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Anomalies
produced by objects or features of small size (relative to the antenna
frequency and other factors), like rocks, pipes, or a narrow wall, produce
hyperbolas in GPR data. The shape of a hyperbola, in particular
its relative width or roundness, is determined by the velocity of the
radar energy in the medium under consideration, so measurement of its
form can yield an estimate of velocity. It is possible to perform the
measurements manually, but modern software allows automation of this
task through direct computer measurement of hyperbolic form. The most
accurate procedure for determining soil velocity is to identify GPR
reflections to objects of known depths through a pipe test, for example.
This figure shows
a GPR profile obtained with a GSSI
400 MHz antenna. The tick marks at top represent meter marks obtained
with a survey wheel, using 50 scans/m. The range setting was 40 nS (10-9
seconds) two-way travel time (TWTT). The ground surface reflection is
approximately at 3 nS while the peak of the hyperbola is at approximately
13 nS. This anomaly was created by inserting a steel pipe (a one-inch
soil corer) horizontally into a vertical exposure, illustrated elsewhere
as a pipe test.
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Modern
GPR software allows the fitting of a mathematically generated
hyperbola to the anomaly. The soil velocity determines its width
or roundness. If soil velocity is very high, as might occur in
a dry sand with a low relative dielectric permittivity (RDP),
the hyperbola tends to be very wide. If the velocity is low, as
in a clay with high RDP, the hyperbola is very narrow. Here, the
hyperbola (in red) fitted with GSSI's RADAN software, indicates
a soil velocity of approximately 0.1 m/nS. This figure agrees
exactly with the results of the pipe test.
To
see an animation of how hyperbola form varies with soil velocity
click
here.
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Relative Dielectric
Permittivity (RDP)
With
an estimate of soil velocity the relative dielectric
permittivity (K) may be computed:
K
= C / V
where
C = speed of light in a vacuum (0.2998 m/nS) and V = velocity
of radar energy as it passes through a material (in m/nS), so:
K
= 0.2998 m/nS / 0.1 m/nS = 2.998,
and
K
= 8.99
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