1. Effect of cathode channel dimensions on the performance of an air-breathing PEM fuel cell
- Author
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P. Manoj Kumar and Ajit Kumar Kolar
- Subjects
Buoyancy ,Materials science ,Cathode channel ,Overpotential ,Cells ,Proton exchange membrane fuel cell ,Channel depth ,Computational fluid dynamics ,engineering.material ,Steady state ,law.invention ,Cell temperature ,Diffusion resistance ,Effect of cathode ,Governing equations ,law ,Mass transfer ,In-cell ,Channel widths ,Current distribution ,Maximum power density ,Water transport ,Voltage loss ,Three dimensional ,General Engineering ,User Defined Functions ,Buoyancy induced flow ,Cathode channel dimensions ,Single-phase model ,Mechanics ,Proton exchange membrane fuel cells (PEMFC) ,Condensed Matter Physics ,Energy–depth relationship in a rectangular channel ,Air breathing ,Cathode ,High current densities ,Species distributions ,Oxygen ,PEM fuel cell ,Nonisothermal ,Cell height ,engineering ,Cell performance ,Low current density ,Current density ,Oxygen mass transfer - Abstract
A three dimensional, steady state, non-isothermal, single phase model was developed and simulations were carried out in order to find the effect of cathode channel dimensions (width, depth and height) on the performance of an air-breathing fuel cell. The model was solved using commercial CFD package Fluent (version 6.3). Separate user defined functions were written to solve the electrochemical equations and the water transport through the membrane along with the other governing equations. Analyses were carried out for three different channel widths (2, 4 and 6�mm), for three different channel depths (2, 6 and 10�mm) and for three different cell heights (15, 30 and 45�mm). Cell characteristics like current distribution, species distribution, oxygen mass transfer coefficient, cell temperature, cathode channel velocities and net water transport coefficients are reported. The results show that the cell performance improves with increase in cathode channel width, channel depth and with decrease in cell height. Maximum power density obtained was 240�mW/cm2 for a channel width of 4�mm and channel depth of 6�mm. When the channel depth was 2�mm the performance was limited mainly due to the resistance offered by the channel for the buoyancy induced flow. For channel depths higher than 2�mm, the diffusion resistance of the porous GDL also contributed significantly to limit the performance to low current densities. At low current densities the fuel cell is prone to flooding whereas at high current densities ohmic overpotential due to dehydration of the membrane significantly contributes to the overall voltage loss. � 2009 Elsevier Masson SAS. All rights reserved.
- Published
- 2010
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