodesigntherobots,
assemblersetc.
66
magneticrefrigerationandinionicbatteries.
d)Dispersednanomaterialsare
usedinmagneticrecordingdevices,rocket
propellant,s
olarcells,fuelcells,etc.
e)Usedtodesignnano-robots,w
hichareusedtoremovethedamag
edcancer
cellsandalsotomodifytheneutronnetworkin
humanbody.
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(iii)
ComputerS
cienceEngineeringandIT
a)Nanomaterialsareusedto
makeCDsandS
emiconductorLa
ser.
b)Theyar
eusedastostoreinformationinsm
allerchips.
c)Theyar
eusedinmobiles,Laptops,etc.,
c
Thear
eusedinO
ticalcom
uters.
67
d)
Nan-d
imensionalphoto
niccrystalsandQ
uantumelectron
ic
devices
playsavitalroleincomputerindustry.
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arbon
anotubes
arbon
anotubes
arbon
anotubes
arbon
anotubes
69
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Certainm
aterialsshouldhavedesirab
lepropertiessothat
nano-sca
lecomponents&structurescanbebuilt.
Carbon-onesuchmaterialsuitablefornanotech-b
ased
C
arbon
C
arbon
C
arbon
C
arbon
(Attractive)
70
compone
nsueosneren
esra
epropere
s.
Carbonisauniqueatomamongotherelementsbecause
ofitsabilitytoexistin
awidevarietyofstructures
and
forms.
(InbuiltorNatural)
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Carbon
isthechemicalelementw
ithsymbolC
and
atomicnumber6.
Asame
mberofgrou
p14onthe
periodictable,
itis
Carbon
Carbon
Carbon
Carbon
71
Physicalpropofcarbonvarywidelyw
iththeallotropic
form.
nonmeta
llic
and
tetr
avalentmaking
four
elec
trons
available
toformcovale
ntchemicalbo
nds.
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D
iamond
G
raphite
Highlytransparent.
Opa
queandblack
.
Hardestmaterials.
Softmaterials.
co
nductivity.
Verygoodconductor.
Crystallizesinthecub
ic
system.
Crystallizesinthehexa
gonal
system.
Used-u
ltimateabrasi
ve.
Used-verygoodlubricant.
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Pu
reCarbon
Pu
reCarbon
Pu
reCarbon
Pu
reCarbon
Diam
ond
Fullerene
4structures
73
Fulleren
eandNanotu
bes-fabricationofnanostructures.
Graphite
Nanotubes
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4
74
1
3
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Allotropes
ofcarbon:
a)Diamond
b)Graphite
c)Lon
sdaleite
75
df)fu
llerenes
(C60,C
540,C70)
g)amorphous
carbon
h)carbon
nanotube.
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Carbo
nNanoTube
s(CNT)
CNTisformedwhenash
eetofgraphite(ahexagonal
latticeofcarbon)rolledintoacylinde
r.
CNTsarelong,thincylindersofcarb
on,werediscovered
in1991by
S.Iijima.
76
Graphite-unrolledsheets-weakbondsatedges.
CNT-Hem
isphericalfullerenecapsat
end-noweak
bonds
atedges.
CNThollowcylinders-thindia-10,000timessma
ller
thanhuma
nhair.
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77
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78
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Varietyof
structurehavingdifferentproperties.
Different
structure-dep
endsonhowtheyrolled.
StructureofCNT
StructureofCNT
StructureofCNT
StructureofCNT
PointsO
&
A
-on
graphite
sheetwithx-axisparallel-side
o
oneycom
rucure.
Chiralvector(Ch)linejoiningO&A.
Ch=na1+ma2.
a1&a2=unitvectorsforH.comblattic
e.
n&m=positionofcarbonatom.
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Drawno
rmalstoCha
tO&A-OB
andAB.
Superimpo
se-OBandAB
toformCNT.
80
basedonC
h.
1
2
h
C
na
ma
=
+
1
3
tan
(2
)
n
m
n
=
+
1
2
2
2
3
(
2
)
c
c
h
a
m
mn
n
C
D
+
+
=
=
Chiralvector
Chiralangle
DiaofCN
T
a1and
a2-realspacelatticetranslationvectors
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CNT
Structure
Ch
Zig-Zag.
0
m=n=0
.
.
.
C
hiral.
0-30
m,n0.n
m.
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82
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83
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84
Sheetofcarbonatoms
isrolledintoatube,i
tcreatesaCNT.
Dependingonthedirectionthesheetisrolledinto,different
patterns
emerge.
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TypesofCNT
85
SingleWallCNT
Mu
ltiWallCNT
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SingleWall
MultipleWall
Mad
e-Onegraphite
sheet.
Groupg
raphitesheets.
Hardestmaterials.
soft
materials.
conductivity.
verygoo
dconductor.
crysta
llizesinthecu
bic
system.
crysta
llizesinthe
hexagonalsystem.
U
sed-ultimate
abrasive.
Used-verygood
lubricant.
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Fabrication
Fabrication
Fabrication
Fabrication
(i)
Pulsedl
aserdepos
ition.
ii
Electric
dischare
method.
(iii)Chemicalvapourdeposition.
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SWCNT
-diameterof5.20nm-produced.
Laserbe
am-vapouriseagraphitetarget-insideoven.
Oven-H
eorArgasmaintainpress
ureat500Torr.
Tempera
tureofoven-maintained-1
200C.
Pulsedlas
erdepositio
n
rape
arge-smaamouns-coa
annce-acas
catalyticnucleation
sites-forma
tionofCNTs.
Intenselaserbeam-target-evaporatecarbon-gra
phite.
Argon-
sweepscarbon-hightemperaturezone
-colder
coppercollector-cond
enseintoCNT
.
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Presenceofcatalyst-preventstheg
rowthoffullerene.
Reaction
temperature-control-tubediameter.
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CNTfrom
hightemperatureplasma-
3700C.
Mostcommon&easiest
waytoproduc
eCNT.
AlsocalledDCArcDisc
harge(DCAD
)method.
Pairofcarbonelectrodesasanodeand
thecathode-potential
difference
ofabout20VDC.
Electric-Arcdischarge
method
Electrodes
-keptinenclosure-filled
withinertgasat50to
500mbar.
Directcurrentof50to1
00A-creates
hightempdischarge-
b/wthetw
oelectrodes-
separatedby1
mm.
Discharge
vapourizeoneofCarbonro
d-produceM
WCNT.
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CNT-uniformdia(2to30nm)and1mmlength.
CNTdep
ositionrate-approximately1mmpermin
ute.
Purecar
bonelectrodes-produce-M
WNT.
AnodedopedwithFe,Co,NiorMo-SWNT.
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Two-step
process
(i)
Catalystprepa
rationstep.
(ii)Synthesisofthenanotubes.
Fe,Ni,Co
oranalloyofthethreecatalyticmetalsisinitially
depositedonasubstra
te.
ChemicalVapourDe
position
usraew
epose
m
sece
usngau
e
solutionw
ithdistilledwater.
Quartzboatcontaining
-etchedsubstrate-plac
edina
CVDreactionfurnace.
Nanosize
catalyticme
talparticles
-formed
-after
additional
etchingofca
talyticmetalfilmusingNH3gasata
temperatureof750to1100C.
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Afternanosizefinemeta
lparticlesare
formed-CN
Twill
begrown
onthemeta
lparticleson
thesubstrate
dueto
inducecatalystparticlen
ucleation.
Diameter
ofCNTdepen
ds-thickness
ofthecatalyticfilm.
Carbonna
notubesformedaremulti-walled.
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Properties
1.SWNTs
aremetallicorsemiconductingdepending
on
chiralityanddiameter.
2.Extreme
lowresistanc
e.
3.SWCNT
withanaturaljunction-ar
ectifyingdiod
e.
-
94
.
.
5.Youngs
modulusis1.8
Tpa-5times
greaterthansteel.
6.Therma
lconductivity
-6kW/km-6
timemoretha
ncopper.
7.Withsta
ndhightemp
-meltingtemp
-3threetime
shigher
thancop
per.
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HighEle
ctricalCondu
ctivity
HighThermalConductivity
VeryHig
hTensileStre
ngth
HighlyF
lexible-canbebentconsiderablywithoutd
amage
Properties
VeryEla
stic~18%elongationtofailu
re
LowThermalExpansionCoefficient
GoodFie
ldEmissionofElectrons
HighAspectRatio(len
gth=~1000x
diameter)
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Com
parisonofmechanical
properties
Material
Young's
Modulus(T
Pa)
Tensilestrength
(GPa)
Elongationat
break(%
)
SWNT
~1(from1to5)
1353E
16
Armchair
SWNT
0.94T
126.2T
23.1
96
ZigzagSW
NT
0.94T
94.5T
15.617.5
ChiralSW
NT
0.92
-
-
MWNT
0.80.9E
11150E
StainlessS
teel
~0.2
~0.653
1550
Kevlar
~0.15
~3.5
~2
KevlarT
0.25
29.6
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(i)Lightw
eight&verystrong-aerosp
ace.
(ii)Constru
ctionofnanoscaleelectronicdevices
(iii)Battery
electrodes,fuelcells,reinforcingfibers.,etc.
(iv)Flatpaneldisplay-computermonitorsandtelevis
ions.
Applica
tionofCNT
97
(v)Shieldingmaterialsforprotectinge.m.radiation.
(vi)Military&communic
ationsystems
-protecting
com
putersandelectronicdevices
.
(vii)SemicondutingCNTs-switchingdevices.
(viii)
Sem
icondutingCN
Ts-chemicalreactions.
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98