2010
DOI: 10.5098/hmt.v1.1.3008
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On Modeling of Heat and Mass Transfer and Other Transport Phenomena in Fuel Cells

Abstract: Depending on specific configuration and design, a variety of physical phenomena is present in fuel cells, e.g., multi-component gas flow, energy and mass transfer of chemical species in composite domains and sites. These physical phenomena are strongly affected by chemical/electrochemical reactions in nano-/micro-scale structured electrodes and electrolytes. Due to the electrochemical reactions, generation and consumption of chemical species together with electric current production take place at the active su… Show more

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Cited by 3 publications
(3 citation statements)
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“…As mentioned earlier, different Nu numbers are defined for H -3 T boundary condition. 8,15 Two different Nu numbers are used, Nu q for porous wall (surface of constant heat flux) and Nu T for nonporous walls (constant temprature surfaces).…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…As mentioned earlier, different Nu numbers are defined for H -3 T boundary condition. 8,15 Two different Nu numbers are used, Nu q for porous wall (surface of constant heat flux) and Nu T for nonporous walls (constant temprature surfaces).…”
Section: Resultsmentioning
confidence: 99%
“…boundary condition. 8,15 Two different Nu numbers are used, Nu q for porous wall (surface of constant heat flux) and Nu T for nonporous walls (constant temprature surfaces). Figure 11 shows the distribution of Nu q versus wall Reynolds numbers for different aspect ratios.…”
Section: Friction Coefficient and Velocity Distributionmentioning
confidence: 99%
“…where q includes the heat generated by the current flow through the electrodes (Ohmic losses) and the activation losses, and the heat due to chemical reactions. Once again additional terms such as heat terms due to convection and radiation appear as boundary conditions [30,31,32].…”
Section: The Electrodesmentioning
confidence: 99%