A NEW APROACH TO STIRRING
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A NEW APROACH TO STIRRING. mesoscale + Time variability. sub-mesoéchelle. Méthod: compute Lyapono exonent. ► localisation of filaments ► stirring intensity. d'Ovidio et al., GRL, 2004. First application to satellitte observations. Chlorophyl filaments (res. 1 km) and lyaponov eponnts.

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A new aproach to stirring

A NEW APROACH TO STIRRING

mesoscale

+

Time variability

sub-mesoéchelle

Méthod: compute Lyapono exonent

► localisation of filaments

► stirring intensity

d'Ovidio et al., GRL, 2004

First application to satellitte observations

Chlorophyl filaments (res. 1 km) and lyaponov eponnts

Lehahn, d'Ovidio, et al., JGR, 2007


A new aproach to stirring

Altimetry-derived unstable manifolds

(spatial+temporal variability)

vs. chlorophyll pattern

Altimetric velocities vs. chlorophyll pattern

The agreement seems to hold at scales larger than altimetric resolution (>1/3 deg.) and not below.

Submesoscale tracer filaments are predicted from altimetry!


A new aproach to stirring

The intensity of stirring can be measured with local Lyapunov Exponents

= initial separation

= amplification factor

= time needed for the perturbation to grow

Aurell et al., Phys. Rev. Lett. 77, 1262 (1996)

Boffetta et al., J. of Phys. A, 30, 1 (1997) chao-dyn/9904049



A new aproach to stirring

How is stirring affected by degrading in space and time

the velocity field?

Method: 2km-reolution model : SST

3000 km x 2000 km


A new aproach to stirring

PRELIMINARY RESULTS

Current altimetry products

8 days

6 days

4 days

2 days

Mean comparison (400x400 km):

Smoother behaviour (temporal variability less important)

Pixel-by-pixel comparison:

space variability dominates >16 km

time variability dominates below

the reduced resolution underestimates stirring (up to 50%)

critical resolution associated to filament position (<-visible in

pixel by pixel comparison, not on regional means)


A new aproach to stirring

SUMMARY

Stirring is an important (main?) effect of the horizontal velocities at the submesoscale.

It depends on both the spatial and temporal variability of the velocity field.

Its quantification through the Lyapunov Exponent is a natural and objective way of quantifying the error when reducing the spatial and/or temporal resolution of a velocity field.

An analysis performed with the high resolution model GYRE suggests that, starting from current altimetry resolution, the highest gain is obtained increasing the spatial resolution up to 16 km. After that, temporal resolution should be increased.

Time resolutiion appears to be critical for filament position not stirring intensity

In general, a reduced resolution underestimates stirring intensity (up to 50%).

The analysis should be repeated resampling the model SSH over simulated (multi-)satellite tracks.



A new aproach to stirring

We are re-processing the entire altimetric dataset processes

15 years, global coverage; near-real time analysis possible


A new aproach to stirring

2003-2006 average: patterns correlated to Eulerian diagnostics (EKE, etc.)

day-1

0.5

0

stirring (Lyapunov exponents)


A new aproach to stirring

2003-2006 average (no time variability): we compute stirring rates also at frozen velocity fields.

day-1

0.5

0

“frozen” stirring (Lyap. exp. from frozen velocity field)


A new aproach to stirring

The difference between stirring and stirring with frozen velocities unveil the role of time variability for mesoscale

dispersion processes.

2003-2006 average (fraction of stirring due to time variability)

1

0

(stirring-(frozen stirring))/stirring


A new aproach to stirring

2003-2006 average (fraction of stirring due to time variability)

In the case of strong currents, like the Gulf stream, stirring processes are dominated by persistent jets and weakly affected by mesoscale time variability.

On the contrary, the weaker stirring occurring in the subtropical gyres is easily affected by mesoscale time variability.

In the subpolar regions mesoscale time variability has also a strong effect, by breaking the “trapping” effect of stationary eddies. This is shown by very localized mesoscale signal in correspondance of the cores of the most stationary eddies.

Note the colorscale: in same cases, the time variability is responsable of almost all (~1) the stirring!

1

0

(stirring-(frozen stirring))/stirring


A new aproach to stirring

CONCLUSION (Time variability of the ocean currents: the role of chaos)

The time variability of surface currents (in fact, chaos) has a strong effect outside permanent jets, especially in supolar regions and inside the subtropical gyres.

These regions are likely to be the ones that will most benefit from next-generation altimetry data at improved temporal resolution.

For high-resolution circulation models, these are also the regions where small-scale transport crucially depends on a correct representation of eddy temporal dynamics.

In these regions, a wrong temporal variability of eddies corresponds to wrong mesoscale dispersion even if the EKE distribution is perfect.

A dynamical interpretation

A two-dimensional system with no time dependence has no chaos: trajectories (and fronts) follow altimetric isolines. In this case, eddies are perfectly isolated from outside. In this case, Lyapunov exponents measure basically the strain. The temporal variability has the main effect of breaking the closed orbits, creating spirals and filaments that connect the eddy interior with the environment. This chaotic dynamics adds to the strain contributing to the stirring.