diffusion and permeability in polymers
TRANSCRIPT
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GCH 6101- Polymer Diffusion PM Wood-Adams 1
Permeation Rate at which a gas or vapor passes through a polymer Consists of 3 processes:
Absorption of the permeating species into the polymer Diffusion through the polymer Desorption of the permeating species from the polymer
surface and removal
Factors affecting permeability of a polymer: Solubility and diffusivity of the small molecule in the
polymer
Chain packing and side group complexity, polarity,crystallinity, orientation, fillers, humidity andplasticization
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GCH 6101- Polymer Diffusion PM Wood-Adams 2
Essential factors for permeation
Free volume: in order for any molecules to move in amaterial there must be holes available
Continuous path through the polymer
increasing elapsed time
Example ofdiffusion:
After some time:
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GCH 6101- Polymer Diffusion PM Wood-Adams 3
Ficks Laws Steady State:
Unsteady state:xc
DJ=
Schematic of steady state diffusion
=
x
cD
xt
c
J is the flux of permeant [=] (mass/area/time)
D is the diffusivity: it depends on polymer, diffusing species,temperature and in some cases on concentration c.
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GCH 6101- Polymer Diffusion PM Wood-Adams 4
Example of diffusion in a rubbery polymer Studying the effect of dissolved CO 2 on viscosity of HDPE The CO 2 was diffused into the sample in the rheometer where
only the edges of the rectangular sample were exposed to the
gas Measurement of stress was performed at the center of the
sample needed to know when the concentration of thediffusant in the center of the sample had reached the solubility.
Reference: Effects of Pressure and Supercritical Fluids on the Viscosity of Polyethylene,
Park and Dealy, Macromolecules 2006, 39, 5438-5452
Gas diffuses in on the sides ofthe sample but not on the top
or bottom.
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GCH 6101- Polymer Diffusion PM Wood-Adams 5
DiffusionDiffusion
and Saturationand Saturation
+= 2
2
2
2
yc
xc D
t c
Saturation TimePrediction
Ficks Model
Polymer
ShearStresstransduceractivehead
High P and T chamber of rheometer
L-L
aL
-aL
Diffusant
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GCH 6101- Polymer Diffusion PM Wood-Adams 6
Solution toSolution to 22 DD -- Fick Fick s Diffusions Diffusion Model:Model:
Prediction of Level of SaturationPrediction of Level of Saturation
( ) ( ) ( ) ( )( )
++
++
=
=
= 0 2
22
0 2
22
4
12exp
12
14
4
12exp
12
141
),0,0(
m
m
n
n
aL
t m D
m L
t n D
nS
t C
Dimensionless center concentration with time:
Relative amount absorbed by polymer with timeto the absorbed quantity after infinite time:
( ) ( )( )
( )( )
( )
2 2
2 220
2 2
2 220
2 1( ) 81 exp
42 1
2 18 exp2 1 4
n
m
D n t M t
M Ln
D m t m aL
=
=
+ = +
+ +
( )( )
(0,0, ) and
M t C t
S M will be 0 at t = 0 and 1 after saturation. ( S is solubility.)
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GCH 6101- Polymer Diffusion PM Wood-Adams 7
Results of Ficks analysis
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GCH 6101- Polymer Diffusion PM Wood-Adams 8
Validation of Ficks analysisIn order to monitor the diffusion, viscosity measurementswere taken every few minutes. The CO2 causes adecrease in viscosity, as long as the concentration of CO2
in the middle of the sample is changing then the viscositywill change. When saturation is reached the viscosityreaches and remains constant.
Relative viscosity Viscosity w/o CO 2
Viscosity at saturation
Viscosity at time t
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Saturation with COSaturation with CO 22 : Prediction and Data: Prediction and Data
0
0.2
0.4
0.6
0.8
1
0 60 120 180 240 300 360t (min)
M ( t ) / M (
) , C
( 0
, 0 , t )
/ S , o
r R
D =9x10-5cm 2/s
HDPE with CO 2
180o
C, 18MPa (2600 psi)
)()0()()0(
t R
1s63.0 = &
99% Satu. time
M (t )/ M ( )C (0,0, t )/S
R: with CO 2 R : w/o CO 2
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GCH 6101- Polymer Diffusion PM Wood-Adams 10
Effect of continuous shearing on diffusion
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GCH 6101- Polymer Diffusion PM Wood-Adams 11
Permeability
Permeability coefficient, P = volume of vapour passingthrough a unit area of polymer per unit time, with a unitpressure difference across the sample
Solubility coefficient, S = volume of vapour per unit volume
of polymer per unit pressure
SDP =
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Permeability Data
=
RTE
expPP 0
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Effect of permeant sizeThe diffusion rate decreases with permeant size.Example from previous table for LDPE:
0.346 nm
Size of permeant
0.364 nm0.33 nm
0
2
4
6
8
10
0.32 0.33 0.34 0.35 0.36 0.37
Size of permeant
P
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GCH 6101- Polymer Diffusion PM Wood-Adams 14
Permeation in glassy polymers vs rubbery
polymers
Free volume ismuch lower inglassy polymers
than in rubberypolymers thereforediffusion tends tobe slower
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Permselectivity of polymer membranes and
gas separations
If the permeabilities of 2gases in one polymerare different then thispolymer may be used toseparate the gases to
some extent. This isproperty of the polymerdescribed by the gasselectivity, A/B.
B
ABA P
P=
Open circles are for rubbery polymers and closedcircles are for glassy polymers. Upper bound is an
empirical relation.
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Gas permeability in polymer blends
The gas permeability in polymer blends where onecomponent is dispersed in the other component will fall inbetween upper and lower bounds defined by the parallel
and series models respectively
Upper bound:
Lower bound:
The permeability of a blend can be maximized if thecontinuous phase is made up of the polymer with thehigher permeability.