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DIFFERENTIAL IMPEDANCE ANALYSIS OF CONDUCTIVITY AND ...

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the effective resistances R 1 and R 2 , the effective capacitance C and the effective time-constant T =<br />

CR 2 . More detailed information on the principle of DIA can be found in [3-6].<br />

The frequency dependence of the LOM parameters’ estimates ˆP LOM<br />

is an important step of<br />

the analysis, termed temporal analysis, since it provides information for the model structure:<br />

lg ˆP LOM = F (lgT f ), (1)<br />

where T f = 1/f is the sinusoidal period and f is the frequency. For convenience Eqn. (1) is<br />

expressed in a logarithmic form.<br />

R 2<br />

R 1<br />

-Im / Ω<br />

C<br />

Re / Ω<br />

Fig. 1. Local operating model (LOM) – first order inertial system: equivalent circuitry<br />

and impedance diagram<br />

When the structure of the LOM corresponds to that of the impedance object in a given<br />

frequency range, the parameters’ estimates have a constant behaviour, i.e. they are presented as<br />

plateaus (Fig.2b). The number of the plateaus yields the number of the time-constants in the<br />

model. For better visualisation of the results obtained by the temporal analysis, a spectral form of<br />

presentation is introduced [4]. Fig. 2c presents the effective time-constant spectrum. The rest of<br />

the parameters’ estimates have the similar spectra.<br />

- Im / Ω<br />

200<br />

a)<br />

0.1Hz<br />

100<br />

10Hz<br />

10mHz<br />

100Hz 1Hz<br />

1mHz<br />

0<br />

0 100 200 300 400<br />

Re / Ω<br />

lg P^<br />

4<br />

2<br />

0<br />

-2<br />

-4<br />

I III II<br />

^<br />

T / s<br />

^<br />

C / F<br />

b)<br />

-3 -2 -1 0 1 2 3<br />

lg (T / Hz -1 )<br />

F<br />

^<br />

R 2 / Ω<br />

Intensity / dB<br />

45<br />

30<br />

15<br />

I<br />

III<br />

c)<br />

0<br />

-6 -4 -2 0 2 4 6<br />

lg T^<br />

II<br />

Fig. 2. DIA of synthetic model of two steps Faradic reaction: a) impedance diagram;<br />

b) temporal plots; c) effective time-constant spectrum.<br />

The regions where the LOM parameters’ estimates are frequency dependent (segment III<br />

in Figs.2b,c) need an additional examination with the so-called Secondary Differential Impedance<br />

Analysis [7-10]. It works with the derivatives of the LOM parameters’ estimates with respect to<br />

the frequency:<br />

P13-2

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