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ekS - Instytut Agrofizyki im. Bohdana Dobrzańskiego PAN w Lublinie ...

ekS - Instytut Agrofizyki im. Bohdana Dobrzańskiego 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

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