SlideShare a Scribd company logo
1 of 16
Download to read offline
Joint 3D inversion of gravity and
magnetic data with geological
constraints - an alternative approach
Ilya Prutkin (1), Peter Vajda (2), and Gerhard Jentzsch (1)
(1) Institute of Earth Sciences, Jena University, Jena, Germany
(2) Earth Science Institute, Slovak Academy of Sciences,
Bratislava, Slovakia
v
Our approach to 3D interpretation of
gravity/magnetic data
• Preliminary separation of sources
- in depth based on subsequent upward and downward
continuation
- in the lateral direction using approximation with the
field of several 3D line segments
- according to density and magnetization contrast by
calculation of pseudo-gravity
• Original algorithms for 3D gravity and magnetic data
inversion
- for restricted objects of arbitrary shape
- for 3D topography of contact surfaces
Initial data set (GGD Leipzig)
Initial data. Left: gravity (Bouguer anomalies, grid distance 500m).
Right: magnetic (total magnetic intensity anomalies, grid distance
250 m)
Long wavelengths
Low-frequency component
of the geological model
effect (top left), the same for
initial data (top right) and for
residuals (bottom right),
which we attribute to an
uplift of Moho
Comparison with magnetic data
Long wavelengths for gravity (left) and magnetic data (right)
Their comparison reveals that gravitational and magnetic anomalies are
caused partly by different objects. The low-frequency component of gravity
is caused by the uplift of Moho and the long-wave effect of the basin
structure, meanwhile the same component of the magnetic field is
generated by the Mid-German Crystalline High
Intermediate wavelengths
ρ = 2.85g/cm3
ρ = 2.75g/cm3
z≈10km
Gravity (intermediate wavelengths)
(top left) and its inversion after
subtracting negative anomalies
Top right: depths to the contact
surface, bottom: 3D model of
topography
Approximation of a local anomaly
Top: zoomed anomaly (left), regional field model (right). Bottom: residuals (left)
and their approximation with 3D line segments (right). RMS=0.41mGal
Problem of low frequencies
z=0
Deep object => long wavelengths
prevail
Equivalently, if the signal contains
high frequencies, it is caused by
near-surface objects
The converse implication is
not necessarily true:
the basin structure contributes
substantially into low frequencies
Top right: density interfaces
with the same field as a point
source; bottom right:
comparison of inversion results
and boreholes data
3D model for intermediate
wavelengths
We transform line segments to 3D restricted bodies with the same field and
put them back. The obtained model for the the main intermediate sources
includes three low-density bodies that we interpret as granitic intrusions,
and a density interface with topography below them (~10 km depth)
Comparison of gravity anomalies
and known faults
Interpretation of the arc-shaped
anomaly
Top: magnetics. Bottom: pseudo-gravity and measured gravity
3D inversion for an uplift of
the crystalline basement
Kyffhäuser
Depths to the
contact surface
Geomagnetische Karte
von Sachsen-Anhalt als
Pseudoreliefdarstellung
© 2014 LAGB
Kyffhäuser represents not
an isolated hill
surrounded by a flat
surface (TLUG model),
but a top of
a prolonged mountain
chain. Magnetic anomaly
continues farther to
Sachsen-Anhalt
3D model of the topography
3D inversion for SW-NE anomaly
Top: gravity (left) and magnetics
(right). Bottom: depths to the
contact surface found by our
inversion algorithm.
Both anomalies are caused
allegedly by the same uplift of
the crystalline basement
Fahner Hoehe: residual gravity
Gravity data. A star – location of the
Neudietendorf borehole, dashed line
- a south-north profile, the section
along it is shown in the next slide
3D inversion for a salt deposit
geometry. Red – upper boundary of
the Zechstein layer (according to the
TLUG geological model), blue –
shape of the salt pillow found based
on our inversion algorithm
Fahner Hoehe: IGMAS modeling
According to IGMAS modeling, for the area of the Fahner
anticline, process of folding affects also the upper boundary of
the crystalline layer
Conclusions

Separating into long, intermediate and short wavelengths
provide opportunity to investigate deep structure of the
Thuringian Basin: granitic intrusions above density interface

For a local area, we subtract the model of the regional field (2D
harmonic function), approximate the residuals with 3D line
segments (quite stable) and transform a chosen set of line
segments into a restricted object or a contact surface (in the
class of uniqueness)

3D inversion of magnetic data allow investigating of fine
structure for the crystalline basement (arc-shaped and linear
uplifts)

We study salt tectonics for local areas. With some preliminary
assumptions it is possible, to isolate the effect of a salt deposit
and to find its unknown geometry

More Related Content

What's hot

experimental stress analysis-Chapter 5
experimental stress analysis-Chapter 5experimental stress analysis-Chapter 5
experimental stress analysis-Chapter 5MAHESH HUDALI
 
Seismic Imaging using wave theory
Seismic Imaging using wave theorySeismic Imaging using wave theory
Seismic Imaging using wave theoryYasir Bashir
 
experimental stress analysis-Chapter 3
experimental stress analysis-Chapter 3experimental stress analysis-Chapter 3
experimental stress analysis-Chapter 3MAHESH HUDALI
 
Hayashi masw gravity
Hayashi masw gravityHayashi masw gravity
Hayashi masw gravityhugang2003
 
Modelling of 3D gelogical structures
Modelling of 3D gelogical structuresModelling of 3D gelogical structures
Modelling of 3D gelogical structuresZawar Khan
 
A Gravity survey is an indirect (surface) means of calculating the density pr...
A Gravity survey is an indirect (surface) means of calculating the density pr...A Gravity survey is an indirect (surface) means of calculating the density pr...
A Gravity survey is an indirect (surface) means of calculating the density pr...Shahid Hussain
 
ESA Module 3 Part-A ME832. by Dr. Mohammed Imran
ESA Module 3 Part-A ME832. by Dr. Mohammed ImranESA Module 3 Part-A ME832. by Dr. Mohammed Imran
ESA Module 3 Part-A ME832. by Dr. Mohammed ImranMohammed Imran
 
The Effect of Topography on The Seismic Wavefield
The Effect of Topography on The Seismic WavefieldThe Effect of Topography on The Seismic Wavefield
The Effect of Topography on The Seismic WavefieldUlrika Miller
 
FR3.TO5.2.pptx
FR3.TO5.2.pptxFR3.TO5.2.pptx
FR3.TO5.2.pptxgrssieee
 
Goodness Dispersion Curves for Ultrasonic Guided Wave based SHM
Goodness Dispersion Curves for Ultrasonic Guided Wave based SHMGoodness Dispersion Curves for Ultrasonic Guided Wave based SHM
Goodness Dispersion Curves for Ultrasonic Guided Wave based SHMInnerspec Technologies
 
Application of atomic force spectroscopy (afs) to studies of adhesion phenomena
Application of atomic force spectroscopy (afs) to studies of adhesion phenomenaApplication of atomic force spectroscopy (afs) to studies of adhesion phenomena
Application of atomic force spectroscopy (afs) to studies of adhesion phenomenaGrupo de Pesquisa em Nanoneurobiofisica
 
Numerical Study of Strong Free Surface Flow and Wave Breaking
Numerical Study of Strong Free Surface Flow and Wave BreakingNumerical Study of Strong Free Surface Flow and Wave Breaking
Numerical Study of Strong Free Surface Flow and Wave BreakingYi Liu
 

What's hot (20)

Seismic Methods
Seismic MethodsSeismic Methods
Seismic Methods
 
Photoelasticity
Photoelasticity Photoelasticity
Photoelasticity
 
experimental stress analysis-Chapter 5
experimental stress analysis-Chapter 5experimental stress analysis-Chapter 5
experimental stress analysis-Chapter 5
 
Seismic Imaging using wave theory
Seismic Imaging using wave theorySeismic Imaging using wave theory
Seismic Imaging using wave theory
 
experimental stress analysis-Chapter 3
experimental stress analysis-Chapter 3experimental stress analysis-Chapter 3
experimental stress analysis-Chapter 3
 
Hayashi masw gravity
Hayashi masw gravityHayashi masw gravity
Hayashi masw gravity
 
Modelling of 3D gelogical structures
Modelling of 3D gelogical structuresModelling of 3D gelogical structures
Modelling of 3D gelogical structures
 
Gravity Method | Geophysics | Geology
Gravity Method | Geophysics | GeologyGravity Method | Geophysics | Geology
Gravity Method | Geophysics | Geology
 
Presentation
PresentationPresentation
Presentation
 
A Gravity survey is an indirect (surface) means of calculating the density pr...
A Gravity survey is an indirect (surface) means of calculating the density pr...A Gravity survey is an indirect (surface) means of calculating the density pr...
A Gravity survey is an indirect (surface) means of calculating the density pr...
 
ESA Module 3 Part-A ME832. by Dr. Mohammed Imran
ESA Module 3 Part-A ME832. by Dr. Mohammed ImranESA Module 3 Part-A ME832. by Dr. Mohammed Imran
ESA Module 3 Part-A ME832. by Dr. Mohammed Imran
 
Gravity method
Gravity method Gravity method
Gravity method
 
3 d potostress
3 d potostress3 d potostress
3 d potostress
 
The Effect of Topography on The Seismic Wavefield
The Effect of Topography on The Seismic WavefieldThe Effect of Topography on The Seismic Wavefield
The Effect of Topography on The Seismic Wavefield
 
FR3.TO5.2.pptx
FR3.TO5.2.pptxFR3.TO5.2.pptx
FR3.TO5.2.pptx
 
Gravity Method
Gravity MethodGravity Method
Gravity Method
 
Goodness Dispersion Curves for Ultrasonic Guided Wave based SHM
Goodness Dispersion Curves for Ultrasonic Guided Wave based SHMGoodness Dispersion Curves for Ultrasonic Guided Wave based SHM
Goodness Dispersion Curves for Ultrasonic Guided Wave based SHM
 
Rocchi
RocchiRocchi
Rocchi
 
Application of atomic force spectroscopy (afs) to studies of adhesion phenomena
Application of atomic force spectroscopy (afs) to studies of adhesion phenomenaApplication of atomic force spectroscopy (afs) to studies of adhesion phenomena
Application of atomic force spectroscopy (afs) to studies of adhesion phenomena
 
Numerical Study of Strong Free Surface Flow and Wave Breaking
Numerical Study of Strong Free Surface Flow and Wave BreakingNumerical Study of Strong Free Surface Flow and Wave Breaking
Numerical Study of Strong Free Surface Flow and Wave Breaking
 

Similar to eguPrutkin

2D and 3D Density Block Models Creation Based on Isostasy Usage
2D and 3D Density Block Models Creation Based on Isostasy Usage2D and 3D Density Block Models Creation Based on Isostasy Usage
2D and 3D Density Block Models Creation Based on Isostasy Usageatsidaev
 
Lateral resolution and lithological interpretation of surface wave profi ling
Lateral resolution and lithological interpretation of surface wave profi lingLateral resolution and lithological interpretation of surface wave profi ling
Lateral resolution and lithological interpretation of surface wave profi lingAdam O'Neill
 
The distribution and_annihilation_of_dark_matter_around_black_holes
The distribution and_annihilation_of_dark_matter_around_black_holesThe distribution and_annihilation_of_dark_matter_around_black_holes
The distribution and_annihilation_of_dark_matter_around_black_holesSérgio Sacani
 
Mapping WGMs of erbium doped glass microsphere using near-field optical probe...
Mapping WGMs of erbium doped glass microsphere using near-field optical probe...Mapping WGMs of erbium doped glass microsphere using near-field optical probe...
Mapping WGMs of erbium doped glass microsphere using near-field optical probe...NuioKila
 
MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...
MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...
MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...ijrap
 
II_Quantum Hall Effects&Quantum Transport
II_Quantum Hall Effects&Quantum TransportII_Quantum Hall Effects&Quantum Transport
II_Quantum Hall Effects&Quantum TransportGiuseppe Maruccio
 
Engineering geophysical study of unconsolidated top soil using shallow seismi...
Engineering geophysical study of unconsolidated top soil using shallow seismi...Engineering geophysical study of unconsolidated top soil using shallow seismi...
Engineering geophysical study of unconsolidated top soil using shallow seismi...Alexander Decker
 
Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ...
 Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ... Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ...
Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ...ijrap
 
Chapter 5-Magnetostatics engineering electromagnetics
Chapter 5-Magnetostatics engineering electromagneticsChapter 5-Magnetostatics engineering electromagnetics
Chapter 5-Magnetostatics engineering electromagneticsDr. Amjad Hussain
 
Magnetic Materials Assignment Help
Magnetic Materials Assignment HelpMagnetic Materials Assignment Help
Magnetic Materials Assignment HelpEdu Assignment Help
 
International Montoro Res. Wicheeda North_Mag_Em_inv_interp_summary
International Montoro Res. Wicheeda North_Mag_Em_inv_interp_summaryInternational Montoro Res. Wicheeda North_Mag_Em_inv_interp_summary
International Montoro Res. Wicheeda North_Mag_Em_inv_interp_summaryFollow me on Twitter @Stockshaman
 

Similar to eguPrutkin (20)

EGU2016-2988
EGU2016-2988EGU2016-2988
EGU2016-2988
 
2D and 3D Density Block Models Creation Based on Isostasy Usage
2D and 3D Density Block Models Creation Based on Isostasy Usage2D and 3D Density Block Models Creation Based on Isostasy Usage
2D and 3D Density Block Models Creation Based on Isostasy Usage
 
Taramelli Melelli
Taramelli MelelliTaramelli Melelli
Taramelli Melelli
 
Lateral resolution and lithological interpretation of surface wave profi ling
Lateral resolution and lithological interpretation of surface wave profi lingLateral resolution and lithological interpretation of surface wave profi ling
Lateral resolution and lithological interpretation of surface wave profi ling
 
Swi seminar final
Swi seminar finalSwi seminar final
Swi seminar final
 
The distribution and_annihilation_of_dark_matter_around_black_holes
The distribution and_annihilation_of_dark_matter_around_black_holesThe distribution and_annihilation_of_dark_matter_around_black_holes
The distribution and_annihilation_of_dark_matter_around_black_holes
 
Magnetic domain and domain walls
 Magnetic domain and domain walls Magnetic domain and domain walls
Magnetic domain and domain walls
 
Mapping WGMs of erbium doped glass microsphere using near-field optical probe...
Mapping WGMs of erbium doped glass microsphere using near-field optical probe...Mapping WGMs of erbium doped glass microsphere using near-field optical probe...
Mapping WGMs of erbium doped glass microsphere using near-field optical probe...
 
MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...
MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...
MAGNETOSTATIC SURFACE WAVES IN A LEFT HANDED / FERRITE/ METAL-STRIP-GRATING S...
 
II_Quantum Hall Effects&Quantum Transport
II_Quantum Hall Effects&Quantum TransportII_Quantum Hall Effects&Quantum Transport
II_Quantum Hall Effects&Quantum Transport
 
Surface Wave Tomography
Surface Wave TomographySurface Wave Tomography
Surface Wave Tomography
 
Surface Wave Tomography
Surface Wave TomographySurface Wave Tomography
Surface Wave Tomography
 
Engineering geophysical study of unconsolidated top soil using shallow seismi...
Engineering geophysical study of unconsolidated top soil using shallow seismi...Engineering geophysical study of unconsolidated top soil using shallow seismi...
Engineering geophysical study of unconsolidated top soil using shallow seismi...
 
gravitywaves
gravitywavesgravitywaves
gravitywaves
 
Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ...
 Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ... Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ...
Magnetostatic Surface Waves in a Left Handed / Ferrite/ Metal-Strip-Grating ...
 
Chapter 5-Magnetostatics engineering electromagnetics
Chapter 5-Magnetostatics engineering electromagneticsChapter 5-Magnetostatics engineering electromagnetics
Chapter 5-Magnetostatics engineering electromagnetics
 
Poster_3D_v04
Poster_3D_v04Poster_3D_v04
Poster_3D_v04
 
Magnetic Materials Assignment Help
Magnetic Materials Assignment HelpMagnetic Materials Assignment Help
Magnetic Materials Assignment Help
 
International Montoro Res. Wicheeda North_Mag_Em_inv_interp_summary
International Montoro Res. Wicheeda North_Mag_Em_inv_interp_summaryInternational Montoro Res. Wicheeda North_Mag_Em_inv_interp_summary
International Montoro Res. Wicheeda North_Mag_Em_inv_interp_summary
 
Cray bh
Cray bhCray bh
Cray bh
 

eguPrutkin

  • 1. Joint 3D inversion of gravity and magnetic data with geological constraints - an alternative approach Ilya Prutkin (1), Peter Vajda (2), and Gerhard Jentzsch (1) (1) Institute of Earth Sciences, Jena University, Jena, Germany (2) Earth Science Institute, Slovak Academy of Sciences, Bratislava, Slovakia v
  • 2. Our approach to 3D interpretation of gravity/magnetic data • Preliminary separation of sources - in depth based on subsequent upward and downward continuation - in the lateral direction using approximation with the field of several 3D line segments - according to density and magnetization contrast by calculation of pseudo-gravity • Original algorithms for 3D gravity and magnetic data inversion - for restricted objects of arbitrary shape - for 3D topography of contact surfaces
  • 3. Initial data set (GGD Leipzig) Initial data. Left: gravity (Bouguer anomalies, grid distance 500m). Right: magnetic (total magnetic intensity anomalies, grid distance 250 m)
  • 4. Long wavelengths Low-frequency component of the geological model effect (top left), the same for initial data (top right) and for residuals (bottom right), which we attribute to an uplift of Moho
  • 5. Comparison with magnetic data Long wavelengths for gravity (left) and magnetic data (right) Their comparison reveals that gravitational and magnetic anomalies are caused partly by different objects. The low-frequency component of gravity is caused by the uplift of Moho and the long-wave effect of the basin structure, meanwhile the same component of the magnetic field is generated by the Mid-German Crystalline High
  • 6. Intermediate wavelengths ρ = 2.85g/cm3 ρ = 2.75g/cm3 z≈10km Gravity (intermediate wavelengths) (top left) and its inversion after subtracting negative anomalies Top right: depths to the contact surface, bottom: 3D model of topography
  • 7. Approximation of a local anomaly Top: zoomed anomaly (left), regional field model (right). Bottom: residuals (left) and their approximation with 3D line segments (right). RMS=0.41mGal
  • 8. Problem of low frequencies z=0 Deep object => long wavelengths prevail Equivalently, if the signal contains high frequencies, it is caused by near-surface objects The converse implication is not necessarily true: the basin structure contributes substantially into low frequencies Top right: density interfaces with the same field as a point source; bottom right: comparison of inversion results and boreholes data
  • 9. 3D model for intermediate wavelengths We transform line segments to 3D restricted bodies with the same field and put them back. The obtained model for the the main intermediate sources includes three low-density bodies that we interpret as granitic intrusions, and a density interface with topography below them (~10 km depth)
  • 10. Comparison of gravity anomalies and known faults
  • 11. Interpretation of the arc-shaped anomaly Top: magnetics. Bottom: pseudo-gravity and measured gravity
  • 12. 3D inversion for an uplift of the crystalline basement Kyffhäuser Depths to the contact surface Geomagnetische Karte von Sachsen-Anhalt als Pseudoreliefdarstellung © 2014 LAGB Kyffhäuser represents not an isolated hill surrounded by a flat surface (TLUG model), but a top of a prolonged mountain chain. Magnetic anomaly continues farther to Sachsen-Anhalt 3D model of the topography
  • 13. 3D inversion for SW-NE anomaly Top: gravity (left) and magnetics (right). Bottom: depths to the contact surface found by our inversion algorithm. Both anomalies are caused allegedly by the same uplift of the crystalline basement
  • 14. Fahner Hoehe: residual gravity Gravity data. A star – location of the Neudietendorf borehole, dashed line - a south-north profile, the section along it is shown in the next slide 3D inversion for a salt deposit geometry. Red – upper boundary of the Zechstein layer (according to the TLUG geological model), blue – shape of the salt pillow found based on our inversion algorithm
  • 15. Fahner Hoehe: IGMAS modeling According to IGMAS modeling, for the area of the Fahner anticline, process of folding affects also the upper boundary of the crystalline layer
  • 16. Conclusions  Separating into long, intermediate and short wavelengths provide opportunity to investigate deep structure of the Thuringian Basin: granitic intrusions above density interface  For a local area, we subtract the model of the regional field (2D harmonic function), approximate the residuals with 3D line segments (quite stable) and transform a chosen set of line segments into a restricted object or a contact surface (in the class of uniqueness)  3D inversion of magnetic data allow investigating of fine structure for the crystalline basement (arc-shaped and linear uplifts)  We study salt tectonics for local areas. With some preliminary assumptions it is possible, to isolate the effect of a salt deposit and to find its unknown geometry