Biomacormolecular Materials
|
|
- Ambrose Sanders
- 5 years ago
- Views:
Transcription
1 Sustainable Bioresource Sciences Biomacormolecular Materials There are close relationships between structures and properties of materials! Contents (1) Rheology property () Scattering (SAXS) structure Daisuke Tatsumi
2 The importance of boundary area especially important for Biomaterials Size from m to nm Research interests from fundamentals (raw materials) to application (industrial products)
3 Utilization of Cellulose Wood fiber assembly Scale Paper fiber re-assembly large Clothes cotton yarn rayon yarnregenerated Foods cocoa microcrystalline Nata de coco gel-like Industrial products Films paints molecular scale small
4 Papermaking c = 1 wt% c = 0 wt% paper c = 9 wt% wire press Wet-end dryer
5 Viscosity of suspensions Cellulose fiber log r 1 Sphere particles r =
6 Pulp fibers
7 Rheological measurements w Wet Pulp Mat C = 5~15 wt% Parallel -plates Rheometer
8 Rheometer Dynamic measurements stress strain strain ( t) exp[ iwt] 0 w * ( t) G 0 exp[ i( t )] ( ) ( w) * G G w ig t 8
9 Frequency dependence log ( G', G" / Pa ) Cellulose fiber web = 0.1% G' G" c / wt% log ( w / s -1 )
10 5 G = kc v 3 log ( G', G'' / Pa ) 4 3 G' G'' PFI mill / rev log ( c v / vol% )
11 LSCM Images mm
12 Microbial Cellulose(BC) pellicle
13 5 log ( G', G" / Pa ) 4 3 G' G" c / wt% log ( w / s -1 )
14 Viscoelastic properties of pellicle log( G', G" / Pa ) w = 0.1 s -1 G = kc 5 slope: 5 G' G" log( c / wt% )
15 Laminated Network Model Fiber D Lattice Model z d l
16 nd d c lz Pc P c lc d Length between Contact Points:
17 Stress transmission z L d l 1 dp dt : transmission efficiency
18 z vd v z L v L v: velocity of momentum When = 1 and /d >> 1, v z vd
19 4 z d l c v d v v G v z = d /lc Here, v = E f / f, l/d p, and f c, E f : Young s modulus of a fiber f : density of a fiber p: axial ratio : density
20 G E For BC pellicle f k p = 1 and /d >> 1 For pulp mat = c*/c c 5 log ( k / Pa ) 4 k p 3 1 slope: log ( p / - )
21 Microcrystalline Cellulose
22 log ( G', G'' / Pa ) Ceolus suspensions G G c (wt%) log ( w / s -1 )
23 log ( G', G" / Pa ) p (approx.) slope: 9/4 log ( c / wt% ) G' G" G = kc.5
24 Summary Pulp Fiber G = kc 3 BC Membrane G = kc 5 MCC G = kc 9/4 a: Network Structure k: Individual Fiber(= Ep )
25 Solution properties of celluloses derived from different origin
26 Cellulose from different origin Crystal structure of natural cellulose Ia Microbial Cellulose Ib Tunicate Cellulose J. Sugiyama, et al., Macromolecules 4, 4168 (1991).
27 Cellulose from different origin Solubility Celluloses 8wt% LiCl/DMAc Soluble Insoluble Tunicin (TC) Dissolving Pulp (DP) Cotton Cellulose (CC) (Isotropic) Microbial Cellulose (BC) (Anisotropic)
28 Liquid crystal from microbial cellulose Polarized microgram plant cellulose 13.6wt% microbial cellulose 13.7wt% 100mm Fiber from liquid crystal
29 Cellulose from Ascidians Halocynthia roretzi High spinnability of TC solution (0.5%)
30
31 Wide range Rubbery plateau G ' G" lim w0 w w G" w 1 0
32 log sp o C DP/DMAc DP/DMI CC/DMAc BC/DMAc TC/DMI log c[] Concentration dependence dilute solution sp c 1 semi-dilute soln. sp c 7.5 c 4 c 3 TC DP,CC BC
33 Critical concentration
34 Elementary particle?? R. P. Feynman t B A x
35 Future work for G = kc a Path Integral b i tb K b, a Dxt exp dtl x, x, t a t a b N P mp 1 1 Dxt exp b x x V x a i1 n1 b P i i n n n N Hamiltonian Harmonic Oscillation Percolation (with renormalization)
36 Progress of Science Induction Deduction Principle Results Experiment Explanation Hypothesis Experiment Francis Bacon René Descartes
37 Structural Analysis Microscope directly Light microscope, Electron microscope, Atomic force microscope Fourier Transform Scattering quantitative Light scattering, X-ray scattering, Neutron scattering
38 X-ray diffraction k k dsin n Laue condition a c b a (k k) = h b (k k) = k c (k k) = l
39 X-ray diffraction of cellulose
40 X-ray diffraction of cellulose TC 004 I / a.u. BC d110 d110 a b CC DP d / deg
41
42 Small angle X-ray scattering(saxs) small angle SPring-8 q k' k 4 sin
43 SAXS image for pellicle
44 particle size Guinier R q e g 3 particle morphology I q q q (6 D ) D m s Surface Fractal Mass Fractal slope: -4 particle surface specific surface area
45 log (I(q) / a.u.) SAXS image for cellulose liquid crystal 4 3 BC/LiCl DMAc 13.6 wt % Debye-Bueche Exp. DATA L d Correlation length a = 4.5 nm I( q ) K s 1 a q log (q / Å 1 )
46 京都市青少年科学センター蔵
47 REPORT: If you introduce rheology and/or SAXS to your own research, what progress is expected? with your impression
Determination of shape parameter of nanocrystalline cellulose rods
Determination of shape parameter of nanocrystalline cellulose rods Yaman Boluk and Liyan Zhao Cellulose and Hemicellulose Program Forest Products Alberta Research Council June 25, 2009 2009 International
More informationStructural characterization. Part 2
Structural characterization Part Determining partial pair distribution functions X-ray absorption spectroscopy (XAS). Atoms of different elements have absorption edges at different energies. Structure
More informationNon contact measurement of viscoelastic properties of biopolymers
Non contact measurement of viscoelastic properties of biopolymers Christelle Tisserand, Anton Kotzev, Mathias Fleury, Laurent Brunel, Pascal Bru, Gérard Meunier Formulaction, 10 impasse Borde Basse, 31240
More informationSOLID STATE 18. Reciprocal Space
SOLID STATE 8 Reciprocal Space Wave vectors and the concept of K-space can simplify the explanation of several properties of the solid state. They will be introduced to provide more information on diffraction
More informationENAS 606 : Polymer Physics
ENAS 606 : Polymer Physics Professor Description Course Topics TA Prerequisite Class Office Hours Chinedum Osuji 302 Mason Lab, 432-4357, chinedum.osuji@yale.edu This course covers the static and dynamic
More informationPolymerization Technology Laboratory Course
Polymerization Technology Laboratory Course Viscometry/Rheometry Tasks 1. Comparison of the flow behavior of polystyrene- solution and dispersion systems 2. Determination of the flow behaviour of polyvinylalcohol
More informationStructural characterization. Part 2
Structural characterization Part Scattering angle Crystalline materials Bragg s law: Scattering vector Q ~ d -1, where d is interplanar distance Q has dimension [m -1 ], hence large Q (large scattering
More informationLecture 7: Rheology and milli microfluidic
1 and milli microfluidic Introduction In this chapter, we come back to the notion of viscosity, introduced in its simplest form in the chapter 2. We saw that the deformation of a Newtonian fluid under
More informationA new interpretation for the dynamic behavior of complex fluids at the sol-gel transition using the fractional calculus
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
More informationAnalytical Methods for Materials
Analytical Methods for Materials Lesson 15 Reciprocal Lattices and Their Roles in Diffraction Studies Suggested Reading Chs. 2 and 6 in Tilley, Crystals and Crystal Structures, Wiley (2006) Ch. 6 M. DeGraef
More informationCharacterization of cellulose nanofibrils (CNF)
Characterization of cellulose nanofibrils (CNF) Ali Naderi Email: ali.naderi@innventia.com Tel: +46-(0)768767321 Cellulose nanofibril (CNF) Length several micrometers Width 100 nanometers www.innventia.com
More informationIntroduction to SAXS at SSRL
Everything You Ever Wanted to Know About Introduction to SAXS at SSRL SAXS But Were Afraid to Ask John A Pople Stanford Synchrotron Radiation Laboratory, Stanford Linear Accelerator Center, Stanford CA
More informationRheological Modelling of Polymeric Systems for Foods: Experiments and Simulations
Rheological Modelling of Polymeric Systems for Foods: Experiments and Simulations P.H.S. Santos a, M.A. Carignano b, O.H. Campanella a a Department of Agricultural and Biological Engineering, Purdue University,
More informationCHAPTER TWO: EXPERIMENTAL AND INSTRUMENTATION TECHNIQUES
CHAPTER TWO: EXPERIMENTAL AND INSTRUMENTATION TECHNIQUES 25 2.1 INSTRUMENTATION The prepared samples were characterized using various techniques. Among which are Dynamic Light Scattering, Zeta Potential
More informationChapter 6 Molten State
Chapter 6 Molten State Rheology ( 流變學 ) study of flow and deformation of (liquid) fluids constitutive (stress-strain) relation of fluids shear flow shear rate ~ dγ/dt ~ velocity gradient dv 1 = dx 1 /dt
More informationSmall Angle X-ray Scattering (SAXS)
Small Angle X-ray Scattering (SAXS) We have considered that Bragg's Law, d = λ/(2 sinθ), supports a minimum size of measurement of λ/2 in a diffraction experiment (limiting sphere of inverse space) but
More informationContents. Foreword by Darrell H. Reneker
Table of Foreword by Darrell H. Reneker Preface page xi xiii 1 Introduction 1 1.1 How big is a nanometer? 1 1.2 What is nanotechnology? 1 1.3 Historical development of nanotechnology 2 1.4 Classification
More informationAging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology
Aging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology Outline Laponite Basic background. Laponite in suspension Bonn et al.,
More informationFoundations of. Colloid Science SECOND EDITION. Robert J. Hunter. School of Chemistry University of Sydney OXPORD UNIVERSITY PRESS
Foundations of Colloid Science SECOND EDITION Robert J. Hunter School of Chemistry University of Sydney OXPORD UNIVERSITY PRESS CONTENTS 1 NATURE OF COLLOIDAL DISPERSIONS 1.1 Introduction 1 1.2 Technological
More informationMethoden moderner Röntgenphysik II Streuung und Abbildung
Methoden moderner Röntgenphysik II Streuung und Abbildung Stephan V. Roth DESY 1.5.15 Outline > 1.5. : Small-Angle X-ray Scattering (SAXS) > 19.5. : Applications & A short excursion into Polymeric materials
More informationEntanglements. M < M e. M > M e. Rouse. Zero-shear viscosity vs. M (note change of slope) Edwards degennes Doi. Berry + Fox, slope 3.4.
Entanglements Zero-shear viscosity vs. M (note change of slope) M < M e Rouse slope 3.4 M > M e Edwards degennes Doi slope 1 Berry + Fox, 1968 Question: Which factors affect the Me: T, P, M, flexibility,
More informationIntroduction to X-ray and neutron scattering
UNESCO/IUPAC Postgraduate Course in Polymer Science Lecture: Introduction to X-ray and neutron scattering Zhigunov Alexander Institute of Macromolecular Chemistry ASCR, Heyrovsky sq., Prague -16 06 http://www.imc.cas.cz/unesco/index.html
More informationElectrospinning of PVB Solved in Methanol and Isopropanol
Electrospinning of PVB Solved in Methanol and Isopropanol M. STENICKA 1,2, P. PEER-SVRCINOVA 3, P. FILIP 3, V. PAVLINEK 1,4, M. MACHOVSKY 1,4 1 Centre of Polymer Systems, University Institute Nad Ovcirnou
More informationViscoelasticity, Creep and Oscillation Experiment. Basic Seminar Applied Rheology
Viscoelasticity, Creep and Oscillation Experiment Basic Seminar Applied Rheology Overview Repetition of some basic terms Viscoelastic behavior Experimental approach to viscoelasticity Creep- and recovery
More informationOrigins of Mechanical and Rheological Properties of Polymer Nanocomposites. Venkat Ganesan
Department of Chemical Engineering University of Texas@Austin Origins of Mechanical and Rheological Properties of Polymer Nanocomposites Venkat Ganesan $$$: NSF DMR, Welch Foundation Megha Surve, Victor
More informationThermally Functional Liquid Crystal Networks by Magnetic Field Driven Molecular Orientation
Supporting information Thermally Functional Liquid Crystal Networks by Magnetic Field Driven Molecular Orientation Jungwoo Shin, Minjee Kang, Tsunghan Tsai, Cecilia Leal, Paul V. Braun and David G. Cahill*,
More informationMethoden Moderner Röntgenphysik II - Vorlesung im Haupt-/Masterstudiengang, Universität Hamburg, SoSe 2016, S. Roth
> 31.05. : Small-Angle X-ray Scattering (SAXS) > 0.06. : Applications & A short excursion into Polymeric materials > 04.06. : Grazing incidence SAXS (GISAXS) Methoden Moderner Röntgenphysik II - Vorlesung
More informationThe Small Angle X-ray Scattering Technique: An Overview
The Small Angle X-ray Scattering Technique: An Overview Dr. Gianluca Croce, Ph.D DISTA - Univ. Piemonte Orientale Via T. Michel 11,15121 Alessandria (Italy) gianluca.croce@mfn.unipmn.it Dr. Gianluca Croce
More informationRheology of Fluids: Newtonian to Non Newtonian
0/26 Rheology of Fluids: Newtonian to Non Newtonian Ali Najafi University of Zanjan, Zanjan Instituet for advanced Studies in Basic Sciences May 2015 1/26 Agenda: Fluid: Definition Rheology: Elementary
More informationViscoelasticity. Basic Notions & Examples. Formalism for Linear Viscoelasticity. Simple Models & Mechanical Analogies. Non-linear behavior
Viscoelasticity Basic Notions & Examples Formalism for Linear Viscoelasticity Simple Models & Mechanical Analogies Non-linear behavior Viscoelastic Behavior Generic Viscoelasticity: exhibition of both
More informationContents. Preface XIII. 1 General Introduction 1 References 6
VII Contents Preface XIII 1 General Introduction 1 References 6 2 Interparticle Interactions and Their Combination 7 2.1 Hard-Sphere Interaction 7 2.2 Soft or Electrostatic Interaction 7 2.3 Steric Interaction
More informationUnit I - Properties of Matter
Unit I - Properties of Matter Elasticity: Elastic and plastic materials Hooke s law elastic behavior of a material stress - strain diagram factors affecting elasticity. Three moduli of elasticity Poisson
More informationLecture 11 - Phonons II - Thermal Prop. Continued
Phonons II - hermal Properties - Continued (Kittel Ch. 5) Low High Outline Anharmonicity Crucial for hermal expansion other changes with pressure temperature Gruneisen Constant hermal Heat ransport Phonon
More informationSAS Data Analysis Colloids. Dr Karen Edler
SAS Data Analysis Colloids Dr Karen Edler Size Range Comparisons 10 1 0.1 0.01 0.001 proteins viruses nanoparticles micelles polymers Q = 2π/d (Å -1 ) bacteria molecules nanotubes precipitates grain boundaries
More informationModelling the Rheology of Semi-Concentrated Polymeric Composites
THALES Project No 1188 Modelling the Rheology of Semi-Concentrated Polymeric Composites Research Team Evan Mitsoulis (PI), Professor, NTUA, Greece Costas Papoulias (Research Student), NTUA, Greece Souzanna
More informationde Broglie Waves h p de Broglie argued Light exhibits both wave and particle properties
de Broglie argued de Broglie Waves Light exhibits both wave and particle properties Wave interference, diffraction Particle photoelectric effect, Compton effect Then matter (particles) should exhibit both
More informationRHEOLOGY Principles, Measurements, and Applications. Christopher W. Macosko
RHEOLOGY Principles, Measurements, and Applications I -56081-5'79~5 1994 VCH Publishers. Inc. New York Part I. CONSTITUTIVE RELATIONS 1 1 l Elastic Solid 5 1.1 Introduction 5 1.2 The Stress Tensor 8 1.2.1
More informationContents. Preface XIII
V Contents Preface XIII 1 General Introduction 1 1.1 Fundamental Knowledge Required for Successful Dispersion of Powders into Liquids 1 1.1.1 Wetting of Powder into Liquid 1 1.1.2 Breaking of Aggregates
More informationintroduction to SAXS for polymers -a user view-
introduction to SAXS for polymers -a user view- Luigi Balzano DSM Ahead/Material Science Center Geleen, The Netherlands luigi.balzano@dsm.com Synchrotron and Neutron Workshop (SyNeW) 2015 Utrecht, June
More informationMethoden moderner Röntgenphysik II Streuung und Abbildung
Methoden moderner Röntgenphysik II Streuung und Abbildung Stephan V. Roth DESY 5.6.14 Two phase Model single particle approximation > Amplitude: Δ 3 > Intensity: = > Closer look at Iq for dilute systems:
More informationThe Cellulose Nanocrystal Electro-optic optic Effect
The Cellulose Nanocrystal Electro-optic optic Effect Chad Teters,, Wei Kong, Melissa Taylor, John Simonsen, Mike Lerner, Tom Plant, Glenn Evans Oregon State University Corvallis, Oregon Presentation Overview
More informationLecture 2. Simple shear devices. Simple shear devices 2. Simple shear devices 3. Moving plate. Velocity V. Force F. Area A. height h.
Lecture 2 Rheometry Simple shear devices Steady shear viscosity Normal stresses Oscillating shear Extensional viscosity Scalings Nondimensional parameter Simple shear devices Conceptual device for simple
More informationUniversity of Alberta
University of Alberta An investigation on interaction between nano crystalline cellulose and watersoluble polymers in aqueous solutions by Zahra Khalili A thesis submitted to the Faculty of Graduate Studies
More informationRheology of cellulose solutions. Puu Cellulose Chemistry Michael Hummel
Rheology of cellulose solutions Puu-23.6080 - Cellulose Chemistry Michael Hummel Contents Steady shear tests Viscous flow behavior and viscosity Newton s law Shear thinning (and critical concentration)
More informationJetting of Isotropic Conductive Adhesives with Silver Coated Polymer Particles
Jetting of Isotropic Conductive Adhesives with Silver Coated Polymer Particles Gustaf Mårtensson 1,2 Kalland, Erik 3, Redford, Keith 3, Oppland, Ottar 5 1 Chalmers University of Technology, Göteborg, Sweden
More informationCONSISTENCY OF RHEOLOGICAL EXPERIMENTS FOR PSA CHARACTERIZATION
CONSISTENCY OF RHEOLOGICAL EXPERIMENTS FOR PSA CHARACTERIZATION Dr. Laura Yao, Senior Research Chemist, Scapa North America, Windsor, CT Robert Braiewa, Research Chemist, Scapa North America, Windsor,
More informationCritical Phenomena under Shear Flow
Critical Phenomena under Shear Flow Pavlik Lettinga, Hao Wang, Jan K.G. Dhont Close to a gas-liquid critical point, effective interactions between particles become very long ranged, and the dynamics of
More informationRheology of Soft Materials. Rheology
Τ Thomas G. Mason Department of Chemistry and Biochemistry Department of Physics and Astronomy California NanoSystems Institute Τ γ 26 by Thomas G. Mason All rights reserved. γ (t) τ (t) γ τ Δt 2π t γ
More informationInterfacial dynamics
Interfacial dynamics Interfacial dynamics = dynamic processes at fluid interfaces upon their deformation Interfacial rheological properties: elasticity, viscosity, yield stress, Relation between macroscopic
More informationIn situ Experiments in Material Science:
In situ Experiments in Material Science: Rheo-Saxs, Rheo-Dielectric, Rheo-NMR, In situ-nmr Prof. Dr. M. Wilhelm Institute of Chemical and Polymer Chemistry Manfred.Wilhelm@kit.edu Fourier Transform-Rheology
More informationOBTAINING MICROCRYSTALLINE CELLULOSE FROM SOFTWOOD AND HARDWOOD PULP
OBTAINING MICROCRYSTALLINE CELLULOSE FROM SOFTWOOD AND HARDWOOD PULP Marianna Laka,* and Svetlana Chernyavskaya Conditions for obtaining microcrystalline cellulose (MCC) by the thermocatalytic method from
More informationRHEOLOGICAL CHARACTERIZATION OF THERMOSETTING RES- IN SYSTEM WITH THERMOPLASTIC FUNCTIONAL LAYER
21 st International Conference on Composite Materials Xi an, 20-25 th August 2017 RHEOLOGICAL CHARACTERIZATION OF THERMOSETTING RES- IN SYSTEM WITH THERMOPLASTIC FUNCTIONAL LAYER W. Surjoseputro 1, G.
More informationNon-linear Viscoelasticity FINITE STRAIN EFFECTS IN SOLIDS
FINITE STRAIN EFFECTS IN SOLIDS Consider an elastic solid in shear: Shear Stress σ(γ) = Gγ If we apply a shear in the opposite direction: Shear Stress σ( γ) = Gγ = σ(γ) This means that the shear stress
More informationUltra Thin Films of Oriented Cellulose Nanocrystals by Electric Field Assisted Convective Assembly
2010 TAPPI Intl Conf. on Nano for the Forest Product Industry Ultra Thin Films of Oriented Cellulose Nanocrystals by Electric Field Assisted Convective Assembly L. Csoka, P. Peralta, I. Peszlen, I. Hoeger,
More information2. Diffraction as a means to determine crystal structure
2. Diffraction as a means to determine crystal structure Recall de Broglie matter waves: He atoms: [E (ev)] 1/2 = 0.14 / (Å) E 1Å = 0.0196 ev Neutrons: [E (ev)] 1/2 = 0.28 / (Å) E 1Å = 0.0784 ev Electrons:
More informationLecture contents. Stress and strain Deformation potential. NNSE 618 Lecture #23
1 Lecture contents Stress and strain Deformation potential Few concepts from linear elasticity theory : Stress and Strain 6 independent components 2 Stress = force/area ( 3x3 symmetric tensor! ) ij ji
More information1 Introduction Why the Interpretive Approach? (Niall W. G. Young).
1 Introduction Why the Interpretive Approach? (Niall W. G. Young). 1.1 Rheology What is in it for me? 1.1.1 Case study. 2 Viscosity and Oscillatory Rheology (Taghi Miri). 2.1 Introduction. 2.2 Food rheology.
More informationGeneral theory of diffraction
General theory of diffraction X-rays scatter off the charge density (r), neutrons scatter off the spin density. Coherent scattering (diffraction) creates the Fourier transform of (r) from real to reciprocal
More informationAbvanced Lab Course. Dynamical-Mechanical Analysis (DMA) of Polymers
Abvanced Lab Course Dynamical-Mechanical Analysis (DMA) of Polymers M211 As od: 9.4.213 Aim: Determination of the mechanical properties of a typical polymer under alternating load in the elastic range
More informationJetting of Isotropic Conductive Adhesives with Silver Coated Polymer Particles
Jetting of Isotropic Conductive Adhesives with Silver Coated Polymer Particles Gustaf Mårtensson 1,2 Kalland, Erik 3, Redford, Keith 3, Oppland, Ottar 5 1 Chalmers University of Technology, Göteborg, Sweden
More informationOne- and two-particle microrheology in solutions of actin, fd-virus and inorganic rods
Microrheology of Biopolymers (ITP Complex Fluids Program 3/05/02) One- and two-particle microrheology in solutions of actin, fd-virus and inorganic rods Christoph Schmidt Vrije Universiteit Amsterdam Collaborators:
More informationRHEOLOGICAL PROPERTIES OF CELLULOSE-NaOH COMPLEX SOLUTIONS: FROM DILUTE TO CONCENTRATED STATES
CELLULOSE CHEMISTRY AND TECHNOLOGY RHEOLOGICAL PROPERTIES OF CELLULOSE-NaOH COMPLEX SOLUTIONS: FROM DILUTE TO CONCENTRATED STATES SHUAI ZHANG, FA-XUE LI * and JIAN-YONG YU * Key Laboratory of Textile Science
More informationExperimental Study of the Induced Residual Stresses During the Manufacturing Process of an Aeronautic Composite Material
Research Journal of Applied Sciences, Engineering and Technology 2(6): 596-602, 2010 ISSN: 2040-7467 Maxwell Scientific Organization, 2010 Submitted Date: July 28, 2010 Accepted Date: August 27, 2010 Published
More informationSalt-induced Hydrogelation of Functionalised-Dipeptides at high ph
Salt-induced Hydrogelation of Functionalised-Dipeptides at high ph Lin Chen, a Guillaume Pont, a Kyle Morris, b Gudrun Lotze, c Adam Squires, c and Dave J. Adams a, * a Department of Chemistry, University
More informationOptical Imaging Chapter 5 Light Scattering
Optical Imaging Chapter 5 Light Scattering Gabriel Popescu University of Illinois at Urbana-Champaign Beckman Institute Quantitative Light Imaging Laboratory http://light.ece.uiuc.edu Principles of Optical
More informationRoger Johnson Structure and Dynamics: X-ray Diffraction Lecture 6
6.1. Summary In this Lecture we cover the theory of x-ray diffraction, which gives direct information about the atomic structure of crystals. In these experiments, the wavelength of the incident beam must
More informationCELLULOSE NANOWHISKER OBTAINED FROM COTTON REJECTED BY TEXTILE INDUSTRY
CELLULOSE NANOWHISKER OBTAINED FROM COTTON REJECTED BY TEXTILE INDUSTRY José Heriberto O. do Nascimento a,, Rodrigo F. Luz a, Felipe M.F. Galvão a, José Daniel D. Melo a, Fernando R. Oliveira a, Rasiah
More informationPolymer Dynamics and Rheology
Polymer Dynamics and Rheology 1 Polymer Dynamics and Rheology Brownian motion Harmonic Oscillator Damped harmonic oscillator Elastic dumbbell model Boltzmann superposition principle Rubber elasticity and
More informationStress Overshoot of Polymer Solutions at High Rates of Shear
Stress Overshoot of Polymer Solutions at High Rates of Shear K. OSAKI, T. INOUE, T. ISOMURA Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan Received 3 April 2000; revised
More informationSmall-angle X-ray scattering a (mostly) theoretical introduction to the basics
Small-angle X-ray scattering a (mostly) theoretical introduction to the basics András Wacha Research Centre for Natural Sciences, Hungarian Academy of Sciences Contents Introduction A bit of history The
More information2. Diffraction as a means to determine crystal structure
Page 1 of 22 2. Diffraction as a means to determine crystal structure Recall de Broglie matter waves: 2 p h E = where p = 2m λ h 1 E = ( ) 2m λ hc E = hυ = ( photons) λ ( matter wave) He atoms: [E (ev)]
More informationSoft matters end use properties analysis thanks to Microrheology
Soft matters end use properties analysis thanks to Microrheology Formulaction, 10 impasse Borde Basse, 31240 L Union, France, www.formulaction.com Abstract. We present a new technique of passive microrheology
More informationCoarse-grained materials properties for fiber-based materials from computer simulations
Coarse-grained materials properties for fiber-based materials from computer simulations Mikko Alava Aalto University, Department of Applied Physics, P.O. Box 14100, FIN-00076, FINLAND The understanding
More informationUncoupling shear and uniaxial elastic moduli of semiflexible biopolymer networks:
Supplemental document for: Uncoupling shear and uniaxial elastic moduli of semiflexible biopolymer networks: compression-softening and stretch-stiffening Anne S. G. van Oosten 1, Mahsa Vahabi 2, Albert
More informationLinearized Theory: Sound Waves
Linearized Theory: Sound Waves In the linearized limit, Λ iα becomes δ iα, and the distinction between the reference and target spaces effectively vanishes. K ij (q): Rigidity matrix Note c L = c T in
More informationExperimental Colloids I (and I)
Experimental Colloids I (and I) Dave Weitz Harvard http://www.seas.harvard.edu/projects/weitzlab Boulder Summer School 7/24/17 Experimental Colloids I (and I) Dave Weitz Harvard http://www.seas.harvard.edu/projects/weitzlab
More informationReview of Last Class 1
Review of Last Class 1 X-Ray diffraction of crystals: the Bragg formulation Condition of diffraction peak: 2dd sin θθ = nnλλ Review of Last Class 2 X-Ray diffraction of crystals: the Von Laue formulation
More informationET-105(A) : PHYSICS. Show that only an infinitesimal rotation can be regarded as a vector.
No. of Printed Pages : 7 ET-105(A) B.Tech. Civil (Construction Management) / B.Tech. Civil (Water Resources Engineering) / BTCLEVI / BTMEVI / BTELVI / BTECVI / BTCSVI Term-End Examination June, 2017 ET-105(A)
More informationSwelling of cellulose. Puu Cellulose Chemistry Michael Hummel
Swelling of cellulose Puu-23.6080 - Cellulose Chemistry Michael Hummel Content Swelling basics Fiber structure Swelling through different solvents Ballooning Nature s functional swelling 2 to swell become
More informationSupplementary material to On the rheology of pendular gels and morphological developments in paste- like ternary systems based on capillary attraction
Electronic Supplementary Material (ESI) for Soft Matter. This journal is The Royal Society of Chemistry 214 Supplementary material to On the rheology of pendular gels and morphological developments in
More informationAlain Dufresne. Nanocellulose. From Nature to High Performance Tailored Materials OE GRUYTER
Alain Dufresne Nanocellulose From Nature to High Performance Tailored Materials OE GRUYTER Contents Preface - vii 1 Cellulose and potential reinforcement-1 1.1 Polysaccharides-1 1.2 Chemical structure
More informationSupporting Information for:
Supporting Information for: "Rheological Link Between Polymer Melts with a High Molecular Weight Tail and Enhanced Formation of Shish-Kebabs" Sara Lindeblad Wingstrand, Bo Shen, Julie A. Korneld, Kell
More informationCHEMISTRY PHYSICAL. of FOODS INTRODUCTION TO THE. CRC Press. Translated by Jonathan Rhoades. Taylor & Francis Croup
Christos Ritzoulis Translated by Jonathan Rhoades INTRODUCTION TO THE PHYSICAL CHEMISTRY of FOODS CRC Press Taylor & Francis Croup Boca Raton London NewYork CRC Press is an imprint of the Taylor & Francis
More informationStructure analysis: Electron diffraction LEED TEM RHEED
Structure analysis: Electron diffraction LEED: Low Energy Electron Diffraction SPA-LEED: Spot Profile Analysis Low Energy Electron diffraction RHEED: Reflection High Energy Electron Diffraction TEM: Transmission
More informationAM11: Diagnostics for Measuring and Modelling Dispersion in Nanoparticulate Reinforced Polymers. Polymers: Multiscale Properties.
AM11: Diagnostics for Measuring and Modelling Dispersion in Nanoparticulate Reinforced Polymers Polymers: Multiscale Properties 8 November 2007 Aims Provide diagnostic tools for quantitative measurement
More informationTHE STRUCTURE OF CELLULOSES
138 THE STRUCTURE OF CELLULOSES Masahisa Wada, 1 Yoshiharu Nishiyama, 2 Henri Chanzy, 1 Trevor Forsyth, 3,4 and Paul Langan 5,6 1 Department of Biomaterials Science, Graduate School of Agriculture and
More informationShear rheology of polymer melts
Shear rheology of polymer melts Dino Ferri dino.ferri@versalis.eni.com Politecnico Alessandria di Milano, 14/06/2002 22 nd October 2014 Outline - Review of some basic rheological concepts (simple shear,
More informationA Technique for Characterizing Complex Polymer Solutions in Extensional Flows. Gavin Braithwaite Stephen Spiegelberg
A Technique for Characterizing Complex Polymer Solutions in Extensional Flows Gavin Braithwaite Stephen Spiegelberg Cambridge Polymer Group Inc. Ward Street, Somerville. MA 0243 http://www.campoly.com
More informationQuiz 1 Introduction to Polymers (Please answer each question even if you guess)
080407 Quiz 1 Introduction to Polymers (Please answer each question even if you guess) This week we explored the definition of a polymer in terms of properties. 1) The flow of polymer melts and concentrated
More informationA Brief Review of Two Theoretical Models Used to Interpret the SAXS Intensities Measurements in Heterogeneous Thin Films.
A Brief Review of Two Theoretical Models Used to Interpret the SAXS Intensities Measurements in Heterogeneous Thin Films. M. Cattani*, M. C. Salvadori and F. S. Teixeira Institute of Physics, University
More informationPharmaceutics I صيدالنيات 1. Unit 6
Pharmaceutics I صيدالنيات 1 Unit 6 1 Rheology of suspensions Rheology, the study of flow, addresses the viscosity characteristics of powders, fluids, and semisolids. Materials are divided into two general
More informationApplicability of Engineering Models in Multiscale Modeling of Natural Fiber Hygro- Elastic Properties
Applicability of Engineering Models in Multiscale Modeling of Natural Fiber Hygro- Elastic Properties Janis Varna and Eri Marlund Department of Applied Physics and Mechanical Engineering Where is Luleå?
More informationThe principals of rheology In pharmaceutical technology
The principals of rheology In pharmaceutical technology Dr. Aleksandar Széchenyi University of Pécs Gyógyszertechnológiai és Biofarmáciai Intézet Institute of Pharmaceutical Technology and Biopharmacy
More informationRheology, Adhesion, and Debonding of Lightly Cross-linked Polymer Gels
Rheology, Adhesion, and Debonding of Lightly Cross-linked Polymer Gels Nicholas B. Wyatt, and Anne M. Grillet 2 Materials Science and Engineering Division 2 Engineering Sciences Division Sandia National
More informationLecture 4. Donnan Potential
Lecture 4 Langmuir-Blodgett films II Langmuir Blodgett films. II. Donnan Potential Floating monolayers Generally, amphiphilic molecules adsorb on the liquid-air interface Insoluble amphiphiles can create
More informationViscoelastic Flows in Abrupt Contraction-Expansions
Viscoelastic Flows in Abrupt Contraction-Expansions I. Fluid Rheology extension. In this note (I of IV) we summarize the rheological properties of the test fluid in shear and The viscoelastic fluid consists
More informationMeasuring the rheology of polymer solutions
Measuring the rheology of polymer solutions John Duffy, Product Marketing Manager, Rheology RHEOLOGY AND VISCOSITY MICRORHEOLOGY Polymers are versatile materials that play an important role in a diverse
More informationPart 8. Special Topic: Light Scattering
Part 8. Special Topic: Light Scattering Light scattering occurs when polarizable particles in a sample are placed in the oscillating electric field of a beam of light. The varying field induces oscillating
More informationVISCOELASTIC PROPERTIES OF POLYMERS
VISCOELASTIC PROPERTIES OF POLYMERS John D. Ferry Professor of Chemistry University of Wisconsin THIRD EDITION JOHN WILEY & SONS New York Chichester Brisbane Toronto Singapore Contents 1. The Nature of
More informationCrystal Structure SOLID STATE PHYSICS. Lecture 5. A.H. Harker. thelecture thenextlecture. Physics and Astronomy UCL
Crystal Structure thelecture thenextlecture SOLID STATE PHYSICS Lecture 5 A.H. Harker Physics and Astronomy UCL Structure & Diffraction Crystal Diffraction (continued) 2.4 Experimental Methods Notes: examples
More information