2016
DOI: 10.1016/j.ocemod.2016.09.013
|View full text |Cite
|
Sign up to set email alerts
|

Baroclinic turbulence on the polar β-plane in the rotating tank: Down to submesoscale

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

1
5
0

Year Published

2017
2017
2024
2024

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 10 publications
(6 citation statements)
references
References 26 publications
1
5
0
Order By: Relevance
“…The 50 and 60 rpm cases clearly show spatiotemporally coherent, multiple zonal jet flow can develop in thermally‐driven laboratory experiments, thus extending the findings of, for example, Smith et al. (2014); Zhang and Afanasyev (2016); Cabanes et al. (2017); Lemasquerier et al.…”
Section: Resultssupporting
confidence: 81%
See 1 more Smart Citation
“…The 50 and 60 rpm cases clearly show spatiotemporally coherent, multiple zonal jet flow can develop in thermally‐driven laboratory experiments, thus extending the findings of, for example, Smith et al. (2014); Zhang and Afanasyev (2016); Cabanes et al. (2017); Lemasquerier et al.…”
Section: Resultssupporting
confidence: 81%
“…It also has similarities to the devices used to study oceanic and atmospheric flows in Matulka et al. (2016); Zhang and Afanasyev (2016, 2021) and to study atmospheric waves and mean flow dynamics in Rodda et al. (2018); Rodda et al.…”
Section: Introductionmentioning
confidence: 99%
“…The kinetic energy spectrum provides insights into the distribution of energy across different scales and is diagnostic of the flow regime. Analysis of rotating tanks with a beta plane may proceed in terms of full cylindrical polar coordinates with Bessel functions in the radial direction and Fourier modes in the azimuthal direction (e.g., Galperin, Hoemann, et al., 2014; Galperin et al., 2016; Y. Afanasyev & Wells, 2005; Zhang & Afanasyev, 2014, 2016), or alternatively, when the focus is on relatively narrow zones as in this study, a local Cartesian framework and double‐Fourier decomposition are effective (e.g., Zhang & Afanasyev, 2014, 2016). Employing the latter, denote the Fourier transform of the Cartesian velocity components as )(trueu,truev $\left(\tilde{u},\tilde{v}\right)$, and the wavenumber components as ( k x , k y ), and define E)(kx,ky=12)(trueuu+truevv $E\left({k}_{x},{k}_{y}\right)=\frac{1}{2}\left(\tilde{u}{\tilde{u}}^{\ast }+\tilde{v}{\tilde{v}}^{\ast }\right)$, where u ${\tilde{u}}^{\ast }$ is the complex conjugate of trueu $\tilde{u}$.…”
Section: Resultsmentioning
confidence: 99%
“…For the first class, the directly forced zonal jets can be shear‐driven by differentially moving boundaries (e.g., Aguiar et al., 2010; Hide & Titman, 1967) or result from the conservation of angular momentum and an imposed radial flow between sources and sinks at different radii (e.g., Hide, 1968; Solomon et al., 1993; Sommeria et al., 1989; Tian et al., 2001; Weeks et al., 1997). Indirectly forced jets are the product of flow dynamics; for example, active forcing can generate and maintain an eddy field characterized by relatively small length scales, which becomes anisotropic due to the β ‐effect and cascades energy into larger‐scale zonal flows, and ultimately, an eddy‐driven zonal jet (e.g., Afanasyev & Wells, 2005; Cabanes et al., 2017; Lemasquerier et al., 2021; Matulka et al., 2016; Zhang & Afanasyev, 2016). Indirectly forced jets can also arise from the turbulence associated with small‐scale convection (e.g., Condie & Rhines, 1994; Matulka et al., 2016; Read et al., 2007; Zhang & Afanasyev, 2014), electromagnetic forcing with a conductive working fluid (e.g., Afanasyev & Wells, 2005; Afanasyev, 2019; Espa et al., 2008, 2019), or the radiation of Rossby waves by eddies via beta‐plume mechanisms (e.g., Afanasyev et al., 2011; Afanasyev & Ivanov, 2019; Zhang & Afanasyev, 2015).…”
Section: Introductionmentioning
confidence: 99%