Treatise on Geophysics 2007
DOI: 10.1016/b978-044452748-6.00127-9
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Large-Scale Flow in the Core

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Cited by 137 publications
(189 citation statements)
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References 82 publications
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“…2 shows the structure of the inferred jet in 2015 defined with M = 1, which is described by just three unknown coefficients and has associated optimal δ = 0.12 (in dimensional units 420 km). The jet has a maximum velocity of about 40 km yr −1 , twice the speed of the equatorial flux patches of 18 km yr −1 [9], and three times the typical rms speed of 13 km yr −1 from globalscale core-flow inversions [21]. This jet is confined in longitude and so it is neither circumpolar nor zonal, despite being predominantly azimuthal.…”
Section: Observationally-constrained High-latitude Flowmentioning
confidence: 99%
See 1 more Smart Citation
“…2 shows the structure of the inferred jet in 2015 defined with M = 1, which is described by just three unknown coefficients and has associated optimal δ = 0.12 (in dimensional units 420 km). The jet has a maximum velocity of about 40 km yr −1 , twice the speed of the equatorial flux patches of 18 km yr −1 [9], and three times the typical rms speed of 13 km yr −1 from globalscale core-flow inversions [21]. This jet is confined in longitude and so it is neither circumpolar nor zonal, despite being predominantly azimuthal.…”
Section: Observationally-constrained High-latitude Flowmentioning
confidence: 99%
“…where u H denotes the horizontal flow [21]. We prescribe δ and M and fit the resulting 2M + 1 modal coefficients by minimising the target residual defined over both northern (N) and southern (S) regions…”
Section: Observationally-constrained High-latitude Flowmentioning
confidence: 99%
“…Using Earth's rotation rate of = 0.729 × 10 −4 s −1 in the numerical calculations gives a root-mean-square (rms) velocity of about 0.037 mm yr −1 . This value is about an order of magnitude smaller than the rms velocity, V rms = 0.38 mm s −1 , inferred from coresurface flow (Holme 2015). By adjusting the rotation rate in the model to = 7.383 × 10 −4 s −1 we produce an rms velocity that matches the core-surface flow.…”
Section: Time Dependence Of Sourcesmentioning
confidence: 78%
“…These are typically based on dynamics relevant to core flow, such as tangentially geostrophic (TG) flow, purely toroidal (PT) flow and helical flow [see, e.g., Holme, 2007], as well as the recent quasigeostrophic flow [Pais and Jault, 2008]. Among these the TG assumption has been most commonly employed, in which the Lorentz force is eliminated from the horizontal force balance at the core surface, resulting in TG equilibrium.…”
Section: Introductionmentioning
confidence: 99%
“…Instead of fitting the observed SV tightly, one needs to allow for a possible error from the unmodeled SV [Pais and Jault, 2008;Gillet et al, 2009]. The theoretical non-uniqueness problem in the flow modeling [e.g., Holme, 2007] is another setback which is even more serious. Assumptions used to alleviate the flow uncertainty can distort resulting flow images more significantly than the errors estimated for the unmodeled SV.…”
Section: Introductionmentioning
confidence: 99%