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Although larval dispersal and settlement <strong>of</strong> this species are apparently hydrodynamic<br />
constrained in almost all populations larval retention appeared to be sufficient to<br />
ensure local recruitment, in spite <strong>of</strong> short larval life span and/or meteorological<br />
conditions. Whereas some populations were mainly self–seeding, larval supply from<br />
neighbouring populations could exceed local retention for other populations<br />
depending on wind forcing.<br />
The flow <strong>of</strong> water in the deep sea is still not fully understood compared to the<br />
surface circulation. Therefore, in most cases, it is not an easy task to predict where<br />
larvae released at a particular location will go and how long the journey will take.<br />
Marsh et al. (2001) studied the larval dispersal potential <strong>of</strong> the tube worm Riftia<br />
pachyptila at deep sea hydrothermal vents on the East Pacific Rise. They showed the<br />
prevailing importance <strong>of</strong> current flow in determining dispersal potential and suggested<br />
that populations at different vent sites may have different dispersal limits depending<br />
on local current conditions. In this region at least, it is apparent that the dispersal<br />
distance <strong>of</strong> R. pachyptila was not limited by the physiological performance <strong>of</strong> the<br />
larvae, but by 1) temporal oscillations in the long axis currents and 2) larval loss in<br />
cross-axis flows.<br />
Global termohaline circulation occurs by a variety <strong>of</strong> pathways that transport<br />
warm waters to high latitudes where they become denser, sink, and finally spread<br />
throughout the oceanic floor (Smethie et al., 2000). One <strong>of</strong> the most important<br />
pathways by which this process occurs is the formation and spreading <strong>of</strong> North<br />
Atlantic Deep Water (NADW). The extension <strong>of</strong> its influence on the deep-ocean<br />
circulation can be measured as the properties <strong>of</strong> this water mass have been observed<br />
throughout much <strong>of</strong> the deep ocean and it may extend as far as the North Pacific (Reid<br />
& Lynn, 1971).<br />
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