TY - JOUR
T1 - Loop Current Eddy formation and baroclinic instability
AU - Donohue, K. A.
AU - Watts, D. R.
AU - Hamilton, P.
AU - Leben, R.
AU - Kennelly, M.
N1 - Funding Information:
The principal authors were supported by the Bureau of Ocean Energy Management (BOEM) through contract M08PC20043 with Leidos, Inc. (formerly Science Applications International Corporation, SAIC). The authors wish to thank Alexis Lugo-Fernandez, the contracting officer's representative for his enthusiastic support. The successful deployment and recovery of the array was due to the instrument development and careful preparation and planning by James Singer, Paul Blankinship, Erran Sousa, Stuart Bishop, Brian Roderick, Gary Savoie and Cathy Cippolla. R. Leben acknowledges support from BOEM contracts M08PC20043 and M10PC00112 to Leidos Corporation, and NASA Ocean Surface Topography Mission Science Team Grants NNX08AR60G and NNX13AH05G .
Publisher Copyright:
© 2016 Elsevier B.V.
PY - 2016/12/1
Y1 - 2016/12/1
N2 - The formation of three Loop Current Eddies, Ekman, Franklin, and Hadal, during the period April 2009 through November 2011 was observed by an array of moored current meters and bottom mounted pressure equipped inverted echo sounders. The array design, areal extent nominally 89° W to 85° W, 25° N to 27° N with 30–50 km mesoscale resolution, permits quantitative mapping of the regional circulation at all depths. During Loop Current Eddy detachment and formation events, a marked increase in deep eddy kinetic energy occurs coincident with the growth of a large-scale meander along the northern and eastern parts of the Loop Current. Deep eddies develop in a pattern where the deep fields were offset and leading upper meanders consistent with developing baroclinic instability. The interaction between the upper and deep fields is quantified by evaluating the mean eddy potential energy budget. Largest down-gradient heat fluxes are found along the eastern side of the Loop Current. Where strong, the horizontal down-gradient eddy heat flux (baroclinic conversion rate) nearly balances the vertical down-gradient eddy heat flux indicating that eddies extract available potential energy from the mean field and convert eddy potential energy to eddy kinetic energy.
AB - The formation of three Loop Current Eddies, Ekman, Franklin, and Hadal, during the period April 2009 through November 2011 was observed by an array of moored current meters and bottom mounted pressure equipped inverted echo sounders. The array design, areal extent nominally 89° W to 85° W, 25° N to 27° N with 30–50 km mesoscale resolution, permits quantitative mapping of the regional circulation at all depths. During Loop Current Eddy detachment and formation events, a marked increase in deep eddy kinetic energy occurs coincident with the growth of a large-scale meander along the northern and eastern parts of the Loop Current. Deep eddies develop in a pattern where the deep fields were offset and leading upper meanders consistent with developing baroclinic instability. The interaction between the upper and deep fields is quantified by evaluating the mean eddy potential energy budget. Largest down-gradient heat fluxes are found along the eastern side of the Loop Current. Where strong, the horizontal down-gradient eddy heat flux (baroclinic conversion rate) nearly balances the vertical down-gradient eddy heat flux indicating that eddies extract available potential energy from the mean field and convert eddy potential energy to eddy kinetic energy.
KW - Baroclinic instability
KW - Mesoscale Eddies
KW - Western boundary currents
UR - http://www.scopus.com/inward/record.url?scp=84962513889&partnerID=8YFLogxK
U2 - 10.1016/j.dynatmoce.2016.01.004
DO - 10.1016/j.dynatmoce.2016.01.004
M3 - Article
AN - SCOPUS:84962513889
SN - 0377-0265
VL - 76
SP - 195
EP - 216
JO - Dynamics of Atmospheres and Oceans
JF - Dynamics of Atmospheres and Oceans
ER -