The DOI matches its Crossref record; 29 of the 31 references it cites were found in a registry or an index.
Waves and turbulence on a beta-plane
Abstract
Two-dimensional eddies in a homogeneous fluid at large Reynolds number, if closely packed, are known to evolve towards larger scales. In the presence of a restoring force, the geophysical beta-effect, this cascade produces a field of waves without loss of energy, and the turbulent migration of the dominant scale nearly ceases at a wavenumber k β = (β/2 U ) ½ independent of the initial conditions other than U , the r.m.s. particle speed, and β, the northward gradient of the Coriolis frequency. The conversion of turbulence into waves yields, in addition, more narrowly peaked wavenumber spectra and less fine-structure in the spatial maps, while smoothly distributing the energy about physical space. The theory is discussed, using known integral constraints and similarity solutions, model equations, weak-interaction wave theory (which provides the terminus for the cascade) and other linearized instability theory. Computer experiments with both finite-difference and spectral codes are reported. The central quantity is the cascade rate, defined as \[ T = 2\int_0^{\infty} kF(k)dk/U^3\langle k\rangle , \] where F is the nonlinear transfer spectrum and 〈 k 〉 the mean wavenumber of the energy spectrum. (In unforced inviscid flow T is simply U −1 d 〈 k 〉 −1 / dt , or the rate at which the dominant scale expands in time t .) T is shown to have a mean value of 3·0 × 10 −2 for pure two-dimensional turbulence, but this decreases by a factor of five at the transition to wave motion. We infer from weak-interaction theory even smaller values for k [Lt ] k β . After passing through a state of propagating waves, the homogeneous cascade tends towards a flow of alternating zonal jets which, we suggest, are almost perfectly steady. When the energy is intermittent in space, however, model equations show that the cascade is halted simply by the spreading of energy about space, and then the end state of a zonal flow is probably not achieved. The geophysical application is that the cascade of pure turbulence to large scales is defeated by wave propagation, helping to explain why the energy-containing eddies in the ocean and atmosphere, though significantly nonlinear, fail to reach the size of their respective domains, and are much smaller. For typical ocean flows, $k_{\beta}^{-1} = 70\,{\rm km} $ , while for the atmosphere, $k_{\beta}^{-1} = 1000\,{\rm km}$ . In addition the cascade generates, by itself, zonal flow (or more generally, flow along geostrophic contours).
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In the citing paper
“Based on the Rhines scale L R ∼ ( u RMS /β ) 1 / 2 (Rhines 1975), where we recall that u RMS takes into account all the components of the flow (equation (3.1)), we do expect an increase of the jets width during the transition, since the RMS eddy velocity increases.”
From Zonal jets at the laboratory scale: hysteresis and Rossby waves resonance (2021) · cites this paper as Rhines 1975
In the citing paper
“Originally defined in Rhines (1975), it has often been associated with the width of zonal jets.”
From Zonal jets at the laboratory scale: hysteresis and Rossby waves resonance (2021) · cites this paper as Rhines 1975
In the citing paper
“Under this scale, the advective term dominates and above it the β -term is dominant.”
From Zonal jets at the laboratory scale: hysteresis and Rossby waves resonance (2021) · cites this paper as Rhines 1975
In the citing paper
“This is likely driven by the topographical β effect, due to the spherical shell geometry, which is stronger near the equator, promoting strong axisymmetric jets, while, at higher latitudes, the β -effect decreases and the system approaches a rotating plane layer where the formation of giant vortices is favored”
From Deep rotating convection generates the polar hexagon on Saturn (2020) · cites this paper as [38]
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Metadata
- Authors
- Rhines, P. B.
- Affiliations
- Woods Hole Oceanographic Institution (US)
- Corresponding author
- Rhines, Peter B.
- Venue
- Journal of Fluid Mechanics
- Publisher
- Cambridge University Press (CUP)
- Published
- 1975-06-10
- Volume
- 69
- Issue
- 3
- Pages
- 417-443
- ISSN
- 0022-1120 (ISSN-L)
- 1469-7645
- OpenAlex
- W2099743374
- Cited by
- 1,177
- References
- 31
- Citations by year
- 2026: 15 · 2025: 27 · 2024: 50 · 2023: 38 · 2022: 43 · 2021: 44 · 2020: 48 · 2019: 71 · 2018: 42 · 2017: 38 · 2016: 28 · 2015: 39 · 2014: 36 · 2013: 38 · 2012: 28
- FWCI
- 26.81
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- Journal of Fluid Mechanics (publishedVersion)
- Topics
- Physical Sciences › Engineering › Computational Mechanics › Fluid Dynamics and Turbulent Flows
- Physical Sciences › Earth and Planetary Sciences › Oceanography › Oceanographic and Atmospheric Processes
- Physical Sciences › Earth and Planetary Sciences › Oceanography › Ocean Waves and Remote Sensing
- Keywords
- beta-plane, two-dimensional turbulence, energy cascade, wave propagation, zonal jets, energy-containing eddies, integral constraints, self-similar solutions, model equations, weakly nonlinear waves
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
Statistics and arithmetic are recomputed, not judged.
Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.
What counts as a claim ›How we measure confidence ›How we check this ›
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