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pCO 2 dynamics and related air-ice CO 2 fluxes during sea ice growth and decay in a ice tank experiment

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pCO 2 dynamics and related air-ice CO 2 fluxes during sea ice growth and decay in a ice tank experiment

B. Delille

1

, D.N. Thomas

2

, G. S. Dieckmann

3

, S. Papadimitriou

2

, H. Kennedy

2

, M. Fischer

3

, K.-U. Evers

4

J.-L. Tison

5

1Unité d’Océanographie Chimique Université de Liège – Belgium (Bruno.Delille@ulg.ac.be)

2School of Ocean Sciences, Bangor University - UK

3Alfred Wegener Institute - Germany

4Ice & Offshore Technology, Hamburgische Schiffbau-Versuchsanstalt GmbH (HSVA), Germany

5 Glaciology Unit, Université Libre de Bruxelles - Belgium

CO

2

uptake by sea-ice

For decades, sea ice has been considered by the scientific community as an inert and impermeable barrier to air-sea gas exchanges. However, this assumption is not supported by studies on the ice permeability to gases and liquids, which show that sea ice is permeable at temperatures above -5°C. Recently, uptake of atmospheric CO2over sea-ice cover has been reported supporting the need to further investigate pCO2dynamics in the sea-ice realm and related CO2fluxes

The experiment

The INTERICE 4 project run at the Arctic Environment Test basin of Hamburgische Schiffbau-Versuchsanstalt GmbH (HSVA) in September 2009. It addressed fundamental questions on the biogeochemistry of carbon during ice formation with an emphasis on precipitation of CaCO3. In the course of the experiment, we followed the pCO2changes within brines

d d l i f l i h i h h i l

24 polyethylene enclosures were filled with North Sea water. 12 were treated to increase phosphate concentration and decrease pH. The experiment was designed to simulate an ice growth phase during 12 days followed by a melt phase of 4 days. Ice growth was about 2 cm d-1. Underlying water of 6 of the bags were sampled every 1~2 days. Ice samples were collected during 4 main sampling session. 6 bags were sampled for ice at each main sampling system. Each bag were sampled for ice only one time. We collected ice for salinity and temperature vertical profile, and we carried out direct measurement of the partial pressure of CO2(pCO2) of brines and underlying water, and air-ice CO2 fluxes with the chamber method.

and underlying water of several ice mesocosms, together with physical parameters of the ice. In addition we measured air-ice CO2fluxes with the chamber method

pCO

2

changes and related air-ice CO

2

fluxes

400

Bag 4 SW 11 Bag 15 SW 10

(ppm)

p

2

g

2

0 100 200

300 Bag 1 SW 12

Bag 4 SW 11 Bag 18 SW pH 10 Bag 20 SW pH 12 Bag 22 SW pH 11

SW pH ( )

pCO2 underlying water (

600 800

SW pm) pH

We observed steady sea ice growth during the first 8 days of freezing, with a slight slowing down of the sea ice growth during the next 6 days of freezing conditions. This phase was followed by the final phase of ice decay in warm conditions. The pCO2in the brines increased during the first 4 days of the ice growth phase and ranged from 444 to 706 ppm. During the ice decay phase, the pCO2of the brine decreased dramatically and ranged from 200 to

0 200 400

5/09 8/09 11/09 14/09 17/09 20/09 Day

pCO2 brines (pp

4 6

SW -2-1ol m d) pH

the brine decreased dramatically and ranged from 200 to 335 ppm. At the beginning of the ice growth, all mesocosms released CO2 to the atmosphere. As the ice temperature and permeability decreased further, the flux of CO2to the atmosphere decreased. During most the ice growth phase, air-ice CO2 fluxes were low or below the detection limit of the measurement. At the beginning of ice decay phase, we measured significant uptake of atmospheric CO2 by the ice in accordance with the observed sharp decrease of the pCO2of brines well below

-4 -2 0 2

p

air-ice CO2fluxes (mmo

observed sharp decrease of the pCO2of brines well below the mean air pCO2 in the ice tank room. However, this uptake decreased significantly afterwards.

SW and pH denotes none treated and treated bags for phosphate and pH, respectively.

Negative fluxes correspond to influx from the atmosphere to the ice. Grey area correspond to pCO2 of the atmosphere inside the tank room.

Driving processes

600

800 pCO2 SW

theroetica change of pCO2 according

(ppm)

pCO2 of brines (none treated bags) appears to be tightly linked to

IGS Tromsø 31/05 – 4/06 2010 57A189

-6 -5 -4 -3 -2 -1

0 200 400

to temperature and related salinity changes

pCO2 brines

pCO2 of brines (none treated bags) appears to be tightly linked to temperature changes. However, there is a strong discrepancy between observed changes and theoretical changes predicted by temperature changes and related salinity changes (predicted by Cox and Weeks 1975). Other temperature-related processes are likely to influence pCO2.

CO2 fluxes are controlled by permeability of the ice at the air-ice interface. During the experiment the threshold of permeability for air-ice CO2transfer was a brine volume of 0.95% almost twice the value predicted by Golden et al.

1998.

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