sea surface

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Sea Surface • SST • Chlorophyll and water colour (reflectance and in water absorption) • Salinity • Sea Ice • Waves (surface roughness) • Foam, Oil spill and water quality Robinson, I.S., 2004, Measuring the Oceans from Space The principles and methods of satellite Oceanography. Jointly published by Springer and Praxis Publishing, UK 2004, XLV, 669 p. ISBN: 978-3-540-42647-9

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Sea Surface. SST Chlorophyll and water colour (reflectance and in water absorption) Salinity Sea Ice Waves (surface roughness) Foam, Oil spill and water quality. - PowerPoint PPT Presentation

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Page 1: Sea Surface

Sea Surface

• SST

• Chlorophyll and water colour (reflectance and in water absorption)

• Salinity

• Sea Ice

• Waves (surface roughness)

• Foam, Oil spill and water quality

Robinson, I.S., 2004, Measuring the Oceans from Space The principles and methods of satellite Oceanography. Jointly published by Springer and Praxis Publishing, UK 2004, XLV, 669 p. ISBN: 978-3-540-42647-9

Page 2: Sea Surface

Sea Surface TemperatureMOIST

DRY

T

10-T

12 [

K]

T10 T12

SST= a*T10+b*(T10-T12)+c

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Page 4: Sea Surface

Cos’e la temperatura superficiale ?

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Comments on applications for air-sea interaction

• SST is needed for estimation of LWup component of the radiation budget, as well as to estimate the saturation humidity for latent heat flux, in the estimation of sensible heat flux and of the evaporation.

• Study of evolution of SST fields may be of interest in process description.

Page 9: Sea Surface

Data characteristics• Spatial resolution ranges from medium (1-10 km

from every 12hours to 15’ e large (10-100 km) (interferometers, MW radiometers)

• Archived data >25 years (e.g. Pathfinder)• Current best (potential) Temporal resolution: 15’

for about 5x5km data.• MW based products are available at relatively

low resolutions (>10 km) and only over open oceans.

• Accuracy 0.5 K (IR & cloud free)

Page 10: Sea Surface

Weaknesses• Skin vs bulk temperature

• Lack of large datasets for diurnal cycle studies

• Problems with coasts, undetected clouds (for IR based) and aerosol contamination.

• Assumptions on the air temperature vertical structure.

• Clouds (IR based)

Page 11: Sea Surface

Chlorophyl/Water Colour/Sediments

Page 12: Sea Surface

Ocean ColourSatellite measurement of ocean colour consists in dedicated* spectral measurements of visible radiation with channels that corresponds to the actualcolours.

*the instrument must be optimized in the range of low values of reflectivity (SPOT, Landsat are not optimized)

Source: http://cimss.ssec.wisc.edu/satmet/home/poes_florida.html

Page 13: Sea Surface

Ocean color depends from• Pure seawater optical characteristics• Phytoplankton• DOM (Dissolved Organic Material) or Yellow

substance or gelbstoff• Suspended particular matter• Seafloor color (shallow waters)• Foam• Oil spills• Sunglint

Page 14: Sea Surface

Applications of ocean colour derived parameters

• Diffuse attenuation coefficient (Kλ):physical modeling -> thermal structure

biological modeling -> available underwater solar radiation

characterization of ocean waters

• Phytoplankton biomassbiological modeling -> primary production (CO2 fluxes)

• Water quality parameters

• Seabed characterization

• Tracer for dynamic processes

Page 15: Sea Surface

Data characteristics• Spatial resolution is about 1 km. • Temporal sampling: For a single low orbit

satellite in principle it is possible to have a measurement each 24 hours. Gaps in the swaths, clouds, aerosols and sunglint reduce the effective temporal sampling.

• Archived data about 10 years (e.g. SeaWifs) from the same platform. Archived observations are available since 1978 (CZCS) but there have been no missions for about 10 years (1986-96)

Page 16: Sea Surface

Weaknesses• Clouds and aerosols and in general atmospheric

contribution.• Problems (seabed, land contamination, sediments

etc..) in coastal areas for phytoplankton estimation• Need for regional algorithms• Assumptions on the effective vertical structure of

phytoplankton for CO2 fluxes estimation.

Page 17: Sea Surface

Relationship between in situ chlorophyll concentration and the Remote Sensing Reflectances band ratios. Red crosses are the data used in the algorithms development. Blue crosses are the new data collected in the Mediterranean. Lines indicate the remote sensing algorithms (OC2-V4 dotted line, NL-DORMA solid line)

Stima della clorofilla tramite ‘ocean colour’ Rapporto BLU/VERDE

Page 18: Sea Surface

Ls=Lp+Lr+Lw Lp=F(aerosols,p)Lr=F(observation geometry, wind (foam, roughness, glint))

Aerosols=F(Ls670,Ls870)

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21235108

255235108

20515352

015352

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Sea Surface Salinity

Page 25: Sea Surface

• Key oceanographic (density) and climatic parameter• Thermohaline circulation / heat fluxes• Variations due to E-P budget, freezing/melting, freshwater run-off• 24% NEVER sampled and 40% less than 5 samples• Oceanographic models already assimilate SST and SSH from satellite data, while SSS is still climatologic

Why should we measure SSS?

Prospective benefits:• Thermohaline circulation monitoring• Ocean precipitation rate estimates• Barrier layer effect• Annual/inter-annual variability (ENSO)

Conveyor Belt

SSS time-series

Page 26: Sea Surface
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Configuration Parameters (f, p, θ, φ)

Scene Parameters (SSS,SST, sea state)

1.4 GHz, L-band (dedicated)

• Optimum SSS sensitivity

• Reasonable pixel dimension

• Atmosphere almost transparent

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Correction terms to be applied in TB computation

Cosmic and galactic radiation

Faraday effect

Atmospheric contributions and losses

Observed scene

Motivation/OverviewWhat will we measure?

Page 32: Sea Surface

Uncertainty in SMOS salinity measurement

Instrumental errors• Radiometric sensitivity, accuracy, calibration stability• Uncomplete characterisation of the system elements• Interferometric image reconstruction

Geophysical effects to be accounted for• Ionosphere (Faraday rotation)• Atmosphere (dry air absorption, water vapour, clouds,

rain)• External radiation (galactic background, sun, moon

reflexions)• Sea surface temperature• Surface roughness (wind waves, swell, foam)

Radio frequency interference

Page 33: Sea Surface

Chen, H.S., 1985. Space Remote Sensing Systems: An introduction. Academic Press. 258 pp.

Page 34: Sea Surface

SMOS

• Sun-synchronous orbit • h=755 Km (LEO) • 3 days revisit time• Launch: October 31st, 2008• 69 elements array, 120º spaced• d= 0.875 λ (Nyquist criterion unaccomplished)

• Dual-pol / Full-pol• Multi-angular capabilities

• Free-alias FOV about 1000 Km: no phase difference ambiguity

• Spatial Reisolution: 35 Km (boresight)

Page 35: Sea Surface

-5 0 5 10

-8

-6

-4

-2

0

2

4

6

8

x/

y/

-10 0 10

-15

-10

-5

0

5

10

15

u

v

u

v

Complex cross-correlations between each antenna pair signals generate Visibility points

( , ) ( , )V u v T F

Motivation/OverviewHow should we measure SSS?

MIRAS (Microwave Imaging Radiometer by Aperture Synthesis)

Page 36: Sea Surface

• Levenberg-Marquardt method

• Multi-parameter (SSS, SST, U10) retrieval

• Fixed upper and lower boundaries

• Semi-empirical TB forward model

• A priori knowledge of the auxiliary data errors

•Mean sea level slope rather than wind

2

21010

2

2

2

2

12

2

2

10

)(1

U

aux

SST

aux

SSS

auxN

n F

modeln

measn

obs

UUSSTSSTSSSSSSFF

N

obs

n

yx TTF , yxvh TTTTIF

SSS Retrieval Cost function

Page 37: Sea Surface

Salinity• Salinity can be retrieved with passive MW radiometry based

on the fact that a change in salinity would introduce a change in the dielectric properties (emissivity) of sea water in the MW.

• Retrieval of salinity requires the knowledge of SST, as well as the knowledge of atmospheric properties and other sea surface factors that are reponsible for the value of emissivity (e.g. wind)

• Although attempt to retrieve salinity has been done with 6.6 Ghz (SMMR) lower frequencies (1-2 GHz) are needed

• 2 satellites should be launched shortly for such mission (SMOS (ESA) and Aquarius (NASA+ Argentina's Comisión Nacional de Actividades Espaciales)

• Spatial resolution will be quite coarse > 10 km and problem close to the coast

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• Starting in 2009, Aquarius mission will measure global SSS with unprecedented resolution. The science instruments will include a set of three radiometers that are sensitive to salinity (1.413 GHz; L-band) and a scatterometer that corrects for the ocean's surface roughness. The spacecraft will be contributed by Argentina's Comisión Nacional de Actividades Espaciales (CONAE).

Page 39: Sea Surface
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Ice

• Sea ice can be retrieved MW radiometry based on the fact that being of fresh water it will have different dielectric properties (emissivity) compared to sea water

• Spatial resolution will be quite coarse > 10 km and problem close to the coast

• Active MW sensing

Page 41: Sea Surface

Sea ICE

Page 42: Sea Surface

Oil spillDue to the nature of an oil slick a satellite remote sensing platform is

required to have the following:

• High temporal resolution, due to the changing nature of the oil and its immediate threat to ecosystem,

• The ability to image a given area regardless of cloud cover and prevailing weather conditions (even time of day),

• High spatial resolution, to identify individual small oil patches (windrows),

• Wide spectral resolution, as the position and width of the spectral band is important in distinguishing the oil from the adjacent water (Clark, 1993).

• http://cearac.poi.dvo.ru/en/background/techniques/

Page 43: Sea Surface

OIL SPILL: VIS

Crude and heavy refined oils have 3 optical properties which vary slightly from oil to oil, and which make them detectable at sea by optical sensors:

• Their refractive index is greater than that of seawater • Their coefficient of light absorption is much stronger

than that of water, particularly at shorter wavelengths • They fluoresce when subjected to bright natural light

Page 44: Sea Surface
Page 45: Sea Surface

* *

1 2* *

1 2

*1 2

* 1 2

cos cos 2 ...

cos cos 2 ...1

sin sin 2 ...2 / 2Resin sin 2 ...

2 Im

v v h ho

v v h h o

v h

v h

E E E EI I II

E E E E Q Q QQ

U UU E EV UV

E E

L

Surface emissivity - Oceans

Plane surface:Sea-water permittivityFresnel equations (I, Q)

Wind roughened surface:Sea-water permittivityFresnel equations (I, Q)Large-scale wavesGravity-capillary, capillary waves (> 2m/s) RTTOV FASTEM-2Whitecaps (> 7 m/s)Foam (> 10-12 m/s)

Directional wind roughened surface: Sea-water permittivity Fresnel equations (I, Q, U, V)Large-scale wavesGravity-capillary, capillary waves (> 2m/s) RTTOV FASTEM-3Whitecaps (> 7 m/s)Foam (> 10-12 m/s)

Page 46: Sea Surface

Modelled emissivity - Oceans10.7 GHz 19.35 GHz = 53.1o

= 0, 180o

v-pol.

h-pol.

37.0 GHz 85.5 GHz

Wind speed [m/s]

Sensitivity of surface emission (EoTs) to real andimaginary part of dielectric constant

(Meissner and Wentz 2004)

Page 47: Sea Surface

3rd Stokes Vector at 10.7 GHz: Models vs. Windsat Data

Data Coppo et al. (1996)

Liu and Weng (2002)

Stephen EnglishMet Office

Wind speed < 4 m/s Windspeed: 4-8 m/s

Relative azimuth angle [deg.] Relative azimuth angle [deg.]

Windspeed: 8-12 m/s Windspeed > 12 m/s

Relative azimuth angle [deg.] Relative azimuth angle [deg.]

Page 48: Sea Surface

4th Stokes Vector at 19.35 GHz: Models vs. Windsat Data

Wind speed < 4 m/s Windspeed: 4-8 m/s

Relative azimuth angle [deg.] Relative azimuth angle [deg.]

Windspeed: 8-12 m/s Windspeed > 12 m/s

Relative azimuth angle [deg.] Relative azimuth angle [deg.]

Liu and Weng (2002) Coppo et al. (1996)

Data

Stephen EnglishMet Office

Page 49: Sea Surface

Sun-glint

Ralf BennartzUniversity of Wisconsin

SufficientData sample