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a Instituto Canario de Investigaciones Agrarias (ICIA), Dep. Suelos y Riegos, Apdo. 60 La Laguna, 38200 Tenerife, Spain
b Imko Micromodultechnik GmbH, Im Stöck 2, D-76275 Ettlingen, Germany
cregalad{at}icia.es
Laurent et al. (2005) proposed an empirical relationship between the permittivity, K, and the pseudo transit time, t2, measured with a TRIME TDR System (Imko GmbH, Ettlingen, Germany). Different probe designs are available for the TRIME System. Among these are access tube cylindrical probes (TRIME-T3), two-rod probes with internal electronics (e.g., TRIME-EZ or TRIME-IT), and simple waveguides without electronics connected to an external TDR instrument (such as the P2 and P2Z probes connected to a handheld TRIME-FM). The P2 probe and TRIME-IT share the same rod geometry and therefore show the same performance. The same holds for the P2Z probe and the TRIME-EZ.
The TRIME System measures the TDR-pulse transit time t1 (ps) relative to an arbitrary reference time. The TRIME coated probes with different geometries all perform differently in that they are characterized by their own specific t1 vs. water content (
) relationship. To reduce small effects of unavoidable tolerances in the electronics, mechanics, and production, a linear transformation was applied, called "basic balancing." This results in a "pseudo transit time" t2, which in fact is a normalized time of the form:
![]() | [1] |
![]() | [2] |
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, and the pseudo transit time, t2 (R2 = 0.9886):
![]() | [3] |
This equation was derived by fitting data obtained with the TRIME-T3 access tube probe on a soil sample, referred as "Cylinder container 10l 2003" (Fig. 7 in Laurent et al., 2005). The importance of Eq. [3] stems from the fact that most TDR techniques provide values of the permittivity rather than pseudo transit times. The equation hence allows either recalibration or comparison of moisture data obtained with other TDR systems using measurements carried with the TRIME System.
We derived an alternative K vs. t2 relationship from (i) measurements obtained with a TRIME-T3 access tube probe on reference materials and glass beads (Table 4 in Laurent et al., 2005), (ii) measurements obtained with a TRIME-P2 probe in two-phase mixtures of water and dioxan (Fig. 5.5 in Stacheder, 1996), and (iii) our own measurements with a TRIME-P2 probe in different media of known permittivity (Table 1).
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![]() | [4] |
Notice that the data deviate substantially from linear behavior, especially for t2 > 700 (Fig. 2a). Linearity is approached for 100 < t2 < 700, which is the range investigated by Laurent et al. (2005). This explains the different forms of Eq. [3] and [4]. As an alternative to Eq. [4], Fig. 2b presents the logarithmic K transformed vs. t2 data. Linearity is closely achieved in most of the t2 range, which causes us to propose the following K vs. t2 relationship (R2 = 0.9718):
![]() | [5] |
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Our results hence suggest that a logarithmic, rather than a square root, transformation is more appropriate for the relationship between the pseudo transit time and the permittivity with the TRIME TDR System. The transformation appears valid for the entire measurement range of the instrument as opposed to the square root transformed permittivity relationship presented by Laurent et al. (2005).
REFERENCES
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