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Remote Sensing:

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Active microwave systems (1) Satellite Altimetry Remote Sensing: John Wilkin jwilkin_at_rutgers.edu IMCS Building Room 214C 732-932-6555 ext 251 609-933-7753 – PowerPoint PPT presentation

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Title: Remote Sensing:


1
Active microwave systems(1) Satellite Altimetry
Remote Sensing
John Wilkin
jwilkin_at_rutgers.eduIMCS Building Room
214C732-932-6555 ext 251609-933-7753
2
Active microwave instruments
  • Scatterometer (scattering from surface roughness)
  • ocean vector winds
  • Synthetic Aperture Radar (SAR)
  • sea ice
  • high resolution wind speed over water
  • land mapping surface roughness and 3-D terrain
  • CODAR
  • coastal ocean surface vector currents
  • Altimeter

3
Active microwave instruments
  • Altimeters (nadir pointing radar)
  • sea surface height (long wavelengths 50 km)
  • mesoscale currents, eddies, fronts
  • thermal expansion
  • significant wave height
  • wind speed
  • gravity and bathymetry
  • ice sheets

http//www.aviso.oceanobs.com
http//topex-www.jpl.nasa.gov
http//earth.esa.int/brat/html/general/overview_en
.html
4
Microwave energy is largely unaffected by the
atmosphere It has almost 100 transmission
5
Radar systems operate in the microwave region of
the EM spectrum
Ku-band 13.6 GHz C-band 5.3
GHz Poseidon dual-frequency altimeteron Topex,
Jason-1 and Jason-2
http//topex-www.jpl.nasa.gov/technology/instrumen
t-altimeter.html
6
Key Components of any Radar System Microwave
transmitter electronic device used to generate
the microwave EM energy transmitted by the
radar Microwave receiver electronic device
used to detect the microwave pulse that is
reflected by the area being imaged by the
radar Antenna electronic component through
which microwave pulses are transmitted or
received (usually shared on satellite systems)
7
  • The relationship betweenpower received P and
    power transmitted PT is given by the radar
    equation
  • (1)
    (2) (3)
  • Power of EM wave at range R. G gain of
    antenna
  • Radiant intensity in the direction of the radar
    produced by scatter from a surface with a
    scattering cross-section s (which depends on area
    of target, fraction of incident radar pulse
    absorbed and scattered)
  • Ae is antenna effective area1/(4pR2) is
    isotropic spreading over range R in both
    transmittedand received signal

8
  • Satellite Altimeters
  • altimeters are nadir-pointing satellite-based
    radars used to measure the height of the surface
    of the Earth
  • transmit a radar pulse that is reflected from
    the Earths surface
  • measure the time it takes for the pulse to
    travel to Earth and back, t
  • range from satellite to surface is R ½ ct
    where c speed of light
  • Precision Orbit Determination (POD) systems
    measure the altitude of the satellite above a
    reference ellipsoid
  • c 3 x 108 m/s
  • satellite altitude 1200 km
  • t 2R/c 0.008 s 8 milliseconds
  • Poseidon uses 1700 pulses per second

9
ERS-1 1991-2000
History of Altimetry
Envisat 2002 -
ERS-2 1995 -
Jason-1 2001 -
OSTM/Jason-2 2008 -
10
Altimetry How it works
Reference ellipsoid Satellite position is
determined relative to an arbitrary reference
surface - an ellipsoid. This reference ellipsoid
is a raw approximation of Earth's surface, a
sphere flattened at the poles. The altitude of
Jason above the reference ellipsoid is measured
to within 3 cm.
11
Sea surface HEIGHT (SSH)
  • Sea Surface Height is satellite altitude minus
    range
  • It comprises two contributions geoid and
    dynamic topography
  • Geoid
  • The sea surface height that would exist without
    any motion. This surface is not flat because of
    gravity variations around the planet due to mass
    and density differences associated with the
    seafloor. The geoid is a geopotential surface.
  • Major bathymetric features deform sea level by
    tens of meters and are visible as hills and
    valleys of the geoid
  • Dynamic topography
  • The ocean circulation comprises a permanent mean
    component linked to Earth's rotation, mean winds,
    and density patterns
  • and a highly variable component (wind
    variability, tides, seasonal heating, mesoscale
    eddies)

12
Sea surface HEIGHT (SSH)
  • Sea Surface Height is ssh altitude
    minus range
  • Geoid and dynamic topography
  • To derive the dynamic topography, D, the easiest
    way would be to subtract the geoid HEIGHT from
    SSH
  • In practice, the geoid is not yet known
    accurately enough for many applications and mean
    sea level is commonly subtracted instead. This
    yields the variable part of the ocean signal (but
    removes the mean ocean circulation)

13
Geoid height (meters)
80
-80
14
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15
The slope of the sea surface relative to the
geoid is directly related to the geostrophic
current that balances the pressure gradient (due
to the sea surface gradient) and the Coriolis
force The long-term mean ocean circulation has
an associated mean dynamic topography that is a
permanent component of the time-mean orbit range
as a function of position.
16
Jason-1 satellite AVISO Web site http//www.aviso.
oceanobs.com/en/missions/current-missions/index.ht
ml
17
Jason launch movies
18
Satellite orbit and tracking
  • The critical orbital parameters for satellite
    altimeter missions are altitude, inclination and
    period
  • Topex/Poseidon and Jason satellites (same orbit)
  • altitude 1336 km
  • relatively high less drag and more stable orbit
  • inclination of 66 to Earth's polar axis
  • it can "see" only up to 66 North and South
  • the satellite repeats the same ground track every
    9.9156 days
  • the ground-tracks are 315 km apart at the equator
  • track repeat precision is about 1km
  • ground scanning velocity is 5.8 km/s, orbit
    velocity 7.2 km/s

19
Where is Jason now?
Where is Topex now?
20
Jason-1 ResearchGround segment
21
OSTM/Jason-2 OperationalGround segment
Tracking
Operational real-time products ground station
redundancy archive
Delayed-mode reanalysis for research quality
datasets
22
Geostrophic current computed from altimeter sea
surface height gives only the component
perpendicular to the ground-track. To get
surface geostrophic current vectors we need to
map the SSH field in two dimensions. The high
alongtrack resolution (20km) is then lost because
of the large separation of the ground-tracks (315
km at Equator)
Where is Jason now?
23
(a) (b)
(c)
Grid of sea surface height measurements by T/P,
ERS-2 and GFO in the Northeast Atlantic over (a)
10 days, (b) 7 days, and (c) and 3 days. There
are gaps in coverage of 200 km and more over 3
days. Combining data from all three missions
increases coverage. gt Multiple satellites are
required to resolve mesoscale current patterns
24
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25
Tropical Cyclonic Heat Potential computed from
altimetry on 28 August 2005, with Hurricane
Katrina's trajectory and intensity overlaid.
Katrina's intensification seems to coincide with
its crossing over the Loop Current.
Altimetry data in combination with historical
hydrographic observations are currently used to
estimate synthetic upper ocean temperature
profiles. These profiles are then used to compute
the integrated vertical temperature from the sea
surface down to the 26C isotherm, the
temperature needed to sustain a tropical cyclone.
This quantity is usually referred to as the
Hurricane or Tropical Cyclone Heat Potential
(TCHP) Leipper and Volgenau, 1972 and
represents the amount of heat in the upper ocean
available for tropical cyclone intensification.
Leipper, D. and D. Volgenau. Hurricane heat
potential of the Gulf of Mexico, J. Phys.
Oceanogr., 2, 218-224, 1972.
26
Altimetry How it works
For altimeter observations to be useful for
oceanography, range accuracy of order 2 cm is
required.
Where is Jason now?
27
  • The challenges to achieving 2 cm accuracy are
  • making range corrections for the atmosphere
  • density of atmosphere, water vapor
  • accounting for the aliasing of tides
  • knowing the shape of a reference gravitational
    potential surface, or geoid, that defines a
    surface along which gravity is constant(and
    therefore dynamically level)
  • computing the satellite position accurately

28
Precision Orbit Determination
  • The Jason-2 satellite is tracked in 3 ways
  • GPS Payload (GPSP)
  • continuously tracks up to 16 GPS satellites
  • dual-frequency receiver
  • estimates position to better than 50 m and time
    to 50 nanoseconds
  • Laser Retroflector Array (LRA)
  • an array of mirrors on the satellite that provide
    a target for laser-tracking measurements from
    ground stations
  • round-trip time of the laser is another range
    measurement
  • accuracy is a few mm, but only 10 to 15 stations
    are in operation
  • DORIS
  • receivers on the satellite measure Doppler shift
    of signal from ground-station beacons (at 2
    frequencies)
  • gives satellite velocity
  • a dynamic orbit model integrates the velocity and
    position data, drag, solar forces on satellite,
    to continuously compute the satellite trajectory

Where is Jason-1 now?
Where is Jason-2 now?
29
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30
Doris beacons transmit signals at two separate
frequencies (2036.25 MHz and 401.25 MHz) to the
satellite. The receiver onboard the satellite
analyzes the received signal frequencies to
calculate its velocity relative to Earth.
This velocity
is fed into orbit determination models to
derive the
satellite's position on orbit to within 2 cm on
the radial
component.
Doris receiving antenna under the satellite. It
receives signals from the terrestrial beacons
network (its length is 42 cm).
31
The LRA is a totally passive reflector designed
to reflect laser pulses back to their point of
origin on Earth. It is used for the calibration
of the Precise Orbit Determination system on the
spacecraft.                                       
    LRA is an array of mirrors that provide
a target for laser tracking measurements from the
ground. By analyzing the round-trip time of the
laser beam, we can locate very precisely where
the satellite is on its orbit. The LRA is used to
calibrate the other location systems on the
satellite (Doris, GPSP) with a very high degree
of precision.
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