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Experimental investigation of the primary and secondary current distribution in a rotating cylinder Hull cell
Authors:C Madore  M Matlosz  D Landolt
Affiliation:(1) Laboratoire de Métallurgie Chimique, Département des Matériaux, Ecole Polytechnique Fédérale de Lausanne, MX-C Ecublens, CH-1015 Lausanne, Switzerland
Abstract:A rotating cylinder cell having a nonuniform current distribution similar to the traditional Hull cell is presented. The rotating cylinder Hull (RCH) cell consists of an inner cylinder electrode coaxial with a stationary outer insulating tube. Due to its well-defined, uniform mass-transfer distribution, whose magnitude can be easily varied, this cell can be used to study processes involving current distribution and mass-transfer effects simultaneously. Primary and secondary current distributions along the rotating electrode have been calculated and experimentally verified by depositing copper.List of symbols c distance between the cathode and the insulating tube (cm) - F Faraday's constant (96 484.6 C mol–1) - h cathode length (cm) - i local current density (A cm–2) - i L limiting current density (A cm–2) - i ave average current density along the cathode (A cm–2) - i 0 exchange current density (A cm–2) - I total current (A) - M atomic weight of copper (63.54 g mol–1) - n valence - r p polarization resistance (OHgr) - t deposition time (s) - V c cathode potential (V) - Wa T Wagner number for a Tafel kinetic approximation - x/h dimensionless distance along the cathode surface - z atomic number Greek symbols betaa anodic Tafel constant (V) - betac cathodic Tafel constant (V) - PHgr solution potential (V) - eegr overpotential at the cathode surface (V) - rgr density of copper (8.86 g cm–3) - kappa electrolyte conductivity (OHgr cm–1) - mgr deposit thickness (cm) - gammaave average deposit thickness (cm) - zeta surface normal (cm)
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