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Capacitance layer, nonfaradaic processes

The charging of the double layer is responsible for the background (residual) current known as the charging current, which limits die detectability of controlled-potential techniques. Such a charging process is nonfaradaic because electrons are not transferred across the electrode-solution interface. It occurs when a potential is applied across the double layer, or when die electrode area or capacitances are changing. Note that the current is the tune derivative of die charge. Hence, when such processes occur, a residual current flows based on die differential equation... [Pg.21]

Residual currents, also referred to as background currents, are the sum of faradaic and nonfaradaic currents that arise from the solvent/electrolyte blank. Faradaic processes from impurities may be practically eliminated by the careful experimentalist, but the nonfaradaic currents associated with charging of the electrode double layer (Chap. 2) are inherent to the nature of a potential sweep experiment. Equation 23.5 describes the relationship between this charging current icc, the double-layer capacitance Cdl, the electrode area A, and the scan rate v ... [Pg.687]


See other pages where Capacitance layer, nonfaradaic processes is mentioned: [Pg.153]    [Pg.22]    [Pg.21]    [Pg.455]    [Pg.5]    [Pg.34]    [Pg.355]   
See also in sourсe #XX -- [ Pg.14 , Pg.15 , Pg.16 , Pg.17 ]




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