Similar documents

V (r,t) = i ˆ u( x, y,z,t) + ˆ j v( x, y,z,t) + k ˆ w( x, y, z,t)

International Journal of Engineering & Technology IJET-IJENS Vol:18 No:03 1

Chapter 6: Incompressible Inviscid Flow

Anindya Aparajita, Ashok K. Satapathy* 1.

Candidates must show on each answer book the type of calculator used. Log Tables, Statistical Tables and Graph Paper are available on request.

Chapter 9: Differential Analysis

Fluid Mechanics II Viscosity and shear stresses

Chapter 9: Differential Analysis of Fluid Flow

Candidates must show on each answer book the type of calculator used. Only calculators permitted under UEA Regulations may be used.

Fluid Dynamics Exercises and questions for the course

Viscoelastic Effects on Dispersion due to Electroosmotic Flow with Variable Zeta Potential

Numerical Heat and Mass Transfer

6.2 Governing Equations for Natural Convection

UNIVERSITY OF EAST ANGLIA

Fundamental Concepts of Convection : Flow and Thermal Considerations. Chapter Six and Appendix D Sections 6.1 through 6.8 and D.1 through D.

ENGR Heat Transfer II

F11AE1 1. C = ρν r r. r u z r


Studies on flow through and around a porous permeable sphere: II. Heat Transfer

Research Article Peristaltic Transport of a Jeffrey Fluid with Variable Viscosity through a Porous Medium in an Asymmetric Channel

Fundamentals of Fluid Dynamics: Elementary Viscous Flow

2.5 Stokes flow past a sphere

How are calculus, alchemy and forging coins related?

CONVECTIVE HEAT TRANSFER

An Exact Solution of MHD Boundary Layer Flow over a Moving Vertical Cylinder

1. Poisson-Boltzmann 1.1. Poisson equation. We consider the Laplacian. which is given in spherical coordinates by (2)

ENGI Multiple Integration Page 8-01

6. Laminar and turbulent boundary layers

Exercise 5: Exact Solutions to the Navier-Stokes Equations I

Electroosmotic Flow Mixing in a Microchannel

Chapter 1. Viscosity and the stress (momentum flux) tensor

Introduction to Heat and Mass Transfer. Week 9

Laminar Flow. Chapter ZERO PRESSURE GRADIENT

MOMENTUM TRANSPORT Velocity Distributions in Turbulent Flow

Interception efficiency in two-dimensional flow past confined porous cylinders Setareh Shahsavari*, Brian L. Wardle, Gareth H.

Basic concepts in viscous flow

Potential changes of the cross section for rectangular microchannel with different aspect ratios

Figure 3: Problem 7. (a) 0.9 m (b) 1.8 m (c) 2.7 m (d) 3.6 m

Week 2 Notes, Math 865, Tanveer

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

A NUMERICAL APPROACH FOR ESTIMATING THE ENTROPY GENERATION IN FLAT HEAT PIPES

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

INTRODUCTION TO FLUID MECHANICS June 27, 2013

Lecture 9 Electric Flux and Its Density Gauss Law in Integral Form

ISO Colloidal systems Methods for zetapotential. Part 1: Electroacoustic and electrokinetic phenomena

Electro-osmotic Flow Through a Rotating Microchannel

Questions Chapter 23 Gauss' Law

Mobility of Power-law and Carreau Fluids through Fibrous Media

Part II: Self Potential Method and Induced Polarization (IP)

Shell Balances in Fluid Mechanics

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

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

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

Microfluidic Devices. Microfluidic Device Market. Microfluidic Principles Part 1. Introduction to BioMEMS & Medical Microdevices.

Design and Modeling of Fluid Power Systems ME 597/ABE Lecture 7

Mathematical Concepts & Notation

Electrolyte Concentration Dependence of Ion Transport through Nanochannels

The purpose of this lecture is to present a few applications of conformal mappings in problems which arise in physics and engineering.

Numerical Modeling of the Bistability of Electrolyte Transport in Conical Nanopores

MAT389 Fall 2016, Problem Set 4

al., 2000) to extend the previous numerical model to account for the effect of interfacial charges. This extension allows the analysis of the electrok

Transport processes. 7. Semester Chemical Engineering Civil Engineering

Lecture 13: Electromagnetic Theory Professor D. K. Ghosh, Physics Department, I.I.T., Bombay. Poisson s and Laplace s Equations

ENGR Heat Transfer II

Convective Mass Transfer

UNIVERSITY of LIMERICK

Conductors and Dielectrics

FLUID MECHANICS. Chapter 9 Flow over Immersed Bodies

Lecture 9 Laminar Diffusion Flame Configurations

Electrophoretic Deposition. - process in which particles, suspended in a liquid medium, migrate in an electric field and deposit on an electrode

Unit operations of chemical engineering

Introduction. Statement of Problem. The governing equations for porous materials with Darcy s law can be written in dimensionless form as:

We are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists. International authors and editors

Spotlight on Laplace s Equation

Key Concepts for section IV (Electrokinetics and Forces)

Research Article Innovation: International Journal of Applied Research; ISSN: (Volume-2, Issue-2) ISSN: (Volume-1, Issue-1)

Outline. Definition and mechanism Theory of diffusion Molecular diffusion in gases Molecular diffusion in liquid Mass transfer

Fundamentals of Fluid Dynamics: Ideal Flow Theory & Basic Aerodynamics

Lab Reports Due on Monday, 11/24/2014

Detailed Outline, M E 521: Foundations of Fluid Mechanics I

An electrokinetic LB based model for ion transport and macromolecular electrophoresis

Transport by convection. Coupling convection-diffusion

MODULE 3: MASS TRANSFER COEFFICIENTS

lim = F F = F x x + F y y + F z

Hydrodynamic permeability of aggregates of porous particles with an impermeable core

Fluid Mechanics Qualifying Examination Sample Exam 2

Microfluidics 1 Basics, Laminar flow, shear and flow profiles

Lecture 2: Hydrodynamics at milli micrometer scale

UNIVERSITY OF OSLO. Faculty of Mathematics and Natural Sciences. MEK4300/9300 Viscous flow og turbulence

3 Chapter. Gauss s Law

1. Fluid Dynamics Around Airfoils

LATTICE BOLTZMANN MODELLING OF PULSATILE FLOW USING MOMENT BOUNDARY CONDITIONS

Effect of charged boundary on electrophoresis: Sphere in spherical cavity at arbitrary potential and double-layer thickness

MATH 332: Vector Analysis Summer 2005 Homework

Physics Lecture: 09

FORMULA SHEET. General formulas:

MA3D1 Fluid Dynamics Support Class 5 - Shear Flows and Blunt Bodies

Primary Electroviscous Effect in a Suspension of Charged Porous Spheres

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER

Transcription:

Number of pages in the question paper : 05 Number of questions in the question paper : 48 Modeling Transport Phenomena of Micro-particles Note: Follow the notations used in the lectures. Symbols have their usual meanings. Variable typed in bold represent vector. Use the following electrokinetic parameters: φ 0 = RT/F = k B T/e = 0.02586 V; permittivity, ε e = 695.39 10 12 C/Vm; elementary charge, e = 1.602 10 19 C; dynamic viscosity, µ = 10 3 Pa s; Faraday constant, F = 96500 C/mol; diffusivity of Na + ion, D Na + = 1.33 10 9 m 2 /s and diffusivity of Cl ion, D Cl = 2.03 10 9 m 2 /s. Also, 1µm=10 6 m and 1 nm= 10 9 m. SECTION-1 [20 x 1 = 20 marks] Questions 1 to 12: Fill the blanks with appropriate answer 1. In case of Newtonian fluids, the fluid stress and strain obey the relation... 2. Dimension of permeability of a porous medium is... 3. If the total number of dimensional parameters is 6 of which 3 are independent, then the number of dimensionless groups is... 4. Let g(x) be a function defined by g(x) = 1 + x + x 2, x R. Then the value of the integral g(x)δ(x 5)dx is equal to... 5. If the streamlines are given by ψ = xy then the resultant velocity at (1, 1) is... 6. In case of a rigid spherical object swimming at very small Reynolds numbers, in the absence of any external forces, the normal velocity condition on the boundary is... 7. If a fluid with velocity u is in contact with an impermeable boundary x = 0, having a velocity v = (3, 2), then the dynamic boundary condition is given by... 8. In case of Stokes flow past a sphere, if one third of the drag force is due to the pressure forces, then two third is due to... 9. Consider a uni-directional flow between two parallel plates under non-zero pressure gradient. If both the plates are at rest, then the velocity is always maximum at... 10. Consider the Brinkman equation governing flow inside a porous medium. If the viscous forces are negligible, then, the Brinkman equation reduces to... 1

11. Coulomb s law provides the force between two point charges. 12. The electric force on a charge q under an electric filed E is. 13. In Cartesian coordinates if E = (A, 0, 0), where A is a constant, then the electric potential φ is. 14. The electric permittivity of a medium is than the electric permittivity of vacuum. 15. If u is the velocity field of an incompressible fluid then.u =. 16. In steady-state, if N i is the molar flux of the i th ionic species then.n i =. 17. If ions are obeying the Boltzmann distribution then the convective transport of ions are. 18. If n 1 and n 2 be the molar concentration of two ionic species with valence z 1 and z 2, respectively, then the charge density is. 19. If u is the electrophoretic velocity of a particle under an electric field E then mobility is. 20. Debye-Hückel approximation is valid for surface charge density. SECTION-II [20 x 2 = 40 marks] 1. Consider the mass conservation equation in (r, θ, z) cylindrical coordinates,( where the flow is axi-symmetric) given by 1 (rv r ) + v z r r z = 0. If the velocity vector is only along the radial direction, then show that the radial velocity component v r is of the form 1 f(z) for some arbitrary function f that depends only on z. r 2. Consider the mass conservation equation given in (r, θ, z) cylindrical coordinates,( where the flow is axi-symmetric). The corresponding velocity components are given in as u r = r2 z 3 z = rz2. Then, compute the corresponding stream function. 2 Answer questions 3 and 4 based on the following information: Consider a sphere of radius 10 cm which is made of limestone. The volume occupied by the void is 40 cm 3. The mean grain diameter of the limestone particles is 1 mm. Then, 3. Find the porosity of the sphere. 2

4. Find the permeability of the sphere using Carman-Kozney relation, K = D2 p φ3. 180(1 φ) 2 5. Consider the steady state heat conduction interior to a rigid impermeable sphere of radius a (with azimuthal axi-symmetry). We are seeking a solution of the form ( T (r, θ) = a n r n + b ) n P r n+1 n (cos θ). n=0 If a heat source is located at the origin given by T S (r, θ) = 50 cos θ, then determine the r 2 coefficients b n. (Hint: P 1 (x) = x). 6. Consider the free-space Green s function of unit strength, G(x, x 0 ) = ln r, where x = (x, y), x 0 = (1, 2) and r = x x 0, then compute G. x Answer questions 7 and 8 based on the following information: Consider Stokes equations governing viscous incompressible flow at very low Reynolds number (two-dimensional), where v represents the velocity, p represents the corresponding pressure, ψ denote the stream function. Then, 7. Decide whether following quantities are harmonic or bi-harmonic, (i). v, (ii). v. 8. Decide whether following quantities are harmonic or bi-harmonic, (i). p, (ii). ψ. 9. If the velocity vector corresponding to a three-dimensional viscous incompressible flow is given by u = (yz x, y+z, 0), then compute the tangential stress components (τ xy, τ yz, τ zx ). 10. Show that u = 2cxy, v = c(a 2 + x 2 y 2 ) are the velocity components of a possible fluid motion. Determine the corresponding stream function. 11. Consider a point charge q = 0.005 C is placed within the center of volume enclosed by a sphere. Find the flux of the electric field through the surface of the sphere. Answer questions 12-16 based on the following statement: A planar surface of ζ-potential as 2.586 10 2 V is in contact with a NaCl solution with inverse of Debye length κ = 3.0 10 9 m 1, then: 12. Find the surface charge density. 13. Use the Debye-Hückel approximation to find the electric potential at a point 0.5 nm. from the planar surface 14. Use Boltzmann distribution to obtain the ionic concentration of Na + at the point 0.5 nm from the planar surface. 3

15. Calculate the ionic concentration of Cl at the point 0.5 nm form the planar surface when the ions obey the Boltzmann distribution. 16. Find the charge density at the point 0.5nm from the planar surface. Answer questions 17 and 18 for the problem: Consider a combined electroosmosis and pressure driven flow of 1 mol/m 3 NaCl electrolyte solution in a slit microchannel of half channel height h = 50 nm under the influence of an external electric field of 10 4 V/m acting along the axis of the channel with a constant pressure gradient (dp/dx) along the length of the channel. Consider the mid-plane of the microchannel as the x-axis. The wall ζ-potential is 0.1 V. 17. Calculate the Debye length. 18. Find the axial velocity,u at y = 5 nm when the constant axial pressure gradient is dp = 0.36 Pa/m. dx 19. A spherical particle of radius a=10 nm with surface potential ζ = 0.02586 V is suspended in a non-conducting liquid i.e., inverse Debye length κ is such that κa << 1. Find the electrophoretic velocity due to an externally imposed electric field E 0 = 100 V/m. 20. Consider the boundary value problem (BVP) (1 + x 2 ) d2 y + 4x dy + 2y = 2, y(0) = 0, y(1) = 1/2 dx 2 dx Derive the discretized form of the BVP by using a central difference scheme when the step size h = 1/3. SECTION-III [8 X 5 = 40 marks] 1. Consider a flow through porous medium that is governed by the extended Brinkman equation ( u ) ρ t + u. u = p + µ 2 u µu K, where u = (u, v) represent the velocity. In order to non-dimensionalize, the following dimensionless variables are used: x = x L, y = y L, t = µt ρl, 2 u = u U, v = v U, p = p ρu, Da = K 2 L. 2 If x-component of the above governing equation is given by ) α u + β (u u u + t v = 1 p ( 2 x y Λ x + u x + 2 u ) γu, 2 y 2 4

then find the parameters α, β, γ and Λ. 2. Consider the governing equation for a viscous incompressible flow inside a porous medium p + µ 2 u µk 1 u = 0, ( ) K1 0 where K is the permeability of the medium that is given by the matrix K =, 0 K 2 where K 1 and K 2 are constants. Then introduce stream function in two-dimensions and hence derive the corresponding equation satisfied by the stream function. Answer questions 3 and 4 based on the following information: Consider a fluid motion inside a porous circular cylinder. Given that the magnitude of the velocity is V and the radius of the cylinder is L, the pressure: P, density of the fluid: ρ and the permeability of the porous medium: K. 3. Find the number of non-dimensional groups involved using Buckingham-π theorem. Further, find one of the non-dimensional groups which is of the form f(p, L, V, ρ) = 0. 4. Find another non-dimensional group which is of the form f(l, V, ρ, K) = 0. 5. Write the equation for the electric field which relates the charge density ρ e at any point in an electrolyte solution of permittivity ε e. If the ions obey the Boltzmann distribution then derive the Poisson-Boltzmann equation for the electric field. 6. Find an expression for the electroosmotic flow velocity in a slit micro-channel with sur- face potential of both the walls as ζ and the electric field applied parallel to the channel walls. 7. Solve the following partial differential equation for the first time step through an implicit scheme. u t = u xx u(x, 0) = sin πx, 0 < x < 1 u(0, t) = u(1, t) = 0, t > 0 with δx = 1/3 and δt = 1/36. 8. Derive the fluid transport equations in non-dimensional form for the electrophoresis of a charged spherical particle of radius a with surface potential ζ in an electrolyte medium of permittivity ε e and charge density ρ e. END OF THE QUESTION PAPER 5