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Mathematically, a CPE's impedance is given by
1 / Z = Y = Q° ( j
)n
where Q° has the numerical value of the admittance (1/
|Z|) at =1
rad/s. The units of Q° are S·sn (ref
1).
A consequence of this simple equation is that the phase angle of the CPE impedance is independent of the frequency and has a value of -(90*n) degrees. This gives the CPE its name.
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1 / Z = Y = j When n is close to 1.0, the CPE resembles a capacitor, but the phase angle is not 90°. It is constant and somewhat less than 90° at all frequencies. In some cases, the 'true' capacitance can be calculated from Q° and n
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