High-Resolution Maps of Outlet Glacier Surface Elevation Change from Combined Laser Altimeter and Digital Elevation Model Data (ID # 962139) Joanna Fredenslund.

Slides:



Advertisements
Similar presentations
IV: Ice velocity – costal regions + select areas (phase 1), all ice sheet (ph. 2) SEC: Surface elevation changes, ERS/Envisat/CryoSat, GLL: Grounding.
Advertisements

David Prado Oct Antarctic Sea Ice: John N. Rayner and David A. Howarth 1979.
Characteristics, uses, and sources Introduction to DEMs.
The Global Digital Elevation Model (GTOPO30) of Great Basin Location: latitude 38  15’ to 42  N, longitude 118  30’ to 115  30’ W Grid size: 925 m.
SPATIAL DATA ANALYSIS Tony E. Smith University of Pennsylvania Point Pattern Analysis Spatial Regression Analysis Continuous Pattern Analysis.
The ICESat-2 Mission: Laser altimetry of ice, clouds and land elevation T. Markus, T. Neumann NASA Goddard Space Flight Center W. Abdalati Earth Science.
Reach-scale morphological changes of a braided river following a 15-year flood with multidate airborne LiDAR S. Lallias-Tacon (1,2), F. Liébault (1), H.
Digital Elevation Models GLY 560: GIS and Remote Sensing for Earth Scientists Class Home Page:
Assessment of Flow Paths in Upland Areas and Vegetated Buffers August 2, 2004 I.J. Kim, S.L. Hutchinson, and J.M.S. Hutchinson* The department of Biological.
OIB Long Range Planning Luthcke and Jezek. OIB Long Term Observation Goals OIB is meant to provide data to improve our understanding of the mass evolution.
WFM 6202: Remote Sensing and GIS in Water Management © Dr. Akm Saiful IslamDr. Akm Saiful Islam WFM 6202: Remote Sensing and GIS in Water Management Akm.
BIIR Cost Preview Preparatory Materials. BIIR Can Help Answer These Science Questions Refined science questions derived in part from the St. Petersburg.
More Raster and Surface Analysis in Spatial Analyst
Global Ice Sheet Mapping Orbiter Understand the polar ice sheets sufficiently to predict their response to global climate change and their contribution.
Ventures Proposal Science Objectives and Requirements.
ICESat dH/dt Thinning Thickening ICESat key findings.
Kostas Andreadis1, Dennis Lettenmaier1, and Doug Alsdorf2
GG313 Lecture 3 8/30/05 Identifying trends, error analysis Significant digits.
A Macroscale Glacier Model to Evaluate Climate Change Impacts in the Columbia River Basin Joseph Hamman, Bart Nijssen, Dennis P. Lettenmaier, Bibi Naz,
Principles of Sea Level Measurement Long-term tide gauge records  What is a tide station?  How is sea level measured relative to the land?  What types.
The Calibration Process
The Global Digital Elevation Model (GTOPO30) of Great Basin Location: latitude 38  15’ to 42  N, longitude 118  30’ to 115  30’ W Grid size: 925 m.
Comparison of LIDAR Derived Data to Traditional Photogrammetric Mapping David Veneziano Dr. Reginald Souleyrette Dr. Shauna Hallmark GIS-T 2002 August.
A Multi-Sensor, Multi-Parameter Approach to Studying Sea Ice: A Case-Study with EOS Data Walt Meier 2 March 2005IGOS Cryosphere Theme Workshop.
Fundamentals of GIS Lecture Materials by Austin Troy except where noted © 2008 Lecture 14: More Raster and Surface Analysis in Spatial Analyst Using.
Digital Terrain Models by M. Varshosaz
Sub-Glacial Topography and Ice Discharge of the Greenland Ice Sheet Ms. Amber E. Smith – REU Student Mr. Eunmok Lee – GRA Dr. Kees van der Veen – Advisor.
Remote Sensing and Active Tectonics Barry Parsons and Richard Walker Michaelmas Term 2011 Lecture 4.
Sea-ice freeboard heights in the Arctic Ocean from ICESat and airborne laser H. Skourup, R. Forsberg, S. M. Hvidegaard, and K. Keller, Department of Geodesy,
Statistical Techniques I EXST7005 Review. Objectives n Develop an understanding and appreciation of Statistical Inference - particularly Hypothesis testing.
1 Assessment of Geoid Models off Western Australia Using In-Situ Measurements X. Deng School of Engineering, The University of Newcastle, Australia R.
Satellite Cross comparisonMorisette 1 Satellite LAI Cross Comparison Jeff Morisette, Jeff Privette – MODLAND Validation Eric Vermote – MODIS Surface Reflectance.
Malcolm McMillan1, Peter Nienow1, Andrew Shepherd1 & Toby Benham2
Orthorectification using
Improvement of Digital Elevation Model of Greenland Ice Sheet by Using ICESat Satellite Laser Altimetry Data Bea Csatho, Taehun Yoon and Yushin Ahn Byrd.
The ALTA Spectrometer Introduction to Remote Sensing Adapted from Fundementals of Remote Sensing
Model Construction: interpolation techniques 1392.
Sea-Level Change Driven by Recent Cryospheric and Hydrological Mass Flux Mark Tamisiea Harvard-Smithsonian Center for Astrophysics James Davis Emma Hill.
Resolution (degree) and RMSE (cm) Resolution (degree) and RMSE (cm)
SWOT Near Nadir Ka-band SAR Interferometry: SWOT Airborne Experiment Xiaoqing Wu, JPL, California Institute of Technology, USA Scott Hensley, JPL, California.
The Semivariogram in Remote Sensing: An Introduction P. J. Curran, Remote Sensing of Environment 24: (1988). Presented by Dahl Winters Geog 577,
MODSCAG fractional snow covered area (fSCA )for central and southern Sierra Nevada Spatial distribution of snow water equivalent across the central and.
Understanding Glacier Characteristics in Rocky Mountains Using Remote Sensing Yang Qing.
RASTERTIN. What is LiDAR? LiDAR = Light Detection And Ranging Active form of remote sensing measuring distance to target surfaces using narrow beams of.
Using instrumented aircraft to bridge the observational gap between ICESat and ICESat-2.
Summary Part 1 Measured Value = True Value + Errors = True Value + Errors Errors = Random Errors + Systematic Errors How to minimize RE and SE: (a)RE –
University of Kansas S. Gogineni, P. Kanagaratnam, R. Parthasarathy, V. Ramasami & D. Braaten The University of Kansas Wideband Radars for Mapping of Near.
J. Lapazaran A. Martín-Español J. Otero F. Navarro International Symposium on Radioglaciology 9-13 September 2013, Lawrence, Kansas, USA On the errors.
Scaling Up Above Ground Live Biomass From Plot Data to Amazon Landscape Sassan S. Saatchi NASA/Jet Propulsion Laboratory California Institute of Technology.
Center for Satellite Applications and Research (STAR) Review 09 – 11 March Arctic Aircraft Altimeter (AAA) Experiment Envisat and ICESat underflights.
Lecture 6: Point Interpolation
Mapping Greenland Using NASA’s Full- Waveform, Medium/High-Altitude, LVIS Lidar System: Potential 2009 Coverage and Expected Performance Michelle Hofton.
How accurately we can infer isoprene emissions from HCHO column measurements made from space depends mainly on the retrieval errors and uncertainties in.
Research and Discover 2003 ICESat Precise Elevation Data Over the Antarctic Megadunes Tom Daigle: NASA/University of New Hampshire Research and Discover.
P B Hunukumbura1 S B Weerakoon1
Stochastic Hydrology Random Field Simulation Professor Ke-Sheng Cheng Department of Bioenvironmental Systems Engineering National Taiwan University.
Potential for estimation of river discharge through assimilation of wide swath satellite altimetry into a river hydrodynamics model Kostas Andreadis 1,
An Accuracy Assessment of a Digital Elevation Model Derived From an Airborne Profiling Laser Joseph M. Piwowar Philip J. Howarth Waterloo Laboratory for.
Integrated spatial data LIDAR Mapping for Coastal Monitoring Dr Alison Matthews Geomatics Manager Environment Agency Geomatics Group.
Integrating LiDAR Intensity and Elevation Data for Terrain Characterization in a Forested Area Cheng Wang and Nancy F. Glenn IEEE GEOSCIENCE AND REMOTE.
MECH 373 Instrumentation and Measurements
Greenland Ice Sheets CCI
PADMA ALEKHYA V V L, SURAJ REDDY R, RAJASHEKAR G & JHA C S
Definition In scientific literature there is no universal agreement about the usage of the terms: digital elevation model (DEM) digital terrain model (DTM)
The Calibration Process
Digital Elevation Models (DEM) Digital Terrain Models (DTM) / Digital Surface Models (DSM) Brief Review Applications in image processing: Inclusion in.
1Civil and Environmental Engineering, University of Washington
DEM products Elevation 0- ~10,000 (earth) 16 bit (signed)
An T Nguyen (MIT) Thomas A Herring (MIT)
Uncertainty “God does not play dice”
Presentation transcript:

High-Resolution Maps of Outlet Glacier Surface Elevation Change from Combined Laser Altimeter and Digital Elevation Model Data (ID # ) Joanna Fredenslund Levinsen 1,2 Ian M. Howat 2, Carl Christian Tscherning 1 1.University of Copenhagen, Niels Bohr Institute, Juliane Maries Vej 30, 2100 Copenhagen, Denmark 2.Ohio State University, School of Earth Sciences, Columbus, Ohio, USA F A C U L T Y O F S C I E N C E U N I V E R S I T Y O F C O P E N H A G E N Abstract: Maps of surface elevation change over rapidly changing outlet glaciers are essential for measuring ice mass balance, understanding glacier dynamics and predicting future changes. Due to the large expanse and inaccessibility of polar outlet glaciers, remote sensing methods for obtaining dz are required. Satellite and airborne laser altimetry provide high accuracy, but are limited spatially due to flight and orbit paths. Photogrammetrically derived Digital Elevation Models (DEM) provide a continuous surface with high spatial resolution, but errors in widely-available satellite-derived DEMs, such as from ASTER and SPOT, are 1-2 orders of magnitude greater than altimetry. Here, we present a statistically rigorous method for combining laser altimeter and DEM data to obtain annual maps of dz at a spatial resolution relevant to outlet glacier flow variability (~100 m). Presently, the method is still being developed, and the current data sets in focus are those from ICESat, ATM and SPOT by Jakobshavn Isbrae. Objective: To combine satellite altimetry data (ICESat GLA12, ATM and LVIS) with photogrammetrically derived DEMs (SPOT and ASTER). To determine the recent years’ surface elevation changes by the Greenland outlet glaciers Helheim, Kangerdlugssuaq and Jakobshavn Isbrae. Approach: This is done using three different approaches: 1.Register SPOT DEMs to laser altimetry data from ICESat and ATM (in focus) 2.Combine ICESat, ATM and ASTER data 3.Combine ICESat, ATM and LVIS data Current and future work Having implemented the ATM slope correction, included ICESat data and performed the registration and correction procedures, the method can now be applied to cover a larger area near the basins of the outlet glaciers. This allows for deriving surface maps and thus maps of surface elevation changes. Perform statistical analysis of results. Proceed to next approach with registering ASTER DEMs to ICESat and ATM and derive similar maps of surface elevation changes. Fig. 3: Original residuals between registered DEM and altimetry data, interpolated residuals estimated using OK and corresponding standard deviations. Fig. 1: Initial map of surface elevation changes by Jakobshavn Isbrae based on differenced SPOT DEMs from 08/ and 08/ Assumptions: Time of data acquisition  Small, relative elevation changes between altimeter data and SPOT image Altimeter elevations are means of horizontal, square cells with 100 m sides Downscaling and interpolation of DEM to altimeter points  DEM elevations representative of altimeter points The DEM errors are larger than those from altimeter data corrected for positioning and ranging DEM errors stem from cloud cover, planimetric and elevation-dependent biases and normally distributed, random errors Fig. 2: Initial map of surface elevation changes by Jakobshavn Isbrae based on differenced ATM data from 05/ and 07/ Fig. 5: Surface elevations produced from registering the SPOT DEM to ICESat and ATM data. Method: For every available SPOT image: Gather ICESat GLA12 and ATM data from laser campaigns closest in time to when SPOT image was acquired. See Fig. 1 and 2 for initial elevation changes derived from ATM data from May 2007 and July 2008 and SPOT DEMs from August 2007 and Too few ICESat data from test area to make similar plots. Perform slope correction on ATM data using ICESS blocks. Assume that altimeter measurements are means of horizontal, square cells with 100 m sides. Downscale DEM to 100 m and reference it to altimeter positions: Apply filters as well as planimetric and elevation-dependent corrections iteratively. The initial horizontal and vertical offsets are usually of the order of 10s of m and the final ones of the order of a few cm, mm or less. Fig. 3 shows available ATM and ICESat data tracks and Fig. 4 the original SPOT surface elevations to be registered to the altimetry data. Consider residuals (dz) between interpolated DEM and altimeter. Use ordinary kriging (OK) on dz values to estimate residuals and uncertainties between altimeter points. Perform the kriging in a grid defined by the DEM end points. Fig. 3. Calculate final DEM in kriging points. This yields a continuous map of surface elevations based on the combination of a DEM and laser altimetry data, Fig The surface elevation changes can then be estimated by deriving the relative elevation changes between the DEMs found from the available SPOT images. Fig. 4: Original surface elevations from SPOT DEM obtained on 08/