【国外标准】 Standard Guide for Using the Surface Ground Penetrating Radar Method for Subsurface Investigation

5.1 Concepts—This guide summarizes the equipment, field procedures, and data processing methods used to interpret geologic conditions, and to identify and provide locations of geologic anomalies and man-made objects with the GPR method. The GPR uses high-frequency EM waves (from 10 to 3000 MHz) to acquire subsurface information. Energy is propagated downward into the ground from a transmitting antenna and is reflected back to a receiving antenna from subsurface boundaries between media possessing different EM properties. The reflected signals are recorded to produce a scan or trace of radar data. Typically, scans obtained as the antenna(s) are moved over the ground surface are placed side by side to produce a radar profile. 5.1.1 The vertical scale of the radar profile is in units of two-way travel time, the time it takes for an EM wave to travel down to a reflector and back to the surface. The travel time may be converted to depth by relating it to on-site measurements or assumptions about the velocity of the radar waves in the subsurface materials. 5.1.2 Vertical variations in propagation velocity due to changing EM properties of the subsurface can make it difficult to apply a linear time scale to the radar profile (Ulriksen (31)). 5.2 Parameter Being Measured and Representative Values:  5.2.1 Two-Way Travel Time and Velocity—A GPR trace is the record of the amplitude of EM energy that has been reflected from interfaces between materials possessing different EM properties and recorded as a function of two-way travel time. To convert two-way times to depths, it is necessary to estimate or determine the propagation velocity of the EM pulses or waves. The relative permittivity of the material (εr) through which the EM pulse or wave propagates mostly determines the propagation velocity of the EM wave. The propagation velocity through the material is approximated using the following relationship (see full formula in Balanis (32)): where: c   =   propagation velocity in free space (3.00 × 108m/s), Vm   =   propagation velocity through the material, and εr   =   relative permittivity. It is assumed that the magnetic permeability is that of free space and the loss tangent is much less than 1. 5.2.1.1 Table 1 lists the relative permittivities (εr) and radar propagation velocities for various materials. Relative permittivity values range from 1 for air to 81 for fresh water. For unsaturated earth materials, εr ranges from 3 to 15. Note that a small change in the water content of earth materials results in a significant change in the relative permittivity. For water-saturated earth material, εr can range from 8 to 30. These values are representative, but may vary considerably with temperature, frequency, density, water content, salinity, and other conditions. (A)   d = function of density,  w = function of porosity and water content,  f = function of frequency,  t = function of temperature  s = function of salinity, and  p = function of pressure. 5.2.1.2 If the relative permittivity is unknown, as is normally the case, it may be necessary to estimate velocity or use a reflector of known depth to calculate the velocity. The propagation velocity, Vm, is calculated from the relationship as follows: where: D   =   measured depth to reflecting interface, and t   =   two-way travel time of an EM wave. 5.2.1.3 Methods for measuring velocity in the field are found in 6.7.3. Note that measured velocities may only be valid at the location where they are measured under specific soil conditions. If there is lateral variability in soil and rock composition and moisture content, velocity may need to be determined at several locations. 5.2.2 Attenuation—The depth of penetration is determined primarily by the attenuation of the radar signal due to the conversion of EM energy to thermal energy through electrical conduction, dielectric relaxation, or magnetic relaxation losses. Conductivity is primarily governed by the water content of the material and the concentration of free ions in solution (salinity). Attenuation also occurs due to scattering of the EM energy in unwanted directions by inhomogeneities in the subsurface. If the scale of inhomogeneity is comparable to the wavelength of EM energy, scattering may be significant (Olhoeft (33)). Other factors that affect attenuation include soil type, temperature (Morey (34)), and clay mineralogy (Doolittle (35)). Environments not conducive to using the radar method include high conductivity soils, sediments saturated with salt water or highly conductive fluids, and metal. 5.3 Equipment—The 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 display devices. 5.3.1 Radar Control Unit—The radar control unit synchronizes signals to the transmitting and receiving electronics in the antennas. The synchronizing signals control the transmitter and sampling receiver electronics located in the antenna(s) in order to generate a sampled waveform of the reflected radar waves. These waveforms may be filtered and amplified and are transmitted along with timing signals to the display and recording devices. 5.3.2 Real-time signal processing for improvement of signal-to-noise ratio is available in most GPR systems. When working in areas with cultural noise and in materials causing signal attenuation, time-varying gain is necessary to adjust signal amplitudes for display on monitors or plotting devices. Filters may be used in real time to improve signal quality. The summing of radar signals (stacking) is used to increase effective depth of exploration by improving the signal-to-noise ratio. 5.3.3 Data Display—The GPR data are displayed as a continuous profile of individual radar traces (Fig. 2). The horizontal-axis represents horizontal traverse distance and the vertical-axis is two-way travel time (or depth). Data are commonly presented in wiggle trace display, where the intensity of the received wave at an instant in time is proportional to the amplitude of the trace (see Fig. 2), or as a gray scale or color scale display, where the intensity of the received wave at an instant in time is proportional to either the intensity of gray scale (that is, black is high intensity, and white is low intensity; see Fig. 3) or to some color assignment defined according to a specified color-signal amplitude relationship. 5.4.2.4 Polarization—The type and alignment of polarization of the vector electromagnetic fields may be important in receiving responses from various scatterers. Two linear, parallel polarized, electric field antennas can maximize the response from linear scatters like pipes when the electric field (typically long axis of the dipole antenna) is aligned parallel with the pipe and towed perpendicular across the pipe. Similarly, alignment with the rebar in concrete will maximize the ability to map the rebar, but alignment perpendicular to the rebar will minimize scattering reflections from the rebar to see through or past the rebar to get the thickness of concrete. Similar arrangement may be made for overhead wires and nearby fences. Cross-polarized antennas (perpendicular to each other) minimize the response from horizontal layers. 5.4.3 Interferences Caused by Ambient, Geologic, and Cultural Conditions:  5.4.3.1 Measurements obtained by the GPR method may contain unwanted signals (noise) caused by geologic and cultural factors. 5.4.3.2 Ambient and Geologic Sources of Noise—Boulders, animal burrows, tree roots, or other inhomogeneities can cause unwanted reflections or scattering of the radar waves. Lateral and vertical variations in EM properties can also be a source of noise. 5.4.3.3 Cultural Sources of Noise—Above-ground cultural sources of noise include reflections from nearby vehicles, buildings, fences, power lines, lampposts, and trees. In cases where this kind of interference is present in the data, a shielded antenna may be used to reduce the noise. (1) Scrap metal at or near the surface can cause interference or ringing in the radar data. The presence of buried structures such as foundations, reinforcement bars (rebar), cables, pipes, tanks, drums, and tunnels under or near the survey line may also cause unwanted reflections (clutter). (2) In some cases, EM transmissions from nearby cellular telephones, two-way radios, television, and radio and microwave transmitters may induce noise on the radar record. (3) Other Sources of Noise—Other sources of noise can be caused by the EM coupling of the antenna with the earth and decoupling of the antenna to the ground due to rough terrain, heavy vegetation, water on the ground surface, or other changes in surface conditions. 5.4.3.4 Summary—All possible sources of noise present during a survey should be noted so that their effects can be considered when processing and interpreting the data. 5.4.4 Alternate Methods—The limitations previously discussed may prohibit the effective use of the GPR method, and other methods or non-geophysical methods may be required to resolve the problem (see Guide D6429). Note 1: The quality of the result produced by applying this standard is dependent on the competence of the personnel performing the work, and the suitability of the equipment and facilities used. Agencies that meet the criteria of Practice D3740 are generally considered capable of competent and objective testing/sampling/inspection/etc. Users of this standard are cautioned that compliance with Practice D3740 does not in itself assure reliable results. Reliable results depend on many factors; Practice D3740 provides a means of evaluating some of those factors.