Design of a novel recirculation system using COMSOL

Slides:



Advertisements
Similar presentations
Fluid Mechanics Research Group Two phase modelling for industrial applications Prof A.E.Holdø & R.K.Calay.
Advertisements

Open Source Field Operation and Manipulation
Instructor: André Bakker
Outline Overview of Pipe Flow CFD Process ANSYS Workbench
Colloid: Electrokinetic properties
Lecture 2 Properties of Fluids Units and Dimensions.
The Flame Deflector and Five Segment Booster By: Geoffrey Husk.
Boundary Layer Flow Describes the transport phenomena near the surface for the case of fluid flowing past a solid object.
© Fluent Inc. 5/10/2015N1 Fluids Review TRN Postprocessing and Visualization.
An Analysis of Hiemenz Flow E. Kaufman and E. Gutierrez-Miravete Department of Engineering and Science Rensselaer at Hartford.
..perhaps the hardest place to use Bernoulli’s equation (so don’t)
Design of Scintillator Die Fermi National Accelerator Laboratory Department of Mechanical Engineering Northern Illinois University.
James Sprittles ECS 2007 Viscous Flow Over a Chemically Patterned Surface J.E. Sprittles Y.D. Shikhmurzaev.
An Ultimate Combination of Physical Intuition with Experiments… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Boundary Layer.
Chapter 14 Fluids Key contents Description of fluids
Plasma Dynamics Group Aerospace & Energetics Research Program Boundary Conditions for MHD Resistive MHD equations in weakly conservative form (balance.
Flow and Thermal Considerations
Natural Convection in free flow: Boussinesq fluid in a square cavity
James Sprittles BAMC 2007 Viscous Flow Over a Chemically Patterned Surface J.E Sprittles Y.D. Shikhmurzaev.
© Cambridge University Press 2010 Brian J. Kirby, PhD Sibley School of Mechanical and Aerospace Engineering, Cornell University, Ithaca, NY Powerpoint.
COMSOL Conference Prague 2006Page 1 Poisson equation based modeling of DC and AC electroosmosis Michal Přibyl & Dalimil Šnita Institute of Chemical Technology,
Lesson 21 Laminar and Turbulent Flow
CFD Pre-Lab 2 Simulation of Turbulent Flow around an Airfoil Seong Mo Yeon, and Timur Dogan 11/12/2013.
Chapter 14 Fluids What is a Fluid? A fluid, in contrast to a solid, is a substance that can flow. Fluids conform to the boundaries of any container.
Presenter : Ahmad Hadadan Adviser : Dr.Nazari Shahrood University Of Technology 1/14.
Lesson 13 CONVECTION HEAT TRANSFER Given the formula for heat transfer and the operating conditions of the system, CALCULATE the rate of heat transfer.
Powerpoint Slides to Accompany Micro- and Nanoscale Fluid Mechanics: Transport in Microfluidic Devices Chapter 6 Brian J. Kirby, PhD Sibley School of.
Department Of Material Science And Engineering FINITE ELEMENT METHOD UNIVERSITY OF CHEMICAL TECHNOLOGY AND METALLURGY Sofia Nina Velikova, June 2010.
EKT241 - Electromagnetic Theory
EKT241 - Electromagnetic Theory Chapter 3 - Electrostatics.
COLLOID: ZETA POTENTIAL
1 distance Potential Diffuse Layer Bulk Solution + dd IHPOHP The electrical double layer ii.
UNIVERSITI MALAYSIA PERLIS
CFD Lab 1 Simulation of Turbulent Pipe Flow Seong Mo Yeon, Timur Dogan, and Michael Conger 10/07/2015.
Appendix A.
CONVECTION : An Activity at Solid Boundary P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Identify and Compute Gradients.
Date of download: 7/7/2016 Copyright © ASME. All rights reserved. From: Effects of Cyclic Motion on Coronary Blood Flow J Biomech Eng. 2013;135(12):
5th International Conference on Nanosciences and Nanotechnologies (NN08) July, 2008 Thessaloniki, GREECE.
PDEs in shells; Example: current conduction in a steel tank
Hamdache Abderrazaq 1*, Belkacem Mohamed 1, Hannoun Nourredine 2
Date of download: 10/25/2017 Copyright © ASME. All rights reserved.
Date of download: 10/26/2017 Copyright © ASME. All rights reserved.
EPM_NM Lab * ** Transient Magnetic – Translating Motion Finite Element Model of the Annular Linear Induction Pump Cristian Roman*, Virgiliu Fireteanu*,
5. Conductors and dielectrics
Multi-physics Simulation of a Wind Piezoelectric Energy Harvester Validated by Experimental Results Giuseppe Acciani, Filomena Di Modugno, Ernesto Mininno,
11th International Conference on Mechanical Engineering (ICME2015)
TURBOMACHINES Chapter 1 INTRODUCTION
Electric Current.
PIV Investigation of EHD Flow Caused by Field-enhanced Dissociation
Title J. A. Smith1, M. B. Fields2
Title J. A. Smith1, M. B. Fields2
Invention of Geometries to Generate Lift
Title J. A. Smith, M. B. Fields2
Alternating Zeta-Potential Pattern to Eliminate Electro-Osmotic Flow
Xiaoxiao Sheng, Xingguo Xiong
Example: Polymer Extrusion
Lecture 20 Today Conductors Resistance Dielectrics
Model Species Transport in a Static Mixer Reacting Flows – Homework 6
Title J. A. Smith1, M. B. Fields2
Laminar and Turbulent Flow
Chapter 1 – Semiconductor Devices – Part 2
FLUID MECHANICS REVIEW
Model: Electric sensor
Mixing (2) Lab -8-.
Title J. A. Smith1, M. B. Fields2
Unit 8 Impulse and Momentum.
Hydrodynamics Presented by Mr.Halavath Ramesh M.A,M.sc,B.ED,PGDCAQM,PGDCA,M.Phil,(P.HD)(UoH) University of Madras Dept.
Mixing (2) Lab -8-.
Priyabrata Mandal, Priya Goel, Anusha Chandra, Dr. Sujay Chattopadhyay
Lecture 4 Dr. Dhafer A .Hamzah
Presentation transcript:

Design of a novel recirculation system using COMSOL Jithin George- 2011A4PS291H

Objective To model a novel recirculation system on COMSOL and input physical constraints on it. To generate Velocity , Pressure and other output results on COMSOL.

Literature Review Design of a novel recirculating system for slow reacting assays in microfluidic domain. N.N. Sharma Electro-osmotic mixer- Comsol manual

Geometry

Theory Electro-osmotic flow is caused by the movement of the electric double layer in the direction of an applied electric field. The direction as well as speed of flow is dependent upon the Zeta Potential of the electric double layer. The end outcome of this coupled electrostatic and fluid flow phenomena is the movement of the shear layer in along the applied electric field. This results in a ‘slip’ boundary condition at the electro-osmotically active walls, with a non-zero velocity tangential to the wall. Electro-osmotic flow is suppressed in the left side of the loop. The net effect of such an arrangement is that there is a continuous flow of fluid in a closed circle,

Formulae Involved Where e is the electric permeability, 𝑈 𝑒𝑜𝑓 = - 𝜇 𝑒𝑜𝑓 X E 𝜇 𝑒𝑜𝑓 = -𝜀z/𝜂 Where e is the electric permeability, h is the dynamic viscosity of fluid, z is the Zeta Potential and E is the applied electric field.

Material Properties Electrical Conductivity 0.01 [S/m] Relative Permeability 78.5 Density 1000[kg/ 𝑚 3 ] Viscousity 0.001 [Pa-s]

Boundary Conditions Applied Voltage [V0] 12 [V] Back Pressure at Outlet [p0] 0 [Pa] Electroosmotic Mobility [mu_eo] 0.06 [mm2/V.s] Device Thickness in third dimension [d] 20 [μm]

Results Electric Potential

Results Velocity Contour

Results Pressure distribution

RESULTS Velocity Variation with Applied Voltage

Thank You