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Extensional Characterization of Fluids
Seminar
Basics on Rheology
2
Why is there a need for Extensional Rheology ?
• Extensional flow fields are relevant in many technical applications
• Extensional behaviour can not be detected with rotational
rheometers
• Interest in extensional rheology is growing steadily in
R&D and QC
• Samples can behave similar in rotation but show pronounced differences in extension
3
Extrensional Rheometry
106 105
104 103
102
101
100
10-1
10-2
Range of zero-shear viscosity [Pas] and used method
Meissner Apparatus
Opposed Jet
4-Roll Mill
Porous Flow
4
Comparison of Flow Fields
Most real flow fields are complex. Aim of Rheology is to resolve that into
simple sections.
Uniaxial Extension
• Most simple extensional flow field
• Streamlines converge
• Velocity gradient in direction of flow
Shear Flow
• Streamlines parallel
• Velocity gradient vertical to flow field
y
X
vx
y
X
vx
5
HAAKE CaBER 1 – What is an extensional flow field ?
Deformation
Shear Rate
Shear Stress
1st Normal Stress Difference
Shear Viscosity
x
h
.
ln( ) L
(Hencky) Strain L0
(Hencky) Strain Rate
Extension
.
.
Shear
6
Impact of flow field on a droplet structure
Droplet in a laminar shearing
flow (a polymer coil would
behave exactly the same)
(im
ag
es T
reth
ew
ay (
20
01
)
• Deformation of a droplet at the infeed of a jet nozzle is determined by extension
7
ln ( )
Extensional Rheology: Parameters
(Hencky) Deformation
natural logarithm of rate of
extension
(Hencky) Deformation rate
temporal change of sample lenght in
regars to the instantenious value
Extensional Viscosity
ratio of tensile stress and rate of
deformation
Trouton-ratio
ratio of extesional viscosity and shear
viscosity
L
L0
. 1 dL
L dt
E . l0
L
Uniaxial deformation of a cylinder
[1/s]
[Pas]
Shear Flow
3eTr
/V h
8
HAAKE CaBER 1 Capillary Breakup Extensional Rheometer
Monitoring
D=f(t)
Sample
Laser Micrometer
Appare
nt E
xt.
Vis
cosity
Result Extensional Viscosity
“Mathematics”
Hencky Deformation
9
HAAKER CaBER 1 - CS or CR Rheometer?
No Controlled-Rate Rheometer
• Rate of Deformation
varies with time
( )2( )
( )
mid
mid
dR tt
R t dt
No Controlled-Stress Rheometer
• Capillary pressure
varies with time
( )driving
midR t
… but this kind of space- and time-dependent flow field driven by capillary
forces are commonly observed for so called free-surface
• Die-swell, Atomization, Misting, Roll-Coating, …
Extensional Viscosity ( )
( )( )
midE
R t
t
10
HAAKE CaBER 1 – Theoretical Backround
Surface Tension
• Fz Tensile Force on a fluid element
• s Zero-shear Viscosity
• zz- rr Normal-stress difference
Fz(t)
R(z,t)2 3 s
2
R
R
t zz rr R1 (R , R )
gR02Z0
R2
Tensile Force
In column
Viscous
stress
Non-Newtonian
stress
Capillary
Pressure
Gravitational
Body force
Force Balance Considers time-dependent Newtonian and non-
Newtonian phenomena
The Force Balance for the CaBER Experiment
gives
11
• Hencky strain : up to 0 = 10
( R0/R = 148, L/L0= 2,2 104 )
• Strain rate regime
Applied strain rate : 0.01 < < 300 s-1
Strain rate in sample : 10-5 < < 10 s-1
• Range of shear viscosities : 10 -106 mPas
• Plate diameters : 4 < Dplate < 8 mm, Standard = 6 mm
• Temperature range : 0 – 80 C
• Laser resolution : 10 m
• Data aqusition rate : 0.1 ms
• Dimensions : 40 x 34 x 60 cm
CaBER 1 : Specifications
.
.
12
Applications
• Industry, R&D, QC
• Research, Extensional Rheology
• Paints, Coatings - Stringiness
- Spattering - Misting
• Food
- Stringiness - Mouth feeling
• Resins - Relaxation behavior
- Spinning behavior
• Personal care - Filling behavior
Applications:
Areas:
13
0.0 0.1 0.2 0.3 0.4 0.5 0.610
-2
10-1
100
diameter / mm
final Height: 11 mm
gap: 3 mm
striketime: 20 ms
time / s
Gravity
Surface Tension
Extension
Life-span
of Filament
HAAKE CaBER 1 - Diameter vs. Time
14
Extensional Viscosity
log Deformation rate / s-1
. log
Vis
co
sity
E
/ P
as
(Illu
str
ation
: C
rísp
ulo
Ga
lleg
os)
.
Extensional viscosities of different fluids in uniaxial extension
15
Strain hardening and shear thinning
Flow behavior of a dilute fibre solution in extensional and shear
deformation. Trouton ratio = 3 for or 0
log Deformation rate or [s-1] . .
log
Vis
cosity
or
E [P
a.s
]
Shear
Extension
(Illu
str
ation
: C
rísp
ulo
Ga
lleg
os)
Trouton ratio
. .
16
Extensional viscosity and Misting
0.0 0.5 1.0 1.5 2.00.0
0.5
1.0
1.5
diameter / mm
time / s
Film-split behavior for coating
applications
Misting 5% Acrylic A
10% CMC low
Short break-up time → less Misting Data : Norbert Willenbacher
• Aqeous thickener solution
17
Paper Coatings
0.0 0.2 0.4 0.60.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
10-2
10-1
100
101
102
103
10-1
100
101
102
103
diameter / mm
binder
XSB / A
XSB / B
S/A / C
S/A / D
time / s
viscosity / Pa.s
shear rate / Pa s
Data : Norbert Willenbacher
Extension Shear
• Influence of different binders
■ A1
A2
B1
B2
18
Cardboard Glue
Clear differentiation: ,,best’’ Sample with shortest break-up time
Sample D +
Sample C and A +/-
Sample B -
19
Wall Paint (1)
Squirting Behavior
Sample B (++) > Sample A (+) > Standard
Correlation with the filament break-up possible
20
Wall Paint (2)
Squirting Behavior
Sample B (++) > Sample A (+) > Standard
Correlation with the apparent extensional viscosity
21
Shampoo (1)
No correlation with shear viscosity possible
Filling behavior of Shampoos
1,2 + / 3,4,5 -
Nozzle
Fluid Thread
22
Shampoo (2)
Filling behavior of Shampoo
1,2 + / 3,4,5 -
Correlation with the break-up time
23
Shampoo (3)
Correlation with the apparent extensional viscosity
Filling behavior of Shampoo
1,2 + / 3,4,5 -
24
Polymer/Clay Nano-Composites (1)
Utilization of a small-wt.% nano-particles as filling agent to modify the material properties of “Engineering Plastics” (Giannelis et al., Adv. Polym. Sci. 1999)
• Fire guard, heat deformation, gas-Iimpermeability, wettability…
• No or minor changes to G-modulus, impact resitance, enhanced durability...
Shear flow : Major yield stress for 3 wt %
MMT
1 02
1 03
1 04
1 00
1 01
1 02
1 03
1 0 %
6 %
3 %
1 %
0 %
yx [Pa]
[P
a.s]
(H
oju
n L
ee
(2
00
3)
un
pu
blis
he
d)
25
Polymer/Clay Nano-Composites (2)
Beneath certain % threshold: nano-particles reduce extensibility (of the polymer chain)
Above a certain threshold %: ‘paste-like’ behavior
• High extensional viscosity at low deformation
• Reduced extensibility: material fracture at low deformation
4
6
8100
2
4
6
81000
Exte
nsio
na
l V
iscosity [P
a*s
]
8642
Strain
0%
3%
10%
Fit 0% Fit 3% Fit 10%
3 wt% Clay particles
10 wt% Clay particles (H
oju
n L
ee
(2
00
3)
un
pu
blis
he
d)
0 % Clay particles
26
Thank you for your attention
Any questions ?