HR: 0800h
AN: NS31B-0393 [Abstracts]
TI: Determining the Empirical Relationship Between Surface Ground Penetrating Radar (GPR) Reflection Amplitudes and Sub-wavelength "Thin-layer" Fracture Aperture Under No-flow Conditions
AU: * Burns, K E
EM: kburns5@utk.edu
AF: University of Tennessee, 1412 Circle Drive #306, Knoxville, TN 37996, United States
AU: Baker, G S
EM: gbaker@tennessee.edu
AF: University of Tennessee, 1412 Circle Drive #306, Knoxville, TN 37996, United States
AB:
Current methods of collecting data for modeling groundwater flow in fractured media (e.g., fractured bedrock)
involve expensive and invasive procedures that typically yield poorly-constrained results due to highly spatially
variable fracture apertures and the resulting channelization. Surface ground penetrating radar (GPR) surveys
present an attractive alternative because the full two-dimensional distribution of fracture aperture may be
determined. Typical fractures have sub-wavelength apertures (i.e., are considered "thin layers") and the fluid flow
through the fractures is governed by the cubic law; therefore, precise aperture estimates are critical. In practice,
researchers have observed a qualitative change in reflection amplitudes and presumed this change correlates
with fracture aperture at the sub-wavelength scale. Several researchers have attempted to determine the
relationship theoretically. One method involves a simplification of the thin-layer problem by reducing the scope of
the investigation to the first interface of the layer. This simplification reduces the thin-layer to a boundary, thereby
effectively removing the noise generated by the constructive or destructive interference generated by the second
interface. The resulting theoretical relationships describe the relationship between the reflected amplitude and
thickness of the layer (e.g., fracture aperture). We have created a physical model consisting of 2 large ultra-high
molecular weight polyethylene (UHMW-PE) blocks that have electromagnetic properties of real earth materials,
separated by thin (~0.1 mm) inserts to create a range of aperture sizes. To change the aperture, we started
by adding 1 insert for the first 51 surveys (0-5 mm) followed by 2 inserts for the next 25 surveys (5.2-10 mm),
followed by 5 inserts for the next 20 surveys (10.5-20 mm) and lastly 1 additional survey taken at 300 inserts (30
mm). At each aperture increment, a GPR survey using 1000 MHz antennae was run at the center of the block. By
directly obtaining the reflected amplitudes in an idealized fracture media, we then tested the various theoretical
equations for modeling fracture aperture. Our preliminary results are not in agreement with the model and
warrant a new empirical equation.
DE: 1835 Hydrogeophysics
DE: 1894 Instruments and techniques: modeling
SC: Near-Surface Geophysics [NS]
MN: 2007 Fall Meeting