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Effects of gas bubbles on the current and potential profiles within porous flow-through electrodes
Authors:B E El-Anadouli  B G Ateya
Affiliation:(1) Chemistry Department, Faculty of Science, Cairo University, Cairo, Egypt
Abstract:This paper presents a mathematical model to calculate the distributions of currenti(x), potentialE(x), gas void fraction epsi(x) and pore electrolyte resistivity rhov(x) within porous flow-through electrodes producing hydrogen. It takes into consideration the following effects: (i) the kinetics of the interfacial charge transfer step, (ii) the effect of the non-uniformly generated gas bubbles on the resistivity of the gas-electrolyte dispersion within the pores of the electrode rhov(x) and (iii) the convective transport of the electrolyte through the pores. These effects appear in the form of three dimensional groups i.e.K=i o agrL where io is the exchange current density, agr is the specific surface area of the electrode andL its thickness.ugr=rgr 0 L wherergr 0 is the pore electrolyte resistivity and tau=piv/lambdaQ where piv is a constant, lambda=tortuosity/porosity of the porous electrode andQ is the superficial electrolyte volume flow rate within it. Two more dimensionless groups appear: i.e. the parameter of the ohmic effect Delta=KPHgr/b and the kinetic-transport parameterI=Ktau. The model equations were solved fori(x),E(x), epsi(x) and rhov(x) for various values of the above groups.Nomenclature agr specific surface area of the bed, area per unit volume (cm–1) - b RT/F in volts, whereR is the gas constant,T is the absolute temperature (K) - B =1–(I 2 Z/4betaDelta)], Equation 9a - C =radic(1–B 2), Equation 9b - E(L) potential at the exit face (V) - E(0) potential at the entry face (V) - E(x) potential at distancex within the electrode (V) - E rev reversible potential of the electrochemical reaction (V) - F Faraday's constant, 96500 C eq–1 - i o exchange current density of the electrode reaction (A cm–2 of true surface area) - i(L) current density at the exit face (A cm–2 of geometrical cross-sectional area of the packed bed) - I K tau=i oagrL(part/lambdaQ) (dimensionless group), Equation 7d - K =i oagrL, effective exchange current density of the packed bed (A cm–2) Equation 7a - L bed thickness (cm) - q tortuosity factor (dimensionless) - Q superficial electrolyte volume flow rate (cm3 s–1) - x =position in the electrode (cm) - Z =exp betaeegr(0)], Equation 7f - beta transfer coefficient, beta=0.5 - Delta =Kphgr/b=(i 0 agrLrgr 0 L)/b (dimensionless group) Equation 7e - epsi(x) gas void fraction atx (dimensionless) - phiv =rgr 0 L, effective resistivity of the bubble-free pore electrolyte for the entire thickness of the electrode (OHgr cm2) - eegr(0) polarization at the entry face (V) - eegr(L) polarization at the exit face (V) - lambda =q/theta, labyrinth factor - part constant (cm3 C–1), Equation 3a - tau =delta/lambdaQ (A –1) conversion factor, Equation 3b - theta porosity of the bed - rhov(x) effective resistivity of the gas-electrolyte dispersion within the pores (OHgr cm) - rgr 0 effective resistivity of the bubble-free pore electrolyte (OHgr cm)
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