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Download (3398Kb) - ePrints Soton - University of Southampton

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which normal embryonic/larval development occurs, but by 1) adult temperature<br />

tolerances, 2) temperatures needed for growth or spawning, or 3) hydrographic<br />

features that limit larval settlement and juvenile survival.<br />

Data from experiments carried out by Tyler et al. (2000) showed that the<br />

embryonic and larval stages <strong>of</strong> the Antarctic echinoid Sterechinus neumayeri (Müller)<br />

are capable <strong>of</strong> surviving low temperatures in surface waters, but only tolerate higher<br />

pressures when water column temperatures are > 0° C. They infer that the larvae <strong>of</strong> S.<br />

neumayeri might be capable <strong>of</strong> penetrating the deep sea through the action <strong>of</strong><br />

formation <strong>of</strong> Antarctic Bottom Water in the Weddell Sea, since this pattern <strong>of</strong><br />

temperature increase is seen during deep water formation.<br />

Only one experiment has been carried out onto pressure tolerances <strong>of</strong> embryos<br />

the bathyal asteroid species Plutonaster bifrons (Wyville Thomson) (Young et al.<br />

1996a). The greatest percentage <strong>of</strong> embryos developing normally occurred at<br />

pressures equivalent to 2000 m depth, the depth at which the species is most common.<br />

No normal development occurred at a pressure corresponding to 3000 m depth.<br />

Therefore, embryonic tolerances could determine the bathymetric limits <strong>of</strong><br />

distribution for this species.<br />

5.2- Effect <strong>of</strong> hydrodynamic mechanisms on larval dispersal<br />

Developmental mode is not the only factor that might determine dispersal<br />

distance, but larval dispersal patterns depend also on hydrodynamic mechanisms and<br />

such mechanisms may be different in distinct regions. Therefore, larval dispersal<br />

patterns vary between populations according to the relative importance <strong>of</strong> water<br />

advection and diffusion at a local scale. The flow <strong>of</strong> water in the deep sea is still not<br />

fully understood compared to the surface circulation. Therefore, in most cases, it is<br />

95

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