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Numerical study of the polarization effect of GPR systems on the detection of buried objects

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HAL Id: hal-01615542

https://hal.archives-ouvertes.fr/hal-01615542

Submitted on 12 Oct 2017

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Numerical study of the polarization effect of GPR

systems on the detection of buried objects

Florence Sagnard

To cite this version:

Florence Sagnard. Numerical study of the polarization effect of GPR systems on the detection of buried objects. EGU - European Geosciences Union General Assembly 2017, Apr 2017, Vienna, Austria. EGU - European Geosciences Union General Assembly 2017, 1p, 2017. �hal-01615542�

(2)

www.

ifsttar

.fr

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Context

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Polarization is a fundamental property of propagation of electromagnetic waves

that provides a unique opportunity for

producing improved images of buried objects. It helps to discriminate different classes of objects and to estimate

parameters such as

the size, shape, orientation, and electrical properties of buried objects

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The definition of the GPR system

and particularly the antenna geometry and the frequency band (UWB) contribute to

provide images where information appears more accessible before applying pre-treatments

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Numerical simulations (FDTD and FIT)

appear essential

to study the polarization effects by means of a parametric study

Simulation senarios (50 MHz-4 GHz)

Conclusion

Numerical study of the polarization effect of GPR

systems on the detection of buried objects

F. Sagnard

LEOST, COSYS, University Lille Nord de France, Villeneuve d’Ascq, France

florence.sagnard@ifsttar.fr

Sub-surface probing using GPR

Bowtie slot antenna

190.4 mm

332.2

m

m

67 mm

313

m

m

TM polarization

TE polarization

Cross polarization

air

dielectric e’=12

soil e’=5.5

s=0,01 S/m

Buried pipes

Buried pipes in trenches

Case 1

Case 2

Case 3

225 mm

250

m

m

165 mm

210

m

m

124.8

m

m

40 mm

Case 4

Leaf antenna : a novel compact antenna geometry

dielectric e’=12

Case 1 (TM)

e’=1

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Case 2 (TE)

e’=7

e’=1

e’=12

Radargrams

air-filled pipe pipe eps=12 2,2 ns direct wave without object 0,8 ns

Case 3 (TM-TE)

e’=12

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3,7 ns 4,3 ns air-filled pipe pipe eps=12

Case 4 (TM)

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frequency [MHz]

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[

d

B

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CST (lossy Copper) CST (PEC) EMPIRE (PEC) CST (ovale ground plane, PEC)

S11 in air (non shielded)

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frequency [MHz]

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S11 in air (bowtie-slot)

CST (non shielded) CST (shielded)

S11/S21 on soil (

e’=5,5)

S11 S21 Config. n°2 Config. n°1 pipe eps=12 air-filled pipe

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Case 4 (TM-TE)

e’=1

 Disymetry observed for cross-polarized antennas

 Object responses depending on the polarization to be superimposed and compared

 Effect of the antenna geometry on the direct coupling in the several polarization configurations

A parameter study to consider :

- Influence of the antenna geometry on polarization

- Contribution of the polarization to reduce the direct coupling and to improve the detection of shallow objects

- Pre-processing techniques to benefit from several components of polarization

- Quantify dielectric characteristics of buried objects

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