university of lyon, france nanoscale interfacial phenomena in complex fluids - may 19 - june 20 2008...
TRANSCRIPT
University of Lyon, France
Nanoscale Interfacial Phenomena in Complex Fluids - May 19 - June 20 2008
E. CHARLAIX
Introduction to nano-fluidics
1. 1. Flows at a nano-scale: where does classical hydrodynamics stop ?
2. 2. Liquid flows on smooth surfaces: the boundary condition
3. 3. Liquid flows on smooth surfaces: experimental aspects
4. 4. Flow on patterned surfaces
5. 5. Effect of boundary hydrodynamics on other surface transport properties
6. 6. Capillarity at a nano-scale
OUTLINE
Why nano-hydrodynamics ?
Surface Force Apparatus: a fluid slit controlled at the Angstrom level
First nano-hydrodynamic experiments performed with SFA
Experiments with ultra-thin liquid films
solid or glass transition ?
a controversy resolved
Nanofluidic devices
Miniaturization increases surface to volume ratio:
importance of surface phenomena
manipulation and analysis of biomolecules . with single molecule resolution specific ion transport
50 nm channelsWang et al, APL 2002
500 nm
Nanochannels are more specifically designed for :
Microchannels…
…nanochannels
Large specific surface (1000m2 /cm3 ~ pore radius 2nm)
catalysis, energy/liquid storage or transfo, …
Mesoporous materials
Water in mesoporous silica (B. Lefevre et al, J. Chem. Phys 2004)
Water in nanotubes Koumoutsakos et al 2003H. Fang & al Nature Nanotech 2007
10nm
Electric fieldelectroosmotic flow
Electrostatic double layer3 nm 300 nm
Electrokinetic phenomena
Electro-osmosis, streaming potential… are determined by nano-hydrodynamics at the scale of the Debye length
Colloid science, biology, nanofluidic devices…
Tribology :
Mechanics, biomechanics, MEMS/NEMS friction
Rheology and mechanics of ultra-thin liquid films
Bowden & Tabor
The friction and lubrication of solids Clarendon press 1958
J. N. Israelachvili
Intermolecular and surface forces Academic press 1985
First measurements at a sub-nanometric scale: Surface Force Apparatus (SFA)
OUTLINE
Importance
Surface Force Apparatus : a slit controlled at the Angstrom level
First nano-hydrodynamic experiments performed with SFA:
Experiments with ultra thin liquid films
solid or glass transition ?
a controversy resolved
Tabor et Winterton, Proc. Royal Soc. London, 1969Israelachvili, Proc. Nat. Acad. Sci. USA 1972
Surface Force Apparatus (SFA)
micaAg
Ag
Optical resonator
D
Franges of equal chromatic order (FECO)
Tolanski, Multiple beam Interferometry of surfaces and films, Clarendon Press 1948
Source of white light
Spectrograph
D=28nm
contact
r : reflexion coefficient n : mica indexa : mica thicknessD : distance between surfaces
Distance between surfaces is obtained within 1 Å
(nm)
Horn & Israelachvili, J. Chem Phys 1981
The
Oscillating force in organic liquid films
Static force in confined organic liquid films(alkanes, OMCTS…).Oscillations reveal liquid structure in layers parallel to the surfaces
OUTLINE
Importance
Surface Force Apparatus : a slit of thickness controlled at the Angstrom level
First nano-hydrodynamic experiments performed with SFA:
thick liquid films (Chan & Horn 1985)
Experiments with very thin liquid films
solid or glass transition ?
a controversy resolved
K ∆(t) = Fstatic (D) + Fhydro (D, D)
Drainage of confined liquids : Chan & Horn 1985
tts
D(t)
D
L(t)
Run-and-stop experiments
Inertia negligible :
Lubrication flow in the confined film
z(x)
xu(x,z)
Hypothesis
PropertiesPressure gradient is // Ox
Average velocity at x:
Velocity profile is parabolic
Quasi-parallel surfaces: dz/dx <<1 Newtonian fluid
Low Re
Slow time variation: T >> z2/
z2
12dPdx
U(x)= -
fluid dynamic viscosity
No-slip at solid wall
Mass conservation 2xz U(x) = - x2 D
Reynolds force (D<<R):
( Re ≤ 10-6 )
Drainage of confined liquids : run-and-stop experiments
K (D - D) = Fstatic (D) + D6R2
D
tts
D(t)
D
L(t)∆(t)
D > 6nm
D(t) - DD(t) KD
6R2
ln = (t - ts ) + Cte
Chan & Horn 1985 (1)
D(t) - DD(t) KD
6R2
ln = (t - ts ) + Cte
D > 50 nm : excellent agreementwith macroscpic hydrodynamics
Various values of D: determination of fluid viscosity excellent agreement with bulk value
Chan et Horn, J. Chem. Phys. 83 (10) 5311 (1985)
Chan & Horn (2)
D ≤ 50nm : drainage too slow
Reynolds drainage
Sticking layers
Hypothesis: fluid layers of thickness Ds
stick onto surfaces
D - 2Ds
D6R2
Fhydro = -
Excellent agreement for 5 ≤D≤ 50nm
OMCTS tetradecane hexadecane
Molecular size
Ds
7,5Å
13Å
4Å
7Å
4Å
7Å
Chan & Horn (3)
D ≤ 5 nm: drainage occurs by steps
Steps height = molecular size
BUT
Occurrence of steps is NOT predictedby « sticky » Reynolds + static forces
Including static force in dynamic equation yields drainage steps
Draining confined liquids with SFA: conclusion
Efficient method to study flows at a nanoscale
Excellent agreement with macroscopic hydrodynamics down to ~ 5 nm (6-7 molecular size thick film)
« Immobile » layer at solid surface, about 1 molecular size
Israelachvili JCSI1985 : water on mica
George et al JCP 1994 : alcanes on metal
Becker & Mugele PRL 2003 : D<5nm
In very thin films of a few molecular layers macroscopic picture does not seem to hold anymore
OUTLINE
Importance
Surface Force Apparatus : a slit of thickness controlled at the Angstrom level
First nano-hydrodynamic experiments performed with SFA :
Experiments with ultra thin liquid films
solid or glass transition ?
a controversy resolved
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Shearing ultra-thin films (1)McGuiggan &Israelachvili, J. Chem Phys 1990
Flattened mica surfaces
Strain gauges
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Velocity
Solid or liquid behaviour depending on V, V/D, historyvery high viscosities, long relaxation times
F
rict
ion
al f
orc
e
‘Continuous’ solid-liquid transition
Granick, Science 1991
Shear force thickness
area velocity
Dodecane D=2,7nm
OMCTS D=2,7 nm
Shear-thinning behaviour
Shearing ultra-thin films (2)
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bulk = 0.01 poise
Giant increase of viscosity under confinement
Confinement-induced liquid-glass transition
Shearing ultra-thin films (3) Klein et Kumacheva, J. Chem. Phys. 1998
tangential motion
times
Shear force response
confined organic liquid
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High precision devicewith both normal and shear force
Confinement-induced solid-liquid transition at n=6 layers
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Flow in ultra-thin liquid films: questions
In very thin films of a few molecular layers macroscopic hydrodynamics does not seem to hold anymore
What is the liquid dynamics:
How can one describe flows ?
Liquid-solid transition ?
Liquid-glass transition ?
OUTLINE
Importance
Surface Force Apparatus : a slit of thickness controlled at the Angstrom level
First nano-hydrodynamic experiments performed with SFA :
Experiments with ultra thin liquid films
solid or glass transition ?
a controversy resolved
Nano- particules are present on mica surfaces when cut with platinum hot-wire
They affect significantly properties of ultra-thin sheared films (Zhu & Granick 2003, Heuberger 2003, Mugele & Salmeron)
Methods to cleave mica without particules have been designed(Franz & Salmeron 98, recleaved mica).
They seem to be removed by water
Drainage of ultra-thin films
Monochromatic light
OMCTS moleculeØ 9-10 Å
recleaved mica(particle free)
Direct imaging with SFA
Becker & Mugele Phys. Rev. Lett 2003
Drainage occurs by steps corresponding to layering transitions
Layering transitions
F. Mugele & T. Becker PRL 2003
The heigth between each steps is the size of a OMCTS molecule
Each step is the expulsion of a single monolayer
2 layers 3 layers
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http://pcf.tnw.utwente.nl/people/pcf_fm.doc/
The growth of the N-1 layers region gives information on the flow in the N-layers film.
Persson & Tossati model for the dynamics of the layer expulsion
N layerstransition
N -1layers
No flowAverage velocity V(x)
x
P=Cte
Hypothesis :transition region moves at velocity r(t)
Lubrication flow in the N-layers region
Constant pressure Po in the non-flowing N-1 layers region
(Assumes some linear friction law for the flow in the thin film)
Hydrodynamic limit:
r(t)
+ lubrication
xo : maximum extend of the layered region
Ao = xo 2 maximum area of the layered region
A = r 2 actual area of the N-1 layers region
Constant pressure in the non-flowing region :
Mass conservation :
d : layer thickness
Nd : flowing film thickness
4 33 2
2 1
2 1
Ao measured
Po = Load / Ao
One ajustable parameter for each curve : µ
Po determined from load
PT model describes very well the dynamics of a monolayer expulsionwith an ad hoc friction coefficient µ depending on the flowing film thickness
PT model:
N
Macroscopic hydrodynamic:(with no-slip at wall)
Comparison with macroscopic hydrodynamics
N
Effective friction is larger than predicted by hydrodynamic.
For N≤5 layers, discrepancies with macroscopic hydrodynamic occur.
Ad hoc friction model meets hydrodynamic friction at large N
P=Cte
N-1
N
Discrete layers flow model
transition
Force balance on one layer of thickness d and length dx
x+dxx
F
i+1 i
i -1 i
F
Hydrodynamic limit:
Solving discrete layers flow model
i,i±1 = ll
1,0 = N,N+1 = lssolid-liquid friction
Solve for 1D flow : mass conservation
liquid-liquid friction
1≤ i ≤N
Velocity of transitionregion, measured
N+1 equations give Vi and dP/dx as a function of ll and ls
Adjust ll and ls so that
Ad hoc friction coefficientof the PT model
Assume two different friction coefficients
Results of Becker & Mugele 2003
Flow in ultra-thin films is very well described by a lubrication flow with . ad-hoc friction coefficient depending on the film thickness.
For N≤5 layers the friction coefficient is slightly larger than predicted by . macroscopic hydrodynamics with no-slip b.c.
The dependence of the ad-hoc friction with the film thickness is well . accounted by 2 intrinsic friction coefficients, one for liquid-liquid friction . and one for liquid-solid friction
Liquid-liquid friction is close to the value of hydrodynamic limit
Liquid-solid friction is about 20 times larger than liquid-liquid friction