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DR. R.K. KHANDALDIRECTOR
TECHNOLOGICAL CHALLENGES FOR MATERIALS OF 21st CENTURY
SHRIRAM INSTITUTE FOR INDUSTRIAL RESEARCH19, UNIVERSITY ROAD, DELHI - 110007
Email : [email protected] Website : www.shriraminstitute.org
OUTLINE Classification of materials Properties of materials
Bulk Materials Internal Structure
NanomaterialsStructure: Size, Shape & Surface area
Designing nanomaterialsApproachesMechanical ParametersIdeal strengthQuantum effectsPhotocatalytic materials
Magnetic materialsOptical materialsAdhesive materials Approaches so farChallenges
Path forward
Defects
Classification of Materials (Type & Structure)
Composites
Ceramics
Polymeric
Crystalline
Polycrystalline
Amorphous
Metallic
Electronic
Biomaterials
NanomaterialsNanomaterials include all classes of materials at the nanoscale
Nanomaterials are categorized as 0-D (nanoparticles),1-D (nanowires, nanotubes, nanorods), 2-D (nanofilms, nanocoatings), 3-D (bulk)
101Properties of Materials : Critical Factors (Bulk Vs Nano)
DefectsDefects
+
Mechanical
Optical
Thermal
Magnetic
At the nanoscale, interactions with heat ,light, stress, electrical field & magnetic field give rise to interesting & novel properties
A thorough understanding of the nature of interactions at the bulk & nano levels are essential for designing nanomaterials
Internal Internal StructureStructure
Bulk (Macro & micro) Nano
SizeSize
ShapeShape
Surface Surface areaarea
+
+
Structure of Bulk Materials : Internal Structure
Atomic Structure
Ionic Bonding e.g. NaCl
Covalent Bonding e.g. CH4, C2H6
Metallic Bonding
Strong High melting, brittleness & poor
electrical conductivity
Aggregate of positively charged cores surrounded by a sea of electrons
Path of electron is completely random Good conductors, highly ductile
Weak Poor ductility & electrical conductivity Brittle & insulators
Shared electrons
FCC
Rock salt
Cesium Chloride
Zinc blende
BCC
HCP
E.g. Cu, Ag, Au, Ni, Al,Fe
E.g. Fe, W, Cr
E.g. Zn, Co, Ti, Fe
E.g. MgO, MnS, LiF, FeO
E.g. ZnTe, SiC
Sim
ple
C
om
ple
x
Some elements exists in more than one crystalline state eg: Iron
Fe BCC750 0C
FCC
RT
125 kbar
HCP
E.g. CsBr, CsI
Crystal Structure
Structure of Bulk Materials : Internal Structure
Molecular structure
Repetition of monomer Homo-polymers & Co-polymers Linear, Branched, Cross-linked & Network structures Spaghetti like structure Presence of many Vander-Waals bonds Examples : PE, PS, Nylon, etc.
Random Co-polymer
Alternating Co-polymer
Block Co-polymer
Graft Co-polymer
Linear polymer
Branched polymer
Crosslinked polymer
Polymers
Structure of Bulk Materials : Internal Structure
Bulk Materials : Defects
Reasons : Atomic packing problems during processing Formation of interfaces with poor atomic registry Generation of defects during deformation.
106
104
102
100
10-2
10-4
10-6
10-8
Bulk defects
Interfacial defects
Line defects
Atomic point defects
Electronic point defects
Micrometers
Point
Micro defects
Macro defects
Planar
Linear
Volume
Types Classification
VacancySelf interstitialSchottky defectsFrenkel defects
Ductility of metals
Brittleness of ceramics
Formation of cavities/bubbles during casting
Effects :(a)Constructive : C in Fe High strength
0.01% of As in Si in Conductivity of Si by 10,000 times (b)Destructive: Dislocations Deformation in plastics
0 - D
1 - D Rods
TubesWires
2 - D
Basic Geometry Large Scale Forms
Nanocomposite thick film
Nanocomposite thick film
Thin film on substrate Bulk
Nanocomposites
Scope: Ability to design materials with tunable optical, electrical, magnetic, thermal & mechanical properties
(Dimension at micro or macro scale)
d 100 nm
d 100 nm
Structure of Nanomaterials: Size and Shape
Structure Nanomaterials : Shape and Surface area
Different shapes
Sphere
Cylinder Cube
Critical Dimension (nm)Su
rfa
ce t
o V
ol.
rati
o (
nm
-1)
0
0.5
1.0
1.52.0
3.0
3.5
20 40 60 80 100
2.5
Sphere : S : V = 3 : r
e.g.: Shape
Volume remains constant
(10 m) (10nm)
523 nm3
V (10 m)
V (10nm)
5.23 x 1011
523= = 1x109 particles
One single particle of 10 microns can generate 1 billion nanosized particles of 10nm; increase in surface area by a factor of 1000
Surface area
SizeVolume 5.23 x 1011nm3
Number of particles
3.14x108 nm2 314 nm2
Scope : Imparts extraordinary properties to various day-to-day products like self cleaning windows, anti-wrinkle textiles, etc.
AV
=
4r2
4r3/3
2rh r2h
6l 2
l 3
AV
=
AV
= Cylinder : S : V = 2 : r
Cube : S : V = 6 : l
Sphere
Distinct surface to volume ratios
Designing Nanomaterials
Designing Nanomaterials : Approaches
Metal
Ceramic
Polymer
Matrix Reinforcing phase
Inorganic
Metals & inorganic
Metals
Examples
Carbides, borides, nitrides, oxides, etc.
SiC, Zr, Fe, W, Mb, Ni, Cu, Co, etc.
C nanotubes, alumina, silica, etc.
Nanocomposites have tremendous scope in all areas of science & technology.
Designing Nanomaterials : Mechanical Parameters
PPPE
PETPSPS
PMMAPC
PTFEFoams
Natural materials
Polymers
Non-technical ceramics (Concrete)
MetalsCompositesGFRPCFRP
Technical ceramics
Yo
un
g’s
Mo
du
lus
(GP
a)
Density (Mg/m3)
Flexible polymer foams
Rigid polymer foams
Wood grain
PSiPUPEVAButyl rubber
Elastomers
Ti alloys Ni alloys
Chart for Modulus & Density : Engineering Bulk Materials
10-4
1
10
100
10-3
1000
0. 1 1.0 10
Bulk MaterialsAl2O3,
Si3N4
SiC
W alloys
WCNi alloys
Cu alloysZn alloysPb alloys
Strongest engineering materials reach levels of about 2000 MPa
Foams
Natural materials
Polymer nano- composites
Polymers
Metals
Metallic nanocomposites
Nanocrys-talline metals
Ceramics
Standard composites
Nanotubes & fibers
Yo
un
g’s
Mo
du
lus
(GP
a)
Density (Mg/m3)
Elastomers
Ceramic nanocomposites
0. 1 1.0 10
10-4
1
10
100
10-3
1000
Chart for Modulus & Density : Engineering Nanomaterials
Nanomaterials
PPPE
PETPSPS
PMMAPC
PTFEFoams
Natural materials
Polymers & Elastomers
MetalsCompositesGFRPCFRPMg Alloys
Ceramics
Yie
ld S
tren
gth
(M
Pa)
Density (Mg/m3)
Flexible polymer foams
Rigid polymer foams
Wood
Al alloys
Cork
Si elastomer
Al2O3, SiC, Al alloys,
Ceramics
0. 1
1.0
10
100
1000
10,000
0. 1 1.0 10
Chart for Yield Strength & Density : Engineering Bulk Materials
Al2O3 alloysSiC alloys WC alloysZn alloys
W alloysPb alloysZn alloys
Bulk Materials
Foams
Natural materials
Polymer CNT composites
Polymers & Elastomers
Metals
Metallic nanocom-posites
Nanocrys-talline metals
Ceramics
Standard composites
Ceramic nanocom-posites
Nanowires (Cu, Ag, Au)
Yie
ld S
tren
gth
(M
Pa)
Density (Mg/m3)0. 1 1.0 10 100
0.1
10
100
104
1
105
103
Nanomaterials
Chart for Yield Strength & Density : Engineering Nanomaterials
PPPE
PETPSPS
PMMAPC
PTFEFoams
Natural materials
Polymers & Elastomers
Metals
CompositesCFRP, Mg Alloys, Concrete
Ceramics
Ten
sile
Str
eng
th (
MP
a)
Density (Mg/m3)
Flexible polymer foams
Rigid foams
Wood
W, Pb, Mg, Ti, Ni, Cu, Zn, Pb alloysSteel,
Cork Si elastomer
0. 1
1.0
10
100
1000
10,000
WC alloys, Al2O3 alloys, SiC alloys, Al alloys
0. 1 1.0 10 100
Chart for Tensile Strength & Density : Engineering Bulk Materials
Bulk Materials
Foams
Natural materials
Polymer CNT composites
Polymers & Elastomers
Metals
Metallic nanocom-posites
Nanocrys-talline metals
Ceramics
Standard composites
Nanowires (Cu, Ag, Au)
Ten
sile
Str
eng
th
(MP
a)
Density (Mg/m3)0. 1 1.0 10 100
0.1
10
100
104
1
105
Polymer-Ceramic nanocomposites
3-D ceramic nanoco-mposite
1-D metallic nanostructures
1-D C-nanostructures
103
Chart for Tensile Strength & Density : Engineering Nanomaterials
Nanomaterials
Nano materials
101
Ti alloysBrassMild steelAl alloysCopper
Lead
PE, PAPP, ABSPS, PETPVC
AluminaZirconia
Glass
ConcreteBricks
Metals Polymers Ceramics
Ideal Strength
Ideal Strength
To make materials stronger than this is a huge Challenge!
Yie
ld S
tren
gth
( y
) / Y
ou
ng
’s M
od
ulu
s (E
)
10-4
10-3
10-2
10-1
Bulk materials fall short of the ideal values in every aspect; mechanical, optical, electronic, magnetic, thermal, etc.
Nanostructure, nanolayers & amorphous materials are strongest
Designing Nanomaterials : Quantum Effects
Designing Nanomaterials : Quantum Effects
Conduction bandVacant state
Conduction bandVacant state
Conduction bandVacant state
Valence bandOccupied state Valence band
Occupied stateValence bandOccupied state
En
erg
y
Conductor(Metals)
Insulator(Ceramics)
Semi-conductor(Silicon)
No band gap Large band gap Small band gap
Bulk level: Atomic energy levels spread out into energy bands; transfer of electrons from one level to the other is not restricted.
Nano level: Free movement of electrons is restricted due to confinement of electrons.
At the nano level: Quantum effects due to confinement of e- become significant
En
erg
y
En
erg
y
Designing Nanomaterials : Quantum Effects
En = Electrons are fully confined
According to quantum mechanics, electron exists inside a deep potential well from which it cannot escape and is confined by the dimensions of the nanostructures
Smaller dimension leads to wider separation of energy levels By spatial confinement of electrons, band gap of a material can be
shifted towards higher frequency
2 h2
2mL2 nx
2 + ny2 + nz
2
0 - D
En = 2 h2
2mL2 nx
2 + ny2 1 - D
En = 2 h2
2mL2 nx
2 2 - D
Electrons confinement in two dimensions
Electrons delocalization in one dimensions
Electrons confinement in one dimensions
Electrons delocalization in two dimensions
h h/2 ; h = Planck’s constant; m = Mass of e- ; L = Width (Confinement)
Implications
Quantum well
Quantum wire
Quantum dot
Designing Nanomaterials : Photocatalytic Materials
Materials with novel approach: Catalytic activity for industrial effluent treatment.
6.3 eV 3.15 eV 1.58 eV
U.V
200 nm 400 nm 800 nm
Visible
TiO2
ZnOCdS
WO3
Band gap Energy
EMS()
TiO2 = 3.20 eV
ZnO = 3.35 eV
WO3 = 2.80 eV
CdS = 2.42 eV
Semiconductors are the most ideal and preferred materials. Challenge : Maneuvering band gap: Make it sensitive to visible light.
Designing Nanomaterials : Photocatalytic Materials
Designing Nanomaterials : Magnetic Materials
Isolated nanoparticles
Nano particles
Ultrafine Nanoparticles core shell morphology in the matrix
Small magnetic nanoparticles embedded in a chemically dissimilar matrixSmall particles
dispersed in nanocrystalline matrix
Magnetic nanoparticles with polymer coating
Metal-matrix nanocomposites are useful for magnetic applications such as magnetic recordings
Consists of hard magnetic nanoparticles (Nd2Fe14BFm2Fe17N3) dispersed in a soft nanocrystalline phase (Ferrite, Fe3Pt)
< 1 nm: Non-magnetic~ 1-10 nm:Super-paramagnetic
>10 nm: Ferromagnetic
E.g. Mn,Co,Fe & Ni
3M2O3.5Fe2O3
Ni0.5Zn0.4Cu0.1Fe2O3
Designing Nanomaterials : Magnetic Materials
In the absence of a magnetic field, magnetic interaction results in spin alignment
When a magnetic field is applied in the opposite direction, only the soft phase is able to reverse the magnetization.
When the magnetic field is reversed, magnetism is again reversed in the soft phase
When the applied magnetic field is high enough to reverse the spins in the hard phase; soft phase does not reverse the magnetization
High remenance & high magnetic energy (200 kJ/m3)Ability to maximize the soft phase content to enhance
saturation magnetization
Approach: Mechanical alloying of two phases
Designing Nanomaterials : Magnetic Materials
This effect is dependent on the size of particles, volume fraction & distribution of each phase
Hard & Soft phases interact magnetically & for best effects, the two phases must be at the nanoscale
Designing Nanomaterials : Optical Materials
=µrr
Most promising area of application : Metamaterials Size, shape & composition of embedded nanoparticles influence the
interactions with light, heat ,sound, waves, etc.
1
2
1
2
+ve R.I.
-ve R.I.
Refractive Index
=µrr
µr: Permeability to magnetic fieldr: Permeability to electric field
• µr, r= -ve
• Induced phenomena
µr, r= +veNatural phenomena
Designing Nanomaterials : Optical Materials
Nano pillars Inhomogeneity
Challenge:Selection of materialCreation of different surface
Reflection Transmission Refraction
Non-uniform surface
Camouflaging
Designing Nanomaterials : Optical Materials
The play of light on a butterfly’s wings has inspired designing of novel photonic materials for solar cells, photovoltaics, camouflaging, optical fibers and military applications.
Invisibility cloak
Color play
Tailor-making of refractive index and dielectric constant
Camouflaging
Designing Nanomaterials : Optical Materials
Designing Nanomaterials : Adhesive Materials
The ability of a Gecko to scamper up walls has been a very big inspiration for designing a number of adhesives; Useful for the lithography industry where nanosurfaces have been patterned after a gecko’s foot soles.
Clinging ability of Gecko
Intermolecular forces between the paw & the surface Nano-pillars
~ to Gecko paw hair
Designing Nanomaterials : Adhesive Materials
Inert gas condensation Evaporation
colloidal methods
Physical or chemical vapour deposition (PVD
OR CVD)
Extrusion, cryomilling &
sintering
Directional growth from catalyst dots
Templating
Lithographic method
Incorporation of Nanotubes and rods into polymer or metal
matrices
Beating (gold foil) Electrodeposition
PVD,CVD Self-assembled
films
Electrodeposition Physical vapor
deposition Chemical vapor deposition
(1) PVD
(2) CVD
(3) Electrodeposition
1-D
2 D
ime
ns
ion
in
na
no
sc
ale
2-D
1
D
imen
sio
n
in
n
an
os
cal
e
0-D
All
3
Dim
ens
ion
in
na
no
sc
ale
Dim
ensi
on
alit
y
Class 1
Discrete objectsClass 2
Surface featuredClass 3
Bulk structures
Designing Nanomaterials : Approaches So Far
Stability ; AgglomerationStability ; Agglomeration Yield ; Scale-upYield ; Scale-up
SynthesisSynthesis
AssemblyAssembly
ApplicationApplication
Designing Nanomaterials: Challenges
Isolated ; Discrete Isolated ; Discrete Hybrid ; DispersionHybrid ; Dispersion
Mechanical Mechanical Optical Optical Electrical Electrical
MagneticMagnetic ThermalThermal
Utilization of single nanostructure for processing electrical, optical or thermal signals.
Assembling nanostructures for electronic, chemical & other applications.
Path Forward
Development of nanotechnology & nanomaterials for: Development of nanotechnology & nanomaterials for: Storing energy rich gasesStoring energy rich gases
Fuel cellsFuel cells
Solar cellsSolar cells
Photovoltaic textilesPhotovoltaic textiles
Self cleaning, Anti-microbial & other surface properties: Self cleaning, Anti-microbial & other surface properties: Nano paintsNano paints
Nano sealantsNano sealants
Smart materialsSmart materials
Only nanomaterials have made possible the development of Only nanomaterials have made possible the development of futuristic materials with extraordinary propertiesfuturistic materials with extraordinary properties
THANK YOU