INTERNAL TIDES IN AUTUMN. TIME/SPACE MOVIES
The M2 internal tide evolution in the Bay of Biscay is
shown here by several movies.
The animations are displayed on the zoom area in white,
plotted on the following figure.
The view point is from the North-West direction.

In the movies, - the French continental slope is
on the left,
- the Spanish continental slope is on the right.
To go on the movie click on the picture.
To go out close the movie window.
More informations
on the model.
Transient state: Spatial Evolution of the North-south baroclinic current after 1 lunar day
MICOM model calculates the evolution of the baroclinic
variables (current and thickness of the different layers) from initial
conditions corresponding to null baroclinic currents and flat thickness
on the horizontal plane (see
3D Micom results). These two movies present the transient state
when the internal tidal wave and associated baroclinic currents are generated.
These one show the different generation areas and the different direction
of propagation of the wave.
Two main sections are shown :
- Movie 1, the evolution of the North-South baroclinic
current on the horizontal plane, in the first layer.
- Movie 2, the evolution of the North-South baroclinic
current on a vertical section defined by a dotted line on
the movie 1.
The different views correspond to the spatial evolution
at the following lunar days: 1-2-4-6-8-10-12-14-16-18-20, the transient
state being defined by the five first steps.
- Step 1 Day 1: One can see the generation area over the French continental slope with two maxima of current on each side of the shelf break , i.e over the continental shelf and over the continental slope.
- Step 2 Day 2: On each side of the French shelf break,
it appears the internal tide wavelength defined by the seasonal thermocline
(the third mode named the "interfacial mode"). At the same time, on can
see a maximum in the current amplitude in the middle of the Bay of Biscay
: it is the fact of the first baroclinic mode defined by the deep ocean
stratification and which propagates more quickly than the third one.
At this time step, the internal tide energy mainly comes
from the French continental slope.
- Step 3 Day 3: Most of the first "deep ocean" baroclinic mode appears in the whole domain. One observe a maxima area of surface current close to the Iberic slope which corresponds to an internal tide coming from the Iberic slope along the second upward energetic ray.
- Step 5 Day 8: The internal tide energy of the first
modes is propagated on the whole domain. After this time step there
are only spatial adjustments in the current repartition due to the propagation
of the high baroclinic modes which have a weaker celerity than the first
ones.
On the vertical plane, we find again the well known repartition
of the internal tide energy along characteristic rays (defined by the stratification
and by the M2 tide frequency). The first mode (characterized by maxima
of currents near the bottom and near the sea surface) appears very
quickly (step 2, day 2), whereas the other one are all propagated only
after time step 5 (day 8). These vertical modes are charaterized by cores
of maximum of current along the rays.
Steady state: Spatial Evolution of the North-south baroclinic
current after 15 lunar days
animation on a tidal cycle
The same two main sections as hereabove are now displayed over one tidal cycle: each view corresponds to one "lunar" hour of the tidal cycle (12 steps).
- Movie 3, the evolution of the North-South baroclinic
current on the horizontal plane, in the first layer.
- Movie 4, the evolution of the North-South baroclinic
current on a vertical section defined by a dotted line on
the movie 1.


Steady state: Spatial Evolution of the North-south baroclinic
current after 15 lunar days.
Series of vertical sections perpendicular to the continental
slope.
The spatial evolution of the internal tide (North- south
baroclinic current) is now presented by successive vertical sections perpendicular
to the French continental slope, with the same orientation as hereabove.
The purpose is to explain the origin of the areas of maxima of surface
current one can see on the horizontal plane.
- Just in front of the view, there is a variation of the
bottom topography, which corresponds to a flat zone by about 2000m of water
depth and named the "plateau de Meriadzeck". For vertical sections coming
from this area, the bottom slope is lower than the characateristics slope,
and the first internal tide ray is an upward ray : it induces a maximum
of surface current (by 47.5N, 9W (see
3D Micom results, section 4)) closer to the French continental slope
than for the other sections, where the first ray is a downward ray.
- Then, there are two other energetic sections, with
maxima of surface current by 46.10N , 7.5W and 44.50N,
5.30 W (see 3D Micom
results): for these sections the bottom slope is upper than the one
of the characteristic rays, and therefore these maxima correpond to the
resurgence of the second ray.
Steady state: Spatial Evolution of the horizontal baroclinic current after 15 lunar days
The horizontal baroclinic vector is plotted here along
the most energetic vertical section, to show its evolution on a tidal cycle.
- The baroclinic current turns clockwise as the barotropic
tidal current over the French continental shelf.
- There are strong vertical shears of current which are
not at the same depth for the different points of this vertical section.
It is due to the particular propagation of the energy along the rays. Over
the plain, there are about two or three vertical shears on a vertical profile,
which show that the three first modes are preponderant.
- Above the French continental slope, on the third vertical
profile, there is an opposition in phase between the bottom and surface
currents. This shear has already been observed on data collected in this
area by doppler current meters (see
data collected in the Bay of Biscay, point PF06).