Ground Penetrating Radar
GRORADAR™ by Gary R. Olhoeft, PhD
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Introduction and History        Electromagnetic Wave Propagation

Velocity   Wavelength    Attenuation   Dispersion

"Among the more profound questions of geologic science are several whose solution requires a knowledge of the chemical and physical properties of rocks...
...and the subject calls urgently for special experimentation."
-John Wesley Powell
Report of the Director
U.S. Geological Survey
1882

Electrical Properties of Rocks, Soils and Fluids

[Under Construction]

     The electrical and magnetic properties of rocks, soils and fluids (natural materials) control the speed of propagation of radar waves and their amplitudes.  In most cases, the electrical properties are much more important than the magnetic properties.  At radar frequencies, electrical properties are dominantly controlled by rock or soil density, and by the chemistry, state (liquid/gas/solid), distribution (pore space connectivity) and content of water.

     Electrical properties (Robert, 1988) come in two basic types: one that describes energy dissipation and one that describes energy storage.   Electrical dissipation comes as the result of charge motion (or transport) called conduction.  Electrical conductivity is the ability of a material to transport charge through the process of conduction, normalized by geometry to describe a material property.   Dissipation (or energy loss) results from the conversion of electrical energy to thermal energy (Joule heating) through momentum transfer during collisions as the charges move.    Electrical storage is the result of charge storing energy when the application of an external force moves the charge from some equilibrium position and there is a restoring force trying to move the charge back.  This process is dielectric polarization, normalized by geometry to be the material property called dielectric permittivity.  As polarization occurs, causing charges to move, the charge motion is also dissipative. (See the animation in the CHARGE.EXE program.)
     In either case, charge motion is described by the diffusion equation.  Charges moving with finite velocity result in frequency dependent properties described by overdamped harmonic oscillators and the Debye single relaxation equation (Pellat, 1897; Debye, 1929) at frequencies below tens of gigahertz.  Adding the storage force balance in the acceleration term to the diffusion equation results in a wave propagation equation.  The combined electrical and magnetic storage (polarization) terms through the properties of dielectric permittivity and magnetic permeability control the velocity of electromagnetic wave propagation.
     Electrical polarization is the result of a wide variety of processes, including polarization of electrons in orbits around atoms, distortion of molecules, reorientation of polar moelcules (like water molecules), accumulation of charge at interfaces, and electrochemical reactions.  Nearly all polarization of importance in earth materials is the result of some interaction involving water (Franks, 1970).  The dominant mechanisms of electrical conduction are ionic charge transport through water filling pore spaces in rocks and soils.
     The electrical mechanisms of importance to ground penetrating radar are (Olhoeft, 1984, 1987, 1994, 1998, 2000):
1) electrical conduction losses, mostly from metals, salt water, and other good conductors which dissipate the energy as heat:  these are good reflectors, easy to see with radar, but impossible to see through or past (radar can see through fresh water).
2) dielectric polarization relaxation by rotational orientation of the water molecule: a >10 GHz process in free water, but in the 10 kHz range in ice, 10 MHz range in clathrate hydrates, and at frequencies from 100 Hz to 100 MHz caused by interactions inside pore structures.  These losses are proportional to the amount of free or mobile water present.
3) electrochemical polarization at the interface between water and clay minerals like montmorillonite, caused by the active surface chemistry and high surface areas.  This is  important below 100 MHz.  This is not an important process in finely ground "rock flour" engineering size fraction clays which have high surface areas but low chemical reactivity.
4) scattering as the wavelength of propagating energy is sent in random directions by scales of geological heterogeneity comparable to the wavelength.  Pea gravel becomes important above 1 GHz.  This is akin to the difference between an ice cube and a snowball to visible light.  They are both made of the same material (ice), but the grain size distribution in the snow is comparable to the wavelength of light, causing scattering, and making the snow look white and opaque compared to the transparent ice cube.  Scattering is both good and bad.   If there is no scattering, then there is nothing for the radar to see.  If there is too much scattering, then the radar can't  see anything through the scatter.   Desirable scattering is called a target or a reflector and undesirable scattering is called clutter.
    These electrical mechanisms create frequency dependence resulting in dispersion (frequency dependent velocity and attenuation that change pulse shape with distance of propagation), contrast resulting in scattering, and they cause energy losses which limit depth of  investigation.  Energy is also lost in magnetic relaxation and by geometric spreading losses (see radar equation).  Geometric spreading losses result as the propagating wavefront expands away from the source (transmitter) antenna, and the power is spread over the surface of the antenna pattern (much like being spread over the surface area of a balloon expanding about the antenna).

(Shivola, 1999)

(BHS mixing formula)

(properties of water equations)

(figures showing frequency dependence with water content)

(Cole-Cole equation)

Dielectric Properties of Body Tissues at RF and Microwave Frequencies

Magnetic Properties       Environmental Influences        Heterogeneity, Anisotropy and Scale       Radar Equation

Scattering     Polarization     Fresnel Reflection     Snell Angle       Stokes-Mueller Matrices      Poincare Sphere

Antennas     Coupling     Near / Far Fields     Waveguides   Multipathing     Resonance

Survey Design     Contrast     Geometry      Resolution     Depth of  Investigation     Orientation  

Noise     Interference     Logistics

Data Acquisition   Data Processing   Modeling   Interpretation   Uncertainty

Applications:     Noninvasive Surface     Borehole      Airborne     Satellite and Space  

GPR Bibliography

 
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