Skip to main content
Log in

Three-Dimensional Reverse Time Migration of Ground-Penetrating Radar Signals

  • Published:
Pure and Applied Geophysics Aims and scope Submit manuscript

Abstract

Three-dimensional (3D) ground-penetrating radar (GPR) systems and 3D seismic imaging techniques have been developing fast and evolving rapidly in the last decade. Ray-based migration methods have been successfully applied to processing 3D GPR signals based on the similarity between electromagnetic and seismic waves. However, reverse time migration (RTM) of 3D GPR signals has not been well studied in the past. In this paper, we present a 3D RTM based on Maxwell’s equations for 3D GPR surveys. Migration recovers the true subsurface structure from a distorted and unfocused time profile and suppresses common electromagnetic clutter and noise. RTM based on Maxwell’s equations can consider conductivity directly and compensate for the attenuation within a high-conductivity zone. Compared with 2D RTM, 3D RTM back-propagates both in-line and cross-line signals simultaneously and can include complex 3D permittivity and conductivity models. We have integrated a parallel finite-difference time-domain (FDTD) algorithm based on a hybrid MPI and OpenMP scheme to reduce the computational cost of 3D problems. The 3D RTM experiments on an anomaly of “EM” shape and a realistic sand dune model demonstrate the effective recovery of 3D subsurface structures.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

Fig. 1
Fig. 2
Fig. 3
Fig. 4
Fig. 5
Fig. 6
Fig. 7
Fig. 8
Fig. 9
Fig. 10

Similar content being viewed by others

References

  • Baysal, E., Kosloff, D. D., & Sherwood, J. W. C. (1983). Reverse time migration. Geophysics, 48(11), 1514–1524.

    Article  Google Scholar 

  • Benson, A. K. (1995). Applications of ground penetrating radar in assessing some geological hazards: examples of groundwater contamination, faults, cavities. Journal of Applied Geophysics, 33(1), 177–193.

    Article  Google Scholar 

  • Biondi, B. (2007). Concepts and Applications in 3D Seismic Imaging. Society of Exploration Geophysicists and European Association of Geoscientists and Engineers.

  • Bourgeois, J. M., & Smith, G. S. (1996). A fully three-dimensional simulation of a ground-penetrating radar: FDTD theory compared with experiment. IEEE Transactions on Geoscience and Remote Sensing, 34(1), 36–44.

    Article  Google Scholar 

  • Bristow, C. S., Bailey, S. D., & Lancaster, N. (2000). The sedimentary structure of linear sand dunes. Nature, 406(6791), 56–59.

    Article  Google Scholar 

  • Bristow, C. S., Porat, N., Duller, G., Armitage, S. J., Roberts, H. M., Clarke, B. M., et al. (2003). Evidence for dune reactivation from GPR profiles on the Maputaland coastal plain, South Africa. Geological Society, London, Special Publications, 211, 29–46.

    Article  Google Scholar 

  • Claerbout, J. F. (1971). Toward a unified theory of reflector mapping. Geophysics, 36(3), 467–481.

    Article  Google Scholar 

  • Daniels, D. J. (2005). Ground Penetrating Radar. Hoboken: Wiley.

    Google Scholar 

  • Ernst, J. R., Maurer, H., Green, A. G., & Holliger, K. (2007). Full-waveform inversion of crosshole radar data based on 2-D finite-difference time-domain solutions of Maxwell’s equations. IEEE Transactions on Geoscience and Remote Sensing, 45(9), 2807–2828.

    Article  Google Scholar 

  • Feng, X., Wang, Q., Lu, Q., Liu, C., Liang, W., Li, H., Yu, Y., Ren, Q. (July 2012). Subsurface imaging by modified migration for irregular GPR data. In: 2012 IEEE International Geoscience and Remote Sensing Symposium (IGARSS). pp. 3194–3197.

  • Fisher, E., McMechan, G. A., Annan, A. P., & Cosway, S. W. (1992). Examples of reverse-time migration of single-channel, ground-penetrating radar profiles. Geophysics, 57(4), 577–586.

    Article  Google Scholar 

  • Fu, L., Liu, S., Liu, L., & Wu, J. (2014). Airborne ground penetrating radar numerical simulation and reverse time migration. Chinese Journal of Geophysics-Chinese Edition, 57(5), 1636–1646.

    Google Scholar 

  • Green, A., Gross, R., Holliger, K., Horstmeyer, H., & Baldwin, J. (2003). Results of 3-D georadar surveying and trenching the San Andreas fault near its northern landward limit. Tectonophysics, 368(1), 7–23.

    Article  Google Scholar 

  • Gross, R., Green, A., Horstmeyer, H., Holliger, K., & Baldwin, J. (2003). 3-D georadar images of an active fault: efficient data acquisition, processing and interpretation strategies. Subsurface Sensing Technologies and Applications, 4(1), 19–40.

    Article  Google Scholar 

  • Herrmann, F. J., & Hennenfent, G. (2008). Non-parametric seismic data recovery with curvelet frames. Geophysical Journal International, 173(1), 233–248.

    Article  Google Scholar 

  • Huang, Q., Li, Z., & Wang, Y. (2010). A parallel 3-D staggered grid pseudospectral time domain method for ground-penetrating radar wave simulation. Journal of Geophysical Research, 115(B12), B12101.

    Article  Google Scholar 

  • Jakubowicz, H., & Levin, S. (1983). A simple exact method of 3-D migration-theory. Geophysical Prospecting, 31(1), 34–56.

    Article  Google Scholar 

  • Jol, H. M. (2008). Ground penetrating radar theory and applications. Amsterdam: Elsevier.

    Google Scholar 

  • Klokov, A., Sato, M. (July 2011). Application of 3-D migration algorithm to GPR on an irregular ground surface. In: 2011 IEEE International Geoscience and Remote Sensing Symposium (IGARSS). pp. 870–873.

  • Knight, R. (2001). Ground penetrating radar for environmental applications. Annual Review of Earth and Planetary Sciences, 29(1), 229–255.

    Article  Google Scholar 

  • Leuschen, C., & Plumb, R. (2001). A matched-filter-based reverse-time migration algorithm for ground-penetrating radar data. IEEE Transactions on Geoscience and Remote Sensing, 39(5), 929–936.

    Article  Google Scholar 

  • Levander, A. R. (1988). Fourth-order finite-difference P-SV seismograms. Geophysics, 53(11), 1425–1436.

    Article  Google Scholar 

  • Liu, S., Lei, L., Fu, L., & Wu, J. (2014). Application of pre-stack reverse time migration based on FWI velocity estimation to ground penetrating radar data. Journal of Applied Geophysics, 107, 1–7.

    Article  Google Scholar 

  • Loewenthal, D., Lu, L., Roberson, R., & Sherwood, J. (1976). The wave equation applied to migration. Geophysical Prospecting, 24(2), 380–399.

    Article  Google Scholar 

  • Mansour, H., Herrmann, F., & Yılmaz, O. (2013). Improved wavefield reconstruction from randomized sampling via weighted one-norm minimization. Geophysics, 78(5), V193–V206.

    Article  Google Scholar 

  • McClymont, A. F., Green, A. G., Villamor, P., Horstmeyer, H., Grass, C., & Nobes, D. C. (2008). Characterization of the shallow structures of active fault zones using 3-D ground-penetrating radar data. Journal of Geophysical Research, 113(B10), B10315.

    Article  Google Scholar 

  • McMechan, G. A. (1983). Migration by extrapolation of time-dependent boundary values. Geophysical Prospecting, 31(3), 413–420.

    Article  Google Scholar 

  • Meles, G. A., Van Der Kruk, J., Greenhalgh, S. A., Ernst, J. R., Maurer, H., & Green, A. G. (2010). A new vector waveform inversion algorithm for simultaneous updating of conductivity and permittivity parameters from combination crosshole/borehole-to- surface GPR data. IEEE Transactions on Geoscience and Remote Sensing, 48(9), 3391–3407.

    Article  Google Scholar 

  • Moran, M. L., Greenfield, R. J., Arcone, S. A., & Delaney, A. J. (2000). Multidimensional GPR array processing using Kirchhoff migration. Journal of Applied Geophysics, 43(2), 281–295.

    Article  Google Scholar 

  • Naghizadeh, M., & Sacchi, M. (2010). Beyond alias hierarchical scale curvelet interpolation of regularly and irregularly sampled seismic data. Geophysics, 75(6), WB189–WB202.

    Article  Google Scholar 

  • Neal, A. (2004). Ground-penetrating radar and its use in sedimentology: principles, problems and progress. Earth-Science Reviews, 66(3–4), 261–330.

    Article  Google Scholar 

  • Olhoeft, G. R. (1998). Electrical, magnetic, and geometric properties that determine ground penetrating radar performance. In: Proceedings of GPR ‘98, Seventh International Conference on Ground Penetrating Radar. University of Kansas, Lawrence, KS. Vol. 98. pp. 177–182.

  • Qian, R., & Liu, L. (2016). Internal structure of sand dunes in the Badain Jaran desert revealed by GPR. IEEE Journal of Selected Topics in Applied Earth Observations and Remote Sensing, 9(1), 159–166.

    Article  Google Scholar 

  • Radzevicius, S. (2008). Practical 3-D migration and visualization for accurate imaging of complex geometries with GPR. Journal of Environmental & Engineering Geophysics, 13(2), 99–112.

    Article  Google Scholar 

  • Roden, J. A., & Gedney, S. D. (2000). Convolutional PML (CPML): an efficient FDTD implementation of the CFS-PML for arbitrary media. Microwave and Optical Technology Letters, 27(5), 334–338.

    Article  Google Scholar 

  • Song, J., Liu, Q. H., Torrione, P., & Collins, L. (2006). Two-dimensional and three-dimensional NUFFT migration method for landmine detection using ground-penetrating radar. IEEE Transactions on Geoscience and Remote Sensing, 44(6), 1462–1469.

    Article  Google Scholar 

  • Su, M., El-Kady, I., Bader, D., Lin, S. (Aug 2004). A novel FDTD application featuring OpenMP-MPI hybrid parallelization. In: ICPP 2004 International Conference on Parallel Processing. Vol. 1. pp. 373–379.

  • Whitmore, N. D. (1983). Iterative depth migration by backward time propagation. SEG Technical Program Expanded Abstracts, 1983, 382–385.

    Google Scholar 

  • Yang, X., Klotzsche, A., Meles, G., Vereecken, H., & Van Der Kruk, J. (2013). Improvements in crosshole GPR full-waveform inversion and application on data measured at the Boise hydrogeophysics research site. Journal of Applied Geophysics, 99, 114–124.

    Article  Google Scholar 

  • Yoon, K., Shin, C., Suh, S., Lines, L. R., & Hong, S. (2003). 3D reverse-time migration using the acoustic wave equation: an experience with the SEG/EAGE data set. The Leading Edge, 22(1), 38–41.

    Article  Google Scholar 

  • Zhu, T., Harris, J., & Biondi, B. (2014). Q-compensated reverse-time migration. Geophysics, 79(3), S77–S87.

    Article  Google Scholar 

  • Zhu, W., & Huang, Q. (2016). Attenuation compensated reverse time migration method of ground penetrating radar signals. Chinese Journal of Geophysics, 59(10), 3909.

    Google Scholar 

Download references

Acknowledgements

This work is supported by the National Science Foundation of China (41574104, 41874082). The calculations were performed on a Tianhe-1(A) supercomputer. We are grateful to the three anonymous reviewers for their excellent reviews and constructive suggestions.

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Qinghua Huang.

Additional information

Publisher's Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Appendix A. Hybrid MPI & OpenMP

Appendix A. Hybrid MPI & OpenMP

This appendix shows the program structure of parallel FDTD (Fig. 11) and the pseudo-code of the hybrid MPI & OpenMP scheme (Fig. 12)  inside each subdomain of Fig. 11. The entire FDTD domain is divided into several subdomains, and each subdomain is distributed to one processor. A hybrid parallelization scheme with both OpenMP and MPI (Su et al. 2004) is used here. MPI is used for communication between nodes, and OpenMP is used to carry out multi-threading parallel computing on a single shared-memory node. Combining MPI and OpenMP makes FDTD fully utilize the power of parallel systems constructed out of interconnected symmetric multiprocessing (SMP) nodes.

Fig. 11
figure 11

Structure of the parallel FDTD algorithm. The code consists of three parts: (1) Input parameters and settings for each subdomain, which include “eps” (model of dielectric permittivity), “mu” (model of magnetic permeability), “sig” (model of electric conductivity), “src” (positions of sources and input signals), “rec” (positions of receivers), etc. (2) The main part for parallel FDTD simulation. The whole computational domain is divided into several subdomains. For each subdomain, E&H components are updated using OpenMP. For each time step, the values on edges of each domain are exchanged through MPI. (3) Output of the recorded gathers, slices, and wavefields during propagation

Fig. 12
figure 12

Pseudo-code for hybrid MPI & OpenMP

Rights and permissions

Reprints and permissions

About this article

Check for updates. Verify currency and authenticity via CrossMark

Cite this article

Zhu, W., Huang, Q., Liu, L. et al. Three-Dimensional Reverse Time Migration of Ground-Penetrating Radar Signals. Pure Appl. Geophys. 177, 853–865 (2020). https://doi.org/10.1007/s00024-019-02341-x

Download citation

  • Received:

  • Revised:

  • Accepted:

  • Published:

  • Issue Date:

  • DOI: https://doi.org/10.1007/s00024-019-02341-x

Keywords

Navigation