On the equilibration of a symmetrically unstable front via a secondary shear instability
By John R. Taylor, Raffaele Ferrari. Journal of Fluid Mechanics, 2009
146 citations recorded by the source corpus.
Subfields: Atmospheric Science, Global and Planetary Change, Oceanography
View Paper: https://www.semanticscholar.org/paper/3f7e04e190c1d5cc7da14a5e68cd40dadf71abe5
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Atmospheric Science
- Raffaele Ferrari
- Robert Hallberg
- S. Griffies
- B. Fox‐Kemper
- James C. McWilliams
- Gokhan Danabasoglu
- A. N. Garabato
- John R. Taylor
In Global and Planetary Change
- Raffaele Ferrari
- S. Griffies
- Robert Hallberg
- James C. McWilliams
- B. Fox‐Kemper
- Gokhan Danabasoglu
- A. N. Garabato
- Mathew E. Maltrud
In Oceanography
- Raffaele Ferrari
- Robert Hallberg
- B. Fox‐Kemper
- S. Griffies
- James C. McWilliams
- Gokhan Danabasoglu
- A. N. Garabato
- Mathew E. Maltrud
Citations in the corpus
- Parameterization of mixed layer eddies. III: Implementation and impact in global ocean climate simulations (2010, background): “submesoscale parameterization and the implementation of GM90 according to Treguier et al. (1997) (see Appendix A).”
- Buoyancy and Wind-Driven Convection at Mixed Layer Density Fronts (2010, methodology): “Qualitatively, this is very similar to the symmetrically unstable front described by Taylor and Ferrari (2009). c. PV budget In upright convection, when M2 5 0, the mean buoyancy equation is decoupled from the equations for the mean horizontal velocity, and Eq.”
- Open-Ocean Submesoscale Motions: A Full Seasonal Cycle of Mixed Layer Instabilities from Gliders (2016, background): “surface buoyancy forcing (Thomas 2005), symmetric instability (SI; Taylor and Ferrari 2009; Thomas et al. 2013), and mixed layer baroclinic instability (BCI; Boccaletti et al.”
- Submesoscale currents in the ocean (2016, background): “GI and CI are well-known processes, and both have finite-amplitude forward energy cascade and dissipation; they are particularly apt in the weakly (or negatively) stratified SBL [56,67].”