Problem 5: Microfluidics Math in Industry Workshop Student Mini-Camp CGU 2009 Abouali, Mohammad (SDSU) Chan, Ian (UBC) Kominiarczuk, Jakub (UCB) Matusik,

Slides:



Advertisements
Similar presentations
Chapter 6 Differential Equations
Advertisements

2ª aula Evolution Equation. The Finite Volume Method.
Subsurface Fate and Transport of Contaminants
Chapter 8 Elliptic Equation.
P. Venkataraman Mechanical Engineering P. Venkataraman Rochester Institute of Technology DETC2014 – 35148: Continuous Solution for Boundary Value Problems.
Chapter 01: Flows in micro-fluidic systems Xiangyu Hu Technical University of Munich.
1cs542g-term Notes  No extra class tomorrow.
Total Recall Math, Part 2 Ordinary diff. equations First order ODE, one boundary/initial condition: Second order ODE.
PART 7 Ordinary Differential Equations ODEs
Finite Difference Solutions to the ADE. Simplest form of the ADE Even Simpler form Plug Flow Plug Source Flow Equation.
UNSTEADY VISCOUS FLOW Viscous effects confined to within some finite area near the boundary → boundary layer In unsteady viscous flows at low Re the boundary.
Combining the strengths of UMIST and The Victoria University of Manchester Aspects of Transitional flow for External Applications A review presented by.
REVIEW. What processes are represented in the governing equation that we use to represent solute transport through porous media? Advection, dispersion,
MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 9: FLOWS IN PIPE
A reaction-advection-diffusion equation from chaotic chemical mixing Junping Shi 史峻平 Department of Mathematics College of William and Mary Williamsburg,
One dimensional models of hydraulic fracture Anthony Peirce (UBC) Collaborators: Jose` Adachi (SLB) Shira Daltrop (UBC) Emmanuel Detournay (UMN) WITS University.
Approximate Asymptotic Solutions to the d-dimensional Fisher Equation S.PURI, K.R.ELDER, C.DESAI.
Instability of electro-osmotic channel flow with streamwise conductivity gradients J. Jobim Santos Brian D. Storey Franklin W. Olin College of Engineering.
高等輸送二 — 質傳 Lecture 3 Dispersion
Atmospheric turbulence Richard Perkins Laboratoire de Mécanique des Fluides et d’Acoustique Université de Lyon CNRS – EC Lyon – INSA Lyon – UCBL 36, avenue.
報 告 者:林 建 文 指導教授:陳 瑞 昇 博士 1 Jesús S. Pérez Guerrero · Todd H. Skaggs · M. Th. van Genuchten {Transp Porous Med (2010) 85:171–188.}
FUNDAMENTAL EQUATIONS, CONCEPTS AND IMPLEMENTATION
SOLUTION FOR THE BOUNDARY LAYER ON A FLAT PLATE
Louisiana Tech University Ruston, LA Slide 1 The Rectangular Channel Steven A. Jones BIEN 501 Friday, April 4th, 2008.
SELFE: Semi-implicit Eularian- Lagrangian finite element model for cross scale ocean circulation Paper by Yinglong Zhang and Antonio Baptista Presentation.
Hydraulic Routing in Rivers
Louisiana Tech University Ruston, LA Lubrication/Thin Film & Peristaltic Flows Juan M. Lopez Lecture 10 BIEN 501 Wednesday, March 28, 2007.
Boundary Collocation Methods: Review and Application to Composite Media P. A. Ramachandran Washington University St. Louis, MO Lecture Presented at UNLV.
BsysE595 Lecture Basic modeling approaches for engineering systems – Summary and Review Shulin Chen January 10, 2013.
Enhancement of Heat Transfer P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Invention of Compact Heat Transfer Devices……
1 EEE 431 Computational Methods in Electrodynamics Lecture 4 By Dr. Rasime Uyguroglu
Mass Transfer Coefficient
Introduction 1. Similarity 1.1. Mechanism and mathematical description 1.2. Generalized variables 1.3. Qualitative analysis 1.4. Generalized individual.
3.3.3: Semi-Lagrangian schemes AOSC614 class Hong Li.
CEE 262A H YDRODYNAMICS Lecture 15 Unsteady solutions to the Navier-Stokes equation.
PDE simulations with adaptive grid refinement for negative streamers in nitrogen Carolynne Montijn Work done in cooperation with: U. Ebert W. Hundsdorfer.
Order of Magnitude Scaling of Complex Engineering Problems Patricio F. Mendez Thomas W. Eagar May 14 th, 1999.
Prof. Mohammad Asif Room 2B45, Building 3
BOUNDARY LAYERS Viscous effects confined to within some finite area near the boundary → boundary layer In unsteady viscous flows at low Re (impulsively.
Hydraulic Routing in Rivers Reference: HEC-RAS Hydraulic Reference Manual, Version 4.1, Chapters 1 and 2 Reading: HEC-RAS Manual pp. 2-1 to 2-12 Applied.
2 how to deal with …? examples of common international 3.
© Cambridge University Press 2010 Brian J. Kirby, PhD Sibley School of Mechanical and Aerospace Engineering, Cornell University, Ithaca, NY Powerpoint.
1 Challenge the future The Lateral Motion of Wafer under the Influence of Thin-film Flow Leilei Hu Solid and Fluid Mechanics
Aula Teórica 9&10 Equação de Evolução. Exemplos. Caso 1D.
FREE CONVECTION 7.1 Introduction Solar collectors Pipes Ducts Electronic packages Walls and windows 7.2 Features and Parameters of Free Convection (1)
Discretization Methods Chapter 2. Training Manual May 15, 2001 Inventory # Discretization Methods Topics Equations and The Goal Brief overview.
Finite Difference Solutions to the ADE. Simplest form of the ADE Even Simpler form Plug Flow Plug Source Flow Equation.
APPLICATION TO EXTERNAL FLOW
Nature of Zero Pressure Gradient BL Flows…… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Solutions for Flat Plate Boundary Layer.
Solving Partial Differential Equation Numerically Pertemuan 13 Matakuliah: S0262-Analisis Numerik Tahun: 2010.
© 2016 Carl Lund, all rights reserved A First Course on Kinetics and Reaction Engineering Class 38.
Viscosità Equazioni di Navier Stokes. Viscous stresses are surface forces per unit area. (Similar to pressure) (Viscous stresses)
Date of download: 9/26/2017 Copyright © ASME. All rights reserved.
Mathematical Simulations of Heat Transfer and Fluid Dynamics in a Microfluidic Calorimeter with Integrated Thin-film Thermopiles G. G. Nestorova 1, Niel.
Fluid Resistance: Micro-channels of the Valve Design
Lamella Mixer CHEM-E7160- FLUID FLOW IN PROCESS UNITS MOHAMMED REFAAT
Date of download: 10/26/2017 Copyright © ASME. All rights reserved.
Turbulence closure problem
Introduction to Partial Differential Equations
Pressure Poisson Equation
Space Distribution of Spray Injected Fluid
AIAA OBSERVATIONS ON CFD SIMULATION UNCERTAINITIES
AIAA OBSERVATIONS ON CFD SIMULATION UNCERTAINTIES
Models of atmospheric chemistry
Mathematical modeling techniques in the engineering of landfill sites.
AE/ME 339 Computational Fluid Dynamics (CFD) K. M. Isaac
AIAA OBSERVATIONS ON CFD SIMULATION UNCERTAINTIES
Step change in the boundary condition of conduction problems
Convective Heat Transfer
Presentation transcript:

Problem 5: Microfluidics Math in Industry Workshop Student Mini-Camp CGU 2009 Abouali, Mohammad (SDSU) Chan, Ian (UBC) Kominiarczuk, Jakub (UCB) Matusik, Katie (UCSD) Salazar, Daniel (UCSB) Advisor: Michael Gratton

Introduction Micro-fluidics is the study of a thin layer of fluid, of the order of 100μm, at very low Reynold’s number (Re<<1) flow To drive the system, either electro-osmosis or a pressure gradient is used This system is used to test the effects of certain analytes or chemicals on the cell colonies

Micro-fluidics in Drug Studies

Problems and Motivations Due to diffusion and the cell reaction, the concentration of the analyte is changing across and along the channel Problems: – Maximize the number of the cell colonies placed along the channels What are the locations where the analyte concentrations are constant?

Peclet Number:Taylor-Aris Dispersion Condition: Width: 1 cm Length: 10 cm Height: 100 µm Dimensions of Channel and Taylor Dispersion

Depth-wise Averaged Equation Governing Equation: Boundary Conditions: where

Two Channels ConcentrationVelocityVorticity

Two Channel x=0 mm

Two Channel x=25 mm

Two Channel x=50 mm

Two Channel x=75 mm

Two Channel x=100 mm

Three Channels ConcentrationVelocityVorticity

Three Channel x=0 mm

Three Channel x=25 mm

Three Channel x=50 mm

Three Channel x=75 mm

Three Channel x=100 mm

Width Changes Along the Channel

Model Equation: Uptake is assumed to be at a constant rate over the cell patch. The reaction rate is chosen to be the maximum over the range of concentrations used

Defining Non-dimensionalize equation: Boundary Conditions:

Analytical solution An analytical solution can be found via Fourier transform: Transformed equation: Solutions:

- Demand continuity and differentiability across boundary, and apply boundary conditions. - Apply inverse Fourier transform

- We are interested the wake far away from the cell patch: - The integral can be evaluated via Laplace’s method: Taylor Expansion For large x: >> φ

Restoration is defined as Restoration length: Larger flow velocity enhances recovery??

Numerical wake computation Advection-Diffusion-Reaction equation with reaction of type C 0 Domain size 10 x 60 to avoid effects of outflow boundary Dirichlet boundary condition at inflow boundary, homogeneous Neuman at sides and outflow Solved using Higher Order Compact Finite Difference Method (Kominiarczuk & Spotz) Grid generated using TRIANGLE

Numerical wake computation Choose a set of neighbors Compute optimal finite difference stencil for the PDE Solve the problem implicitly using SuperLU Method of order, reduce locally due to C 0 solution

Conclusions from numerical experiments Diffusion is largely irrelevant as typical Peclet numbers are way above 1 „Depth” of the wake depends on the relative strength of advection and reaction terms Because reaction rates vary wildly, we cannot conclude that it is safe to stack colonies along the lane given the constraints of the design

Outstanding Issues: Will vertically averaging fail for small diffusivity? What are the limitations of the vertically averaging? Taylor dispersion? Pattern of colony placements? Realistic Reaction Model? Effect of Boundaries along the device?

References Y.C. Lam, X. Chen, C. Yang (2005) Depthwise averaging approach to cross-stream mixing in a pressure-driven michrochannel flow Microfluid Nanofluid 1: R.A. Vijayendran, F.S. Ligler, D.E. Leckband (1999) A Computational Reaction-Diffusion Model for the Analysis of Transport-Limited Kinetics Anal. Chem. 71,