D a y o f th e e x p e r im e n t 0 2 4 6 8 1 0 1 2 1 4 1 6 p C O2 ( ma tm ) 0 2 0 0 4 0 0 6 0 0 A t m o s p h e r ic p C O2 I c e s u r f a c e p C O2 D a y o f th e e x p e r im e n t 0 2 4 6 8 1 0 1 2 1 4 1 6 A ir -i c e in te rf a c e t e m p e ra tu re ( °C ) -1 0 -9 -8 -7 -6 -5 -4 -3 -2 A ir -i c e C O2 f lu x ( m m o l m -2 d -1) -6 -2 -1 0 1 C O2 s in k C O2 s o u r c e
Gas transfer coefficient :
K = F / (pCO
2 ice- pCO
2 air) =
2,5
mol m
-2d
-1atm
-1The study of air-ice CO
2exchange emphasize the importance of gas
bubble transport during sea ice growth
TAKE HOME MESSAGES:
Sea ice exchange gas with the atmosphere
During sea ice growth, gas are transported by diffusion and buoyancy while convection is limited
The gas transfer coefficient for CO2 at the air- ice
interface of growing sea ice is 2,5 mol m-2 d-1 atm-1
Our 1D model can simulate air-ice CO2 fluxes and
point to the role of gas bubbles in sea ice
Gas bubbles may explain a large part (~ 92 %) of the observed CO2 fluxes in the present experiment
Cooling ->
Marie Kotovitch1,2, Sébastien Moreau3, Jiayun Zhou1,2, Jean-Louis Tison2, Fanny Van der Linden1,
Gerhard Dieckmann4, Karl-Ulrich Evers5, David Thomas6,7 and Bruno Delille1
1D MODELLING EMPHASIZES THE ROLE OF BUBBLE
1D MODELLING EMPHASIZES THE ROLE OF BUBBLE
Carbon dioxide (CO2) plays a crucial role in climate changes and global warming. Sea ice is
involved in CO2 exchanges between the ocean and the atmosphere. In the present study, we used a tank that allows to
control freezing of seawater in order to reproduce ice growth and decay over a 19 days experiment. The aims of this study were to: (1) determine a gas transfer coefficient for CO2 in sea ice during its growth, (2) understand the processes
responsible for CO2 transport between air and sea ice by comparing our results with a 1D biogeochemical model.
Materials and Methods: The temperature of the atmosphere above the tank water was set to -15 °C the first 14 days, then
to -1 °C until the end of the experiment. We measured continuously in situ ice temperature, underwater salinity and air-ice CO2 fluxes. Ice cores were also collected regularly to measure biogeochemical variables.
INTRODUCTION
INTRODUCTION
F = air-ice CO
2fluxes
F = air-ice CO
2fluxes
Warming -> Cooling ->We measured temperature and air-ice CO2 flux
in continuous with a chamber over the ice. Sea ice shifts from:
(i) a sink during the first crystals formation,
(ii) to a source during ice growth and, finally
(iii) return to a sink during ice melt.
From the difference in partial pressure of CO2
in the air and the ice, we calculated daily dC.
The evolution of dC is consistent with measured flux (F), shifting from: (i) negative,
(ii) to positive and, finally (iii) return negative.
We define dx from the observation of the total inorganic carbon (DIC) profiles. We observed a CO2
depletion in the 12 first centimetres. We assumed that it was due to a CO2
release from the ice to the air.
dC = air-ice difference in CO
2partial pressure
dC = air-ice difference in CO
2partial pressure
dx = depth in ice for air-ice
CO
2exchange
dx = depth in ice for air-ice
CO
2exchange
We included the 3 parameters determined above in the equation define by Liss and Slater (1974) and Sarmiento and Gruber (2004) and deduced a gas transfer coefficient for CO2 (K). This coefficient is applicablefor a growing permeable and artificial sea ice.
References: Moreau et al., 2015. Drivers of inorganic carbon dynamics in first-year sea ice : a model study. J. Geophys. Res. Ocean. 120, 471–495.
To mimic the observed air-ice CO2 fluxes, we used the 1D model of Moreau et
al. (2015). The inversion between outward CO2 fluxes during ice growth and
inward CO2 fluxes during ice melt depicts well the observations. However, the
model (M2015) strongly underestimates the fluxes during the cold phase if the
formation rate of gas bubbles is low. Since ice is permeable throughout the
cold phase, higher gas bubble formation rates lead to higher CO2 fluxes (i.e.
gas bubbles escape the ice surface and add to the outward CO2 flux).
1Unité d’Océanographie Chimique, Ulg, Belgium, 2Laboratoire de
Glaciologie, ULB, 3Georges Lemaître Centre for Earth and Climate
Research, UCL, 4Alfred Wegener Institute Helmhotz Center for Polarand
Marine Research, Germany, 5Hamburgische Schiffbau-Versuchsanstalt
GmbH (HSVA), 6Marine Research Center, Helsinki, Finland, 7School of Ocean Sciences, Bargor University, United Kingdom
Warming -> D IC 7 ( µ m o l k g - 1) 4 0 0 4 5 0 5 0 0 D ep th ( cm ) 0 5 1 0 1 5 2 0 2 5 D a y 5 D a y 8 D a y 1 4 D a y 1 5 D a y 1 6 D a y o f th e e x p e r im e n t 4 5 6 7 8 9 1 0 1 1 1 2 1 3 1 4 1 5 1 6 1 7 A ir -ic e C O2 fl u xe s (m m o l m -2 d -1) -1 .0 -0 .5 0 .0 0 .5 1 .0 O b s H ig h B u b C T R L L o w B u b M o r e a u 2 0 1 5