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  • Spall, Michael A.  (14)
  • 1
    Online-Ressource
    Online-Ressource
    American Meteorological Society ; 2015
    In:  Journal of Physical Oceanography Vol. 45, No. 11 ( 2015-11), p. 2806-2819
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 45, No. 11 ( 2015-11), p. 2806-2819
    Kurzfassung: An eastward-flowing current of a homogeneous fluid with velocity U , contained in a channel of width L , impinges on an island of width of O ( L ), and the resulting interaction and dynamics are studied for values of the supercriticality parameter, b = βL 2 / U , both larger and smaller than π 2 . The former case is subcritical with respect to Rossby waves, and the latter is supercritical. The nature of the flow field depends strongly on b , and in particular, the nature of the flow around the island and the proportion of the flow passing to the north or south of the island are sensitive to b and to the position of the island in the channel. The problem is studied analytically in a relatively simple, nonlinear quasigeostrophic and adiabatic framework and numerically with a shallow-water model that allows a qualitative extension of the results to the equator. Although the issues involved are motivated by the interaction of the Equatorial Undercurrent and the Galapagos Islands, the analysis presented here focuses on the fundamental issue of the distinctive nature of the flow as a function of Rossby wave criticality.
    Materialart: Online-Ressource
    ISSN: 0022-3670 , 1520-0485
    Sprache: Unbekannt
    Verlag: American Meteorological Society
    Publikationsdatum: 2015
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 2
    Online-Ressource
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    American Meteorological Society ; 2005
    In:  Journal of Physical Oceanography Vol. 35, No. 3 ( 2005-03-01), p. 363-373
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 35, No. 3 ( 2005-03-01), p. 363-373
    Kurzfassung: The interaction of equatorial Rossby waves with a western boundary perforated with one or more narrow gaps is investigated using a shallow-water numerical model and supporting theory. It is found that very little of the incident energy flux is reflected into eastward-propagating equatorial Kelvin waves provided that at least one gap is located within approximately a deformation radius of the equator. Because of the circulation theorem around an island, the existence of a second gap off the equator reduces the reflection of short Rossby waves and enhances the transmission of the incident energy into the western basin. The westward energy transmitted past the easternmost island is further reduced upon encountering islands to the west, even if these islands are located entirely within the “shadow” of the easternmost island. A localized patch of wind forcing was also used to generate low-frequency Rossby waves for cases with island configurations representative of the western equatorial Pacific. For both idealized islands and a coastline based on the 200-m isobath, the amount of incident energy reflected into Kelvin waves depends on both the duration of the wind event and the meridional decay scale of the anomalous winds. For wind events of 2-yr duration with a meridional decay scale of 700 km, the reflected energy is 37% of the incident flux, and the energy transmitted into the Indian Ocean is approximately 10% of the incident flux, very close to that predicted by previous theories. For shorter wind events or winds confined more closely to the equator the reflected energy is significantly less.
    Materialart: Online-Ressource
    ISSN: 1520-0485 , 0022-3670
    Sprache: Englisch
    Verlag: American Meteorological Society
    Publikationsdatum: 2005
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 3
    Online-Ressource
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    American Meteorological Society ; 2005
    In:  Journal of Physical Oceanography Vol. 35, No. 12 ( 2005-12-01), p. 2487-2500
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 35, No. 12 ( 2005-12-01), p. 2487-2500
    Kurzfassung: The buoyancy-driven circulation of simple two-layer models on the β plane is studied in order to examine the role of beta in determining the magnitude and structure of the vertical motions forced in response to surface heating and cooling. Both analytical and numerical approaches are used to describe the change in circulation pattern and strength as a consequence of the planetary vorticity gradient. The physics is quasigeostrophic at lowest order but is sensitive to small nonquasigeostrophic mass fluxes across the boundary of the basin. The height of the interface between the two layers serves as an analog of temperature, and the vertical velocity at the interface consists of a cross-isopycnal velocity, modeled in terms of a relaxation to a prescribed interface height, as well as an adiabatic representation of eddy thickness fluxes parameterized as lateral diffusion of interface displacement. In the numerical model the lateral eddy diffusion of heat is explicitly represented by a resolved eddy field. In the plausibly more realistic case, when the lateral diffusion of buoyancy dominates the diffusion of momentum, the major vertical velocities occur at the boundary of the basin as in earlier f-plane studies. The effect of the planetary vorticity gradient is to intensify the sinking at the western wall and to enhance the magnitude of that sinking with respect to the f-plane models. The vertical mass flux in the Sverdrup interior exactly balances the vertical flux in the region of the strong horizontal transport of the western boundary current, leaving the net flux to occur in a very narrow region near the western boundary tucked well within the western boundary current. On the other hand, if the lateral diffusion of heat is arbitrarily and unrealistically eliminated, the vertical mass flux is forced to occur in the interior. The circulation pattern is extremely sensitive to small net inflows or outflows across the basin perimeter. The cross-basin flux determines the interface height on the basin’s eastern boundary and affects the circulation pattern across the entire basin.
    Materialart: Online-Ressource
    ISSN: 1520-0485 , 0022-3670
    Sprache: Englisch
    Verlag: American Meteorological Society
    Publikationsdatum: 2005
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 4
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    Journal of Marine Research/Yale ; 2011
    In:  Journal of Marine Research Vol. 69, No. 2 ( 2011-03-01), p. 347-382
    In: Journal of Marine Research, Journal of Marine Research/Yale, Vol. 69, No. 2 ( 2011-03-01), p. 347-382
    Materialart: Online-Ressource
    ISSN: 0022-2402
    Sprache: Englisch
    Verlag: Journal of Marine Research/Yale
    Publikationsdatum: 2011
    ZDB Id: 410655-6
    ZDB Id: 2066603-2
    SSG: 12
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 5
    Online-Ressource
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    Journal of Marine Research/Yale ; 1997
    In:  Journal of Marine Research Vol. 55, No. 6 ( 1997-11-01), p. 1199-1251
    In: Journal of Marine Research, Journal of Marine Research/Yale, Vol. 55, No. 6 ( 1997-11-01), p. 1199-1251
    Materialart: Online-Ressource
    ISSN: 0022-2402 , 1543-9542
    Sprache: Englisch
    Verlag: Journal of Marine Research/Yale
    Publikationsdatum: 1997
    ZDB Id: 410655-6
    ZDB Id: 2066603-2
    SSG: 12
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 6
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    American Meteorological Society ; 2013
    In:  Journal of Physical Oceanography Vol. 43, No. 5 ( 2013-05-01), p. 1028-1041
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 43, No. 5 ( 2013-05-01), p. 1028-1041
    Kurzfassung: The circulation induced by the interaction of surface Ekman transport with an island is considered using both numerical models and linear theory. The basic response is similar to that found for the interaction of Ekman layers and an infinite boundary, namely downwelling (upwelling) in narrow boundary layers and deformation-scale baroclinic boundary layers with associated strong geostrophic flows. The presence of the island boundary, however, allows the pressure signal to propagate around the island so that the regions of upwelling and downwelling are dynamically connected. In the absence of stratification the island acts as an effective barrier to the Ekman transport. The presence of stratification supports baroclinic boundary currents that provide an advective pathway from one side of the island to the other. The resulting steady circulation is quite complex. Near the island, both geostrophic and ageostrophic velocity components are typically large. The density anomaly is maximum below the surface and, for positive wind stress, exhibits an anticyclonic phase rotation with depth (direction of Kelvin wave propagation) such that anomalously warm water can lie below regions of Ekman upwelling. The horizontal and vertical velocities exhibit similar phase changes with depth. The addition of a sloping bottom can act to shield the deep return flow from interacting with the island and providing mass transport into/out of the surface Ekman layer. In these cases, the required transport is provided by a pair of recirculation gyres that connect the narrow upwelling/downwelling boundary layers on the eastern and western sides of the island, thus directly connecting the Ekman transport across the island.
    Materialart: Online-Ressource
    ISSN: 0022-3670 , 1520-0485
    Sprache: Englisch
    Verlag: American Meteorological Society
    Publikationsdatum: 2013
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 7
    Online-Ressource
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    American Meteorological Society ; 2018
    In:  Journal of Physical Oceanography Vol. 48, No. 1 ( 2018-01), p. 163-174
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 48, No. 1 ( 2018-01), p. 163-174
    Kurzfassung: The general problem of exchange from a shallow shelf across sharp topography to the deep ocean forced by narrow, cross-shelf wind jets is studied using quasigeostrophic theory and an idealized primitive equation numerical model. Interest is motivated by katabatic winds that emanate from narrow fjords in southeast Greenland, although similar topographically constrained wind jets are found throughout the world’s oceans. Because there is no net vorticity input by the wind, the circulation is largely confined to the region near the forcing. Circulation over the shelf is limited by bottom friction for weakly stratified flows, but stratification allows for much stronger upper-layer flows that are regulated by weak coupling to the lower layer. Over the sloping topography, the topographic beta effect limits the deep flow, while, for sufficient stratification, the upper-layer flow can cross the topography to connect the shelf to the open ocean. This can be an effective transport mechanism even for short, strong wind events because damping of the upper-layer flow is weak. A variety of transients are generated for an abrupt onset of winds, including short topography Rossby waves, long topographic Rossby waves, and inertial waves. Using parameters representative of southeast Greenland, katabatic wind events will force an offshore transport of O (0.4) Sv (1 Sv ≡ 10 6 m 3 s −1 ) that, when considered for 2 days, will result in an offshore flux of O (5 × 10 10 ) m 3 .
    Materialart: Online-Ressource
    ISSN: 0022-3670 , 1520-0485
    Sprache: Unbekannt
    Verlag: American Meteorological Society
    Publikationsdatum: 2018
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 8
    Online-Ressource
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    American Meteorological Society ; 2008
    In:  Journal of Physical Oceanography Vol. 38, No. 10 ( 2008-10-01), p. 2294-2307
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 38, No. 10 ( 2008-10-01), p. 2294-2307
    Kurzfassung: A linear stability analysis of a meridional boundary current on the beta plane is presented. The boundary current is idealized as a constant-speed meridional jet adjacent to a semi-infinite motionless far field. The far-field region can be situated either on the eastern or the western side of the jet, representing a western or an eastern boundary current, respectively. It is found that when unstable, the meridional boundary current generates temporally growing propagating waves that transport energy away from the locally unstable region toward the neutral far field. This is the so-called radiating instability and is found in both barotropic and two-layer baroclinic configurations. A second but important conclusion concerns the differences in the stability properties of eastern and western boundary currents. An eastern boundary current supports a greater number of radiating modes over a wider range of meridional wavenumbers. It generates waves with amplitude envelopes that decay slowly with distance from the current. The radiating waves tend to have an asymmetrical horizontal structure—they are much longer in the zonal direction than in the meridional, a consequence of which is that unstable eastern boundary currents, unlike western boundary currents, have the potential to act as a source of zonal jets for the interior of the ocean.
    Materialart: Online-Ressource
    ISSN: 1520-0485 , 0022-3670
    Sprache: Englisch
    Verlag: American Meteorological Society
    Publikationsdatum: 2008
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 9
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    American Meteorological Society ; 2017
    In:  Journal of Physical Oceanography Vol. 47, No. 9 ( 2017-09), p. 2251-2265
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 47, No. 9 ( 2017-09), p. 2251-2265
    Kurzfassung: The problem of localized dense water formation over a sloping bottom is considered for the general case in which the topography forms a closed contour. This class of problems is motivated by topography around islands or shallow shoals in which convection resulting from brine rejection or surface heat loss reaches the bottom. The focus of this study is on the large-scale circulation that is forced far from the region of surface forcing. The authors find that a cyclonic current is generated around the topography, in the opposite sense to the propagation of the dense water plume. In physical terms, this current results from the propagation of low sea surface height from the region of dense water formation anticyclonically along the topographic contours back to the formation region. This pressure gradient is then balanced by a cyclonic geostrophic flow. This basic structure is well predicted by a linear quasigeostrophic theory, a primitive equation model, and in rotating tank experiments. For sufficiently strong forcing, the anticyclonic circulation of the dense plume meets this cyclonic circulation to produce a sharp front and offshore advection of dense water at the bottom and buoyant water at the surface. This nonlinear limit is demonstrated in both the primitive equation model and in the tank experiments.
    Materialart: Online-Ressource
    ISSN: 0022-3670 , 1520-0485
    Sprache: Unbekannt
    Verlag: American Meteorological Society
    Publikationsdatum: 2017
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 10
    Online-Ressource
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    American Meteorological Society ; 2008
    In:  Journal of Physical Oceanography Vol. 38, No. 6 ( 2008-06-01), p. 1267-1277
    In: Journal of Physical Oceanography, American Meteorological Society, Vol. 38, No. 6 ( 2008-06-01), p. 1267-1277
    Kurzfassung: A two-layer quasigeostrophic model in a channel is used to study the influence of lateral displacements of regions of different sign mean potential vorticity gradient (Πy) on the growth rate and structure of linearly unstable waves. The mean state is very idealized, with a region of positive Πy in the upper layer and a region of negative Πy in the lower layer; elsewhere Πy is zero. The growth rate and structure of the model’s unstable waves are quite sensitive to the amount of overlap between the two regions. For large amounts of overlap (more than several internal deformation radii), the channel modes described by Phillips’ model are recovered. The growth rate decreases abruptly as the amount of overlap decreases below the internal deformation radius. However, unstable modes are also found for cases in which the two nonzero Πy regions are separated far apart. In these cases, the wavenumber of the unstable waves decreases such that the aspect ratio of the wave remains O(1). The waves are characterized by a large-scale barotropic component that has maximum amplitude near one boundary but extends all the way across the channel to the opposite boundary. Near the boundaries, the wave is of mixed barotropic–baroclinic structure with cross-front scales on the order of the internal deformation radius. The perturbation heat flux is concentrated near the nonzero Πy regions, but the perturbation momentum flux extends all the way across the channel. The perturbation fluxes act to reduce the isopycnal slopes near the channel boundaries and to transmit zonal momentum from the region of Πy & gt; 0 to the region on the opposite side of the channel where Πy & lt; 0. These nonzero perturbation momentum fluxes are found even for a mean state that has no lateral shear in the velocity field.
    Materialart: Online-Ressource
    ISSN: 1520-0485 , 0022-3670
    Sprache: Englisch
    Verlag: American Meteorological Society
    Publikationsdatum: 2008
    ZDB Id: 2042184-9
    ZDB Id: 184162-2
    Standort Signatur Einschränkungen Verfügbarkeit
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