4.1 Article

A laboratory study of global-scale wave interactions in baroclinic flow with topography II: vacillations and low-frequency variability

期刊

GEOPHYSICAL AND ASTROPHYSICAL FLUID DYNAMICS
卷 109, 期 4, 页码 359-390

出版社

TAYLOR & FRANCIS LTD
DOI: 10.1080/03091929.2015.1055477

关键词

Baroclinic instability; Baroclinic waves; Sloping convection; Topography; Flow regimes

资金

  1. UK Natural Environment Research Council
  2. EPSRC [EP/K029428/1] Funding Source: UKRI
  3. NERC [NE/F002157/1] Funding Source: UKRI
  4. Engineering and Physical Sciences Research Council [EP/K029428/1] Funding Source: researchfish
  5. Natural Environment Research Council [NE/F002157/1] Funding Source: researchfish

向作者/读者索取更多资源

A laboratory investigation is presented with the aim of studying systematically the occurrence and characteristics of low-frequency variability of flows resulting from the interaction of a baroclinic flow with periodic bottom topography. Low-frequency variability within the baroclinic wave regime occurred in two distinct forms in separate regions of parameter space. One corresponded to the transition region between the baroclinic travelling and stationary wave regimes. It involved primarily an interaction between the drifting baroclinic waves and stationary components of the topographically forced wave. The resulting flow had characteristics similar to amplitude vacillation and had a time-scale of 30-60 annulus revolutions (days), which also corresponded to the wave drift period. A new regime of low-frequency amplitude vacillation was discovered in the transition region with the axisymmetric flow regime. As the complexity of the flow increased the period of the vacillation cycles grew to similar to 100-180 days. This slower vacillation seemed to involve a cyclic enabling and disabling of nonlinear interactions between the forced stationary wave and the growing and azimuthally drifting wave, which in turn was linked to a decrease in mean flow shear. Subsequent chains of wave-wave interactions characterised the complex but robust oscillation phenomenon. The resulting behaviour has several features in common with some recent models of intraseasonal oscillations in the mid-latitude troposphere and with sudden stratospheric warmings.

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