Dissertation - HQ
Dissertation - HQ
Dissertation - HQ
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142 Oceanography vs. behaviour<br />
Simple Euler-forward<br />
advection is appropriate<br />
the steep topography of the island or the promontory would otherwise<br />
be smoothed). The time step of the biological model is 3 hours and the<br />
output of the ROMS is stored at the same frequency so no temporal<br />
interpolation is needed.<br />
Larvae are released all around the island and the promontory, 1 km<br />
away from the 10 m isobath. The spawning strategy of adults may<br />
influence where larvae are released and how they are initially advected.<br />
For example, some tropical marine fishes were observed to spawn near<br />
the surface when tides entrain eggs toward the open ocean 185 . While<br />
potentially important, these behaviours are very location-specific and<br />
require fine scale representations of the topography and currents near<br />
the coast. This model focuses on general mesoscale features and the<br />
configuration used in the ROMS does not resolve fine scale structures,<br />
so we are only interested in what happens once the first moments of<br />
dispersal are over, 1 km away from shore. From there on, particles are<br />
advected using a simple Euler forward scheme with a 3 h time step.<br />
Particles are active in this model and de-correlate from the flow at a<br />
rate very different from that of passive particles. Therefore elaborate<br />
Lagragian advection methods, which feature a fading memory of currents<br />
in a random flight scheme or parameterised diffusion in a random<br />
walk one for example, cannot be used (see section 1.4.5, page 35). Finer<br />
advection schemes (e.g. Runge-Kutta) or shorter time steps could be<br />
used, but end positions would still have to be brought back to grid<br />
nodes. Indeed, the optimisation is performed at those points only, and<br />
optimal decisions cannot be interpolated (see Note – Computer memory<br />
and speed, page 129).<br />
6.4.2 Continuous and quantitative description of swimming<br />
behaviour<br />
In this model, at each time step, larvae can choose between several<br />
swimming speeds, oriented toward twenty-five different directions<br />
homogeneously distributed in space. In addition, instead of a three<br />
step progress, as in section 6.3, the development of swimming speed is<br />
described in a continuous fashion. To model swimming continuously<br />
in time, the ontogeny of maximum sustainable swimming speed and of<br />
swimming endurance (i.e. of the energetics of swimming) have to be<br />
described. Unfortunately, there are still very few observations of those<br />
variables throughout the larval phase.<br />
Development of swimming abilities and temperature effects<br />
Continuous, almost<br />
linear, development<br />
of swimming speed<br />
During ontogeny, maximum swimming speed increases because of<br />
allometry: even with a constant speed in body length per second (bl s -1 ),<br />
the actual speed in cm s -1 increases as larvae grow. However, on top of<br />
that, fin and muscle develop and the speed in bl s -1 actually increases<br />
during larval life 95 . A handful of studies 56,57,60 described the evolution