1995
DOI: 10.2151/jmsj1965.73.1_37
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Laboratory Experiments of Lagrangian Motions in a Steady Baroclinic Wave

Abstract: The basic structure of steady baroclinic waves observed in a differentially-heated rotating-fluid annulus is found to be composed of high-and low-pressure vortices, upper-level (eastward) and lower-level (westward) jet-streams meandering through the vortices, and boundary layers. On the basis of this structure, recently, Sugata and Yoden (1994) numerically studied the Lagrangian motion of a fluid particle in the annulus. Stimulated by their results, we conducted experiments on a rotating-fluid annulus by injec… Show more

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Cited by 6 publications
(9 citation statements)
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“…As in the f -plane experiment, the regular eddy features seen with oppositely sloping endwalls in the present system consist of a series of closed, compact, oval anti-cyclonic eddies ͑at the upper level͒. The vortex character of these essentially baroclinic eddies not only suggests that fluid may be trapped for extended periods within their stagnant core, 36,44 but also that the dispersion of the individual wave components expected from the linear perturbation theory of Hide 45 is being effectively suppressed by nonlinear interactions between the various competing wave modes. Further departures from this linear theory are indicated by the profound asymmetry between the regular wave regimes of the ‫ץ‬D/‫ץ‬rϾ0 and ‫ץ‬D/‫ץ‬rϽ0 endwall experiments, with regular modes mϭ1 to 5 being observed with the former boundary arrangement, but only the mode mϭ1 being observed with the latter configuration.…”
Section: Discussionsupporting
confidence: 53%
“…As in the f -plane experiment, the regular eddy features seen with oppositely sloping endwalls in the present system consist of a series of closed, compact, oval anti-cyclonic eddies ͑at the upper level͒. The vortex character of these essentially baroclinic eddies not only suggests that fluid may be trapped for extended periods within their stagnant core, 36,44 but also that the dispersion of the individual wave components expected from the linear perturbation theory of Hide 45 is being effectively suppressed by nonlinear interactions between the various competing wave modes. Further departures from this linear theory are indicated by the profound asymmetry between the regular wave regimes of the ‫ץ‬D/‫ץ‬rϾ0 and ‫ץ‬D/‫ץ‬rϽ0 endwall experiments, with regular modes mϭ1 to 5 being observed with the former boundary arrangement, but only the mode mϭ1 being observed with the latter configuration.…”
Section: Discussionsupporting
confidence: 53%
“…As was found in SY and experimentally in our previous paper (Tajima et al, 1995a(Tajima et al, , 1995b, the structure of vortices is composed of a core region, which is rather well isolated, and next to the core, a transition zone (sometimes called a separatrix layer in the papers concerning a chaotic advection (cf. Weiss and Knobloch, 1989)) where fluid particles are frequently transported to and from its outside, but rarely to the core.…”
Section: Observed Trajectoriessupporting
confidence: 63%
“…Sugata and Yoden (1994), hereafter referred to as SY, investigated the Lagrangian motion in a steady baroclinic wave of wavenumber-5 by tracing a marked fluid particle for a long time in a numerical solution of their model (Sugata and Yoden, 1993). As was schematically shown in our previous papers (Tajima and Nakamura, 1995;Tajima et al, 1995aTajima et al, , 1995b, the steady baroclinic wave has been well known to have the following basic structure: the upper (UJ, eastward)-and lower (U, Jwestward)-level jets, the high (HV)-and low (LV)-pressure vortices, and the inner (TB)-, outer (OB)-and lower (LB)-boundary layers. Based on this structure, Sugata and Yoden calculated the residence time of the fluid particle in each region and the transition matrix which expresses frequencies of transitions between the regions.…”
Section: Introductionmentioning
confidence: 99%
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