Nigel Clarke Department of Chemistry Durham University Effect of Shear Flow on Polymer-Polymer Miscibility: Theoretical Advances and Challenges With.

Slides:



Advertisements
Similar presentations
Boundary layer with pressure gradient in flow direction.
Advertisements

P.W. Terry K.W. Smith University of Wisconsin-Madison Outline
Instructor: André Bakker
Vortex instability and the onset of superfluid turbulence
Computer simulations of amphiphilic worms and bi-layers.
Ch 24 pages Lecture 8 – Viscosity of Macromolecular Solutions.
Convection.
Self-propelled motion of a fluid droplet under chemical reaction Shunsuke Yabunaka 1, Takao Ohta 1, Natsuhiko Yoshinaga 2 1)Department of physics, Kyoto.
Thermodynamics of Oxygen Defective Magnéli Phases in Rutile: A First Principles Study Leandro Liborio and Nicholas Harrison Department of Chemistry, Imperial.
Electro-Hydro-Dynamics Enhancement of Multi-phase Heat Transfer
Boundary Layer Flow Describes the transport phenomena near the surface for the case of fluid flowing past a solid object.
Dr. Kirti Chandra Sahu Department of Chemical Engineering IIT Hyderabad.
..perhaps the hardest place to use Bernoulli’s equation (so don’t)
Active and hibernating turbulence in channel flow of Newtonian and viscoelastic fluids Li Xi and Michael D. Graham University of Wisconsin-Madison Turbulent.
Stress Relaxation of Comb Polymers Keith M. Kirkwood a, Dimitris Vlassopoulos b,c, and L. Gary Leal a a Department of Chemical Engineering, University.
Transport phenomena in chemical processes part III Michał Araszkiewicz PhD.
Generalities Separated Flows Wakes and Cavities. 1.1 What is separation ? A streamline leaves the body and turns into the interior of the fluid 2D separation.
Results It was found that variations in wettability disturb the flow of adjacent liquid (Fig. 3). Our results suggest that for a given liquid the normal.
Center for High-rate Nanomanufacturing Numerical Simulation of the Phase Separation of a Ternary System on a Heterogeneously Functionalized Substrate Yingrui.
Granular flows under the shear Hisao Hayakawa* & Kuniyasu Saitoh Dept. Phys. Kyoto Univ., JAPAN *
Enclosure Fire Dynamics
Dynamics of a Colloidal Glass During Stress-Mediated Structural Arrest (“Relaxation in Reverse”) Dynamics of a Colloidal Glass During Stress-Mediated Structural.
16/12/ Texture alignment in simple shear Hans Mühlhaus,Frederic Dufour and Louis Moresi.
James Sprittles ECS 2007 Viscous Flow Over a Chemically Patterned Surface J.E. Sprittles Y.D. Shikhmurzaev.
CHE/ME 109 Heat Transfer in Electronics
高等輸送二 — 質傳 Lecture 3 Dispersion
Perfect Fluid: flow measurements are described by ideal hydro Problem: all fluids have some viscosity -- can we measure it? I. Radial flow fluctuations:
Perfect Fluid: flow measurements are described by ideal hydro Problem: all fluids have some viscosity -- can we measure it? I. Transverse flow fluctuations:
Rheological study of a simulated polymeric gel: shear banding
Flow and Thermal Considerations
Effect of Shear Flow on Polymer Demixing- the unanswered questions H. GERARD, J. T. CABRAL, J. S. HIGGINS Department of Chemical Engineering Imperial College,
James Sprittles BAMC 2007 Viscous Flow Over a Chemically Patterned Surface J.E Sprittles Y.D. Shikhmurzaev.
Polymer Dynamic.
Protein oligomerization in homogenous protein solutions Crosslinker:GlutaraldehydeOHC-CH 2 -CH 2 -CH 2 -CHO Y. Wang and O. Annunziata Langmuir, 24,
Cosmological Perturbations in the brane worlds Kazuya Koyama Tokyo University JSPS PD fellow.
Dynamics of ITG driven turbulence in the presence of a large spatial scale vortex flow Zheng-Xiong Wang, 1 J. Q. Li, 1 J. Q. Dong, 2 and Y. Kishimoto 1.
Structural origin of non-Newtonian rheology Computer simulations on a solution of telechelic associating polymers J. Stegen +, J. Billen°, M. Wilson °,
Chapter 6 Introduction to Forced Convection:
Travels Between Micro and Macro: Bridging the gap between molecular level descriptions and bulk material behavior Jane E.G. Lipson, Dartmouth College,
LATTICE BOLTZMANN SIMULATIONS OF COMPLEX FLUIDS Julia Yeomans Rudolph Peierls Centre for Theoretical Physics University of Oxford.
Measurements in Fluid Mechanics 058:180:001 (ME:5180:0001) Time & Location: 2:30P - 3:20P MWF 218 MLH Office Hours: 4:00P – 5:00P MWF 223B-5 HL Instructor:
Effects of molecular weight distribution on the flow-enhanced crystallization of poly(1-butene) Stefano Acierno 1, Salvatore Coppola 2, Nino Grizzuti 3.
Constant stress experiment ductile elastic Constant stress (strain varies) Constant strain (stress varies)
Complex dynamics of shear banded flows Suzanne Fielding School of Mathematics, University of Manchester Peter Olmsted School of Physics and Astronomy,
A novel approach for thermomechanical analysis of stationary rolling tires within an ALE-kinematic framework A. Suwannachit and U. Nackenhorst Institute.
Compressible Frictional Flow Past Wings P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Small and Significant Region of Curse.
INTRODUCTION TO CONVECTION
Chapter 3. Instability of the free plane and near – wall plane jet
The Stability of Laminar Flows
Fluctuating hydrodynamics confronts rapidity dependence of p T -correlations Rajendra Pokharel 1, Sean Gavin 1 and George Moschelli 2 1 Wayne State University.
Intermittent Oscillations Generated by ITG-driven Turbulence US-Japan JIFT Workshop December 15 th -17 th, 2003 Kyoto University Kazuo Takeda, Sadruddin.
1 Oldroyd B Model Bead formation in filament stretching Stretching phase Capillary thinning phase Connection between the bead and filament becomes unstable.
Chen-Yang Liu, Roland Keunings, Christian Bailly UCL, Louvain la Neuve, Belgium Dynamics of complex fluids: 10 years on, Cambridge, October Old.
Definitions Polymer Solubility and Thermo $100 $200 $300 $400 $500 Multi- component Materials Polymer Transitions Phase Continuity and Diagrams $400.
Y. Kishimoto 1,2), K. Miki 1), N. Miyato 2), J.Q.Li 1), J. Anderson 1) 21 st IAEA Fusion Energy Conference IAEA-CN-149-PD2 (Post deadline paper) October.
Slow Relaxations in Complex Fluids: Origin and Nature of Dynamical Heterogeneities B. Chakraborty, Brandeis University, DMR Materials as diverse.
Arthur Straube PATTERNS IN CHAOTICALLY MIXING FLUID FLOWS Department of Physics, University of Potsdam, Germany COLLABORATION: A. Pikovsky, M. Abel URL:
IAEA-TM 02/03/2005 1G. Falchetto DRFC, CEA-Cadarache Association EURATOM-CEA NON-LINEAR FLUID SIMULATIONS of THE EFFECT of ROTATION on ION HEAT TURBULENT.
Interaction between vortex flow and microturbulence Zheng-Xiong Wang (王正汹) Dalian University of Technology, Dalian, China West Lake International Symposium.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
CONVECTION : An Activity at Solid Boundary P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Identify and Compute Gradients.
An investigation into the stability and solubility of amorphous solid dispersion of BCS class II drugs Shrawan Baghel, WIT.
The Standard, RNG, and Realizable k- Models. The major differences in the models are as follows: the method of calculating turbulent viscosity the turbulent.
1.1 General description - Sample dissolved in and transported by a mobile phase - Some components in sample interact more strongly with stationary phase.
Non-equilibrium theory of rheology for non-Brownian dense suspensions
Ship Hydrodynamics - Resistance
Deposition and Removal
Microrheology and Rheological Phenomena in Microfluidics
Heat Transfer Coefficient
Polymer Dynamics and Rheology
Presentation transcript:

Nigel Clarke Department of Chemistry Durham University Effect of Shear Flow on Polymer-Polymer Miscibility: Theoretical Advances and Challenges With thanks to: Gavin Buxton, Hervé Gerard, Julia Higgins, Tom McLeish, Dmitri Miroshnychenko

Overview Does flow increase or decrease stability in polymer blends? Coupling phase separation dynamics and stress relaxation in entangled blends Scattering – a quantitative test of theory can we describe concentration fluctuations under shear?

Towards a Theoretical Description Fluctuations in concentration fluctuation in stress if viscosities are different Thermodynamic shear stresses and normal forces directly affect free energy Dynamic stresses affect dynamics of concentration fluctuations hblue >> hgreen regions of high stress regions of low stress

Stress relaxation in polymer blends Constraint release stress relaxed more rapidly if surrounded by short polymers dynamics depends on concentration well defined concentration dependence of stresses … relaxation times in fixed tubes

Doi and Onuki J. Phys. II, 1990, vol. 2, 1631 Equation of motion Doi and Onuki J. Phys. II, 1990, vol. 2, 1631 Coupling between concentration fluctuations Stress fluctuations stress gradients convection thermodynamics

Concentrations fluctuations and the diffusion coefficient One phase region fluctuations decay: D > 0 Two phase region fluctuations grow: D < 0 Phase boundary defined by: D (q  0) = 0 D +ve cs c -ve Increasingly unfavourable interactions

Linear stability analysis Neglect the dynamics of stress evolution Deff < 0  growth of fluctuations Define stability by Deff = 0 stability only affected for non-zero Normal forces Deff depends on intrinsic dynamics thermodynamics stress variation with composition

Fluctuations: Polymer Solutions A. Onuki, S.T. Milner direction of shear x y z Fluctuations in the z direction are suppressed  shear induced mixing Fluctuations in the y direction are enhanced  shear induced de-mixing

Why strong directional dependence? Stress balance flow gradient direction shear stress constant shear rate must vary with composition vorticity direction shear stress can vary shear rate constant N1 increases as f2 opposes fluctuations in z direction in y direction shear rate variations dominate and favour fluctuations

Fluctuations: Blends direction of shear x y z Fluctuations in the z direction are suppressed or enhanced  shear induced mixing or demixing Fluctuations in the y direction are enhanced or suppressed  shear induced de-mixing or mixing

Temperature effects: closed-loops No shear Generally tA/tB has a complex dependence on temperature due to glass transition temperature differences between components Temperature 5s-1 polyethylene-co-vinyl acetate / solution chlorinated polyethylene

Beyond stability analysis Scattering as a more demanding test of theory scattering patterns can be measured in a steady state Significant advances in our understanding of the dynamics of miscible polymer blends in the past 10 years near quantitative constitutive equations that include concentration dependence of friction coefficients

Arbitrary stress relaxation function for blend Blend rheology data Arbitrary stress relaxation function for blend Prediction of steady state scattering Improved theory Predictive tools for phase transitions and microstructure evolution

Summary In polymer blends Scattering patterns possible to induce mixing or de-mixing in both the shear gradient and the vorticity directions quantitative description elusive Scattering patterns Polymer solutions e.g., qualitative agreement with experimental results (Hashimoto et al) for oscillatory shear Miscible polymer blends with viscosity difference a quantitative test of stress gradient contributions to stability ?