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Structures and Composite Materials Laboratory CRIAQ COMP5 CRIAQ COMP5 Modelling Work Progress Modelling Work Progress Erin Quinlan McGill University February 16, 2009

Structures and Composite Materials Laboratory CRIAQ COMP5 Modelling Work Progress Erin Quinlan McGill University February 16, 2009

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Structures and Composite Materials Laboratory

CRIAQ COMP5CRIAQ COMP5Modelling Work ProgressModelling Work Progress

Erin QuinlanMcGill University

February 16, 2009

Structures and Composite Materials Laboratory

Outline

• Background• Objectives• Modelling approach• Work plan• Next steps

Structures and Composite Materials Laboratory

Thermoplastic Composites Processing

Comprehensive Composite Materials

Structures and Composite Materials Laboratory

Consolidation Steps

• Plies come into contact with each other with added temperature and pressure

• Resin flow begins to fill the voids

• Polymer chains link together (autohesion)

• Fibres impregnate through the resin

• Cooling and crystallization

Structures and Composite Materials Laboratory

Processing Window

Cooling rate, log (dT/dt)

Pressure

High void content

Equipment limitationsUncontrolled flow

Fibre damageResin starvation

Eco

no

mic

lim

itat

ion

sT

her

mal

deg

rad

atio

n

Res

tric

ted

flo

wP

ract

ical

lim

itat

ion

s

Optimal

processing

region

Comprehensive Composite Materials

Structures and Composite Materials Laboratory

Objectives

• Model the thermoplastic tape behaviour during the Automated Fibre Placement (AFP) process

Tool

New ply

Laminate

Pressure

Temperature

Structures and Composite Materials Laboratory

Modelling Approach

materialscharacterization

science of processing

numerical implementation

data analysis & verification

‘raw’ material process compositepart

equations material properties

solve equations

what does it mean?

Structures and Composite Materials Laboratory

State VariablesDatabase

Void

AFP Machine

Thermo-chemical

FlowCompaction

Input

Output

Typical Process Model Architecture

Structures and Composite Materials Laboratory

Thermochemical Module

• The thermochemical module is responsible for calculation of – temperature in the structure of interest– degree of crystallinity in composite components

• The thermochemical module consists of a combination of analyses for heat transfer and crystallization kinetics.

Structures and Composite Materials Laboratory

Laminate

Semicrystalline Thermoplastic Thermal Analysis

umP Hdt

dcm

z

TK

zt

Tc

*

Heat generation due tocrystallization

Tool

z

Ply

Structures and Composite Materials Laboratory

Semicrystalline Thermoplastic• Heat generation

– c* : crystallinity of matrix

– mm : matrix mass fraction

– Hu : ultimate heat of crystallization of the polymer at 100% crystallinity

• Rate of degree of crystallinity– g : functional relationship– dT/dt : heating rate (cooling rate)

um Hdt

dcm

*

Tdt

dTg

dt

dc,

*

Structures and Composite Materials Laboratory

Flow-compaction Module

• The flow-compaction module is responsible for calculation of – prepreg consolidation– degree of intimate contact– autohesion

Phenomenon Mechanism

Interfacial bond formation (consolidation)

Autohesion

Interfacial deformation (coalescence)

Viscoelastic deformation of prepreg tows

Structures and Composite Materials Laboratory

Modelling Consolidation

• Intimate contact• Interply bonding

Structures and Composite Materials Laboratory

Prepreg Interply Intimate Contact

• Modelling approach:– Characterize prepreg surface roughness– Measure neat resin viscosity– Fluid mechanics

• Modelling results:– Time required to achieve complete interply intimate

contact for a given set of temperature, pressure and prepreg geometric parameters

• Verification– Optical microscope– Scanning acoustic microscope

Structures and Composite Materials Laboratory

Prepreg Surface Roughness Model

Structures and Composite Materials Laboratory

Single Ply ModelRigid Flat Surface

Prepreg

ho

wo bo

t = 0

Rigid Flat Surface

Prepreg

hw b

t > 0

Papp

Degree of intimate contact Dic 00 bw

bDic

Structures and Composite Materials Laboratory

Single Ply Model• Assumptions:

– Squeezing flow between two rigid parallel plates– Viscous laminar flow– Viscosity is independent of shear rate

– w0 = b0

Dic : degree of intimate contact

Papp : consolidation pressure

0 : zero-shear rate viscosity

5

12

0

0

000

1012

1

1

t

w

hP

bw

hhD appoic

Structures and Composite Materials Laboratory

Neat Resin Rheology

Structures and Composite Materials Laboratory

Degree of Intimate Contact Versus Time

APC-2 Prepreg surface against a rigid flat surface

Structures and Composite Materials Laboratory

Autohesion Phenomenon

Initial Contactt=0

PartiallyDiffused

t>0

CompletelyDiffused

t=t∞

Interface

Chain Like Molecules

Structures and Composite Materials Laboratory

Autohesive Strength Measurements

Structures and Composite Materials Laboratory

Autohesive Strength Measurements

Structures and Composite Materials Laboratory

Isothermal Autohesion Model

TCT

a

T

Ta

tTCG

tGR

T

T

IC

IC

5

21

1094.1

46926.11

469604.1log

)(

T is in °K

Structures and Composite Materials Laboratory

Modelling Void Fraction

• Voids form after heating during the consolidation phase

Resin

Void

Fiber

Structures and Composite Materials Laboratory

Void Formation

Apply heatApply pressure

Structures and Composite Materials Laboratory

Void Fraction Content vs. Pressure

Structures and Composite Materials Laboratory

Work Plan

• Model development:– Implement 1D heat transfer model– Implement crystallinity kinetics model– Tape machine heat source model

• Material characterization– Crystallinity model– Tape roughness measurement

• Validation experiments– Get temperature-time data from AFP experiments

(effect of pressure, temperature, layup speed)

Structures and Composite Materials Laboratory

References

• “Automated Dynamics” http://www.automateddynamics.com/

• “Thermoplastic Composites: Module 6”• S. Ranganathan, S.G. Advani, and M.A. Lamontia, “A

Non-Isothermal Process Model for Consolidation and Void Reduction During In-Situ Tow Placement of Thermoplastic Composites”, Journal of Composite Materials 29(8), 1995, pp. 1040-1062.

• J.M. Tang, W.I. Lee, G.S. Springer. “Effects of Cure Pressure on Resin Flow, Voids, and Mechanical Properties”. Journal of Composites 21, 1987, pp. 421-440.