1887
Volume 35, Issue 4
  • ISSN: 0812-3985
  • E-ISSN: 1834-7533

Abstract

A novel rotating magnetic gradiometer system (GETMAG) has been designed, constructed, and demonstrated. The sensor is a high temperature superconducting quantum interference device (SQUID) operating in liquid nitrogen (-196°C). By making measurements about three separate axes, the full magnetic gradient tensor is determined.

The system has been demonstrated over a magnetite skarn deposit at Tallawang, near Gulgong, NSW, which is essentially two-dimensional (2D). The 2D structure was important because it allowed an unaliased total magnetic intensity (TMI) survey to be carried out in parallel, from which tensor components could be calculated to directly compare with the tensor components measured with the rotating gradiometer. The agreement was found to be excellent, confirming the accuracy and calibration of GETMAG and the Fourier filtering method of the calculation.

Methods developed to analyse 2D tensor data utilise eigenvalue and eigenvector systematics. Notwithstanding underlying non-uniqueness of solutions for 2D structures, all determinable parameters of location, geometry, and magnetization were found to accord with directly measured properties, i.e., information gained from either exploration drilling or laboratory measurements. Only a few tensor gradiometer stations were needed to extract the same information as a whole TMI survey.

A more general method to determine structure and location of sources is Tensor Euler Deconvolution. This method has been adapted for the magnetic gradient tensor in a least-squares fashion and applied to the tensors calculated from the TMI survey. Generally, an Euler index of = 1 was found, as is expected for 2D sources. However, this approach allowed second-order features of the source, where > 1, to be discerned. The skarn is interpreted to comprise a fresh, more highly magnetic, core at depth (~25-30 m) surrounded by a less magnetic mantle. The skarn extends to within 10 m of the surface where weathering has presumably contributed to diminished magnetization. Elsewhere, away from the skarn, Euler indices are low, approaching that of a magnetic annihilator = 0). This presumably reflects the uniformly magnetized alluvial soil cover.

Our next stage is to demonstrate an airborne capability of GETMAG, beginning with a helicopter platform before moving to fixed-wing. In addition to mineral and oil exploration, we envisage applications in environmental, military, and unexploded ordnance (UXO) surveys.

Loading

Article metrics loading...

/content/journals/10.1071/EG04297
2004-12-01
2026-01-12
Loading full text...

Full text loading...

References

  1. Bick, M., Clark, D.A., Foley, C.P., Leslie, K.E., Schmidt, P.W., and Tilbrook, D.L., 2004a, GETMAG Phase 1 Completion: CSIRO Confidential Report to Sponsors.
  2. Bick, M., Leslie, K.E., Binks, R.A., Tilbrook D.L., Lam, S.K.H., Gnanarajan, S., Du, J., and Foley, C.P., 2004b, Axial high-Tc superconducting gradiometer with a flexible flux transformer, Appl. Phys. Lett.,84, 5347-5349.
  3. Blakely, R.J., 1996, Potential theory in gravity and magnetic applications: Cambridge University Press, 441pp.
  4. Christensen, A., and Rajagopalan, S., 2000, The magnetic vector and gradient tensor in mineral and oil exploration: Preview,84, 77.
  5. Clark, D.A., 1997, Theory of Differential Vector Magnetometry - a new method for remote determination of in situ magnetic properties and improved drill targeting: Exploration and Mining, North Ryde, Report 395R, 19 pp.
  6. Clark, D.A., Schmidt, P.W., Coward, D.A., and Huddleston, M.P., 1998, Remote determination of magnetic properties and improved drill targeting of magnetic anomaly sources by Differential Vector Magnetometry (DVM): Exploration Geophysics,29, 312-319.
  7. Emerson, D.W., Clark, D.A., and Saul, S.J., 1985, Magnetic exploration models incorporating remanence, demagnetisation and anisotropy: HP 41C handheld computer algorithms: Exploration Geophysics,16, 1-122.
  8. Foley, C.P., and Leslie, K.E., 1998, Potential use of High Tc SQUIDs for Airborne electromagnetics: Exploration Geophysics,29, 30-34.
  9. Foley, C.P., Leslie, K.E., Binks, R., Lewis, C., Murray, W., Sloggett, G.J., Lam, S., Sankrithyan, B., Savvides, N., Katzaros, A., Muller, K.H., Mitchell, E.E., Pollock, J., Lee, J., Dart, D.L., Barrow, R.R., Asten, M., Maddever, A., Panjkovic, G., Downey, M., Hoffman C., and Turner, R., 1999, Field Trials using HTS SQUID Magnetometers for Ground-based and Airborne Geophysical Applications: IEEE Trans. Appl. Supercond.,9, 3786-3792.
  10. Frahm, C.P., 1972, Inversion of the magnetic field gradient equation for a magnetic dipole field: NCSL Informal Report, 135-72.
  11. Heath, P., Heinson, G., and Greenhalgh, S., 2003, Some comments on potential field tensor data: Exploration Geophysics,34, 57-62.
  12. Schmidt, P.W., and Clark, D.A., 2000, Advantages of measuring the magnetic gradient tensor: Preview,85, 26-30.
  13. Tilbrook, D.L., 2004, The design of a new concept HTSC axial gradiometer: Physica C,407, 1-9.
  14. Vrba, J., 1996, SQUID gradiometers in real environments: in Weinstock, H. (ed.), SQUID Sensors: Fundamentals and Applications, Kluwer Academic, p117.
  15. Weekes, G., 1995, Tallawang South magnetite deposit; report on geological investigations 1993 to 1995, Vols. I and II: Commercial Minerals Limited, Report 19959.
  16. Wilson, H., 1985, Analysis of the magnetic gradient tensor: Defence Research Establishment Pacific: Canada Technical Memorandum, 85-13, 47.
  17. Wynn, W.M., Frahm, C.P., Carroll, P.J., Clark, R.H., Wellhoner, J., and Wynn, M.J., 1975, Advanced superconducting gradiometer/magnetometer arrays and a novel signal processing technique: IEEE Trans. Mag.,MAG-11, 701-707.
  18. Zhang, C., Mushayandevu, M.F., Reid, A.B., Fairhead, J.D., and Odegard, M.E., 2000, Euler deconvolution of gravity tensor gradient data: Geophysics,65, 512-520.
/content/journals/10.1071/EG04297
Loading
  • Article Type: Research Article
Keyword(s): Euler; Fourier; gradiom eter; SQUID; ten ser

Most Cited This Month Most Cited RSS feed

This is a required field
Please enter a valid email address
Approval was a Success
Invalid data
An Error Occurred
Approval was partially successful, following selected items could not be processed due to error