2013
DOI: 10.1016/j.dsr2.2013.02.021
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Quasi-Lagrangian observations of the upper ocean response to wintertime forcing in the Gulf Stream

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Cited by 5 publications
(5 citation statements)
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“…Drifting spar buoys generally require less motion correction, experience less flow-distortion and place sensors above the difficult-to-resolve processes within the wave-boundary layer (Hara and Sullivan, 2015); all of which results in accurate direct flux estimates (Edson et al, 2013;Drennan et al, 2014). Another advantage of a Lagrangian measurement of the air-sea fluxes in combination with oceanic temperature and salinity is that, to the extent the drifter follows the mean mixed layer currents, an ocean heat budget assessment can be simplified by reducing the advective flux divergence contribution to the budget (e.g., Silverthorne and Toole, 2013). Thus the surface fluxes measured by a drifter can be more directly constrained by changes in the upper ocean heat or salt content, and more directly compared to one-dimensional ocean models to evaluate the effects of surface forcing on the upper ocean (e.g., du Penhoat et al, 2002).…”
Section: CMmentioning
confidence: 99%
“…Drifting spar buoys generally require less motion correction, experience less flow-distortion and place sensors above the difficult-to-resolve processes within the wave-boundary layer (Hara and Sullivan, 2015); all of which results in accurate direct flux estimates (Edson et al, 2013;Drennan et al, 2014). Another advantage of a Lagrangian measurement of the air-sea fluxes in combination with oceanic temperature and salinity is that, to the extent the drifter follows the mean mixed layer currents, an ocean heat budget assessment can be simplified by reducing the advective flux divergence contribution to the budget (e.g., Silverthorne and Toole, 2013). Thus the surface fluxes measured by a drifter can be more directly constrained by changes in the upper ocean heat or salt content, and more directly compared to one-dimensional ocean models to evaluate the effects of surface forcing on the upper ocean (e.g., du Penhoat et al, 2002).…”
Section: CMmentioning
confidence: 99%
“…This surface heat loss initiates strong convection in the Sargasso Sea, which can lead to mixed layer depths (MLD) of up to 500 m (Buckley et al., 2014; Rossby, 1999). Re‐stratification then preserves beneath the surface the 18 Degree Water formed in the early spring (Leetmaa, 1977; Mensa et al., 2013; Silverthorne & Toole, 2013). This deepening of the thermocline combined with an increase in meridional temperature gradients across the GS will have a significant influence on its baroclinic transport, given the thermal wind relation (Bane & Osgood, 1989; Kelly et al., 1996; Leetmaa, 1977; Sato & Rossby, 1995; S. Dong et al., 2007), see Section 2.2.…”
Section: Introductionmentioning
confidence: 99%
“…Strong heat losses, and associated buoyancy forcing, are often induced during widespread outbreaks of cold, continental air from the northeast of North America extending over the GS region (Bane & Osgood, 1989; Grossman & Betts, 1990; Joyce et al., 2009; Kelly et al., 2010; Ma et al., 2015). These losses are often the largest seen globally with extreme values sometimes exceeding 1,000 Wm −2 during an outbreak (Silverthorne & Toole, 2013). This surface heat loss initiates strong convection in the Sargasso Sea, which can lead to mixed layer depths (MLD) of up to 500 m (Buckley et al., 2014; Rossby, 1999).…”
Section: Introductionmentioning
confidence: 99%
“…The advection was particularly important in the convergence of warmer and saltier water in the formation region which changed the characteristics of the EDW in its early stages. Silverthorne and Toole () deployed quasi‐Lagrangian profilers in the GS region to observe changes in the heat storage in the upper ocean. During the winter the variations of heat storage in the mixed layer were dominated by forcing associated with the passage of severe storms.…”
Section: Introductionmentioning
confidence: 99%