Title: Nanotechnology in Mechanical Engineering
1Nanotechnology in Mechanical Engineering
UEET 101 Introduction to Engineering
- Presented By
- Pradip Majumdar
- Professor
- Department of Mechanical Engineering
- Northern Illinois University
- DeKalb, IL 60115
2Outline of the Presentation
- Lecture
- In-class group activities
- Homework
3Lecture II Outline
-
- Nano-Mechanics
- Classical Mechanics Assumptions
- Material mechanical properties
- Nanoscale Thermal Phenomena
- - Basics of Heat Transfer
- - Thermal Conductivity
- - Heat Transfer Coefficients
4Nanomechanics
- Classical theories
- Structure Property relations
- Stress-strain relations
- Mechanical properties
- Issues in nanomechanics
- Mechanics of nanotubes
5Classical Mechanics Assumptions
- Solid is assumed as homogeneous
- Smallest material element has macroscopic
properties - Involves only mechanical forces such as inertia,
gravity and friction - Motion is uniquely determined by forces -give by
Newton s law of motion - Total Energy Internal EnergyKinetic Energy
- Potential Energy
- Single phase no phase transformation
6Basics of Classical Mechanics
- Mechanical Behavior of Materials
- Materials response to applied and residual
forces - Deformation
- When a material is subjected forces, its atoms
may be displaced from their equilibrium position. - Any separation of displacement from the
equilibrium position requires energy, which is
supplied by the force. - - As a material is stretched, atoms tend
to separate and - brings attractive forces into play.
- - As a material is compressed, atoms tend
to come together - and causes repulsion
7- Elastic Deformation Atoms resumes back to the
original position when imposed forces are
released represents the relative resilience of
the materials. - Plastic Deformation When a material exceeds the
elastic capability (elastic limit) to restore
back to equilibrium position as the imposed
forces are released - the deformation is
permanent
Engineering Strain It is the deformation
defined as the ratio of the dimensional change to
the original dimension.
Extensional Strain
8- Shear Strain
- This is the deformation of a material between
two parallel plane through a certain angle when
subjected to tangential or shear forces. - - Shear strain is defined as the
displacement to the distance between the planes
Poissons Ratio Defined as the ratio of strain in
x-direction to the strain in y-direction and
expressed as
9- Stress
- Stress is the internal response or resistance
that a material creates when exposed to some kind
of external force. - This internal resistance is due to the
inter-atomic attractive and repulsive forces. - Displacement in either direction produces an
increase in the force (tensile or Compression)
that oppose the deformation
Defined based on balance of external force with
the internal resistance force as
Where Average stress (Internal
resistance force per unit area) F External
load or force A Cross-sectional area over
which the force acts
10- Hookss Law ( Macroscopic Constitutive Relation
or Stress-strain relation) - Defines the proportional relation between the
- stress and strain for material below the
elastic - limit as
- Where E Modulus of Elasticity (Youngs
Modulus)
- Elastic modulus (E) is a measure of the stiffness
of the engineering material - Greater the values of E results in a smaller
elastic strains smaller the response of the
material structure to imposed load - Important parameter for the design and analysis
in the estimation of allowable displacements and
deflection of a component or structure
11- Modulus of Rigidity (G)
- The modulus of rigidity is the modulus of
- elasticity in shear (Relation between shear
stress - and shear strain) and defined as
- Values of G is usually determined by torsion
- testing and related to E by the relation
-
12Tensile Strength
- Yield Strength (Point-C)
- Stress required to produce a small amount of
plastic deformation - Ultimate Strength (Point D)
- Maximum stress that a material can withstand
under the condition of uniaxial loading - - undergone substantial plastic deformation
- - not often used for designing a component
13Beam Deformation for Different Materials
- Many materials are not strength limited, but
modulus limited - In some applications, we need material of high
modulus of elasticity rather than high strength - These structure may not fail if low modulus of
elasticity is used - It, however, may reach too much of deflection
Higher the modulus of elasticity lower is the
deformation
14Typical Material Properties
- Material Elastic Shear
Tension Posssonsratio - Modulus (E) Modulus
Yield - (GPa) (GPa)
(MPa) - Aluminum
- Alloy 72.4 27.6
504 0.31 - Steel-
- Low Carbon 207.0 75.9 140
0.33 - SS -304 193.2 65.6
960-1450 0.28 - Titanium 110.5 44.8
1035 0.31 - Silcon Carbide 469.2
- Polycarbonate 3.4
- SWNT 0.191(TPa) 0.45 TPa
0.18
15Breakdown of Continuum Concepts- Thresholds of
Micromechanics
Force, stress balance/equilibrium Constitutive
relation Hooks law Classical thermodynamics
Stress Strain Area/volume
Scale
Micromechanics
Force/surface energy balance Constitutive
relation nonlinear Structure property
relation Adhesion friction laws
Structure Interface Adhesion Phases
Scale
16Breakdown of Continuum Concepts- Thresholds of
Micromechanics
Force/energy/structure balance Constitutive
relation ?? Molecular mechanics
effects Structure property relation ?? Energies
are linked
Molecule Atoms Quantum energies
Scale
17Structure Property Relations
- Nano Macro
- Inter-molecular
Strength - interaction
- Bond rotation/
Modulus - angle/strength
- Chemical sequence
Viscosity/conductivity - Nanotube diameter/
density/toughness/ - Nanotube l/d ratio
dielectric/plasticity
18Nano-scale Science Hierarchy
- Average of material properties
- - Surface effects vs volume average
- - Molecular network homgenization
- - Electromechanical interactions
- Nano-scale laws
- - Application of classical mechanics law
- - new and coupling forces
- - properties/energy depend on molecular
structure - - role of quantum effects
19Nanomechanics
- Nanomechanics vs. molecular mechanics
- Structure property relations and dependencies
- Scaling analysis of molecuar structures
- Reliability of characterization techniques at
nano-scale what are to be measured?
20Issues in Nanomechanics
- Nano-Materials Science
- - Nanotubes purity
- - Characterization of NTs
- - NT polymer properties
- Multifunctional composites
- Approaches- Top down
- Continuum models fro NTs
- Strain gradient
- Lattice structure
21Models for Multiscale Effects
- Development of constitutive laws fro nano-scale
- - modeling of nano-structural behaviors
- Average nano-constitutive laws for use higher
scale model - Models for nano-structure/force potentials to
take into account of multi-scale model
Nanotechnology Modeling Methods
- Quantum Mechanics
- Atomistic Simulations
- Molecular mechanics and Dynamics
- - nanomechanics
22Nano-scale Measurement Techniques and Tools
- Atomic Force Microscopy (AFM)
- Magnetic Force Microsopy (MFM)
- - Scanning Electron Microscopy (SEM)
- - Transmission Electron Microscopy (TEM)
- - Scanning Tunnel Microscopy (STM)
- Raman (IR) Spectroscopy
- Electron Nano-Difraction
- Neutron Scattering
- Electron Spin Resonance (ESR)
23Nano-Structured Material Properties
- Physical Material
Mechanical - Thermal Density
Stiffness - Optical Crystallinity
Strength - Electronic Crosslink density
Fracture toughness - Magnetic Orientation
Fatigue - Chemical Textures
Durability - Acoustic Absorption
Viscoelastic
24Mechanics of Carbon Nanotubes
- The structure of single wall nanotubes (SWNTs)
- - molecules or crystals
- - Effective geometry
- - length scales
- - geometric parameters
- Properties of Carbon nanotubes
- - Thermal and electrical conductivities
- - density
- - mechanical properties such as modulus,
strength - - effect of geometry and molecular structure
- - classes of NTs
- Deformation of NTs
- - Tension, compression, torsion
- - nonlinear elastic and plastic deformation
25Nanotubes Mechanical Properties
NASA Langley ResearchCenter
26 Nanotubes Density and Thermal Conductivity
27VI Nano-Scale Heat Transfer
- Classical theories
- Thermal energy transport in a solid by two
primary mechanisms - - Excitation of the free electrons
- - Lattice vibration or phonons
- Scattering phenomena in micro and nanoscale heat
transfer
28Basics of Heat Transfer
Basic Modes and Transport Rate Equation Conductio
n Heat Transfer This mode is primarily important
for heat transfer in solid and stationary fluid
Conduction heat transfer is due to the activity
in atomic and molecular level
- Heat transfer is thermal energy in
- transit as a result of a spatial
- temperature difference.
- Temperature at a point is defined
- by the energy associated with
- random molecular motions such as
- translational, rotational and
- vibrational motions.
29Physical Mechanism
Conduction Rate Equation
- Gas Energy transfer due to random
- molecular motion and collision with
- each other
- Liquid Molecular interactions are
- more stronger and more frequent
- resulting in an enhanced energy
- transfer than in a gas
- Solid Energy transfer due to the
- Lattice vibration and waves induced
- by the atoms.
- - In a electrical nonconductor, the energy
transfer is entirely due to lattice waves. - - In a electrical conductor it also due to the
translational motion of the free electrons.
Fouriers law
Where q Heat flow per unit area per unit time
or heat flux, k is the thermal conductivity of
the material defined as
30Macroscopic Thermal Conductivity Values of
Substance Type Density Thermal
Conductivity Gases Air
0.026 Liquid Water
0.63 Ethylene Glycol
0.25
Solid Aluminum
2702
237 Copper
8930
401 Gold
19300 317
Carbon Steel 7850
60.5 SS
304 7900
14.9 Carbon
Amorphous 1950
1.6 Diamond
3500
2300 Silicon Carbide
3160
490
31- Convection Heat Transfer
- The convection heat transfer occurs between a
moving fluid and an - exposed solid surface.
- The fluid upstream
- temperature and velocity
- are and
- respectively.
Convection Modes Natural Convection Flow
induced by natural forces such as
buoyancy Forced Flow induced by mechanical means
such as fan, blower or pump. Phase Change
Boiling or condensation- Bubble formations and
collapses
32- Convection Rate Equation
- Newtons Law Cooling
Where, is called the convection heat
transfer coefficient or film coefficient.
Convection heat transfer coefficients is defined
as
- Convection heat transfer coefficients are
influenced by the velocity field and
temperature field in the boundary layers. - This depends on fluid types and properties,
solid surface geometry and orientations.
33Typical Convection Heat Transfer Coefficients
- Convection Types Typical Values
( ) - Free Convection
- Gases
2-30 - Liquids
50-1000 - Forced Convection
- Gases 30
300 - Liquids 100
15000 - Phase Change
- Boiling or Condensation 2500 100,000
34Nano-scale Heat Transfer
- Heat conduction in the micro-nanometer scale is
becoming more important because of the increasing
demand of cooling requirements in smaller devices
with increasingly higher heat fluxes such as in
electronic devices, circuits and chips - The main difficulty with the simulation of heat
flow through thin films is that bulk material
properties are not accurate when applied on the
small scale - The understanding of the mechanism of thermal
energy transfer by conduction in thin films
ranging in thicknesses from micro-scale to
nano-scale is becoming very important. - Thin films should be modeled at the atomic level
and this entails treating the heat transfer as
energy transferred by the vibrations in a crystal
lattice. -
35Thermal Interactions
- phonon phonon interaction
- electron electron interaction
- phonon electron interaction
- In most pure metals, the electron electron
interaction is the dominant scattering process
and the conduction of heat by phonon is
negligible - In dielectric crystalline solid, the phonon
phonon interaction is the dominant scattering
process and heat conduction by free electron is
negligible.
36Heat Conduction Dielectric Thin Films
- The vibration of a crystal structure can be
modeled with the concept of phonons, which is
described as the quanta of lattice vibration
energy. - The distribution of phonons represents the
distribution of crystal energy. Heat
transmission takes place as the distribution of
phonons changes. - When a temperature gradient is setup in the
material a steady - state distribution of phonons can be kept.
- Thermal conductivity therefore depends on the
extent by which a distribution deviates from
equilibrium for a given temperature gradient. - The distribution of phonons is modeled by the
Boltzmann transport equation
37Applications nanothin films and nanoparticles in
Heat Transfer
- Used for enhanced conduction heat spreaders in
electronic chips, devices and circuits. Use of
dielectric thin films of diamond or nitrides - Used as filler materials (SWNTs) between two
material surfaces in contact - Reduces resistance to heat transfer
38Nanofluids
- Nanofluids are engineered colloid formed with
stable suspensions of solid nano-particles in
traditional base liquids. - - Thermal conductivity of solids are order
of magnitude higher - than liquids.
- - Use of macro or micro-size particle can
not form stable - suspensions
- Base fluids Water, organic fluids, Glycol, oil,
lubricants and other fluids - Nanoparticle materials
- - Metal Oxides
- - Stable metals Au, cu
- - Nitrides AIN, SIN
- - Carbon carbon nanotubes (SWNTs,
MWNTs), - diamond, graphite, fullerene,
Amorphous Carbon - - Polymers Teflon
- Nanoparticle size 1-100 nm
39Major Characteristics and Challenges
- Stability in dispersion of nanoparticles in base
fluid - - Nanoparticles can stay suspended for a
longer period of time - - sustained suspension is achieved by using
surfactants/stabilizers - Surface area per unit volume is much higher for
nanoparticles - Forming a homogeneous mixture of nanoparticles in
base fluid - Reduce agglomeration of nanoparticles and
formation of bigger articles. - Sedimentation over a period of time.
40Nanofluid Heat Transfer Enhancement
- Thermal conductivity enhancement
- - Reported breakthrough in substantially
increase ( 20-30) in thermal conductivity of
fluid by adding very small amounts (3-4) of
suspended metallic or metallic oxides or
nanotubes. - Convective heat transfer enhancement
- Critical Heat Flux enhancement (CHF)
41Enhanced Nanofluid Conductivity
Shows increase in effective thermal conductivity
of nanofluid with an increase in temperature and
CNT concentration.
42Possible Mechanisms for Enhanced Thermal
Conductivity
- Energy transport due to mixing effect of Brownian
motion of nanoparticles - Formation of liquid molecule layer around
nanoaprticles, enhancing local ordering (Phonon
energy transport) - Balastic transport in nanoparticles Balastic
phonon initated by a nanoparticle transmits
through fluid to other nanoparticles - Possibility of formations of clusters of
nanoparticles - Micro convection and turbulence formed due to
nanoparticle concentration and motion.
43Forced Heat Convection
44Boiling Heat transfer
- Boiling is considered as convection which occurs
at solid-liquid interface. - In the case of boiling fluid phase changes from
liquid to vapor through rapid formation of
bubbles and subsequent collapse in the bulk
fluid. - - This causes heat transfer from solid
heating surface - surface.
- - Fluid temperature remains constant
- Latent heat contributes to the heat
transfer - Surface roughness influences critical heat flux.
- - Critical heat flux can be enhanced by
roughening surface. -
45Enhanced Critical Heat Flux
Experiment with nanofluid (suspending alumina
nanoparticles in distilled water) indicate
increase in critical heat flux by 200 in
comparison to pure water. The nucleate boiling
heat transfer coefficients remain almost the
same.
Kim and You
46Critical Heat Flux Enhancement (CHF)
- Pool boiling heat transfer tests with nanfluids
containing alumina, zirconia and silica
nanoparticles show increased critical heat flux
values (Kim et al. 2006 - Nanoparticles settles and forms porous layer of
heat surface - - Surface wettability increases
- - Show increased contact angle on nanofluid
boiled surface - compared to pure water boiled surface.
- Helps formation of bubbles at boiling surfaces
- Boiling heat transfer is increased mainly due to
the formation of nanoparticle coating on heating
surface.
47Nanofluid Applications
- Energy conversion and energy storage system
- Electronics cooling techniques
- Thermal management of fuel cell energy systems
- Nuclear reactor coolants
- Combustion engine coolants
- Super conducting magnets
- Biological systems and biomedicine
48Nanofluids as Engine Coolant
- Selection potential nanofluids as coolant
- Develop correlations for heat transfer
coefficients and - pressure drop
- Development of radiator, heat exchanger and air-
- preheater using nanofluids.
-
49Group Project
- Engine cylinders are typically cooled by forced
convection heat transfer technique by circulating
water-glycol solution through the cooling jackets
around the cylinder walls. - Identify new cooling techniques based on
nanotechnology for improved - cooling system performance.
- Identify major advantages and gains
- Identify major challenges and technical
difficulties
50Home Work
- Problem 1
- A load of 4000 N is suspended from three
identically sized - wire 1-mm diameter. Wires are made of SS-304,
Aluminum - and wire made of SWNTs. Determine the strain
- (deformation) produce in three wires.
- Problem 2
- A square chip of width 5-mm in size is
mounted on a substrate that is insulated in all
sides while the top surface is cooled to
dissipate heat generated in the chip. From
reliability point, the chip surface has to be
maintained at 85 C. Determine the maximum
allowable chip power for he following three
cases - a) Forced convection with water at 20 C
and h 2000 - b) Forced convection with nanofluid made
of water and copper - naoparticles at 20 C and h 2500
51- http//www.youtube.com/watch?vsITy14zCvI8