Lecture 4a - Ground Penetrating Radar (GPR)

GPR Basic Principles

  • GPR transmits short pulses of electromagnetic radiation (10-1000 MHz) into the ground.
  • Antenna transmits pulses that reflect off subsurface features and are detected by a receiving antenna
  • Reflections are caused by contrasts in electrical properties, similar to how reflection seismics work with seismic properties.

GPR Data Acquisition and Processing

  • GPR data processing and analysis are similar to reflection seismics.
  • Radograms (reflection profile plots) display reflected amplitude against two-way travel time.
  • Time is measured in nanoseconds (1 ns = 10910^{-9} seconds) due to the high speed of radar waves.
  • Data processing converts travel times to depths using radar wave velocity:
    • Distance=SpeedxTimeDistance = Speed \, x \, Time

GPR Profile Interpretation

  • GPR profiles show wiggles representing single shot measurements.
  • Time increases down the plot, with durations on the order of tens of nanoseconds.
  • Hyperbolas are similar to those seen in seismic sections.
  • Strong, coherent horizontal signal near zero travel time.
  • Depth estimates are made based on radar wave velocity (e.g., 0.12 meters/nanosecond).

GPR Characteristics and Applications

  • GPR provides high-resolution data but with limited depth penetration.
  • Used for near-surface investigations requiring high detail.
  • Applications:
    • Assessing hydrological properties.
    • Identifying geological structures.
    • Determining depths to ice.
    • Evaluating infrastructure (walls, road surfaces).
    • Detecting unexploded ordnance (landmines).

GPR Instrumentation

  • Instrumentation includes a transmitter and a receiver.
  • The transmitter releases radar pulses into the ground.
  • The receiver detects the reflected signals and sends the information to a control and display unit.
  • Optical fibers are used to connect the receiver to the control unit to reduce electromagnetic interference.

Antenna Styles

Unshielded Antennae
  • Transmit and receive signals from a wide range of directions.
    • More susceptible to noise (e.g., signals from passing cars).
    • Flexible systems because the antennae can be moved apart, allowing different survey styles.
    • Lighter and easier to maneuver.
Shielded Antennae
  • Focus the transmitted pulse into the ground.
  • Reduce likelihood of interference from external sources.
  • Improve signal quality.
  • Fixed geometry (transmitter and receiver cannot be separated).
  • Heavier due to shielding.

Data Visualization

  • Signal amplitude exceeding a threshold is infilled with black on the wiggly trace or scanline.
  • Colored regions indicate large amplitude reflections.
  • Time increases downwards on the plot.

Waveform Analysis

  • First signals represent the transmitted source pulse (artifacts).
  • Ground-coupled wave represents the pulse traveling directly from the transmitter to the receiver along the ground surface and is not useful for reflection surveys.
  • Useful signals are found at longer travel times corresponding to the first primary reflector.
  • GPR pulse is a series of rapidly decreasing amplitude oscillations (triplets).

Profile Plots

  • Time-position profile plots visualize GPR data.
  • Position is on the horizontal axis, and time is on the vertical axis.
  • Plots indicate where large magnitude reflections have been received.
  • The direct wave between the receiver and the antenna appears as a consistent horizontal return (artifact).
  • Below the direct wave, laterally discontinuous reflectors and a more continuous reflector can be observed.

Radar Wave Velocity and Permittivity

  • Radar waves travel at the speed of light in a vacuum but are slowed when traveling through matter.
  • Electromagnetic wave speed is calculated as:
    • v=cϵrv = \frac{c}{\sqrt{\epsilon_r}},
      • Where:
        • vv = electromagnetic wave speed
        • cc = speed of light
        • ϵr\epsilon_r = relative permittivity

Permittivity

  • Permittivity is a material's ability to electrically polarize and transmit an electric field.
  • Relative permittivity is the ratio between a material's permittivity and the permittivity of free space (ϵ0\epsilon_0).
  • Relative permittivity is unitless and increases from one.
  • When relative permittivity is greater than one, the wave speed in matter is lower than the speed of light in a vacuum.

Electrical Properties of Geomaterials

  • Water has a high relative permittivity (approximately 80).
  • Sedimentary rocks have relative permittivity ranges going up to the into the few tens.
  • Dry materials (sand, granite, salt) have faster wave velocities.
  • Cold ice also has a fast wave velocity.

Reflection Coefficient

  • Contrast in relative permittivity generates reflection interfaces.
  • Reflection coefficient (R) is calculated as:
    • R=k<em>2k</em>1k<em>2+k</em>1R = \frac{k<em>2 - k</em>1}{k<em>2 + k</em>1},
      • Where:
        • k1k_1 = relative permittivity of the upper layer.
        • k2k_2 = relative permittivity of the lower layer.
  • Reflections represent interfaces between regions of different relative permittivity, often due to variations in water content.

Summary

  • GPR is a high-frequency electromagnetic imaging method for near-surface investigations (depths of meters to a few tens of meters).
  • Data is measured in terms of signal travel times to reflectors generated by contrasts in relative permittivity.
  • Converting travel times to depths requires estimating wave velocity, which is a function of relative permittivity.
  • Water has a high relative permittivity, so reflections often indicate changes in water content.