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Application of porous flow through electrodes: IV. Hydrogen evolution on packed bed electrodes of iron spheres in flowing alkaline solutions
Authors:B E El-Anadouli  M M Khader  M M Saleh  B G Ateya
Affiliation:(1) Chemistry Department, Faculty of Science, Cairo University, Cairo, Egypt
Abstract:Packed bed electrodes of small iron spheres have been used for the electrolytic production of hydrogen from alkaline solutions at different temperatures under conditions of electrolyte flow. The effects of temperature, electrolyte type, concentration and flow rate on the polarization behavior of the electrode were evaluated and analyzed. It was shown that increases in the conductivity of the electrolyte or the operating temperature decreases the potential required to support the reaction. The generated gas bubbles disperse in the pore electrolyte, resulting in an increase in its resistivity and, subsequently, an increase in the potential. It was shown that some gas bubbles are trapped within the porous electrode. The implications of the trapped gas bubbles on the behaviour of the electrode are discussed.Nomenclature A geometrical cross-sectional area (cm2) - a empirical constant (cm3 C–1) - b RT/F in volt, withR the gas constant,T the absolute temperature - E 0 electrode potential at the entry face (V) - E L electrode potential at the exit face (V) - F Faradays's constant - i 0 exchange current density of the electrode reaction (A cm–2) - i L experimentally measured current density at the exist face (A cm–2) - L bed thickness (cm) - q tortuosity - Q electrolyte volume flow rate (cm3 s–1) - V electrolyte flow rate,V=Q/A (cm s–1) - S specific surface area of the bed (cm–1) - x position in the electrode - agr transfer coefficient - ohgr gas void fraction - eegr0 polarization at the entry face (V) - eegrL polarization at the exit face (V) - thetav porosity - rgr pore electrolyte resistivity (OHgr cm) - rgr0 resistivity of the bubble-free pore electrolyte (OHgr cm) - eegr 0 b resistivity of the bulk electrolyte (OHgr cm)
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