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(1)

CLS-SHOM98.2-EIGEN2

‘forbidden’

(2)

Mean ocean surface and geoid have to be expressed:

in the same coordinate system

• in the same coordinate type

• with respect to the same reference ellipsoid

• in the same permanent tide system

and they have to be

• spectrally consistent ( a real challenge)

(3)

GEOTOP

Sea Surface Topography and Mass Transport of the Antarctic Circumpolar Current

(4)

verify results in Southern Ocean and Weddell Sea, a “cold” spot,

“tipping point” of climate system Schellenhuber

GEOTOP

determination of DOT with proper spatial and spectral characteristics impact of ICESat and GOCE

impact on ocean circulation

assimilation of DOT(t) in OGCM

(5)

Geodetic DOT - rationale

Global Approach:

- Filter in the spectral domain - Use MSS to compute h

- Extent MSS to land (!) - hMSS in sperical harmonics

DOT = 2D[hMSS – N ] Mean DOT

(for MSS period)

Profile Approach

- Avoid gridding of h

- Filter h on altimeter profiles

- Apply filter correction FC to account for diff 1D[] ≠ 2D[]

DOT = 1D[h] – 2D[N] + FC DOT snapshots

for every track

AGU 2011 ,San Francisco, G41C, GOCE... 6

DOT = h – N

h and N differ spectrally; h defined only on altimeter tracks; N given by spherical harmonics

DOT = 2D[ h – N ]

POSTER

(6)

Mean Sea Surface

1992- 2010 from altimetry (W. Bosch, 2011)

Geoid

based on six months GOCE

[Quelle: W. Bosch, DGFI, 2011]

GOCE and oceanograpy

Gulf current

Antarctic Circumpolar Curre Kuroshio

(7)

Differences between

global and profile approach

8

POSTER

(8)

Gain in variance

by lowering the filter length

9

GRACE versus GOCE; Filter D=241km/L=60 GOCE: ΔFilter D=121km/L=120 – D=241km/L=60

GOCE: ΔFilter D=97km/L=150 – D=121km/L=120 GOCE: ΔFilter D=80km/L=180 – D=97km/L=150

(9)

local geoid from terrestrial data ICESat and GOCE

airborne gravity POSTER N

(10)

Assimilation of DOT in OGCM

absolute DOT, mean + anomalies EnKF with weighting by

error variance-covariance matrix assimilation of 10day maps

(11)

resolution:

20km to 150 km

hydrostatic primitive equation Sea Ice- Ocean

General Circulation model

non linear free surface, boussinesq,

GentMCWilliams, Smagorinski, KPP, Redi etc.

freshwater flux is flux of volume and mass, no salinity restoring, resolution varies locally to include the impact of small scale processes on the global circulation

(12)

Assimilation of DOT (d/o150)

RMS differences [m], 2004

(13)

potential temperature 400m

Sub Arctic Front Orsi,climatology assimilation

(14)

POSTER

temperature in 800m in Weddell SEA

southern ACC front Orsi,climatology

assimilation

RMS error 0.4ºC -> 0.2ºC

(15)

We appreciate the funding be DFG SPP1257 good visibility of GEOTOP

in national and international conferences and workshops

> 60 oral and poster presentations > 20 conference papers and reports

Janjić T., et al. (2012) Journal of Geodynamics

Albertella, et al. (2012):Geophysical International Journal

Janjic et al. (2012 Ocean Science

Albertella et al. ( 2012) DGFI/IAPG Report No.82

Schwabe & Scheinert (2012) Journal of Geodesy

Nerger et al.(2012) Quarterly Journal of the Royal Meteorological Society

Nerger et al. (2012) Monthly Weather Review

Nerger & Hiller W. (2012) Computers & Geosciences

Janjic et al. (2011) Monthly Weather Review

Janjic et al. (2011) Journal of Geodynamics

Dettmering & Bosch (2010) Marine Geodesy

Albertella & Rummel (2009) Journal of Geodesy

Rollenhagen et al. (2009) Journal of Geophysical Research

Skachko et al.( 2008) Ocean Science

(16)

strong impact of GOCE on oceanic fronts and temporal variability

Results

DOT in two approaches are reliable but different in detail,

mostly small scale and coastal

impact of ICESat in Weddell Sea

(17)

Global DOT (left), Profile DOT (right), Diff‘s

AGU 2011 ,San Francisco,

G41C, GOCE... 21

(18)

Diff Maximenko ´09 – MiDOT, period 1992-2002

AGU 2011 ,San Francisco,

G41C, GOCE... 23

(19)

Filter correction (with EGM2008, N

max

= 2190)

AGU 2011 ,San Francisco,

G41C, GOCE... 24

DOT = 1D[h] + (2D[NEGM08] – 1D[NEGM08]) - 2D[N]

(20)

apply spectral expansion for N, SSH a) treat SSH over land as missing

b) extend SSH over land

DOT

apply spatial expansion for N, SSH treat 2D filtering (N) and

1D filtering (alongtrack altimetry) with filter correction

(21)

Determination of the mean sea-surface topography in sea-ice covered areas (Weddell Sea)

utilizing ICESat release 31 (02/2003 – 10/2009)

classification problem, solved by:

lowest-level filtering in a remove-compute-restore technique

working steps:

• ICESat specific corrections/reductions o correction of offsets (global MMXO) o robust outlier elimination

o DAC reduction

o ocean tide reduction (EOT11a) o geoid reduction (EGM2008, d/o 2190)

• median filter, interpolation, restore

• final Gauss filter (d/o 210, 69 km halfwidth)

conclusions:

• ICESat delivers suitable data to determine sea- surface heights in (partly) ice-covered Southern Ocean

(only static surfaces)

• further improvement by careful application of techniques and by combination with Cryosat-2 data

Fig.: mean sea-surface topography

(referenced to GOCO02S) (unit: meter)

Projekt: SCHE 1426/6

Mirko Scheinert, Joachim Schwabe diploma thesis: Verena Lieb (2011)

(22)

Regional Geoid Improvement in the Weddell Sea region

utilizing heterogeneous data

remove-compute-restore technique least-squares collocation

background model: GOCO02S (Pail et al., 2010)

upper left: terrestrial and airborne gravity anomalies right: improved regional geoid upper right: prediction error

conclusions:

• GOCE already delivers reliable information

• more signal added at shorter wavelengths by incorporation of terrestrial gravity anomalies

• a more complete terrestrial data coverage would further improve the solution

Schwabe & Scheinert (2012):

Journal of Geodesy (in review)

Projekt: SCHE 1426/6

Mirko Scheinert, Joachim Schwabe

(23)

legrand vergleich sr3 etc

glolbal + localization

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