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time elapsed between when this energy is transmitted <strong>and</strong> received back at <strong>the</strong> surface is<br />

measured. The delay between <strong>the</strong> transmitted pulse <strong>and</strong> <strong>the</strong> arrival <strong>of</strong> a reflection is proportional<br />

to <strong>the</strong> depth <strong>of</strong> <strong>the</strong> subsurface feature that generated <strong>the</strong> reflection (Harari, 1996). A receiving<br />

antenna detects <strong>the</strong> waves that are reflected back up to <strong>the</strong> ground surface when <strong>the</strong> transmitted<br />

pulse encounters a subsurface interface (Harari, 1996). All sedimentary layers <strong>and</strong> o<strong>the</strong>r buried<br />

materials have particular physical <strong>and</strong> chemical properties that affect <strong>the</strong> velocity <strong>of</strong><br />

electromagnetic energy propagation. Changes in <strong>the</strong>se properties can be a result <strong>of</strong> changes in<br />

water content, grain size, porosity or mineralogy (Davis <strong>and</strong> Annan, 1989; Van Dam <strong>and</strong><br />

Schlager, 2000; Best et al., 2003). The greater <strong>the</strong> change in velocity at an interface, <strong>the</strong> higher<br />

<strong>the</strong> amplitude <strong>of</strong> <strong>the</strong> reflected wave. The antenna receives <strong>the</strong> reflected waves <strong>and</strong> stores <strong>the</strong>m in<br />

a digital control unit. The reflected signal is amplified, recorded <strong>and</strong> processed (Best et al.,<br />

2003). Once thous<strong>and</strong>s <strong>of</strong> reflections have been measured <strong>and</strong> recorded, a two-dimensional<br />

picture is created. The depth <strong>of</strong> penetration is determined by <strong>the</strong> frequency <strong>of</strong> <strong>the</strong> antenna used.<br />

Low frequency antennas (25-200 MHz) obtain subsurface reflections from great depths (30-100<br />

ft) but have low resolution. High frequency antennas (300-1000 MHz) obtain reflections from<br />

shallower depths <strong>and</strong> provide a higher resolution.<br />

A GPR transect <strong>of</strong> <strong>the</strong> isl<strong>and</strong> using a MALA CU-II GPR system was conducted. A 100<br />

MHz unshielded antenna with a 1 m separation was used. A repeat transect with a shielded 250<br />

MHz antenna <strong>and</strong> with a 50 MHz unshielded antenna was later carried out over <strong>the</strong> same<br />

transect. Figure 3.10 illustrates how <strong>the</strong> GPR surveys were carried out. All data was analyzed<br />

using MALA Ground Vision S<strong>of</strong>tware. The data was filtered for DC removal <strong>and</strong> time varying<br />

gain (TVG). The time to depth conversion assumed a velocity <strong>of</strong> 60 meters/microsecond. The<br />

GPR pr<strong>of</strong>iles were not corrected for elevation. They were conducted along a road that cut<br />

through, ra<strong>the</strong>r than over <strong>the</strong> beach ridges. The road was essentially horizontal, with a slight<br />

sou<strong>the</strong>rly dip. Therefore, <strong>the</strong> pr<strong>of</strong>ile is more or less representative <strong>of</strong> <strong>the</strong> actual depth <strong>of</strong> <strong>the</strong><br />

beach ridge reflectors. All GPR data was processed <strong>and</strong> stored at <strong>the</strong> Florida Geologic Survey.<br />

A summary <strong>of</strong> <strong>the</strong> data is presented in chapter 4.<br />

44

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