Electrical double-layer properties of variously treated Bi͑001͒ and Bi͑111͒ electrodes were studied in terms of the Debye length dependent roughness theory ͑i.e., nonlinear Poisson-Boltzmann theory͒, recently developed by Daikhin et al. The geometrical roughness factor, root mean square ͑rms͒ departure of the surface from flatness, the medium lateral correlation length values have been obtained. According to the experimental data and results of theoretical calculations, the surface roughness increases in the order of Bi electrodes: electrochemically polished single-crystal Bi͑111͒ plane Ͻ cut at the temperature of liquid nitrogen Bi͑111͒ plane Ͻ electrochemically etched Bi͑111͒ plane Ͻ chemically etched Bi͑111͒ plane Ͻ chemically etched Bi͑001͒ plane. This order of the electrode surface roughness is in agreement with the ex situ AFM data, i.e., with the rms roughness R ms values. At small electrolyte concentrations (c el р 0.01 M), the deviation of experimental roughness function vs. inverse Debye length curves from the theoretically calculated ones has been observed, which is explained by the influence of energetic inhomogeneity of the polycrystalline surfaces, i.e., the nonequal surface charge density values at the various homogeneous regions exposed at the macropolycrystalline electrode surface, on the interfacial capacitance values.The phase-boundary structure and adsorption properties, as well as the kinetics of various interfacial reactions at the solid surfaces depend significantly, not only on the chemical composition, but also on the morphology of the surface studied. 1-4 Thus, the surface roughness is an important property in electrochemistry of solid electrodes as the most of electric double-layer and adsorption characteristics, as well as kinetic parameters are extensive quantities and are referred to the unit apparent area ͑flat cross-sectional area͒ of the electrode surface. The examination of the working area of solid electrodes is a difficult matter owing to the irregularities at a submicroscopic level. For the determination of the real surface area of the solid electrodes different in situ and ex situ methods have been proposed and used. The in situ methods more commonly used in electrochemistry to obtain the surface roughness R ϭ S real /S geom ͓where S real and S geom are the real ͑working͒ surface and geometrical, so-called flat gross section surface area, respectively͔ are: ͑i͒ differential capacitance measurements in the region of ideal polarizability, 1-5 Parsons-Zobel plot method, 9 Valette-Hamelin approach, 7 and other similar methods; 1-5 ͑ii͒ mass transport under diffusion control with assumption of homogeneous current distribution; 12 ͑iii͒ adsorption of ratio-active organic compounds, hydrogen, oxygen as well as metal monolayers; 5,12 (iv) microscopy ͑optical, electron, scanning tunneling microscopy ͑STM͒, and atomic force microscopy ͑AFM͒; [2][3][4][5][14][15][16]24,25 (v) quartz microbalance, 16 as well as a number of ex situ methods. 1-5 It is to be noted that depending on the irr...