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Time‐Domain Reflectometry Probe for Water Content and Electrical Conductivity Measurements in Saline Porous Media
Author(s) -
Persson Magnus,
Bendz David,
Flyhammar Peter
Publication year - 2004
Publication title -
vadose zone journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.036
H-Index - 81
ISSN - 1539-1663
DOI - 10.2136/vzj2004.1146
Subject(s) - reflectometry , rod , materials science , coating , dielectric , porosity , composite material , porous medium , electrical conductor , conductivity , time domain , chemistry , optoelectronics , medicine , alternative medicine , pathology , computer science , computer vision
A new coated time‐domain reflectometry (TDR) probe design is described and evaluated. In contrast to previous coated TDR probes, our probe may be used to measure both the dielectric constant ( K a ) and bulk electrical conductivity (σ a ) in saline porous media. This was made possible by attaching two coaxial cables to a 0.27‐m three‐rod probe with a coated central rod. The shield of the first cable was connected to one of the outer rods and the conductor was connected to the coated central rod. The conductor and shield of the other coaxial cable were connected to each of the two outer rods, respectively. Thus, our probe consists of two unbalanced, two‐rod probes. The probe is called coated–uncoated probe (CUP). Four prototypes with two different coating materials (i.e., polyolefin and kynar heat‐shrink tubes) were evaluated. The probes were calibrated in several fluids having different K a and σ a The K a measurement of the coated part of the probe was successfully fitted to target K a using a two‐phase dielectric mixing model. Due to signal attenuation, measurements of K a were not possible for σ a higher than 9 dS m −1 for the polyolefin‐coated probes whereas the upper limits for the kynar‐coated probes and the uncoated probe were 5 and 2.5 dS m −1 , respectively. Measurements of σ a are only possible with the uncoated part. Measurements of K a and σ a were also taken during three upward infiltration experiments in sand using soil solution electrical conductivities of 0.01, 6.31, and 12.03 dS m −1 For the uncoated part, K a could not be measured when σ a was higher than about 2 dS m −1 , whereas K a measurements were possible using the coated part even when σ a was 3 dS m −1

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