95 research outputs found
Critical effects of a tall seamount on a drifting vortex
The initial-value problem for the evolution of an isolated vortex encountering a tall seamount during its westward beta-drift is studied within an equivalent-barotropic model, that is generalized to allow for the intersection of the layer interface with a sloping bottom. Given the Rossby radius and linear wave speed in the model, the parabolic shape of a seamount top and initial potential vorticity profile in the vortex core, the outcome is controlled by the vortex sign and a number of parameters: the seamount radius and height of penetration into the active layer, the radius and intensity of the vortex, the initial offset of the vortex center relative to the seamount, the Ekman layer depth over the seamount top, and the momentum lateral diffusion coefficient. Here we consider regimes for narrow seamounts where cyclonic vorticity generated in the water column swept off the top of the seamount plays a negligible role. The most significant effect on the vortex evolution is provided by a topographically induced anti-cyclonic circulation that is formed after squashing of water column replaced over the top of the seamount by the approaching vortex. The Geostrophic Vorticity intermediate model is used for numerical experiments. When the area of penetration is small and the topographic anticyclone is weak, the vortex drifts either predominantly westward north of the seamount or rotates around the seamount which is explained by presence of a separatrix in a simple kinematic model. For a larger area of penetration and stronger topographic anticyclone, violent interactions result in substantial deformations of the vortex core and loss of the material from the vortex periphery that leads to anomalous transport and diffusion. Vortex capture over the seamount is found in one range of parameters
Stabilization of Isolated Vortices in a Rotating Stratified Fluid
The key element of Geophysical Fluid Dynamicsβreorganization of potential vorticity (PV) by nonlinear processesβis studied numerically for isolated vortices in a uniform environment. Many theoretical studies and laboratory experiments suggest that axisymmetric vortices with a Gaussian shape are not able to remain circular owing to the growth of small perturbations in the typical parameter range of abundant long-lived vortices. An example of vortex destabilization and the eventual formation of more intense self-propagating structures is presented using a 3D rotating stratified Boussinesq numerical model. The peak vorticity growth found during the stages of strong elongation and fragmentation is related to the transfer of available potential energy into kinetic energy of vortices. In order to develop a theoretical model of a stable circular vortex with a small Burger number compatible with observations, we suggest a simple stabilizing procedure involving the modification of peripheral PV gradients. The results have important implications for better understanding of real-ocean eddies
Modeling of composite beams and plates for static and dynamic analysis
The main purpose of this research was to develop a rigorous theory and corresponding computational algorithms for through-the-thickness analysis of composite plates. This type of analysis is needed in order to find the elastic stiffness constants for a plate and to post-process the resulting plate solution in order to find approximate three-dimensional displacement, strain, and stress distributions throughout the plate. This also requires the development of finite deformation plate equations which are compatible with the through-the-thickness analyses. After about one year's work, we settled on the variational-asymptotical method (VAM) as a suitable framework in which to solve these types of problems. VAM was applied to laminated plates with constant thickness in the work of Atilgan and Hodges. The corresponding geometrically nonlinear global deformation analysis of plates was developed by Hodges, Atilgan, and Danielson. A different application of VAM, along with numerical results, was obtained by Hodges, Lee, and Atilgan. An expanded version of this last paper was submitted for publication in the AIAA Journal
Test of Einstein Equivalence Principle for 0-spin and half-integer-spin atoms: Search for spin-gravity coupling effects
We report on a conceptually new test of the equivalence principle performed
by measuring the acceleration in Earth's gravity field of two isotopes of
strontium atoms, namely, the bosonic Sr isotope which has no spin vs the
fermionic Sr isotope which has a half-integer spin. The effect of
gravity upon the two atomic species has been probed by means of a precision
differential measurement of the Bloch frequency for the two atomic matter waves
in a vertical optical lattice. We obtain the values for the E\"otv\"os parameter and
for the coupling between nuclear spin and gravity.
This is the first reported experimental test of the equivalence principle for
bosonic and fermionic particles and opens a new way to the search for the
predicted spin-gravity coupling effects.Comment: 5 pages, 4 figures. New spin-gravtity coupling analysis on the data
added to the manuscrip
Transformation of an Agulhas eddy near the continental slope
The transformation of Agulhas eddies near the
continental slope of southern Africa and their subsequent
self-propagation are analyzed in both observational data and
numerical simulations. Self-propagation results from a net
dipole moment of a generalized heton structure consisting
of a surface-intensified anticyclonic eddy and deep cyclonic
pattern. Such Agulhas vortical structures can form near the
retroflection region and further north along the western coast
of southern Africa. We analyze nonlinear topographic wave
generation, vortex deformations, and filament production as
an important part in water mass exchange. Self-propagating
structures provide a conduit for exchange between the deeNational Science Foundation (U.S.) (Grant OCE-0752346
Deep cyclogenesis by synoptic eddies interacting with a seamount
Strong deep eddies with cyclonic vorticity greater than 0.2 f0 were detected using an array of bottom current and pressure measurements in the Kuroshio Extension System Study (KESS) in 2004β2006. Daily maps showed these deep eddies developed locally. As in the Gulf Stream, meandering of the upper baroclinic jet generates deep cyclones and anticyclones by stretching and squashing the lower water column. However, unlike the Gulf Stream, the smaller vertical stretching and greater water depth in the Kuroshio Extension limits the relative vorticity generated by this vertical coupling process to about 0.1 f0. In the deep Kuroshio Extension the strong cases of vorticity generation and cyclone development are related to stretching driven when water columns are advected off isolated seamounts in the region. The large observed values of relative vorticity are consistent with a straightforward calculation of deep layer potential vorticity conservation.A barotropic model is used to illustrate the topographic generation of cyclones by ambient currents in synoptic eddies. Positive potential vorticity filaments also develop during the cyclogenetic process with width LR = O(20 km), where LR is the topographic Rhines scale, and travel anticyclonically around the seamount. Observational evidence lends support to the existence of submesoscale filaments, insomuch as current meter records near the flanks of seamounts exhibited bursts of eddy kinetic energy when bandpass-filtered between the inertial period and eight days
Impact of tropical cyclones on a baroclinic jet in the ocean
The initial evolution of a baroclinic jet under influence of a barotropic flow induced by the tropical cyclones is considered using a two-layer model and the thin-jet approximation. In spite of antisymmetric structure of the barotropic flow, the jet meander growth due to the barotropic flow advection is shown to favor an anticyclonic meander to the right of the storm track. This enhancement of the anticyclonic meander is found to be related to the dispersion properties of frontal waves along the jet described by the thin-jet theory and coupling with deep eddies developing in the lower layer during the jet meandering.Π£ ΡΠ°ΠΌΠΊΠ°Ρ
Π΄Π²ΠΎΡΠ°ΡΠΎΠ²ΠΎΡ ΠΌΠΎΠ΄Π΅Π»Ρ ΡΠ° Π² Π½Π°Π±Π»ΠΈΠΆΠ΅Π½Π½Ρ ΡΠΎΠ½ΠΊΠΎΠ³ΠΎ ΡΡΡΡΠΌΠ΅Π½Ρ ΡΠΎΠ·Π³Π»ΡΠ΄Π°ΡΡΡΡΡ Π΅Π²ΠΎΠ»ΡΡΡΡ Π±Π°ΡΠΎΠΊΠ»ΠΈΠ½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠΌΠ΅Π½Ρ, Π²ΠΈΠΊΠ»ΠΈΠΊΠ°Π½ΠΎΠ³ΠΎ Π±Π°ΡΠΎΡΡΠΎΠΏΠ½ΠΎΡ ΡΠ΅ΡΡΡΡ, ΡΠ½Π΄ΡΠΊΠΎΠ²Π°Π½ΠΎΡ ΡΡΠΎΠΏΡΡΠ½ΠΈΠΌ ΡΠΈΠΊΠ»ΠΎΠ½ΠΎΠΌ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΠΎ, Π½Π΅ Π΄ΠΈΠ²Π»ΡΡΠΈΡΡ Π½Π° Π°Π½ΡΠΈΡΠΈΠΌΠ΅ΡΡΠΈΡΠ½Ρ ΡΡΡΡΠΊΡΡΡΡ Π±Π°ΡΠΎΡΡΠΎΠΏΠ½ΠΎΡ ΡΠ΅ΡΡΡ, ΡΡ Π°Π΄Π²Π΅ΠΊΡΡΡ ΠΏΡΠΈΠ·Π²ΠΎΠ΄ΠΈΡΡ Π΄ΠΎ ΠΌΠ΅Π°Π½Π΄ΡΡΠ²Π°Π½Π½Ρ Π±Π°ΡΠΎΠΊΠ»ΠΈΠ½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠΌΠ΅Π½Ρ ΡΠ° Π΄ΠΎ Π·ΡΠΎΡΡΠ°Π½Π½Ρ Π³ΠΎΠ»ΠΎΠ²Π½ΠΈΠΌ ΡΠΈΠ½ΠΎΠΌ Π°Π½ΡΠΈΡΠΈΠΊΠ»ΠΎΠ½ΡΡΠ½ΠΎΠ³ΠΎ ΠΌΠ΅Π°Π½Π΄ΡΡ ΠΏΡΠ°Π²ΠΎΡΡΡ Π²ΡΠ΄ ΡΡΠΎΡΠΌΡΡΠ΅ΠΊΠ°. ΠΠ½Π°ΠΉΠ΄Π΅Π½ΠΎ, ΡΠΎ ΠΏΠΎΡΠΈΠ»Π΅Π½Π½Ρ Π°Π½ΡΠΈΡΠΈΠΊΠ»ΠΎΠ½ΡΡΠ½ΠΎΠ³ΠΎ ΠΌΠ΅Π°Π½Π΄ΡΡ ΠΏΠΎΠ²'ΡΠ·Π°Π½Π΅ Π· Π΄ΠΈΡΠΏΠ΅ΡΡΡΠΉΠ½ΠΈΠΌΠΈ Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΡΠΌΠΈ ΡΡΠΎΠ½ΡΠ°Π»ΡΠ½ΠΈΡ
Ρ
Π²ΠΈΠ»Ρ (ΡΠΊΡ ΠΎΠΏΠΈΡΡΡΡΡΡΡ Ρ ΡΠ°ΠΌΠΊΠ°Ρ
ΡΠ΅ΠΎΡΡΡ ΡΠΎΠ½ΠΊΠΎΠ³ΠΎ ΡΡΡΡΠΌΠ΅Π½Ρ) Ρ Π· Π²Π·Π°ΡΠΌΠΎΠ΄ΡΡΡ Π· Π³Π»ΠΈΠ±ΠΈΠ½Π½ΠΈΠΌΠΈ Π²ΠΈΡ
ΠΎΡΠ°ΠΌΠΈ, ΡΠΊΡ ΡΠΎΠ·Π²ΠΈΠ²Π°ΡΡΡΡΡ Π² Π½ΠΈΠΆΠ½ΡΠΎΠΌΡ ΡΠ°ΡΡ ΠΎΠΊΠ΅Π°Π½Ρ ΠΏΡΠΈ ΠΌΠ΅Π°Π½Π΄ΡΡΠ²Π°Π½Π½Ρ Π±Π°ΡΠΎΠΊΠ»ΠΈΠ½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠΌΠ΅Π½Ρ.Π ΡΠ°ΠΌΠΊΠ°Ρ
Π΄Π²ΡΡ
ΡΠ»ΠΎΠΉΠ½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈ Π² ΠΏΡΠΈΠ±Π»ΠΈΠΆΠ΅Π½ΠΈΠΈ ΡΠΎΠ½ΠΊΠΎΠΉ ΡΡΡΡΠΈ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΡΡΡ ΡΠ²ΠΎΠ»ΡΡΠΈΡ Π±Π°ΡΠΎΠΊΠ»ΠΈΠ½Π½ΠΎΠΉ ΡΡΡΡΠΈ, Π²ΡΠ·Π²Π°Π½Π½ΠΎΠΉ Π±Π°ΡΠΎΡΡΠΎΠΏΠ½ΡΠΌ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ΠΌ, ΠΈΠ½Π΄ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ ΡΡΠΎΠΏΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠΈΠΊΠ»ΠΎΠ½ΠΎΠΌ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ, Π½Π΅ΡΠΌΠΎΡΡΡ Π½Π° Π°Π½ΡΠΈΡΠΈΠΌΠΌΠ΅ΡΡΠΈΡΠ½ΡΡ ΡΡΡΡΠΊΡΡΡΡ Π±Π°ΡΠΎΡΡΠΎΠΏΠ½ΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΡ, Π΅Π³ΠΎ Π°Π΄Π²Π΅ΠΊΡΠΈΡ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΠΌΠ΅Π°Π½Π΄ΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π±Π°ΡΠΎΠΊΠ»ΠΈΠ½Π½ΠΎΠΉ ΡΡΡΡΠΈ ΠΈ ΠΊ ΡΠΎΡΡΡ Π³Π»Π°Π²Π½ΡΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ Π°Π½ΡΠΈΡΠΈΠΊΠ»ΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠ΅Π°Π½Π΄ΡΠ° ΡΠΏΡΠ°Π²Π° ΠΎΡ ΡΡΠΎΡΠΌΡΡΠ΅ΠΊΠ°. ΠΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΎ, ΡΡΠΎ ΡΡΠΈΠ»Π΅Π½ΠΈΠ΅ Π°Π½ΡΠΈΡΠΈΠΊΠ»ΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠ΅Π°Π½Π΄ΡΠ° ΡΠ²ΡΠ·Π°Π½ΠΎ Ρ Π΄ΠΈΡΠΏΠ΅ΡΡΠΈΠΎΠ½Π½ΡΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ ΡΡΠΎΠ½ΡΠ°Π»ΡΠ½ΡΡ
Π²ΠΎΠ»Π½ (ΠΎΠΏΠΈΡΡΠ²Π°Π΅ΠΌΡΡ
Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΡΠ΅ΠΎΡΠΈΠΈ ΡΠΎΠ½ΠΊΠΎΠΉ ΡΡΡΡΠΈ) ΠΈ Ρ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ Ρ Π³Π»ΡΠ±ΠΈΠ½Π½ΡΠΌΠΈ Π²ΠΈΡ
ΡΡΠΌΠΈ, ΡΠ°Π·Π²ΠΈΠ²Π°ΡΡΠΈΠΌΠΈΡΡ Π² Π½ΠΈΠΆΠ½Π΅ΠΌ ΡΠ»ΠΎΠ΅ ΠΎΠΊΠ΅Π°Π½Π° ΠΏΡΠΈ ΠΌΠ΅Π°Π½Π΄ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Π±Π°ΡΠΎΠΊΠ»ΠΈΠ½Π½ΠΎΠΉ ΡΡΡΡΠΈ
Evidence of Vertical Coupling between the Kuroshio Extension and Topographically Controlled Deep Eddies
Strong energy in the 30β60 day band was observed using 39 deep pressure and current records from the Kuroshio Extension System Study (KESS). Energy in this band accounted for 25β50% of the total deep-pressure variance and was strongest under the Kuroshio Extension jet axis. Often, deep-pressure anomalies propagated into the region from the north-northeast and locally intensified as they passed under and interacted with the Kuroshio Extension. The topographically controlled deep-pressure anomalies translate nearly along lines of constant f/H. Statistically significant coherence between 30β60 day upper- and deep-ocean streamfunction anomalies demonstrated that there was strong vertical coupling in that time band. Twenty-five percent of the total upper-ocean streamfunction variance was contained within the 30β60 day band near the Kuroshio Extension. Joint CEOFs of the upper- and deep-ocean streamfunctions revealed that near the axis of the Kuroshio Extension the phases were laterally offset alongstream, with the deep ocean leading the upper ocean. This arrangement is attributed to producing joint development of upper-ocean meanders and deep-pressure anomalies.A numerical process model simulated the interaction of barotropic TRWs with an eastward-flowing baroclinic jet. When the TRWs, used as a surrogate for topographically steered deep-pressure anomalies, passed under the jet, they intensified and upper-ocean meanders steepened, much like the observed interactions. The model illustrates how the interaction between TRWs and an eastward-flowing jet, at its simplest level, can reproduce many of the major traits of our observations. The Ocean General Circulation Model for the Earth Simulator also showed similar processes in the 30β60 day band in the KESS region. The strongest variance in the deep fields occurred under the Kuroshio Extension. Upper and deep low- and high-pressure anomalies propagated south southwestward across the Kuroshio Extension, with model phase speeds and wavelengths matching the KESS observations
The Dok Cold Eddy
Current and temperature patterns in the Ulleung Basin of the Japan/East Sea are examined using acoustic travel-time measurements from an array of pressure-gauge-equipped inverted echo sounders moored between June 1999 and July 2001. The focus here is the formation and behavior of a persistent cold eddy observed south of Dok Island, referred to as the Dok Cold Eddy (DCE), and meandering of the Subpolar Front. The DCE is typically about 60 km in diameter and originates from the pinching off of a Subpolar Front meander between Ulleung and Dok Islands. After formation, the DCE dwells southwest of Dok Island for 1β6 months before propagating westward toward Korea, where it deflects the path of the East Korean Warm Current (EKWC). Four such DCE propagation events between January and June 2000 each deflected the EKWC, and after the fourth deflection the EKWC changed paths and flowed westward along the Japanese shelf as the βOffshore Branchβ from June through November 2000. Beginning in March 2001, a deep, persistent meander of the Subpolar Front developed and oscillated with a period near 60 days, resulting in the deformation and northwestward displacement of the Ulleung Eddy. Satellite-altimeter data suggest that the Ulleung Eddy may have entered the northern Japan/East Sea. The evolution of this meander is compared with thin-jet nonlinear dynamics described by the modified KortewegβdeVries equation
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