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Rheology and microstructure in concentrated non-Brownian suspensions
Frédéric Blanc, Talib Dbouk, Stany Gallier, Giovanni GhigliottiLaurent Lobry, François Peters, Elisabeth Lemaire
Ubiquitous suspensionssandcement
muds
Blood
Propergols
Stone
Model suspensions Spherical mono-dispersed particles nearly hard spheres buoyant particles
Model experiments: Local measurements of viscosity of normal stresses Of microstructure
Various behaviors various particle interactions various shapes and sizes effect of the flow
Main question: are there solid contacts betweenparticles? What is their effect?
Hydrodynamic collision, rigid particles reversible trajectory
But: the microstructure is anisotropic
trajectories are anisotropic
N spheres hydrodynamic Interactions Pine et al. Nature (2005)
contact Interactions Metzger & Butler Phys.Rev. E (2010)
Why perform local measurements ?
After migrationBefore migration
Outline
Vicosity measurement using PIV and PTVTransient behavior under shear reversalViscous and contact contribution to the
viscosityMicrostructure characterizationDependence on the particle concentrationQuantitative information on contacts
Normal stresses
PIV facility
PMMA particles + Cargille oil nparticules=nfluide
particules=fluide
Themostated box
R1=1.4cmR2=2.4cm
Suspensions and flow regime
0=1 Pa.s. 20%<<55%
Negligible Brownian motion
Negligible inertia
35 906 aPe 10 10
kT
2 29 6 4 2
p0 0
a RRe 10 10 Re 10 10
=55%=44%
PIV experiments2a=30µm0.25% fluorescent particles
PTV experiments 2a=170µmFluorescent suspending fluid
High shear deformations
Newtonian fluid2 2in out
2 2 2out in
R R 1(r) 2R R r
2(r)2 Lr
Migration toward the stator
vr
(r) rr
=44%
0.6 0.7 0.8 0.9 1
20
40
60
/R
/ 0
2000 revolutions
2 revolutions (first plateau)
0.7710 revolutions
cste
cste
Newtonian fluid2 2in out
2 2 2out in
R R 1(r) 2R R r
2(r)2 Lr
Migration toward the stator
=44%
High shear deformations
Viscosity vs particle concentration
Kriegger Dougherty :
02( )
1*
0 1 2 30
10
20
30
40
/
0
Transient response
t
0 1 2 30
10
20
30
40
/
0
Transient response
t
compression
Gadala-Maria and Acrivos (1980) Couette small gap
Kolli et al. (2002), Narumi et al. (2002)Torsionnal flow
Dilatat
ion
Variation with particle concentration
0.5 1 1.5 2 2.5
101
102
/
0
=0.30
=0.40
=0.444
=0.47
=0.50
0.3 0.4 0.50
0.2
0.4
0.6
0/min
(0/plateau)0.5
(0/plateau)0.5= - 2.117 + 1.124
0/min = - 1.243 + 0.667
*=0.538
*=0.531
Viscosité de plateau
Kriegger Dougherty
plateau 2
1( )
1*
Minimum viscosity
min1( )
1*
Mills & Snabre EPJ E (2009)4
3
hydro ( )1
*
Sierou & Brady JFM (2001)
Stokesian dynamics
Random suspension
0.4 0.6 0.8 10
0.1
0.2
0.3
0.4
/ *
(0/
)PIV *=0.53SD *=0.64 [Sierou and Brady (2001)
Structural viscosity
0.1 0.2 0.3 0.4 0.5 0.60
0.2
0.4
0.6
0.8
1
pa
rt/pl
atea
u
0 1 2 30
10
20
30
40
/
0
part plateau min struct
struct
=0.44
Microsture characterization
fluorescent liquid
Particules 170µm
Laser sheet d30µm
R1=1.9cm
R1=2.4cm
=55%
PDF for =0
(r, )g(r, )
r/2a
<2a>=170 µm
compression
Dilatat
ion
=35%Parsi & Gadala-Maria J. Rheol. (1987)
Expérimental Numéric (DS)=32% Pe =1700
Gao et al. PRL (2010)
=40%
PDF for 0
PDF versus
Structure en aller-retour (1)
0 1 2 3 4 5 6 7 83
3.5
4
4.5
5
local
[
pa.s
]
0 2 4 6 80.3
0.35
0.4
moyen
[r
pm]
Retour
=35%
Aller
Da Cunha & Hinch (1996)
expérimental PDF f=5% interactions de paires
2(a+e)
PDF of diluted suspension
experimental PDF f=5% theoretical PDF
AFM200 nm
model 250 nm
PDF of diluted suspension
Normal stresses
• Experimental state of art
11
22
F=21S
33
Negative compressional normal stresses
1 11 22 1 0
2 22 33 2 0
NN
Gadala-Maria (1979) N1, N2
Zarraga J. Rheol. (2000) N1<0, N2<0
Singh & Nott J.F.M. (2003) N1<0, N2<0
Boyer, Couturier Guazzelli, Pouliquen (2011)
profilometry
s
N10 N2()<0
1) Normal stress differences
V J J
2
0
2a f ( )9
J p. Nott & Brady, J. Fluid Mech. (1994).Morris & Boulay, J. Rheol. (1999).
2) Particle normal stresses Experiment from Deboeuf et al. Phys. Rev. Lett. 102, 108301(2009)
Prasad D. & Kytomaa H.. Int J Multiphase Flow; 21(5):775 (1995)
Paroi semi-perméable
≠0=0
|P|=
colloïdes
Motivation : Shear induced migarationSuspension Balance Model :
Measurement of N1, N2 andTorsionnal flow
zv rh
rh
h
Capteurs directs 22 Capteurs à grille
Pf
h=2 mm
R=5.5 cm
Direct pressure sensors 22(r)
33 33 11 0r r
1. .e
22 0 R 1 2 1 2r(r) 2R
33(R)=pa=0
11
33
22
pii
p p11 22 1p p33 22 2
N
N
N1 et N2
p f f22 22 22 22Σ =Σ -Σ =Σ +P
fluid pressure sensors
Experiment (1)
SuspensionsPolystyrene particles (2a=40 ou 140 µm) 0.2<<0.5Mixture water, ucon oil, Zinc Bromide 1 Pa.s.
Stress controlled rheometerR=5.5 cm h2 mm
11 100 s
Protocol
t
40 s
20 s
Experiment (2)
Direct sensors Grid sensors
Experiment (3)direct sensors
22 R 1 2 1 2r(r) 2R
Experiment (4)
Grid sensors
Normal stress differences
1 11 22 1 0
2 22 33 2 0
NN
-N1/ -N2/
Normal stress differences comparison
Boyer Couturier GuazzelliPouliquen JFM (2011)
2
1+2 2
1+2 2 21 0
Some numerical results, Force Coupling Method
Hertz contact, rugosity 5 10-3 a 10 a
Measurement at center Average measurement
2 frictionless
1 friction (µ=0.5) 1 friction (µ=0.5)
1 frictionless
2 friction (µ=0.5)
2 friction (µ=0.5)
2 frictionless
1 frictionless
Comparison between numerical and experimental results
1 friction (µ=0.5)
1 frictionless
2 friction (µ=0.5)
2 frictionless
Role of friction on viscosity
Results ( )
p11
p 211 12
p11
p 211 12
p11 p11
p 211 12
Re-suspensionp33 Re-suspensionp33
0 0 p( ) 2 ( ) Q EpΣ
n 2
3
1 0 0( ) ( ) 0 0
0 0
Q 2=0.8 ; 3=0.5
p22
12
p11
12
0 0 p( ) 2 ( ) Q EpΣ
n 2
3
1 0 0( ) ( ) 0 0
0 0
Q 2=0.8 ; 3=0.5
p22
12
p11
12
pii
F
Boyer F., Guazzelli E. & Pouliquen O.Phys Rev Lett. 107 (2011)
p 110
/
stru
ct
=0.21
Déplétion angle
0 0 .1 0 .2 0 .3 0 .4 0 .50
0 .2
0 .4
0 .6
0 .8
1
Boyer et al.JFM 2011
1+2 2s 2a=140µm
0 0 .1 0 .2 0 .3 0 .4 0 .50
0 .2
0 .4
0 .6
0 .8
1
Boyer et al.JFM 2011
1+2 2s
1+2 2s 2a=140µm
Rheology-microstructure
Conclusions / Perspectives
Coupling between rheology and microstructure(0.5, hmax 10 min )
Importance of the contact forces Change the particle rugosity
Study of emulsuions
Difficulties of measuring the bulk properties of a suspension, effect of confinementNumerical simulations and back-and-forth with experiments
Nanoparticlesgraftted