EGEE 520 project presentation

Slides:



Advertisements
Similar presentations
Presented by: Bradley Fontenault Rensselaer Polytechnic Institute General Dynamics Electric Boat Corresponding Author: Ernesto Gutierrez-Miravete Rensselaer.
Advertisements

Atkins & de Paula: Atkins’ Physical Chemistry 9e
Selective Catalytic Reduction (SCR) by NH 3 in a Fixed-Bed Reactor HEE JE SEONG The Department of Energy and Geo-Environmental Engineering The Pennsylvania.
Hongjie Zhang Purge gas flow impact on tritium permeation Integrated simulation on tritium permeation in the solid breeder unit FNST, August 18-20, 2009.
Example: Electrokinetic valve
Modeling in Electrochemical Engineering
Adsorptive Desulfurization of Liquid Hydrocarbons: Langmuir Adsorption modeling using COMSOL Ram EGEE 520 Spring 2007.
Chemistry 232 Transport Properties.
Transport phenomena in chemical processes part II Michał Araszkiewicz PhD.
CHE/ME 109 Heat Transfer in Electronics
Thermal Development of Internal Flows P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Concept for Precise Design ……
LINEAR SECOND ORDER ORDINARY DIFFERENTIAL EQUATIONS
1-D Steady Conduction: Plane Wall
Fluid Dynamics and Heat Transfer in a Hartmann Flow RPI Master’s Project Proposal Timothy DePuy – 9/28/2010.
Flow and Thermal Considerations
CHE/ME 109 Heat Transfer in Electronics LECTURE 5 – GENERAL HEAT CONDUCTION EQUATION.
Impedance Spectroscopy Study of an SOFC Unit Cell
Heat Transfer Rates Conduction: Fourier’s Law
MECHANISMS OF HEAT TRANSFER
Heat Transfer Lecture 1.
Heat Transfer: Physical Origins and Rate Equations
Membrane Transport Chapter 6.
STEADY HEAT TRANSFER AND THERMAL RESISTANCE NETWORKS
Qixiu Li Prof. Derek Elsworth EGEE
INTRODUCTION TO CONDUCTION
LOGO Heat Exchanger with cooling fins Hyun Jae Kim EGEE 520, Mathematical Modeling.
One Dimensional Non-Homogeneous Conduction Equation P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi A truly non-homogeneous.
Section 1 Temperature and Heat. Kinetic Theory  All objects (even people) are made of particles and atoms that constantly and randomly move. All atoms.
Modeling of Rock Structure Changes due to Stress Induced by CO 2 Sequestration EGEE 520 – 2007 Denis Pone.
Fluid Dynamics and Heat Transfer in a Hartmann Flow RPI Master’s Project Update Timothy DePuy – 11/15/2010.
Polarization.
Modelling & Simulation of Chemical Engineering Systems Department of Chemical Engineering King Saud University 501 هعم : تمثيل الأنظمة الهندسية على الحاسب.
By: Narendra Babu N M110247ME THERMAL ANALYSIS OF MICROPROCESSOR.
Heat transfer gradient through the reactor
Chapter 1: Fourier Equation and Thermal Conductivity
Convection: Internal Flow ( )
EGEE 520 A 2-D Diesel Particulate Filter Regeneration Model Yu Zhang.
Chapter 5 Thermal Energy
Sarthit Toolthaisong FREE CONVECTION. Sarthit Toolthaisong 7.2 Features and Parameters of Free Convection 1) Driving Force In general, two conditions.
HW/Tutorial # 1 WRF Chapters 14-15; WWWR Chapters ID Chapters 1-2
Heat Transfer: Physical Origins and Rate Equations Chapter One Sections 1.1 and 1.2.
Heat Transfer: Physical process by which thermal energy is exchanged between material bodies or inside the same body as a result of a temperature difference.
Heat Transfer Introduction and Conduction. Conduction  If a temperature gradient exits in a continuous substance, heat can flow unaccompanied by any.
HW/Tutorial # 1 WRF Chapters 14-15; WWWR Chapters ID Chapters 1-2 Tutorial #1 WRF#14.12, WWWR #15.26, WRF#14.1, WWWR#15.2, WWWR#15.3, WRF#15.1, WWWR.
Chemistry 232 Transport Properties. Definitions Transport property. The ability of a substance to transport matter, energy, or some other property along.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 8 Internal flow.
Chapter 1. Essential Concepts
* Materials that allow heat, electricity, or sound waves to pass through them.
Bulk Electrolysis: Electrogravimetry and Coulometry
AFE BABALOLA UNIVERSITY
Hamdache Abderrazaq 1*, Belkacem Mohamed 1, Hannoun Nourredine 2
Heat Transfer: Physical Origins and Rate Equations
Chapter 8: Internal Flow
HW/Tutorial # 1 WRF Chapters 14-15; WWWR Chapters ID Chapters 1-2
MODELING A METAL HYDRIDE HYDROGEN STORAGE SYSTEM
Fourier’s Law and the Heat Equation
Extended Surface Heat Transfer
Heating and Cooling, the art of Thermal Energy
UNIT - 4 HEAT TRANSFER.
Fundamentals of Heat Transfer
Chapter Three Section 3.5, Appendix C
Reactive transport of CO2 in a brine cavity
Heat Transfer: Physical process by which thermal energy is exchanged between material bodies or inside the same body as a result of a temperature difference.
Heat Exchangers Heat Exchangers.
Heat Transfer.
Chemical Engineering Department
What are Fins ? Fins are extended surfaces used to increase the rate of heat transfer. It is made of highly conductive materials such as aluminum.
Fundamentals of Heat Transfer
Heat Transfer: Physical process by which thermal energy is exchanged between material bodies or inside the same body as a result of a temperature difference.
Presentation transcript:

EGEE 520 project presentation Electrodeposition of charged particles onto fuel cell coolant channel walls Chao Xie Good evening, every one! Our topic today is heat transfer gradient through the reactor. EGEE 520 project presentation 5/1/2007

Introduction A fuel cell is an electrochemical energy conversion device that is able to covert externally supplied H2 to electricity with a very high efficiency. During the operation period a huge amount of heat will be produced, which needs a cooling system to ensure fuel cells to run in an appropriate temperature range. After long-term operation charged particles can leach into the coolant, and be attracted onto the coolant channel walls via electrodeposition. This phenomenon is believed to impair the cooling effect of the coolant.

Governing equations Electrodeposition is a complex multidimensional process that include transport of charged particles via diffusion, electromigration, and convection in the coolant, as well as their sorption on the coolant channel walls . 1. Coolant fluid flow Fluid flow in the coolant channel follows Narier-Stokes equations: 2. Convection, migration and diffusion of charged particles in the coolant 3. Sorption of charged particles onto the walls The Random Sequential Adsorption model

Formulation Assumptions: 1. The charged particles are in a suspension so dilute that they do not experience significant agglomerations. 2. Given the dilute nature of the suspension, the removal of particles from the fluid over time is not expected to affect the hydrodynamic properties of the coolant. 1. Steady-state process, 2. Ignore contact thermal resistance between each boundary, 3. Thermal conductivity for each material is constant in every direction, 4. The radiation from steel to ambient can be neglected.

Solution The charged particle concentrations in the coolant channel (left: T=20 S; right: T= 35 S)

Validation Electrodeposition of charged particles onto coolant channel walls occur in two stages The plot of depositions of charged particles with different sizes versus deposition time. 1. The surfaces are free of charged particles Coolant channel wall The deposition rate is predominantly determined by the interaction between charged particles and the wall. 2. The surfaces are covered by particles Coolant channel wall The charged particles already adsorbed onto the surfaces have great influences on the subsequent particle sorption onto the wall. 1st stage 2nd stage

Parametric Study Charged particle concentrations in the channel at different particle’s concentrations (left: 0.5 x 10-7 M; right: 5 x 10-7 M)

Conclusion 1. COMSOL Multiphysics has proven to be a powerful tool to predict the electrodeposition processes of charged particles onto fuel cell coolant channel walls. 2. The predicted charged particle deposition rates are not uniform along the channel. More depositions occur near the inlet region. 3. The concentration of particles has a remarkable effect on their depositions onto the walls, i.e., the higher the concentration of particles in the coolant, the more the depositions occur. 4. It was proven that charged particle electrodeposition onto the walls is fairly sensitive to the particle sizes. If the particle sizes are out of nanoscale (1-100 nm), the bulk charged particles will exhibit distinct electrodeposition behaviors as compared with nanosized particles.

Questions?