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Submesoscale Currents in the Atlantic. Jeroen Molemaker, Jim McWilliams, Jonathan Gula, Florian Lemarie, Alexander Shchepetkin UCLA. Characteristics of submesoscale. Middle sized: L = 10 m-10s km, t = hrs - days. Rotating, stratified dynamics, mostly not waves.
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Submesoscale Currentsin the Atlantic • Jeroen Molemaker, • Jim McWilliams, Jonathan Gula, Florian Lemarie, • Alexander Shchepetkin • UCLA
Characteristics of submesoscale • Middle sized: L = 10 m-10s km, t = hrs - days. • Rotating, stratified dynamics, mostly not waves. • Geostrophic dynamics are relaxed. • Arising out of mesoscale currents. • Disappearing into micro-scale mixing and dissipation
Sources of submesoscale energy • Mixed layer baroclinic instabilities • Horizontal/Vertical shear • Interaction between straining and density gradients • One instability can lead to the next.
Gulf Stream (dx = 5-7 km) Many subsequent nested solutions Improved through reduced diapycnal mixing Marchesiello (2010), Lemarie etal. (2012) Rio
Examples of validation AVISO ROMS – ATLBIG (5-7km)
Surface current Magenta lines are 0.3 m/s contour level of AVISO surface geostrophic velocities Mean path of the Gulf Stream
SSH variability – AVISO SSH variability – ROMS
Nest level 1 South West Atlantic (dx = 1.5 km, 1500km x 2000km) Submesoscale on top of mesoscale
Back to submesoscale dynamics • Submesoscale range often start with mixed layer instability • Source is potential energy. • Deep mixed layer or strong horizontal density gradients
Mixed layer depth Summer Winter
Summer Winter
Surface Relative Vorticity (dx = 1.5 km)
Relative Vorticity: PDF Summer Winter Text Blue: Surface, Red: -100 meter
Cold-core cyclonic eddy with sub-mesoscale features
Relative vorticity (Ro > 4) Velocity amplitude
Surface relative vorticity [-3f, 3f] Rio, dx = 500 m)
Surface horizontal divergence [-3f, 3f] (Rio, dx = 500 m)
50km x 40 km dx = 180 m