CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
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Chapter 3<br />
corrosion science in recent years due to development of sophisticated electronics which employs<br />
latest digital electronics and computer control overcoming the earlier limitations.<br />
EIS study is carried out in properly designed standard electrochemical cell consisting of<br />
specimen as working electrode, counter electrode, and a reference electrode as shown in Fig. 3.8<br />
[93]. The basic design feature of the electrochemical cell is to measure the impedance at the<br />
working electrode-electrolyte interface only, and to eliminate the impedance contribution from the<br />
counter electrode. This is done by making the resistance of the counter electrode negligible<br />
compared to that of working electrode, and capacitance of the counter electrode very large<br />
compared to that of working electrode [98]. Since, resistance in series add and capacitance in<br />
series add reciprocally, the influence of the counter electrode can be eliminated by making its area<br />
large compared to that of working electrode. Often platinised platinum with large area is used as<br />
counter electrode.<br />
In EIS measurements a perturbing sinusoidal voltage E = E 0 Sin (t) with frequency is<br />
applied to the electrode system under test [95,102,103]. The response is analysed in terms of the<br />
resultant current I = I 0 Sin (t + ), where represents a characteristics phase angle shift. The<br />
frequency response is analyzed by instruments known as Frequency Response Analyzers (FRA)<br />
interfaced with potentiostat. Frequency response analyzer provides scope for studying wide range<br />
of frequencies, faster analysis, and removal of harmonic distortions. The corresponding complex<br />
impedance spectrum Z() obtained by varying the signal frequency is expressed in terms of<br />
displacement vector Z(). In the plane of cartesian coordinates impedance is expressed by its real<br />
and imaginary parts as presented in Eq. 8.<br />
Z() = Z Re + jZ Im. (8)