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Analysis of induced electromagnetic signals from elementary geometries in the subsurface

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Title: Analysis of induced electromagnetic signals from elementary geometries in the subsurface


1
Analysis of induced electromagnetic signals from
elementary geometries in the subsurface
Applied Geophysics Potential Field Methods, May
12th 2005
  • Alejandra Reynaldos, Christina Schell,
  • Corinne Bachmann, Laura Alisic Tonie Davidsen

2
(No Transcript)
3
Introduction
  • Necessary to recognize shapes in EM signals to
    delineate geometries in subsurface
  • No standard shapes due to different methods and
    layouts
  • Case study of some signals / geometries in FD and
    TD

4
Sphere in Frequency Domain
  • HLEM, frequency domain. T R L
  • 5 setups with sphere at increasing depth (L/8,
    L/4, L/2, L, 2L)
  • Perfectly symmetric with shoulders on 3 (4) of
    the responses
  • Below L you can not see the sphere
  • Difficult to determine the exact shape

5
Sphere in Frequency Domain
6
FDEM System over Dipping Sheets
  • Dip-Angle fixed-transmitter system over dipping
    sheets
  • Upper picture dipping sheet, lower vertical sheet
    with varying depth
  • Real Crossover over top of sheet, false crossover
    from bottom of sheet or resistive structures
  • Variance with depth perfectly asymmetric

7
FDEM System over Dipping Sheets
8
Two Semi-Infinite Vertical Sheets
  • Multiple conductors
  • Frequency domain by means of VLF
  • 3 configurations of spacing
  • Curves show wiggles around midpoint
  • caused by mutual coupling influence
  • false crossover
  • Influence disappears with distance

9
Two Semi-Infinite Vertical Sheets
10
Time Domain EM
  • Main difference with FDEM two measure-ments
    available, early and late stage
  • Early stage profile is only dependent on the size
    and shape of the conductor
  • Late stage profile can be used for estimating the
    conductivity
  • Some examples of vertical component signal for a
    number of simple shapes

11
TDEM profiles (normalized)
12
Discussion Conclusions
  • Different methods and layouts cause different
    responses for same geometry
  • A signal can be explained with different
    geometries
  • Thorough study of EM results is necessary to come
    to the right conclusions in a research
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