The double-layer impedance of a porous electrode is generally modelled
by a transmission-line model or by invoking fractal geometry. In a ni
ckel oxide electrode at low state-of-charge, however, the porosity doe
s not affect significantly the impedance of the electrode below 100 Hz
. Even then, the double-layer impedance cannot be represented by a pur
e capacitor. The reasons for this are to be found in the physical natu
re of the impregnated active material. Based on a phenomenological the
ory, the double-layer impedance can be modelled by a set of resistor/c
apacitor elements connected in parallel.