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1 The experimental validation of numerical simulation for precise polymer melt processing by Malcolm Mackley, David Hassell* Tim Lord and Lino Scelsi. Department of Chemical Engineering and Biotechnology. University of Cambridge. UK *School of Chemical and Environmental Engineering. University of Nottingham. Selanger, Darul Ehsan, Malaysia Hong Kong 2009

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This presentation reviews how it is now possible to model the processing flow of molten polymer

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Page 1: Hong Kong MPR -09

1

The experimental validation of numerical simulation for precise polymer melt processing

by

Malcolm Mackley, David Hassell* Tim Lord and Lino Scelsi.

Department of Chemical Engineering and Biotechnology. University of Cambridge. UK

*School of Chemical and Environmental Engineering. University of Nottingham.Selanger, Darul Ehsan, Malaysia

Hong Kong 2009

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Mission

• Carry out precise polymer processing experiments that can be compared with simulation.

• Characterise rheology of polymer and select constitutive equation.

• Numerically simulate viscoelastic flow and match result with experiment.

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The Cambridge Multipass Rheometer (MPR)

Rheo Optic slit flow mode Cross-slot flow mode

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The Cambridge Multipass Rheometer (MPR)

Top section

Test section

Bottom section

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Test section geometries

• Slit

Depth =10, 7 and 1.5 mm

1.4 mm

1.5 mm

1.5 mm

1.5 mm

10 mm

0.75 mm

• Cross-Slot

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Depth =10, 7, and 1.5 mm

R = 0.375 mm

Z ~ 1.4 mm

10 mm

The Geometries: Contraction Expansion Slit

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An example of Rheo optic slit flow for LDPE

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Visit MPR Slit Flow movie

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The Cross-Slot

• Generates a hyperbolic pure shear flow pattern as shown.• Near centre. Essentially uniform extensional flow with residence time, which

is equivalent to strain, inversely dependant on distance from the exit symmetry axis

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MPR Cross-Slot Flow

• The MPR action modified for cross-slot flow

• Pistons force polymer melt through a cross-slot geometry

Kris Coventry and Collaborative project with Leeds University; Tom Mcleish et al

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Typical Result

-Dow PS680E

-Piston velocity of 0.5 mm/s (maximum extension rate =4.3/s).

-Inlet slit width=1.5mm

-Section depth=10mm

- T=180°C.

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Visit MPR Cross Slot Flow movie

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Rheology and Characterisation

• Linear viscoelasticity

Obtain spectrum of relaxation times• Non Linear response.

Sentmanat Extensional Rheometry fixtures (SER)• Constitutive equations

Pom Pom or Rolie Poly• Simulation

Leeds 2D Flowsolve or 3D EUsolve

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Simulation

For linear polymer melts, “Rolie-Poly” theory is used

Constitutive equation;

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Multimode Pom-Pom model

Viscoelastic stress:

Backbone orientation:

Stretch:

Time scales:

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16dP = 3.32 bar dP = 3.76 bar

3D simulation2D simulation

Vp = 0.44 mms-1

2D FlowsolveAnd3D EUsolve

Polystyrene (PS2)

10mm depth

Pom Pom

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17dP = 3.96 bardP = 3.76 bar

Vp = 0.44 mms-1

3D simulation Experiment

3D EUsolve

Polystyrene (PS2)

10mm depth

LHS Pom Pom

RHS Experiment

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3D EUsolve

Polystyrene (PS2)

7 mm depth

LHS Pom Pom

RHS Experiment

dP = 5.46 bar dP = 5.18 bar

Vp = 0.44 mms-1

3D simulation Experiment

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3D EUsolve

Polystyrene (PS2)

1.5 mm depth

LHS Pom Pom

RHS Experiment

dP=9.66bardP=17.24bar

Vp = 0.07 mms-1

3D simulation Experiment

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t= 0.1 s t= 10 s t= 18.9 ss

t = 0.1 s t = 8 s t = 12 s

PomPom

RoliePoly

Pom Pom vs Rolie Poly, 3D EUsolve

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Vp = 0.04 mms-1 Vp = 0.09 mms-1

MPR experiment3D simulation MPR experiment3D simulation

Cross Slot Pom Pom 3D EUsolve

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Vp = 0.07 mms

Cross Slot 1.5mm depth. Pom Pom 3D EUsolve

Simulation Experiment

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t = .1 s t = 8.5 s t = 37 s

t = 0.1 s t =17 s t =37 s

Cross Slot Pom Pom vs Rolie poly 3D EUsolve

PomPom

RoliePoly

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24EPSRC Microscale Polymer Processing project

Tim Lord, David Hassell and Dietmar Auhl 2008

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10-1 100 101 102 103

103

104

105

106

LDPET = 150°C 10

5

2

10.5

0.10.010.001

shear

visc

osi

ty (

t), P

as

elo

ngatio

nal v

isco

sity

(t)

, P

as

time t, s

10

3

10.3

0.001

0.003

0.010.030.1.0 [s-1]

.0 [s-1]

Stagnation Point flows as rheometersDr Dietmar Auhl et al, Leeds University 2008

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ststyyxxstE /)(,

pistonst VxA

22 4 xyyyxxSOCn X-4 -2 0 2 4

steady-state elongational viscosity at the stagnation point

=

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Dr Dietmar Auhl et al , Leeds University

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Conclusions

• MPR experiments provide precise processing data.

• Both Rolie Poly and Pom Pom models can be simulated to give good experimental matching.

• Simulation can be sensitive to both constitutive equations,

relaxation spectra and non linear fit.

Acknowledgements. Tom Mcleish for masterminding Microscale Polymer Processing project and EPSRC for providing most of the funds