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School of Engineering and Science - Jacobs University

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10 2 world seawater (x10 8 )<br />

sample/PAAS<br />

10 1<br />

10 0<br />

hydrogenetic Fe-Mn crust<br />

La Ce Pr Nd PmSm Eu Gd Tb Dy Y Ho Er Tm Yb Lu<br />

Figure 8. Comparison <strong>of</strong> REY patterns in average world seawater (data same as Fig. 4) <strong>and</strong> average<br />

(n=12) non-phosphatized hydrogenetic Fe-Mn crusts from the central Pacific Ocean (data from Bau et<br />

al., 1996). Note complementary Ce <strong>and</strong> Y anomalies between seawater <strong>and</strong> precipitated Fe-Mn oxide<br />

particles as represented by Fe-Mn crust.<br />

However, the strong positive Y anomaly observed in seawater results from particle<br />

surface complexation effects, as Y adsorbed to particle surfaces is bound less strongly<br />

than the lanthanide elements (e.g., Bau, 1999). The significant fractionation <strong>of</strong> both Y<br />

<strong>and</strong> Ce from the other REY in seawater due to processes occurring on particle surfaces<br />

is clearly evident in the REY patterns for hydrogenetic Fe-Mn crusts as shown in Figure<br />

8. This does not imply that hydrogenetic Fe-Mn crusts are solely responsible for these<br />

anomalies, as Ce <strong>and</strong> Y fractionation has been observed to develop as a function <strong>of</strong><br />

increasing salinity in estuaries (Lawrence <strong>and</strong> Kamber, 2006). It therefore appears that<br />

significant Ce <strong>and</strong> Y anomalies begin to form during mixing <strong>of</strong> river waters <strong>and</strong><br />

seawater, <strong>and</strong> may be present in the truly dissolved REY fraction <strong>of</strong> river waters (Byrne<br />

<strong>and</strong> Liu, 1998).<br />

Of the remaining REY, La, Gd, <strong>and</strong> Lu display anomalous behavior in seawater to<br />

varying degrees. Strong positive La anomalies are typical <strong>of</strong> seawater, though this<br />

17

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