1995
DOI: 10.1029/94jc02509
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Thermal evolution of the Greenland Sea Gyre in 1988–1989

Abstract: Slice inverses of temperature and heat content from the 1988–1989 Greenland Sea Tomography experiment and other observations, including standard conductivity‐temperature‐depth stations, moored thermistors, surface meteorological variables, and surface ice cover are combined to better understand the thermodynamics of the Greenland Sea Gyre. Thermal evolution of the gyre center seems to divide naturally into the following three periods: a preconditioning phase (November–January), during which surface salinity is… Show more

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Cited by 21 publications
(9 citation statements)
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“…Intermediate convection down to 1500 m depth occurred in early March [GSP Group, 1990], and later on, rapid restratification was seen, as a series of warm and cold water masses encountered the mooring with a general warming trend. Note that this general picture was also seen in the slice inversion from the tomographic array [Greenland Sea Tornography Group, 1993; Pawlowicz et al, 1995] and hence seems to be characteristic for a larger region within the center of the Greenland Sea gyre.…”
Section: Thermal Stratificationmentioning
confidence: 99%
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“…Intermediate convection down to 1500 m depth occurred in early March [GSP Group, 1990], and later on, rapid restratification was seen, as a series of warm and cold water masses encountered the mooring with a general warming trend. Note that this general picture was also seen in the slice inversion from the tomographic array [Greenland Sea Tornography Group, 1993; Pawlowicz et al, 1995] and hence seems to be characteristic for a larger region within the center of the Greenland Sea gyre.…”
Section: Thermal Stratificationmentioning
confidence: 99%
“…These signals sug gest that mesoscale eddies, maybe generated around the con vective region as a consequence of the deep mixing (Gascard, 1978), were penetrating into the region. Moreover, the heat budget considerations from Pawlowicz et al (1995], which show a significant mismatch between the tomographically measured heat content and the integrated surface heat loss during March-April 1989, suggest that strong lateral mixing was tak ing place after the intensive mixing phase of early March 1989. During the previous month both estimates track quite nicely, which is consistent with a one-dimensional evolution.…”
Section: (A) Surface Heat Flux (Solid Line) Heat Of Fusion (Dashed Lmentioning
confidence: 99%
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“…In order to understand how the system presently works, it is necessary to analyze observational data carefully in order to determine basic parameters like the basin‐wide convection depths and to refer to clear criteria for these estimates. Although convection processes are studied by a variety of means (tomography arrays [ Worcester et al , 1993; Pawlowicz et al , 1995; Morawitz et al , 1996; Sutton et al , 1997], moorings equipped with ADCPs [ Schott et al , 1993], winter ship campaigns, and artificial tracer injection [ Watson et al , 1999]), a time series of winter convection relies on summer data as the majority of data are collected during summer. Winter cruises investigate the convection process itself more directly but normally do not detect the maximum ventilation depth unless one is certain to have observed the very last convection event.…”
Section: Introductionmentioning
confidence: 99%
“…In the Western Mediterranean Sea, the ninemonths-long experiment THETIS-2 (Send et al, 1997) has estimated the seasonal heat budget, but this experience remains an unicum among tomographic Mediterranean basinscale studies. Convective events have been successfully obCorrespondence to: S. Salon (ssalon@ogs.trieste.it) served in the northwestern Mediterranean (Send et al, 1995) and in the Greenland Sea (Pawlowicz et al, 1995;Morawitz et al, 1996). Ocean acoustic tomography has also proved to be a methodology for the observation of currents and internal tides (Shang and Wang, 1994;Demoulin et al, 1997).…”
Section: Introductionmentioning
confidence: 99%