nanotechnology2
TRANSCRIPT
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INTRODUCTION TO NANOTECHNOLOGY
An Overview of Fluid Mechanics for MEMS
-Reni Raju
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MEMS (Applications)
Accelerometers for airbagsMicro heat exchangersSensorsActuatorsMicropumps
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NEMS (Application)
Nanostructured CatalystsDrug Delivery systemsMolecular Assembler/ReplicatorsSensorsMagnetic Storage ApplicationsReinforced PolymersNanofluids
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Fluid Mechanics of MEMS
Devices having a characteristic length of less than 1 mm but more than 1 micron.
10-16 10-14 10-12 10-10 10-8 10-6 10-4 10-2 100 102
Dia. Of Proton H-Atom Diameter
Human Hair Man
NEMS MEMS
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FLUID MODELLING
Conventional Navier Stokes with no-slip boundary conditions cannot be used.
Pressure Gradient is non-constant along a microduct and flowrate greater than predicted.
Surface to volume ratio is high of the order of 106 m-1 for a characteristic length of 1 micron.
Other factors like thermal creep, rarefaction, viscous dissipation, compressibility etc.
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For Gases
Fluid Modeling
Molecular Modeling Continuum Models
Deterministic Statistical Euler Burnett
Navier StokesMD Liouville
DSMC Boltzmann
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Either as a collection of molecules or as a continuum.
Mean Free path,
Characteristic Length,
Knudsen Number,
22
1
n
y
L
Re2
Ma
LKn
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Local value of Knudsen Number determines the degree of rarefaction and the degree of validity of the continuum model.
Kn=0.0001 0.001 0.01 0.1 1 10 100
Continuum Flow
(Ordinary Density Levels)Slip-Flow Regime
(Slightly Rarefied)
Transition Regime
(Moderately Rarefied)Free-Molecule Flow
(Highly rarefied)
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CONTINUUM MODEL
Local Properties such as Density and Velocity are averages over elements large compared with the microscopic structure of the fluid but small enough to permit the use of differential calculus.
Conservation of Mass:
Conservation of Momentum:
0
kk
uxt
ik
ki
k
ik
i gxx
uu
t
u
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Conversation of Energy:
Closure:
k
iki
k
k
kk x
u
x
q
x
eu
t
e
kij
j
i
k
k
ikiki x
u
x
u
x
up
)(radiationFluxx
Tkq
ii
RTp
dTcde v
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Euler’s Equation: Fluid is invisicid and non-conducting,
0
kk
uxt
ikk
ik
i gx
p
x
uu
t
u
k
k
kkv x
up
x
Tu
t
Tc
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Compressibility
DENSITY CHANGES DUE TO TEMPERATURE Strong wall Heating or cooling may cause density change.
DENSITY CHANGES DUE TO PRESSURE Pressure changes due to viscous effects even for Ma<0.3.
Continuity Equation:
0
k
k
x
u
Dt
D
Dt
DT
Dt
Dp
Dt
D
1
p
T
TTp
pTp
1),(
1),(
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For Adiabatic Walls;
0
0
0
Pr
*
pcu
TTT
*
**Pr
*
**
*
*
*
1 20 Dt
DT
A
B
Dt
DpMa
Dt
D
00
0000 ;
TB
TcA p
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For Isothermal Wall;
0
0ˆTT
TTT
w
*
ˆ*
*
**
*
*
*
1
0
020 Dt
TD
T
TTB
Dt
DpMa
Dt
D w
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Boundary Conditions
At the Fluid- Solid Interface No-slip and no-temperature jump is based on no discontinuities of
velocity/temperature. Continuum applicable for Kn<0.001
Tangential Slip velocity at wall,
For Real gases,
w
wallgasw y
uuuu
wv
vwallgasw y
uuuu
2
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Slip velocity & Temperature Jump,
where
wwv
v
x
T
Ec
Kn
y
uuu
wallgas
*
*2
*
*** Re)1(
4
32
wT
Tgas
y
TKnTT
wall
*
***
Pr1
22
wi
riT
wi
riv
dEdE
dEdE
,
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MOLECULAR BASED MODELS
Goal is to determine the position , velocity and state of all particles at all times.
DETERMINISTIC MODEL:
Particle described in the form of two body potential energy and time evolution of the molecular positions by integrating Newton’s Law of motion.
Shortcomings:
Need to choose a proper and convenient potential for a fluid & solid combination.
Vast computer resources.
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STATISTICAL MODEL: Based on probability of finding a molecule at a particular position and
state. Six-dimensional phase space. Assumption, for dilute gases with binary collision with no degrees of
freedom.
Liouville equation, conservation of N-particle distribution function in 6N-dimensional space,
Boltzmann equation for monatomic gases with binary collision,
0..11
k
N
kk
k
N
kk x
Fxt
3,2,1
*),()()()(
j
ffJx
nfF
x
nf
t
nf
jj
jj
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Non-linear collision integral, describes the net effect of populating and depopulating collisions on the distribution.
1
4
0
1*
1*2 )()(*),(
ddffffnffJ r
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LIQUID FLOWS
The Average distance between the molecules approaches the molecular diameter.
Molecules are always in collision state. Difficult to predict. Non-Newtonian behaviour commences,
Contradictory results in experimental data and modelling. MD seems to be the best option available. Based on MD, the degree of slip increases as the relative wall density
increases or the strength of the wall-fluid coupling decreases.
12
y
u
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Slip length,
cos LL
1
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SURFACE PHENOMENA
Surface to Volume ratio for 1 micron is 106 m-1.
High Radiative and Convective Heat transfer. Increased importance to surface forces and waning importance of body
forces. Significant cohesive intermolecular forces between surface, stiction
independent of device mass. Adsorbed layer. Surface tension and nonlinear volumetric intermolecular forces.
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Fluid Mechanics for NEMS
Nanofluids - thermal conductivity fluids.
Possibility of applying Continuum Model for low Knudsen number.(?)
Model applicability to Dense and rare gas.
Possible treatment of Liquids as dense gas at Nano scale.(?)
Importance of Quantum Mechanics.
Importance of Surface Phenomenon's.
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TASKS AHEAD
Modeling using the Continuum model for the Slip Flow Regime Knudsen Numbers.
Understanding the mechanics of Nano-scaled Domains.
Arriving at a suitable modeling technique comparable with the experimental data (if available.)