Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport...

27
Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with the thermal wind relation this become /dz v dx = -g/fρ 0 [ ρ(x 2 ) – ρ(x 1 ) ] Thus density profiles at the end points allow to obtain transport v dxdz . Bottom pressure gives reference layer velocity fluctuations. Here: example from

Transcript of Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport...

Page 1: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Chapter 11: Remote sensingA: Acoustic remote sensing (was chapter 9)

B: Geostrophic transport estimates

∫ v dx = 1/fρ0 [ p(x2) – p(x1) ] and with the thermal wind relation this becomes

d/dz ∫ v dx = -g/fρ0 [ ρ(x2) – ρ(x1) ]

Thus density profiles at the end points allow to obtain

transport ∫ v dxdz .

Bottom pressure gives reference layer velocity fluctuations.

Here: example fromMOVE array

Page 2: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Total geostrophic NADW transport variability

Page 3: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

C: Satellites (and aircraft)(most figures from Summerhayes&Thorpe “Oceanography: an illustrated guide

Spectrum used: visible to microwave, for microwaves have passive and active sensors

Page 4: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.
Page 5: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.
Page 6: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Non-scanning versus scanning

Page 7: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Geostationary versus orbiting

Page 8: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Space-time scales

Page 9: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.
Page 10: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

SST observations

Page 11: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Ocean color observations

Page 12: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Synthetic aperture radar (SAR) observations

Page 13: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

SAR example

Page 14: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

SAR example

Page 15: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Waves and winds (scatterometer)

Page 16: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Altimetry

After the success of SEASAT, the newplanned altimetry missions were adustedto best complement the in-situ observations.Topex/Poseidon (T/P) was essentially designed for WOCE.

Rationale:• cm-accuracy sea-surface height • geostrophic surface flow relative to geoid• heat storage from large-scale steric effect• variability from 20-10000km, 20days-10years

Challenges and limitations:• geoid insufficient at <3000km • aliasing of tides at 62, 173,... days• aliasing of high-frequ. wind-forced variability• extrapolation to ocean interior• no coverage in polar (and ice-covered) regions• land motion of tide gauges for SL rise

Page 17: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.
Page 18: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Example result: extremely active time-dependence of the circulation (barotropic, baroclinic current systems,eddy motions, etc)

Quantified SSH and slope variance on all space/time scales globally

(C. Wunsch)

(D.Stammer)

Page 19: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Eddy contribution tomeridional heat flux:

Other results/achievements:• open-ocean tides measured globally to 2-3cm• surface heat-flux estimates on basin-scales from storage• observation of interannual variability (ENSO, circumpolar wave, etc)• kinetic energy of geostrophic currents in agreement with moorings• eddy energy helped to demonstrate that models need 0.1° resolution• agreement of T/P currents and ADCP data to 3-5cm/s• global test of Rossby wave speeds• global SL rise (calibrated with tide gauges) accurate to 0.5mm/yr• transports of baroclinic current systems (variability)• drove advances in earth´s gravity field• drove most of the work in assimilation• many more.....

(D. Stammer)

Page 20: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Missions at:http://airsea-www.jpl.nasa.gov/mission/missions.html(OLD) now see seperate ppt file.....

More about altimetry at:http://topex-www.jpl.nasa.gov/www.aviso.oceanobs.com/en/altimetry/index.html

More about scatterometer athttp://winds.jpl.nasa.gov/

General satellite missionswww.aviso.oceanobs.com/

Page 21: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Some sensor types/names:

Scatterometers: NSCAT (on Japanese ADEOS), QuickScat, SeaWinds (on ADEOS-II), ASCAT. Deliver vector wind (stress), sea ice, iceberg drift.

Radars: altimeter, SAR

Radiometer: AVHRR (advanced very high resolution radiometer), has several IR bands, can be used to estimate absorption in atmosphere, gives SST; Also in microwave now – SMMR (scanning multi-channel microwave radiometer), passive, also yields ice cover and humidity

SSM/I: special sensor microwave imager, gives only wind speed (not direction), 4 bands, precipitation

CZCS: coastal zone color scanner (on Nimbus satellite), many visible channels

Page 22: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

More neat stuff, e.g. “Iridium flares” atwww.heavens-above.com/

GRACE gravity mission

Page 23: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

See also:

www.eohandbook.com

And

www.esa.int/esaEO/index.html

Page 24: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

Overview over some satellite-derived products: http://podaac.jpl.nasa.gov/http://coastwatch.pfeg.noaa.gov/coastwatch/CWBrowser.jsp

Altimetry:AVISO: http://www.aviso.oceanobs.com/

http://las.aviso.oceanobs.com/las/servlets/dataset/ftp://ftp.cls.fr/pub/oceano/AVISO/SSH/duacs/

Ocean color and SST (MODIS, SeaWIFS, ...) http://oceancolor.gsfc.nasa.gov/

Ocean surface currents (using wind, altimetry:) http://www.oscar.noaa.gov/(from sequential satellite imagery:) http://ccar.colorado.edu/research/cali/

GRACE gravimetryhttp://op.gfz-potsdam.de/grace/http://podaac.jpl.nasa.gov/DATA_CATALOG/graceinfo.html

Satellite Data Websites:

Page 25: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

altimetry

Altimetry and ARGO

Sea surface height (SSH) consists of - the steric (dynamic height Hdyn) contribution of T and S - a barotropic flow component (reference level pressure Pref)

Symbolically SSH = Pref + Hdyn = SSH’ + SSH

Altimetry has good spatial and temporal coverage but cannot determine

- steric and non-steric components- mean SSH field (relative to geoid)- T and S contributions (spiciness)- interior structure (vertical distribution) of Hdyn

ARGO data can help resolve these issues

Page 26: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

altimetryFloat profiles

Symbolically SSH = Pref + Hdyn = SSH’ + SSH

scatter is a measurefor non-stericcontributions(plus errors)

altimetric SSH‘ vs in-situ H‘dyn

Compare SSH‘ and float H‘dyn :

large barotropiccontributions athigh latitudes

Correlation vs latitude

(from P.-Y. Le Traon)

Page 27: Chapter 11: Remote sensing A: Acoustic remote sensing (was chapter 9) B: Geostrophic transport estimates ∫ v dx = 1/fρ 0 [ p(x 2 ) – p(x 1 ) ] and with.

altimetryFloat profiles

deeptrajectories

residual

Symbolically SSH = Pref + Hdyn = SSH’ + SSH

Deep mean flow (pref) from float trajectories :

(from R.Davis)