USE SAR INTERFEROMETRY DINSAR AND PSI TO IDENTIFY THE GEOHAZARD RISK OF NATO AIRPORT NORTH EAST LARISSA (CENTRAL GREECE) Falah FAKHRI Harokopio University.

Slides:



Advertisements
Similar presentations
APPLICATION OF SATELLITE RADAR INTERFEROMETRY ON THE AREAS OF UNDERGROUND EXPLOITATION OF COPPER ORE IN LGOM - POLAND ZASTOSOWANIE SATELITARNEJ INTERFEROMETRII.
Advertisements

Surface Water and Ocean Topography (SWOT) Satellite Mission
2. The WAM Model: Solves energy balance equation, including Snonlin
GROUND DEFORMATION OCCURRING IN THE GREATER VANCOUVER REGION FROM TWENTY YEARS OF ERS-ENVISAT-RADARSAT-2 INSAR OBSERVATIONS Sergey Samsonov 1, Pablo J.
Page 1 ASAR Validatoin Review - ESRIN – 9-13 December 2002 Ocean geophysical results from ASAR  Geophysical overview  ocean spectra : the isidore case.
Page 1 ENVISAT Press Day - ESTEC, 1 February 2001 Fabio Rocca Dipartimento di Elettronica e Informazione Politecnico di Milano Envisat for the physics.
1 Verification of wave forecast models Martin Holt Jim Gunson Damian Holmes-Bell.
Statistics on Obesity, PA & Diet: England, Jan 08 i Compiled by Sally Cornfield on behalf of PAN-WM Headline Findings.
Radar Remote Sensing By Falah Fakhri Post-doctoral Scholar
USEReST - Naples 2008 Terrain Deformation Monitoring with PSInSAR TM Marco Bianchi Sensing the planet Marco Basilico
SAR Interferometry (InSAR): principles
ACKNOWLEDGEMENT: We thank the Canadian Space Agency (CSA) for providing RADARSAT-2 data. Figures were plotted with GMT and Gnuplot software and statistical.
Studying Volcanoes With InSAR: Where Have We Been and Where Are We Going? Howard Zebker, Cody Wortham Stanford University.
Batch processing, stacking and time series analysis
Generation of the 2004 Sumatra-Andaman Tsunami WHIO, 30 Oct., 2006.
The Mw 6.5 Bam earthquake of 26 Dec 2003: Precise source parameters from D-InSAR by R. Wang, Y. Xia, H. Grosser, H.-U. Wetzel, H. Kaufmann, M. Motagh,J.
ALOS PALSAR interferometry of Taupo Volcanic Zone, New Zealand Sergey Samsonov 1,3, John Beavan 1, Chris Bromley 2, Bradley Scott 2, Gill Jolly 2 and Kristy.
(1) ASRC Research and Technology Solutions, Contractor to U.S.Geological Survey (USGS) Cascades Volcano Observatory (CVO), Vancouver, WA, USA;
Motion of Glaciers, Sea Ice, and Ice Shelves in Canisteo Peninsula, West Antarctica Observed by 4-Pass Differential Interferometric SAR Technique Hyangsun.
Pierre Briole1, Panagiotis Elias2, Giuseppe Puglisi3, Makoto Murakami4
Deformation along the north African plate boundary observed by InSAR Ian Hamling 1,2 Abdelkrim Aoudia 2 1.GNS Science, Avalon, New Zealand 2.ICTP, Trieste,
Active and Neotectonic Structures 1) What's the difference
C.C.Tscherning, Nov Synthetic Aperture Radar. Material from: SAR Light Lectures by J.J.Mohr ESA TM-19 A,B,C. Skagen Investigation DESCW - ESA.
Page 1 Alain Arnaud, CEO Ground displacement monitoring using radar satellite images Alain ARNAUD, CEO.
Data Acquisition and Processing GPRI-II imaged the glacier and peripheral ice at 3-minute intervals Gamma’s Differential Interferometry and Geocoding Software.
Remote Sensing and Active Tectonics Barry Parsons and Richard Walker Michaelmas Term 2011 Lecture 4.
IGARSS 2011 – July, Vancouver, Canada Investigating the seismic cycle in Italy by multitemporal analysis of ALOS, COSMO-SkyMed and ERS/Envisat DInSAR.
The Extraction of Ocean Wind, Wave, and Current Parameters Using SAR Imagery Moon-kyung Kang 1*, Hoonyol Lee 2, Moonjin Lee 3, Yong-Wook Park 4, Wang-Jung.
Urs Wegmüller Gamma Remote Sensing AG, Gümligen, Switzerland Monitoring Alpine Transportation Infrastructures Using Space Techniques.
The 2003 Bam, Iran earthquake: what we knew, what we didn’t know and what we expect in the future Gareth Funning (University of California, Berkeley) with.
Long Time Span Interferograms and Effects of Snow Cover on Interferometric Phase at L-Band Khalid A. Soofi (ConocoPhillips), David Sandwell (UCSD, SCRIPPS)
Quaternary volcanism in the Afar Depression (Ethiopia and Eritrea) ) Merged Landsat TM and Synthetic Aperture Radar (JERS-1) satellite image of Dubbi volcano,
1 SPACE BORNE RADAR INTERFEROMETRIC MAPPING OF PRECURSORY DEFORMATIONS OF A DYKE COLLAPSE, DEAD SEA, JORDAN Closson, Abou Karaki, al-Fugha
Research Groups: Global Environmental Measurements Group for Advanced Receiver Development Radar Remote Sensing Radio Astronomy Space Geodesy.
Page 1 Alain Arnaud, CEO Contribution to GEOSS Satellite InSAR – PSI for ground displacement mapping Alain ARNAUD, CEO.
THE APRIL 3, 2010 EARTHQUAKE ALONG THE PERNICANA FAULT (MT. ETNA - ITALY): ANALYSIS OF SATELLITE AND IN SITU GROUND DEFORMATION DATA INTEGRATED BY THE.
InSAR and LIDAR Lecture 8 Oct 13, 2004.
Sea ice thickness from CryoSat – A new data set for operational ice services? Christian Haas German CryoSat Office AWI.
I hope its ok to do these InSAR exercises as the lab
LONG TERM GEODETIC MONITORING OF THE DEFORMATION OF A LIQUID STORAGE TANK FOUNDED ON PILES P. Savvaidis Laboratory of Geodesy Dept. of Civil Engineering.
Geodetic Monitoring of the Deformation of a 50,000 t Sugar Storage Tank Founded on 124 Long Bored Piles P. Savvaidis and I. Ifadis Laboratory of Geodesy.
0 Riparian Zone Health Project Agriculture and Agri-Food Canada Grant S. Wiseman, BS.c, MSc. World Congress of Agroforestry Nairobi, Kenya August 23-28,
How does InSAR work? Gareth Funning University of California, Riverside.
InSAR Processing and Applications
C.C.Tscherning, Sat_geoph11, lec_day_10_1.ppt, Synthetic Aperture Radar. Material from: SAR Light Lectures by J.J.Mohr ESA TM-19 A,B,C. Skagen.
Introduction to Interferometric Synthetic Aperture Radar - InSAR
Measurement of a Temporal Sequence Of DInSAR Phase Changes Due to Soil Moisture Variations Keith Morrison 1, John Bennett 2, Matt Nolan 3, and Raghav Menon.
Francesco Casu IREA - CNR, Napoli, Italy
Synthetic aperture radar (SAR) data … also, use ENVISAT (C-band) data from the same time period to resolve vertical/horizontal components of surface velocity.
2002/05/07ACES Workshop Spatio-temporal slip distribution around the Japanese Islands deduced from Geodetic Data Takeshi Sagiya Geographical Survey Institute.
South East Strategic Regional Coastal Monitoring Programme – Annual Review Meeting, November 2009 Satellite Data for Coastal Monitoring Trevor Burton Fugro-BKS.
IGARSS’ July, Vancouver, Canada Subsidence Monitoring Using Polarimetric Persistent Scatterers Interferometry Victor D. Navarro-Sanchez and Juan.
Fault Plane Solution Focal Mechanism.
Norris subsidence Caldera-wide uplift Figure 1 – ENVISAT beam mode 1 interferogram spanning and showing deformation in the region of Yellowstone.
Tectonic landscapes. What impact does tectonic activity have on landscapes and why does this impact vary? Volcanic activity: Variations in the form,
MOMENT TENSOR INVERSION OF POSSIBLY MULTIPLE EVENTS AT REGIONAL DISTANCES Petra Adamová 1, Jiří Zahradník 1, George Stavrakakis 2 1 Charles University.
GEOGG141 / GEOG3051 Principles & Practice of Remote Sensing (PPRS) RADAR II: Interferometry Dr. Mathias (Mat) Disney UCL Geography Office: 113, Pearson.
Motion of David Glacier in East Antarctica Observed by
Class tutorial Measuring Earthquake and volcano activity from space Shimon Wdowinski University of Miami.
HSAF Soil Moisture Training
Royal Military Academy
Images courtesy of Google Earth (top), and USGS (bottom).
Figure 1 ENVISAT beam mode 2, track 61 interferogram covering June 26, 2004 to Febrary 26, Inflation amounts to several tens of centimeters and.
Analysis of the Ms=6.2, June 15, 1995 Aigion earthquake(Greece) :
Figure 1. ENVISAT beam mode 4, track 136 interferogram spanning 11 April to 20 June Bulls-eye-shaped subsidence at the summit was caused by withdrawal.
module Using DInSAR to assess vertical ground motions at Tide Gauges
學生:林承恩(Cheng-en Lin) 指導老師:陳卉瑄(Kate Huihsuan Chen)
Long and short term monitoring of ground deformation in Thessaly basin using space-based SAR Interferometry Harokopio University of Athens Department of.
For the next 4 problems, consider the following:
Dr. Mathias (Mat) Disney UCL Geography Office: 113, Pearson Building
Presentation transcript:

USE SAR INTERFEROMETRY DINSAR AND PSI TO IDENTIFY THE GEOHAZARD RISK OF NATO AIRPORT NORTH EAST LARISSA (CENTRAL GREECE) Falah FAKHRI Harokopio University of Athens, Department of Geography, El. Venizelou 70, Athens, 17671, Greece. Abstract The aim of this study is to estimate the ground deformation over the NATO airport of Larissa in Thessaly prefecture in Central Greece, for the time period between 1992 and Dataset, including a total of 24 images C band SLC (Single Look complex) SAR images, acquired from European Space Agency (ESA).Between 1995 and 2008 of ERS-1/-2 along Ascending Track 143, and 15 ENVISAT- between 2003 and Another dataset has been used is a total of 48 ERS-1/-2 C-band SLC between 1992 and 2000 ERS-1/-2, and from ENVISAT Satellite a total of 25 Scenes a long of Descending Track 279, between 2002 and Co-registration between the two datasets has been done for each track.Two separates processing techniques have been applied, the first one is Differential Intreferometric Synthetic Aperture Radar (DINSAR), interferogram stacking and the second technique is Persistent Scatters Interferometry (PSI). GAMMA S/W, 2010 has been used. The deformation rate pattern of NATO airport has been detected with interferogram stacking. Additionally many of points candidates have been detected with the PSI technique with two frames ascending and descending respectively, In order to investigate the effect of some earth phenomena, characteristics and events, such as fissures, lithology, and faults and earthquake on the estimated ground deformation rates. The deformation rate which is estimated after application both techniques, has been analyzed and presented and were correlated with the parameters mentioned above. The subsidence rate of the interferogram stacking, Ascending was varying between - 0, ,274 mm/year. However the airport has an uplift between 0,645 – 4,294 mm/year, this uplift maybe attributed to the local reason or for the location of the airport in the southwest of the normal fault in the side of footwall with distance 3,504 Km, and it is located in the west of the end of the normal fault in the side of the footwall too with distance 0,927 Km. While the result of descending track, interferogram stacking, was the subsidence between -0, ,213 mm/year, the result of subsidence Descending is near or similar with the result of the Ascending. This subsidence maybe attributed for many reasons one of these reasons is the lithology, the airport over an alluvial lithology. The second important reason is the location of the airport in the east of the side of the hanging wall of the normal fault with distance 0,625 Km. The other reason as mentioned by (Kontogianni et. al, 2007) maybe attributed to the fissures phenomena. However the airport uplift was between 0,031– 0,312 mm/year, this result is different with the result of the Ascending Track maybe this attributed to the huge of the data, number of interferograms inside the stacking were 84 while the number of interferograms inside the stacking of the Ascending track were 29. The subsidence rate of PSI Ascending was varying between mm/year however the uplift was between 1 – 25 mm/year. The result of the Descending track subsidence were between mm/year however the uplift was 1 – 11 mm/year. Table 1. Subsidence of NATO AIRPORT Ascending Track 143. NATO AIRPORT OF LARISSA Deformation rate mm/year Subsidence MinimumMaximumMeanStd.devCV% -0,085 -2,274-1,1790,9420,798 NATO AIRPORT OF LARISSA Deformation rate mm/year Uplift MinimumMaximumMeanStd.devCV% 0,6454,2942,4691,3650,552 Table 2. Uplift of NATO AIRPORT Ascending Track 143. NATO AIRPORT OF LARISSA Deformation rate mm/year Subsidence MinimumMaximumMeanStd.devCV% -0,249-2,213-1,2310,6870,558 Table 3. Subsidence of NATO AIRPORT Descending Track 279. NATO AIRPORT OF LARISSA Deformation rate mm/year Uplift MinimumMaximumMeanStd.devCV% 0,0310,3120,1710,1981,157 Table 4. Uplift of NATO AIRPORT Descending Track Figure Ground deformation rates along the LOS direction deduced by interferometric stacking, for the considered time intervals and the different acquisition Thessaly Ascending Track In background the corresponding average multi-looked SAR intensities. The selected area of NATO Airport. Normal Faults. Figure Ground deformation rates along the LOS direction deduced by interferometric stacking, for the considered time intervals and the different acquisition Thessaly Ascending Track In background the corresponding average multi-looked SAR intensities. The selected area of NATO Airport. Normal Faults. Figure Ground deformation rates along the LOS direction deduced by interferometric stacking, for the considered time intervals and the different acquisition Thessaly Ascending Track In background the corresponding average multi-looked SAR intensities. The selected area of NATO Airport. Normal Faults. Figure Ground deformation rates along the LOS direction deduced by interferometric stacking, for the considered time intervals and the different acquisition Thessaly Ascending Track In background the corresponding average multi-looked SAR intensities. The selected area of NATO Airport. Normal Faults. Figure Ground deformation rates along the LOS direction deduced by interferometric stacking, for the considered time intervals and the different acquisition Thessaly Descending Track In background the corresponding average multi-looked SAR intensities. The selected area of NATO Airport. Normal Faults. Figure Ground deformation rates along the LOS direction deduced by interferometric stacking, for the considered time intervals and the different acquisition Thessaly Ascending Track In background the corresponding average multi-looked SAR intensities. The selected area of NATO Airport. Normal Faults. Figure Ground deformation rates along the LOS direction deduced by interferometric stacking, for the considered time intervals and the different acquisition Thessaly Ascending Track In background the corresponding average multi-looked SAR intensities. The selected area of NATO Airport. Normal Faults mm/yr in LOS direction Figure points candidates of the Point Scatters Interferometric. Mean displacement rates between Ascending Track143. Movements are in the satellite line-of- sight direction,. Points are selected just inside the NATO airport. Two points with blue colour are explained mm/yr in LOS direction mm/yr in LOS direction mm/yr in LOS direction mm/yr in LOS direction mm/year in LOS Figure points candidates of the Point Scatters Interferometric. Mean displacement rates between Descending Track279. Movements are in the satellite line-of- sight direction,. Points are selected just inside the NATO airport. Two points with blue colour are explained. mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/year in LOS mm/yr in LOS direction mm/yr in LOS direction mm/yr in LOS direction Table 1. Subsidence of NATO AIRPORT Ascending Track 143. NATO AIRPORT OF LARISSA Deformation rate mm/year Subsidence MinimumMaximumMeanStd.devCV% -0,085 -2,274-1,1790,9420,798 Table 2. Uplift of NATO AIRPORT Ascending Track 143. Harokopio University of Athens, Department of Geography