1. Sounding of Subsurface Water throughSounding of Subsurface Water through
Conductive Media in Mars AnalogConductive Media in Mars Analog
Environments Using TransientEnvironments Using Transient
Electromagnetics and Low Frequency GroundElectromagnetics and Low Frequency Ground
Penetrating RadarPenetrating Radar
joern@jernsletten.namjoern@jernsletten.nam
eehttp://joern.jernsletten.name/http://joern.jernsletten.name/
Mandag, 14. JuniMandag, 14. Juni
20042004
Universitetet iUniversitetet i
BergenBergen
Det Matematisk-NaturvitenskapeligeDet Matematisk-Naturvitenskapelige
FakultetFakultet
Institutt for GeovitenskapInstitutt for Geovitenskap
DoctorDoctor
PhilosophiaePhilosophiae
Prøveforelesning, SelvvalgtPrøveforelesning, Selvvalgt
EmneEmne
Jørn AtleJørn Atle
JernslettenJernsletten
heggy@lpi.usra.edheggy@lpi.usra.ed
EssamEssam
HeggyHeggyLunar and Planetary Institute, Houston, TexasLunar and Planetary Institute, Houston, Texas
2. IntroductionIntroduction
To show how these methods differ and complement each other,To show how these methods differ and complement each other,
we show data from three field studies:we show data from three field studies:
1)1) EMEM diffusivediffusive spreading sounding data (TEM) from Pimaspreading sounding data (TEM) from Pima
County, ArizonaCounty, Arizona
2)2) Shallower sounding data, using the Fast-Turnoff TEMShallower sounding data, using the Fast-Turnoff TEM
method, from Peña de Hierro, near Minas de Riotinto, Spainmethod, from Peña de Hierro, near Minas de Riotinto, Spain
3)3) WaveWave propagationpropagation radar sounding data (GPR) from theradar sounding data (GPR) from the
Nubian aquifer, Baharïya Oasis, EgyptNubian aquifer, Baharïya Oasis, Egypt
GPR and TEM discussed and compared in terms of:GPR and TEM discussed and compared in terms of:
a)a) Spatial resolutionSpatial resolution
b)b) Depth of investigationDepth of investigation
c)c) Sensitivity to highly conductive layers (clay, ore bodies,Sensitivity to highly conductive layers (clay, ore bodies,
brines, metal-rich fluids, etc.)brines, metal-rich fluids, etc.)
d)d) Sounding frequenciesSounding frequencies
e)e) Logistical efficiencyLogistical efficiency
f)f) Appropriate applicationsAppropriate applications
3. EM Sounding Scenarios for MarsEM Sounding Scenarios for Mars
( Grimm, 2002 )( Grimm, 2002 )
21. Arizona USGS Well DataArizona USGS Well Data
Water table at ~120 m depthWater table at ~120 m depth
22. Arizona TEM Line 1 Field DataArizona TEM Line 1 Field Data
100 m x 100 m Tx loop,100 m x 100 m Tx loop,
ferrite-core Hferrite-core Hzz coil Rxcoil Rx
antennaantenna
16 Hz sounding frequency16 Hz sounding frequency
Depth of investigationDepth of investigation
~500 m~500 m
23. Arizona TEM Line 1 Model DataArizona TEM Line 1 Model Data
Water table at ~120 m depth (horizontal blue line)Water table at ~120 m depth (horizontal blue line)
Consistent with depth to water table from USGS test wellsConsistent with depth to water table from USGS test wells
100 m x 100 m Tx loop, ferrite-core H100 m x 100 m Tx loop, ferrite-core Hzz coil Rx antennacoil Rx antenna
16 Hz sounding frequency16 Hz sounding frequency
Depth of investigation ~500 mDepth of investigation ~500 m
24. Arizona TEM Line 2 Field DataArizona TEM Line 2 Field Data
100 m x 100 m Tx loop,100 m x 100 m Tx loop,
ferrite-core Hferrite-core Hzz coil Rxcoil Rx
antennaantenna
16 Hz sounding frequency16 Hz sounding frequency
Depth of investigationDepth of investigation
~500 m~500 m
25. Arizona TEM Line 2 Model DataArizona TEM Line 2 Model Data
Water table at ~120 m depth (horizontal blue line)Water table at ~120 m depth (horizontal blue line)
Consistent with depth to water table from USGS test wellsConsistent with depth to water table from USGS test wells
100 m x 100 m Tx loop, ferrite-core H100 m x 100 m Tx loop, ferrite-core Hzz coil Rx antennacoil Rx antenna
16 Hz sounding frequency16 Hz sounding frequency
Depth of investigation ~500 mDepth of investigation ~500 m
26. Arizona TEM Line 3 Field DataArizona TEM Line 3 Field Data
100 m x 100 m Tx loop,100 m x 100 m Tx loop,
ferrite-core Hferrite-core Hzz coil Rxcoil Rx
antennaantenna
16 Hz sounding frequency16 Hz sounding frequency
Depth of investigationDepth of investigation
~350 m~350 m
27. Arizona TEM Line 3 Model DataArizona TEM Line 3 Model Data
Water table at ~120 m depth (horizontal blue line)Water table at ~120 m depth (horizontal blue line)
Consistent with depth to water table from USGS test wellsConsistent with depth to water table from USGS test wells
100 m x 100 m Tx loop, ferrite-core H100 m x 100 m Tx loop, ferrite-core Hzz coil Rx antennacoil Rx antenna
16 Hz sounding frequency16 Hz sounding frequency
Depth of investigation ~350 mDepth of investigation ~350 m
28. Peña de Hierro, MARTE Field AreaPeña de Hierro, MARTE Field Area
29. Peña de Hierro, Main Source AreaPeña de Hierro, Main Source Area
Morris et al., 2004Morris et al., 2004
Kargel and Marion, 2004Kargel and Marion, 2004
Stoker et al., 2004Stoker et al., 2004
Fernández-Remolar et al., 2004Fernández-Remolar et al., 2004
A.k.a. MER-B in the Late Hesperian?A.k.a. MER-B in the Late Hesperian?
Jarosite =Jarosite = KFeKFe3+3+
33 (SO(SO44 ))22 (OH)(OH)66
Basic hydrous potassium iron sulfate
Yellow-brown, brown, orange-brown
Light yellow streaks
30. Peña de Hierro, MARTE Drill Site #3Peña de Hierro, MARTE Drill Site #3
31. Typical Fast-Turnoff TEM Field SetupTypical Fast-Turnoff TEM Field Setup
( Adapted from Zonge, 1992 )( Adapted from Zonge, 1992 )
32. Peña de Hierro, Field ConditionsPeña de Hierro, Field Conditions
34. Fast-Turnoff TEM Line 4 Field DataFast-Turnoff TEM Line 4 Field Data
40 m x 40 m Tx loop, 10 m x 10 m Rx loop40 m x 40 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
35. Fast-Turnoff TEM Line 4 Model DataFast-Turnoff TEM Line 4 Model Data
Water table at ~90 m depthWater table at ~90 m depth
Consistent with initial drilling results (MARTE Drill Site #4)Consistent with initial drilling results (MARTE Drill Site #4)
40 m x 40 m Tx loop, 10 m x 10 m Rx loop40 m x 40 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
Depth of investigation ~160 mDepth of investigation ~160 m
36. Fast-Turnoff TEM Line 7 Field DataFast-Turnoff TEM Line 7 Field Data
40 m x 40 m Tx loop, 10 m x 10 m Rx loop40 m x 40 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
37. Fast-Turnoff TEM Line 7 Model DataFast-Turnoff TEM Line 7 Model Data
Water table at ~90 m depthWater table at ~90 m depth
Consistent with initial drilling results (MARTE Drill Site #4)Consistent with initial drilling results (MARTE Drill Site #4)
40 m x 40 m Tx loop, 10 m x 10 m Rx loop40 m x 40 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
Depth of investigation ~130 mDepth of investigation ~130 m
39. Fast-Turnoff TEM Line 15 Field DataFast-Turnoff TEM Line 15 Field Data
20 m x 20 m Tx loop, 10 m x 10 m Rx loop20 m x 20 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
40. Fast-Turnoff TEM Line 15 Model DataFast-Turnoff TEM Line 15 Model Data
Water interface at ~15 m depthWater interface at ~15 m depth
Consistent with initial drilling results (MARTE Drill Site #1)Consistent with initial drilling results (MARTE Drill Site #1)
20 m x 20 m Tx loop, 10 m x 10 m Rx loop20 m x 20 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
Depth of investigation ~50 mDepth of investigation ~50 m
41. Fast-Turnoff TEM Line 14 Field DataFast-Turnoff TEM Line 14 Field Data
20 m x 20 m Tx loop, 10 m x 10 m Rx loop20 m x 20 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
42. Fast-Turnoff TEM Line 14 Model DataFast-Turnoff TEM Line 14 Model Data
Water interface at ~15 m depthWater interface at ~15 m depth
Consistent with initial drilling results (MARTE Drill Site #1)Consistent with initial drilling results (MARTE Drill Site #1)
20 m x 20 m Tx loop, 10 m x 10 m Rx loop20 m x 20 m Tx loop, 10 m x 10 m Rx loop
32 Hz sounding frequency32 Hz sounding frequency
Depth of investigation ~50 mDepth of investigation ~50 m
43. Rio Tinto Drill Site RelocationsRio Tinto Drill Site Relocations
53. Dolomitic limestone
Gravel
Saturated Sandstones:
Nubian aquifer
Fractured interface of Limestone-Gravel
Geological Profile of the NubianGeological Profile of the Nubian
Aquifer in the Baharïya Oasis AreaAquifer in the Baharïya Oasis Area
57. ConclusionsConclusions
Parameter GPR TEM
Physical process Wave propagation Diffusive spreading
Spatial resolution
Higher
( < 1 m possible )
Lower
( m – km )
Depth of
investigation
m – 10’s of m m – km
Sensitivity to
highly conductive
layers
More Less
Sounding
frequencies
1 MHz – 1 GHz 1 Hz – 64 Hz
Logistical
efficiency
Higher Lower
Appropriate
applications
Shallow groundwater,
near-surface clays,
etc.
Very deep water
tables, aquifers, etc.
58. Acknowledgements & References CitedAcknowledgements & References Cited
Grant. F. S., and West, G. F.,Grant. F. S., and West, G. F., Interpretation Theory in Applied GeophysicsInterpretation Theory in Applied Geophysics . McGraw-Hill,. McGraw-Hill,
New York, New York, 1965.New York, New York, 1965.
Grimm, R. E., “Low-Frequency Electromagnetic Exploration for Groundwater on Mars”.Grimm, R. E., “Low-Frequency Electromagnetic Exploration for Groundwater on Mars”.
Journal of Geophysical ResearchJournal of Geophysical Research , Vol. 107, No. E2, 12 February 2002., Vol. 107, No. E2, 12 February 2002.
Grimm, R. E., “A Comparison of Time Domain Electromagnetic and Surface Nuclear MagneticGrimm, R. E., “A Comparison of Time Domain Electromagnetic and Surface Nuclear Magnetic
Resonance Sounding for Subsurface Water On Mars”.Resonance Sounding for Subsurface Water On Mars”. Journal of Geophysical ResearchJournal of Geophysical Research ,,
Vol. 108, No. E4, 22 April 2003.Vol. 108, No. E4, 22 April 2003.
McNeill, J. D., “Use of Electromagnetic Methods for Groundwater Studies”. In:McNeill, J. D., “Use of Electromagnetic Methods for Groundwater Studies”. In: GeotechnicalGeotechnical
and Environmental Geophysics, Volume 1, Review and Tutorialand Environmental Geophysics, Volume 1, Review and Tutorial . Ward, S. H., editor.. Ward, S. H., editor.
Society of Exploration Geophysicists, Tulsa, Oklahoma, 1990.Society of Exploration Geophysicists, Tulsa, Oklahoma, 1990.
Palacky, G. J., “Resistivity Characteristics of Geologic Targets”. In:Palacky, G. J., “Resistivity Characteristics of Geologic Targets”. In: Electromagnetic MethodsElectromagnetic Methods
in Applied Geophysics, Volume 1, Theoryin Applied Geophysics, Volume 1, Theory . Nabighian, M. N., editor. Society of Exploration. Nabighian, M. N., editor. Society of Exploration
Geophysicists, Series: Investigations in Geophysics, Volume 3. Tulsa, Oklahoma, 1987.Geophysicists, Series: Investigations in Geophysics, Volume 3. Tulsa, Oklahoma, 1987.
Reynolds, J. M.,Reynolds, J. M., An Introduction to Applied and Environmental GeophysicAn Introduction to Applied and Environmental Geophysic s. John Wiley & Sonss. John Wiley & Sons
Ltd., Chichester, England, 1997.Ltd., Chichester, England, 1997.
Zonge, K. L., “Introduction to TEM”. In:Zonge, K. L., “Introduction to TEM”. In: Practical Geophysics II, for the Exploration GeologisPractical Geophysics II, for the Exploration Geologis t.t.
Van Blaricom, R., editor. Northwest Mining Association, Spokane, Washington, 1992.Van Blaricom, R., editor. Northwest Mining Association, Spokane, Washington, 1992.
Kenneth L. Zonge, Owner and President, Zonge Engineering and Research Organization, Inc.,Kenneth L. Zonge, Owner and President, Zonge Engineering and Research Organization, Inc.,
Tucson, ArizonaTucson, Arizona
Carol R. Stoker, NASA Ames, Principal Investigator, Mars Analog Research and TechnologyCarol R. Stoker, NASA Ames, Principal Investigator, Mars Analog Research and Technology
Experiment (MARTE)Experiment (MARTE)
Jean Jacques Berthelier, Valerie Ciarletti and Richard Ney , Centre d’Etudes Terrestres etJean Jacques Berthelier, Valerie Ciarletti and Richard Ney , Centre d’Etudes Terrestres et
Planetaires, Velizy, FrancePlanetaires, Velizy, France
Editor's Notes
Dick Morris’ talk at LPSC 35 referred to Rio Tinto as an analog environment to that of the MER-B landing site for the formation of jarocite (acidic environment; pH ~1.5-3). Jeff Kargel also referred to Rio Tinto at the same meeting. If you want to know more about the Rio Tinto analog, refer to David Fernandez’ and Carol Stoker’s talks at LPSC 35, and earlier work in Rio Tinto by them and others.
More radiated power than orbital, better resolution, no surface scattering. Reflection off dielectric contrast. 2-D profile of subsurface. Layers &lt; 1 m thick (high resolution).
Field setup of experimental static (sounding) radar system in 1-5 MHz range (low frequency GPR). Netlander prototype, developed by CETP (Centre d’Etudes Terrestres et Planetaires), Velizy, France.
Penetration depth depends on electric and magnetic properties of the soil. Penetration depth in single homogeneous layer, assuming propagation. Mars analog materials. More conductive material =&gt; smaller penetration depth. Basalt: 2 MHz ~ 600 m ; 10 MHz ~ 300 m.
In this location, with the presence of the thin clay layers, the radar was unable to sound the water table at ~100 m depth.
LR corner: hydrogeological map (depths to water table), ‘Exposed’: Baharïya Oasis. Red stars = radar shots. Blue line is the location of the hydrogeological cross-section in the following slide (SE is to the left in the following slide).
Clays at T1 & T2, water table ~100 m, radar unable to sound this relatively shallow water table.
T3: Water table ~600 m, no clays, highly resistive, radar was able to sound water table at ~600 m.
T4: Analysis still in progress, preliminary results show water table at ~900 m.
Amplitude after many iterations of amplification / gain.
Relative dielectric constant. Geoelectrical model from laboratory measurements of samples from surface outcrop of each layer.