This document discusses using radar altimetry data from multiple satellite missions spanning 1992-2012 to analyze changes in Antarctic ice shelves. It presents three key challenges: integrating data from different radar altimetry systems; accounting for time-varying surface properties; and applying spatial and temporal corrections. The goal is to capture ice shelf variability at spatial scales of 20-30 km over 20+ years. Results show high spatial and temporal elevation change variability, with coherent changes tracked around the Antarctic coast. Validation with ICESat data is also discussed.
A slightly updated version of the talk I gave at the Lunar and Planetary Sciences Conference 2012. This talk was presented to a more general audience (the Earth and Planetary Sciences Department of University of California Santa Cruz).
Avo ppt (Amplitude Variation with Offset)Haseeb Ahmed
AVO/AVA can physically explain presence of hydrocarbon in the reservoirs and the thickness, porosity, density, velocity, lithology and fluid content of the reservoir of the rock can be estimated.
Estimation of Dipping Angles of Refracting Interfacesiosrjce
IOSR Journal of Environmental Science, Toxicology and Food Technology (IOSR-JESTFT) multidisciplinary peer-reviewed Journal with reputable academics and experts as board member. IOSR-JESTFT is designed for the prompt publication of peer-reviewed articles in all areas of subject. The journal articles will be accessed freely online.
A slightly updated version of the talk I gave at the Lunar and Planetary Sciences Conference 2012. This talk was presented to a more general audience (the Earth and Planetary Sciences Department of University of California Santa Cruz).
Avo ppt (Amplitude Variation with Offset)Haseeb Ahmed
AVO/AVA can physically explain presence of hydrocarbon in the reservoirs and the thickness, porosity, density, velocity, lithology and fluid content of the reservoir of the rock can be estimated.
Estimation of Dipping Angles of Refracting Interfacesiosrjce
IOSR Journal of Environmental Science, Toxicology and Food Technology (IOSR-JESTFT) multidisciplinary peer-reviewed Journal with reputable academics and experts as board member. IOSR-JESTFT is designed for the prompt publication of peer-reviewed articles in all areas of subject. The journal articles will be accessed freely online.
Seismic data Interpretation On Dhodak field PakistanJamal Ahmad
I (Jamal Ahmad) presented this on 21 Feb, 2009 to defend my M.Phil dissertation in Geophysics at QAU, Islamabad, Pakistan. For more information about this, you may contact me directly at jamal.qau@gmail.com.
Interannual and decadal variations of Antarctic ice shelves using multi-mission satellite radar altimetry, and links with oceanic and atmospheric forcings
On 17/10/2013 TU Delft Climate Institute organised the symposium The Greenland and Antarctic ice sheets: present, future, and unknowns. This is one of the four presentations given there.
http://www.tudelft.nl/nl/actueel/agenda/event/detail/symposium-tu-delft-climate-institute-17th-october-2013/
Seismic data Interpretation On Dhodak field PakistanJamal Ahmad
I (Jamal Ahmad) presented this on 21 Feb, 2009 to defend my M.Phil dissertation in Geophysics at QAU, Islamabad, Pakistan. For more information about this, you may contact me directly at jamal.qau@gmail.com.
Interannual and decadal variations of Antarctic ice shelves using multi-mission satellite radar altimetry, and links with oceanic and atmospheric forcings
On 17/10/2013 TU Delft Climate Institute organised the symposium The Greenland and Antarctic ice sheets: present, future, and unknowns. This is one of the four presentations given there.
http://www.tudelft.nl/nl/actueel/agenda/event/detail/symposium-tu-delft-climate-institute-17th-october-2013/
CSP Training series : solar resource assessment 2/2Leonardo ENERGY
Fifth session of the 2nd Concentrated Solar Power Training dedicated to solar resource assessment.
* DNI Variability, Frequency Distributions
* Typical Meteorological Years
* DNI measurements: broadband vs. spectral, and their limitations
* What is circumsolar radiation and why should we care in CSP/CPV?
* How much diffuse irradiance can be used in concentrators?
* How to measure and model the circumsolar irradiance?
* Spectral irradiance standards and their use for PV/CPV rating
* The AM1.5 direct standard spectrum: Why did it change? Why AM1.5?
* Use of the SMARTS radiative code to evaluate clear-sky spectral irradiances
* Sources of measured spectral irradiance data
* Spectral effects on silicon and multijunction cells and their dependence on climate
In the first part of the talk, we will present a sensitivity analysis of a novel sea ice model. neXtSIM is a continuous Lagrangian numerical model that uses an elastobrittle rheology to simulate the ice response to external forces. The response of the model is evaluated in terms of simulated ice drift distances from its initial position and from the mean position of the ensemble. The simulated ice drift is decomposed into advective and diffusive parts that are characterized separately both spatially and temporally and compared to what is obtained with a free-drift model, i.e. when the ice rheology does not play any role. Overall the large-scale response of neXtSIM is correlated to the ice thickness and the wind velocity fields while the free-drift model response is mostly correlated to the wind velocity pattern only. The seasonal variability of the model sensitivity shows the role of the ice compactness and rheology at both local and Arctic scales. Indeed, the ice drift simulated by neXtSIM in summer is close to the free-drift model, while the more compact and solid ice pack is showing a significantly different mechanical and drift behavior in winter. In contrast of the free-drift model, neXtSIM reproduces the sea ice Lagrangian diffusion regimes as found from observed trajectories. The forecast capability of neXtSIM is also evaluated using a large set of real buoy’s trajectories. We found that neXtSIM performs better in simulating sea ice drift, both in terms of forecast error and as a tool to assist search-and-rescue operations. Adaptive meshes, as the one used in neXtSIM, are used to model a wide variety of physical phenomena. Some of these models, in particular those of sea ice movement, use a remeshing process to remove and insert mesh points at various points in their evolution. This represents a challenge in developing compatible data assimilation schemes, as the dimension of the state space we wish to estimate can change over time when these remeshings occur.
In the second part of the talk, we highlight the challenges that such a modeling framework represents for data assimilation setup. We then describe a remeshing scheme for an adaptive mesh in one dimension. The development of advanced data assimilation methods that are appropriate for such a moving and remeshed grid is presented. Finally we discuss the extension of these techniques to two-dimensional models, like neXtSIM.
First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...Sérgio Sacani
The Earth’s hum is the permanent free oscillations of the Earth recorded in the absence ofearthquakes, at periods above 30 s. We present the first observations of its fundamental spheroidaleigenmodes on broadband ocean bottom seismometers (OBSs) in the Indian Ocean. At the ocean bottom,the effects of ocean infragravity waves (compliance) and seafloor currents (tilt) overshadow the hum. In ourexperiment, data are also affected by electronic glitches. We remove these signals from the seismic traceby subtracting average glitch signals; performing a linear regression; and using frequency-dependentresponse functions between pressure, horizontal, and vertical seismic components. This reduces the longperiod noise on the OBS to the level of a good land station. Finally, by windowing the autocorrelation toinclude only the direct arrival, the first and second orbits around the Earth, and by calculating its Fouriertransform, we clearly observe the eigenmodes at the ocean bottom.
Airborne and underground matter-wave interferometers: geodesy, navigation and...Philippe Bouyer
The remarkable success of atom coherent manipulation techniques has motivated competitive research and development in precision metrology. Matter-wave inertial sensors – accelerometers, gyrometers, gravimeters – based on these techniques are all at the forefront of their respective measurement classes. Atom inertial sensors provide nowadays about the best accelerometers and gravimeters and allow, for instance, to make the most precise monitoring of gravity or to device precise tests of the weak equivalence principle (WEP). I present here some recent advances in these fields
Interannual and decadal variability of Antarctic ice shelf elevations from multi-mission satellite radar altimetry
1.
2. Large scale studies on ice shelves
ERS-1/2 1992-2001 ERS-2/Envisat 1994-2008 ICESat 2003-2008
Zwally et al., 2005 Shepherd et al., 2010 Pritchard et al., 2012
Duration 9 years 14 years 5 years
Spat. Res. 100 km One value per ice shelf 30 km
Time Res. 3 months 35 days (!) 1-2 years
This study: ERS-1/ERS-2/Envisat 1992-2012 2
*
3. The need for multi-mission RA
Long vs short records in detecting climate trends
How long?
Decadal records
(20+ years)
Interannual and
decadal variability
unexplored
Fricker and Padman, 2012
Our goal → to capture the variability in space and time on the
ice shelf spatial scales: 20+ years / 20-30 km 3
*
4. Penetration depth (backscatter)
Penetration depth:
! Water ! "(mm)
! Wet snow ! O(cm)
! Dry snow ! O(m)
! And varies with time
A
Radar
penetrates
into firn layer
B
4
*
5. Constructing time series of dh
Similar (but not the same) method as
Davis & Segura (2001), Zwally et al. (2005), Khvorostovsky (2011).
5
*
6. Averaging in time and space
1 vs 3-month averages
less crossovers
per bin → larger
error bars
improved signal-to-
noise ratio and no
gaps
20-30 km bins
6
*
7. Crossing all possible time combinations
Now we have one time series per reference time: t1, t2, t3, ...
These are elevation changes with respect to different epochs
7
*
8. One grid per time combination
Crossovers t1
~ 1500 grids
t2
t3
8
*
9. Multi-referenced time series
At every individual grid-cell we have now several time series
outliers
1) To align we use average of the offset for overlap period only
2) Then we frequency-weighted average the aligned time series 9
*
10. Cross-calibration of average TS
Cross-calibration is done using overlap periods between missions
dh = elevation change dAGC = backscatter power change
ERS-1 ERS-2 Envisat
10
*
11. Backscatter correction (approach 1)
By correlating absolute values ! dAGC x dh
11
Wingham et al., 1998; Davis & Ferguson, 2004; Zwally et al., 2005
27. Conclusions
!
Multi-mission RA can be used to construct continuous
long records with their variability content
!
There is a lot of variability both in time and space
!
Variability is the key to understand forcings and climate-
induced changes (ocean and atmospheric circulation)
!
Relative error (precision) vs absolute error (penetration)
!
Different b/s approaches yield different results?
!
How can we validate b/s correction when there are so little
ground truthing data and in practice:
27
28. We thanks
!
NASA NESSF Fellowship
!
Jay Zwally & Jairo Santana (NASA/GSFC)
!
Curt Davis (UM) & Duncan Wingham (UCL)
!
NASA grants NNX06AD40G and NNX10AG19G
!
ESA for ERS-1, ERS-2 and Envisat altimeters!
!
San Diego Super Computer Center
!
Geir Moholdt
!
Python and Open Source
fpaolo@ucsd.edu
28
29. Antarctic ice shelf mask
A reliable and complete ice shelf mask is a problem
So we (Geir Moholdt) created our own using all data available: MOA (Scambos
et al. 2007), ASAID (Bindschadler et al. 2011), InSAR (Rignot et al. 2011),
ICESat (Fricker/Brunt et al. 2006-10)
29
*
31. Challenges of multi-mission integration
!
Differences between missions:
- RA systems, orbit configurations, time spans...
!
Radar interaction with time variable surface properties
!
Spatial and temporal dependent corrections:
- Ocean tides (for high lat)
- Atm pressure (IBE)
- Surface density (firn densification)
- Penetration depth (backscatter)
31
32. How to reduce the noise?
!
Due to hydrostatic equilibrium the altimeter only see 10%
of the grounded ice signal (in elevation change)
!
So to increase signal-to-noise ratio → requires lots of
averaging both in time and space
32
*
33. The uncertainty
!
How well do we know the error?
!
What do error bars in the time series actually represent?
After all the averaging a mean error is: ± 5-20 cm over 20-30 km
!
What about the uncertainty in penetration depth?
O(m/cm)
33