A new interpretation for the dynamic behavior of complex fluids at the sol-gel transition using the fractional calculus

Similar documents
Fractional Calculus The Murky Bits

Glass Transition as the Rheological Inverse of Gelation

Viscoelasticity, Creep and Oscillation Experiment. Basic Seminar Applied Rheology

Quiz 1. Introduction to Polymers

Abvanced Lab Course. Dynamical-Mechanical Analysis (DMA) of Polymers

Contents. Introduction.

Rheology, Adhesion, and Debonding of Lightly Cross-linked Polymer Gels

Chapter 6 Molten State

Quiz 1 Introduction to Polymers

Rheology and Constitutive Equations. Rheology = Greek verb to flow. Rheology is the study of the flow and deformation of materials.

Fractional Derivatives and Fractional Calculus in Rheology, Meeting #3

Rheological Behaviors of PVA/H 2 O Solutions of High-Polymer Concentration

Entanglements. M < M e. M > M e. Rouse. Zero-shear viscosity vs. M (note change of slope) Edwards degennes Doi. Berry + Fox, slope 3.4.

Mechanical selfsimilarity of polymers during chemical gelation*)

The Internal Friction and the Relaxation Time Spectrum of Ferroelectric Ceramic PZT Type

Viscoelastic Flows in Abrupt Contraction-Expansions

SPECTRAL ANALYSIS AND THE INTERCONVERSION OF LINEAR VISCOELASTIC FUNCTIONS

Viscoelasticity. Basic Notions & Examples. Formalism for Linear Viscoelasticity. Simple Models & Mechanical Analogies. Non-linear behavior

3.032 Problem Set 4 Solutions Fall 2007 Due: Start of Lecture,

University Graz / Austria Institut für Chemie Volker Ribitsch

Stress Overshoot of Polymer Solutions at High Rates of Shear

arxiv: v3 [physics.bio-ph] 2 May 2018

Rheology of cellulose solutions. Puu Cellulose Chemistry Michael Hummel

Polymer Dynamics and Rheology

Self-Similar Relaxation Behavior at the Gel Point of a Blend of a Cross-Linking Poly(ɛ-caprolactone) Diol with a Poly(styrene-co-acrylonitrile)

Experimental Colloids I (and I)

Relaxation Patterns of Nearly Critical Gels

3.032 Problem Set 4 Fall 2007 Due: Start of Lecture,

CM4655 Polymer Rheology Lab. Torsional Shear Flow: Parallel-plate and Cone-and-plate

Supporting Information

For an imposed stress history consisting of a rapidly applied step-function jump in

Effects of dissolution temperature on the rheological properties of polyvinyl alchol solutions in dimethyl sulfoxide

Session 11: Complex Modulus of Viscoelastic Polymers

The Solidification Rheology of Amorphous Polymers - Vitrification as Compared to Gelation

Non-linear Viscoelasticity FINITE STRAIN EFFECTS IN SOLIDS

In-depth analysis of viscoelastic properties thanks to Microrheology: non-contact rheology

Sol Gel Transition in Aqueous Alginate Solutions Induced by Cupric Cations Observed with Viscoelasticity

Contents. Preface XIII. 1 General Introduction 1 References 6

ModellingTwoDifferentDispersePolystyrenewithMaxwellFractionalModelinSAOSExperiments

Rheology, or the study of the flow of matter. Panta rei. (Panta rhei)

Period #1 : CIVIL MATERIALS COURSE OVERVIEW

NEW RHEOLOGICAL PROBLEMS INVOLVING GENERAL FRACTIONAL DERIVATIVES WITH NONSINGULAR POWER-LAW KERNELS

Rheology of Soft Materials. Rheology

Rheological And Dielectric Characterization of Thermosetting Polymers. Jeffrey Gotro, Ph.D.

Aging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology

Dynamic Mechanical Analysis of Solid Polymers and Polymer Melts

I. Comparison between rheological data obtained by using the shear rate sweep and frequency

Guideline for Rheological Measurements

Fundamentals of Polymer Rheology. Sarah Cotts TA Instruments Rubber Testing Seminar CUICAR, Greenville SC

Monitoring the Kinetics of UV Curing Using In Situ Rheology and Real-Time Fourier Transform Infrared Spectroscopy

2007 Summer College on Plasma Physics

Elements of Polymer Structure and Viscoelasticity. David M. Parks Mechanics and Materials II February 18, 2004

The Large Amplitude Oscillatory Strain Response of Aqueous Foam: Strain Localization and Full Stress Fourier Spectrum

Non contact measurement of viscoelastic properties of biopolymers

Lecture 7 Constitutive Behavior of Asphalt Concrete

Relaxation in filled polymers: A fractional calculus approach

Lecture 5. Rheology. Earth Structure (2 nd Edition), 2004 W.W. Norton & Co, New York Slide show by Ben van der Pluijm

ON FRACTIONAL RELAXATION

Soft matters end use properties analysis thanks to Microrheology

Modelling the Rheology of Semi-Concentrated Polymeric Composites

C subjected to large deformation rates exhibit

On the scaling of molecular weight distribution functionals

SEISMOLOGY. Master Degree Programme in Physics - UNITS Physics of the Earth and of the Environment ANELASTICITY FABIO ROMANELLI

Colloidal Suspension Rheology Chapter 1 Study Questions

Quantitative prediction of transient and steady-state elongational viscosity of nearly monodisperse polystyrene melts

Introduction and Fundamental Concepts (Lectures 1-7)

Mechanical Models for Asphalt Behavior and Performance

Analytical Rheology Linear Viscoelasticity of Model and Commercial Long-Chain-Branched Polymer Melts

Response of an elastic Bingham fluid to oscillatory shear

A Phenomenological Model for Linear Viscoelasticity of Monodisperse Linear Polymers

Rheological properties of polymer micro-gel dispersions

Origins of Mechanical and Rheological Properties of Polymer Nanocomposites. Venkat Ganesan

MP10: Process Modelling

Chapter 4. The Effect of Elastic Softening and Cooperativity on the Fragility of

4/14/11. Chapter 12 Static equilibrium and Elasticity Lecture 2. Condition for static equilibrium. Stability An object is in equilibrium:

Influence of steady shear flow on dynamic viscoelastic properties of un-reinforced and Kevlar, glass fibre reinforced LLDPE

Electric Field Induced Gelation of Poly(3-Thiopheneacetic Acid)/Polydimethylsiloxane

Chemically and Physically Cross-linked Gelatin Gels Dominique Hellio and Madeleine Djabourov

Measuring structure of low viscosity fluids in oscillation using rheometers with and without a separate torque transducer

Synergy of the combined application of thermal analysis and rheology in monitoring and characterizing changing processes in materials

Micromechanics of Colloidal Suspensions: Dynamics of shear-induced aggregation

Lecture 4: viscoelasticity and cell mechanics

Colloidal particles aggregating by attractive interactions form disordered, highly ramied clusters however, despite their apparent complexity, these s

Thermal Analysis of Polysaccharides Mechanical Methods

Math 2214 Solution Test 1D Spring 2015

Biomacormolecular Materials

Creep. Creep behavior of viscoelastic polymeric materials

CONSISTENCY OF RHEOLOGICAL EXPERIMENTS FOR PSA CHARACTERIZATION

The ph Dependence on the Rheology of Wheat Protein Isolate Suspensions

ELASTIC INSTABILITIES IN CONE{AND{PLATE FLOW: SMALL GAP THEORY. David O. Olagunju. University of Delaware. Newark, DE 19716

Polymers. Steep Slope = 3/5 : Self-Avoiding Walk (Polymer Solution) Shallow Slope = 1/2 : Gaussian Random Walk (Polymer Melt)

Quiz 1 Introduction to Polymers (Please answer each question even if you guess)

Mechanical Properties of Monodomain Side Chain Nematic Elastomers

RHEOLASER LAB MICRORHEOLOGY & END USE PROPERTIES ANALYSIS. MICRORHEOLOGY

RHEOLOGY & LINEAR ELASTICITY. B Importance of fluids and fractures in deformation C Linear elasticity for homogeneous isotropic materials

Lecture 5: Macromolecules, polymers and DNA

Nonequilibrium transitions in glassy flows II. Peter Schall University of Amsterdam

A Technique for Characterizing Complex Polymer Solutions in Extensional Flows. Gavin Braithwaite Stephen Spiegelberg

Shear rheology of polymer melts

Connection-improved conductive network of carbon nanotubes in the rubber crosslink network

Transcription:

A new interpretation for the dynamic behavior of complex fluids at the sol-gel transition using the fractional calculus By Stephane Warlus and Alain Ponton Rheol. Acta (009) 48:51-58 Chris Dimitriou NNF Summer Reading Group 7/1/010 1

The Critical Gel Terminology Liquid Solid Transition (LST) Sol-Gel Trasition (SGT) Critical Gel For a polymer, as crosslinking increases, the material approaches a gel Idea of p p is the ratio of the number of chemical bonds to the total number of possible bonds * As RH we have a critical gel, I.e. the whole network is interconnected p = p c Idea can be extended to physical gels not restricted to crosslinking in polymers *Winter and Mours, Rheology of Polymers near Liquid- Solid Transitions, Advances in Polymer Science, 1997

When do we have a critical gel? The material transitions from behaving like a fluid (relaxes completely) to a solid (has a non zero equilibrium modulus) Relaxation Modulus, G(t) p increasing Viscoelastic Moduli n Phase Angle Relaxation modulus Winter & Mours Warlus & Ponton (p,t) G(t) St n G(t, p c ) S pc t pc t G(t t ') & (t ')dt ' *Winter and Mours, Rheology of Polymers near Liquid- Solid Transitions, Advances in Polymer Science, 1997 3

Contribution of Warlus & Ponton Use of Riemann-Liouville integral operator to solve for constitutive model of a critical gel: (p,t) t G(t t ') & (t ')dt ' t (p c,t) S pc (t t ') pc & (t ')dt ' G(t, p c ) S pc t pc Fractional Element (spring pot) Behavior intermediate between elastic solid and Newtonian fluid, described by following: pc S pc (1 pc ) D f (t) 1 () D f (t) d f (t) dt t 0 f (t ') dt ' 1 (t t ') (p c,t) S pc (1 pc ) d pc (t) dt pc Fractional Element! 4

What does the springpot predict for G, G and tan()? As expected, a power law relaxation modulus: G FE (t) (1 ) t G,G and tan() are given by: d sint 0 dt 0 sin t G '() cos G ''() sin tan() tan 5

Friedrich vs. Warlus Different ways to extract viscoelasti moduli Friedrich, Schiessel and Blumen: E d (t) dt G * () %() / % () %() E d (t) dt e it dt E (i) G * () E (i) ; where: E Multiplication rule % () Warlus and Ponton: d dt sint 0 0 sin t G '() cos G ''() sin 6

The Post-SGT State Warlus and Ponton argue that the behavior in the post SGT state can be described by the fractional Kelvin-Voigt model (KVF) G ep p, p G ep p Shear stress relationship: KVF (p,t) p, p d p (t) dt p G ep (t) Shear stress relaxation modulus: G KVF (p,t) p, p (1 p ) t p G ep 7

The Pre-SGT state Although not written in their 009 paper, the authors have used expressions for the relaxation modulus in the pre SGT state Extended relaxation modulus expression*: G(p p c,t) S p t p exp(t / p ) G ep Pre SGT: CG: Post SGT: G(p p c,t) S p t p exp(t / p ) G(p p c,t) S pc t pc G(p p c,t) S p t p G ep This expression allows the parameters to have relevance in regions not directly at the SGT *Warlus et. al., Eur. Phys. E, 003 8

The fractional derivative order and fractal dimension Warlus states that dynamic light scattering (DLS) experiments show power law relaxation in the dynamic structure factor of some systems Structure and the critical exponent can be related as follows: M : R d f M Molecular Mass of clusters d d d f d d f M. Muthukumar, Macromolecules 1989 R d f d Size of clusters Fractal Hausdorff Dimension Dimension of space (3d space) The fractal dimension can be understood by considering the Koch curve: Box counting is a common method used to determine the fractal dimension of a particular shape 9

Connection to physical gels: wax-oil mixtures Wax-Oil gels are formed when wax precipitates out of the solution at lowered temperatures. A clear gelation point can be identified A 5% wax in oil mixture: T wa =30 C 10s 1 0 0.1% 1s 1 T gel =5.5 C 0.4mm T=7 C T=7.5 T=8 C 0 0.1% C 0 0.1% 0 0.1% n ~ 0.5 10

Relating slope of G () to fractal dimension Warlus and Ponton (Rheol. Acta 009) give the following relation: n d d d f d d f Where d f is the fractal dimension Study by Gao (J Phys. Cond. Matter 006) 10% Wax Oil System (5 C): d f 1.9 11

Box Counting Algorithm The box counting algorithm is an simple algorithm to implement so as to determine the fractal dimension from digital images Begin with raw image: Threshold/Extract boundary: Box Size With boxes of varying size (), measure how many are required to cover the boundary (N boxes) Plot log(n) vs log() and the slope is equal to the box counting fractal dimension 1

Conclusion Critical gel: Terminology and behavior Using fractional calculus and fractional elements to understand behavior at the critical gel point Viscoelastic moduli, relaxation modulus Pre and post SGT state according to Warlus and Ponton Connection between fractional derivative order and fractal dimension Connecting Warlus work with a physical gel Thank you for your attention! Questions? 13