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134 CHAPTER 3. TERRESTRIAL SYSTEMS<br />
3.1.13 Simulation and Observation of an Evanescent Wave in Ground Penetrating<br />
Radar Applications<br />
Participating scientist Holger Gerhards, Benedikt Oswald<br />
Abstract A radiating dipole near a single boundary layer was simulated to observe air and ground<br />
wave occurring in Ground Penetrating Radar applications. A semi-analytical approach to solve<br />
Maxwell’s equations in frequency domain with Green’s functions was used. The evanescent characteristic<br />
of the ground wave in air was demonstrated theoretically and experimentally.<br />
x<br />
air<br />
soil<br />
(4)<br />
(3)<br />
(1)<br />
antenna<br />
z<br />
(2)<br />
Background Ground Penetrating Radar<br />
(GPR) is a fast and nondestructive electromagnetic<br />
method to do near subsurface explorations<br />
to estimate soil water content. Reflections are<br />
measured, which occur at boundaries with a dielectric<br />
contrast. Because the relative dielectric<br />
permittivity (εw ≈ 81) of water is much higher<br />
than the soil matrix (εs ≈ 3) in the used frequency<br />
range between 0.1 to 1.0 GHz and assuming that<br />
high water content changes coincides with soil<br />
layers, temporal changes of water content can be<br />
easily detected analyzing travel times.<br />
As shown in Fig. 3.13 for a two layer (air/soil)<br />
model a direct wave from transmitter to receiver<br />
in air and another in the soil can be observed. The<br />
measured ground wave in the air has an evanescent<br />
character, which means, that its amplitude<br />
decays exponentially with the height of the receiving<br />
antenna over the soil. The knowledge about<br />
this phenomena can help to separate the interfering<br />
air and ground waves or to obtain information<br />
about the dielectric properties of the soil surface.<br />
Funding DFG RO 1080 / 10-1<br />
Methods and results A radiating dipole<br />
within a two layer medium was modeled using a<br />
semi-analytical approach based on a spectral decomposition<br />
of the Green’s functions in frequency<br />
domain. The obtained electric field components<br />
were transformed into time domain to be able to<br />
compare the simulation with field measurements.<br />
Figure 3.13: Propagation modes at a single<br />
boundary layer; (1) and (2) spherical wave like<br />
propagation modes in the according material,<br />
(3) ground wave coupling in air (evanescent<br />
wave), (4) air wave coupling in soil (lateral/head<br />
wave)<br />
The exponential decay and its frequency dependence<br />
can be shown by analyzing the amplitudes<br />
of the ground wave wavelet and its shape with<br />
increasing height above the soil.<br />
Analogous to the simulation experiments were<br />
arranged, where the evanescent behavior of the<br />
ground wave was verified and therefore validates<br />
the semi-analytical approach. Furthermore, it was<br />
shown, how far the ground wave interferes with<br />
the air wave.<br />
To obtain insight on the parameters that determine<br />
the attenuation, an equation was derived<br />
from the plane wave approach used in optics. The<br />
dependency on frequency and dielectric contrast<br />
was obtained, which can be qualitatively shown<br />
with the simulated and measured time signals.<br />
Outlook/Future work A frequency analysis<br />
must be applied to check the derived frequency<br />
dependence for experimental data. If air and<br />
ground waves interfere with each other, a quantitative<br />
separation must be developed, such as using<br />
a wavelet analysis. Furthermore, the semianalytical<br />
approach will be extended to simulated<br />
multilayered models, which may help to understand<br />
the depth-dependency of the ground wave<br />
when a near subsurface water content gradient exists.<br />
Main publication Gerhards, Holger, Diplomarbeit,<br />
<strong>Universität</strong> Jena, 2004