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Semicircle Rotation of the Impedance

From Equations 3.102 and 3.103, the real and imaginary parts of the total impedance can be calculated  [Pg.118]

Dividing both denominator and nominator by (cobRctCd)2, Equation 3.105 becomes [Pg.119]

Adding (, ty + (—eJ—)2 to both sides of the above equation, we obtain [Pg.119]

Now let us calculate the length of the chord using the polar coordinates. The total complex admittance Y and complex impedance Z in the polar coordinates can be [Pg.120]


In the study of impedance plots, we may observe the depression of semicircles. This is the so-called semicircle rotation of the impedance. This phenomenon is associated with electrode/electrolyte interface double-layer properties. For example, the rough surface of the electrodes or porous electrodes can result in an uneven distribution of the double-layer electric field. This semicircle rotation can be explained using the equivalent circuit presented in Figure 3.10, where R is inversely proportional to the frequency CO (and b is a constant). [Pg.118]

Figure 3.10. Equivalent circuit for explaining the semicircle rotation of the impedance... Figure 3.10. Equivalent circuit for explaining the semicircle rotation of the impedance...

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