Ch 11 Particulate suspensions

Similar documents
LECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12

Test 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.

ATMO 551a Fall 08. Diffusion

Formula Formula symbols Units. s = F A. e = x L. E = s ε. k = F δ. G = t γ. e = at. maximum load original cross sectional area. s M E = = N/m.

Force & Motion: Newton s Laws

Perhaps the greatest success of his theory of gravity was to successfully explain the motion of the heavens planets, moons, &tc.

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09

Mon , (.12) Rotational + Translational RE 11.b Tues.

Charged particle motion in magnetic field

Honors Classical Physics I

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the

Introduction to Dielectric Properties and Magnetism

FARADAY'S LAW dt

( ) rad ( 2.0 s) = 168 rad

SPH4U Magnetism Test Name: Solutions

? this lecture. ? next lecture. What we have learned so far. a Q E F = q E a. F = q v B a. a Q in motion B. db/dt E. de/dt B.

Chapter 19 Webassign Help Problems

Content 5.1 Angular displacement and angular velocity 5.2 Centripetal acceleration 5.3 Centripetal force. 5. Circular motion.

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2.

ASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241

) 1.5"10 11 m. ( )( 1.99 "10 30 kg)

Chapter 5. Uniform Circular Motion. a c =v 2 /r

Physics 2B Chapter 22 Notes - Magnetic Field Spring 2018

Static Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E.

( n x ( ) Last Time Exam 3 results. Question. 3-D particle in box: summary. Modified Bohr model. 3-D Hydrogen atom. r n. = n 2 a o

Solutions Practice Test PHYS 211 Exam 2

The geometric construction of Ewald sphere and Bragg condition:

V7: Diffusional association of proteins and Brownian dynamics simulations

Do not turn over until you are told to do so by the Invigilator.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

A moving charged particle creates a magnetic field vector at every point in space except at its position.

Chap 5. Circular Motion: Gravitation

MAGNETIC FIELD INTRODUCTION

16.1 Permanent magnets

8-3 Magnetic Materials

Tidal forces. m r. m 1 m 2. x r 2. r 1

Electrostatics (Electric Charges and Field) #2 2010

Circular motion. Objectives. Physics terms. Assessment. Equations 5/22/14. Describe the accelerated motion of objects moving in circles.

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s

PHYS 1441 Section 002. Lecture #3

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

r ˆr F = Section 2: Newton s Law of Gravitation m 2 m 1 Consider two masses and, separated by distance Gravitational force on due to is

3-7 FLUIDS IN RIGID-BODY MOTION

What molecular weight polymer is necessary to provide steric stabilization? = [1]

Determining solar characteristics using planetary data

RE 11.e Mon. Review for Final (1-11) HW11: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. Final Exam (Ch. 1-11)

Electrostatics. 1. Show does the force between two point charges change if the dielectric constant of the medium in which they are kept increase?

CHAPTER 25 ELECTRIC POTENTIAL

Calculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m

Physics 2212 GH Quiz #2 Solutions Spring 2016

Addition of Angular Momentum

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D.

Electromagnetism Physics 15b

one primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems

Physics 107 TUTORIAL ASSIGNMENT #8

COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM

Eventually transatlantic signals! From Last Time. Electromagnetic Waves. The idea of electric fields. The electric field.

Chapter 5 Page 5.1 CHAPTER 5. r Force times distance has units of energy. Therefore, fxr=u, or f / is dimensionless.

Algebra-based Physics II

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session.

Gravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003

[ ] = jω µ [ + jω ε E r

3.2 Centripetal Acceleration

Between any two masses, there exists a mutual attractive force.

Rydberg-Rydberg Interactions

ω = θ θ o = θ θ = s r v = rω

Skin Effect and Formation Damage

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )

LC transfer of energy between the driving source and the circuit will be a maximum.

Ch. 4: FOC 9, 13, 16, 18. Problems 20, 24, 38, 48, 77, 83 & 115;

Magnetic Field. Conference 6. Physics 102 General Physics II

CHAPTER 5: Circular Motion; Gravitation

Stress, Cauchy s equation and the Navier-Stokes equations

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

CBE Transport Phenomena I Final Exam. December 19, 2013

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

But for simplicity, we ll define significant as the time it takes a star to lose all memory of its original trajectory, i.e.,

Orbital Angular Momentum Eigenfunctions

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

( ) ( ) Last Time. 3-D particle in box: summary. Modified Bohr model. 3-dimensional Hydrogen atom. Orbital magnetic dipole moment

Ch 13 Universal Gravitation

Van Bistrow, Department of Physics, University of Chicaqgo. Experiment VI. Electron Spin Resonance

Chapter 31 Faraday s Law

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Announcements. Description Linear Angular position x θ displacement x θ rate of change of position v x ω x = = θ average rate of change of position

Written as per the revised syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune.

Course Updates. Reminders: 1) Assignment #8 will be able to do after today. 2) Finish Chapter 28 today. 3) Quiz next Friday

Lecture 8 - Gauss s Law

Chapter 13 Gravitation

rt () is constant. We know how to find the length of the radius vector by r( t) r( t) r( t)

CHAPTER: 4 MOVING CHARGES AND MAGNETISM

Potential Energy. The change U in the potential energy. is defined to equal to the negative of the work. done by a conservative force

Waves and Polarization in General

SPH3UW/SPH4U Unit 3.2 Forces in Cetripetal Motion Page 1 of 6. Notes Physics Tool Box

Circular-Rotational Motion Mock Exam. Instructions: (92 points) Answer the following questions. SHOW ALL OF YOUR WORK.

Faraday s Law. Faraday s Law. Faraday s Experiments. Faraday s Experiments. Magnetic Flux. Chapter 31. Law of Induction (emf( emf) Faraday s Law

HW #5 Hints. Today. HW #5 Hints. HW #5 Hints. Announcements:

LECTURE 15. Phase-amplitude variables. Non-linear transverse motion

Transcription:

Ch 11 Paticulate upenion

Iue Stability (dipeion) edientation igation wall lip

Had phee Only igid epulion peent when paticle coe into contact Zeo hea vicoity ( 1+. φ) 5 1+.5φ + 6.φ d.5 ( φ) dφ exp( 5φ / ) exp( [ ] φ) [ ] li φ φ 0 φ [ ] φ 1 φ Kiege-Doughety equation

Had phee Vicoity can be educed when paticle of diffeent ize ae ixted Highe volue faction of paticle can be packed into a upenion Of pactical ipotance in the foulation of highly loaded upenion -> allow theal expanion coefficient be cloely atched to the device -> pevent cack and debonding

Had phee Shea thinning a T k D B 6π 0 T k a D a t B D 3 0 6π D B t T k a Pe γ γ 3 T k a B 3 σ σ σ c σ / 1 1 0 + tie fo a paticle to diffue a ditance equal to it adiu Univeal function of Pecle nube fo fixed volue faction

Had phee Mechani of hea thinning & hea thickening Shea thinning; 1.diappeaance of Bownian contibution -> vicoity eduction by a facto of.foation of line of paticle (ting) paallel to the flow diection -> evidenced by copute iulation & light catteing Shea thickening; 1.foation of clute containing paticle diven by hea into cloe poxiity.defoation of clute poduce lage lubication tee in the thin fil epaating cloely paced paticle 3.the echani depend on the natue of the epulive potential

Non-pheical paticle Dilute upenion Jeffey obit In the abence of Bownian otion and of intepaticle inteaction, p u u ω + p 1 + 1 ( u D uuu : D) In a heaing flow, γt tanθ p tan + tanθ0 p + 1/ p θ; the angle of the axi of yety eaued in the clockwie diection fo the flow diection θ i tie-peiodic; a non-bownian axiyetic paticle otate indefinitely in a hea flow with a peiod π 1 P p + γ p When paticle otation ae ditubed by Bownian otion, D D 0 0 3k 3k B B T (ln( p) 0.5) 3 π L T (ln( L / d) 0.8) 3 π L Rotay diffuivity fo a pheoid of apect atio p Rotay diffuivity fo od

Non-pheical paticle Dilute upenion of pheoid e v σ σ + σ + σ σ e p p 3 1 ν k + 1 B T uu σ υ { A uuuu D + B[ uu D + D uu ] CD} φ : + σ D

Non-pheical paticle Dilute upenion of high-apect-atio paticle o olecule 1 σ D + νς t uuuu : D + 3ν k B T uu δ 3 ς t π L ε T 3 B f ( ) 6ln(L / d) D 0 k

Non-pheical paticle Sei-dilute upenion of Bownian od + + δ uu D uuuu D σ 3 1 3 : T k B t ν νς 0 ˆ ) ( + u uuu : D u u u ψ ψ ψ D t ) ( 4 ) ( ˆ u d D D u u u u ψ π Oientation dependent otay diffuivity

Non-pheical paticle Sei-dilute non-bownian fibe upenion 1.vicoity inceae i not uch.noal te ~ 0.4 tie hea 5/ te N p φ p ln( p) 1 C 3/ 3.lage extenional tee 4 γ 4φp 3 + νς t 3 1 + 9ln( π / φ )

Electically chaged paticle Had phee; coated with an oganic laye that povide a teic baie to pevent flocculation The chage lead to long-ange epulion that can keep the paticle fa enough apat that they ae not dawn togethe by hot-ange van de Waal foce The uface chage inceae the effective paticle diaete vicoity at all volue faction 5 3 d 1.5φ.5 φ 0 40 eff + + + a d eff 1 ln κ { α / ln[ α / ln( α /)]}

Electically chaged paticle vicoity at effective volue faction lage than 0.1 φeff 1 φ (5/ ) φ

Electically chaged paticle vicoity: hea ate dependence a hea ate inceae, hydodynaic contibution inceae, the effective paticle diaete goe down, the paticle appoach each othe oe cloely

Electically chaged paticle Yield te and odulu The yield te appea when the paticle epulion ae tong enough to induce acocytallization. A the ionic tength deceae futhe, the epulion becoe tonge, and the yield te becoe lage. 3 ) / ( ) ( B y T k W K σ 3 1/ φ φ a ) ( 5 4 5 W N d W d d dw N G κ π φ π φ +

Electically chaged paticle Flow echani - foation of liding laye - beakdown of thee laye a hea ate inceae

Electically chaged paticle Shea thinning; due to lipping of the laye pat each othe Shea thickening equie not only that liding laye be boken down by hea, but that the fagent of thee laye ut otate and collide with each othe to fo tuctue whoe aveage dienion in the flowgadient diection ae lage. Such tuctue can ja the flow, leading to abupt hea thickening.

Electically chaged paticle Noal te diffeence N N1 σ appea only when - LCP copoed of od-like olecule - electoheological upenion which fo chain-like aggegate iilaity uppot the notion that in the hea thickening egion, the elevant flow unit ae no longe phee, but ae od-like o dik-like paticle aggegate

Paticle in vicoelatic liquid - to add pefoance, to ave cot, to potentially educe theal expanion tee effectively le elatic than polye alone effect of coupling agent enhanced hea thinning, becaue the hea ate expeienced by polye confined between two paticle can be uch lage than the oveall hea ate

Paticle in vicoelatic liquid Thixotopy; a the diffuion tie contant i too lage (ode of an hou) due to high vicoity, it take a long tie fo a gel-like paticle tuctue to elax o efo, hence, flow induce change in fluid tuctue that ae eaed only afte hou of quiecence