M. Roybarman et al., TH-230-TH-232 SYSTEMATICS IN THE CENTRAL PACIFIC-OCEAN - THE SOURCES AND THE FATES OF THORIUM, Earth and planetary science letters, 139(3-4), 1996, pp. 351-363
Th-232 and Th-230 of unfiltered and filtered sea water samples were me
asured along a depth profile of the central Pacific Ocean using isotop
ic dilution and thermal ionization mass spectrometry. The Th-232 conce
ntration is rather constant from below 25 m down to over 2000 m (45-60
x 10(6) atom cm(-3)) and it then increases rapidly towards the bottom
(119-360 X 10(6) atom cm(-3) at 4000 m). The Th-230 concentration inc
reases linearly with depth from 3 X 10(3) atom cm(-3) at 25 m to 110 X
10(3) atom cm(-3) at 4000 m. The reproducibility of replicate analyse
s and the regularity of the profiles demonstrate the reliability of th
e procedure, However, some lack of reproducibility among different sam
ples from the same depth has to be explained by natural variability or
by contamination during sample collection. Due to the very low Th-232
concentrations and relatively high Th-230 concentrations, the Th-230/
Th-232 ratios can be as high as 1.6 X 10(-3). The ratio of the amount
of Th on particles (> 0.2 mu m) to the amount of Th in solution is sig
nificantly higher for Th-232 (approximate to 0.37) than for Th-230 (ap
proximate to 0.18). These data are interpreted in terms of a model tha
t specifically treats particle transport assuming local equilibrium be
tween particles and sea water. The relatively high Th-230 concentratio
ns and Th-230/Th-232 ratios measured at 25 m are consistent with a mix
ed layer of about 100 m. The linear increase in Th-230 with depth impl
ies that the effect of eddy diffusion is negligible for most of the wa
ter column over the Th removal time scale. This profile is consistent
with transport of Th-230 by reversible uptake on particles settling wi
th a constant velocity. The Th-232 data are inconsistent with this mod
el and they suggest that particles carrying Th-232 experience 70% of m
ass loss between the surface and 4000 m and must follow different tran
sport rules. This difference in the transport of Th-230 and Th-232 dem
onstrates the distinctive behavior of these isotopes during particle f
ormation and subsequent remineralization and repackaging in the water
column. Different speciation of Th-230 and Th-232 may be explained by
their distinctive sources in the ocean (as Th-230 is produced in solut
ion and Th-232 is carried by detrital material) and by their respectiv
e packaging mechanisms, which are not yet known.