Here, B-scan data collection of a simple ground penetrating radar (GPR) is animated through the use of Finite-difference time-domain (FDTD) method. The upper part of the animation shows the 2D spatial propagation of the short pulse transmitted from the antenna at different spatial locations. The transmitting antenna shoots a short electromagnetic pulse (with a central frequency of 600 MHz) into the subsurface where the relative dielectric permittivity is 4. The short pulse is reflected from the air-soil interface and then from the target embedded in the subsurface. Then, the scattered signals are recorded by the same antenna in the receiving mode. The lower part of the animation corresponds to the received signals (A-scan) at the same antenna for each of the positions. This constitutes the so-called B-scan data collection.
Showing posts with label B-scan. Show all posts
Showing posts with label B-scan. Show all posts
Wednesday, May 09, 2012
Tuesday, January 10, 2012
Ground Penetrating Radar (GPR) FDTD Animation
Finite-difference time-domain (FDTD) animation of a sample ground penetrating radar (GPR) in action. Basically, a transmitting antenna shoots a short electromagnetic pulse (with a central frequency of 600 MHz) into the subsurface where the relative dielectric permittivity is 4. The short pulse is reflected from the air-soil interface and then either the rectangular or circular targets embedded in the subsurface. Then, the scattered signals are recorded by the receiving antenna of the GPR unit. This constitutes a single A-scan for the GPR measurement. Collection of A-scans along a spatial range constitutes the so called B-scans. Depending on the reflectivity of the target and soil properties, the success of GPR detection varies.
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Ground Penetrating Radar - Propagation within the subsurface |
Labels:
A-scan,
antenna,
B-scan,
detection,
electromagnetics,
FDTD,
Finite-difference time-domain,
georadar,
GPR,
Ground Penetrating Radar,
Maxwell’s equations,
radar,
scatterer,
target,
ultrawideband,
UWB
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