jens eggers hydrodynamic theory of coating …with bruno andreotti, marc fermigier, jacco snoeijer,...
TRANSCRIPT
Jens Eggers
Hydrodynamic theory of coating
…with Bruno Andreotti, Marc Fermigier,
Jacco Snoeijer, Johanna Ziegler
Dynamical wetting transition
crU
2 cL
Deraguin+Levi 1964
crU
2 cL
continuous transition discontinuous transition
de Gennes 1986
apparent contact angle at the transition?
Small scale physics
moving contact lineHuh and Scriven’s paradox: no motion for 0!micro
stationary
U
h
23 ln( / )micro
L
diss micro
dzU L
h
Lubrication equations
liquid bath
gh(x)
x
y
plate
/slip e /plate e viscous s.t. gravity
(0) 0, (0) 1, ( )h h h
cin units of /( ) :g 33 /( )eCa U
( ,0) slip
uu x U
y
eqnm
(0) eqh
2 3
Cah h
h h
note additional parameter
outer meniscus
( ) ( ) xout apph x e
Matching: Pull!
U<Uc
liquid bath
gmatch!
U>Uc
liquid bath
g
no overlap!
inh outh
compare
0
curvature
matching impossible!
: microscopic length
2
3
3inin in
Cah
h h
1(3 )( ) 3in advh x H x
ap
Critical speed
0
curvatureouth
app
1/ 3
2/3 1/(3 )1
1/3 21 1
2 ( )
( ) 3 2 ( )
CaAi s e
Ca Ai s Ai s
1solve for !s
2/3 1/31
1
2 ( )
( )ap
Ca Ai s
Ai s
Ca
crCa
inh
1/3 1/(3 )
1/3 212 ( )
CaCa e
Ai s
1/3 1/(3 )
1/3 2max2 ( )
Ca
cr
Ca e
Ai s
1/3 1/(3 )
1/32 0.287
Ca
cr
Ca e
1
1/3 2max
1ln
3 54 ( )cr
cr
CaCa
Ai s
“Cox-Voinov”
3 2( 1)1 3 ln
3ap Ca
matching condition
Wetting transition
Delon et al., JFM 2007
transient experiment:
pl crU U
0app at transition
•Derjaguin+Levi 1964:
2cl
c
x
Ca
0.3plate eq
410
simtheory
Beyond the transition
h
x
before
contact line
apparent
contact line
h
x
after
Another transition
Ca
plate angle
Ziegler et al.,
EPJ `09
Wetting transition
Delon et al., JFM 2007
*Ca Ca0q
new film solution!
The Landau Levich Derjaguin film
fhCa
2
31 1
q
h
Ca
h
I: bath
2
2
31Q
HH H
LL-equation
II
2/31/3
CaCa
xh H
2/3q QCa
2/30.95f Cah
2H ( ) 0H
The dimple!
fh
Ca
I: bath
2 II
2/31/3
CaCa
xh H
2/3q QCa
2H ( ) 0H III
1/ 21/ 6
xh Ca H
Ca
balance
includes
gravity!
2
31 1
q
h
Ca
h
A range of new solutions
2/31/3
CaCa
xh H
2/3q QCa
2H
( ) 0H
0Q
2
31Q
HH H
max 1.376Q Q
Phase diagram
Ca
fh0Q
max 1.376Q Q
2
31 1
q
h
Ca
h
1/ 2 2/332f
QCh a Ca
new thick film
solutions!
2/30.95f Cah partial wettingcomplete wetting
Experiment:
The film profile
fh
Snoeijer et al., PRL `08
bath
39.3 10Ca 38.1 10Ca
new thick
film
theory
LLD
film
theory
the dimple!
The big picture
log( )Ca1
log( )fh
2/3
1/2
so far!
1/2
sinfp
Cah
Derjaguin
A fun movie made in Bristol
…work withPhilippe Brunet,Robert Deegan
Bristol Evening Post