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Sediment trap data
0
500
1000
1500
2000
2500
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
1000 m
23
0T
hxs
flux
(fg
/m2/d
)
in situ production
0
500
1000
1500
2000
2500
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
230T
hxs fl
ux (f
g/m
2 /d)
400 m
in situ production
0,00E+00
1,00E-05
2,00E-05
3,00E-05
4,00E-05
5,00E-05
6,00E-05
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
230T
h/23
2T
h (a
tom
ic r
atio
)
400 m
1000 m
suspended particles collected between 400 m and 1000 m
Constraining the seasonal particle flux in the eastern North Atlantic with Thorium isotopes
M. Roy-Barman (1), R. El Hayek (1), I. Voege (2), M.Souhaut (3), N. Leblond (4), C. Jeandel (2).(1) LSCE, Avenue de la Terrasse, 91198 Gif sur Yvette, France, (2) AWI, PO Box 120161, 27515 Bremerhaven, Germany, (3) LEGOS, 14 Avenue E. Belin, 31400, Toulouse France, (4) LOV, BP 28, 06234 Villefranche sur mer, France
Poster Area Esplanade
poster board number P0600
Principle of the sediment trap calibration.
Problems … = trapping efficiency
230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
Problems … = trapping efficiency
230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
Problems… = trapping efficiency
230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
change of 230Th inventory in the water column
-Problems…
= trapping efficiency230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
change of 230Th inventory in the water column
-
Time dependent of the sediment trap calibration.
T
H
H THT T
H
T
H
H TH THTHT
Eddy structure of the sampling area (M. Assenbaum et al., 2003)
Pomme 1 Pomme 2 Pomme 3 (winter) (spring) (Automn)
dissolved + particulate 230Thxs (fg/kg )
-1200
-1000
-800
-600
-400
-200
0
0 1 2 3 4 5 6 7
Dep
th (
m)
Pomme1 Pomme 2 Pomme 3
35,6
35,7
35,8
35,9
36
36,1
3 4 5 6 7
Pomme1
Pomme2
Pomme3
dissolved + particulate 230Thxs (fg/kg )
salin
ity
mixing trend
--> 230Thxs in not controlled
by production-scavenging only
1000 m samples
POMME 1 POMME 2 POMME 2 POMME 3 400 m 1000 m 400 m 1000 m
230Thxs flux in sediment trap (fg/m2/d)
744 935 195 439
in situ production above the trap (fg/m2/d)
592 1479 592
1479
apparent trapping efficiency
126 % 63 % 30 % 31 %
Change of 230Thxs inventory (fg/m2/d)
- 231 ± 1500 + 5830 ± 6674 + 755 ± 591 + 2737 ± 1647
corrected trapping efficiency (fg/m2/d)
> 23 %
> 40 % > 7 % > 100 %
dissolved + particulate 230Thxs (fg/kg )
-1200
-1000
-800
-600
-400
-200
0
0 1 2 3 4 5 6 7
Dep
th (
m)
Pomme1 Pomme 2 Pomme 3
T
H
H THT T
H
T
H
H TH THTHT
Constraining the seasonal particle flux in the eastern North Atlantic with Thorium isotopes
M. Roy-Barman (1), R. El Hayek (1), I. Voege (2), M.Souhaut (3), N. Leblond (4), C. Jeandel (2).(1) LSCE, Avenue de la Terrasse, 91198 Gif sur Yvette, France, (2) AWI, PO Box 120161, 27515 Bremerhaven, Germany, (3) LEGOS, 14 Avenue E. Belin, 31400, Toulouse France, (4) LOV, BP 28, 06234 Villefranche sur mer, France
[email protected]: Constraining the present and past oceanic biological pump requires a good understanding of the marine particle dynamics and of their interaction with the surrounding water column. Particle fluxes are studied mainly with sediment traps, so that it is critical to evaluate their efficiency. The average efficiency of moored sediment traps is calibrated by the 230Th method. 230Th is produced uniformely in the ocean by radioactive decay of 238U and it is rapidely removed from the water column by scavenging on settling particles. The trapping efficiency is obtained by comparing the 230Thxs trapped flux with the 230Th production in the
overlying watercolumn. This was previously done with trap data obtained over a year in order to avoid the problem of estimating the change of 230Th inventory in the water column. The idea: Here we propose to extend this method to estimate the efficiency of moored traps on a seasonal scale. It requires high precision data to measure the change of 230Th inventory in the water column. By combining sediment trap data with the change of 230Th inventory, it is possible to obtain the trapping efficiency for a short time period.
Water column results: While the 230Thxs decreases in the surface waters from POMME 1 to
POMME 3, there is a significant increase of 230Thxs in the deep waters that cannot be solely due
to the remineralisation of the settling particles. The increasing rate of the 230Thxs inventory
from 0 to 400 or 1000 m in larger than the in situ production rate suggesting that advective inputs of 230Th are significant. The effect of water mass mixing is supported by the correlation between the 230Thxs content and the salinity of the water masses at 1000 m .
Trapping efficiency: For short periods, the flux/production ratio (apparent efficiency) may be different from the trapping efficiency. However during a high flux period, when particulate export must dominate over in situ production, it provides an upper bound of the trapping efficiency. The uncertainties on the change of 230Thxs inventory are large so that the corrected
efficiencies are not well constrained. Negative efficiencies are found when the 230Thxs
inventory increases faster than the in situ production. If we neglect the effect water mass mixing, we can obtain a lower bound for the corrected trapping efficiency.
Conclusion: By comparing apparent and corrected trapping efficiencies, a good braketing of the trapping efficiency can be obtained (eg. at 1000 m between P 1 and P 2 or at 400 m between P 2 and P 3). An explicit treatment of the mixing effect is required to improve the the method.
Principle of the sediment trap calibration.
Sampling: During the POMME program, we have measured Thorium isotopes in seawater, small particles and large particles collected in early March 2001 (POMME 1), mid April 2001 (POMME 2) and September 2001 (POMME 3) in the eastern North Atlantic. Here, we report results obtained on large particles collected with moored sediment traps (at 400 and 1000 m) and dissolved and small particles samples collected between 10 and 1000 m in anticyclonic eddies closely associated to the sediment trap at the time of sampling. All these samples were analysed for 230Th and 232Th by ID-TIMS.
Trap results: During the spring bloom (from POMME 1 to POMME 2), strong variations of total mass flux and of the 230Thxs flux are recorded by the sediment traps. Over this period, the
trapped 230Thxs flux represents 125% of the overlying production at 400 m and 65% at 1000
m. From POMME 2 to POMME 3, the 230Thxs fluxes are more constant and they represent
30% of the overlying production only. Beside the trap calibration aspect, Th isotopes provide important information on the particle dynamics: the increase of 230Th/232Th ratio in the trapped material between 400 and 1000 m implies (independently of the flux data) that small particles have been aggregated to the sinking particles between these depths.
35,6
35,7
35,8
35,9
36
36,1
3 4 5 6 7
Pomme1
Pomme2
Pomme3
dissolved + particulate 230Thxs (fg/kg )
salin
ity
mixing trend
--> 230
Thxs in not controlled
by production-scavenging only
Problems… = trapping efficiency
230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
change of 230Th inventory in the water column
-Problems…
= trapping efficiency230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
change of 230Th inventory in the water column
-
Eddy structure of the sampling area (M. Assenbaum et al., 2003)
Sediment trap data
Water column data
POMME 1 POMME 2 POMME 2 POMME 3 400 m 1000 m 400 m 1000 m
230Thxs flux in sediment trap (fg/m2/d)
744 935 195 439
in situ production above the trap (fg/m2/d)
592 1479 592
1479
apparent trapping efficiency
126 % 63 % 30 % 31 %
Change of 230Thxs inventory (fg/m2/d)
- 231 ± 1500 + 5830 ± 6674 + 755 ± 591 + 2737 ± 1647
corrected trapping efficiency (fg/m2/d)
> 23 %
> 40 % > 7 % > 100 %
0
500
1000
1500
2000
2500
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
1000 m
230 T
hxs
flux
(fg
/m2 /d
)
in situ production
0
500
1000
1500
2000
2500
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
230 T
hxs
flux
(fg/
m2 /d
)
400 m
in situ production
0,00E+00
1,00E-05
2,00E-05
3,00E-05
4,00E-05
5,00E-05
6,00E-05
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
23
0T
h/2
32T
h (a
tom
ic r
atio
)
400 m
1000 m
suspended particles collected between 400 m and 1000 m
dissolved + particulate 230Thxs (fg/kg )
-1200
-1000
-800
-600
-400
-200
0
0 1 2 3 4 5 6 7
Dep
th (
m)
Pomme1 Pomme 2 Pomme 3
T
H
H THT T
H
T
H
H TH THTHT
Constraining the seasonal particle flux in the eastern North Atlantic with Thorium isotopes
M. Roy-Barman (1), R. El Hayek (1), I. Voege (2), M.Souhaut (3), N. Leblond (4), C. Jeandel (2).(1) LSCE, Avenue de la Terrasse, 91198 Gif sur Yvette, France, (2) AWI, PO Box 120161, 27515 Bremerhaven, Germany, (3) LEGOS, 14 Avenue E. Belin, 31400, Toulouse France, (4) LOV, BP 28, 06234 Villefranche sur mer, France
[email protected]: Constraining the present and past oceanic biological pump requires a good understanding of the marine particle dynamics and of their interaction with the surrounding water column. Particle fluxes are studied mainly with sediment traps, so that it is critical to evaluate their efficiency. The average efficiency of moored sediment traps is calibrated by the 230Th method. 230Th is produced uniformely in the ocean by radioactive decay of 238U and it is rapidely removed from the water column by scavenging on settling particles. The trapping efficiency is obtained by comparing the 230Thxs trapped flux with the 230Th production in the
overlying watercolumn. This was previously done with trap data obtained over a year in order to avoid the problem of estimating the change of 230Th inventory in the water column. The idea: Here we propose to extend this method to estimate the efficiency of moored traps on a seasonal scale. It requires high precision data to measure the change of 230Th inventory in the water column. By combining sediment trap data with the change of 230Th inventory, it is possible to obtain the trapping efficiency for a short time period.
Water column results: While the 230Thxs decreases in the surface waters from POMME 1 to
POMME 3, there is a significant increase of 230Thxs in the deep waters that cannot be solely due
to the remineralisation of the settling particles. The increasing rate of the 230Thxs inventory
from 0 to 400 or 1000 m in larger than the in situ production rate suggesting that advective inputs of 230Th are significant. The effect of water mass mixing is supported by the correlation between the 230Thxs content and the salinity of the water masses at 1000 m .
Trapping efficiency: For short periods, the flux/production ratio (apparent efficiency) may be different from the trapping efficiency. However during a high flux period, when particulate export must dominate over in situ production, it provides an upper bound of the trapping efficiency. The uncertainties on the change of 230Thxs inventory are large so that the corrected
efficiencies are not well constrained. Negative efficiencies are found when the 230Thxs
inventory increases faster than the in situ production. If we neglect the effect water mass mixing, we can obtain a lower bound for the corrected trapping efficiency.
Conclusion: By comparing apparent and corrected trapping efficiencies, a good braketing of the trapping efficiency can be obtained (eg. at 1000 m between P 1 and P 2 or at 400 m between P 2 and P 3). An explicit treatment of the mixing effect is required to improve the the method.
Principle of the sediment trap calibration.
Sampling: During the POMME program, we have measured Thorium isotopes in seawater, small particles and large particles collected in early March 2001 (POMME 1), mid April 2001 (POMME 2) and September 2001 (POMME 3) in the eastern North Atlantic. Here, we report results obtained on large particles collected with moored sediment traps (at 400 and 1000 m) and dissolved and small particles samples collected between 10 and 1000 m in anticyclonic eddies closely associated to the sediment trap at the time of sampling. All these samples were analysed for 230Th and 232Th by ID-TIMS.
Trap results: During the spring bloom (from POMME 1 to POMME 2), strong variations of total mass flux and of the 230Thxs flux are recorded by the sediment traps. Over this period, the
trapped 230Thxs flux represents 125% of the overlying production at 400 m and 65% at 1000
m. From POMME 2 to POMME 3, the 230Thxs fluxes are more constant and they represent
30% of the overlying production only. Beside the trap calibration aspect, Th isotopes provide important information on the particle dynamics: the increase of 230Th/232Th ratio in the trapped material between 400 and 1000 m implies (independently of the flux data) that small particles have been aggregated to the sinking particles between these depths.
35,6
35,7
35,8
35,9
36
36,1
3 4 5 6 7
Pomme1
Pomme2
Pomme3
dissolved + particulate 230Thxs (fg/kg )
salin
ity
mixing trend
--> 230
Thxs in not controlled
by production-scavenging only
Problems… = trapping efficiency
230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
change of 230Th inventory in the water column
-Problems…
= trapping efficiency230Th productionabove the trap
230Th trapped flux
230Th fixed on particles 234U 230Th
change of 230Th inventory in the water column
-
Eddy structure of the sampling area (M. Assenbaum et al., 2003)
Sediment trap data
Water column data
POMME 1 POMME 2 POMME 2 POMME 3 400 m 1000 m 400 m 1000 m
230Thxs flux in sediment trap (fg/m2/d)
744 935 195 439
in situ production above the trap (fg/m2/d)
592 1479 592
1479
apparent trapping efficiency
126 % 63 % 30 % 31 %
Change of 230Thxs inventory (fg/m2/d)
- 231 ± 1500 + 5830 ± 6674 + 755 ± 591 + 2737 ± 1647
corrected trapping efficiency (fg/m2/d)
> 23 %
> 40 % > 7 % > 100 %
0
500
1000
1500
2000
2500
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
1000 m
230 T
hxs
flux
(fg
/m2 /d
)
in situ production
0
500
1000
1500
2000
2500
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
230 T
hxs
flux
(fg/
m2 /d
)
400 m
in situ production
0,00E+00
1,00E-05
2,00E-05
3,00E-05
4,00E-05
5,00E-05
6,00E-05
1/2/01 3/3/01 2/4/01 2/5/01 1/6/01 1/7/01 31/7/01 30/8/01 29/9/01
23
0T
h/2
32T
h (a
tom
ic r
atio
)
400 m
1000 m
suspended particles collected between 400 m and 1000 m