GPR THEORY OF OPERATION

GPR uses high frequency pulsed electromagnetic (EM) waves (typically from 10 MHz to 1,000 MHz) to acquire subsurface information. Energy is propagated downward into the ground and is reflected back to the surface from boundaries at which there are EM property contrasts (Annan, 1992, Daniels, 1989). GPR equipment utilized for the measurement of subsurface conditions normally consists of a transmitter and receiver antenna, a radar control unit, and suitable data storage and/or display devices. A circuit within the radar control unit generates trigger pulses that are sent simultaneously to the transmitter and receiver electronics. The transmitter electronics produce output pulses that are radiated into the ground from the transmitting antenna, and the receiver is turned on to wait for radar energy that is transmitted into the subsurface. When the transmitted radar energy encounters and abrupt change in the EM properties (primarily the relative dielectric permittivity) of the subsurface, a portion of the energy is reflected back to the radar antenna and the remaining energy is transmitted downward to deeper material. The reflected EM energy is detected by the receive antenna, and these signals are sent to the control unit for amplification. As the antenna(s) are moved along a survey line, a series of scans are collected at discrete points along the line. These scans positioned side by side to form a display profile of the subsurface.


Schematic diagram of a ground penetrating radar system.


 

 

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