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Opening and closing of the Storfjorden polynya Frank Nilsen Frank Nilsen 1,2 1,2 , Ragnheid Skogseth , Ragnheid Skogseth 1 , , Katja Weigel Katja Weigel 1 1.The University Centre in Svalbard (UNIS), 1.The University Centre in Svalbard (UNIS), Longyearbyen, Norway Longyearbyen, Norway 2.Geophysical Institute, University of Bergen, 2.Geophysical Institute, University of Bergen, Bergen, Norway Bergen, Norway

Opening and closing of the Storfjorden polynya. Coastal Polynya Skogseth (2003), PhD thesis Storfjorden is estimated to supply 5-10% of the newly formed

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Opening and closing of the Storfjorden polynya

Frank NilsenFrank Nilsen1,21,2, Ragnheid Skogseth, Ragnheid Skogseth11, Katja Weigel, Katja Weigel11

1.The University Centre in Svalbard (UNIS), Longyearbyen, Norway1.The University Centre in Svalbard (UNIS), Longyearbyen, Norway

2.Geophysical Institute, University of Bergen, Bergen, Norway2.Geophysical Institute, University of Bergen, Bergen, Norway

Coastal Polynya

Skogseth (2003), PhD thesis

Storfjorden is estimated to supply 5-10% of the newly formed dense waters of the Arctic Ocean

The Barents Sea and Storfjorden

Storfjorden

Skogseth et al. (2005), CSR

• Is approximately 190 km long and 190 m deep at its maximum depth.

• A 120 m deep sill at about 77°N in the south.

•The basin covers an area of about 13·103 km2 with a volume of 8.5·1011 m3.

Storfjorden Polynya

Skogseth (2003), PhD thesis

Maximum Salinity observed in the deepest part of Storfjorden

Skogseth & Fer (2005), AGU Anderson et al. (2004), JGR

Polynya Area and SAR

• We utilize the polynya width model formulated by Haarpaintner et al. (2001) and Skogseth et al. (2004).

• The model calculates the area of open water and thin ice defined as the polynya area, and the area of fast and pack ice.

• The model consist of two algorithms: polynya width algorithm and an open water width algorithm.

• The polynya width algorithm needs two empirical factors as input: the opening (OF) and closing (CF) factors.

Empirical Tuning

Wind Stress Curl field (DJFM, 1970-2004)

From the Hindcast data base (met.no) with a 75 km resolution

Sea Ice Drift

waa UUUU 21

DJFMA wind stress

OF and CF correlated with the winter mean wind stress curl

DJFMA wind stress

Mechanical and thermodynamical sea ice growth

FF

fph

Fp U

Uh

W

tL

SU

dt

dW

)(

1

000,

0

1- O(1) + O(10) = CF1+ O(1) + O(0) = OF

Result Summary

Winters with low Iw

More positive curl Divergence

Winters with high Iw

More negative curl Convergence

Reproduced OF as a function of the curl at 75.4°N, 25.1°E

Total ice production (normalized)

Conclusions• Physical explanations for the empirical OF and CF

are found.• CF is dominated by thermodynamical ice growth

through consolidation of frazil ice, but mechanical ice growth determine the interannual variations.

• OF’s deviations from the free drift solution is determined by divergence and convergence in the compact ice cover outside Storfjorden.

• Annual variations in OF and CF are directly linked to the wind stress curl field and an empirical relations is found from the hindcast data base (met.no) time series.

• The polynya model gives a more realistic sea ice production when the model is run with time varying OF and CF.

The Barents Sea Ice Index Iw

Ådlandsvik & Loeng (1990), Polar Res.

The integrated winter ice covered area south of 76ºN in a zone between 25ºE and 45ºE.

Correlation between the curl (DJFM) and Iw (1970-2003)