PhD student at Centre de Recherche Paul-Pascal, Pessac Research Directors: Patrick SNABRE and Bernard POULIGNY

Size: px
Start display at page:

Download "PhD student at Centre de Recherche Paul-Pascal, Pessac Research Directors: Patrick SNABRE and Bernard POULIGNY"

Transcription

1 PhD student at Centre de Recherche Paul-Pascal, Pessac Research Directors: Patrick SNABRE and Bernard POULIGNY

2 Our motivation Monodisperse system Basic models for granular systems are 2D and monodisperse particles. Polydisperse system Shear Shear A large number of experimental work dedicated to density matched cases. Most of the experiment in the Couette flow do not take into account secondary flows(piv and MRI). Parralel disk geometry Convection & segregation PMMA 30µm (1%) Polydispersity plays a huge role upon transport phenomena(size segregation).

3 Our model granular system and shear cell. Sample and Couette cell Spheres of Polymethyl methacrylate (PMMA) and a mixture of Hexadecane and Immersion Oil. Sample polydospersity PMMA diameter is between µm Particles and fluid are index matched. PMMA: n=1.48; r =1.18 g.cm -3 Immersion fluid: n=1.48; r =0.88 g.cm -3 Optical microscopy 100µm Difference in density results in particle settling. Couette cell: Inner Cylinder Radius : 15 mm Outer Cylinder Radius : 20 mm Bottom gap : 1.5mm Angular velocities up to 5.7 rad/s Investigation Strategy Scanning Electron Microscopy Single Particle Tracking (SPT) Particle Trajectography

4 Single Particle Tracking (SPT) Following a single fluorescent particle Single Particle Tracking Setup Two independent cameras for particle tracking Autofocus based on astigmatic system I m special, I m the tracer Too far In focus Too near O. Blaj et al. Euromech. Fluid Mechanics Conference-8, Bad Reichenhall, September (2010)

5 Single Particle Tracking (SPT) Results Sample Tracer 2aT=100µm + 2aT=200µm 2a0=200µm

6 Single Particle Tracking (SPT) Results Sample Tracer 2aT=100µm + 2aT=200µm 2a0=200µm

7 Single Particle Tracking (SPT) Results Sample 2a0=200µm + Tracer 2aT=100µm 2aT=200µm 2aT=600µm Primary Flow: Short time fluctuations. Particles migration under shear. Secondary Flow: Shear-induced self diffusion. Particles collision are responsable for diffusion. Particle size secondary motion dependence. t ~ 8h t ~ 26h t ~ 3h

8 Particles Trajectography Trajectography Setup Particles trajectories Autocorrelation Trajectography movie. Inner cylinder rotation 0.57 rad/s Data analisys. ROI deformation. Red arrow velocity; green - fluctuations Slope and grey level variation along the brightest line

9 Particles Trajectography Results migration Outer Cylinder Inner Cylinder Trajectography results (fluorescent fluid) Normalized Velocity Map 1 Active Quasistatic 0 Velocity profile at 10mm for a angular velocity of rad/s Two zones were observed in Couette flow: Active close to inner cylinder Quasistatic close to the outer cylinder Before shearing After shearing R.P. Behringer Border separation depends on altitude and shear rate In presence of shear, particles tend to accumulate outwards, i.e. from inner to outer cylinder (migration)

10 Particles Trajectography Results z=10mm Slip close to the inner cylinder depends upon the shear rate and altitude (concentration) Fluctuations are maximum at about 2 particle diameters. Slow exponential decay of the velocity fluctuations (Patrick s report) z=15mm z=20mm

11 Particles Trajectography Results z=10mm Slip close to the inner cylinder depends upon the shear rate and altitude (concentration) Fluctuations are maximum at about 2 particle diameters. Slow exponential decay of the velocity fluctuations (Patrick s report) z=15mm z=20mm Ω = rad/s Ω = rad/s

12 Gather Results From Single Particle Tracking Experiment: - 3D trajectories of fluorescent tracers recorded in automated contra-rotation mode. -Evidence of localization and recirculation flows in the active zone. Recirculation ~ 0.01 primary flow. - Different secondary flow for different tracers size. From Particle Trajectography Experiment: - Different velocity profiles as a function of altitude. - Slip dependence upon Ω and z (due to concentration gradients in both θ and z plane) - Particle fluctuations - Azimuthal fluctuation versus local concentration

13 In Progress Inner cylinder rotation rad/s Big vs. Smalls Small vs. Bigs 2aT=100µm 2aT=200µm 2aT=600µm

14

Flow and viscous resuspension of a model granular paste in a large gap Couette cell

Flow and viscous resuspension of a model granular paste in a large gap Couette cell Flow and viscous resuspension of a model granular paste in a large gap Couette cell Résumé : O. BLAJ a,c, P. SNABRE a, S. WIEDERSEINER b, C. ANCEY b and B. POULIGNY a a. Centre de Recherche Paul-Pascal

More information

The flow of a very concentrated slurry in a parallel-plate device: influence of gravity

The flow of a very concentrated slurry in a parallel-plate device: influence of gravity The flow of a very concentrated slurry in a parallel-plate device: influence of gravity Marie Lenoble, Patrick Snabre and Bernard Pouligny Centre de recherche Paul-Pascal, CNRS, av. A. Schweitzer, 33600

More information

The Counter Rotating Cone-Plate Shear Cell

The Counter Rotating Cone-Plate Shear Cell 2 The Counter Rotating Cone-Plate Shear Cell Abstract We report on novel possibilities to study colloidal suspensions in a steady shear field in real space. Fluorescence confocal microscopy is combined

More information

Supplementary table I. Table of contact angles of the different solutions on the surfaces used here. Supplementary Notes

Supplementary table I. Table of contact angles of the different solutions on the surfaces used here. Supplementary Notes 1 Supplementary Figure 1. Sketch of the experimental setup (not to scale) : it consists of a thin mylar sheet (0, 02 4 3cm 3 ) held fixed vertically. The spacing y 0 between the glass plate and the upper

More information

CENG 501 Examination Problem: Estimation of Viscosity with a Falling - Cylinder Viscometer

CENG 501 Examination Problem: Estimation of Viscosity with a Falling - Cylinder Viscometer CENG 501 Examination Problem: Estimation of Viscosity with a Falling - Cylinder Viscometer You are assigned to design a fallingcylinder viscometer to measure the viscosity of Newtonian liquids. A schematic

More information

Fuel Tracer Laser Induced Fluorescence for Droplet Liquid Vapor Visualization

Fuel Tracer Laser Induced Fluorescence for Droplet Liquid Vapor Visualization Fuel Tracer Laser Induced Fluorescence for Droplet Liquid Vapor Visualization Presenter: Keisuke Sato Mentor: Dr. Terrence Meyer 1 Motivation Combustor inside engine Droplet & Vapor cloud Vapor cloud Droplet

More information

J. Matthew Treinen & Justin Jacobs. Paterson & Cooke USA, 221 Corporate Circle Suite D, Golden CO, 80401, USA.

J. Matthew Treinen & Justin Jacobs. Paterson & Cooke USA, 221 Corporate Circle Suite D, Golden CO, 80401, USA. ISBN 978-83-927084-8-3 ISSN 0867-7964 THE APPLICABILITY OF THE EULERIAN-EULERIAN CFD APPROACH USING GRANULAR KINETIC THEORY TO PREDICT PARTICLE SETTLING AND MIGRATION IN VISCOPLASTIC FLUIDS J. Matthew

More information

Experimental setup. Chapter Rheometer

Experimental setup. Chapter Rheometer 21 Chapter 2 Experimental setup The current experiments are designed to examine the effect of volume fraction and Stokes number (and equivalently the Reynolds number) at shear rates sufficiently high enough

More information

Lecture PowerPoints. Chapter 10 Physics for Scientists and Engineers, with Modern Physics, 4 th edition Giancoli

Lecture PowerPoints. Chapter 10 Physics for Scientists and Engineers, with Modern Physics, 4 th edition Giancoli Lecture PowerPoints Chapter 10 Physics for Scientists and Engineers, with Modern Physics, 4 th edition Giancoli 2009 Pearson Education, Inc. This work is protected by United States copyright laws and is

More information

Rheology of concentrated hard-sphere suspensions

Rheology of concentrated hard-sphere suspensions Rheology of concentrated hard-sphere suspensions Complex behaviour in a simple system Wilson Poon School of Physics & Astronomy, The University of Edinburgh Rut Besseling Lucio Isa ( ETH, Zürich) Khoa

More information

Separation of Chiral Particles in Shear Flow

Separation of Chiral Particles in Shear Flow Separation of Chiral Particles in Shear Flow Johannes Jansson, Brian McMahon, Christian Reitz, William Savoie School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332-0430 (Dated: December

More information

Statistical Analysis of the Effect of Small Fluctuations on Final Modes Found in Flows between Rotating Cylinders

Statistical Analysis of the Effect of Small Fluctuations on Final Modes Found in Flows between Rotating Cylinders Statistical Analysis of the Effect of Small Fluctuations on Final Modes Found in Flows between Rotating Cylinders Toshiki Morita 1, Takashi Watanabe 2 and Yorinobu Toya 3 1. Graduate School of Information

More information

Tuesday, September 29, Page 453. Problem 5

Tuesday, September 29, Page 453. Problem 5 Tuesday, September 9, 15 Page 5 Problem 5 Problem. Set up and evaluate the integral that gives the volume of the solid formed by revolving the region bounded by y = x, y = x 5 about the x-axis. Solution.

More information

7.1 Describing Circular and Rotational Motion.notebook November 03, 2017

7.1 Describing Circular and Rotational Motion.notebook November 03, 2017 Describing Circular and Rotational Motion Rotational motion is the motion of objects that spin about an axis. Section 7.1 Describing Circular and Rotational Motion We use the angle θ from the positive

More information

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.685 Electric Machines Problem Set 10 Issued November 11, 2013 Due November 20, 2013 Problem 1: Permanent

More information

REE Internal Fluid Flow Sheet 2 - Solution Fundamentals of Fluid Mechanics

REE Internal Fluid Flow Sheet 2 - Solution Fundamentals of Fluid Mechanics REE 307 - Internal Fluid Flow Sheet 2 - Solution Fundamentals of Fluid Mechanics 1. Is the following flows physically possible, that is, satisfy the continuity equation? Substitute the expressions for

More information

Measurement of wakefields in hollow plasma channels Carl A. Lindstrøm (University of Oslo)

Measurement of wakefields in hollow plasma channels Carl A. Lindstrøm (University of Oslo) Measurement of wakefields in hollow plasma channels Carl A. Lindstrøm (University of Oslo) in collaboration with Spencer Gessner (CERN) presented by Erik Adli (University of Oslo) FACET-II Science Workshop

More information

Performance evaluation of different model mixers by numerical simulation

Performance evaluation of different model mixers by numerical simulation Journal of Food Engineering 71 (2005) 295 303 www.elsevier.com/locate/jfoodeng Performance evaluation of different model mixers by numerical simulation Chenxu Yu, Sundaram Gunasekaran * Food and Bioprocess

More information

1.060 Engineering Mechanics II Spring Problem Set 3

1.060 Engineering Mechanics II Spring Problem Set 3 1.060 Engineering Mechanics II Spring 2006 Due on Monday, March 6th Problem Set 3 Important note: Please start a new sheet of paper for each problem in the problem set. Write the names of the group members

More information

Curvilinear flows of noncolloidal suspensions: The role of normal stresses

Curvilinear flows of noncolloidal suspensions: The role of normal stresses Curvilinear flows of noncolloidal suspensions: The role of normal stresses Jeffrey F. Morris a) and Fabienne Boulay b) School of Chemical Engineering, Georgia Institute of Technology, Atlanta, Georgia

More information

Single Molecule Electrochemistry on a Porous Silica-Coated Electrode

Single Molecule Electrochemistry on a Porous Silica-Coated Electrode Supporting information for Single Molecule Electrochemistry on a Porous Silica-Coated Electrode Jin Lu, Yunshan Fan, Marco Howard, Joshua C. Vaughan, and Bo Zhang* Department of Chemistry, University of

More information

Particles, drops, and bubbles. Lecture 3

Particles, drops, and bubbles. Lecture 3 Particles, drops, and bubbles Lecture 3 Brownian Motion is diffusion The Einstein relation between particle size and its diffusion coefficient is: D = kt 6πηa However gravitational sedimentation tends

More information

Hands-on table-top science

Hands-on table-top science Hands-on table-top science Harry L. Swinney University of Texas fluid convection bacterial colony chemical pattern daffodil 5 cm A special thanks to the students and postdocs at U. Texas who did this work

More information

Application of Binary Sequences to Problems of Chaos

Application of Binary Sequences to Problems of Chaos Application of Binary Sequences to Problems of Chaos P. Singh, P. Mohr, D.D. Joseph Department of Aerospace Engineering and Mechanics, University of Minnesota 107 Akerman Hall, Minneapolis, M 55455 ABSTRACT

More information

Astronomy 310/510: Lecture 2: In stars, hydrostatic equilbrium means pressure out cancels gravity in.

Astronomy 310/510: Lecture 2: In stars, hydrostatic equilbrium means pressure out cancels gravity in. Astronomy 310/510: Lecture 2: Newton s laws, his second law in particular: F = ma. If a = 0, then no net forces act. In stars, hydrostatic equilbrium means pressure out cancels gravity in. When pressure

More information

Introduction to Dynamic Light Scattering for Particle Size Determination

Introduction to Dynamic Light Scattering for Particle Size Determination www.horiba.com/us/particle Jeffrey Bodycomb, Ph.D. Introduction to Dynamic Light Scattering for Particle Size Determination 2016 HORIBA, Ltd. All rights reserved. 1 Sizing Techniques 0.001 0.01 0.1 1 10

More information

(2.1) Is often expressed using a dimensionless drag coefficient:

(2.1) Is often expressed using a dimensionless drag coefficient: 1. Introduction Multiphase materials occur in many fields of natural and engineering science, industry, and daily life. Biological materials such as blood or cell suspensions, pharmaceutical or food products,

More information

Pattern Formation in a Rotating Aqueous Suspension arxiv:cond-mat/ v3 [cond-mat.soft] 13 Feb 2003

Pattern Formation in a Rotating Aqueous Suspension arxiv:cond-mat/ v3 [cond-mat.soft] 13 Feb 2003 Europhysics Letters PREPRINT Pattern Formation in a Rotating Aqueous Suspension arxiv:cond-mat/373v3 [cond-mat.soft] 3 Feb 3 A. P. J. Breu, C. A. Kruelle and I. Rehberg Experimentalphysik V, Universität

More information

Mixing by piecewise isometry in granular media

Mixing by piecewise isometry in granular media in granular media Department of Mathematics University of Leeds PANDA, 16 September 2008 Leeds Joint work with Steve Meier, Julio Ottino, Northwestern Steve Wiggins, University of Bristol Mixing Mixing

More information

Measuring Particle Mass and Other Properties with the Couette Centrifugal Particle Mass Analyzer

Measuring Particle Mass and Other Properties with the Couette Centrifugal Particle Mass Analyzer Measuring Particle Mass and Other Properties with the Couette Centrifugal Particle Mass Analyzer Jason Olfert & Nick Collings Cambridge University Engineering Department May 2006 Outline Introduction Description

More information

A discrete element model for simulation of a spinning disc fertilizer spreader

A discrete element model for simulation of a spinning disc fertilizer spreader A discrete element model for simulation of a spinning disc fertilizer spreader P. Van Liedekerke; E. Tijskens; E. Dintwa; H. Ramon Departement of Agro-engineering and Economics, K.U.Leuven, Kasteelpark

More information

Gold-poly(N-isopropylacrylamide) core-shell colloids with homogeneous density profiles: A small angle scattering study

Gold-poly(N-isopropylacrylamide) core-shell colloids with homogeneous density profiles: A small angle scattering study Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2014 Supporting Information Gold-poly(N-isopropylacrylamide) core-shell colloids with

More information

Exercise: concepts from chapter 10

Exercise: concepts from chapter 10 Reading:, Ch 10 1) The flow of magma with a viscosity as great as 10 10 Pa s, let alone that of rock with a viscosity of 10 20 Pa s, is difficult to comprehend because our common eperience is with s like

More information

The role of micro-scale inertia in transport processes. - Ganesh Subramanian (JNCASR, Bangalore)

The role of micro-scale inertia in transport processes. - Ganesh Subramanian (JNCASR, Bangalore) The role of micro-scale inertia in transport processes - Ganesh Subramanian (JNCASR, Bangalore) Micro-scale inertia (suspensions and emulsions) Navier-Stokes equations : Re u t + Re u u = Inertial acceleration

More information

( u,v). For simplicity, the density is considered to be a constant, denoted by ρ 0

( u,v). For simplicity, the density is considered to be a constant, denoted by ρ 0 ! Revised Friday, April 19, 2013! 1 Inertial Stability and Instability David Randall Introduction Inertial stability and instability are relevant to the atmosphere and ocean, and also in other contexts

More information

Linear shear of two dimensional foams

Linear shear of two dimensional foams Chapter 2 Linear shear of two dimensional foams In this chapter, we first review recent research on the rheology of two dimensional foams. We then describe experiments to unravel the connection between

More information

Table of Contents. Foreword... xiii. Preface... xv

Table of Contents. Foreword... xiii. Preface... xv Table of Contents Foreword.... xiii Preface... xv Chapter 1. Fundamental Equations, Dimensionless Numbers... 1 1.1. Fundamental equations... 1 1.1.1. Local equations... 1 1.1.2. Integral conservation equations...

More information

)WILEY A John Wiley and Sons, Ltd., Publication. Introduction to Biological Physics for the Health and Life Sciences

)WILEY A John Wiley and Sons, Ltd., Publication. Introduction to Biological Physics for the Health and Life Sciences to Biological Physics for the Health and Life Sciences Kirsten Franklin Paul Muir Terry Scott Lara Wilcocks Paul Yates Staff at the University of Otago, New Zealand i )WILEY A John Wiley and Sons, Ltd.,

More information

Entropic Crystal-Crystal Transitions of Brownian Squares K. Zhao, R. Bruinsma, and T.G. Mason

Entropic Crystal-Crystal Transitions of Brownian Squares K. Zhao, R. Bruinsma, and T.G. Mason Entropic Crystal-Crystal Transitions of Brownian Squares K. Zhao, R. Bruinsma, and T.G. Mason This supplementary material contains the following sections: image processing methods, measurements of Brownian

More information

Momentum transport from magnetic reconnection in laboratory an. plasmas. Fatima Ebrahimi

Momentum transport from magnetic reconnection in laboratory an. plasmas. Fatima Ebrahimi Momentum transport from magnetic reconnection in laboratory and astrophysical plasmas Space Science Center - University of New Hampshire collaborators : V. Mirnov, S. Prager, D. Schnack, C. Sovinec Center

More information

Study on Non-Uniqueness of Taylor Vortex Flow Changing Inner Cylinder Acceleration Time

Study on Non-Uniqueness of Taylor Vortex Flow Changing Inner Cylinder Acceleration Time World Journal of Mechanics, 2018, 8, 301-310 http://www.scirp.org/journal/wjm ISSN Online: 2160-0503 ISSN Print: 2160-049X Study on Non-Uniqueness of Taylor Vortex Flow Changing Inner Cylinder Acceleration

More information

Chaotic Advection in a Blinking Vortex Flow

Chaotic Advection in a Blinking Vortex Flow PHY492: Final Report Chaotic Advection in a Blinking Vortex Flow Rohan Isaac May 2, 2013 Fluid Dynamics Advection is the transport of substance by a fluid due to its motion. It differs from convection

More information

E. not enough information given to decide

E. not enough information given to decide Q22.1 A spherical Gaussian surface (#1) encloses and is centered on a point charge +q. A second spherical Gaussian surface (#2) of the same size also encloses the charge but is not centered on it. Compared

More information

DYNAMO THEORY: THE PROBLEM OF THE GEODYNAMO PRESENTED BY: RAMANDEEP GILL

DYNAMO THEORY: THE PROBLEM OF THE GEODYNAMO PRESENTED BY: RAMANDEEP GILL DYNAMO THEORY: THE PROBLEM OF THE GEODYNAMO PRESENTED BY: RAMANDEEP GILL MAGNETIC FIELD OF THE EARTH DIPOLE Field Structure Permanent magnetization of Core? 80% of field is dipole 20 % is non dipole 2)

More information

Description: Supplementary Figures, Supplementary Methods, and Supplementary References

Description: Supplementary Figures, Supplementary Methods, and Supplementary References File Name: Supplementary Information Description: Supplementary Figures, Supplementary Methods, and Supplementary References File Name: Supplementary Movie 1 Description: Footage of time trace of seeds

More information

) = slugs/ft 3. ) = lb ft/s. ) = ft/s

) = slugs/ft 3. ) = lb ft/s. ) = ft/s 1. Make use of Tables 1. in the text book (See the last page in this assignent) to express the following quantities in SI units: (a) 10. in./in, (b) 4.81 slugs, (c).0 lb, (d) 7.1 ft/s, (e) 0.04 lb s/ft.

More information

Rotational Motion. Rotational Motion. Rotational Motion

Rotational Motion. Rotational Motion. Rotational Motion I. Rotational Kinematics II. Rotational Dynamics (Netwton s Law for Rotation) III. Angular Momentum Conservation 1. Remember how Newton s Laws for translational motion were studied: 1. Kinematics (x =

More information

Lecture 19. ROLLING WITHOUT SLIPPING. Figure 4.8 Gear rolling in geared horizontal guides. Figure 4.9 Wheel rolling on a horizontal surface.

Lecture 19. ROLLING WITHOUT SLIPPING. Figure 4.8 Gear rolling in geared horizontal guides. Figure 4.9 Wheel rolling on a horizontal surface. Lecture 19. ROLLING WITHOUT SLIPPING Figure 4.8 Gear rolling in geared horizontal guides. Figure 4.9 Wheel rolling on a horizontal surface. The derivation and understanding of velocity and acceleration

More information

Digital Holographic Measurement of Nanometric Optical Excitation on Soft Matter by Optical Pressure and Photothermal Interactions

Digital Holographic Measurement of Nanometric Optical Excitation on Soft Matter by Optical Pressure and Photothermal Interactions Ph.D. Dissertation Defense September 5, 2012 Digital Holographic Measurement of Nanometric Optical Excitation on Soft Matter by Optical Pressure and Photothermal Interactions David C. Clark Digital Holography

More information

Numerical Simulation of the Hagemann Entrainment Experiments

Numerical Simulation of the Hagemann Entrainment Experiments CCC Annual Report UIUC, August 14, 2013 Numerical Simulation of the Hagemann Entrainment Experiments Kenneth Swartz (BSME Student) Lance C. Hibbeler (Ph.D. Student) Department of Mechanical Science & Engineering

More information

COMSOL Conference 2015 Boston Session: Computational Fluid Dynamics

COMSOL Conference 2015 Boston Session: Computational Fluid Dynamics COMSOL Conference 2015 Boston Session: Computational Fluid Dynamics Boston Marriot Newton Charles River West Boston, MA 1:00 pm-2:45 pm October 8 th, 2015. Fluid Motion Between Rotating Concentric Cylinders

More information

Experimental test of an expression for the decay of an autocorrelation function

Experimental test of an expression for the decay of an autocorrelation function Supplemental Material for: Experimental test of an expression for the decay of an autocorrelation function Journal: Physical Review Letters Authors: Zach Haralson and J. Goree I. Experimental setup The

More information

Hydrodynamic Electrodes and Microelectrodes

Hydrodynamic Electrodes and Microelectrodes CHEM465/865, 2004-3, Lecture 20, 27 th Sep., 2004 Hydrodynamic Electrodes and Microelectrodes So far we have been considering processes at planar electrodes. We have focused on the interplay of diffusion

More information

Vortices in accretion discs: formation process and dynamical evolution

Vortices in accretion discs: formation process and dynamical evolution Vortices in accretion discs: formation process and dynamical evolution Geoffroy Lesur DAMTP (Cambridge UK) LAOG (Grenoble) John Papaloizou Sijme-Jan Paardekooper Giant vortex in Naruto straight (Japan)

More information

A velocity of 5 m s 1 can be resolved along perpendicular directions XY and XZ.

A velocity of 5 m s 1 can be resolved along perpendicular directions XY and XZ. T1 [154 marks] 1. A velocity of 5 m s 1 can be resolved along perpendicular directions XY and XZ. The component of the velocity in the direction XY is of magnitude 4 m s 1. What is the magnitude of the

More information

Rotational viscometers

Rotational viscometers 42 Non-Newtonian Flow in the Process Industries Rotational viscometers Due to their relative importance as tools for the rheological characterisation of non-newtonian fluid behaviour, we concentrate on

More information

Physics Education Centre EXAMINATION. PHYS2016_Semester 2 Electromagnetism

Physics Education Centre EXAMINATION. PHYS2016_Semester 2 Electromagnetism Venue Student Number Physics Education Centre EXAMINATION This paper is for ANU students. Examination Duration: Reading Time: 180 minutes 15 minutes Exam Conditions: Central Examination Students must return

More information

Measuring shear-induced self-diffusion in a counterrotating geometry

Measuring shear-induced self-diffusion in a counterrotating geometry PHYSICAL REVIEW E, VOLUME 63, 021403 Measuring shear-induced self-diffusion in a counterrotating geometry Victor Breedveld,* Dirk van den Ende, Maarten Bosscher, Robert J. J. Jongschaap, and Jorrit Mellema

More information

Cuttings transport with drillstring rotation

Cuttings transport with drillstring rotation A-1 Cuttings transport with drillstring rotation Problem presented by Paul Bolchover Schlumberger Problem statement When an oil well is being drilled, rock cuttings are transported up to the surface by

More information

Modular Microscope Accessory

Modular Microscope Accessory Modular Microscope Accessory Modular Microscope Accessory SAMPLE STRUCTURE OBSERVATION DHR MMA Key Features Compact, modular design that directly installs to the DHR frame for easy alignment and minimal

More information

Introduction to Heat and Mass Transfer. Week 10

Introduction to Heat and Mass Transfer. Week 10 Introduction to Heat and Mass Transfer Week 10 Concentration Boundary Layer No concentration jump condition requires species adjacent to surface to have same concentration as at the surface Owing to concentration

More information

Applications in Biofluidics

Applications in Biofluidics Applications in Biofluidics Last Class: 1. Introduction of μpiv 2. Considerations of Microscopy in μpiv 3. Depth of Correlation 4. Physics of Particles in Micro PIV 5. Measurement Errors 6. Special Processing

More information

Supporting Information. Even Hard Sphere Colloidal Suspensions Display. Fickian yet Non-Gaussian Diffusion

Supporting Information. Even Hard Sphere Colloidal Suspensions Display. Fickian yet Non-Gaussian Diffusion Supporting Information Even Hard Sphere Colloidal Suspensions Display Fickian yet Non-Gaussian Diffusion Juan Guan, a Bo Wang, a and Steve Granick a,b,c,* Departments of Materials Science, a Chemistry,

More information

Practice Test 3. Name: Date: ID: A. Multiple Choice Identify the choice that best completes the statement or answers the question.

Practice Test 3. Name: Date: ID: A. Multiple Choice Identify the choice that best completes the statement or answers the question. Name: Date: _ Practice Test 3 Multiple Choice Identify the choice that best completes the statement or answers the question. 1. A wheel rotates about a fixed axis with an initial angular velocity of 20

More information

CHARACTERISING THE FAILURE AND REPOSE ANGLES OF IRREGULARLY SHAPED THREE-DIMENSIONAL PARTICLES USING DEM

CHARACTERISING THE FAILURE AND REPOSE ANGLES OF IRREGULARLY SHAPED THREE-DIMENSIONAL PARTICLES USING DEM Ninth International Conference on CFD in the Minerals and Process Industries CSIRO, Melbourne, Australia 10-12 December 2012 CHARACTERISING THE FAILURE AND REPOSE ANGLES OF IRREGULARLY SHAPED THREE-DIMENSIONAL

More information

5. 3P PIV Measurements

5. 3P PIV Measurements Micro PIV Last Class: 1. Data Validation 2. Vector Field Operator (Differentials & Integrals) 3. Standard Differential Scheme 4. Implementation of Differential & Integral quantities with PIV data 5. 3P

More information

Moving walls accelerate mixing

Moving walls accelerate mixing Moving walls accelerate mixing Jean-Luc Thiffeault Department of Mathematics University of Wisconsin Madison Uncovering Transport Barriers in Geophysical Flows Banff International Research Station, Alberta

More information

Turbulent Mixing of Passive Tracers on Small Scales in a Channel Flow

Turbulent Mixing of Passive Tracers on Small Scales in a Channel Flow Turbulent Mixing of Passive Tracers on Small Scales in a Channel Flow Victor Steinberg Department of Physics of Complex Systems, The Weizmann Institute of Science, Israel In collaboration with Y. Jun,

More information

Turbulence Model Affect on Heat Exchange Characteristics Through the Beam Window for European Spallation Source

Turbulence Model Affect on Heat Exchange Characteristics Through the Beam Window for European Spallation Source International Scientific Colloquium Modelling for Material Processing Riga, September 16-17, 2010 Turbulence Model Affect on Heat Exchange Characteristics Through the Beam Window for European Spallation

More information

Vector mechanics PHY1021: Jan 2011 exam- Hints and tips. Lecturer: Dr. Stavroula Foteinopoulou

Vector mechanics PHY1021: Jan 2011 exam- Hints and tips. Lecturer: Dr. Stavroula Foteinopoulou Vector mechanics PHY1021: Jan 2011 exam- Hints and tips Lecturer: Dr. Stavroula Foteinopoulou 1(i) W

More information

The Navier-Stokes equations for an incompressible fluid in indicial notation are. i u i = 0 (9.1)

The Navier-Stokes equations for an incompressible fluid in indicial notation are. i u i = 0 (9.1) Chapter 9 Viscous flow The Navier-Stokes equations for an incompressible fluid in indicial notation are i u i = 0 9.1 ρ t + u j j u i = i p + µ 2 j u i 9.2 When these are applied to practical problems,

More information

Flow in two-dimensions: novel fluid behavior at interfaces

Flow in two-dimensions: novel fluid behavior at interfaces Flow in two-dimensions: novel fluid behavior at interfaces M. Dennin U. C. Irvine Department of Physics and Astronomy and Institute for Surface and Interfacial Science Research Overview Fluid Instabilities

More information

Level 3 Physics, 2018

Level 3 Physics, 2018 91524 915240 3SUPERVISOR S Level 3 Physics, 2018 91524 Demonstrate understanding of mechanical systems 2.00 p.m. Tuesday 20 November 2018 Credits: Six Achievement Achievement with Merit Achievement with

More information

Supplementary Informations Spatial cooperativity in soft glassy flows

Supplementary Informations Spatial cooperativity in soft glassy flows doi:.38/nature76 Supplementary Informations Spatial cooperativity in soft glassy flows J. Goyon, A. Colin, G. Ovarlez, A. Ajdari, L. Bocquet I. SUPPLEMENTARY METHOD. Static properties of the emulsions

More information

elements remain in high frequency region and sometimes very large spike-shaped peaks appear. So we corrected the PIV time histories by peak cutting an

elements remain in high frequency region and sometimes very large spike-shaped peaks appear. So we corrected the PIV time histories by peak cutting an The Seventh International Colloquium on Bluff Body Aerodynamics and Applications (BBAA7) Shanghai, China; September 2-6, 2012 LES of fluctuating wind pressure on a 3D square cylinder for PIV-based inflow

More information

Turbulent Convection in Air

Turbulent Convection in Air SMR.1771-33 Conference and Euromech Colloquium #480 on High Rayleigh Number Convection 4-8 Sept., 2006, ICTP, Trieste, Italy ------------------------------------------------------------------------------------------------------------------------

More information

Winter Midterm Review Questions

Winter Midterm Review Questions Winter Midterm Review Questions PHYS106 February 24, 2008 PHYS106 () Winter Midterm Review Questions February 24, 2008 1 / 12 MassCenter003 Calculate the position of the mass center of the rigid system

More information

EFFECT OF CHANNEL BENDS ON TRANSVERSE MIXING

EFFECT OF CHANNEL BENDS ON TRANSVERSE MIXING NIJOTECH VOL. 10. NO. 1 SEPTEMBER 1986 ENGMANN 57 EFFECT OF CHANNEL BENDS ON TRANSVERSE MIXING BY E. O. ENGMANN ABSTRACT Velocity and tracer concentration measurements made in a meandering channel are

More information

The effective slip length and vortex formation in laminar flow over a rough surface

The effective slip length and vortex formation in laminar flow over a rough surface The effective slip length and vortex formation in laminar flow over a rough surface Anoosheh Niavarani and Nikolai V. Priezjev Movies and preprints @ http://www.egr.msu.edu/~niavaran A. Niavarani and N.V.

More information

Modelling of dispersed, multicomponent, multiphase flows in resource industries. Section 3: Examples of analyses conducted for Newtonian fluids

Modelling of dispersed, multicomponent, multiphase flows in resource industries. Section 3: Examples of analyses conducted for Newtonian fluids Modelling of dispersed, multicomponent, multiphase flows in resource industries Section 3: Examples of analyses conducted for Newtonian fluids Globex Julmester 017 Lecture # 04 July 017 Agenda Lecture

More information

Granular Experiments. Wolfgang Losert, Department of Physics University of Maryland

Granular Experiments. Wolfgang Losert, Department of Physics University of Maryland Summer School: Granular Materials from Simulations to Astrophysical Applications Hosted by CSCAMM and the University of Maryland Burgers Program in Fluid Dynamics Granular Experiments Wolfgang Losert,

More information

Supplementary material to On the rheology of pendular gels and morphological developments in paste- like ternary systems based on capillary attraction

Supplementary 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 information

Concentrated suspensions under flow in microfluidic channel and migration effect

Concentrated suspensions under flow in microfluidic channel and migration effect Mid-Term Review June 16-17 2011 Concentrated suspensions under flow in microfluidic channel and migration effect Florinda SCHEMBRI*, Hugues BODIGUEL, Annie COLIN LOF Laboratory of the Future University

More information

PHY 001 (Physics I) Lecture 7

PHY 001 (Physics I) Lecture 7 PHY 001 (Physics I) Instructor: Dr. Mohamed Fouad Salem mohamed.salem@gmail.com Textbook University Physics, 12 th edition, Young and Freedman Course Material Website http://meryesk.wordpress.com/phy001/

More information

ΣF = ma Στ = Iα ½mv 2 ½Iω 2. mv Iω

ΣF = ma Στ = Iα ½mv 2 ½Iω 2. mv Iω Thur Oct 22 Assign 9 Friday Today: Torques Angular Momentum x θ v ω a α F τ m I Roll without slipping: x = r Δθ v LINEAR = r ω a LINEAR = r α ΣF = ma Στ = Iα ½mv 2 ½Iω 2 I POINT = MR 2 I HOOP = MR 2 I

More information

Rigid Object. Chapter 10. Angular Position. Angular Position. A rigid object is one that is nondeformable

Rigid Object. Chapter 10. Angular Position. Angular Position. A rigid object is one that is nondeformable Rigid Object Chapter 10 Rotation of a Rigid Object about a Fixed Axis A rigid object is one that is nondeformable The relative locations of all particles making up the object remain constant All real objects

More information

Planet disk interaction

Planet disk interaction Planet disk interaction Wilhelm Kley Institut für Astronomie & Astrophysik & Kepler Center for Astro and Particle Physics Tübingen March 2015 4. Planet-Disk: Organisation Lecture overview: 4.1 Introduction

More information

Clément Surville, Lucio Mayer. Insitute for Computational Science, University of Zürich. Yann Alibert. Institute of Physics, University of Bern

Clément Surville, Lucio Mayer. Insitute for Computational Science, University of Zürich. Yann Alibert. Institute of Physics, University of Bern The code a multi-fluid method for the formation of primordial bodies in protoplanetary disks Carving through the Codes : Challenges in Computational Astrophysics Clément Surville, Lucio Mayer Insitute

More information

Chapter 10 Practice Test

Chapter 10 Practice Test Chapter 10 Practice Test 1. At t = 0, a wheel rotating about a fixed axis at a constant angular acceleration of 0.40 rad/s 2 has an angular velocity of 1.5 rad/s and an angular position of 2.3 rad. What

More information

Supporting Information

Supporting Information Supporting Information Wiley-VCH 2013 69451 Weinheim, Germany Colloidal Clusters by Using Emulsions and Dumbbell-Shaped Particles: Experiments and Simulations** Bo Peng,* Frank Smallenburg,* Arnout Imhof,

More information

Lecture 6 Physics 106 Spring 2006

Lecture 6 Physics 106 Spring 2006 Lecture 6 Physics 106 Spring 2006 Angular Momentum Rolling Angular Momentum: Definition: Angular Momentum for rotation System of particles: Torque: l = r m v sinφ l = I ω [kg m 2 /s] http://web.njit.edu/~sirenko/

More information

RHEOLOGY Principles, Measurements, and Applications. Christopher W. Macosko

RHEOLOGY 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 information

Big Idea 4: Interactions between systems can result in changes in those systems. Essential Knowledge 4.D.1: Torque, angular velocity, angular

Big Idea 4: Interactions between systems can result in changes in those systems. Essential Knowledge 4.D.1: Torque, angular velocity, angular Unit 7: Rotational Motion (angular kinematics, dynamics, momentum & energy) Name: Big Idea 3: The interactions of an object with other objects can be described by forces. Essential Knowledge 3.F.1: Only

More information

Questions on the December Assessment are broken into three categories: (Both MC and FR type questions can be in the following forms):

Questions on the December Assessment are broken into three categories: (Both MC and FR type questions can be in the following forms): December Assessment Review AP Physics C Mechanics Nuts and Bolts: Students will be provided an equation sheet and table of given values. Students should bring their own graphing calculator and a pencil.

More information

Physical & Interfacial Electrochemistry 2013.

Physical & Interfacial Electrochemistry 2013. Physical & Interfacial Electrochemistry 13. Lecture 8 Hydrodynamic Voltammetry Hydrodynamic voltammetry Hydrodynamic voltammetry deals with voltammetric measurements conducted under conditions where there

More information

Turbulent Rotating Rayleigh-Bénard Convection: DNS and SPIV Measurements

Turbulent Rotating Rayleigh-Bénard Convection: DNS and SPIV Measurements Turbulent Rotating Rayleigh-Bénard Convection: DNS and SPIV Measurements Rudie Kunnen 1 Herman Clercx 1,2 Bernard Geurts 1,2 1 Fluid Dynamics Laboratory, Department of Physics Eindhoven University of Technology

More information

ME 431A/538A/538B Homework 22 October 2018 Advanced Fluid Mechanics

ME 431A/538A/538B Homework 22 October 2018 Advanced Fluid Mechanics ME 431A/538A/538B Homework 22 October 2018 Advanced Fluid Mechanics For Friday, October 26 th Start reading the handout entitled Notes on finite-volume methods. Review Chapter 7 on Dimensional Analysis

More information

Stellar structure and evolution. Pierre Hily-Blant April 25, IPAG

Stellar structure and evolution. Pierre Hily-Blant April 25, IPAG Stellar structure and evolution Pierre Hily-Blant 2017-18 April 25, 2018 IPAG pierre.hily-blant@univ-grenoble-alpes.fr, OSUG-D/306 10 Protostars and Pre-Main-Sequence Stars 10.1. Introduction 10 Protostars

More information

Do not fill out the information below until instructed to do so! Name: Signature: Student ID: Section Number:

Do not fill out the information below until instructed to do so! Name: Signature: Student ID:   Section Number: Do not fill out the information below until instructed to do so! Name: Signature: Student ID: E-mail: Section Number: Formulae are provided on the last page. You may NOT use any other formula sheet. You

More information

LAMMPS Simulation of a Microgravity Shear Cell 299r Progress Report 2 Taiyo Wilson. Introduction:

LAMMPS Simulation of a Microgravity Shear Cell 299r Progress Report 2 Taiyo Wilson. Introduction: Introduction: After our initial simulations outlined in the first progress report, we determined that a shear cell with a bidisperse composition of particles would be a promising system to explore. However,

More information