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water orientation polarization [s], h is the parameter describing interaction of
water dipoles: 0 < h < 1. After substituting (17) in (15) we can have Im(ε) for the
electrolyte:
⎡ 1−h
hπ ⎤
( εs
− ε ∞)
⎢( ωτ ) cos
2 ⎥ σ e
Im( ε ) =
⎣
⎦
+
2
( ) ( 1−h
) 1−h
hπ
1+
ωτ + 2( ωτ ) sin
ωε 0
2
(18)
The absolute value of the complex dielectric permittivity of electrolyte, k, is:
[ Re( ε )] 2 [ Im( ε )] 2
k = ε = +
(19)
Presenting the values from Eq. (16) and Eq. (19) for different w gives the
information about the frequency dispersion of ε’ and k, ie the dependence of the
related values on the frequency of the applied electric field (Malicki [54]).
Fig. 7.
Frequency dispersion of the real part, ε’, and module, k, of the complex dielectric
constant of the electrolyte for different conductivities
Fig. 7 shows the frequency dispersion of the module, k, of the complex
dielectric permittivity of an electrolyte and the dispersion of its real value, ε’, for
the electrolyte of variable conductivity, EC a . The assumptions in the presented
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