Title: Electromagnetic Scattering Model Performance Assessment of the Global Ice Sheet Mapping Orbiter Conc
1Electromagnetic Scattering Model Performance
Assessment of the Global Ice Sheet Mapping
Orbiter Concept
- N. Niamsuwan(1), J. T. Johnson(1), S. P. Gogineni
(2) and K. C. Jezek(3)
(1) Dept. of Electrical and Computer Engineering
Ohio State University, USA
(2) Dept. of Electrical Eng. and Computer Sci.
University of Kansas, USA
(3) Dept. of Geological Sciences
Ohio State University, USA
AGU Fall meeting 2006, San Francisco, CA Dec
12th, 2006
2Motivation
Global Ice Sheet Mapping Orbiter (GISMO)
First airborne SAR images of the base of the
Greenland ice sheet May 2006
Right Wing
- 150 MHz air-borne radar, one array antenna on
each wing. - From an individual wing, SAR images can be
produced. 2-D information basal reflectance
maps. - Both signals altogether are used to generate
interferogram, providing 3-D information digital
elevation models.
Left Wing
Basal Return At Nadir
Surface
1.5 km image swath
SAR Interferogram of the base
surface
layers
base
noise
3Outline
Outline
Goal Preliminary formulation and evaluation of
scattering model for interpreting GISMO images
- Electromagnetic models for glaciers
- Physical Optics approximation
- Example simulations for nadiral observation
- Summary
4Electromagnetic models
EM Models
surface
- Neglecting volume scattering, problem reduces to
scattering from multi-layer rough surfaces
(incl. ice, water and rock layers)
Near Nadir Radar
base
- Interested in modeling both deterministic and
stochastic surfaces
- 1-D surface profiles are considered here to
simplify the analysis methods also applicable to
2-D but requires more computation
500 m 5 km
- Although GISMO operates at somewhat low
frequencies, surface height variations of
interest are on scales much larger than the EM
wavelength. - Near normal incidence geometry motivates
examination of Physical Optics (PO) approximation
plus extension to Geometrical Optics (GO) limit.
unknown depth
5Physical Optics Approximation
1-D surface
One interface problem
Fields on surface estimated using a local tangent
plane approximation
Multi-layer problems Neglecting multiple
interaction, we can cascade scattering effects
from each layer.
Using a plane wave spectrum approach,
deterministic PO theory involves a set of
transition matrices coupling incident and
scattered plane waves
6Example simulation
nadir observation
Surface Profile
Freq-response Time-response
- Permittivity of ice/pure water/rock labeled above
(Debye formula/Malmberge and Maryott Model) - Large scale surface domain split into 100m
sections for analysis. - For each 100m-surface, scattered fields versus
frequency computed from 140-160 MHz. - Fourier transform provides scattered field
amplitude envelope versus time (0-sec delay
0-meter height)
7Results
Time-response along the profile
Exact Solution - MoM
Approximate Solution - PO
- Bottom plots outline the rock (red) and water
(blue) surfaces. - PO solution is consistent with MoM note
potential for observing weak scattering from
basal rock even below pure water region - Time resolution is limited by the bandwidth
(20MHz) of the system.
8Results (cont.)
Thin layer of water
Surface profile thin water
Time response MoM
S 0 ppt
- As water layer becomes thinner, multiple
interactions between interfaces can be observed
(not captured in current PO model) - However, for water with a slight salinity (2
ppt), returns below water surface as well as
multiple interactions vanish due to larger
attenuation - Detailed salinity properties of sub-glacier water
an important issue
S 2 ppt
9Results (cont.)
Local roughness
Surface Profile with local roughness
Time response
- local-scale power-law (k-3 spectrum) roughness
(rms height 1m) has been added to the base-rock
profile. - Time response due to 6 distinct surface
realizations are shown on the right. - Presence of local roughness affects both signal
strength and range estimation.
- Dielectric contrast and roughness effects are
dominant factor producing scattered field
returns.
10Summary
Summary
- PO solution for (1-D) deterministic multi-layer
surface implemented matches MoM well for assumed
base surface properties - Simulations show possibility of imaging sub-water
layer rock if water layeris pure and relatively
thin possibility of multiple reflections also
shown. - Sub-water effects eliminated if water is even
slightly saline - As expected, dielectric contrast (i.e. presence
of water) and local large/small scale roughness
determine scattering amplitudes observed - Next steps
- - Ensemble averaging for stochastic surfaces
- - Formulation for 2-D surfaces
- - Apply to GISMO image interpretation.