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Low FSSIE Low FSSIE

2D Atmospheric Blocking2D Atmospheric Blocking frequencyfrequencyAdvective Sea Ice Advective Sea Ice Streamfunction [Sv]Streamfunction [Sv]Anomalous Surface Anomalous Surface Wind Stress [N/m²]Wind Stress [N/m²]

High FSSIE High FSSIE

(a) Anomalous Sea(a) Anomalous Sea Ice Velocity [m/s] Ice Velocity [m/s] and (b) Anomalous and (b) Anomalous Sea Ice Thicknes [m]Sea Ice Thicknes [m]

(a) (b) (a) (b)

Composite Map Analysis of FSSIE:

Composite Map Analysis of FSSIE:

Composite Map Analysis of FSSIE:

Composite Map Analysis of FSSIE:

Causes and consequences of the late 1960s Causes and consequences of the late 1960s

GSA event ?!

GSA event ?!

Causes and consequences of the late 1960s Causes and consequences of the late 1960s

GSA event ?!

GSA event ?!

Modeled Great Salinity Modeled Great Salinity

Anomaly (GSA):

Anomaly (GSA):

Modeled Great Salinity Modeled Great Salinity

Anomaly (GSA):

Anomaly (GSA):

POLARSTERN

References References

[*] M. Ionita, P. Scholz,et al. (2015), Abrupt shift of the Atlantic Ocean circulation during the 1970s induced by atmospheric blocking. Under review in Nature Climate Change [*] M. Ionita, P. Scholz,et al. (2015), Abrupt shift of the Atlantic Ocean circulation during the 1970s induced by atmospheric blocking. Under review in Nature Climate Change

[1] Scholz, P. et al. (2014), Evaluation of Labrador Sea water formation in a global finite-element sea-ice ocean model setup based on a comparison with observational data, J. Geophys. Res. Ocean, 119, DOI: 10.1002/2013JC009232 [1] Scholz, P. et al. (2014), Evaluation of Labrador Sea water formation in a global finite-element sea-ice ocean model setup based on a comparison with observational data, J. Geophys. Res. Ocean, 119, DOI: 10.1002/2013JC009232 [2] Scholz, P., et al. (2013), Evaluation of a Finite-Element Sea-Ice ocean model (FESOM) setup to study the interannual to decadal variability in the deep-water formation rates, Ocean Dynamics, 63 (4), 347-370

[2] Scholz, P., et al. (2013), Evaluation of a Finite-Element Sea-Ice ocean model (FESOM) setup to study the interannual to decadal variability in the deep-water formation rates, Ocean Dynamics, 63 (4), 347-370 [3] Häkkinen, S.,et al. (2011), Atmospheric Blocking and Atlantic Multidecadal Ocean Variability, Science, 334 (6056), 655-659. [DOI:10.1126/science.1205683]

[3] Häkkinen, S.,et al. (2011), Atmospheric Blocking and Atlantic Multidecadal Ocean Variability, Science, 334 (6056), 655-659. [DOI:10.1126/science.1205683]

¹ Alfred Wegener Institute Helmholtz Center for Polar and Marine Research, Bremerhaven, Germany¹ Alfred Wegener Institute Helmholtz Center for Polar and Marine Research, Bremerhaven, Germany, ² , ² MARUM – Center for Marine MARUM – Center for Marine Environmental Sciences, University of Bremen, Bremen, Germany

Environmental Sciences, University of Bremen, Bremen, Germany, ³ , ³ Bucharest University, Faculty of Physics, Bucharest, RomaniaBucharest University, Faculty of Physics, Bucharest, Romania

Abrupt shift of the Atlantic Ocean circulation Abrupt shift of the Atlantic Ocean circulation

induced by atmospheric blocking induced by atmospheric blocking

Abrupt shift of the Atlantic Ocean circulation Abrupt shift of the Atlantic Ocean circulation

induced by atmospheric blocking induced by atmospheric blocking

➢ Modeled (solid) and observational derived (dashed, Schmith and

Hansen 2003) time-series of FSSIE.

➢ Correlation 0.61 (Significance level 99.9%)

➢ Modeled FSSIE above

above/below 75% below of standard devi- ation

Modeled & observational derived Fram Strait Modeled & observational derived Fram Strait

Sea Ice Export (FSSIE):

Sea Ice Export (FSSIE):

Modeled & observational derived Fram Strait Modeled & observational derived Fram Strait

Sea Ice Export (FSSIE):

Sea Ice Export (FSSIE):

2d Blocking Index:2d Blocking Index:

➢ Scherrer et al. 2006, based on data of

geopotential height

➢ Blocked grid point when at least five consecutive days fulfill the condition

H H L L

H H L L H H

Ω-type

GHGS= Z 0)−Z S) ϕ0−ϕS

GHGN= Z N )−Z 0) ϕN−ϕ0

ϕN0+15° , ϕS0−15° ϕ0=grid point latitude

GHGS>0 , GHGN<−10 m

deglat

Southwest-northeast dipole

Southeast-northwest dipole

51-55 51-55

Mean atmospheric blocking frequency Mean atmospheric blocking frequency

56-60

56-60 61-6561-65

66-70 66-70

81-85 81-85

71-75

71-75 76-8076-80

96-00 96-00

86-90 86-90

01-05 01-05

91-95 91-95

06-10 06-10

Atmospheric Blocking:

Atmospheric Blocking:

Atmospheric Blocking:

Atmospheric Blocking:

DJF surface salinity anomaly DJF surface salinity anomaly

0-100 m, 1967-1972 0-100 m, 1967-1972

TempTemp..SalinitySalinity

➢ Surface fresh water

anomaly that occupied central Labrador Sea for several years

➢ Known GSA events,

~1970 (Dickson et

al. 1988), ~1982 and ~1982

~1988

~1988 (Belkin et al.

1998 & 2004)

➢ Linked with increased sea ice transport

through Fram or Davis Strait

I

II

3 year running mean

Change of ArcticChange of Arctic Sea Ice VolumeSea Ice Volume [1 km³/yr][1 km³/yr]

Mean BlockingMean Blocking IndexIndexDJF FSSIEDJF FSSIE [Sv][Sv] Lab. Sea DJFLab. Sea DJF SSS [psu]SSS [psu]

AMOC at AMOC at 4N [Sv]4N [Sv]

Strongest Greenland blocking event in 1962- 1966, reduced meridional air mass exchange Accumulation of Arctic sea ice volume until 1966, afterwards decrease in sea ice volume Flush out of Arctic sea ice by increased sea ice export through Fram Strait ~ 1968/69. Cre- ates freshwater anomaly by sea ice melting

Surface freshwater anomaly occupies ~1971 the central Labrador Sea and creates strong- est GSA event of the last 5-6 decades.

Reduced deep ventilation in the central Labrador

Sea leads to a drop in AMOC around 1971

Introduction Introduction : :

Fram Strait sea ice export from the Arctic represents a key source of fresh water for the North Atlantic. Although variations in the ice ex- port may have a strong influence on the Atlantic meridional overturn- ing circulation (AMOC), their causes and consequences are not yet fully understood. Using a global ocean-sea ice model with increased resolution over the Arctic and northern hemisphere deep-water form- ation areas, here it is shown that enhanced blocking activity over Greenland and the northern North Atlantic during the period 1962- 1966 favored sea ice accumulation in the Arctic. Whereas the period 1967-1971 was characterized by weak blocking activity in the region, leading to intensified Arctic sea ice export and, hence, reduced Lab- rador Sea surface salinity and a weakened AMOC. These results in- dicate that AMOC shifts toward weak states, as the one emphasized here in the 1970s, may be induced by rapid sea ice flushes from the Arctic after periods of enhanced blocking activity over Greenland.

They imply also that an important part of the atmosphere-ocean dy- namics at mid- and high latitudes requires a proper representation of the Fram Strait and associated sea ice transport as well as synoptic scale variability such as atmospheric blocking, which is a challenge for current coupled climate models. In this study we investigate the potential driving role of the atmospheric blocking activity for FSSIE as well as the associated consequences for the North Atlantic fresh- water budget and ocean circulation in this sector.

➢Regional resolution of the global model setup in the Northwest

Atlantic Ocean. The dashed line marks the position of the AR7W cruise line

➢The resolution in

Labrador Sea varies between 15 km in the North and 30 km in the South

Ø Ø ~24k~24kResoResommlut.lut.

Fram Strait Fram Strait

Methodology:

Methodology:

➢Use Finite Element Sea Ice- Ocean Model (FESOM,

developed at Alfred Wegener Institute)

➢Solve primitive equation under Boussinesq

approximation Forcing:

Forcing:

➢COREv2.0 (tair,specific

humidity, precipitation, wind speed, radiation flux, SSS climatology)

Mesh:

Mesh:

➢Unstructured triangular surface mesh (53.382 surface nodes, 101.827

triangular surface elements)

➢41 vertical levels

➢3D tetrahedral elements (~1 Mio. 3D nodes, ~6 Mio 3D elements)

P. Scholz

P. Scholz

1,21,2

(Patrick.Scholz@awi.de) (Patrick.Scholz@awi.de) , M. Ionita , M. Ionita

1,21,2

, M. Dima , M. Dima

1,31,3

, G. Lohmann , G. Lohmann

1,21,2

, ,

M. Prange M. Prange

22

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