ekS - Instytut Agrofizyki im. Bohdana DobrzaÅskiego PAN w Lublinie ...
ekS - Instytut Agrofizyki im. Bohdana DobrzaÅskiego PAN w Lublinie ...
ekS - Instytut Agrofizyki im. Bohdana DobrzaÅskiego PAN w Lublinie ...
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assumed that the conductivity of soil solid phase and air is negligible). Therefore<br />
the soil dielectric permittivity is a complex value with the real part conditioned by<br />
its water content and <strong>im</strong>aginary part by its salinity. The presented discussion<br />
refers to the conditions when the dielectric measurement of soil water content is<br />
not influenced by the conductivity of the electrolyte in it. The objective of the<br />
considerations below is the determination of the frequency of the electric field<br />
applied to the soil that would allow interpreting its reaction only on the basis of<br />
water and solid phase in it.<br />
3.4.1. Frequency dispersion of the electrolyte dielectric permittivity<br />
Dielectric permittivity, ε, of an electrolyte is a complex value dependent on<br />
the frequency of the applied electric field, f. Its real, Re(ε), and <strong>im</strong>aginary Im(ε)<br />
parts have the form (Chełkowski [14], Hasted [37]):<br />
Re( ε ) = ε '<br />
(14)<br />
ECw<br />
Im( ε ) = ε"<br />
+<br />
ωε<br />
0<br />
(15)<br />
where: ε’ and ε” are real and <strong>im</strong>aginary parts of the complex dielectric<br />
permittivity of water, respectively, EC w – electrical conductivity of the electrolyte<br />
[Sm -1 ], ω - angular frequency of the applied electric field (equals to 2πf)[s -1 ], ε 0<br />
–<br />
is the dielectric permittivity of free space [Fm -1 ].<br />
The real and <strong>im</strong>aginary parts of the complex dielectric permittivity are<br />
modeled by Cole-Cole formulas [14,37]:<br />
⎡ 1−h<br />
hπ ⎤<br />
( ε<br />
s − ε<br />
∞<br />
)<br />
⎢<br />
1 + ( ωτ ) sin<br />
2 ⎥<br />
ε ' = ε<br />
∞<br />
+<br />
⎣<br />
⎦<br />
(16)<br />
( ) ( 1 h ) 1 h hπ<br />
1<br />
2 −<br />
−<br />
+ ωτ + 2( ωτ ) sin<br />
2<br />
⎡ 1−h<br />
hπ ⎤<br />
( ε<br />
s<br />
− ε<br />
∞<br />
)<br />
⎢( ωτ ) cos<br />
2 ⎥<br />
ε " =<br />
⎣<br />
⎦<br />
(17)<br />
( ) ( 1 h ) 1 h hπ<br />
1<br />
2 −<br />
−<br />
+ ωτ + 2( ωτ ) sin<br />
2<br />
−1<br />
where: ε ∞<br />
is the relative water dielectric permittivity when ω > τ , ε is the<br />
s<br />
relative dielectric permittivity of water when ω = 0, τ is the relaxation t<strong>im</strong>e of<br />
26