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Salt imaging in the Nordkapp Basin with electromagnetic data
Classification: Internal Status: Draft Salt imaging in the Nordkapp Basin with electromagnetic data Ketil Hokstad*, Eva Andrea Myrlund, Bente Fotland, StatoilHydro Harstad Harald Westerdahl, StatoilHydro (formerly NGI) Kai Hogstad, Arild Ingebrigtsen, formerly Statoil Luca Masnaghetti, Geosystem WG EM Lina Uri, EMGS AAPG Moscow 1. October 2009
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The Nordkapp Basin - Location
Disputed Area Two wells in the basin. Bjarmeland Platform Nordkapp basin North Hammerfest basin Nordkapp basin South Finnmark Platform
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Main reservoir target- Carnian sst
Quaternary Tertiary Cretaceous Jurassic Triassic Approximately 30 salt bodies. Diapirs in South Salt walls in North Main reservoir target- Carnian sst Permian
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Uranus pre and post-well interpretations
Max salt interpretation post-well: Worst case scenario ! Pre-well Point on 7227/11-1A well path Depth (m) TD 7227/11-1A The seismic imaging problem Weak primaries Strong multiples Diffractions
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High-resolution image of the sea floor from site survey data
The seismic shadow zone- seafloor 5 km 7227/11-1S High-resolution image of the sea floor from site survey data These are present in the whole region.
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The seismic shadow zone- where is top salt?
Cretaceous sediments Seafloor Young sediments Top diapir Salt? Obs this is not the main reason behind the shadow zone, but it contributes a great deal The top of salt often represents a very strong and undulating reflector resulting in focusing/defocusing energy effects and generating diffractions.
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The seismic shadow zone - caprock and salt inpurities
Cap rock (Permian) Pandora From the original deposition of salt in the evaporittic sequence other sediments such as gypsum, its dewatered equivalent anhydrite, shales muds and carbonates will exist in the matter that makes up the diapir, as the matter moves into the diapir and upwards these layers will be broken up and transported with the lines of flow in the salt. As top of the diapir is exposed to meteoric water during times of terrestrial conditions the halite part of the diapir will be desolved and leaves a caotic, cumulated cap rock layer. These bits and bobs of vareing density and velocity will set up random reflections that adds to the allready difficult seismic image. (Diapir)
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Velocity models “Dirty salt”
Model 1: Clean salt model Model 2: Clean salt model with top diffractors Model 3: Dirty salt model (pertubations 70% of salt velocity) Model 4: Dirty salt model with top diffractors(pertubations 70% of salt velocity) Haugen, Arntsen and Mispel, SEG 2008
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PSDM with clean-salt velocity model
Diffractors Diffractors and rugous top salt Real data Haugen, Arntsen and Mispel, SEG 2008
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Can we image the salt-sediment interface with alternative geophysical methods?
Characteristic properties of rock salt: Low mass density Gravimetry High electric resitivity Magnetotellurics Controlled-Source EM Imaging the salt-sediment interface with gravity and EM Seismic is needed to get the details Top Salt Top Diapir
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Salt imaging with CSEM Phase 1: Proving the concept
Novel idea proposed by Harald Westerdahl, formerly NGI: Salt has high resistivity (we logged 1000 Ohm-m in Uranus well) Salt imaging using CSEM should be feasible Receiver development and field test with NGI in 2006 Receiver sled landing on Uranus seabed, 15. August 2006 Pre-survey modeling Real data – 100 Hz
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Feasibility - CSEM Max and min salt models
Salt resistrivity: 1000 Ohmm Can CSEM discriminate between max and min salt cases? Can CSEM see the salt stem? Statoil in-house
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Real vs 3D synthetic data
Total field amplitude, 1 and 10 Hz Statoil in-house
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Min vs max salt interpretation
Relative Magnitude Difference Phase Difference Statoil in-house
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Min salt with and without stem
Relative Magnitude Difference Phase Difference Statoil in-house
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Depth is correct, but lateral resolution is poor
Feasibility - MT MT is sensitive to thick high-resistive bodies Model Depth is correct, but lateral resolution is poor Inversion emgs – Lina Uri
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Feasibility - MT MT is sensitive to thick high-resistive bodies
MT is sensitive to salt shape and depth Well known from the literature Model Inversion emgs – Lina Uri
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Salt imaging with CSEM and MMT Phase 2: Acquisition with EMGS April 2007
EM acquisition with emgs, Nordkapp Basin April-May 2007 Same receivers for both CSEM and MT CSEM: Purpose designed high-frequency source signal MT: 48 hours nominal listening time
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CSEM magnitude and phase - Up-going Ex
Magnitude 3 Hz Phase 3 Hz
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CSEM salt-flood model and depth migration
StatoilHydro in-house
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Raw WVSP data; HR-comp (Otnes and Hokstad, EAGE 2009)
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WVSP after SRME; HR-comp (Otnes and Hokstad, EAGE 2009)
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WVSP Virtual source image
Uranus S01 (well line) – 3D PSDM Gravity inversion WVSP Virtual source image
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WVSP Virtual source image CSEM BoS interpretation
Uranus S01 (well line) – CSEM migration Gravity inversion WVSP Virtual source image CSEM BoS interpretation
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WVSP Virtual source image CSEM BoS interpretation
Uranus S01 (well line) – CSEM migration Gravity inversion WVSP Virtual source image CSEM BoS interpretation
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Magnetotellurics (MT)
Passive exploration method Naturally occuring geomagnetic variations is the power source
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Uranus S01 (well line) – MT apparent resistivity
TM mode MT processing by Geosystem – Luca Masnaghetti
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Account for static shift in inversion
MT inversion – typical approach 100 s Account for static shift in inversion 1D 2D 3D 02Rx302 Inversion with smoothness constraints Account for static in inversion (fixed or free parameter) Typical periods used: > 1 sec to 200 sec (1 Hz to Hz) Significance of 3D effects jugded on polarization ellipses or skew 3D near surface effects 3D basement effects
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CSEM BoS interpretation
Uranus S01 (well line) – MT inversion CSEM BoS interpretation
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WVSP Virtual source image CSEM BoS interpretation
Uranus S01 (well line) – MT and CSEM WVSP Virtual source image Pick 10 Ohm-m iso-resistivity surface as BoS, concistent with CSEM and gravity CSEM BoS interpretation
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Nordkapp Basin - Brief geological history
Early Triassic: Reactive diapirism Tertiary: Diapir shortening and uplift Middle Triassic: Differential loading Tertiary: Erosion Middle Triassic: Rapid diapir rise and salt extrusion Nilsen, Vendeville and Johansen (1995)
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Economic implications of salt body size and shape
Uranus Large salt – small volumes Small salt and overhang – large volumes
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Salt imaging with CSEM and MMT Phase 3: EM campaign in Seismic Area F (PL230)
Layout 4 Layout 3 Layout 2 Layout 1 Uranus ST0750 Mostly Harmless Jupiter 4 layouts of 48 receivers 13 EM lines Including mini 3D Covering 11 diapirs
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EM campaign – Results MT inversion CSEM depth migration
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Photo: Eva Andrea Myrlund
Conclusions Base and flanks of salt in NKB can not be properly imaged using seismic alone MT and CSEM contribute important information, but with lower resolution than seismics Data integration is important to complete the NKB imaging puzzle (EM, grav, seismic) Most likely there are no diapirs like the Uranus pre-well model in Southern Nordkapp Basin Photo: Eva Andrea Myrlund
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Photo: Eva Andrea Myrlund
Acknowledgements StatoilHydro GET/R&D Christopher Stadtler Kerstin Henneberg Erik Gundersen Andreas Becht Christine Fichler Alexander Kritski Lars Løseth Jon Andre Haugen Børge Arntsen Rune Kyrkjebø Partners: GdF Suez (PL230) Chevron and RWE (PL397) emgs: Kristoffer Engenes (Aker) Rune Mittet Crew of OS Relume Geosystem WG-EM: Don Watts StatoilHydro Management Geir Richardsen John Reidar Granli Tage Røsten ex-Statoil: Einar Otnes (WG) Constantin Gerea (Total) Photo: Eva Andrea Myrlund
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